弱尺度超對稱

內(nèi)容概要

　　超對稱是自然界中一種新的對稱性。本書全面系統(tǒng)地介紹了粒子物理學中的超對稱，首先闡述了超對稱的基本概念，接著展示了如何將超對稱納入到描述基本粒子的理論框架中。書中采用了高能物理實驗學家和唯象學家們所熟悉的四分量旋量表示，從而使得本書的可讀性大為增強。本書迅速地將讀者從抽象描述帶入到構(gòu)造基本粒子的超對稱性規(guī)范理論，并最終給出對撞機和宇宙學實驗觀測量的計算。本書與高能實驗和唯象理論結(jié)合得非常緊密，這是本書的一大特色。對于從事粒子物理實驗和唯象研究的物理學家和研究生而言，這是一本全面、實用且易懂的教學參考書，并且包括大量的練習和補充材料，非常合適作為超對稱理論的入門教材。閱讀本書需要一些基本的標準模型和量子場論知識。
　　讀者對象：粒子物理、理論物理和場論等專業(yè)的高年級本科生、研究生和相關(guān)專業(yè)的科研人員。

作者簡介

　　Howard Baer，美國佛羅里達州立大學J. D.
Kimel物理學教授，美國物理學會會士。1984在威斯康星大學獲得理論物理博士學位，先后在歐洲粒子物理實驗中心，阿貢國家實驗室，佛羅里達州立大學做博士后。在基本粒子物理領(lǐng)域內(nèi)發(fā)表了一百多篇學術(shù)論文。
Xerxes
Tata，美國夏威夷大學物理和天文學系教授，美國物理學會會士。在德克薩斯大學奧斯汀分校獲得理論高能物理博士學位。先后在俄勒岡大學，歐洲粒子物理實驗中心和威斯康星大學做博士后。在基本粒子物理領(lǐng)域內(nèi)發(fā)表了一百多篇學術(shù)論文。

書籍目錄

preface
the standard model
1.1 gauge invariance
1.2 spontaneous symmetry breaking
1.3 brief review of the standard model
2 what lies beyond the standard model?
2.1 scalar fields and quadratic divergences
2.2 why is the tev scale special?
2.3 what could the new physics be?
3 the wess-zumino model
3.1 the wess-zumino lagrangian
3.2 quantization of the wz model
3.3 interactions in the wz model
3.4 cancellation of quadratic divergences
3.5 soft supersymmetry breaking
the supersymmetry algebra
4.1 rotations
4.2 the lorentz group
4.3 the poincar6 group
4.4 the supersymmetry algebra
5 superfieid formalism
5.1 superfields
5.2 representations of symmetry generators: a recap
5.3 representation of susy generators as differential
operators
5.4 useful 0 identities
5.5 susy transformations of superfields
5.6 irreducible susy multiplets
5.7 products of superfields
5.8 supercovariant derivatives
5.9 lagrangians for chiral scalar superfields
5.10 the action as an integral over superspace
6 supersymmetric gauge theories
6.1 gauge transformations of superfields
6.2 the wess-zumino gauge
6.3 the curl superfield in the wess-zumino gauge
6.4 construction of gauge kinetic terms
6.5 coupling chiral scalar to gauge superfields
7 supersymmetry breaking
7.1 susy breaking by elementary fields
7.2 f-type susy breaking: the o'raifeartaigh model
7.3 d-type susy breaking
7.4 composite goldstinos
7.5 gaugino condensation
7.6 goldstino interactions
7.7 a mass sum rule
7.8 explicit supersymmetry breaking
7.9 a technical aside: ys-dependent fermion mass matrices
8 the minimal supersymlnetric standard model
8.1 constructing the mssm
8.2 electroweak symmetry breaking
8.3 particle masses in the mssm
8.4 interactions in the mssm
8.5 radiative corrections
8.6 should the goldstino be part of the mssm?
9 implications of the mssm
9.1 low energy constraints on the mssm
9.2 renormalization group equations
9.3 constraints from b → sy decay
9.4 bs → μ+μ- decay
9.5 muon anomalous magnetic moment
9.6 cosmological implications
9.7 neutrino masses
10 local supersymmetry
10.1 review of general relativity
10.2 local supersymmetry implies (super)gravity
10.3 the supergravity lagrangian
10.4 local supersymmetry breaking
11 realistic supersymmetric models
11.1 gravity-mediated supersymmetry breaking
11.2 anomaly-mediated susy breaking
11.3 gauge-mediated susy breaking
11.4 gaugino-mediated susy breaking
11.5 an afterword
12 sparticle production at colliders
12.1 sparticle production at hadron colliders
12.2 sparticle production at e+e- colliders
13 sparticle decays
13.1 decay of the gluino
13.2 squark decays
13.3 slepton decays
13.4 chargino decays
13.5 neutralino decays
13.6 decays of the higgs bosons
13.7 top quark decays to susy particles
13.8 decays to the gravitino/goldstino
14 supersymmetric event generation
14.1 event generation
14.2 event generator programs
14.3 simulating susy with isajet
15 the search for supersymmetry at coiliders
15.1 early searches for supersymmetry
15.2 search for susy at lep and lep2
15.3 supersymmetry searches at the tevatron
15.4 supersymmetry searches at supercolliders
15.5 beyond susy discovery
15.6 photon, muon, and very large hadron colliders
16 r-parity violation
16.1 explicit (trilinear) r-parity violation
16.2 spontaneous (bilinear) r-parity violation
17 epilogue
appendix a sparticle production cross sections
a.1 sparticle production at hadron colliders
a.2 sparticle production at e+e- colliders
appendixb sparticle decay widths
b.1 gluino decay widths
b.2 squark decay widths
b.3 slepton decay widths
b.4 neutralino decay widths
b.5 chargino clecay widths
b.6 top quark decay to susy particles
appendix c higgs boson decay widths
c.1 decays to sm fermions
c.2 decays to gauge bosons
c.3 decays to sfermions
c.4 decays to charginos and neutralinos
c.5 decays to higgs bosons
bibliography
index

章節(jié)摘錄

版權(quán)頁：   插圖：   At the one—loop level，however，a coupling of （H）u to down—type fermions is induced．This induced coupling leads to a new contribution，proportional to vu，tothe down—type fermion mass matrix．Although this contribution is suppressed bya loop factor relative to the tree—level contribution，this suppression is （partially）compensated if tan β is sufficiently large．As a result， down—type Yukawa interactions and down—type quark mass matrices are no longer diagonalized by the sametransformation，and flavor—violating couplings of neutral Higgs scalars h，H，and Aemerge．In the limit of large mA，the Higgs sector becomes equivalent to the Stan—dard Model （SM） Higgs sector with a light Higgs boson h （） HSM，and the effectsof flavor violation decouple from the low energy theory．The interesting featureis that the flavor—violating couplings of h，H， and A do not decouple for largesuperparticle mass parameters：being dimensionless，these couplings depend onlyon ratios of these mass parameters，and so remain finite even for very large valuesof SUSY mass parameters．

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《弱尺度超對稱:從超場到散射事例》是由世界圖書出版公司北京公司出版的。

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