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pscp-1993.csv
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# Data from paperscape.org
# If you use this data, please give due credit to: Damien P. George and Rob Knegjens, Paperscape
# A citable DOI for this data can be found at http://github.com/paperscape/paperscape-data
#
# Format is 1 line per entry, with 7 fields separated by semicolons:
# arxiv-id;comma-separated-arxiv-categories;num-found-refs;num-total-refs;comma-separated-refs;comma-separated-authors;title
# Parse with Python code: entries = [line.split(";", 7) for line in open("file")]
# See comments at the bottom of this file for statistics
hep-th/9301001;hep-th;0;22;;G.K.Savvidy,K.G.Savvidy;Gonihedric String and Asymptotic Freedom
cond-mat/9301001;cond-mat;0;13;;H.Nakanishi;Effect of Loops on the Vibrational Spectrum of Percolation Network
cs/9301101;cs.LO;0;26;;L.C.Paulson;Verifying the Unification Algorithm in LCF
cs/9301102;cs.LO;0;25;;L.C.Paulson;Constructing Recursion Operators in Intuitionistic Type Theory
cs/9301103;cs.LO;0;12;;L.C.Paulson;Proving Termination of Normalization Functions for Conditional Expressions
cs/9301104;cs.LO;0;38;;L.C.Paulson;Natural Deduction as Higher-Order Resolution
cs/9301105;cs.LO;0;35;;L.C.Paulson;The Foundation of a Generic Theorem Prover
cs/9301106;cs.LO;0;0;;L.C.Paulson;Isabelle: The Next 700 Theorem Provers
cs/9301107;cs.LO;0;0;;L.C.Paulson;A Formulation of the Simple Theory of Types (for Isabelle)
cs/9301108;cs.LO;0;0;;L.C.Paulson;A Higher-Order Implementation of Rewriting
cs/9301109;cs.LO;0;46;;L.C.Paulson,A.W.Smith;Logic Programming, Functional Programming, and Inductive Definitions
cs/9301110;cs.LO;0;0;;L.C.Paulson;Designing a Theorem Prover
cs/9301111;cs.CC;0;0;;D.E.Knuth;Nested satisfiability
cs/9301112;cs.GR;0;0;;D.E.Knuth;A note on digitized angles
cs/9301113;cs.CC;0;0;;D.E.Knuth;Textbook examples of recursion
cs/9301114;cs.GL;0;0;;D.E.Knuth;Theory and practice
cs/9301115;cs.DS;0;0;;D.E.Knuth;Context-free multilanguages
cs/9301116;cs.DS,math.CO;0;0;;D.E.Knuth,A.Raghunathan;The problem of compatible representatives
hep-th/9301002;hep-th,gr-qc;0;0;;I.Antoniadis,P.O.Mazur,E.Mottola;Scaling behavior of quantum four-geometries
nucl-th/9301001;nucl-th,hep-ph;0;43;;B.-Q.Ma;Effect due to compositeness of nucleons in deep inelastic lepton nucleus scattering
hep-th/9301003;hep-th;0;19;;J.A.Minahan;Summing Over Inequivalent Maps in the String Theory Interpretation of Two Dimensional QCD
hep-ph/9301201;hep-ph;0;0;;T.Vachaspati;Electroweak Strings: A Progress Report
hep-ph/9301202;hep-ph;0;19;;J.R.Forshaw;On the Validity of Perturbative Evolution of Structure Functions from Low $Q^2$
hep-ph/9301203;hep-ph;0;12;;R.Decker,E.Mirkes;Measuring the Wess-Zumino Anomaly in Tau Decays
hep-ph/9301204;hep-ph;0;29;;J.H.K"uhn,E.Mirkes;QCD Corrections to Toponium Production at Hadron Colliders
hep-th/9301004;hep-th;1;23;hep-th/9204082;B.Eynard,J.Zinn-Justin;Large Order Behaviour of 2D Gravity Coupled to $d<1$ Matter
nucl-th/9301002;nucl-th;0;24;;J.Piekarewicz,A.G.Williams;The Momentum Dependence of the $ρ-ω$ Mixing Amplitude in a Hadronic Model
alg-geom/9301001;alg-geom,math.AG;0;0;;A.Libgober,J.Teitelbaum;Lines on Calabi Yau complete intersections, mirror symmetry, and Picard Fuchs equations
hep-th/9301005;hep-th;3;8;hep-th/9110053,hep-th/9112070,hep-th/9206051;M.Henningson,C.R.Nappi;Duality, Marginal Perturbations and Gauging
hep-ph/9301205;hep-ph;0;0;;J.F.Gunion,H.E.Haber;Errata for Higgs Bosons in Supersymmetric Models: I, II and III
hep-ph/9301206;hep-ph;0;0;;H.J.Lipkin;Implications of $τ$ Decays into Strange Scalar and Axial Vector Mesons
hep-ph/9301207;hep-ph;0;41;;O.W.Greenberg;Color, from baryon spectroscopy to qcd
gr-qc/9301001;gr-qc;0;31;;O.Coussaert,M.Henneaux;Bianchi Cosmological Models and Gauge Symmetries
hep-ph/9301208;hep-ph;0;0;;K.S.Gupta,S.Guruswamy,S.G.Rajeev;Spherical Quantum Chromodynamics of Heavy Quark Systems
hep-ph/9301209;hep-ph;0;7;;A.R.White,I.G.Knowles,K.Kang;The $η_6$ and Massive Photon Pairs at LEP
hep-ph/9301210;hep-ph;0;3;;F.D.T.Smith;Calculation of 130 Gev Mass for T-Quark
hep-th/9301006;hep-th;0;29;;K.Demeterfi,I.R.Klebanov;Light-cone approach to random surfaces embedded in two dimensions
hep-th/9301007;hep-th;0;43;;F.W.Nijhoff,H.W.Capel;Integrability and Fusion Algebra for Quantum Mappings
hep-th/9301008;hep-th,cond-mat,hep-ph;0;8;;D.Spector;A Simple Method for Computing Soliton Statistics
hep-th/9301009;hep-th,math.QA;0;22;;Y.-Z.Huang,J.Lepowsky;Vertex operator algebras and operads
hep-th/9301010;hep-th;0;5;;A.Ali,A.Kumar;A New $N = 4$ Superconformal Algebra
hep-th/9301011;hep-th,math.QA;0;6;;E.Ragoucy;Characteristic Dynkin diagrams and W-algebras
hep-th/9301012;hep-th;0;8;;B.Nienhuis,R.Rietman;A Solvable Model for Intersecting Loops
hep-th/9301013;hep-th;0;17;;M.P.Fry;Fermionic Determinant of the Massive Schwinger Model
nucl-th/9301003;nucl-th;0;22;;H.Mishra,S.P.Misra,P.K.Panda,B.K.Parida;Neutron matter - Quark matter phase transition and Quark star
hep-th/9301014;hep-th,hep-ph;0;27;;Z.Hlousek,D.Spector;Solitons and Instantons with(out) Supersymmetry
cond-mat/9301002;cond-mat,hep-ph;0;49;;O.W.Greenberg;Quons, an interpolation between bose and fermi oscillators
alg-geom/9301002;alg-geom,math.AG;0;0;;O.Debarre;Minimal Cohomology Classes and Jacobians
cond-mat/9301003;cond-mat;0;28;;N.E.Bonesteel;Spin-Orbit Scattering and Pair Breaking in a Structurally Disordred Copper-Oxide Layer
cond-mat/9301004;cond-mat;0;0;;J.Lee;Heap Formation in Granular Media
hep-th/9301015;hep-th;10;57;hep-th/9108001,hep-th/9110053,hep-th/9110054,hep-th/9111040,hep-th/9112070,hep-th/9202092,hep-th/9205037,hep-th/9206006,hep-th/9206007,hep-th/9207118;A.A.Tseytlin;Effective action of gauged WZW model and exact string solutions
hep-th/9301016;hep-th;0;0;;H.Arfaei,A.Shirzad;Modular Invariant Partition Functions and Method of Shift Vector
nucl-th/9301004;nucl-th;0;60;;S.S.Kamalov,L.Tiator,C.Bennhold;Pion interaction with the trinucleon up to the eta production threshold
gr-qc/9301002;gr-qc;0;0;;E.Malec;Event horizons and apparent horizons in spherically symmetric geometries
alg-geom/9301003;alg-geom,math.AG;0;12;;M.Coppens,T.Kato;Non-trivial Linear Systems on Smooth Plane Curves
gr-qc/9301003;gr-qc,astro-ph;1;50;gr-qc/9209010;L.S.Finn,D.F.Chernoff;Observing binary inspiral in gravitational radiation: One interferometer
hep-ph/9301211;hep-ph,astro-ph;0;24;;E.Kh.Akhmedov,S.T.Petcov,A.Yu.Smirnov;Neutrinos with Mixing in Twisting Magnetic Fields
hep-th/9301017;hep-th;1;42;hep-th/9109037;K.Becker,M.Becker;Nonperturbative Solution of the Super-Virasoro Constraints
hep-lat/9301001;hep-lat;0;10;;A.Duncan,E.Eichten,H.Thacker;Heavy-Light Wavefunctions in Lattice QCD
hep-ph/9301212;hep-ph;1;20;hep-ph/9209291;T.Ohl,G.Ricciardi,E.H.Simmons;D\bar D$ Mixing in Heavy Quark Effective Field Theory: The Sequel
hep-ph/9301213;hep-ph;1;57;hep-ph/9205230;K.S.Babu,I.Z.Rothstein,D.Seckel;Planck Scale Symmetry Breaking and Majoron Physics
hep-th/9301018;hep-th;3;39;hep-th/9109021,hep-th/9202020,hep-th/9206034;A.Kuniba,T.Nakanishi,J.Suzuki;Characters in Conformal Field Theories from Thermodynamic Bethe Ansatz
hep-th/9301019;hep-th;1;35;hep-th/9204039;A.Aurilia,A.Smailagic,E.Spallucci;Gauge Theory of the String Geodesic Field
hep-th/9301020;hep-th;0;0;;T.TADA,S.UEHARA;On the Mass of Two Dimensional Quantum Black Hole
cond-mat/9301005;cond-mat;0;0;;D.Poilblanc,T.Ziman,J.Bellissard,F.Mila,G.Montambaux;Poisson versus GOE statistics in integrable and non-integrable quantum hamiltonian
nucl-th/9301005;nucl-th;0;0;;M.Baldo,A.Causa,A.Rapisarda;Revealing Intermittency in Nuclear Multifragmentation with 4$\PI $ Detectors
hep-ph/9301214;hep-ph;1;28;hep-ph/9207233;G.Triantaphyllou;QED Radiative Corrections to the Decay $π^0 →e^+e^-$
hep-ph/9301215;hep-ph;0;10;;J.Pumplin;Quark-Gluon Jet Differences at LEP
hep-ph/9301216;hep-ph;0;20;;J.Pumplin;Double Pomeron Opportunities at SQRT(s) = 1.8 Tev
astro-ph/9301001;astro-ph;0;49;;P.Marziani,J.W.Sulentic,M.Calvani,E.Perez,M.Moles,M.V.Penston;The Peculiar Balmer Line Profiles of OQ 208
hep-ph/9301217;hep-ph;1;19;hep-ph/9203203;J.Ignatius;Bubble Free Energy in Cosmological Phase Transitions
astro-ph/9301002;astro-ph,hep-ph;0;19;;S.Dodelson,J.M.Jubas;Microwave Anisotropies in the Light of COBE
hep-ph/9301218;hep-ph;1;19;hep-ph/9208206;E.Shuryak,L.Xiong;Dilepton and photon production in the 'hot-glue' scenario
cond-mat/9301006;cond-mat;0;9;;S.C.Erwin,M.R.Pederson;Electronic Structure of Superconducting Ba6c60
hep-th/9301021;hep-th,gr-qc;6;13;hep-th/9203054,hep-th/9205069,hep-th/9206020,hep-th/9206070,hep-th/9209012,hep-th/9209118;A.Bilal;Positive Energy Theorem and Supersymmetry in Exactly Solvable Quantum-Corrected 2D Dilaton-Gravity
gr-qc/9301004;gr-qc,hep-th;0;7;;J.Finkelstein;On the Definition of Decoherence
hep-ph/9301219;hep-ph;0;0;;J.Anderson,M.A.Luty;Chiral Corrections to Hyperon Vector Form Factors
hep-th/9301022;hep-th;7;25;hep-th/9108004,hep-th/9109032,hep-th/9111021,hep-th/9111035,hep-th/9201056,hep-th/9202072,hep-th/9206111;M.Li;A proposal on the topological sector of 2d string
astro-ph/9301003;astro-ph;0;0;;M.A.Abramowicz,G.Bao,V.Karas,A.Lanza;Similarity of the variability patterns in the Exosat and Ginga folded light curves of the Seyfert galaxy NGC 6814
hep-th/9301023;hep-th,math.QA;0;11;;C.Schwiebert;Reflection equation and link polynomials for arbitrary genus solid tori
hep-ph/9301220;hep-ph,hep-th;0;14;;A.E.Faraggi;Construction of Realistic superstring Standard--like Models
hep-ph/9301221;hep-ph;0;19;;J.Bartelski,S.Tatur;A possible glueball contribution to the Goldberger-Treiman relations
cond-mat/9301007;cond-mat;0;19;;H.J.Schulz;Wigner Crystal in One Dimension
hep-th/9301024;hep-th,cond-mat;0;23;;F.Delduc,E.Ivanov;$N=4$ super KdV equation
hep-th/9301025;hep-th,hep-ph;0;0;;C.-I.Tan;Ideal Gas of Strings and QCD at Hadronic Scales
gr-qc/9301005;gr-qc;0;0;;R.Laflamme;Time Symmetric Quantum Cosmology and Our Universe
cond-mat/9301008;cond-mat,gr-qc;0;10;;M.R.Gallis;Models for local ohmic quantum dissipation
hep-th/9301026;hep-th,nlin.SI,solv-int;1;24;hep-th/9204036;O.Warnaar,B.Nienhuis;Solvable lattice models labelled by Dynkin diagrams
hep-ph/9301222;hep-ph,hep-lat;0;48;;D.Kominis,R.S.Chivukula;Triviality Bounds in Two-Doublet Models
hep-lat/9301002;hep-lat;2;54;hep-lat/9107002,hep-th/9503230;C.Holm,W.Janke;Critical Exponents of the Classical 3D Heisenberg Model: A Single-Cluster Monte Carlo Study
hep-ph/9301223;hep-ph;0;0;;L.Lellouch,L.Randall,E.Sather;The Rate for $e^+e^-→B B^±π^∓$ and its Implications for the Study of CP Violation, $B_s$ Identification, and the Study of $B$ Meson Chiral Perturbation Theory
hep-ph/9301224;hep-ph,nucl-th;0;7;;D.Seibert,K.Haglin,C.Gale;Measuring velocity ratios with correlation functions
gr-qc/9301006;gr-qc,hep-th;1;18;hep-th/9205022;S.Carlip;Real Tunneling Solutions and the Hartle-Hawking Wave Function
cond-mat/9301009;cond-mat;1;20;hep-th/9109041;A.H.C.Neto,E.Fradkin;The Thermodynamics of Quantum Systems and Generalizations of Zamolodchikov's C-theorem
hep-th/9301027;hep-th;1;16;hep-th/9111001;Y.Tanii,M.Yamashita;Physical States in Two-Dimensional Topological Gauge Theories
gr-qc/9301007;gr-qc;0;15;;Y.Ohkuwa;Decoherence Functional and Probability Interpretation
hep-th/9301028;hep-th,gr-qc,math.QA;2;87;hep-th/9202054,hep-th/9203079;J.Pullin;Knot theory and quantum gravity in loop space: a primer
hep-th/9301029;hep-th;1;14;hep-th/9203056;V.O.Rivelles;Topological Two Dimensional Dilaton Supergravity
hep-ph/9301225;hep-ph;0;23;;A.Soni,R.M.Xu;Probing CP Violation Via Higgs Decays to Four Leptons
hep-ph/9301226;hep-ph;1;8;hep-ph/9208220;A.Abbasabadi,D.Bowser-Chao,D.A.Dicus,W.W.Repko;The effects of a strongly interacting Higgs sector on $γ γ→W_L^+ W_L^-, Z_L^{ 0} Z_L^{ 0}$ scattering
chao-dyn/9301001;chao-dyn,nlin.CD;0;16;;R.Mainieri;Zeta function for the Lyapunov exponent of a product of random matrices
chao-dyn/9301002;chao-dyn,nlin.CD;0;0;;D.H.U.Marchetti;An alternative to Plemelj-Smithies formulas on infinite determinants
hep-ph/9301227;hep-ph;0;18;;H.Reinhardt,K.Langfeld,L.v.Smekal;Instantons in Field Strength Formulated Yang-Mills Theories
nucl-th/9301006;nucl-th;0;27;;C.Wilkin;Near-Threshold Production of $η$-Mesons
hep-th/9301030;hep-th,cond-mat;0;20;;G.Falkovich,A.Hanany;Is 2d Turbulence a Conformal Turbulence?
hep-th/9301031;hep-th,math.QA;2;25;hep-th/9208016,hep-th/9211138;C.Imbimbo;New modular representations and fusion algebras from quantized SL(2,R) Chern-Simons theory
cond-mat/9301010;cond-mat;0;17;;P.Fazekas,H.-Y.Kee;Underscreened Kondo Necklace
hep-ph/9301228;hep-ph;0;0;;J.-M.Frère,L.Houart,J.M.Moreno,J.Orloff,M.Tytgat;Generation of the Baryon Asymmetry of the Universe within the Left--Right Symmetric Model
hep-th/9301032;hep-th;0;10;;K.Zarembo;The Spatial Dynamics in Kazakov--Migdal Model
hep-th/9301033;hep-th,hep-ph;0;25;;I.Antoniadis,T.R.Taylor;String loop corrections to gauge and Yukawa couplings
hep-th/9301034;hep-th;0;22;;E.C.Marino;Quantum Electrodynamics of Particles on a Plane and the Chern-Simons Theory
hep-ph/9301229;hep-ph,nucl-th;0;0;;M.J.Musolf,M.Burkardt;Stranger Still: Kaon Loops and Strange Quark Matrix Elements of the Nucleon
hep-th/9301035;hep-th;4;24;hep-th/9111045,hep-th/9205051,hep-th/9205052,hep-th/9205081;R.R.Khuri;A Comment on the Stability of String Monopoles
cond-mat/9301011;cond-mat;0;0;;Y.Meir,O.Entin-Wohlman;Random Matrix Theory of Transition Strengths and Universal Magnetoconductance in the Strongly Localized Regime
cond-mat/9301012;cond-mat;0;9;;O.Heinonen,W.Kohn;Surface Effects on Bulk Plasmons
cond-mat/9301013;cond-mat;0;13;;J.M.P.Carmelo,A.H.C.Neto;Dynamical decoupling and Kac-Moody current representation in multicomponent integrable systems
hep-th/9301036;hep-th;0;12;;M.Bergeron,D.Eliezer,G.Semenoff;Canonical Chern-Simons Theory and the Braid Group on a Riemann Surface
hep-th/9301037;hep-th,cond-mat;0;0;;C.Chou,V.P.Nair,A.Polychronakos;On the Electromagnetic Interactions of Anyons
gr-qc/9301008;gr-qc,hep-th;12;26;hep-th/9109038,hep-th/9201061,hep-th/9202014,hep-th/9202037,hep-th/9206055,hep-th/9207016,hep-th/9209055,hep-th/9210012,hep-th/9210050,hep-th/9210119,hep-th/9211015,hep-th/9211030;G.T.Horowitz;What is the True Description of Charged Black Holes?
gr-qc/9301009;gr-qc;0;39;;P.Sisterna,H.Vucetich;Cosmology, Oscillating Physics and Oscilllating Biology
hep-th/9301038;hep-th;4;35;hep-th/9203030,hep-th/9207097,hep-th/9209083,hep-th/9211064;M.Staudacher;Combinatorial Solution of the Two-Matrix Model
hep-ph/9301230;hep-ph;0;53;;K.Langfeld,H.Reinhardt;Instanton Condensation in Field Strength Formulated QCD
hep-ph/9301231;hep-ph;3;31;hep-ph/9203201,hep-ph/9203203,hep-ph/9207269;J.T.Peltoniemi,J.W.F.Valle;Massive neutrinos and electroweak baryogenesis
hep-ph/9301232;hep-ph;1;22;hep-ph/9206242;V.Pleitez,M.D.Tonasse;Heavy Charged Leptons in an $SU(3)_L⊗U(1)_N$ Model
astro-ph/9301004;astro-ph;0;0;;T.Piran,A.Shemi,R.Narayan;Hydrodynamics of Relativistic Fireballs
gr-qc/9301010;gr-qc,hep-th;0;0;;M.Gasperini,M.Giovannini;Entropy Production in the Cosmological Amplification of the Vacuum Fluctuations
hep-ph/9301233;hep-ph;0;19;;F.Schlumpf;Nucleon Form Factors in a Relativistic Quark Model
hep-ph/9301234;hep-ph;0;0;;K.Kang,A.R.White;Color--Sextet Quark Condensation in QCD
nucl-th/9301007;nucl-th;0;0;;M.A.Alberg,E.M.Henley,L.Wilets,P.D.Kunz;A Quark Model of Antilambda-Lambda Production in Pbar-P Interactions
hep-th/9301039;hep-th;1;11;hep-th/9212094;B.Feigin,E.Frenkel;Coinvariants of nilpotent subalgebras of the Virasoro algebra and partition identities
hep-th/9301040;hep-th;0;16;;L.Frappat,E.Ragoucy,P.Sorba;Folding the W Algebras
hep-th/9301041;hep-th;0;20;;A.Fayyazuddin;On the origin of multi-component anyon wave functions
hep-th/9301042;hep-th;2;67;hep-th/9110053,hep-th/9111016;E.Witten;Phases of $N=2$ Theories In Two Dimensions
hep-th/9301043;hep-th;0;33;;P.S.Aspinwall,B.R.Greene,D.R.Morrison;Multiple Mirror Manifolds and Topology Change in String Theory
hep-th/9301044;hep-th;0;22;;S.D.Mathur;Kinetic theory in curved space: a first quantised approach
hep-th/9301045;hep-th;0;22;;D.Gepner,J.Fuchs;Braiding in Conformal Field Theory and Solvable Lattice Models
hep-th/9301046;hep-th;7;54;hep-th/9111014,hep-th/9111022,hep-th/9206034,hep-th/9211034,hep-th/9211102,hep-th/9212094,hep-th/9212150;R.Kedem,T.R.Klassen,B.M.McCoy,E.Melzer;Fermionic Sum Representations for Conformal Field Theory Characters
hep-th/9301047;hep-th;6;37;hep-th/9108001,hep-th/9110054,hep-th/9202092,hep-th/9205037,hep-th/9206006,hep-th/9206048;I.Bars,K.Sfetsos;Exact Effective Action and Spacetime Geometry in Gauged WZW Models
hep-th/9301048;hep-th;0;0;;O.Mokhov;Nonlinear Sigma Models and Symplectic Geometry on Loop Spaces of (Pseudo)Riemannian Manifolds
hep-ph/9301235;hep-ph;0;42;;A.Riotto;The Singlet Majoron Model with Hidden Scale Invariance
nucl-th/9301008;nucl-th;0;0;;D.Seibert;Correlation measurements in high-multiplicity events
cond-mat/9301014;cond-mat;0;12;;P.Ossadnik,J.Lee;Power law tail in the radial growth probability distribution for DLA
cond-mat/9301015;cond-mat,hep-th;0;34;;D.Li;Hierarchical wave function, Fock cyclic condition and spin-statistics relation in the spin-singlet fractional quantum Hall effect
hep-th/9301049;hep-th;0;45;;M.Gunaydin;N=4 Superconformal Algebras and Gauged WZW Models
hep-th/9301050;hep-th;0;16;;M.Gunaydin;Generalized Conformal and Superconformal Group Actions and Jordan Algebras
astro-ph/9301005;astro-ph,hep-ph;0;0;;R.Mayle,D.N.Schramm,M.S.Turner,J.Wilson;Constraints on Dirac Neutrinos from SN 1987A
hep-ph/9301236;hep-ph;0;24;;J.-P.BLAIZOT,E.IANCU;Kinetic Equations for Longwavelength Excitations of the Quark-Gluon Plasma
hep-th/9301051;hep-th,math-ph,math.MP,nlin.SI,solv-int;0;0;;J.Harnad,C.A.Tracy,H.Widom;Hamiltonian Structure of Equations Appearing in Random Matrices
hep-lat/9301003;hep-lat,hep-th;0;16;;R.Ben-Av,G.Bhanot;Measuring the Decorrelation Times of Fourier Modes in Simulations
gr-qc/9301011;gr-qc,hep-th,quant-ph;0;0;;J.B.Hartle;The Reduction of the State Vector and Limitations on Measurement in the Quantum Mechanics of Closed Systems
hep-th/9301052;hep-th,gr-qc;0;0;;R.Gregory,R.Laflamme;Black Strings and p-Branes are Unstable
hep-lat/9301004;hep-lat;0;22;;V.Singh,D.A.Browne,R.W.Haymaker;Structure of Abrikosov Vortices in SU(2) Lattice Gauge Theory
hep-ph/9301237;hep-ph;1;17;hep-ph/9205245;A.Czarnecki,S.Davidson;QCD corrections to the charged Higgs decay of a heavy quark
gr-qc/9301012;gr-qc,hep-th;0;15;;M.Porrati;Massive Spin-5/2 Fields Coupled to Gravity: Tree-Level Unitarity vs. the Equivalence Principle
hep-th/9301053;hep-th;2;21;hep-th/9112009,hep-th/9205117;F.Yu;Many Boson Realizations of Universal Nonlinear $W_∞$-Algebras
hep-ph/9301238;hep-ph;0;14;;F.K.Diakonos,O.Korakianitis,C.G.Papadopoulos,C.Philippides,W.J.Stirling;W + gamma + jet production as a test of the electromagnetic couplings of W at LHC and SSC
cond-mat/9301016;cond-mat;0;13;;J.Miekisz;The Global Minimum of Energy Is Not Always a Sum of Local Minima - a Note on Frustration
cond-mat/9301017;cond-mat.stat-mech;0;32;;J.Miekisz;Stable quasicrystalline ground states
hep-ph/9301239;hep-ph,astro-ph;1;45;hep-ph/9203213;E.Kh.Akhmedov,A.Lanza,S.T.Petcov;Implications of Gallium Solar Neutrino Data for the Resonant Spin-Flavor Precession Scenario
hep-th/9301054;hep-th;0;28;;M.Sakamoto;Topological Aspects of an Antisymmetric Background Field on Orbifolds
cond-mat/9301018;cond-mat;1;24;hep-th/9202057;E.Westerberg,T.H.Hansson;Quantum Mechanics on Thin Cylinders
hep-th/9301055;hep-th;0;0;;M.Tonin;Twistor-Like Formulation of Heterotic Strings
hep-th/9301056;hep-th;1;21;hep-th/9110074;H.Hinrichsen,V.Rittenberg;Quantum Groups, Correlation Functions and Infrared Divergences
gr-qc/9301013;gr-qc,astro-ph,hep-th;0;0;;M.Campanelli,C.O.Lousto;"Are Black Holes in Brans-Dicke Theory precisely the same as in General Relativity?"
nucl-th/9301009;nucl-th;0;10;;D.Seibert;Chemical equilibration of $π$, $ρ$ and $ω$ mesons in ultra--relativistic nuclear collisions
gr-qc/9301014;gr-qc,hep-th;0;24;;J.D.E.Grant;On Self-Dual Gravity I
astro-ph/9301006;astro-ph;0;0;;R.Capuzzo-Dolcetta;The Evolution of the Globular Cluster System in a Triaxial Galaxy: Can a Galactic Nucleus Form by Globular Cluster Capture?
astro-ph/9301007;astro-ph;0;0;;P.Mészáros,P.Laguna,M.J.Rees;Gasdynamics of Relativistically Expanding Gamma-Ray Burst Sources: Kinematics, Energetics, Magnetic Fields and Efficiency
gr-qc/9301015;gr-qc,hep-th;0;0;;R.Penrose,R.D.Sorkin,E.Woolgar;A Positive Mass Theorem Based on the Focusing and Retardation of Null Geodesics
hep-th/9301057;hep-th;0;18;;J.Gonzalez,M.A.Martin-Delgado;Exact Finite Size Results on the Ising Model in 2D Curved Space
hep-lat/9301005;hep-lat,nucl-th;1;9;hep-lat/9205007;C.J.Morningstar;The Heavy Quark Self-Energy in Nonrelativistic Lattice QCD
hep-th/9301058;hep-th,gr-qc;0;0;;J.D.Bekenstein;How Fast Does Information Leak out from a Black Hole?
hep-ph/9301240;hep-ph;0;25;;B.Rai,G.Senjanovic;Gravity and Domain Wall Problem
hep-lat/9301006;hep-lat;1;23;hep-lat/9205010;A.M.Green,C.Michael,J.E.Paton,M.E.Sainio;Multi-Quark Energies in SU(2) Lattice Gauge Theory
hep-lat/9301007;hep-lat;0;31;;J.F.Wheater,P.W.Stephenson;On the Crumpling Transition in Crystalline Random Surfaces
nucl-th/9301010;nucl-th;0;0;;D.Seibert;Analysis techniques for high-multiplicity collisions
hep-ph/9301241;hep-ph;1;25;hep-ph/9206241;P.Colangelo,F.D.Fazio,G.Nardulli;Study of the Reactions $B →D^* ππ$ and $B →D^* ρπ$
hep-ph/9301242;hep-ph,nucl-th;0;54;;H.K.Lee,M.A.Nowak,M.Rho,I.Zahed;Nonabelian Berry Phases in Baryons
gr-qc/9301016;gr-qc,hep-th;11;96;hep-th/9201061,hep-th/9201074,hep-th/9202037,hep-th/9202054,hep-th/9202076,hep-th/9203052,hep-th/9203054,hep-th/9203079,hep-th/9209055,hep-th/9209058,hep-th/9210119;L.Smolin;Time, measurement and information loss in quantum cosmology
astro-ph/9301008;astro-ph;0;0;;P.L.Biermann;Cosmic Rays I.: The cosmic ray spectrum between 10 TeV and 3 EeV
cond-mat/9301019;cond-mat;0;22;;A.H.MacDonald,S.-R.E.Yang,M.D.Johnson;Quantum Dots in Strong Magnetic Fields: Stability Criteria for the Maximum Density Droplet
cond-mat/9301020;cond-mat;0;17;;G.Date,M.V.N.Murthy;Classical Dynamics of Anyons and the Quantum Spectrum
cond-mat/9301021;cond-mat;0;23;;G.Date,M.Krishna,M.V.N.Murthy;Asymptotic analysis and spectrum of three anyons
hep-th/9301059;hep-th;1;23;hep-th/9206033;A.J.Niemi,O.Tirkkonen;On Exact Evaluation of Path Integrals
hep-th/9301060;hep-th,hep-ph;0;12;;A.Lahiri;Generating Vector Boson Masses
hep-th/9301061;hep-th;0;0;;L.Crane;Categorical Physics
hep-ph/9301243;hep-ph;0;21;;P.Langacker;Implications of Solar and Atmospheric Neutrinos
hep-th/9301062;hep-th,math.QA;0;7;;L.Crane,D.N.Yetter;A categorical construction of 4D TQFTs
hep-th/9301063;hep-th,math.QA;0;21;;J.C.Baez;Link Invariants, Holonomy Algebras and Functional Integration
hep-th/9301064;hep-th;0;18;;L.Brekke,S.J.Hughes,T.D.Imbo;Rings and Balls
hep-th/9301065;hep-th;0;31;;I.Ya.Aref'eva;A Simple Model Inducing QCD
funct-an/9301001;funct-an,math.OA;1;35;hep-th/9209077;A.Turbiner;Lie-algebras and linear operators with invariant subspaces
hep-ph/9301244;hep-ph;0;55;;J.Stern,H.Sazdjian,N.H.Fuchs;What $π-π$ Scattering Tells Us About Chiral Perturbation Theory
hep-th/9301066;hep-th;0;9;;G.Sotkov,M.Stanishkov;Off-critical $W_∞$ and Virasoro Algebras As Dynamical Symmetries Of the Integrable Models
hep-ph/9301245;hep-ph;0;12;;E.Ma,D.Ng;Symmetry Remnants: Rationale for Having Two Higgs Doublets
nucl-th/9301011;nucl-th;0;20;;S.Frankel,W.Frati,N.R.Walet;Extracting Nuclear Transparency from p-A Cross sections
hep-th/9301067;hep-th,gr-qc;3;17;hep-th/9201059,hep-th/9202037,hep-th/9210012;M.Maggiore;A Generalized Uncertainty Principle in Quantum Gravity
hep-th/9301068;hep-th,hep-ph;0;12;;D.J.Gross,W.Taylor;Two Dimensional QCD is a String Theory
hep-th/9301069;hep-th;0;34;;W.Chen,Y.Makeenko,G.W.Semenoff;Four-Fermion Theory and the Conformal Bootstrap
hep-th/9301070;hep-th;1;15;hep-th/9112042;K.Takasaki,T.Takebe;Quasi-classical limit of Toda hierarchy and W-infinity symmetries
hep-lat/9301008;hep-lat;1;13;hep-lat/9207032;P.Rossi,E.Vicari;Finite size scaling in CP(N-1) models
hep-th/9301071;hep-th;0;0;;J.L.Cortés,J.Gamboa,L.Velázquez;Second Order Formalism for Fermions
hep-th/9301072;hep-th;0;0;;J.L.Cortés,J.Gamboa,L.Velázquez;Second Order Formalism for fermions: Anomalies and Species doubling on the Laticce
hep-th/9301073;hep-th;0;0;;F.Ardalan;2D Black Holes and 2D Gravity
hep-th/9301074;hep-th;3;49;hep-th/9110027,hep-th/9110028,hep-th/9211113;C.M.Hull;Geometry and W-Gravity
hep-ph/9301246;hep-ph;0;0;;H.J.Lipkin;Quark Models and Quark Phenomenology
hep-ph/9301247;hep-ph;0;17;;E.Kh.Akhmedov,S.T.Petcov,A.Yu.Smirnov;Pontecorvo's Original Oscillations Revisited
cond-mat/9301022;cond-mat,hep-lat;0;0;;I.Vattulainen,K.Kankaala,J.Saarinen,T.Ala-Nissila;Hidden Errors in Simulations and the Quality of Pseudorandom Numbers
gr-qc/9301017;gr-qc,astro-ph;0;0;;S.W.Hawking,R.Laflamme,G.W.Lyons;The Origin of Time Asymmetry
hep-th/9301075;hep-th,math.QA;0;0;;L.Begin,A.N.Kirillov,P.Mathieu,M.A.Walton;Berenstein-Zelevinsky triangles, elementary couplings and fusion rules
hep-th/9301076;hep-th,math-ph,math.MP;0;0;;J.Harnad;Dual Isomonodromic Deformations and Moment Maps to Loop Algebras
gr-qc/9301018;gr-qc,hep-th;0;0;;J.D.Brown,J.W.York;Jacobi's Action and the Density of States
astro-ph/9301009;astro-ph;0;0;;J.E.Howe,D.T.Jaffe,E.N.Grossman,W.F.Wall,J.G.Mangum,G.J.Stacey;Extended Co(7-6) Emission from Warm Gas in Orion
hep-ph/9301248;hep-ph;0;13;;G.Jungman;Fermion Masses in SO(10)
hep-th/9301077;hep-th;1;25;hep-th/9108003;C.M.Yung,R.C.Warner;The $N=2$ super $W_4$ algebra and its associated generalized KdV hierarchies
hep-th/9301078;hep-th;0;0;;A.D.de Veigy,S.Ouvry;Topological 2-Dimensional Quantum Mechanics
hep-th/9301079;hep-th;2;29;hep-th/9109053,hep-th/9205068;D.Bailin,A.Love,W.A.Sabra;Twisted Sector Yukawa Couplings For The ${\bf Z}_M×{\bf Z}_N$ Orbifolds
hep-th/9301080;hep-th;0;0;;P.Dargis,P.Mathieu;Nonlocal conservation laws in N=1,2 Supersymetric KdV equation
hep-ph/9301249;hep-ph;0;14;;S.Chakravarty,S.M.Kim,P.Ko;Is Upsilon(3S) a pure S-wave?
chao-dyn/9301003;chao-dyn,nlin.CD;0;36;;K.T.Hansen;Symbolic dynamics I. Finite dispersive billiards
chao-dyn/9301004;chao-dyn,nlin.CD;0;17;;K.T.Hansen;Symbolic dynamics II. The stadium billiard
chao-dyn/9301005;chao-dyn,nlin.CD;0;20;;K.T.Hansen;Symbolic dynamics III. Bifurcations in billiards and smooth potentials
hep-ph/9301250;hep-ph,hep-lat,hep-th;0;0;;E.D'Hoker,P.Sikivie;Casimir forces between beads on strings
hep-th/9301081;hep-th;0;25;;I.Ya.Aref'eva;Large-N Quenching in the Kazakov-Migdal Model
hep-th/9301082;hep-th;1;5;hep-th/9206056;J.Liu;Evolution of Pure States into Mixed States
hep-th/9301083;hep-th;9;77;hep-th/9108004,hep-th/9109032,hep-th/9111001,hep-th/9111035,hep-th/9201005,hep-th/9201056,hep-th/9202008,hep-th/9203066,hep-th/9206085;S.Mukhi,C.Vafa,E.Frenkel;Two dimensional black-hole as a topological coset model of c=1 string theory
hep-lat/9301009;hep-lat,hep-th;1;11;hep-lat/9212024;Y.Shen;Does the 2d Higgs-Yukawa Model Have a Symmetric Phase at Small Yukawa Coupling Region?
nucl-th/9301012;nucl-th;0;23;;M.F.Jiang,R.Machleidt,T.T.S.Kuo;Relativistic Ring-Diagram Nuclear Matter Calculations
alg-geom/9301004;alg-geom,math.AG;0;19;;A.Aure,W.Decker,K.Hulek,S.Popescu,K.Ranestad;The Geometry of Bielliptic Surfaces in P^4
cond-mat/9301023;cond-mat;0;13;;A.E.Rana,S.M.Girvin;Soluble `Supersymmetric' Quantum XY Model
hep-ph/9301251;hep-ph;0;22;;A.R.White,I.G.Knowles,K.Kang;The $η_6$ at LEP and TRISTAN
cond-mat/9301024;cond-mat,hep-th;0;0;;J.McCabe;Anyons as Dirac Strings the $A_x=0$ Gauge
hep-ph/9301252;hep-ph;1;25;hep-ph/9204202;D.Bowser-Chao,K.Cheung;Detection of the heavy Higgs boson at $γγ$ colliders
nucl-th/9301013;nucl-th;0;21;;D.C.Zheng,J.P.Vary,B.R.Barrett;Exact Solutions of Model Hamiltonian Problems with Effective Interactions
hep-lat/9301010;hep-lat;0;29;;K.Cahill;Noncompact Lattice Simulations of SU(2) Gauge Theory
nucl-th/9301014;nucl-th;0;15;;A.Ono,H.Horiuchi,T.Maruyama,A.Ohnishi;Momentum distribution of fragments in heavy ion reactions: Dependence on the stochastic collision process
hep-lat/9301011;hep-lat,cond-mat;0;0;;M.Grabenstein,B.Mikeska;Multigrid Monte Carlo with higher cycles in the Sine Gordon model
cond-mat/9301025;cond-mat;0;13;;A.Sanchez,F.Dominguez-Adame;Enhanced suppresion of localization in a continuous Random-Dimer Model
hep-ph/9301253;hep-ph,nucl-th;0;41;;F.E.Close,N.Isgur,S.Kumano;Scalar Mesons in $φ$ Radiative Decay: their implications for spectroscopy and for studies of CP-violation at $φ$ factories
hep-lat/9301012;hep-lat;0;0;;B.Alles,M.Campostrini,A.Feo,H.Panagopoulos;Lattice Perturbation Theory by Computer Algebra: A Three-Loop Result for the Topological Susceptibility
hep-ph/9301254;hep-ph;0;35;;P.Chiappetta,M.Greco,J.Ph.Guillet,S.Rolli,M.Werlen;Next to leading order determination of pion fragmentation functions
cond-mat/9301026;cond-mat;0;0;;N.S.Wingreen,A.-P.Jauho,Y.Meir;Time-Dependent Transport through a Mesoscopic Structure
hep-th/9301084;hep-th,cond-mat;2;16;hep-th/9202057,hep-th/9206049;D.Bernard,M.Gaudin,F.D.M.Haldane,V.Pasquier;Yang-Baxter equation in spin chains with long range interactions
hep-lat/9301013;hep-lat;0;0;;D.J.E.Callaway;Landau, Abrikosov, Hofstadter: Magnetic Flux Penetration in a Lattice Superconductor
hep-ph/9301255;hep-ph;0;11;;B.H.Smith;Calculation of processes involving many particles at the kinematical threshold
astro-ph/9301010;astro-ph;0;0;;J.P.Rachen,P.L.Biermann;Extragalactic ultra high energy cosmic rays, I. Contribution from hot spots in FR-II galaxies
cond-mat/9301027;cond-mat;1;31;cond-mat/9204001;A.V.Chubukov,S.Sachdev;Universal Magnetic Properties of $La_{2-δ} Sr_δ Cu O_4$ at Intermediate Temperatures
hep-th/9301085;hep-th;0;0;;S.Panda,S.Roy;On the Symmetry Algebra of the Discrete States in $d<2$ Closed String Theory
hep-lat/9301014;hep-lat,cond-mat,hep-th;0;48;;M.C.D.E.L.G.W.S.P.Sodano;SU(N) Quantum Antiferromagnets and the Phase Structure of QED in the Strong Coupling Limit
hep-ph/9301256;hep-ph,hep-th;1;35;hep-th/9207039;M.C.D.G.W.S.P.Sodano;Chiral Dynamics and Fermion Mass Generation in Three Dimensional Gauge Theory
hep-ph/9301257;hep-ph;0;17;;V.M.Belyaev;Delta-Isobar Magnetic Form Factor in QCD
astro-ph/9301011;astro-ph;0;0;;A.H.Jaffe,A.Stebbins,J.A.Frieman;Minimal Microwave Anisotropy from Perturbations Induced at Late Times
nucl-th/9301015;nucl-th;0;19;;N.Auerbach,D.C.Zheng,L.Zamick,B.A.Brown;Correlation between the quenching of total GT+ strength and the increase of E2 strength
hep-th/9301086;hep-th;0;0;;J.Kellendonk,M.Rösgen,R.Varnhagen;Path Spaces and W-Fusion in Minimal Models
hep-ph/9301258;hep-ph;0;32;;S.G.Naculich;Third Generation Effects on Fermion Mass Predictions in Supersymmetric Grand Unified Theories
hep-th/9301087;hep-th;0;33;;A.H.Bougourzi;Uniqueness of the bosonization of the $U_q(su(2)_k)$ quantum current algebra
hep-th/9301088;hep-th;6;80;hep-th/9108013,hep-th/9110055,hep-th/9111014,hep-th/9111016,hep-th/9202011,hep-th/9203066;N.P.Warner;$N=2$ Supersymmetric Integrable Models and Topological Field Theories
hep-lat/9301015;hep-lat;9;86;hep-lat/9205012,hep-lat/9206005,hep-lat/9207004,hep-lat/9207005,hep-lat/9207021,hep-lat/9209002,hep-lat/9210022,hep-lat/9210026,hep-lat/9211021;D.N.Petcher;Chiral Gauge Theories and Fermion-Higgs Systems
hep-th/9301089;hep-th;0;33;;D.Gepner;String Theory on Calabi--Yau Manifolds: The Three Generations Case
hep-th/9301090;hep-th;1;16;hep-th/9112042;K.Takasaki;Quasi-classical limit of BKP hierarchy and W-infinity symmeties
hep-th/9301091;hep-th,math.QA;0;0;;B.Broda;Chern-Simons approach to three-manifold invariants
hep-ph/9301259;hep-ph;1;27;hep-ph/9301265;D.Chang,W.-Y.Keung,I.Phillips;CP Violation in top pair production at an e^+e^- collider
nucl-th/9301016;nucl-th;0;59;;W.Melnitchouk,A.W.Thomas;Shadowing in Deuterium
hep-ph/9301260;hep-ph;0;12;;S.F.Novaes,D.Spehler;Gravitational Laser Back-Scattering
hep-th/9301092;hep-th,math.QA;0;39;;B.Jurco;More on quantum groups from the the quantization point of view
hep-ph/9301261;hep-ph,hep-th;0;21;;A.E.Faraggi,E.Halyo;Cabibbo Mixing in Superstring Derived Standard--like Models
hep-ph/9301262;hep-ph,nucl-th;0;0;;S.Kumano;Nuclear Gluon Distributions in a Parton Model
hep-ph/9301263;hep-ph;0;76;;V.A.Naumov,S.I.Sinegovsky,E.V.Bugaev;High-Energy Cosmic-Ray Muons Under Thick Layers of Matter I. a Method to Solve the Transport Equation
hep-th/9301093;hep-th;0;0;;M.Yu.Lashkevich;Superconformal 2D Minimal Models and an Unusual Coset Construction
hep-th/9301094;hep-th;0;0;;M.Yu.Lashkevich;Conformal Blocks of Coset Construction: Zero Ghost Number
cond-mat/9301028;cond-mat;0;34;;M.L.Plumer,A.Mailhot,R.Ducharme,A.Caillé,H.T.Diep;Histogram Monte Carlo study of next-nearest-neighbor Ising antiferromagnet on a stacked triangular lattice
cond-mat/9301029;cond-mat;0;6;;A.Mailhot,M.L.Plumer;Comment on "Critical properties of highly frustrated pyrochlore antiferromagnets"
hep-th/9301095;hep-th;0;19;;D.Boyanovsky;Quantum Spinodal Decomposition
hep-ph/9301264;hep-ph;0;14;;P.B.Pal;Rare K-Decays as Crucial Tests for Unified Models with Gauged Baryon Number:
funct-an/9301002;funct-an,math.OA;0;0;;L.B.Schweitzer;Summary of Spectral Invariance Results
cond-mat/9301030;cond-mat;0;31;;A.Angelucci,S.Sorella;Phase separation in the large-spin {\it t}-{\it J} model
hep-th/9301096;hep-th,math.QA;0;0;;C.-P.Sun,M.-L.Ge;Quantum double of Heisenberg-Weyl algebra, its universal R-matrix and their representations
hep-th/9301097;hep-th;10;26;hep-th/9201056,hep-th/9205088,hep-th/9206084,hep-th/9208027,hep-th/9210065,hep-th/9210115,hep-th/9211072,hep-th/9211096,hep-th/9212043,hep-th/9212072;H.Hata,B.Zwiebach;Developing the Covariant Batalin-Vilkovisky approach to String Theory
hep-th/9301098;hep-th;0;0;;Ch.Devchand,A.N.Leznov;Bäcklund transformation for supersymmetric self-dual theories for semisimple gauge groups and a hierarchy of $A_1$ solutions
alg-geom/9301005;alg-geom,math.AG;0;0;;M.A.Guest;The topology of the space of rational curves on a toric variety
hep-lat/9301016;hep-lat;0;0;;R.Gupta,A.Patel,S.Sharpe;$I=2$ pion scattering amplitude with Wilson fermions
hep-th/9301099;hep-th;0;0;;H.Lu,C.N.Pope,S.Schrans,X.J.Wang;On the Spectrum and Scattering of W_3 Strings
gr-qc/9301019;gr-qc;0;0;;Y.Fujiwara,H.Ishihara,H.Kodama;Comments on Closed Bianchi Models
hep-th/9301100;hep-th,cond-mat;0;0;;A.Lerda,S.Sciuto;Anyons and Quantum Groups
hep-ph/9301265;hep-ph;0;20;;D.Chang,W.-Y.Keung;CP Violation in the Decay of Neutral Higgs Boson into $t-{\bar t}$ or $W^+-W^-$
hep-ph/9301266;hep-ph;0;14;;E.R.Poppitz;Fermion Density Induced Instability of the W-Boson Pair Condensate in Strong Magnetic Field
hep-th/9301101;hep-th;0;0;;D.Giulini;On the possibility of spinorial quantization in the Skyrme model
gr-qc/9301020;gr-qc;0;0;;D.Giulini;On the configuration space topology in general relativity
hep-ph/9301267;hep-ph;1;45;hep-ph/9207219;R.G.Roberts,L.Roszkowski;Implications for Minimal Supersymmetry from Grand Unification and the Neutralino Relic Abundance
cond-mat/9301031;cond-mat;0;0;;V.E.Korepin,A.G.Izergin,N.M.Bogoliubov;Quantum Inverse Scattering Method and Correlation Functions
hep-ph/9301268;hep-ph,hep-th;3;20;hep-th/9109053,hep-th/9205068,hep-th/9208024;A.E.Faraggi;Gauge Coupling Unification in Superstring Derived Standard--like Models
hep-lat/9301017;hep-lat,hep-th;0;0;;G.Bhanot,M.Creutz,U.Glassner,I.Horvath,J.Lacki,K.Schilling,J.Weckel;Low Temperature Expansions for Potts Models
hep-ph/9301269;hep-ph;0;8;;V.M.Belyaev;Soft Modes Contribution into Path Integral
hep-th/9301102;hep-th;0;20;;K.Lee;The Dual Formulation of Cosmic Strings and Vortices
hep-th/9301103;hep-th;3;30;hep-th/9202021,hep-th/9205005,hep-th/9206097;J.Alfaro,P.H.Damgaard;Origin of Antifields in the Batalin-Vilkovisky Lagrangian Formalism
hep-th/9301104;hep-th;0;0;;J.Harnad,M.-A.Wisse;Moment Maps to Loop Algebras, Classical R-Matrix and Integrable Systems
hep-th/9301105;hep-th;0;18;;S.Chaudhuri,D.Minic;On the Black Hole Background of Two-Dimensional String Theory
hep-th/9301106;hep-th;12;52;hep-th/9111056,hep-th/9201061,hep-th/9201074,hep-th/9203042,hep-th/9203052,hep-th/9203054,hep-th/9204026,hep-th/9204072,hep-th/9205049,hep-th/9206043,hep-th/9206070,gr-qc/9208002;E.Elizalde,S.Naftulin,S.D.Odintsov;Convenient Versus Unique Effective Action Formalism in 2D Dilaton-Maxwell Quantum Gravity
hep-ph/9301270;hep-ph;0;0;;H.J.Lipkin;Application of Mössbauer-Type Sum Rules for $B$ Meson Decays
hep-ph/9301271;hep-ph;0;36;;M.Reuter,N.Tetradis,C.Wetterich;The Large N Limit and the High Temperature Phase Transition for the φ^4 Theory
hep-ph/9301272;hep-ph;0;16;;G.Cvetic,M.Nowakowski,A.Pilaftsis;CP-Violation with Bosons
hep-ph/9301273;hep-ph;0;55;;A.Pilaftsis,M.Nowakowski;CP-odd Neutral Higgs Effects in Top -- anti-Top Production
hep-th/9301107;hep-th;0;42;;N.Engberg,B.E.W.Nilsson,P.Sundell;An Algorithm for Computing Four-Ramond Vertices at Arbitrary Level
hep-ph/9301274;hep-ph;0;32;;C.Coriano',A.Radyushkin,G.Sterman;QCD Sum Rules and Compton Scattering
hep-ph/9301275;hep-ph;0;15;;C.Best,P.Gornicki,W.Greiner;The phase-space structure of the Klein-Gordon field
hep-ph/9301276;hep-ph;0;45;;A.Dobado,J.R.Pelaez;A global fit of $ππ$ and $πK$ elastic scattering in ChPT with dispersion relations
hep-th/9301108;hep-th;1;25;hep-th/9203075;E.Abdalla,M.C.B.Abdalla,O.H.G.Branco,L.E.Saltini;Current Algebra of Super WZNW Models
hep-ph/9301277;hep-ph;0;0;;X.Zhang;Operator Analysis for the Higgs Potential and Cosmological Bound on the Higgs-Boson Mass
hep-th/9301109;hep-th;0;0;;E.Abdalla,A.C.V.V.de Siqueira;String inspired effective Lagrangian and Inflationary Universe
hep-lat/9301018;hep-lat;0;0;;K.M.Bitar,T.DeGrand,R.Edwards,S.Gottlieb,U.M.Heller,A.D.Kennedy,J.B.Kogut,A.Krasnitz,W.Liu,M.C.Ogilvie,R.L.Renken,P.Rossi,D.K.Sinclair,R.L.Sugar,D.Toussaint,K.C.Wang;Simple Hadronic Matrix Elements with Wilson Valence Quarks and Dynamical Staggered Fermions at ${\bf 6/g^2=5.6}$
hep-ph/9301278;hep-ph;0;21;;P.J.O'Donnell,H.K.K.Tung;The Rare Decay $B→K^∗γ$: A More Precise Calculation
hep-th/9301110;hep-th;0;0;;J.Anandan,C.R.Hagen;Neutron Acceleration in Uniform Electromagnetic Fields
hep-ph/9301279;hep-ph;0;0;;A.Das,V.Mathur;Nonleptonic Decays of Charmed Mesons into two Pseudoscalar Mesons
hep-th/9301111;hep-th,math.SG;0;14;;L.Takhtajan;On Foundation of the Generalized Nambu Mechanics
gr-qc/9301021;gr-qc,hep-th;0;0;;M.Lu,M.B.Wise;Black Holes with a Generalized Gravitational Action
cond-mat/9301032;cond-mat;0;15;;M.Leibig;A Model for the Propagation of Sound in Granular Materials
cond-mat/9301033;cond-mat;0;15;;C.Pich,F.Schwabl;Order of Two-Dimensional Isotropic Dipolar Antiferromagnets
hep-ph/9301280;hep-ph;0;0;;A.D.Randall;Breaking Of Conformal Invariance And Electromagnetic Field Generation In The Universe
cond-mat/9301034;cond-mat;0;0;;M.E.Flatte;Lower Bound on the Energy Gap at Precise Locations on the Bi_2Sr_2CaCu_2O_8 Fermi Surface
nucl-th/9301017;nucl-th;0;60;;W.Melnitchouk,A.W.Thomas;Role of Vector Mesons in High-Q^2 Lepton-Nucleon Scattering
hep-th/9301112;hep-th;0;0;;C.V.Johnson;On Integrable c<1 Open--Closed String Theory
hep-th/9301113;hep-th;1;26;hep-th/9202026;J.A.Gracey;Gauge Independent Critical Exponents for QED Coupled to a Four Fermi Interaction with and without a Chern Simons Term
hep-ph/9301281;hep-ph;0;81;;F.Feruglio;The Chiral Approach to the Electroweak Interactions
hep-ph/9301282;hep-ph;0;0;;Harry.J.Lipkin;Interference Effects in B-Decays to Flavor-Mixed Neutral Mesons - Clues to Small Amplitudes and CP-Violation
hep-ph/9301283;hep-ph;0;0;;R.Decker,M.Nowakowski,A.Pilaftsis;Dominant Three-Body Decays of a Heavy Higgs and Top Quark
hep-ph/9301284;hep-ph;0;13;;C.Best,J.M.Eisenberg;Pair creation in transport equations using the equal-time Wigner function
hep-lat/9301019;hep-lat;1;32;hep-ph/9203203;J.Kripfganz,C.Michael;Lattice study of sphaleron transitions in a 2D O(3) sigma model
nucl-th/9301018;nucl-th;0;32;;H.Krauss,K.Gr"un,T.Rauscher,H.Oberhummer;The Astrophysical S-Factor of the Reaction $^7$be(p,$γ$)$^8$B in the Direct Capture Model
cond-mat/9301035;cond-mat;0;28;;Z.-Y.LU,Zhao-Bin,SU,L.YU;The Haldane Energy Gap of A Doped Linear-Chain Heisenberg Antiferromagnet
hep-ph/9301285;hep-ph;5;41;hep-ph/9203201,hep-ph/9203203,hep-ph/9204228,hep-ph/9206227,hep-ph/9206266;J.R.Espinosa,M.Quirós;The electroweak phase transition with a singlet
hep-th/9301114;hep-th;0;16;;M.Bonini,M.D'Attanasio,G.Marchesini;Perturbative renormalization and infrared finiteness in the Wilson renormalization group: the massless scalar case
hep-th/9301115;hep-th,cond-mat;0;0;;A.Cappelli,G.V.Dunne,C.A.Trugenberger,G.R.Zemba;Symmetry Aspects and Finite-Size Scaling of Quantum Hall Fluids
hep-ph/9301286;hep-ph;0;0;;R.N.Mohapatra,X.Zhang;Restrictions on B-L Symmetry Breaking Implied by a Fourth Generation Neutrino
hep-ph/9301287;hep-ph;1;25;hep-th/9201063;M.Joyce,N.Turok;Family Symmetry, Fermion Mass Matrices and Cosmic Texture
gr-qc/9301022;gr-qc;0;0;;M.C.V.de Alfaro,F.de Felice;An Anisotropic Wormhole:TUNNELLING in Time and Space
hep-ph/9301288;hep-ph;0;17;;K.Cheung;$WZ$, $Wγ$, $WW$ and $ZZ$ pair productions at TeV $eγ$ colliders
hep-th/9301116;hep-th,hep-ph;0;25;;H.Nakazato,S.Pascazio;Macroscopic limit of a solvable dynamical model
alg-geom/9301006;alg-geom,hep-th,math.AG;0;12;;S.Katz;Rational curves on Calabi-Yau manifolds: verifying predictions of Mirror Symmetry
cond-mat/9301036;cond-mat;0;75;;C.A.Stafford,A.J.Millis;Scaling theory of the Mott-Hubbard metal-insulator transition in one dimension
cond-mat/9301037;cond-mat,hep-th;0;55;;W.Chen,M.P.A.Fisher,Y.-S.Wu;Mott Transition in An Anyon Gas
hep-lat/9301020;hep-lat;6;40;hep-lat/9107002,hep-lat/9202001,hep-lat/9202004,astro-ph/9205006,cond-mat/9207003,hep-lat/9207026;B.Grossmann,M.L.Laursen;The Confined-Deconfined Interface Tension in Quenched QCD using the Histogram Method
hep-th/9301117;hep-th;0;20;;J.A.Gracey;Analysis of Abelian Gauge Theory with Four Fermi Interaction at $O(1/N^2)$ in Arbitrary Dimensions
hep-ph/9301289;hep-ph;1;36;hep-ph/9901206;J.G.Koerner,A.Pilaftsis,K.Schilcher;Leptonic CP Asymmetries in Flavor-changing H0 Decays
hep-ph/9301290;hep-ph;1;27;hep-ph/9901206;J.G.Koerner,A.Pilaftsis,K.Schilcher;Leptonic Flavor-changing Z0 Decays in SU(2)xU(1) Theories with Right- handed Neutrinos
hep-ph/9301291;hep-ph;0;0;;G.K.Leontaris,J.D.Vergados;Neutrino Masses in Flipped SU(5)
hep-th/9301118;hep-th;3;5;hep-th/9111020,hep-th/9204020,hep-th/9211138;O.Aharony;Generalized Fusion Potentials
cond-mat/9301038;cond-mat;0;30;;W.Li,G.Vidali,O.Biham;Scaling of Island Growth in Pb Overlayers on Cu(001)
math/9301201;math.FA;0;0;;P.G.Dodds,T.K.Dodds,P.N.Dowling,C.J.Lennard,F.A.Sukochev;A Uniform Kadec-klee Property For Symmetric Operator Spaces
math/9301202;math.CO;0;0;;D.Zeilberger;Theorems for a Price: Tomorrow's Semi-Rigorous Mathematical Culture
math/9301203;math.LO,math.RA;0;0;;A.H.Mekler,E.Nelson,S.Shelah;A variety with solvable, but not uniformly solvable, word problem
math/9301204;math.LO;0;16;;A.H.Mekler,S.Shelah;Some compact logics --- results in ZFC
math/9301205;math.LO;0;0;;S.Shelah,H.Tuuri,J.Väänänen;On the number of automorphism of uncontable models
math/9301206;math.LO;0;4;;T.Bartoszyński,M.Goldstern,H.Judah,S.Shelah;All meager filters may be null
math/9301207;math.LO,math.RA;0;13;;P.C.Eklof,S.Shelah;Explicitly nonstandard uniserial modules
math/9301208;math.LO;0;6;;J.T.Baldwin,M.C.Laskowski,S.Shelah;Forcing isomorphism
math/9301209;math.LO;0;7;;A.Louveau,B.Veličković,S.Shelah;Borel partitions of infinite subtrees of a perfect tree
math/9301210;math.LO;0;5;;M.C.Laskowski,S.Shelah;On the existence of atomic models
math/9301211;math.KT,math.AT;0;0;;A.Adem;Representations and $K$-theory of Discrete Groups
math/9301212;math.GT;0;0;;S.Bryson,M.H.Freedman,Z.-X.He,Z.Wang;Möbius invariance of knot energy
math/9301213;math.AP,math.DG,math.KT;0;0;;G.Gong;Relative $K$-cycles and elliptic boundary conditions
math/9301214;math.RT;0;0;;R.E.Howe;Homogeneous functions on light cones: the infinitesimal structure of some degenerate principal series representations
math/9301215;math.CA;0;0;;A.G.Ramm,A.I.Zaslavsky;Singularities of the Radon transform
math/9301216;math.CO,math.GT;0;0;;N.Robertson,P.Seymour,R.Thomas;Linkless embeddings of graphs in $3$-space
math/9301217;math.CA;0;0;;H.Stahl;Best uniform rational approximation of $x^α$ on $[0,1]$
math/9301218;math.AP;0;0;;L.-F.Wu;A new result for the porous medium equation derived from the Ricci flow
math/9301219;math.OA,math.AT;0;0;;S.Zhang;Factorizations of invertible operators and $K$-theory of $C^*$-algebras
math/9301220;math.DS;0;0;;E.Bedford,M.Lyubich,J.Smillie;Distribution of periodic points of polynomial diffeomorphisms of C^2
hep-lat/9301021;hep-lat;0;21;;L.DelDebbio,M.Faber,J.Greensite;Charge Screening, Large-N, and the Abelian Projection Model of Confinement
hep-th/9301119;hep-th,gr-qc;3;18;hep-th/9203054,hep-th/9205069,hep-th/9206070;A.Bilal,I.Kogan;Hamiltonian Approach to 2D Dilaton-Gravities and Invariant Adm Mass
hep-th/9301120;hep-th;0;26;;A.P.Balachandran,G.Bimonte,P.Teotonio-Sobrinho;Edge States in 4D and their 3D Groups and Fields
cond-mat/9301039;cond-mat;0;108;;B.Y.-K.Hu,S.D.Sarma;Many-body exchange-correlation effects in the lowest subband of semiconductor quantum wires
hep-lat/9301022;hep-lat,hep-ph;9;112;hep-th/9108015,hep-th/9109007,hep-th/9201054,hep-lat/9204007,hep-lat/9204011,hep-lat/9205016,hep-lat/9205020,hep-lat/9207009,hep-lat/9209008;A.Patel;Recent Developments in Lattice QCD
funct-an/9301003;funct-an,math.OA;0;0;;L.B.Schweitzer;A Factorization Theorem for Smooth Crossed Products
funct-an/9301004;funct-an,math.OA;0;5;;B.Abadie;"Vector bundles" over quantum Heisenberg manifolds
funct-an/9301005;funct-an,math.OA;0;13;;B.Abadie;Generalized fixed-point algebras of certain actions on crossed products
hep-th/9301121;hep-th,math.QA;0;27;;S.Ramgoolam;New Modular Hopf Algebras related to rational $k$ $\widehat {sl(2)}$
nucl-th/9301019;nucl-th;0;52;;R.Machleidt,G.Q.Li;Nucleon-Nucleon Potentials in Comparison: Physics or Polemics?
hep-th/9301122;hep-th;0;19;;F.D.Jonghe,R.Siebelink,W.Troost;Hiding Anomalies
hep-ph/9301292;hep-ph;0;29;;N.Bilić,J.Cleymans,E.Suhonen,D.W.von Oertzen;Indications for a Detonating Quark-Gluon Plasma
hep-th/9301123;hep-th;0;26;;J.A.Gracey;Algorithm for Computing the $\BETA $-Function of Quantum Electrodynamics in the Large N_f Expansion
astro-ph/9301012;astro-ph;0;0;;B.Nath,D.Eichler;A Possible Forest of Emission Lines from Proto-galaxies
hep-th/9301124;hep-th;1;27;hep-th/9203013;T.R.Govindarajan,R.Shankar,N.Shaji,M.Sivakumar;O(3) Non-linear $σ$ model with Hopf term and Higher spin theories
hep-th/9301125;hep-th;0;0;;S.Mahapatra;On the Rotating Charged Black String Solution
hep-th/9301126;hep-th;1;40;hep-th/9205103;O.F.Dayi;BFV--BRST Analysis of the Classical and Quantum q-deformations of the sl(2) Algebra
gr-qc/9301023;gr-qc,hep-th;0;0;;E.W.Mielke,J.D.McCrea,Y.Ne'eman,F.W.Hehl;Avoiding degenerate coframes in an affine gauge approach to quantum gravity
hep-th/9301127;hep-th;0;0;;P.Ruelle;Automorphisms of the affine SU(3) fusion rules
nucl-th/9301020;nucl-th;0;5;;C.A.Barnes,S.E.Koonin,K.Langanke;Comment on Shadow model for sub-barrier fusion applied to light systems
alg-geom/9301007;alg-geom,math.AG;0;12;;Z.-J.Chen;Bounds of automorphism groups of genus 2 fibrations
nucl-th/9301021;nucl-th;0;26;;S.J.Lee,A.Z.Mekjian;Self-Similarity and Scaling Behavior in Nuclear Collision
nucl-th/9301022;nucl-th;0;17;;A.Z.Mekjian,S.J.Lee;Geometry, Scaling and Universality in the Mass Distributions in Heavy Ion Collisions
gr-qc/9301024;gr-qc,astro-ph,hep-th;1;33;gr-qc/0106035;J.Audretsch,A.Economou,C.O.Lousto;Topological Defects in Gravitational Theories with Non Linear Lagrangians
hep-ph/9301293;hep-ph;0;21;;M.Booth;The Electric Dipole Moment of the W and Electron in the Standard Model
hep-th/9301128;hep-th;3;16;hep-th/9108004,hep-th/9109032,hep-th/9208028;K.G.Selivanov;Geometry and Physics on $w_∞$ Orbits
hep-ph/9301294;hep-ph;0;41;;K.Cahill;A More-Effective Potential
hep-ph/9301295;hep-ph,nucl-th;2;50;hep-ph/9209257,hep-ph/9210208;T.-S.Park,D.-P.Min,M.Rho;Chiral Dynamics and Heavy-Fermion Formalism in Nuclei: I. Exchange Axial Currents
hep-ph/9301296;hep-ph;0;0;;X.Artru;Probes of parton transversity
hep-th/9301129;hep-th,gr-qc,hep-ph;3;39;hep-th/9201029,hep-th/9202014,hep-th/9204046;B.A.Campbell,N.Kaloper,R.Madden,K.A.Olive;Physical Properties of Four Dimensional Superstring Gravity Black Hole Solutions
hep-th/9301130;hep-th,cond-mat,hep-lat;1;52;hep-th/9203013;H.S.Sharatchandra;Bosonisation in any dimension
hep-th/9301131;hep-th;1;21;hep-th/9211070;D.Depireux,P.Mathieu;Integrable Supersymmetry Breaking Perturbations of N=1,2 Superconformal Minimal Models
hep-th/9301132;hep-th;0;0;;A.M.E.Gradechi;On the Supersymplectic Homogeneous Superspace Underlying the OSp(1/2) Coherent States
cond-mat/9302001;cond-mat;0;0;;R.H.McKenzie,J.A.Sauls;Comment on the Coupling of Zero Sound to the $J=1^-$ Modes of $^3$He-B
alg-geom/9302001;alg-geom,math.AG;0;0;;M.Andreatta,J.A.Wiśniewski;A note on non-vanishing and applications
gr-qc/9302001;gr-qc;0;0;;L.K.Patel,N.Dadhich;Singularity Free Inhomogeneous Cosmological Stiff Fluid Models
hep-th/9302001;hep-th;0;52;;A.Berkovich,C.Gomez,G.Sierra;Spin-Anisotropy Commensurable Chains: Quantum Group Symmetries and N=2 SUSY
hep-th/9302002;hep-th;0;0;;E.Abdalla,M.C.B.Abdalla,G.Sotkov,M.Stanishkov;Off critical current algebras
hep-th/9302003;hep-th;0;0;;E.D'Hoker,D.H.Phong;Momentum Analyticity and Finiteness of the 1-Loop Superstring Amplitude
cond-mat/9302002;cond-mat,hep-th;0;0;;Y.Hosotani;Neutral and Charged Anyon Fluids
hep-th/9302004;hep-th;0;9;;A.Nakamichi,T.Ueno;New Vector Field and BRST Charges in 2-form Einstein Gravity
hep-th/9302005;hep-th;0;23;;M.Lukin,A.Stern,I.Yakushin;Lagrangian and Hamiltonian Formalism on a Quantum Plane
hep-ph/9302201;hep-ph;1;15;hep-ph/9206242;V.Pleitez,M.D.Tonasse;Neutrinoless double beta decay in an $SU(3)_L⊗U(1)_N$ model
cond-mat/9302003;cond-mat;0;29;;A.V.Chubukov,A.Sokol;Theory of p-wave Pairing for $^3$He on Grafoil
cond-mat/9302004;cond-mat;0;0;;O.Narikiyo,D.Yoshioka;Excitation Spectrum of a Double Quantum Well System
cond-mat/9302005;cond-mat;0;0;;G.Ristow,H.J.Herrmann;Density Patterns in Granular Media
hep-ph/9302202;hep-ph;1;27;hep-ph/9212305;T.Elliott,S.F.King,P.L.White;Supersymmetric Higgs Bosons at the Limit
hep-th/9302006;hep-th;0;28;;J.de Boer,T.Tjin;The Relation between Quantum W algebras and Lie algebras
hep-ph/9302203;hep-ph,nucl-th;0;42;;J.F.Donoghue,B.R.Holstein;Photon-Photon Scattering, Pion Polarizability and Chiral Symmetry
hep-ph/9302204;hep-ph;0;0;;Harry.J.Lipkin;Physics at B-Factories
hep-th/9302007;hep-th;0;13;;I.Pesando;Vector Induced Lattice Gauge Theories
hep-th/9302008;hep-th;0;8;;E.Alvarez,J.M.Gracia-Bondia,C.P.Martin;Parameter restrictions in a non-commutative geometry model do not survive standard quantum corrections
nucl-th/9302001;nucl-th;0;25;;D.C.Zheng,L.Zamic,H.Müther;Medium corrections to the tensor interaction in nuclei: Energy difference of T=1 and T=0 J=0- states in 16O
gr-qc/9302002;gr-qc;0;20;;G.W.Gibbons,H.J.Pohle;Complex Numbers, Quantum Mechanics and the Beginning of Time
hep-ph/9302205;hep-ph;7;48;hep-ph/9203203,hep-ph/9206212,hep-ph/9206227,hep-ph/9206266,hep-ph/9207237,hep-ph/9209245,hep-ph/9302221;D.V.Nanopoulos,H.Pois;The Electroweak Phase Transition in Minimal Supergravity Models
chao-dyn/9302001;chao-dyn,nlin.CD;0;17;;N.B.Tufillaro;Topological organization of (low-dimensional) chaos
patt-sol/9302001;patt-sol,nlin.PS;0;13;;M.B.Mineev--Weinstein;Multidimensional Pattern Formation Has an Infinite Number of Constants of Motion
hep-th/9302009;hep-th,gr-qc;0;0;;M.Crescimanno;Equilibrium Two-Dimensional Dilatonic Spacetimes
hep-ph/9302206;hep-ph;0;19;;M.Hayakawa,A.I.Sanda;Searching for T,CP,CPT,and ΔS = ΔQ rule violations in the neutral K meson system - a guide
hep-th/9302010;hep-th;0;9;;T.Brzezinski,J.Rembielinski,K.A.Smolinski;Quantum Particle on a Quantum Circle
cond-mat/9302006;cond-mat;0;0;;H.J.Schulz;Interacting fermions in one dimension: from weak to strong correlation
hep-th/9302011;hep-th;0;11;;F.Belgiorno,A.S.Cattaneo,M.Martellini,F.Fucito;A Conformal Affine Toda Model of 2D-Black Holes the End-Point State and the S-Matrix
hep-ph/9302207;hep-ph;0;13;;D.Comelli,M.Pietroni;Spontaneous CP Violation in the Minimal Supersymmetric Standard Model at Finite Temperature
hep-th/9302012;hep-th;0;0;;G.Kelnhofer;On the Geometrical Structure of Covariant Anomalies in Yang-Mills Theory
hep-ph/9302208;hep-ph;1;19;hep-ph/9207228;S.A.Larin,J.A.M.Vermaseren;The three-loop QCD $β$-function and anomalous dimensions
hep-ph/9302209;hep-ph;1;36;hep-ph/9208207;M.R.Ahmady,D.Liu,Z.Tao;Long Distance Contributions to B-Decays into Higher K-Resonances
gr-qc/9302003;gr-qc,astro-ph;0;22;;D.Nunez,H.P.de Oliveira,J.Salim;Dynamics and Collision of Massive Shells in Curved Backgrounds
astro-ph/9302001;astro-ph;0;0;;E.Vishniac,P.Diamond;Angular Momentum Loss in Low Mass Accretion Disks
nucl-th/9302002;nucl-th,hep-ph;0;51;;M.Beyer;Test of Time Reversal Invariance in Proton Deuteron System
hep-ph/9302210;hep-ph;4;179;hep-ph/9203203,hep-ph/9204216,hep-ph/9204228,hep-ph/9208202;A.G.Cohen,D.B.Kaplan,A.E.Nelson;Progress in Electroweak Baryogenesis
astro-ph/9302002;astro-ph,hep-ph;1;20;astro-ph/9211011;Y.Hu,M.S.Turner,E.J.Weinberg;Dynamical Solutions to the Horizon and Flatness Problems
hep-lat/9302001;hep-lat;1;31;hep-th/9209094;C.F.Baillie,D.Espriu,D.A.Johnston;Steiner Variations on Random Surfaces
hep-ph/9302211;hep-ph;0;14;;P.Nason,M.Porrati;Small-Size Instanton Corrections to the $τ$ Hadronic Width
hep-th/9302013;hep-th;0;7;;E.Tyurin;Wave-type Solutions in the Nonlinear $σ$-model with the Dilaton
hep-th/9302014;hep-th;5;50;hep-th/9112069,hep-th/9201001,hep-th/9201011,hep-th/9201033,hep-th/9207020;J.Ambjørn,L.Chekhov,C.F.Kristjansen,Yu.Makeenko;Matrix Model Calculations beyond the Spherical Limit
hep-th/9302015;hep-th;0;4;;F.Vanderseypen;Klein-Gordon-Langevin Quantum Geometry
hep-th/9302016;hep-th,astro-ph,gr-qc;1;35;gr-qc/9509003;J.H.Kung;Quantization of the Closed Mini-Superspace Models as Bound States
hep-ph/9302212;hep-ph;0;30;;T.Gherghetta,G.Jungman;Cosmological Consequences of Spontaneous Lepton Number Violation in $SO(10)$ Grand Unification, EFI-93-07
hep-ph/9302213;hep-ph;0;23;;E.Braaten,D.Segel;Neutrino Energy Loss from the Plasma Process at all Temperatures and Densities
hep-ph/9302214;hep-ph,nucl-th;0;18;;M.N.Butler,M.J.Savage,R.P.Springer;E2/M1 Mixing Ratio of $Δ→Nγ$ and Hyperon Resonance Radiative Decay
math/9302201;math.LO;0;0;;S.D.Friedman;Provable Pi-1-2 Singletons
hep-th/9302017;hep-th;0;5;;D.Polyakov;Curvature Singularity as the Vertex Operator
hep-ph/9302215;hep-ph;0;8;;M.Y.Wang,E.D.Carlson;The Breaking of the SU(3)^3 Gauge Group
astro-ph/9302003;astro-ph,hep-ph;0;125;;M.S.Turner;Dark Matter: Theoretical Perspectives
hep-th/9302018;hep-th,cond-mat;0;19;;R.Iengo;Anyon Mean Field as an Exact Limit of a Gauge Theory
hep-th/9302019;hep-th;0;0;;J.Rembielinski;Noncommutative Dymanics
cond-mat/9302007;cond-mat;0;0;;Z.-S.Ma,Z.-B.Su;The Constraint for the Lowest Landau Level and the Chern-Simons Field Theory Approach for the Fractional Quantum Hall Effect: Infinite and Finite Systems
hep-ph/9302216;hep-ph;0;18;;K.Kołodziej,F.Jegerlehner,G.J.van Oldenborgh;Production of two hard isolated photons in $e^+e^-→μ^+μ^-γγ$ at LEP
hep-ph/9302217;hep-ph;0;13;;J.Bijnens;Violations of Dashen's Theorem
hep-ph/9302218;hep-ph;0;0;;D.Comelli,C.Verzegnassi;One Loop Corrections To The Lightest Higgs Mass In The Minimal $η$ Model
hep-ph/9302219;hep-ph;0;19;;Ll.Ametller,J.Bijnens,A.Bramon,F.Cornet;Semileptonic $π$ and $K$ Decays and the Chiral Anomaly at One-loop
astro-ph/9302004;astro-ph;0;40;;G.D.Zotti,A.Franceschini,L.Toffolatti,P.Mazzei,L.Danese;Background Radiation
astro-ph/9302005;astro-ph;0;0;;J.P.Rachen,T.Stanev,P.L.Biermann;Extragalactic ultra high energy cosmic rays, II. Comparison with experimental data
astro-ph/9302006;astro-ph,hep-ph;0;0;;K.Mannheim;The Proton Blazar
cond-mat/9302008;cond-mat;0;28;;O.Heinonen,M.D.Johnson;Mesoscopic transport beyond linear response
chao-dyn/9302002;chao-dyn,nlin.CD;0;24;;R.Artuso,G.Casati,R.Lombardi;Periodic Orbit Theory of Anomalous Diffusion
hep-ph/9302220;hep-ph,hep-th;3;50;hep-ph/9206216,hep-ph/9211215,hep-ph/9212286;H.La;Vortex Solutions in Two-Higgs Systems and $\tan β$
hep-ph/9302221;hep-ph;0;22;;B.A.Campbell,S.Davidson,J.Ellis,A.K.A.Olive;On the Baryon, Lepton-Flavour and Right-Handed Electron Asymmetries of the Universe
hep-ph/9302222;hep-ph;0;15;;B.A.Campbell,S.Davidson,K.A.Olive;Supersymmetric (S)Neutrino-Mass Induced Baryogenesis
hep-ph/9302223;hep-ph;0;70;;B.A.Campbell,S.Davidson,K.A.Olive;Inflation, Neutrino Baryogenesis, and (S)Neutrino-Induced Baryogenesis
cond-mat/9302009;cond-mat;0;89;;N.Ito;Non-equilibrium relaxation and interface energy of the Ising model
nucl-th/9302003;nucl-th,hep-ph;0;38;;J.-M.Richard;Spin and Flavour: Concluding Remarks
hep-ph/9302224;hep-ph;0;26;;U.Ellwanger;Radiative Corrections to the Neutral Higgs Spectrum in Supersymmetry with a Gauge Singlet
nucl-th/9302004;nucl-th;0;26;;C.J.Horowitz,J.Piekarewicz;Relativistic and Nuclear Structure Effects in Parity-Violating Quasielastic Electron Scattering
gr-qc/9302004;gr-qc;1;26;hep-ph/0111190;S.D.Odintsov;Two-loop effective potential in quantum field theory in curved space-time
gr-qc/9302005;gr-qc,astro-ph;0;16;;F.M.Paiva,M.J.Rebouças,M.A.H.MacCallum;On limits of spacetimes -- a coordinate-free approach
hep-ph/9302225;hep-ph;0;69;;W.T.Giele,E.W.N.Glover,D.A.Kosower;Higher Order Corrections to Jet Cross Sections in Hadron Colliders
hep-ph/9302226;hep-ph;3;33;hep-ph/9206249,hep-ph/9206254,hep-ph/9206255;S.G.Naculich,C.-P.Yuan;Inelastic Channels in WW Scattering
hep-ph/9302227;hep-ph;1;37;hep-th/9201047;J.A.Casas,C.Munoz;A Natural Solution to the MU Problem
gr-qc/9302006;gr-qc,hep-th;1;22;hep-th/9203052;J.Gegenberg,G.Kunstatter;Quantum Theory of Black Holes
hep-th/9302020;hep-th;16;82;hep-th/9108004,hep-th/9109032,hep-th/9110021,hep-th/9110062,hep-th/9111001,hep-th/9111021,hep-th/9111028,hep-th/9112061,hep-th/9201005,hep-th/9201056,hep-th/9202008,hep-th/9202021,hep-th/9203008,hep-th/9205018,hep-th/9205107,hep-th/9208027;P.Horava;Spacetime Diffeomorphisms and Topological W-Infinity Symmetry in Two Dimensional Topological String Theory
hep-ph/9302228;hep-ph;0;0;;H.E.Haber,Y.Nir;Z→A^0 A^0ν\bar ν$ and $e^+e^-→A^0 A^0 Z$ in Two Higgs Doublet Models
hep-ph/9302229;hep-ph;0;18;;J.E.Kim,B.-A.Lindholm;Neutrino masses from discrete gauge symmetries
cond-mat/9302010;cond-mat;0;29;;F.Mila,X.Zotos;Phase diagram of the one-dimensional extended Hubbard model at quarter filling
cond-mat/9302011;cond-mat;0;10;;M.Long,X.Zotos;Hole-hole correlations in the $U=∞$ limit of the Hubbard model and the stability of the Nagaoka state
hep-th/9302021;hep-th,math.QA;0;0;;B.Broda;SU(2) and the Kauffman bracket
hep-th/9302022;hep-th;3;19;hep-th/9110017,hep-th/9111056,hep-th/9203060;E.Verlinde,H.Verlinde;A Unitary S-matrix for 2D Black Hole Formation and Evaporation
hep-lat/9302002;hep-lat;0;30;;N.Ito,M.Kikuchi,Y.Okabe;Recycle of random sequences
hep-th/9302023;hep-th;3;33;hep-th/9202057,hep-th/9204063,hep-th/9206049;L.Brink,T.H.Hansson,S.Konstein,M.A.Vasiliev;The Calogero Model - Anyonic Representation, Fermionic Extension and Supersymmetry
chao-dyn/9302003;chao-dyn,nlin.CD;0;0;;N.I.Chernov,G.L.Eyink,J.L.Lebowitz,Ya.G.Sinai;Steady-State Electrical Conduction in the Periodic Lorentz Gas
hep-th/9302024;hep-th;7;21;hep-th/9201061,hep-th/9201074,hep-th/9203054,hep-th/9205069,hep-th/9206070,hep-th/9206087,hep-th/9207095;S.Nojiri,I.Oda;Black Hole from Black Hole in Two Dimensions
hep-ph/9302230;hep-ph;0;16;;X.-G.He,J.P.Ma,B.McKellar;CP violation in Higgs decays
hep-th/9302025;hep-th,cond-mat,hep-lat;0;47;;C.Münkel,D.W.Heermann;The Crumpling Transition of Dynamically Triangulated Random Surfaces
hep-th/9302026;hep-th,gr-qc;0;0;;D.Cangemi,R.Jackiw;Poincaré Gauge Theory for Gravitational Forces in (1+1) Dimensions
hep-ph/9302231;hep-ph;0;25;;C.Coriano',H.-nan.Li;QCD Sum Rule and Perturbative QCD Approaches to Pion Compton Scattering
hep-th/9302027;hep-th;1;27;hep-th/9201056;O.Aharony,O.Ganor,J.Sonnenschein,S.Yankielowicz;c=1 String Theory as a Topological G/G Model
cond-mat/9302012;cond-mat;0;15;;B.A.Sanborn,B.Y.-K.Hu,S.D.Sarma;Enhancement of the decay rate of nonequilibrium carrier distributions due to scattering-in processes
hep-ph/9302232;hep-ph;0;0;;M.Burkardt,R.L.Jaffe;Polarized $q→Λ$ Fragmentation Functions from $e^+e^-→Λ+X^*$
hep-ph/9302233;hep-ph,hep-lat;0;0;;A.Gocksch,R.D.Pisarski;Partition function for the eigenvalues of the Wilson line
hep-ph/9302234;hep-ph;2;20;hep-ph/9207219,hep-ph/9211228;J.Lopez,D.Nanopoulos,H.Pois,X.Wang,A.Zichichi;Improved LEP lower bound on the lightest SUSY Higgs mass from Radiative Electroweak Breaking and its Experimental Consequences
hep-ph/9302235;hep-ph,hep-lat;0;20;;S.D.H.Hsu;Complementarity and Chiral Fermions in SU(2) gauge Theories
gr-qc/9302007;gr-qc;1;74;gr-qc/9507004;A.O.Barvinsky,A.Yu.Kamenshchik,I.P.Karmazin;The renormalization group for non-renormalizable theories: Einstein gravity with a scalar field
hep-th/9302028;hep-th,math.QA;0;3;;A.Ocneanu;A note on simplicial dimension shifting
alg-geom/9302002;alg-geom,math.AG;0;0;;R.Paoletti;On the surjectivity of Wahl maps on a general curve
cond-mat/9302013;cond-mat;0;22;;A.Sokol,E.Gagliano,S.Bacci;Theory of Nuclear Spin-Lattice Relaxation in La$_2$CuO$_4$ at High Temperatures
hep-th/9302029;hep-th,cond-mat;0;8;;W.Chen,Y.Makeenko,G.W.Semenoff;Solving the Conformal Bootstrap: Four-Fermion Interactions at 2<d<4
hep-th/9302030;hep-th;1;15;hep-ph/9301210;F.D.T.Smith;Hermitian Jordan Triple Systems, the Standard Model plus Gravity, and Alpha = 1/137.03608
hep-ph/9302236;hep-ph;1;11;hep-ph/9204205;L.E.Ibanez,F.Quevedo;Baryon Asymmetry, Supersymmetry and Gravitational Anomalies
gr-qc/9302008;gr-qc;0;0;;P.S.Joshi,I.H.Dwivedi;The Structure of Naked Singularity in Self-similar Gravitational Collapse II
gr-qc/9302009;gr-qc,astro-ph,hep-ph;1;31;cond-mat/9211003;A.Mezhlumian;Towards the Theory of Stationary Universe
hep-th/9302031;hep-th;0;7;;A.A.A.Jr;White Noise and Heating of Open Quantum Field Fermi Systems
hep-th/9302032;hep-th;0;0;;D.Dalmazi,E.Abdalla;Correlators in non-critical superstrings including the spinor emission vertex
hep-th/9302033;hep-th;16;63;hep-th/9108011,hep-th/9109038,hep-th/9110004,hep-th/9110053,hep-th/9110065,hep-th/9110067,hep-th/9112044,hep-th/9112070,hep-th/9202092,hep-th/9203039,hep-th/9204046,hep-th/9205046,hep-th/9206077,hep-th/9206078,hep-th/9209052,hep-th/9210015;E.Kiritsis;Exact Duality Symmetries in CFT and String Theory
alg-geom/9302003;alg-geom,math.AG;0;22;;S.Sardo-Infirri;Lefschetz Fixed Point Theorem and Lattice Points in Convex Polytopes
hep-th/9302034;hep-th;0;17;;S.E.Derkachov,N.A.Kivel,A.S.Stepanenko,A.N.Vasiliev;On Calculation of 1/n Expansions of Critical Exponents in the Gross-Neveu Model with the Conformal Technique
hep-ph/9302237;hep-ph;0;24;;P.A.Rączka,A.Szymacha,S.Tatur;Experimental Constraints on the Neutrino Oscillations and a Simple Model of Three Flavour Mixing
hep-ph/9302238;hep-ph;0;36;;E.V.Shuryak,J.J.M.Verbaarschot;Quark Propagation in the Random Instanton Vacuum
hep-ph/9302239;hep-ph;0;28;;E.V.Shuryak,J.J.M.Verbaarschot;Mesonic Correlation Functions in the Random Instanton Vacuum
hep-th/9302035;hep-th;1;37;hep-th/9205034;E.Cremmer,J.-L.Gervais,J.-F.Roussel;The Quantum Group Structure of 2D Gravity and Minimal Models II: The Genus-Zero Chiral Bootstrap
funct-an/9302001;funct-an,math.OA;0;0;;R.Exel;The Bunce-Deddens Algebras as Crossed Products by Partial Automorphisms
cond-mat/9302014;cond-mat;0;13;;Z.Xi,B.Chakraborty;Kinetics of Ordering in Cu3Au: An Atomistic Approach
hep-ph/9302240;hep-ph;0;25;;S.A.Larin;The renormalization of the axial anomaly in dimensional regularization
nucl-th/9302005;nucl-th;0;0;;S.Schramm,S.E.Koonin;Can Plasma Scattering Mimic a Cosmological Red-Shift?
hep-th/9302036;hep-th;0;0;;W.Siegel;Two-Vierbein Formalism for String-Inspired Axionic Gravity
funct-an/9302002;funct-an,math.OA;0;22;;S.C.Power;Algebraic orders on $K_0$ and approximately finite operator algebras
funct-an/9302003;funct-an,math.OA;0;1;;S.C.Power;On the outer automorphism groups of triangular alternation limit algebras
hep-ph/9302241;hep-ph;0;0;;R.D.Pisarski;Medley in finite temperature field theory
hep-ph/9302242;hep-ph;0;0;;R.D.Pisarski;Damping rates for moving particles in hot QCD
hep-ph/9302243;hep-ph;0;12;;K.Saririan;On Fermion Zero-Modes in Instanton $V-A$ Models With Spontaneous Symmetry Breaking
hep-ph/9302244;hep-ph;0;0;;K.Adel,Y.-P.Yao;Effective Lagrangian for $b →s$ Processes with QCD-Corrections
hep-th/9302037;hep-th;5;18;hep-th/9108001,hep-th/9202092,hep-th/9204090,hep-th/9205037,hep-th/9206006;M.J.Perry,E.Teo;Non-Singularity of the Exact Two-Dimensional String Black Hole
comp-gas/9302001;comp-gas,nlin.CG;0;0;;J.Theiler;Some comments on the correlation dimension of $1/f^α$ noise
hep-th/9302038;hep-th;0;0;;A.Sen;SL(2, Z) Duality and Magnetically Charged Strings
gr-qc/9302010;gr-qc;0;44;;L.Amendola;Cosmology with Nonminimal Derivative Couplings
astro-ph/9302007;astro-ph;0;0;;A.M.Dunn,R.Laflamme;The Least Action Principle And The Spin Of Galaxies In The Local Group
hep-ph/9302245;hep-ph,nucl-th;0;11;;V.Bernard,A.H.Blin,B.Hiller,U.-G.Meißner,M.C.Ruivo;Strong and Radiative Meson Decays in a Generalized Nambu--Jona-Lasinio Model
gr-qc/9302011;gr-qc,hep-th;2;53;hep-th/9202076,hep-th/9203079;L.Smolin;Finite, diffeomorphism invariant observables in quantum gravity
gr-qc/9302012;gr-qc;4;30;hep-th/9108001,hep-th/9111056,hep-th/9204099,hep-th/9205095;M.Banados,M.Henneaux,C.Teitelboim,J.Zanelli;Geometry of the 2+1 Black Hole
gr-qc/9302013;gr-qc;2;96;gr-qc/9208005,gr-qc/9208006;E.Calzetta,B.L.Hu;Decoherence of Correlation Histories
hep-th/9302039;hep-th;3;26;hep-th/9108003,hep-th/9111002,hep-th/9210010;K.Ito;Free Field Realization of $N=2$ Super $W_3$ Algebra
hep-th/9302040;hep-th;1;13;hep-th/9201021;S.N.Solodukhin;Two-dimensional Black Hole With Torsion
astro-ph/9302008;astro-ph;0;8;;F.D.S.Jr;Gamma Ray Bursts and CETI
gr-qc/9302014;gr-qc,astro-ph,hep-th;0;12;;R.H.Brandenberger;Towards a Nonsingular Universe
hep-ph/9302246;hep-ph;0;51;;J.Prades;Massive Spin-1 Field Chiral Lagrangian from an Extended Nambu-Jona-Lasinio Model of QCD
hep-ph/9302247;hep-ph,nucl-th;0;0;;U.-G.Meißner;Recent Developments in Chiral Perturbation Theory
hep-ph/9302248;hep-ph;2;18;hep-ph/9209205,hep-ph/9209230;E.Gotsman,E.M.Levin,U.Maor;Large Rapidity Gaps in PP Collisions
hep-ph/9302249;hep-ph;0;0;;Ph.Brax,J.-L.Meunier,R.Peschanski;Angular Intermittency in QCD Jets
cond-mat/9302015;cond-mat;0;29;;J.J.Dorado,F.Flores;Molecular-orbital theory for the stopping power of atoms in the low velocity regime:the case of helium in alkali metals
hep-lat/9302003;hep-lat;0;0;;T.Hara,G.Slade,A.D.Sokal;New Lower Bounds on the Self-Avoiding-Walk Connective Constant
hep-th/9302041;hep-th;3;24;hep-th/9205071,hep-th/9207001,hep-th/0209014;T.Strobl;Comment on Gravity and the Poincare Group
hep-th/9302042;hep-th,math.QA;1;8;hep-th/9111043;A.A.Vladimirov;A method for obtaining quantum doubles from the Yang-Baxter R-matrices
hep-th/9302043;hep-th,math.QA;1;14;hep-th/9111043;A.A.Vladimirov;On the Hopf algebras generated by the Yang-Baxter R-matrices
hep-ph/9302250;hep-ph;0;22;;Yu.L.Dokshitzer,V.A.Khoze,L.H.Orr,W.J.Stirling;Properties of Soft Radiation Near $\tt $ and $W^+W^-$ Threshold
hep-ph/9302251;hep-ph;0;0;;K.L.Sterner;Search for Anomalous $γγ$ Production at TRISTAN
hep-ph/9302252;hep-ph;0;22;;T.K.Kuo,G.T.Park,M.Zralek;Boson Pair Productions In $e^+$ $e^-$ Annihilation
hep-ph/9302253;hep-ph;0;44;;T.G.Rizzo;Constraints on New Physics From Tevatron Dijet Data
gr-qc/9302015;gr-qc;0;18;;J.Twamley;The quantum behavior of general time dependent quadratic systems linearly coupled to a bath
gr-qc/9302016;gr-qc;0;0;;A.Vilenkin;Quantum Cosmology
hep-th/9302044;hep-th,gr-qc;0;0;;C.A.Manogue,J.Schray;Finite Lorentz Transformations, Automorphisms, and Division Algebras
hep-th/9302045;hep-th;0;15;;H.Kikuchi;Poincare invariance in temporal gauge canonical quantization and \(θ\)-vacua
hep-th/9302046;hep-th;1;24;hep-th/9201059;A.Lahiri;Constrained Dynamics of the Coupled Abelian Two-Form
hep-ph/9302254;hep-ph,astro-ph;1;15;hep-ph/9208247;R.H.Brandenberger,A.T.Sornborger,M.Trodden;Gamma Ray Bursts from Ordinary Cosmic Strings
cond-mat/9302016;cond-mat,hep-lat;0;38;;M.C.D.E.L.G.W.S.P.Sodano;SU(N) Antiferromagnets and Strongly Coupled QED: Effective Field Theory for Josephson Junctions Arrays
hep-ph/9302255;hep-ph;2;44;hep-ph/9206262,hep-ph/9209245;C.Im,G.Kane,P.Malde;Could Large CP Violation Be Detected at Colliders?
cond-mat/9302017;cond-mat;0;31;;H.Castella,X.Zotos;Exact calculation of spectral properties of a particle interacting with a one dimensional fermionic system
nucl-th/9302006;nucl-th;0;12;;G.Martinez-Pinedo,A.Poves;The Beta Decay of 44V
alg-geom/9302004;alg-geom,math.AG;0;4;;A.H.Durfee;Intersection homology Betti numbers
cond-mat/9302018;cond-mat;0;0;;P.Coleman,E.Miranda,A.Tsvelik;Possible Realization of Odd Frequency Pairing in Heavy Fermion Compounds
hep-th/9302047;hep-th;0;29;;S.Deser,A.Schwimmer;Geometric Classification of Conformal Anomalies in Arbitrary Dimensions
hep-th/9302048;hep-th;1;20;hep-th/9209122;T.Eguchi,H.Kanno,Y.Yamada,S.-K.Yang;Topological Strings, Flat Coordinates and Gravitational Descendants
hep-th/9302049;hep-th;6;20;hep-th/9108004,hep-th/9111047,hep-th/9111059,hep-th/9203008,hep-th/9204005,hep-th/9204085;A.Giveon,M.Rocek;On the BRST Operator Structure of the N=2 String
hep-th/9302050;hep-th;2;26;hep-th/9205018,hep-th/9206097;P.H.Damgaard,F.D.Jonghe;Master Equations for Extended Lagrangian BRST Symmetries
hep-th/9302051;hep-th;0;46;;G.Cognola,K.Kirsten,S.Zerbini;One-loop effective potential on hyperbolic manifolds
hep-th/9302052;hep-th,astro-ph,gr-qc;0;39;;H.J.de Vega;Strings in Curved Spacetimes
hep-ph/9302256;hep-ph;0;127;;M.Drees,R.M.Godbole;Resolved Photon Processes
hep-ph/9302257;hep-ph;1;25;hep-ph/9208249;E.L.Berger,R.Meng;Longitudinal Structure Function at Intermediate x and the Gluon Density
hep-ph/9302258;hep-ph;0;21;;P.Arnold;One-loop fluctuation-dissipation formula for bubble-wall velocity
hep-th/9302053;hep-th;0;0;;C.Grosche,F.Steiner;Classification of Solvable Feynman Path Integrals
hep-th/9302054;hep-th;0;0;;C.Grosche;Path Integral Solution of a Class of Explicitly Time-Dependent Potentials
hep-th/9302055;hep-th;0;0;;C.Grosche;$δ$-Function Perturbations and Boundary Problems by Path Integration
hep-th/9302056;hep-th;0;0;;C.Grosche;Selberg Supertrace Formula for Super Riemann Surfaces III: Bordered Super Riemann Surfaces
hep-ph/9302259;hep-ph,astro-ph;3;91;hep-th/9202046,hep-ph/9207219,hep-ph/9211201;L.Roszkowski;Supersymmetric Dark Matter - a Review
hep-th/9302057;hep-th;0;0;;J.M.Figueroa-O'Farrill,S.Stanciu;On a New Supersymmetric KdV Hierarchy in $2-d$ Quantum Supergravity
hep-th/9302058;hep-th;2;40;hep-th/9202092,hep-th/9205046;C.Kounnas;Construction of String Solutions around Non-trivial Backgrounds
hep-th/9302059;hep-th;2;15;hep-th/9205065,hep-th/9207004;V.Sadov;Free field resolution for nonunitary representations of N=2 SuperVirasoro
hep-th/9302060;hep-th;0;0;;V.Sadov;On the spectra of $\hat {sl}(N)_k/\hat {sl}(N)_k$-cosets and $W_N$ gravities
hep-th/9302061;hep-th;1;21;hep-th/9302062;A.Anderson;Quantum Canonical Transformations and Integrability: Beyond Unitary Transformations
hep-th/9302062;hep-th;0;9;;A.Anderson;Quantum Canonical Transformations: Physical Equivalence of Quantum Theories
hep-th/9302063;hep-th;0;17;;N.Aizawa;A Classically Singular Representation of $ su_q(n) $
hep-th/9302064;hep-th;0;29;;T.Kobayashi,T.Uematsu;q-deformed superconformal algebra on quantum superspace
cond-mat/9302019;cond-mat;0;20;;T.Bhattacharya,A.Billoire,R.Lacaze,Th.Jolicœur;Critical Behavior of the Antiferromagnetic Heisenberg Model on a Stacked Triangular Lattice
hep-ph/9302260;hep-ph;0;27;;H.B.Kim,J.E.Kim;Coupling Constant Unification and LEP Data
hep-ph/9302261;hep-ph,astro-ph;0;0;;N.Kaiser,R.A.Malaney,G.D.Starkman;Neutrino-Lasing in The Early Universe
astro-ph/9302009;astro-ph;0;27;;J.N.Fry,E.Gaztanaga;Biasing and Hierarchical Statistics in Large-scale Structure
gr-qc/9302017;gr-qc;8;33;hep-th/9209055,hep-th/9209113,hep-th/9303048,hep-th/9305040,gr-qc/9305012,hep-th/9306041,hep-th/9306069,hep-th/9306083;V.P.Frolov,D.N.Page;Proof of the Generalized Second Law for Quasistationary Semiclassical Black Holes
hep-th/9302065;hep-th;3;33;hep-th/9202014,hep-th/9203083,hep-th/9205027;G.-J.Cheng,R.-R.Hsu,W.-F.Lin;Dyonic Black Holes in String Theory
hep-th/9302066;hep-th;0;6;;P.Caban,A.Dobrosielski,A.Krajewska,Z.Walczak;On the q-Deformed Hamiltonian Mechanics
hep-th/9302067;hep-th;0;35;;A.Mikovic;Canonical quantization approach to 2d gravity coupled to c<1 matter
hep-th/9302068;hep-th,cond-mat;0;0;;D.M.McAvity,H.Osborn;Energy Momentum Tensor in Conformal Field Theories Near a Boundary
hep-th/9302069;hep-th;0;0;;S.P.Khastgir,J.Maharana;Topology changing processes and symmetries of string effective action
hep-th/9302070;hep-th;5;27;hep-th/9110065,hep-th/9201061,hep-th/9201074,hep-th/9202004,hep-th/9206070;P.Yi;Nonsingular 2-D Black Holes and Classical String Backgrounds
hep-th/9302071;hep-th;0;0;;G.B.Cleaver,P.J.Rosenthal;Aspects of Fractional Superstrings
hep-ph/9302262;hep-ph;0;8;;G.Cvetic,M.Nowakowski,Y.-L.Wu;Multi-Higgs Doublet Model: Can It Account for l^+l^-γγEvents?
hep-th/9302072;hep-th;0;0;;M.B.Paranjape,R.Ross;Instantons and the Ground State of the Massive Schwinger Model
cond-mat/9302020;cond-mat;0;27;;T.Hsu,B.Doucot;Effect of three-particle correlations in low dimensional Hubbard models
hep-ph/9302263;hep-ph;0;39;;M.A.Doncheski,M.B.G.Ducati,F.Halzen;$J/ψ$ at small-$x$
cond-mat/9302021;cond-mat;0;0;;P.Ossadnik;New model for crack growth using random walkers
hep-th/9302073;hep-th;0;0;;J.Barrett,G.W.Gibbons,M.J.Perry,C.N.Pope,P.J.Ruback;Kleinian Geometry and the N=2 Superstring
hep-ph/9302264;hep-ph;0;10;;J.Chýla;Strong renormalization scheme dependence in $τ$-lepton decays: fact or fiction?
hep-ph/9302265;hep-ph;2;18;hep-ph/9204207,hep-ph/9206241;A.F.Falk;Excited Heavy Mesons and Kaon Loops in Chiral Perturbation Theory
chao-dyn/9302004;chao-dyn,nlin.CD;0;16;;R.Mainieri;Can averaged orbits be used to extract scaling functions?
hep-ph/9302266;hep-ph,hep-lat;1;43;hep-lat/9208025;D.B.Leinweber;Do Quarks Really Form Diquark Clusters in the Nucleon?
gr-qc/9302018;gr-qc,hep-th;0;0;;R.D.Sorkin;Impossible Measurements on Quantum Fields
hep-ph/9302267;hep-ph;1;20;hep-ph/9206205;D.Chang,W.-S Hou,W.-Y.Keung;Two--loop Contributions of Flavor Changing Neutral Higgs Boson to $μ→eγ$
hep-th/9302074;hep-th;0;35;;E.Elizalde,S.D.Odintsov;Renormalization-group improved effective potential for gauge theories in curved spacetime
hep-th/9302075;hep-th,gr-qc;2;14;hep-th/9111056,hep-th/9207095;S.K.Rama;Tachyon Splits the (d = 2 String) Black Hole Horizon and Turns it Singular
hep-th/9302076;hep-th,math.QA;0;16;;S.Majid;Free Braided Differential Calculus, Braided Binomial Theorem and the Braided Exponential Map
nucl-th/9302007;nucl-th;1;83;hep-ph/9207251;T.Barnes,S.Capstick,M.D.Kovarik,E.S.Swanson;NN Core Interactions and Differential Cross Sections from One Gluon Exchange
hep-th/9302077;hep-th;7;51;hep-th/9110073,hep-th/9112060,hep-th/9201039,hep-th/9203039,hep-th/9205037,hep-th/9301015,hep-th/9301047;I.Jack,J.Panvel;WZW-Toda Reduction using the Casimir Operator
hep-th/9302078;hep-th;1;18;gr-qc/9506091;D.V.Fursaev,G.Miele;Finite-Temperature Scalar Field Theory in Static de Sitter Space
hep-ph/9302268;hep-ph;0;21;;F.Schlumpf;The Electric and Magnetic Form Factors of the Neutron
hep-ph/9302269;hep-ph;5;20;hep-ph/9203222,hep-ph/9204229,hep-ph/9204237,hep-ph/9205228,hep-ph/9908362;M.Neubert;Reparametrization invariance and the expansion of currents in the heavy quark effective theory
hep-ph/9302270;hep-ph;0;0;;E.P.Gilson,R.L.Jaffe;Very Small Strangelets
hep-th/9302079;hep-th;0;15;;P.Argyres;Fractional Superstring Tree Scattering Amplitudes
hep-th/9302080;hep-th,gr-qc;0;0;;A.Strominger,S.P.Trivedi;Information Consumption by Reissner-Nordstrom Black Holes
cond-mat/9302022;cond-mat;1;17;cond-mat/9209002;K.Okumura;Various condensed matter Hamiltonians in terms of U(2/2) operators and their symmetry structures
hep-ph/9302271;hep-ph;2;22;hep-ph/9206242,hep-ph/9303304;J.T.Liu,D.Ng;$Z$--$Z'$ mixing and oblique corrections in an ${\rm SU(3) ×U(1)}$ model
hep-ph/9302272;hep-ph;0;0;;J.F.Gunion,H.E.Haber,G.L.Kane,S.Dawson;Errata for "The Higgs Hunter's Guide"
hep-ph/9302273;hep-ph;0;8;;C.Q.Geng,K.Whisnant,B.-L.Young;Right-handed Neutral Currents, Families and the LEP $l^+l^-γγ$ Events
gr-qc/9302019;gr-qc,astro-ph,hep-ph;0;22;;E.D.Stewart,D.H.Lyth;A more accurate analytic calculation of the spectrum of cosmological perturbations produced during inflation
hep-lat/9302004;hep-lat;1;25;hep-lat/9207032;B.Alles,M.Campostrini,A.D.Giacomo,Y.Gunduc,E.Vicari;Renormalization and topological susceptibility on the lattice: SU(2) Yang-Mills theory
hep-ph/9302274;hep-ph;1;27;hep-ph/9208238;H.K.Lee,M.Rho;Vanishing of Nonabelian Berry Phases in Heavy Solitonic Baryons
hep-ph/9302275;hep-ph;0;19;;A.Ballestrero,E.Maina,S.Moretti;Hard Photon Pair Production at LEP
cond-mat/9302023;cond-mat;0;18;;B.Bonnier,M.Hontebeyrie,C.Meyers;On the random filling of $R^d$ by non-\-overlapping d-dimensional cubes
cond-mat/9302024;cond-mat;0;17;;M.Raykin,A.Auerbach;The 1/N Expansion and Long Range Antiferromagnetic Order
cond-mat/9302025;cond-mat;0;0;;A.Auerbach;The Semiclassical Expansion of the t-J model
funct-an/9302004;funct-an,math.FA;0;9;;J.Ramanathan,P.Topiwala;Time-Frequency Localization and the Gabor Transform
astro-ph/9302010;astro-ph,gr-qc,hep-ph;0;25;;A.R.Liddle,D.H.Lyth;The End for Extended Inflation?
hep-ph/9302276;hep-ph;2;30;hep-ph/9205230,hep-ph/9209206;Z.Tao;Charged Scalar Particles and $τ$ Leptonic Decay
nucl-th/9302008;nucl-th;0;23;;W.van Dijk,M.W.Kermode,D.-C.Zheng;The $^3S_1-^3D_1$ effective-range parameters of some realistic nucleon-nucleon potentials
cond-mat/9302026;cond-mat;1;11;cond-mat/9209002;K.Okumura;The supergroup U(M/N) with regard to electronic Hamiltonians
hep-ph/9302277;hep-ph;1;12;hep-ph/9207212;E.Ma;Derivation of $m_A \simeq M_Z$ and $\tan β> \sqrt 3$ in the Minimal Supersymmetric Standard Model
hep-th/9302081;hep-th,hep-ph;0;29;;A.Davidson,U.Paz;Threefold Family of Charged Spin-1/2 Dirac Bubbles
hep-th/9302082;hep-th;0;0;;B.Urosevic;Perturbation Theory in Two Dimensional Open String Field Theory
gr-qc/9302020;gr-qc;0;26;;R.Capovilla,J.Dell,T.Jacobson;The Initial Value Problem in Light of Ashtekar's Variables
cond-mat/9302027;cond-mat;0;20;;A.V.Balatsky,J.Bonca;Even and odd-frequency pairing correlations in 1-D t-J-h model: a comparative study
hep-th/9302083;hep-th;5;91;hep-th/9110054,hep-th/9111040,hep-th/9202092,hep-th/9205037,hep-th/9206006;A.A.Tseytlin;Conformal sigma models corresponding to gauged Wess-Zumino-Witten theories
gr-qc/9302021;gr-qc;0;139;;B.L.Hu;Fluctuation, Dissipation and Irreversibility in Cosmology
hep-th/9302084;hep-th,math.QA;0;0;;S.Piunikhin;Combinatorial expression for universal Vassiliev link invariant
hep-th/9302085;hep-th;1;25;hep-th/9503230;L.V.Avdeev,D.I.Kazakov,I.N.Kondrashuk;Difficulties of an Infrared Extension of Differential Renormalization
astro-ph/9302011;astro-ph;0;0;;C.C.Dudley,C.G.Wynn-Williams;The 8-13 Micron Spectrum of Arp 299C
hep-th/9302086;hep-th,math.QA;0;0;;P.Bouwknegt,J.McCarthy,K.Pilch;Semi-infinite cohomology of W-algebras
hep-ph/9302278;hep-ph;0;18;;A.L.Macpherson,B.A.Campbell;Toponium Tests Of Top-Quark Higgs Bags
hep-th/9302087;hep-th;0;0;;D.R.Grigore;On the Uniqueness of the Newton-Wigner Position Operator
gr-qc/9302022;gr-qc;0;0;;J.M.Mourão;Symmetric solutions of Einstein-Yang-Mills equations
hep-th/9302088;hep-th,cond-mat,math.QA;2;16;hep-th/9110074,hep-th/9203035;D.Arnaudon,V.Rittenberg;Quantum Chains with U_q(SL(2)) Symmetry and Unrestricted Representations
hep-th/9302089;hep-th;2;24;hep-th/9110074,hep-th/9202011;R.Cuerno,C.Gomez,E.Lopez,G.Sierra;The Hidden Quantum Group of the 8-vertex Free Fermion Model: q-Clifford Algebras
hep-th/9302090;hep-th;0;30;;A.P.Isaev,Z.Popowicz;Quantum Group Gauge Theories and Covariant Quantum Algebras
gr-qc/9302023;gr-qc;0;0;;N.Ó.Murchadha;Brill Waves
hep-th/9302091;hep-th;4;67;hep-th/9112010,hep-th/9204005,hep-th/9207024,hep-th/9207062;S.V.Ketov;Space-Time Supersymmetry of Extended Fermionic Strings in $2 + 2$ Dimensions
hep-ph/9302279;hep-ph;0;41;;M.MANGANO;On the B and J/Psi Cross Section Measurements at Ua1 and CDF
hep-th/9302092;hep-th,alg-geom,math.QA;0;0;;B.Broda;Surgical invariants of four-manifolds
cond-mat/9302028;cond-mat,nlin.PS,patt-sol;0;24;;E.Hernandez-Garcia,J.Vinals,R.Toral,M.S.Miguel;Fluctuations and Pattern Selection Near an Eckhaus Instability
hep-lat/9302005;hep-lat;1;27;hep-lat/9208013;F.Karsch,M.L.Laursen,T.Neuhaus,B.Plache;Vacuum Tunneling and Periodic Structure in Lattice Higgs Models
hep-th/9302093;hep-th,nucl-th;0;15;;N.Poliatzky;Levinson's Theorem for Dirac Equation
cond-mat/9302029;cond-mat;0;16;;R.A.Jalabert,J.-L.Pichard,C.W.J.Beenakker;Long-Range Energy-Level Interaction in Small Metallic Particles
cond-mat/9302030;cond-mat;0;17;;P.Kopietz;Universal persistent currents in mesoscopic metal rings due to long-range Coulomb interactions
gr-qc/9302024;gr-qc,hep-th;0;0;;A.Ashtekar;Mathematical Problems of Non-perturbative Quantum General Relativity
cond-mat/9302031;cond-mat;0;16;;K.Schönhammer,V.Meden;Nonuniversal spectral properties of the Luttinger model
cond-mat/9302032;cond-mat;0;0;;M.-H.Chung;Many Particle Hamiltonian for the Fractional Quantum Hall Effect
hep-lat/9302006;hep-lat;0;0;;V.V.Matveev;Numerical Study of Periodic Instanton Configurations in Two-dimensional Abelian Higgs Theory
hep-lat/9302007;hep-lat;0;33;;RTN Collaboration,G.Perez,Gonzalez-Arroyo,Martinez,Fernandez,M.Sudupe,Ruiz-Lorenzo,Azcoiti,Campos,Ciria,Cruz,Iniguez,Lesmes,Piedrafita,Rivero,Tarancon,Tellez,Badoni,Pech;Instanton-like Contributions to the Dynamics of Yang-Mills Fields on the Twisted Torus
hep-th/9302094;hep-th;0;22;;P.Martin,H.Saleur;The Blob Algebra and the Periodic Temperley-Lieb Algebra
hep-th/9302095;hep-th;0;20;;P.Martin,H.Saleur;Algebras in Higher Dimensional Statistical Mechanics - the Exceptional Partition (MEAN Field) Algebras
hep-ph/9302280;hep-ph;0;0;;Z.Bern,L.Dixon,D.A.Kosower;One-Loop Corrections to Five-Gluon Amplitudes
hep-ph/9302281;hep-ph;0;0;;K.Melnikov,O.Yakovlev;Higgs - Two Photon Decay: QCD radiative correction
hep-th/9302096;hep-th;1;9;hep-th/9202014;F.Wilczek;Quantum Purity at a Small Price: Easing a Black Hole Paradox
gr-qc/9302025;gr-qc;0;109;;B.L.Hu,J.P.Paz,S.Sinha;Minisuperspace as a Quantum Open System
hep-ph/9302282;hep-ph;1;29;hep-ph/9205233;R.Garisto,G.Kane;What is the Natural Size of Supersymmetric $CP$ Violation?
hep-th/9302097;hep-th;0;0;;C.Grosche;An Introduction into the Feynman Path Integral
hep-ph/9302283;hep-ph;0;21;;M.C.Gonzalez-Garcia,F.Halzen,R.A.Vazquez,E.Zas;Empirical Determination of the Very High Energy Heavy Quark Cross Section from Non-Accelerator Data
hep-ph/9302284;hep-ph;0;11;;O.J.P.Eboli,M.C.Gonzalez-Garcia,F.Halzen,D.Zeppenfeld;Measuring the Gamma-Gamma Coupling of the Higgs at Linear Colliders
cond-mat/9302033;cond-mat;0;10;;P.Nielaba,V.Privman,J.-S.Wang;Irreversible Multilayer Adsorption
gr-qc/9302026;gr-qc;0;30;;A.Ashtekar,R.S.Tate,C.Uggla;Minisuperspaces: Symmetries and Quantization
gr-qc/9302027;gr-qc;0;40;;A.Ashtekar,R.S.Tate,C.Uggla;Minisuperspaces: Observables and Quantization
hep-th/9302098;hep-th,cond-mat,funct-an,math.FA;0;0;;O.Mokhov;On the Squeezed Vacuum States Corresponding to the General Two-Mode Bogolubov Transformation
hep-ph/9302285;hep-ph;0;17;;K.Hagiwara,S.Matsumoto,M.Tanaka;Consequences of a Possible Di-Gamma Resonace at TRISTAN
hep-th/9302099;hep-th;0;0;;A.Sagnotti;Anomaly Cancellations and Open-String Theories
hep-th/9302100;hep-th;0;44;;Z.Jaskolski,K.A.Meissner;Static Quark Potential from the Polyakov Sum over Surfaces
hep-th/9302101;hep-th;6;17;hep-th/9201061,hep-th/9201074,hep-th/9203042,hep-th/9203052,hep-th/9203054,hep-th/9206071;K.-ji.Hamada,A.Tsuchiya;Quantum Gravity and Black Hole
hep-th/9302102;hep-th,math.QA;0;0;;M.Nazarov,V.Tarasov;Yangians and Gelfand-Zetlin bases
hep-ph/9302286;hep-ph;0;15;;R.Decker,M.Finkemeier;Radiative Tau Decays with One Pseudoscalar Meson
hep-ph/9302287;hep-ph;5;31;hep-ph/9206242,hep-ph/9207264,hep-ph/9212271,hep-ph/9301232,hep-ph/9304294;V.Pleitez;$SU(n)_c⊗SU(m)_L⊗U(1)_N$ generalizations of the Standard Model
gr-qc/9302028;gr-qc;0;0;;L.Diosi,B.Lukacs;Karolyhazy's quantum space-time generates neutron star density in vacuum
hep-th/9302103;hep-th,alg-geom,math.AG;1;35;hep-th/9204102;M.Bershadsky,S.Cecotti,H.Ooguri,C.Vafa,S.Katz;Holomorphic Anomalies in Topological Field Theories
hep-ph/9302288;hep-ph;1;19;hep-ph/9205238;G.Degrassi;Current Algebra Approach to Heavy Top Effects in $Z →b+ \bar b$
hep-th/9302104;hep-th;2;16;hep-th/9110017,hep-th/9112020;H.Verlinde,E.Verlinde;QCD at High Energies and Two-Dimensional Field Theory
hep-th/9302105;hep-th,alg-geom,math.AG;0;42;;J.M.Rabin;Super Elliptic Curves
gr-qc/9302029;gr-qc;0;54;;B.L.Hu,Y.Zhang;Quantum and Thermal Fluctuations, Uncertainty Principle, Decoherence and Classicality*
hep-th/9302106;hep-th;0;0;;A.Jevicki;Fields and Symmetries of 2D Strings
hep-ph/9302289;hep-ph;0;0;;D.A.Kosower;Light Composite Vector Bosons
hep-ph/9302290;hep-ph;2;8;hep-ph/9207207,hep-ph/9209299;C.D.Carone;Double Beta Decay with Vector Majorons
gr-qc/9302030;gr-qc;0;35;;B.L.Hu;Critical Dynamics in the Early Universe
funct-an/9302005;funct-an,math.OA;0;0;;K.J.Dykema;Factoriality and the Connes invariant T(M) for free products of von Neumann algebras
funct-an/9302006;funct-an,math.OA;0;8;;K.Dykema,A.Nica;On the Fock representation of the q-commutation relations
hep-th/9302107;hep-th;0;25;;W.-M.Zhang,A.Harindranth;Residual Gauge Fixing in Light-Front QCD
hep-th/9302108;hep-th;0;0;;R.R.Khuri;Instantons, Monopoles, Strings and Fivebranes
gr-qc/9302031;gr-qc;0;87;;B.L.Hu;Quantum Statistical Processes in the Early Universe
gr-qc/9302032;gr-qc;0;0;;J.W.Moffat;Do Black Holes Exist?
chao-dyn/9302005;chao-dyn,nlin.CD;0;0;;G.G.Szpiro;Cycles and Circles in Roundoff Errors
chao-dyn/9302006;chao-dyn,nlin.CD;0;2;;N.B.Tufillaro;Teardrop and heart orbits of a swinging Atwood's Machine
patt-sol/9302002;patt-sol,nlin.PS;0;0;;N.B.Tufillaro;Discrete Dynamical Models Showing Pattern Formation in Subaqueous Bedforms
hep-ph/9302291;hep-ph;0;33;;A.Stange,S.Willenbrock;Yukawa correction to top-quark production at the Tevatron
hep-ph/9302292;hep-ph,astro-ph;0;17;;A.D.Dolgov,I.Z.Rothstein;New Upper Limits on the Tau Neutrino Mass from Primordial Helium Considerations
hep-th/9302109;hep-th;1;24;hep-th/9205027;R.Kallosh,T.Ortin;Charge Quantization of Axion-Dilaton Black Holes
nucl-th/9302009;nucl-th;0;34;;G.E.Brown,J.Wambach;Model for the Quasifree Polarization-Transfer Measurements in the (p,n) reaction at 495 MeV
hep-ph/9302293;hep-ph;0;25;;S.Wycech,A.M.Green;The Production of the Exotic Atoms $π^+π^-$, $K^+π^-$ and $K^+K^-$
astro-ph/9302012;astro-ph;1;49;astro-ph/9207001;L.Moscardini,S.Borgani,P.Coles,F.Lucchin,S.Matarrese,A.Messina;Large--Scale Angular Correlations in CDM Models
hep-th/9302110;hep-th;10;91;hep-th/9109028,hep-th/9110015,hep-th/9201050,hep-th/9202060,hep-th/9209111,hep-th/9210134,hep-th/9211113,hep-th/9212016,hep-th/9212017,hep-th/9212117;C.M.Hull;Lectures on W-Gravity, W-Geometry and \W -Strings
astro-ph/9302013;astro-ph,hep-ph;5;58;hep-ph/9205212,astro-ph/9207001,hep-ph/9207239,hep-ph/9207245,astro-ph/9208007;M.S.Turner;On the Production of Scalar and Tensor Perturbations in Inflationary Models
hep-ph/9302294;hep-ph;0;0;;D.J.Summers;Calculation of the contributions to the signals and backgrounds for intermediate mass Higgs detection at the LHC and SSC from the q qbar initial state
nucl-th/9302010;nucl-th;0;14;;E.J.O.Gavin,H.Leeb,H.Fiedeldey;Determination of two-body potentials from n-body spectra
cond-mat/9302034;cond-mat;0;10;;F.W.J.Hekking,Yu.V.Nazarov;Subgap Conductivity of a Superconducting-Normal Tunnel Interface
hep-th/9302111;hep-th;0;0;;R.Caracciolo,M.A.R-Monteiro;Anyonic Realization of $SU_q(N)$ Quantum Algebra
cond-mat/9302035;cond-mat;0;15;;F.W.J.Hekking,Yu.V.Nazarov;Interference of two electrons entering a superconductor
alg-geom/9302005;alg-geom,math.AG;0;23;;C.LeBrun;A Finiteness Theorem for Quaternionic-Kaehler Manifolds with Positive Scalar Curvature
alg-geom/9302006;alg-geom,math.AG;0;54;;C.LeBrun,M.Singer;Existence and Deformation Theory for Scalar-Flat Kaehler Metrics on Compact Complex Surfaces
hep-th/9302112;hep-th,cond-mat,hep-lat;1;74;cond-mat/9207001;F.C.Alcaraz,M.Droz,M.Henkel,V.Rittenberg;Reaction-Diffusion Processes, Critical Dynamics and Quantum Chains
hep-ph/9302295;hep-ph;0;21;;M.Jeżabek,J.H.Kühn;The Top Width - Theoretical update
hep-th/9302113;hep-th,math.RA;0;6;;G.Dixon;Division algebras, Galois fields, quadratic residues
cond-mat/9302036;cond-mat;0;23;;D.Coffey,K.S.Bedell;Non-Analytic Contributions to the Self-Energy and the Thermodynamics of Two-Dimensional Fermi Liquids
gr-qc/9302033;gr-qc;0;0;;C.G.Torre,I.M.Anderson;Symmetries of the Einstein Equations
gr-qc/9302034;gr-qc;0;0;;M.C.Bento,O.Bertolami,P.V.Moniz,J.M.Mourao,P.M.Sá;On the Cosmology of Massive Vector Fields with SO(3) Global Symmetry
hep-ph/9302296;hep-ph;2;23;hep-ph/9203225,hep-ph/9209248;N.Kitazawa,T.Kurimoto;Unified Description of Hadrons and Heavy Hadron Decays
hep-ph/9302297;hep-ph;0;13;;K.A.Peterson,S.Godfrey;Constraints on Anomalous $WWγ$ Couplings From $eγ$ Collisions
astro-ph/9302014;astro-ph;0;0;;L.Danese,L.Toffolatti,A.Franceschini,J.M.Martin-Mirones,G.D.Zotti;Angular Correlations of the X-Ray Background and Clustering of Extragalactic X-Ray Sources
hep-ph/9302298;hep-ph,nucl-th;0;22;;V.L.Eletsky,B.L.Ioffe;On the current correlators in QCD at finite temperature
hep-ph/9302299;hep-ph;1;17;hep-ph/9206247;V.L.Eletsky,B.L.Ioffe;Estimates of $m_d - m_u$ and $\langle \bar dd\rangle - \langle \bar uu\rangle $ from QCD sum rules for $D$ and $D^∗$ isospin mass differences
hep-th/9302114;hep-th;0;0;;M.Freeman,P.West;The covariant scattering and cohomology of $W_3$ strings
hep-ph/9302300;hep-ph,nucl-th;0;28;;V.Eletsky,P.Ellis,J.Kapusta;Temperature Dependence of Electric and Magnetic Gluon Condensates
hep-th/9302115;hep-th;1;10;hep-th/9201067;D.Gepner;On RSOS models associated to Lie algebras and RCFT
astro-ph/9302015;astro-ph;1;61;astro-ph/9207001;P.Coles,L.Moscardini,F.Lucchin,S.Matarrese,A.Messina;Skewness as a Test of Non-Gaussian Primordial Density Fluctuations
hep-ph/9302301;hep-ph;1;30;hep-ph/9204215;A.Santamaria;Masses, Mixings, Yukawa Couplings and their Symmetries
nucl-th/9302011;nucl-th;0;32;;S.Drozdz,S.Nishizaki,J.Speth,J.Wambach;Modeling Complex Nuclear Spectra - Regularity versus Chaos
hep-ph/9302302;hep-ph;1;16;hep-ph/9205209;F.Cuypers,G.J.van Oldenborgh,R.Rückl;Supersymmetric Signals in $γγ$ Collisions
astro-ph/9302016;astro-ph;0;0;;S.Borgani,P.Coles,L.Moscardini,M.Plionis;Angular Distribution of Clustersin Skewed CDM Models
hep-th/9302116;hep-th;0;0;;O.Bergman,G.Lozano;Aharonov-Bohm Scattering, Contact Interactions and Scale Invariance
hep-th/9302117;hep-th;0;12;;K.Yee,M.Bander;Equations of Motion for Spinning Particles in External\\Electromagnetic and Gravitational Fields
hep-ph/9302303;hep-ph;1;29;hep-ph/9205233;E.Christova,M.Fabbrichesi;Testing Supersymmetry by Means of Time Reversal Invariance
nucl-th/9302012;nucl-th;0;0;;D.Seibert,T.Altherr;Pre-equilibrium dileptons look thermal
hep-ph/9302304;hep-ph;0;41;;Ll.Ametller,A.Bramon,E.Massó;The $π^0→e^+e^-$ and $η→μ^+ μ^-$ Decays Revisited
hep-ph/9302305;hep-ph;0;0;;M.A.G.Aivazis,W.-K.Tung,F.Olness;Next-to-Leading Order QCD Formulation of Deep Inelastic Scattering
hep-ph/9302306;hep-ph;2;223;hep-ph/9208249,hep-th/0509223;J.HUTH,M.MANGANO;QCD Tests in Proton-Antiproton Collisions
hep-ph/9302307;hep-ph;0;11;;E.Braaten,K.Cheung,T.C.Yuan;Z^0 Decay into Charmonium via Charm Quark Fragmentation
hep-th/9302118;hep-th,math.QA;0;0;;D.N.Yetter,L.Crane;We Are Not Stuck With Gluing
hep-th/9302119;hep-th;0;62;;W.-M.Zhang,A.Harindranath;Light-Front QCD: Role of Longitudinal Boundary Integrals
hep-th/9302120;hep-th;5;35;hep-th/9202092,hep-th/9205037,hep-th/9206078,hep-th/9206084,hep-th/9207118;A.Kostelecky,M.Perry;Condensates and Singularities in String Theory
hep-th/9302121;hep-th,cond-mat;0;0;;D.Wesolowski,Y.Hosotani,C.-L.Ho;Multiple Chern-Simons Fields on a Torus
nucl-th/9302013;nucl-th;0;22;;R.Schiavilla,R.B.Wiringa,J.Carlson;The Coulomb Sum and Proton-Proton Correlations in Few-Body Nuclei
hep-ph/9302308;hep-ph,hep-th;0;0;;G.Levin,C.-I.Tan;Heterotic Pomeron: A Unified Treatment of High Energy Hadronic Collisions in QCD
math/9302202;math.LO;0;0;;T.Jech,J.Witzany;Full Reflection at a Measurable Cardinal
astro-ph/9302017;astro-ph;0;33;;E.Cappellaro,M.Turatto,Benetti,D.Yu.Tsvetkov,O.S.Bartunov,I.N.Makarova;The Rate of Supernovae. II. the Selection Effects and the Frequencies Per Unit Blue Luminosity
funct-an/9302007;funct-an,math.OA;0;0;;V.G.Pestov;Operator spaces and residually finite-dimensional $C^∗$-algebras
cond-mat/9302037;cond-mat;0;0;;G.G.Batrouni,B.Larson,R.T.Scalettar,J.Tobochnik,J.Wang;Universal Conductivity in the Two dimensional Boson Hubbard Model
hep-th/9302122;hep-th;0;25;;O.Piguet,S.P.Sorella;On the finiteness of the BRS modulo-d cocycles
hep-th/9302123;hep-th;1;47;hep-th/9302122;O.Piguet,S.P.Sorella;Adler-Bardeen theorem and vanishing of the gauge beta function
hep-th/9302124;hep-th;0;0;;W.Eholzer,A.Honecker,R.Huebel;How Complete is the Classification of W-Symmetries ?
astro-ph/9302018;astro-ph;0;0;;A.Dar,A.Laor,A.Loeb;Constraints on the Cosmic Rays in the Small Magellanic Cloud
hep-ph/9302309;hep-ph;0;15;;S.Dawson,G.Valencia;$K_L \ra μ^±e^∓ν\overline ν$ as background to $K_L \ra μ^±e^∓$
hep-ph/9302310;hep-ph;2;54;hep-th/9201058,hep-ph/9205235;R.R.Parwani;Dimensionality of spacetime as a gauge-invariance parameter in Yang-Mills calculations
hep-ph/9302311;hep-ph;0;7;;K.Melnikov,O.Yakovlev;Top Near Threshold: All QCD Radiative Corrections are Trivial
hep-th/9302125;hep-th;2;23;hep-th/9112009,hep-th/9203062;H.Aratyn,L.A.Ferreira,J.F.Gomes,R.T.Medeiros,A.H.Zimerman;Generalized Miura Transformations, Two-Boson KP Hierarchies and their Reduction to KDV Hierarchies
nucl-th/9302014;nucl-th,hep-ph;0;31;;H.W.Fearing,G.I.Poulis,S.Scherer;Effective Hamiltonians with Relativistic Corrections I: The Foldy--Wouthuysen transformation versus the direct Pauli reduction
nucl-th/9302015;nucl-th,hep-ph;0;26;;S.Scherer,G.I.Poulis,H.W.Fearing;Effective Hamiltonians with Relativistic Corrections II: Application to Compton Scattering by a Proton
funct-an/9302008;funct-an,math.OA;0;0;;R.Brunetti,D.Guido,R.Longo;Modular Structure and Duality in Conformal Quantum Field Theory
hep-lat/9302008;hep-lat,cond-mat,q-bio.BM;4;41;hep-lat/9202001,hep-lat/9202004,hep-lat/9204001,hep-lat/9205018;U.H.E.Hansmann,Y.Okamoto;Prediction of Peptide Conformation by Multicanonical Algorithm: A New Approach to the Multiple-Minima Problem
comp-gas/9302002;comp-gas,nlin.CG;0;0;;J.Theiler,T.Lookman;Statistical error in a chord estimator of correlation dimension: the ``rule of five''
comp-gas/9302003;comp-gas,nlin.CG;0;0;;J.Theiler,P.S.Linsay,D.M.Rubin;Detecting Nonlinearity in Data with Long Coherence Times
math/9302203;math.LO;0;3;;J.Sharp;Combinatorics on Ideals and Axiom A
math/9302204;math.FA;0;0;;M.Girardi,W.B.Johnson;The Complete Continuity Property and Finite Dimensional Decompositions
math/9302205;math.FA;0;0;;N.T.Peck;Twisted sums and a problem of Klee
math/9302206;math.FA;0;14;;M.Junge;Comparing gaussian and Rademacher cotype for operators on the space of continous functions
math/9302207;math.FA;0;12;;M.Defant,M.Junge;How many vectors are needed to compute (p,q)-summing norms?
math/9302208;math.FA;0;0;;P.N.Dowling,C.J.Lennard;Every nonreflexive subspace of L_1[0,1] fails the fixed point property
math/9302209;math.FA;0;0;;R.R.Phelps;Lectures on maximal monotone operators
math/9302210;math.MG,math.FA;0;0;;C.Schütt;Random polytopes and affine surface area
math/9302211;math.FA;0;13;;J.M.Borwein,M.Fabian,J.Vanderwerff;Locally Lipschitz Functions and Bornological Derivatives
math/9302212;math.FA;0;0;;J.M.Borwein,J.Vanderwerff;Dual Kadec-Klee norms and the relationships between Wijsman, slice and Mosco convergence
math/9302213;math.FA;0;0;;N.T.Peck;A factorization constant for $l^n_p
math/9302214;math.FA;0;0;;U.Haagerup,G.Pisier;Bounded linear operators between C^*-algebras
math/9302215;math.FA;0;0;;G.Pisier;Projections from a von Neumann algebra onto a subalgebra
math/9302216;math.FA,math.SP;0;0;;Y.Latushkin,S.Montgomery-Smith;Lyapunov theorems for Banach spaces
hep-th/9302126;hep-th,gr-qc;15;31;hep-th/9108001,hep-th/9110053,hep-th/9110065,hep-th/9112070,hep-th/9204099,hep-th/9206006,hep-th/9206048,gr-qc/9209002,hep-th/9210119,hep-th/9210121,hep-th/9301047,hep-th/9302033,hep-th/9302037,hep-th/9302070,hep-th/9302083;G.T.Horowitz,D.L.Welch;Exact Three Dimensional Black Holes in String Theory
hep-th/9302127;hep-th;0;14;;J.Garcia-Bellido;Quantum Black Holes
hep-th/9302128;hep-th;0;0;;L.G.Zastavenko;On the problem of unboundedness from below of the spinor QED Hamiltonian
hep-th/9302129;hep-th;0;0;;M.I.Dobroliubov,D.Eliezer,I.I.Kogan,G.W.Semenoff,R.J.Szabo;The Spectrum of Topologically Massive Quantum Electrodynamics
hep-th/9302130;hep-th;1;32;hep-th/9210038;T.Fujiwara,T.Tabei,Y.Igarashi,K.Maeda,J.Kubo;Canonical treatment of two dimensional gravity as an anomalous gauge theory
hep-th/9302131;hep-th;0;9;;M.Natsuume;Natural Generalization of Bosonic String Amplitudes
hep-th/9302132;hep-th;4;30;hep-th/9111056,hep-th/9206070,hep-th/9209122,hep-th/9210038;T.Fujiwara,Y.Igarashi,J.Kubo;Unrecognizable Black Holes in Two Dimensions
hep-th/9302133;hep-th,hep-lat;0;18;;H.Kawai,N.Kawamoto,T.Mogami,Y.Watabiki;Transfer Matrix Formalism for Two-Dimensional Quantum Gravity and Fractal Structures of Space-time
hep-ph/9302312;hep-ph;1;21;hep-ph/9204214;N.Kitazawa;Non-oblique Correction in Extenden Technicolor Theory
hep-th/9302134;hep-th;1;28;hep-th/9201056;S.Penati,M.Pernici,D.Zanon;Solitons in Two--Dimensional Topological Field Theories
hep-th/9302135;hep-th,hep-lat;1;14;hep-th/9202047;D.Birmingham,M.Rakowski;Subdivision Invariant Models in Lattice Gauge Theory
cond-mat/9302038;cond-mat;0;43;;P.Fazekas,H.-Y.Kee;Multi-Channel Kondo Necklace
cond-mat/9302039;cond-mat;0;0;;H.Leschhorn;Interface Depinning in a Disordered Medium - Numerical Results
hep-ph/9302313;hep-ph;0;22;;J.Kunz,Y.Brihaye;Fermions in the background of the sphaleron barrier
hep-ph/9302314;hep-ph;0;0;;S.Braibant,Y.Brihaye,J.Kunz;Sphalerons at finite temperature
hep-th/9302136;hep-th;0;33;;S.P.Sorella;Algebraic characterization of the Wess-Zumino consistency conditions in gauge theories
gr-qc/9302035;gr-qc,hep-th;3;40;hep-th/9202037,hep-th/9205022,hep-th/9211030;D.Brill,K.-T.Pirk;A Pictorial History of Some Gravitational Instantons
hep-ph/9302315;hep-ph;1;23;hep-ph/9205233;E.Christova,M.Fabbrichesi;T Violation Induced by Supersymmetry in t\bar t and W^+W^- Physics
hep-ph/9302316;hep-ph;1;68;hep-ph/9203201;J.T.Peltoniemi,J.W.F.Valle;Reconciling Dark Matter, Solar and Atmospheric Neutrinos
hep-th/9302137;hep-th;0;0;;T.J.Allen,D.B.Crossley;Harmonic BRST Quantization of Systems with Irreducible Holomorphic Boson and Fermion Constraints
hep-th/9302138;hep-th,math.QA;0;6;;D.B.Uglov;The Lie algebra of sl(2)-valued automorphic functions on a torus
hep-th/9302139;hep-th,math.QA;0;5;;D.B.Uglov;The quantum bialgebra associated with the eight-vertex R-matrix
gr-qc/9302036;gr-qc;0;58;;L.P.Grishchuk;Quantum Effects In Cosmology
hep-ph/9302317;hep-ph;0;0;;R.Arnowitt,P.Nath;Cosmological Constraints and SU(5) Supergravity Grand Unification
gr-qc/9302037;gr-qc,hep-th;0;0;;M.Ferraris,M.Francaviglia,I.Volovich;A Model of Topological Affine Gravity in Two Dimensions
hep-ph/9302318;hep-ph;0;0;;P.Nath,R.Arnowitt;Predictions in SU(5) Supergravity Grand Unification with Proton Stability and Relic Density Constraints
hep-lat/9302009;hep-lat;0;15;;Y.Peng,R.W.Haymaker;SU(2) Flux Distributions on Finite Lattices
hep-lat/9302010;hep-lat;0;9;;V.Singh,D.Browne,R.W.Haymaker;Measurement of the penetration depth and coherence length in U(1) and SU(2) dual Abrikosov vortices
hep-lat/9302011;hep-lat;1;37;hep-lat/9205010;R.W.Haymaker,V.Singh,D.Browne,J.Wosiek;Vacuum structure of pure gauge theories on the lattice
nucl-th/9302016;nucl-th;0;0;;W.Bauer;Particle-particle correlations and the space-time structure of heavy ion collisions
hep-ph/9302319;hep-ph;3;96;hep-ph/9204203,hep-ph/9205201,hep-ph/9205209;S.Godfrey,K.A.Peterson;Single $W$ Boson Production in High Energy $eγ$ Collisions
hep-th/9302140;hep-th;0;15;;R.Koberle,A.Lima-Santos;Exact solution of the deformed biquadratic spin 1 hamiltonian
hep-th/9302141;hep-th,math.QA;0;0;;F.Akman;A characterization of the differential in semi-infinite cohomology
hep-ph/9302320;hep-ph,nucl-th;0;0;;S.Kumano;Tensor Structure Function b$_1$(x) For Spin-One Hadrons
hep-th/9302142;hep-th;0;9;;T.Hori,M.Kamata;Wave Functional of Quantum Black Holes in Two Dimensions
hep-th/9302143;hep-th;0;0;;W.Lerche;Chiral Rings in Topological (W-)Gravity
hep-th/9302144;hep-th,gr-qc;10;17;hep-th/9201061,hep-th/9201074,hep-th/9203054,hep-th/9205028,hep-th/9205069,hep-th/9206020,hep-th/9206070,hep-th/9207095,hep-th/9209012,hep-th/9307140;S.P.de Alwis;Two Dimensional Quantum Dilaton Gravity and the Positivity of Energy
hep-ph/9302321;hep-ph;0;0;;F.C.Adams;General Solutions for Tunneling of Scalar Fields with Quartic Potentials
hep-lat/9302012;hep-lat,hep-ph;0;8;;F.Butler,H.Chen,J.Sexton,A.Vaccarino,D.Weingarten;Meson Decay Constant Predictions of the Valence Approximation to Lattice QCD
hep-th/9303001;hep-th;1;21;hep-ph/9210210;A.L.Larsen,V.P.Frolov;Propagation of perturbations along strings
hep-th/9303002;hep-th;3;12;hep-th/9201074,hep-th/9203054,hep-th/9206070;U.H.Danielsson;Super Black Holes
hep-ph/9303201;hep-ph;0;0;;R.Casalbuoni,P.Chiappetta,A.Deandrea,S.D.Curtis,D.Dominici,R.Gatto;Vector Resonances from a Strong Electroweak Sector at Linear Colliders
nucl-th/9303001;nucl-th;0;36;;S.Kamerdzhiev,J.Speth,G.Tertychny,J.Wambach;M1 Resonances in Unstable Magic Nuclei
hep-th/9303003;hep-th,hep-ph;0;0;;D.Luest;Consistency and Phenomenology of Four-Dimensional Strings
cond-mat/9303001;cond-mat;0;40;;M.L.Plumer,A.Mailhot,A.Caillé;Magnetic-Field Induced First-Order Transition in the Frustrated XY Model on a Stacked Triangular Lattice
cond-mat/9303002;cond-mat;0;37;;C.S.Hellberg,E.J.Mele;Luttinger Liquid Instability in the One Dimensional t-J Model
gr-qc/9303001;gr-qc,astro-ph,hep-th;2;41;hep-th/9109048,hep-th/9112044;R.Brandenberger,V.Mukhanov,A.Sornborger;A Cosmological Theory without Singularities
cond-mat/9303003;cond-mat;0;0;;S.Mazumdar,F.Guo,D.Guo,K.-C.Ung,J.T.Gammel;Infinite Volume Extrapolations of Finite Cluster Calculations, ---How Correct are These?
astro-ph/9303001;astro-ph,gr-qc,hep-ph;1;41;astro-ph/9206005;A.Albrecht,P.Ferreira,M.Joyce,T.Prokopec;Inflation and squeezed quantum states
hep-th/9303004;hep-th;2;25;hep-th/9112075,hep-th/9202013;V.Spiridonov;Symmetries of the Self-Similar Potentials
hep-th/9303005;hep-th;1;17;hep-th/9112075;A.A.Andrianov,M.V.Ioffe,V.P.Spiridonov;Higher-Derivative Supersymmetry and the Witten Index
gr-qc/9303002;gr-qc,hep-th;0;7;;T.Dray,C.A.Manogue,R.W.Tucker;The Scalar Field Equation in the Presence of Signature Change
gr-qc/9303003;gr-qc,hep-th;0;0;;A.Burinskii;String-Like Structures in Complex Kerr Geometry
hep-ph/9303202;hep-ph;2;55;hep-ph/9206203,hep-ph/9211228;M.Carena,S.Pokorski,C.E.M.Wagner;On the Unification of Couplings in the Minimal Supersymmetric Standard Model
cond-mat/9303004;cond-mat;0;28;;Rudolf A.R"omer,B.Sutherland;Conformal Invariance in Periodic Quantum Chains
astro-ph/9303002;astro-ph;0;30;;S.E.Thorsett,Z.Arzoumanian,M.M.McKinnon,J.H.Taylor;The Masses of Two Binary Neutron Star Systems
hep-ph/9303203;hep-ph;0;0;;J.P.Ma,B.H.J.McKellar;CP Test in the W Pair Production via Photon Fusion at NLC
hep-th/9303006;hep-th;0;28;;H.Kawai,R.Nakayama;Quantum $R^2$ Gravity in Two Dimensions
hep-th/9303007;hep-th,gr-qc;0;0;;N.Kaloper;Miens of The Three Dimensional Black Hole
hep-th/9303008;hep-th;0;6;;V.I.Man'ko,G.Marmo,S.Solimeno,F.Zaccaria;Correlation functions of quantum q-oscillators
hep-ph/9303204;hep-ph;0;18;;B.Grządkowski;CP Violation in $t \bar t$ Production at $e^+ e^-$ Colliders
hep-th/9303009;hep-th;0;0;;P.Bantay;Algebraic Aspects of Orbifold Models
hep-th/9303010;hep-th;0;11;;C.-P.Sun;Dynamical Realizability for Quantum Measurement and Factorization of Evolution Operator
hep-ph/9303205;hep-ph;0;11;;E.Braaten,T.C.Yuan;Gluon Fragmentation into Heavy Quarkonium
hep-th/9303011;hep-th;3;26;hep-th/9201061,hep-th/9203054,hep-th/9203059;M.Schiffer;Is it possible to recover information from the black-hole radiation?
hep-ph/9303206;hep-ph;0;19;;J.Ellis,D.N.Schramm;Could a nearby supernova explosion have caused a mass extinction?
gr-qc/9303004;gr-qc,astro-ph,hep-th;0;0;;C.O.Lousto,N.Sanchez;The Quantization of the Spacetime Geometry Generated by Planckian Energy Particles
gr-qc/9303005;gr-qc;0;0;;C.Farina,J.Gamboa,A.J.Segui-Santonja;Motion and Trajectories of Particles Around Three-Dimensional Black Holes
gr-qc/9303006;gr-qc;0;0;;S.A.Hayward;General Laws of Black-Hole Dynamics
hep-th/9303012;hep-th;0;19;;J.J.M.Verbaarschot,I.Zahed;Spectral Density of the QCD Dirac Operator near Zero Virtuality
hep-th/9303013;hep-th,cond-mat;4;79;hep-th/9206034,hep-th/9211034,hep-th/9212094,hep-th/9212150;S.Dasmahapatra,R.Kedem,T.R.Klassen,B.M.McCoy,E.Melzer;Quasi-Particles, Conformal Field Theory, and $q$-Series
cond-mat/9303005;cond-mat;0;0;;J.Boronat,F.Dalfovo,F.Mazzanti,A.Polls;Dynamic Structure Function in 3he-4he Mixtures
gr-qc/9303007;gr-qc,hep-th;1;40;hep-th/0209014;M.Ferraris,M.Francaviglia,I.Volovich;The Universality of Einstein Equations
gr-qc/9303008;gr-qc;0;0;;D.N.Page;No Superluminal Expansion of the Universe
hep-ph/9303207;hep-ph;12;37;hep-ph/9203225,hep-ph/9205243,hep-ph/9207235,hep-ph/9208221,hep-ph/9208248,hep-ph/9209239,hep-ph/9209248,hep-ph/9209275,hep-ph/9211239,hep-ph/9211248,hep-ph/9301242,hep-ph/9302296;K.S.Gupta,M.A.Momen,J.Schechter,A.Subbaraman;Heavy Quark Solitons
hep-ph/9303208;hep-ph;1;23;hep-ph/9206241;P.Bialas,J.G.Koerner,K.Zalewski;Complete angular analysis of the decay cascade $B →D^{**}( →D^*(→D π) + π) + W(→l ν)$
hep-th/9303014;hep-th;0;0;;S.Hirano,Y.Kazama,Y.Satoh;Exact Operator Quantization of a Model of Two-Dimensional Dilaton Gravity
hep-th/9303015;hep-th;2;24;hep-th/9202039,hep-th/9205004;M.Kreuzer;Where are the Mirror Manifolds?
hep-ph/9303209;hep-ph;0;9;;G.Mangano,F.Sannino;A Mass Spectrum for Leptons and Quarks
hep-ph/9303210;hep-ph;0;26;;F.Buccella,F.Lombardi,G.Miele,P.Santorelli;Nonleptonic Cabibbo Favoured $B$-Decays and $CP$-Asymmetries for Charmed Final Hadron States in Isgur and Wise Theory
hep-ph/9303211;hep-ph;0;0;;Chr.V.Christov;Baryons as solitons in Effective Chiral Quark - Meson Theory
hep-ph/9303212;hep-ph;0;0;;Chr.V.Christov,K.Goeke;B=1 Soliton of the Nambu - Jona-Lasinio model in medium}
hep-ph/9303213;hep-ph;0;0;;Chr.V.Christov,E.R.Arriola,K.Goeke;Nucleon Properties and Restoration of Chiral Symmetry at Finite\nl Density and Temperature in an Effective Theory
gr-qc/9303009;gr-qc;0;0;;V.Tapia,A.L.Marrakchi,M.Cataldo;Conformal Fourth-Rank Gravity
hep-ph/9303214;hep-ph;0;48;;E.Laenen,S.Riemersma,J.Smith,W.L.van Neerven;$O(α_S)$ Corrections to the Photon Structure Functions $F^γ_2(x,Q^2)$ and $F_L^γ(x,Q^2)$
hep-th/9303016;hep-th;11;34;hep-th/9110053,hep-th/9112070,hep-th/9201040,hep-th/9206023,hep-th/9206051,hep-th/9210121,hep-th/9212089,hep-th/9301005,hep-th/9301042,hep-th/9301043,hep-th/9302033;A.Giveon,E.Kiritsis;Axial Vector Duality as a Gauge Symmetry and Topology Change in String Theory
hep-ph/9303215;hep-ph,astro-ph,hep-lat;0;0;;U.M.Heller,M.Klomfass,H.Neuberger,P.Vranas;Numerical analysis of the Higgs mass triviality bound
hep-th/9303017;hep-th;5;46;hep-th/9109053,hep-th/9202046,hep-th/9204030,hep-th/9205068,hep-th/9211027;P.Mayr,S.Stieberger;Threshold Corrections to Gauge Couplings in Orbifold Compactifications
hep-ph/9303216;hep-ph;0;5;;J.F.Gunion,T.C.Yuan,B.Grzadkowski;Gluon Fusion: A Probe of Higgs Sector CP Violation
hep-th/9303018;hep-th,math.QA;0;0;;P.Etingof;Representations of affine Lie algebras, elliptic r-matrix systems, and special functions
hep-th/9303019;hep-th;0;0;;V.Tapia;Integrable Conformal Field Theory in Four Dimensions and Fourth-Rank Geometry
hep-th/9303020;hep-th,gr-qc;1;23;hep-th/9202090;M.Visser;van Vleck determinants: geodesic focussing and defocussing in Lorentzian spacetimes
hep-ph/9303217;hep-ph;1;41;hep-ph/9204225;L.J.Hall;Towards a theory of quark and lepton masses
hep-th/9303021;hep-th;0;18;;O.K.Kalashnikov;Gauge Fields Condensation at Finite Temperature
hep-th/9303022;hep-th;0;0;;O.K.Kalashnikov;SU(2)-Effective Action Wiht the Nonanalytic Term
hep-th/9303023;hep-th,gr-qc;1;17;hep-th/9202090;M.Visser;Hawking's chronology protection conjecture: singularity structure of the quantum stress--energy tensor
hep-th/9303024;hep-th,hep-ph;0;21;;J.Garriga,M.Sakellariadou;Effects of friction on cosmic strings
hep-th/9303025;hep-th;0;0;;N.Berkovits;A New Sigma Model Action for the Four-Dimensional Green-Schwarz Heterotic Superstring
hep-ph/9303218;hep-ph;0;32;;J.M.Grandy,M.P.Mattis;Valley Bifurcation in an $O(3)$ $σ$ Model: Implications for High-Energy Baryon Number Violation
hep-ph/9303219;hep-ph;0;21;;C.Csáki,F.Csikor;Mirror fermions and LEP precision data
hep-lat/9303001;hep-lat;1;40;hep-lat/9206026;M.Goeckeler,R.Horsley,P.E.L.Rakow,G.Schierholz;Is the Chiral Phase Transition in Non-Compact Lattice QED Driven by Monopole Condensation?
hep-ph/9303220;hep-ph;0;0;;P.Colangelo,G.Nardulli,N.Paver;QCD Sum Rules and B Decays
hep-ph/9303221;hep-ph;0;30;;A.Abada,H.Merabet;The Breathing Mode in Extended Skyrme Model
cond-mat/9303006;cond-mat;1;29;0910.4576;A.Abada,D.Vautherin;Two-Phonon States in Alkali-Metal Clusters
hep-lat/9303002;hep-lat;0;0;;G.Bhanot,M.Creutz,I.H.J.Lacki,J.Weckel;Series expansions without diagrams
hep-ph/9303222;hep-ph;0;38;;G.Nardulli;Theory Review of CP Violations in B Decays at Hadron Colliders
hep-ph/9303223;hep-ph;0;14;;A.K.Likhoded,S.R.Slabospitsky,M.Mangano,G.Nardulli;$B_c$ Physics at Hadron Colliders
hep-ph/9303224;hep-ph;0;13;;W.Kilian,T.Mannel,T.Ohl;Unimagined Imaginary Parts in Heavy Quark Effective Field Theory
gr-qc/9303010;gr-qc;1;38;hep-th/9202054;C.D.Bartolo,R.Gambini,J.Griego;The Extended Loop Group: An Infinite Dimensional Manifold Associated with the Loop Space
nucl-th/9303002;nucl-th;0;0;;G.Bathas,W.M.Kloet;Generalized $^3P_0$ and $^3S_1$ Annihilation Potentials for $\bar pp$ Decay into Two Mesons based on a Simple Quark Model
hep-th/9303026;hep-th,math.QA;1;16;hep-th/9110066;A.S.Gorsky,A.V.Zabrodin;Degenerations of Sklyanin algebra and Askey-Wilson polynomials
hep-th/9303027;hep-th;0;26;;F.D.Jonghe;Schwinger-Dyson BRST-Symmetry and the Equivalence of Hamiltonian and Lagrangian Quantistion
hep-th/9303028;hep-th,math.DG;0;47;;G.Cognola,L.Vanzo;The trace of the heat kernel on a compact hyperbolic 3-orbifold
hep-th/9303029;hep-th,gr-qc;4;18;hep-th/9112065,hep-th/9201059,hep-th/9203057,hep-th/9204046;M.Visser;Dirty black holes: Entropy versus area
hep-th/9303030;hep-th,cond-mat;2;34;hep-th/9202012,hep-th/9209003;A.Cappelli,C.A.Trugenberger,G.R.Zemba;Large N Limit in the Quantum Hall Effect
hep-th/9303031;hep-th;2;6;hep-th/9206095,hep-th/9208002;J.M.Cline,S.Paban;Is Induced QCD really QCD? The preservation of asymptotic freedom by matter interactions
hep-th/9303032;hep-th;9;17;hep-th/9109038,hep-th/9110065,hep-th/9112070,hep-th/9201015,hep-th/9204011,hep-th/9204099,hep-th/9205078,hep-th/9205095,hep-th/9206051;A.Ali,A.Kumar;$O(\tilde d,\tilde d)$ Transformations and 3D Black Hole
hep-ph/9303225;hep-ph;2;157;hep-ph/9206205,hep-ph/9207222;L.Littenberg,G.Valencia;Rare and Radiative Kaon Decays
math/9303201;math.FA;0;0;;C.P.Stegall;Spaces Of Lipschitz Functions On Banach Spaces
comp-gas/9303001;comp-gas,nlin.CG;0;22;;D.Grunau,S.Chen,K.Egger;A Lattice Boltzmann Model for Multi-phase Fluid Flows
chao-dyn/9303001;chao-dyn,nlin.CD;0;11;;S.Chen,G.Doolen,J.R.Herring,R.H.Kraichnan,S.A.Orszag,Z.S.She;Far Dissipation Range of Turbulence
hep-th/9303033;hep-th;0;0;;H.Nishino;Self-Dual Supersymmetric Yang-Mills Theory Generates Witten's Topological Field Theory
nucl-th/9303003;nucl-th;1;32;nucl-th/9211004;B.Q.Chen,P.Vogel;Atomic parity nonconservation and neutron radii in cesium isotopes
alg-geom/9303001;alg-geom,math.AG;0;0;;Y.Kawamata;Semistable Minimal Models of Threefolds in Positive or Mixed Characteristic
nucl-th/9303004;nucl-th,hep-ph;0;47;;T.S.Biro,E.van Doorn,B.Mueller,M.H.Thoma,X.N.Wang;Parton Equilibration in Relativistic Heavy Ion Collisions
hep-ph/9303226;hep-ph;4;33;hep-ph/9301259,hep-ph/9301265,hep-ph/9303204,hep-ph/9307232;D.Chang,W.-Y.Keung,I.Phillips;CP--odd Correlation in the Decay of Neutral Higgs Boson into $ZZ$, $W^+W^-$, or $t{\bar t}$
hep-th/9303034;hep-th,math.QA;0;0;;F.M.Moras,J.Mas,E.Ramos;Diffeomorphisms from higher dimensional W-algebras
cond-mat/9303007;cond-mat;0;19;;J.Gonzalez,F.Guinea,M.A.H.Vozmediano;Electrostatic screening in fullerene molecules
cond-mat/9303008;cond-mat;0;17;;M.Bernasconi,G.L.Chiarotti,E.Tosatti;The (001) surface of alpha-Ga is covered with GaIII
hep-th/9303035;hep-th,math.QA;0;10;;C.Burdik,P.Hellinger;Quantum-double for a nonstandard deformation of a Borel subalgebra $sl(2,C)$
hep-th/9303036;hep-th,math.DG;0;0;;M.Furuta,M.A.Guest,M.Kotani,Y.Ohnita;On the fundamental group of the space of harmonic $2$-spheres in the $n$-sphere
hep-th/9303037;hep-th,math.DG;0;0;;M.A.Guest,Y.Ohnita;Group actions and deformations for harmonic maps
hep-th/9303038;hep-th,math.SG;0;13;;A.Yu.Alekseev,A.Z.Malkin;Symplectic structures associated to Lie-Poisson groups
gr-qc/9303011;gr-qc;0;0;;P.Tuckey;The Construction of Sorkin Triangulations
hep-th/9303039;hep-th;0;0;;G.Dixon;Division Algebras, (1,9)-Space-Time, Matter-Antimatter Mixing
adap-org/9303001;adap-org,nlin.AO;0;9;;R.Schack;The length of a typical Huffman codeword
chao-dyn/9303002;chao-dyn,nlin.CD;0;25;;R.Schack,C.M.Caves;Hypersensitivity to Perturbations in the Quantum Baker's Map
hep-ph/9303227;hep-ph;3;54;nucl-th/9211009,hep-ph/9211329,hep-ph/9212287;A.M.H.Mishra,S.P.Misra;Gluon Condensates at Finite Baryon Densities and Temperature
cond-mat/9303009;cond-mat;0;0;;V.Privman,C.R.Doering,H.L.Frisch;Crossover from Rate-Equation to Diffusion-Controlled Kinetics in Two-Particle Coagulation
hep-ph/9303228;hep-ph;0;22;;O.V.Teryaev;The Emc Spin Crisis: Comparing Proton and Photon
adap-org/9303002;adap-org,nlin.AO,q-bio.PE;0;16;;K.Kaneko,J.Suzuki;Evolution to the Edge of Chaos in Imitation Game
cond-mat/9303010;cond-mat;0;66;;M.Yamanaka,Y.Hatsugai,M.Kohmoto;Phase diagram of the S=1/2 quantum spin chain with bond alternation
hep-th/9303040;hep-th,hep-ph;0;37;;V.Kaplunovsky,J.Louis;Model-Independent Analysis of Soft Terms in Effective Supergravity and in String Theory
cond-mat/9303011;cond-mat;0;36;;A.J.Bray,A.D.Rutenberg;Growth Laws for Phase Ordering
hep-th/9303041;hep-th,gr-qc,hep-lat;1;23;hep-lat/9204004;J.Ambjorn,S.Jain,J.Jurkiewicz,C.F.Kristjansen;Observing 4D Baby Universes in Quantum Gravity
hep-th/9303042;hep-th,gr-qc,hep-lat;4;33;hep-lat/9204002,hep-lat/9204003,hep-lat/9204004,hep-lat/9205009;J.Ambjorn,Z.Burda,J.Jurkiewicz,C.F.Kristjansen;4D Quantum Gravity Coupled to Matter
hep-th/9303043;hep-th,cond-mat;0;0;;H.J.de Vega,L.Mezincescu,R.I.Nepomechie;Thermodynamics of Integrable Chains with Alternating Spins
nucl-th/9303005;nucl-th;0;22;;J.Piekarewicz;Off-shell Behavior of the $π\!-\!η$ Mixing Amplitude
hep-th/9303044;hep-th;0;0;;J.I.Latorre,C.Manuel,X.Vilasis-Cardona;Systematic Differential Renormalization to All Orders
hep-ph/9303229;hep-ph;0;0;;J.N.Bahcall,P.Kumar;g-modes and the Solar Neutrino Problem
hep-th/9303045;hep-th,nlin.SI,solv-int;3;30;hep-th/9208058,hep-th/9209006,hep-th/9210037;R.Paunov;W-infinity structure of the $sl(N)$ conformal affine Toda theories
hep-th/9303046;hep-th,hep-ph;0;30;;D.J.Gross,W.Taylor;Twists and Wilson Loops in the String Theory of Two Dimensional QCD
hep-ph/9303230;hep-ph;3;22;hep-th/9202046,hep-th/9205011,hep-ph/9205227;M.Dine,A.E.Nelson;Dynamical Supersymmetry Breaking at Low Energies
astro-ph/9303003;astro-ph,hep-lat;0;36;;P.Hut;Blue Stragglers as Tracers of Globular Cluster Evolution
gr-qc/9303012;gr-qc,astro-ph,hep-th;0;0;;J.D.Brown,J.W.York;Microcanonical Action and the Entropy of a Rotating Black Hole
cond-mat/9303012;cond-mat;1;17;cond-mat/9205014;K.Harigaya;Polaron excitations in doped C60: Effects of disorders
cond-mat/9303013;cond-mat;0;20;;G.Chu,J.V.Jose;Giant Shapiro Resonances in a Flux Driven Josephson Junction Necklace
hep-ph/9303231;hep-ph;4;42;hep-ph/9203223,hep-ph/9207212,hep-ph/9207219,hep-ph/9211228;J.Lopez,D.Nanopoulos,H.Pois,X.Wang,A.Zichichi;Sparticle and Higgs Production and Detection at LEPII in two Supergravity Models
hep-th/9303047;hep-th,math.QA;0;0;;P.Etingof,I.B.Frenkel;Central extensions of current groups in two dimensions
hep-th/9303048;hep-th,gr-qc,hep-lat;0;0;;M.Srednicki;Entropy and Area
hep-th/9303049;hep-th;0;4;;T.Hori;Exact Solutions to the Wheeler-DeWitt Equation of Two Dimensional Dilaton Gravity
hep-th/9303050;hep-th;6;14;hep-th/9209046,hep-th/9212010,hep-th/9212015,hep-th/9212019,hep-th/9212021,hep-th/9212145;B.K.Chung,S.Nam,Q.-H.Park,H.J.Shin;Conformal Turbulence with Boundary
hep-lat/9303003;hep-lat,hep-th;0;27;;P.Cea,L.Cosmai;Unstable Modes in Three-Dimensional SU(2) Gauge Theory
hep-ph/9303232;hep-ph;1;76;hep-ph/9210249;R.Guida,K.Konishi;Fermions in Instanton Anti-Instanton Background
astro-ph/9303004;astro-ph;0;0;;M.Umemura,A.Loeb,E.L.Turner;Early Cosmic Formation of Massive Black Holes
hep-th/9303051;hep-th;3;33;hep-th/9201050,hep-th/9207067,hep-th/9209037;E.Bergshoeff,H.J.Boonstra,M.de Roo,S.Panda,A.Sevrin;On the BRST Operator of $W$-Strings
hep-lat/9303004;hep-lat;1;22;hep-lat/9205012;S.A.Frolov,A.A.Slavnov;Removing fermion doublers in chiral gauge theories on the lattice
cond-mat/9303014;cond-mat;1;105;cond-mat/9204001;S.Sachdev;Quantum Antiferromagnets in Two Dimensions
hep-ph/9303233;hep-ph;0;53;;P.N.Maher,L.Durand,K.Riesselmann;Two-loop renormalization constants and high energy $2→2$ scattering amplitudes in the Higgs sector of the standard model
cond-mat/9303015;cond-mat;0;22;;L.Balents,M.Kardar;Delocalization of Flux Lines from Extended Defects by Bulk Randomness
hep-ph/9303234;hep-ph;0;38;;L.Durand,P.N.Maher,K.Riesselmann;Two-loop unitarity constraints on the Higgs boson coupling
hep-ph/9303235;hep-ph;0;23;;K.Langfeld,L.v.Smekal,H.Reinhardt;The Non-Trivial Phase of $\PHI ^4$-Theory in a Renormalisation Group Invariant Approach
hep-th/9303052;hep-th,nlin.SI,solv-int;3;24;hep-th/9108007,hep-th/9203065,hep-th/9204064;C.Destri,H.J.de Vega;Yang--Baxter symmetry in integrable models: new light from the Bethe Ansatz solution
hep-th/9303053;hep-th,hep-ph;0;83;;A.R.White;Analytic Multi-Regge Theory and the Pomeron in QCD : II. Gauge Theory Analysis
gr-qc/9303013;gr-qc;0;0;;J.-paul.Berthias,B.Shahid-Saless;Torsion and Nonmetricity in Scalar-Tensor Theories of Gravity
comp-gas/9303002;comp-gas,nlin.CG;0;0;;D.M.Beazley,P.S.Lomdahl;Message-Passing Multi-Cell Molecular Dynamics on the Connection Machine 5
cond-mat/9303016;cond-mat;0;28;;M.C.Martin,D.Koller,L.Mihaly;In-Situ Infrared Transmission Study of Rb- and K-Doped Fullerenes
cond-mat/9303017;cond-mat;0;33;;A.Mailhot,M.L.Plumer,A.Caillé;Histogram Monte Carlo study of multicritical behavior in the hexagonal easy-axis Heisenberg antiferromagnet
hep-th/9303054;hep-th;0;0;;A.A.Tseytlin;Two-dimensional conformal sigma models and exact string solutions
hep-th/9303055;hep-th;0;0;;J.Kiskis,R.Narayanan,P.Vranas;The Hausdorff dimension of random walks and the correlation length critical exponent in Euclidean field theory
hep-ph/9303236;hep-ph;0;16;;A.Aeppli,F.Cuypers,G.J.van Oldenborgh;$\order (Γ)$ Corrections to $W$ pair production in $e^+e^-$ and $γγ$ collisions
hep-ph/9303237;hep-ph;0;0;;V.D.Duca,M.E.Peskin,W.-K.Tang;Computation of Mini-Jet Inclusive Cross Sections
hep-th/9303056;hep-th,hep-lat;0;28;;G.W.Semenoff,N.Weiss;Symmetry and Observables in Induced QCD
cond-mat/9303018;cond-mat;0;0;;F.Liu,H.Metiu;Dynamics of Phase Separation of Crystal Surfaces
hep-th/9303057;hep-th;0;0;;A.Sen;Magnetic Monopoles, Bogomol'nyi Bound and SL(2,Z) Invariance in String Theory
hep-th/9303058;hep-th;0;16;;A.Sevrin,P.van Nieuwenhuizen;Quantum gauging from classical gauging of nonlinear algebras
cond-mat/9303019;cond-mat,hep-th;0;15;;K.-H.Kwon,D.Kim;Honeycomb lattice solvable models
cond-mat/9303020;cond-mat;0;0;;R.S.Markiewicz;Van Hove Excitons and High-T$_c$ Superconductivity: VIIIC Dynamic Jahn-Teller Effects vs Spin-Orbit Coupling in the LTO Phase of La$_{2-x}$Sr$_x$CuO$_4$
cond-mat/9303021;cond-mat;0;0;;R.S.Markiewicz;Van Hove Exciton-Cageons and High-T$_c$ Superconductivity: VIIID Solitons and Nonlinear Dynamics
hep-th/9303059;hep-th,gr-qc;0;0;;N.Kaloper;Exact Primordial Black Strings in Four Dimensions
hep-th/9303060;hep-th;1;24;hep-th/9208024;A.E.Faraggi,E.Halyo;Neutrino Masses in Superstring Derived Standard--like Models
hep-lat/9303005;hep-lat,hep-ph;0;0;;Y.Shamir;Chiral Fermions from Lattice Boundaries
hep-th/9303061;hep-th;0;44;;A.Bytsenko,K.Kirsten,S.Odintsov;Self-interacting scalar fields on spacetime with compact hyperbolic spatial part
hep-th/9303062;hep-th;0;0;;P.Renaud;The Energy-Momentum Tensor in Fulling-Rindler Vacuum
hep-th/9303063;hep-th;0;11;;C.Bachas;Schwinger Effect in String Theory
hep-th/9303064;hep-th;1;39;hep-th/9206009;E.Aldrovandi,L.Bonora;Liouville and Toda field theories on Riemann surfaces
hep-th/9303065;hep-th;0;10;;E.Alvarez,J.Cespedes,E.Verdaguer;Quantum properties of the polytopic action in some simple geometries
hep-th/9303066;hep-th,math.QA;0;0;;P.Etingof;Quantum Knizhnik-Zamolodchikov equations and holomorphic vector bundles
gr-qc/9303014;gr-qc;0;0;;I.Racz;Maxwell Fields in Spacetimes Admitting Non-Null Killing Vectors
hep-th/9303067;hep-th;1;5;hep-th/9208027;K.Li,E.Witten;Role of Short Distance Behavior in Off-Shell Open-String Field Theory
hep-ph/9303238;hep-ph;0;0;;H.Nadeau,D.London;Leptoquarks at $eγ$ Colliders
astro-ph/9303005;astro-ph,hep-ph;1;9;hep-ph/9207256;A.T.Sornborger;A Semi-Analytical Analysis of Texture Collapse
nucl-th/9303006;nucl-th;0;40;;N.N.Nikolaev,A.Szczurek,J.Speth,J.Wambach,B.G.Zakhorov,V.R.Zoller;The Onset of Color Transparency in $(e,e'p)$ Reactions on Nuclei