規(guī)范理論和現(xiàn)代粒子物理學(xué)導(dǎo)論（第1卷）

前言

　　for a book of its genre，our previous book，An introduction to gauoetheories and the"new physic"（1982）was a great success.It was not.alas，sold in airport lounges，but it did run to two additional printings（1983，198s），and to extensively revised editions in Russian（1990）.and oin-Polish（1991）.More importantly，it seemed to achieve the principal goal which we had set ourselves，namely，to present a pedagogical account ofmodern particle physics with a balance of theory and experiment，whichwould be intelligible and stimulating for both theoretical and experimental raduate students.We did not try to write a profound book on fieldtheory，nor a treatise on sophisticated experimental techniques.But wedid wish to stress the deep，intimate and fruitful interaction betweentheoretical ideas and experimental results.Indeed，for US，it iS just thisaspect of physics which makes it seem so much more exciting than say puremathematics our greatest pleasure came from the favourable reaction ofstudents who were working through the book and from those reviewerswho caught what we hoped was its essential flaV0ur——the writing createsthe reeling of an active progression of ideas arising from the repeatedinteraction of theoretical prejudice with experimental observation unlikemost textbooks，it is highly readable，and makes everything appear simpleand obviousWeII，the last comment iS surely an exaggeration but that was our aim.

內(nèi)容概要

本書分為兩冊(cè)，詳細(xì)地介紹了粒子物理學(xué)的現(xiàn)代理論和實(shí)驗(yàn)。條理分明，表述連貫。作者以簡(jiǎn)明直觀的方式，闡釋隱藏在實(shí)驗(yàn)現(xiàn)象背后的深刻的物理原理，同時(shí)循序漸進(jìn)地講解從事粒子物理研究用到的現(xiàn)代方法。本書收入了許多粒子物理領(lǐng)域的新成果，還有若干很有特色的議題，例如高階弱電效應(yīng)，夸克混合，噴流，深度非彈性輕子—強(qiáng)子散射，簡(jiǎn)單部分子模型的量子色動(dòng)力學(xué)修正，以及量子色動(dòng)力學(xué)的非微擾理論等。本書可以作為現(xiàn)代粒子物理學(xué)方向的研究生教材，對(duì)該領(lǐng)域的科研人員也有很好的參考價(jià)值。本書第一冊(cè)主要包括電弱相互作用，新的基本粒子的探索及其物理性質(zhì)的研究，部分子的發(fā)現(xiàn)，以及簡(jiǎn)單部分子模型的構(gòu)建和預(yù)測(cè)等。第二冊(cè)在介紹了CP破壞之后，主要講解量子色動(dòng)力學(xué)及其在“硬”過程中的應(yīng)用，同時(shí)也介紹了“軟”強(qiáng)子物理和非微擾量子色動(dòng)力學(xué)。　　讀者對(duì)象：理論物理、高能物理和場(chǎng)論等專業(yè)的高年級(jí)本科生、研究生和相關(guān)專業(yè)的科研人員。

書籍目錄

Preface Acknowledgements Notational conventions Note added in proof: the discovery of the top quark (?) Note added in proof: the demise of the SSC 1 Field theory and pre-gauge theory of weak interactions 　1.1 A brief introduction to field theory 　1.2 Pre-gange theory of weak interactions 　1.3 The spin and isospin structure 　1.4 Tests of the V-A structure and 'lepton universality' 2 The need for a gauge theory 　2.1 The intermediate vector boson 　2.2 Towards a renormalizable theory 　2.3 Gauge symmetry 　2.4 Freedom to choose the gauge 　2.5 Summary 3 Spontaneous symmetry breaking: the Goldstone theorem and the Higgs phenomenon 　3.1 Spontaneously broken symmetries in field theory: Goldstone's theorem 　3.2 The Higgs mechanism 　3.3 Unitarity and renormalizability 　3.4 Suwmmary 4 Construction of the standard model 　4.1 Model building (towards the standard model) 　4.2 The standard model 　4.3 Discovery of W and Z0 5 Lowest order tests of the SM in the leptonic sector 　5.1 Phenomenology of purely leptonic reactions 　5.2 A check of the minimal Higgs mechanism 　5.3 Support for the SM from hadronic collider data 　5.4 Concluding remarks 6 The Higgs boson 　6.1 Introductory remarks 　6.2 Higgs decay 　6.3 Higgs production at the Z0 mass 　6.4 Limits on the Higgs mass 　6.5 Concluding comments 7 The standard model beyond lowest order 　7.1 Radiative corrections 　7.2 Renormalization and physical parameters 　7.3 The effective fine structure constant 　7.4 The muon lifetime revisited 　7.5 Estimates of one loop corrections 　7.6 Higher order corrections 　7.7 Practical problems in testing radiative corrections 　7.8 Strategies to overcome the imprecision in Mw 　7.9 Testing the minimal Higgs mechanism 　7.10 Beyond the standard model 8 e+e- physics and the standard model 　8.1 Electron-positron storage rings 　8.2 The new e+e- colliders: TRISTAN and LEP 　8.3 e+e- physics at energies [[ Mz 　8.4 e+e- and the standard model 　8.5 LEP data near the Z0 peak 　8.6 Determination of the SM parameters of the Z0 　8.7 Neutrino counting 　8.8 Asymmetries and polarization measurements at the Z0 peak 　8.9 Conclusions 9 Extension to the hadrons; quark-lepton universality 　9.1 Charm, bottom and top 　9.2 Quark mixing 　9.3 Electroweak interaction of the quarks 　9.4 The GIM mechanism 　9.5 Colour 　9.6 Summary of the quark sector of the standard model 　9.7 Quark masses and the KM matrix 10 Phenomenology of semi-leptonic reactions 　10.1 Model independent tests 　10.2 Parity violation in electron-nucleus scattering 　10.3 Optical rotation 　10.4 Summary 11 The discovery of the narrow vector resonances 　11.1 Introduction 　11.2 The 'new' particles 　11.3 Some qualitative features of QCD 　11.4 Quark-lepton parallelism 　11.5 Flavour classification of hadrons 　11.6 The J/ψ and the OZI rule 　11.7 Experimental status of the J/ψ spectroscopy 　11.8 Properties of the J/ψ(3097) and ψ'(3685) 　11.9 Baryouic decay of J/ψ 　11.10 The T family and its experimental status 12 Hidden flavour bound states 　12.1 Quarkonium 　12.2 J/ψ decays. Calculation of the widths 　12.3 Determination of as 　12.4 Leptonic widths 　12.5 Exotics: glueballs, hybrids, etc. 　12.6 ψ'→π: a puzzle 　12.7 Conclusions 13 Open heavy flavours 　13.1 Discovery and basic properties of charm and bottom particles 　　13.2 Charm decay 　13.3 B physics 　13.4 Production of heavy fiavours 　13.5 Heavy fiavours at LEP 　13.6 Final comments 14 The heavy lepton τ 　14.1 Introduction 　14.2 Discovery of the τ lepton 　14.3 Properties of the τ lepton 　14.4 τ decay 　14.5 The τ neutrino 　14.6 Rare τ decays 　14.7 Miscellaneous and conclusions 15 Towards the parton model deep inelastic scattering 　15.1 Electron-muon scattering 　15.2 Elastic electron-proton scattering 　15.3 Inelastic electron-nucleon scattering 　15.4 Inelastic neutrino-nucleon scattering 　15.5 Deep inelastic scattering and scaling behaviour 　15.6 Polarization effects in deep inelastic scattering 16 The quark-parton model 　16.1 The introduction of partons 　16.2 Antipartons 　16.3 Partons as quarks 　16.4 The detailed quark-parton model 　16.5 Charged lepton induced reactions for Q2 of order M2z 　16.6 Behaviour of the quark number densities as x → 0 　16.7 The missing constituents--gluons 　16.8 The parton model in polarized deep inelastic scattering 　16.9 Appendix to Chapter 16: The patton model as an impulse approximation 17 Experimental tests of the quark-parton model 　17.1 Deep inelastic scaling functions for Q2 [[ M2Z 　17.2 Neutrino cross-sections in the quark-parton model for Q2 [[M2Z 　17.3 Cross-sections in the quark-parton model for Q2 comparable with M2Z 　17.4 Application of the parton model to related processes Appendix 1: Elements of field theory 　A1.1 Fields and creation operators 　A1.2 Parity, charge conjugation and G-parity 　A1.3 The S-matrix Appendix 2: Feynman rules for QED, QCD and the SM 　A2.1 Relation between S-matrix and Feynman amplitude 　A2.2 QCD and QED 　A2.3 The SM 　A2.4 Some examples of Feynman amplitudes 　A2.5 Colour sums 　A2.6 The Gell-Mann SU(3) matrices 　A2.7 The Fierz reshuffle theorem 　A2.8 Dimension of matrix elements Appendix 3: Conserved vector currents and their charges References Analytic subject index for vols. 1 and 2

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