LEADER 01195nam--2200385---450- 001 990002912410203316 005 20070427130048.0 010 $a90-420-0880-6 035 $a000291241 035 $aUSA01000291241 035 $a(ALEPH)000291241USA01 035 $a000291241 100 $a20070427d2004----km-y0itay0103----ba 101 $aeng 102 $aNL 105 $a||||||||001yy 200 1 $aAfrican diasporas in the New and Old Worlds$econsciousness and imagination$fedited by Genevičve Fabre and Klaus Benesch 210 $aAmsterdam$aNew York$cRodopi$d2004 215 $aXXI, 358 p.$d23 cm 225 2 $aCross cultures$v69 410 $12001$aCross cultures$v69 606 0 $aLetteratura africana$xSaggi 676 $a896 702 1$aFABRE,$bGenevičve 702 1$aBENESCH,$bKlaus 801 0$aIT$bsalbc$gISBD 912 $a990002912410203316 951 $aVIII.2.B. 34$b191856 L.M.$cVIII.2.$d00122359 959 $aBK 969 $aUMA 979 $aVITALE$b90$c20070427$lUSA01$h1259 979 $aVITALE$b90$c20070427$lUSA01$h1300 979 $aVITALE$b90$c20070427$lUSA01$h1300 996 $aAfrican diasporas in the New and Old Worlds$9988622 997 $aUNISA LEADER 00800nam0-22002771i-450 001 990005436550203316 005 20210402123430.0 035 $a000543655 035 $aUSA01000543655 035 $a(ALEPH)000543655USA01 100 $a20010829d1984----km y1itay5003----ba 101 0 $aita 102 $aIT 200 1 $aBilancia dei pagamenti e sistema monetario internazionale$fGiuseppe Mauro 210 $aTorino$cGiappichelli$d1984 215 $a369 p.$d21 cm 606 0 $aBilancia commerciale$2BNCF 676 $a382.17 700 1$aMAURO,$bGiuseppe$0354142 801 0$aIT$bSOL$c20120104 912 $a990005436550203316 951 $a300 382.17 MAU$b1923 DISES 959 $aBK 969 $aDISES 996 $aBilancia dei pagamenti e sistema monetario internazionale$9195167 997 $aUNISA LEADER 05532nam 2200661 450 001 9910453251603321 005 20200520144314.0 010 $a981-4520-72-1 035 $a(CKB)2550000001160091 035 $a(EBL)1561238 035 $a(OCoLC)860388739 035 $a(SSID)ssj0001163052 035 $a(PQKBManifestationID)11652053 035 $a(PQKBTitleCode)TC0001163052 035 $a(PQKBWorkID)11141625 035 $a(PQKB)10829597 035 $a(MiAaPQ)EBC1561238 035 $a(WSP)00008875 035 $a(Au-PeEL)EBL1561238 035 $a(CaPaEBR)ebr10801048 035 $a(CaONFJC)MIL543296 035 $a(EXLCZ)992550000001160091 100 $a20131202h20142014 uy| 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 00$aLuttinger model $ethe first 50 years and some new directions /$fedited by Vieri Mastropietro, University of Milan, Italy, Daniel Charles Mattis, University of Utah, USA 210 1$aNew Jersey :$cWorld Scientific,$d[2014] 210 4$d©2014 215 $a1 online resource (312 p.) 225 1 $aSeries on directions in condensed matter physics,$x1793-1444 ;$vvolume 20 300 $aDescription based upon print version of record. 311 $a981-4520-71-3 311 $a1-306-12045-4 320 $aIncludes bibliographical references. 327 $aCONTENTS; Preface Vieri Mastropietro; Introduction Daniel C. Mattis; Chapter I:. The Luttinger Model and Its Solution; An Exactly Soluble Model of a Many-Fermion System Joaquin M. Luttinger; I. INTRODUCTION; II. EXACT SOLUTION OF THE MODEL; III. EXPLICIT EVALUATION OF MOMENTUM DISTRIBUTION; IV. COMPARISON WITH PERTURBATION THEORY; V. RESPONSE TO EXTERNAL FIELDS; APPENDIX; ACKNOWLEDGMENTS; Exact Solution of a Many-Fermion System and Its Associated Boson Field Daniel C. Mattis and Elliott H. Lieb; I. INTRODUCTION; II. MODEL HAMILTONIAN; III. CASE OF THE FILLED DIRAC SEA 327 $aIV. SOLUTIONS OF THE MODEL HAMllTONIANV. EVALUATION OF THE MOMENTUM DISTRIBUTION; VI. DIELECTRIC CONSTANT; APPENDIX; ACKNOWLEDGMENTS; Chapter II: Lattice, Dynamical and Nonlinear Effects; Luttinger Model and Luttinger Liquids Vieri Mastropietro; 1. Introduction; 2. The Luttinger Model Exact Solution; 3. Nonsolvable Lattice Models and the Luttinger Liquid Conjecture; 4. Exact Renormalization Group Analysis; 5. Emerging Symmetries and Vanishing of Beta Function; 6. Ward Identities and Anomalies; 7. Proof of the Luttinger Liquid Relations in Nonsolvable Models; 8. Conclusions; References 327 $aThe Luttinger Liquid and Integrable Models Jesko Sirker1. Introduction; 2. Quantum Integrability; 2.1. Consequences for transport; 2.2. Consequences for thermalization in closed systems; 3. Low-Energy Description of the XXZ Model; 3.1. Irrelevant operators in the finite field case; 3.2. Irrelevant operators for zero field; 4. The Bethe Ansatz Solution; 5. Fixing Parameters of the Luttinger Model Using Integrability; 5.1. Velocity and Luttinger liquid parameter; 5.2. Coupling constants of irrelevant operators; 5.2.1. The zero field case; 5.2.2. The finite field case; 6. Applications 327 $a6.1. Impurities, Friedel oscillations and nuclear magnetic resonance6.2. The spin-lattice relaxation rate and transport; 7. Conclusions; Acknowledgments; References; Long Time Correlations of Nonlinear Luttinger Liquids Rodrigo G. Pereira; 1. Introduction; 2. Breakdown of LL Theory by Band Curvature Effects; 3. High Energy Contributions to Time-Dependent Correlation Functions; 4. Long Time Decay at Finite Temperatures; 5. Conclusion and Outlook; Acknowledgments; References; An Expanded Luttinger Model Daniel C. Mattis; 1. Introduction; 2. Review of the (Original) Dispersionless Model 327 $a3. Neglect of Exchange Terms4. Important Features of the Original Luttinger Model; 5. Dispersion: The New Feature; 6. Notation; 7. Equations of Motion in the Generalized Model; 8. Eigenvalue Equation at Long Wavelengths; 9. Attractive Versus Repulsive Forces; 10. Conclusion; Appendix A; References; Chapter III: Applications and Experimental Test; Quantum Hall Edge Physics and Its One-Dimensional Luttinger Liquid Description Orion Ciftja; 1. Introduction; 2. Luttinger Liquid and Bosonization; 3. Quantum Hall Effect and the Laughlin States 327 $a4. Luttinger Liquid Description of Quantum Hall Edge States 330 $aThe Luttinger Model is the only model of many-fermion physics with legitimate claims to be both exactly and completely solvable. In several respects it plays the same role in many-body theory as does the 2D Ising model in statistical physics. Interest in the Luttinger model has increased steadily ever since its introduction half a century ago. 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