QCD as a Theory of Hadrons: From Partons to Confinement (Cambridge Monographs on Particle Physics, Nuclear Physics and Cosmology, Series Number 17)
معرفی کتاب «QCD as a Theory of Hadrons: From Partons to Confinement (Cambridge Monographs on Particle Physics, Nuclear Physics and Cosmology, Series Number 17)» نوشتهٔ Narison S., Ericson T., Landshoff P.Y. (eds.)، منتشرشده توسط نشر Cambridge University Press (Virtual Publishing) در سال 2004. این کتاب در 20 صفحه، فرمت pdf، زبان انگلیسی ارائه شده است.
Half-title......Page 2 Series-title......Page 3 Title......Page 4 Copyright......Page 5 Dedication......Page 6 Contents......Page 8 About Stephan Narison......Page 26 Outline of the book......Page 28 Preface......Page 30 Acknowledgements......Page 33 Part I General introduction......Page 34 1 A short flash on particle physics......Page 36 2.1 The quark model......Page 43 2.2.2 Currents and charges......Page 46 2.2.3 Chiral symmetry and pion PCAC......Page 48 2.2.4 Soft pion theorem and the Goldberger–Treiman relation......Page 49 2.2.5 The Adler–Weisberger sum rule and soft pion theorems......Page 50 2.2.6 Soft pion theorem for ... and the KSFR relation......Page 52 2.2.7 Weinberg current algebra sum rules......Page 54 Electromagnetic current......Page 55 Charged current......Page 56 2.3 Parton model and Bjorken scaling......Page 57 2.4.2 The Veneziano model and duality......Page 60 2.4.3 Duality diagrams......Page 61 3.1 QCD and the notion of quarks......Page 64 3.2 The notion of colours......Page 66 3.4 Indirect evidence of quarks......Page 67 3.5 Evidence for colours......Page 68 3.6 The SU(3) colour group......Page 70 3.7 Asymptotic freedom......Page 71 3.8 Quantum mechanics and non-relativistic aspects of QCD......Page 72 4.1 Wick's theorem......Page 73 4.2 Time-ordered product......Page 74 4.3.2 Applications: cross-section and decay rate......Page 75 4.4 Reduction formula......Page 77 4.5.1 Transition matrix of quantum mechanics in one dimension......Page 78 4.5.2 The Green's functions......Page 81 4.6.1 Scalar field quantization......Page 83 4.6.2 Application to...theory......Page 84 4.6.4 Gauge field quantization......Page 86 Part II QCD gauge theory......Page 88 5.1 Introduction......Page 90 5.3 The QED Lagrangian as a prototype......Page 91 5.4 The QCD Lagrangian......Page 93 5.5 Local invariance and BRST transformation......Page 94 6.1 Path integral technique for QCD......Page 96 6.2.1 Free-field propagators......Page 98 6.2.2 Vertices......Page 99 6.4 Qualitative feature of quantization......Page 101 7.1 U(1) global invariance......Page 103 7.2 SU(n)L × SU(n)R global chiral symmetry......Page 104 Part III MS scheme for QCD and QED......Page 106 Introduction......Page 107 8.1.2 Analytic regularization......Page 109 8.2.1 Naïve dimensional regularization......Page 110 8.2.3 't Hooft-Veltman regularization......Page 111 8.2.4 Momentum integrals in n dimensions......Page 112 8.2.5 Example of the pseudoscalar two-point correlator......Page 114 9.1 Renormalizability and power counting rules......Page 117 9.3 Dimensional renormalization......Page 119 9.4 Renormalization constants......Page 120 9.5 Check of the renormalizability of QCD......Page 122 10.1 Outline of the background field approach......Page 124 10.3 Renormalization of composite operators......Page 126 10.3.2 Renormalization of G G......Page 127 10.3.3 Renormalization of the axial anomaly......Page 129 10.3.4 Renormalizations of higher-dimension operators......Page 130 11 The renormalization group......Page 131 11.2 The Beta function and the mass anomalous dimension......Page 132 11.3 Gauge invariance of β(α) and γm in the MS scheme......Page 134 11.4 Solutions of the RGE......Page 135 11.6 The RGE for the two-point function in the MS scheme......Page 137 11.7.1 Lowest order expression and the definition of the QCD scale A......Page 139 11.7.2 Renormalization group invariance of the first two coefficients of Β......Page 140 11.7.3 Higher order expression......Page 141 11.9 Input values of α and matching conditions......Page 142 11.10 Running gauge......Page 143 11.11 Running masses......Page 144 11.12 The perturbative pole mass......Page 145 11.12.1 The b and c pole mass difference......Page 150 11.14 MS scheme and RGE for the pseudoscalar two-point correlator......Page 151 11.14.1 Lowest order perturbative calculation......Page 152 11.14.2 Two-loop perturbative calculation in the MS scheme......Page 153 12.1 The MS scheme......Page 156 12.2 The momentum subtraction scheme......Page 157 12.4 The BLM scheme......Page 158 12.5 The PMS optimization scheme......Page 160 12.6 The effective charge scheme......Page 162 13.2 Renormalization constants and RGE......Page 164 13.4 Effective charge and link between the MS and on-shell scheme......Page 165 14.1.1 The electron anomaly and measurement of fine structure constant Alpha......Page 168 14.1.2 The muon anomaly and the rôle of the hadronic contributions......Page 169 14.1.3 The lowest order hadronic contributions......Page 170 14.1.4 The higher order hadronic contributions......Page 174 14.1.5 The total theoretical contributions to a......Page 176 14.2.1 Lowest order hadronic contributions......Page 177 14.2.2 QED running coupling Alpha(MZ)......Page 178 14.2.3 Muonium hyperfine splitting......Page 179 14.3 Conclusions......Page 181 Part IV Deep inelastic scatterings at hadron colliders......Page 182 15.1 Introduction......Page 184 15.2 The OPE for free fields at short distance......Page 185 15.3 Application of the OPE for free fields: parton model and Bjorken scaling......Page 186 15.4 Light-cone expansion in...(x) theory and operator twist......Page 191 16.1 Moment sum rules......Page 193 16.3 Anomalous dimension of the non-singlet structure functions......Page 197 16.4.1 Non-singlet part of the Bjorken sum rule......Page 200 Non-singlet part......Page 202 Singlet part......Page 203 16.5 Singlet anomalous dimensions and moments......Page 204 17.1 The non-singlet case......Page 207 17.2 The singlet case......Page 208 17.3 Some physical interpretations and factorization theorem......Page 209 17.4 Polarized parton densities......Page 210 18.2.1 The limit x → 1......Page 213 18.2.3 The limit x → 0 for the singlet case and the BFKL pomeron......Page 214 18.3 Experimental tests and new developments......Page 215 18.4 Neutrino scattering sum rules......Page 218 18.5 Summary of α measurements from DIS......Page 220 19.2 Extension of the method to massive quarks......Page 221 19.3.2 Semi-inclusive polarized ep scattering......Page 223 1. Introduction......Page 225 2. The first moment sum rule for g…......Page 228 3. QCD spectral sum rule estimate of X'(0)......Page 232 4. Tests of the Bjorken sum rule and estimate of higher twist effects......Page 238 5. Further discussion......Page 239 Chiral Ward identities and the renormalisation group......Page 241 Decay constants and the π'......Page 242 Acknowledgements......Page 246 References......Page 247 20.1 Kinematics......Page 249 20.2.1 Cross-section......Page 250 20.3 Higher order corrections to the cross-section......Page 251 20.4 The K factor......Page 253 21 One 'prompt photon' inclusive production......Page 254 Part V Hard processes in...collisions......Page 256 Introduction......Page 257 22.1 Process and fragmentation functions......Page 258 22.2 Inclusive density, correlations and hadron multiplicity......Page 259 22.3 Parton model and QCD description......Page 260 23.1 OPE and moment sum rules......Page 265 23.2 Unpolarized photon structure functions......Page 267 23.3.1 Moments and cross-section......Page 268 The AVV vertex and chiral Ward identities......Page 269 Non-singlet form factors......Page 270 Singlet form factors......Page 272 Implications for the moment sum rules......Page 273 24.2 IR divergences: Bloch–Nordsieck and KLN theorems......Page 274 24.3 Two-jet events......Page 277 24.4 Three-jet events......Page 279 24.4.1 Thrust as a jet observable......Page 280 24.4.2 Other event-shape variables......Page 281 24.4.3 Event-shape distributions......Page 282 24.4.4 Energy-energy correlation......Page 283 24.4.5 Jade and Durham algorithms......Page 284 24.5 QCD tests from jet analysis......Page 285 24.6 Jets from heavy quarkonia decays......Page 286 24.7 Jets from ep, pp and pp collisions......Page 288 25.1 Heavy quarkonia OZI-violating decays......Page 289 25.2 Alternative extractions of α from heavy quarkonia......Page 291 25.3 ... hadrons total cross-section......Page 292 25.4 Z → hadrons......Page 295 25.5 Inclusive semi-hadronic τ decays......Page 296 25.5.1 Running of α below the τ-mass......Page 303 25.6.1 α from other τ widths......Page 304 25.6.2 α from…I = 1 hadrons data......Page 305 25.6.3 Strange quark mass from τ-like processes......Page 306 Part VI Summary of QCD tests and α measurements......Page 308 VI.2.1 Deep inelastic scatterings......Page 309 VI.3 Summary of the α determinations......Page 310 Part VII Power corrections in QCD......Page 316 26 Introduction......Page 318 27.1 The anatomy of the SVZ expansion......Page 320 27.2 SVZ expansion in the...model......Page 321 27.3.1 Scale invariant D = 4 condensates......Page 323 27.3.2 D = 5 mixed quark-gluon condensate......Page 325 27.3.3 D = 6 gluon condensates......Page 326 27.3.4 D = 6 four-quark condensates......Page 327 27.3.5 Higher dimensions gluonic condensates......Page 328 27.3.6 Relations among the different condensates......Page 329 27.3.7 Non-normal ordered condensates and cancellation of mass singularities......Page 330 28.1.2 Gluon fields and condensates......Page 332 28.1.4 Mixed quark-gluon condensate......Page 334 28.1.6 Quark propagator......Page 335 28.2 Application of the Fock–Schwinger technology to the light quarks pseudoscalar two-point correlator......Page 336 28.2.1 Quark condensate.........Page 337 28.2.2 Gluon condensate.........Page 338 28.2.3 Mixed quark-gluon condensate......Page 339 28.2.4 Four-quark condensates......Page 340 28.3.1 General procedure......Page 341 28.3.2 D = 4 gluon condensate of the electromagnetic correlator......Page 342 28.3.3 D = 6 condensates of the electromagnetic correlator......Page 343 28.3.4 Matching the heavy and light quark expansions......Page 344 28.3.5 Cancellation of mass singularities......Page 345 28.4 The plane wave method......Page 346 28.5 On the calculation in a covariant gauge......Page 347 29.1 Introduction......Page 348 29.2 Convergence of the Borel integral......Page 350 29.4 IR renormalons......Page 351 29.5 UV renormalons......Page 354 29.6.1 The D-function......Page 355 29.6.2 Semi-hadronic inclusive Tau decays......Page 356 29.7 Power corrections for jet shapes......Page 357 29.8.1 Drell–Yan process......Page 358 29.8.3 Gross–Llewellyn Smith and polarized Bjorken sum rules......Page 359 29.9 Power corrections to the heavy quark pole mass......Page 360 30.1 Tachyonic gluon mass......Page 362 30.2.1 't Hooft instanton solution......Page 364 30.2.3 Dilute gas approximation......Page 366 30.2.4 The instanton liquid model......Page 368 30.3 Lattice measurements of power corrections......Page 369 Part VIII QCD two-point functions......Page 374 31.3 Quark mass corrections to the (pseudo)scalar and (axial)-vector quark correlators......Page 376 31.9 Hybrid correlators......Page 377 32.1 Exact two-loop perturbative expression in the MS scheme......Page 378 32.2 Three-loop expressions in the chiral limit......Page 379 32.4 Dimension-four......Page 380 32.5 Dimension-five......Page 381 32.7 Exact two-loop expression of the spectral function......Page 382 32.8 Heavy-light correlator......Page 383 33.1 Exact two-loop perturbative expression in the MS scheme......Page 385 33.2 Three-loop expression including the m-terms......Page 386 33.3 Dimension-four......Page 387 33.5 Dimension-six......Page 389 33.6.1 Complete two-loop perturbative expression of the spectral function......Page 390 33.6.2 Four-loop perturbative expression of the spectral function......Page 391 33.7 Heavy-light correlator......Page 392 33.8.1 Vector correlator......Page 393 33.8.2 (Pseudo)scalar correlator......Page 394 34 Tensor-quark correlator......Page 395 35.1.1 The decuplet......Page 397 35.1.2 The octet......Page 398 35.2.1 Spin 1/2 baryons......Page 400 35.2.2 Spin 3/2 baryon......Page 402 36.1 Four-quark states......Page 404 36.2 S = 1 correlator and I = 1/2 rule......Page 405 36.3 The S = 2 correlator......Page 407 36.4 The B = 2 correlator......Page 408 37.1 Pseudoscalar gluonia......Page 411 37.2 Pseudoscalar meson-gluonium mixing......Page 413 37.4 Scalar meson-gluonium mixing......Page 414 37.6 Scalar di-and tri-gluonium mixing......Page 415 37.8 Tensor meson-gluonium mixing......Page 416 37.9 Contributions beyond the OPE: tachyonic gluon mass......Page 417 38.1 Light hybrid correlators......Page 419 38.2 Heavy hybrid correlators......Page 421 39.1 (Axial-)vector correlators......Page 422 39.2 (Pseudo)scalar correlators......Page 423 Part IX QCD non-perturbative methods......Page 426 40 Introduction......Page 428 41.1 Introduction......Page 429 41.2 Gluons on the lattice: the Wegner–Wilson action......Page 430 41.3 Quarks on the lattice......Page 432 41.4 Quark and gluon interactions......Page 435 41.5.1 The QCD coupling and the weak coupling regime......Page 437 41.5.2 Wilson loop, confinement and the strong coupling regime......Page 438 41.5.3 Some other applications and limitations of the lattice......Page 440 42.1 Introduction......Page 442 42.2 PCAC relation from ChPT......Page 443 42.3 Current algebra quark mass ratios......Page 446 42.4.2 Chiral loops......Page 447 42.4.3 The non-Abelian chiral anomaly......Page 449 42.5 Some low-energy phenomenology to order ρ......Page 450 42.5.1 Decay constants......Page 451 42.5.2 Electromagnetic form factors......Page 452 42.5.3 K decays......Page 453 42.5.4 Ratios of light quark masses to order ρ......Page 454 43.1 Introduction......Page 457 43.2.1 Large N counting rules for mesons......Page 458 43.2.2 Chiral Lagrangian in the large N-limit......Page 459 43.2.3 Minimal hadronic ansatz to large N QCD......Page 460 43.2.4 Baryons in the large N limit......Page 463 43.3 Lowest meson dominance models......Page 464 43.4 The constituent chiral quark model......Page 465 43.5 Effective action approach models......Page 466 43.6 The Extended Nambu–Jona-Lasinio Model......Page 467 44.2 Heavy-quark symmetry......Page 475 44.3.1 Introduction......Page 476 44.3.2 The HQET Lagrangian......Page 477 44.3.3 Symmetries of the Lagrangian......Page 480 44.3.4 Heavy quark wave-function renormalization in HQET......Page 481 44.3.5 Residual mass term and definition of the heavy quark mass......Page 482 44.4 Hadron spectroscopy from HQET......Page 483 44.5.1 Semi-leptonic form factors: the Isgur–Wise function......Page 485 44.5.2 The Luke's theorem for the 1/mQ corrections......Page 488 44.5.3 Short-distance corrections and matching conditions......Page 489 44.5.4 Determination of |V| from HQET......Page 490 44.6 The inclusive…weak process......Page 491 44.7 Rare B decays and CP-violation......Page 495 45.1 The Schrödinger equation......Page 497 45.2 The QCD static Coulomb potential......Page 498 45.3.3 Martin potential......Page 501 45.4.1 Relativistic corrections......Page 502 45.4.2 Radiative and non-perturbative corrections......Page 504 45.4.4 Some phenomenological applications......Page 505 45.5 Bell–Bertlmann equivalent potentials......Page 506 45.6 Stochastic vacuum model......Page 507 45.6.1 The model......Page 508 45.6.2 Application to the static potential......Page 510 45.7 Non-relativistic effective theories for quarkonia......Page 512 46 On monopole and confinement......Page 517 Part X QCD spectral sum rules......Page 520 47 Introduction......Page 522 48.1 Generalities and dispersion relations......Page 524 48.2 Explicit derivation of the dispersion relation......Page 525 48.3 General proof of the dispersion relation......Page 527 48.4 The QCD side of the sum rules......Page 529 49.1 Moment sum rules in QCD......Page 532 49.2 Laplace sum rule (LSR)......Page 533 49.3 Ratio of moments......Page 534 49.4 Finite energy sum rule (FESR)......Page 536 49.5 Features of FESR and an example......Page 537 49.6 The Gaussian sum rules......Page 538 49.8 Analytic continuation......Page 541 49.10 Optimization criteria......Page 542 49.10.1 The harmonic oscillator......Page 543 49.10.2 Non-relativistic charmonium sum rules......Page 544 49.10.3 Implications for QCD......Page 545 49.12 Test of the QCD-duality ansatz in the charmonium sum rules......Page 546 49.13 HQET sum rules......Page 548 49.13.1 Decay constant, meson-quark mass gap, kinetic energy and chromomagnetic operator......Page 549 49.14 Vertex sum rules and form factors......Page 551 49.14.1 Spectral representation......Page 552 49.14.2 Illustration from the evaluation of the g...coupling......Page 553 49.15.1 Basics and illustration by the...process......Page 555 49.15.2 Distribution amplitudes......Page 558 50.1 Sacrosanct Weinberg sum rules (WSR) in the chiral limit......Page 560 50.1.2 Matching between the low- and high-energy regions......Page 561 50.2 ...and f in the chiral limit......Page 563 50.3 Masses and power corrections to the Weinberg sum rules......Page 564 50.4 DMO sum rules in QCD......Page 565 51.1 α from...hadrons and Tau-decays data......Page 566 51.2 α from heavy quarkonia mass-splittings......Page 567 1. The double ratio of moments......Page 568 3. Balmer-mass formula from the ratio of moments......Page 570 4. ... hyperfine and P – S-wave splittings......Page 572 5. Leptonic width and quarkonia wave function......Page 573 6. Gluon condensate from…......Page 574 7. Charmonium P-wave splittings......Page 575 9. ... mass splitting......Page 577 10. ... mass splittings and new estimate of the gluon condensate......Page 578 12. Toponium: illustration of the infinite mass limit......Page 579 References......Page 580 52.1 Dimension-two tachyonic gluon mass......Page 583 52.3 Dimension-four gluon condensate......Page 584 52.5 Dimension-six four-quark condensates......Page 586 52.7 Dimension-eight condensates......Page 588 52.8 Instanton like-contributions......Page 589 1. Introduction......Page 590 2. α from ... hadrons data......Page 591 3. The condensates from -like decays......Page 594 4. The condensates from the ratio of the Laplace sum rules......Page 597 6. Test of the size of the 1/M2-term......Page 599 7. Sum of the non-perturbative corrections to R......Page 600 8. Implication on the value of from R......Page 601 9. Conclusion......Page 602 References......Page 603 53.1 Introduction......Page 605 53.2 Quark mass definitions and ratios of light quark masses......Page 606 53.3.1 Bounds on the sum of light quark masses from pseudoscalar channels......Page 607 53.3.3 Bounds on the sum of light quark masses from the quark condensate and…......Page 611 53.4.1 The (pseudo)scalar Laplace sum rules......Page 613 53.4.2 The ud channel......Page 615 53.4.3 The us channel and QSSR prediction for the ratio.........Page 617 53.5 Direct extraction of the chiral condensate (uu)......Page 618 53.6 Final estimate of ... from QSSR and consequences on .........Page 619 53.7.1 The scalar ud channel......Page 620 53.9.1 ... hadrons data and the Φ-meson channel......Page 621 53.9.2 Tau decays......Page 622 53.9.3 Summary for the estimate of light quark masses......Page 623 53.10.1 Pseudoscalar mesons......Page 624 53.10.2 Scalar mesons......Page 626 53.11.1 SU(3) corrections to kaon PCAC......Page 627 53.11.2 Subtraction constant from the scalar sum rule......Page 630 53.11.4 (ss) / (uu) from the Bs meson......Page 631 53.12 Heavy quark masses......Page 632 53.12.1 The quarkonia channel......Page 633 53.12.2 The heavy-light D and B meson channels......Page 635 Summary for the heavy quark masses and consequences......Page 639 53.13 The weak leptonic decay constants.........Page 640 53.13.1 Upper bound on the value of fD......Page 641 53.13.2 Estimate of the D decay constant fD......Page 642 53.13.3 Ratio of the decay constants…......Page 643 53.13.5 Static limit and 1/M-corrections to fB......Page 645 53.14 Conclusions......Page 647 54.2 Light baryons......Page 648 54.3.2 Baryons with one heavy quark......Page 651 54.4 Hadrons with charm and beauty......Page 653 54.6 Gluonia spectra......Page 654 54.7.2 ...couplings to.........Page 655 54.7.3 G(1.5) coupling to nn'......Page 657 54.7.4 ... couplings to 4 Pi......Page 658 54.7.5 …and G couplings to........Page 659 54.7.6 J/ψ → γ S radiative decays......Page 660 54.9 Mixing schemes for scalar mesons......Page 661 54.9.2 Nature of the.........Page 662 54.10 Mixing and decays of the tensor gluonium......Page 664 54.12 Test of the four-quark nature of the α (980)......Page 665 54.13 Light hybrids......Page 667 54.13.2 Decay widths of the.........Page 668 54.14.1 Conclusions......Page 669 55.1.1 Introduction and notations......Page 671 55.1.2 Estimate of the form factors and of V......Page 674 55.1.4 Large Mb-limit of the form factors......Page 676 55.1.5 q-behaviour of the form factors......Page 677 55.2 Slope of the Isgur–Wise function and value of V......Page 678 55.3 B(D) → B(D) Π (γ) couplings and decays......Page 682 55.4 Weak semi-leptonic decays of the B mesons......Page 683 55.4.1 Anomalous thresholds......Page 685 56.1.1 Phenomenology of...mixings......Page 687 56.1.2 The Bell–Steinberger unitarity constraint......Page 690 56.1.3 K → 2Pi amplitudes......Page 692 56.2.1 Introduction......Page 697 56.2.2 Two-point function sum rule......Page 698 56.2.3 Results and implications on.........Page 700 56.3.2 Estimate of the CP violation parameters .........Page 701 56.4.1 SM theory of .........Page 702 56.4.2 Soft pion and kaon reductions of... to vacuum condensates......Page 706 56.4.3 The...condensates from DMO-like sum rules in the chiral limit......Page 707 56.4.4 The...condensates from hadronic tau inclusive decays......Page 709 56.4.5 Impact of the results on the CP violation parameter.........Page 712 56.4.6 Summary and conclusions......Page 713 57.1 The QCD phases......Page 714 57.3 Hadronic correlations at finite temperature......Page 715 57.4 Asymptotic behaviour of the correlator in hot hadronic matter......Page 717 57.5 Quark condensate at finite Τ......Page 719 57.8 Four-quark condensate......Page 723 57.9 The ρ-meson spectrum in hot hadronic matter......Page 724 57.10 ρ-meson coupling and width......Page 726 57.12 Hadronic couplings......Page 727 57.13 Nucleon sum rules and neutron electric dipole moment......Page 728 58.2 Electroweak models with dynamic symmetry breaking......Page 729 Part XI Appendices......Page 732 A.2 High-energy physical constants......Page 734 A.3 CKM weak mixing matrix......Page 735 A.4 Some astrophysical constants......Page 736 B.2 Adjoint representation of the gluon fields......Page 737 B.4 The case of SU(3)......Page 738 Appendix C Coordinates and momenta......Page 740 D.1 Definition and notations......Page 742 D.3 Polarizations......Page 743 D5. Dirac algebra in n-dimensions......Page 744 D.6 The totally anti-symmetric tensor......Page 746 E.2 Factors induced by closed loops......Page 747 E.3 Propagators and vertices......Page 748 E.4 Composite operators in deep-inelastic scattering......Page 749 E.5 Rules in the background field approach......Page 750 F.1.2 Original Feynman parametrization......Page 752 F.2 The...function......Page 753 F.3 The beta function Β(x, y)......Page 754 F.6 One-loop massless integrals......Page 755 F.7 Two- and three-loop massless integrals......Page 757 F.8 One-loop massive integrals......Page 759 F.9 A two-loop massive integral......Page 760 F.10 The dilogarithm function......Page 761 F.11 Some useful logarithmic integrals......Page 762 F.12 Further useful functions......Page 764 G.1 Laplace sum rule......Page 765 G.4 Cauchy contour integrals......Page 766 Current algebra......Page 768 Parton models......Page 769 The QCD story......Page 770 The MS scheme......Page 773 Renormalizations of operators......Page 774 Heavy quark pole masses......Page 775 MS scheme for QED and high-precision tests of QED......Page 776 Unpolarized DIS processes......Page 778 Polarized DIS processes and the proton spin crisis......Page 779 Processes......Page 780 Heavy quarkonia decays......Page 781 Tau-decays and QCD perturbative series......Page 782 Strange quark mass......Page 783 Reviews on QCD spectral sum rules......Page 784 Instantons......Page 785 Gluon condensate from.........Page 786 Baryon sum rules......Page 787 Heavy baryons......Page 788 Renormalons 3......Page 789 Chiral perturbation theory......Page 790 Large Nc......Page 791 Heavy quark symmetry and HQET......Page 792 Inclusive weak processes......Page 793 Non-relativistic effective theories for quarkonia......Page 794 Laplace, FESR sum rules,.........Page 795 Light cone sum rules......Page 796 Light quark masses......Page 797 Heavy quark masses......Page 798 Gluonia......Page 799 Heavy to light exclusive decays......Page 801 B decays......Page 802 Theory of .........Page 803 Plasma......Page 804 XI Appendices......Page 805 Index......Page 806 "This book provides a pedagogical introduction to the perturbative and non-perturbative aspects of quantum chromodynamics (QCD)." "Introducing the basic theory and recent advances in QCD, it also reviews the historical development of the subject up to the present day, covering pre-QCD ideas of strong interactions such as the quark and parton models, the notion of colours and the S-matrix approach. The author then discusses gauge theory, techniques of dimensional regularization and renormalization, deep inelastic scattering and hard processes in hadron collisions, hadron jets, and e[superscript +]e[superscript -] annihilations. Other topics include power corrections and the technologies of the Shifman-Vainshtein-Zakharov operating product expansion. The final parts of the book are devoted to modern non-perturbative approaches to QCD and the phenomenological aspects of QCD spectral sum rules." "The book will be a valuable reference for graduate students and researchers in high-energy particle and nuclear physics, both theoretical and experimental."--BOOK JACKET
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