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量子場(chǎng)論自學(xué)教程

量子場(chǎng)論自學(xué)教程

定 價(jià):¥139.00

作 者: (英)湯姆·蘭卡斯,斯蒂芬·布倫德?tīng)?/td>
出版社: 世界圖書(shū)出版公司
叢編項(xiàng):
標(biāo) 簽: 暫缺

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ISBN: 9787519296032 出版時(shí)間: 2023-08-01 包裝: 平裝-膠訂
開(kāi)本: 16開(kāi) 頁(yè)數(shù): 字?jǐn)?shù):  

內(nèi)容簡(jiǎn)介

  量子場(chǎng)論可以說(shuō)是有史以來(lái)影響最深遠(yuǎn)、最優(yōu)美的物理理論,與物理學(xué)中的任何其他理論相比,量子場(chǎng)論在各方面都得到了更嚴(yán)格的檢驗(yàn)和更精確的驗(yàn)證。然而這門(mén)科目卻以難著稱,在各種針對(duì)專業(yè)人士的厚重教材中,數(shù)學(xué)晦澀難懂,還要使用一種由氣泡、波浪線、頂點(diǎn)和其他幾何結(jié)構(gòu)組成的奇怪圖示語(yǔ)言來(lái)描述物理過(guò)程。對(duì)于任何懷有抱負(fù)的理論物理學(xué)家而言,學(xué)習(xí)這種數(shù)學(xué)與幾何語(yǔ)言都是一場(chǎng)重要的入門(mén)儀式,絕大多數(shù)大學(xué)都設(shè)有量子場(chǎng)論研究生課程,并輔以大量具有參考價(jià)值的量子場(chǎng)論教材。這些書(shū)由專業(yè)的量子場(chǎng)理論家所寫(xiě),為那些渴望加入他們的讀者而設(shè)計(jì)。因此,這些書(shū)往往寫(xiě)得細(xì)致而又嚴(yán)謹(jǐn),同時(shí)還需要用到高水平的復(fù)雜數(shù)學(xué)技巧。作者寫(xiě)這本書(shū)的初衷是:量子場(chǎng)論如此重要無(wú)比又充滿魅力,不該局限于研究量子場(chǎng)論的專業(yè)人士,實(shí)驗(yàn)物理學(xué)家、粒子物理學(xué)家、凝聚態(tài)物理學(xué)家等也能從量子場(chǎng)論中受益良多,獲得洞見(jiàn),但并非人人都像理論物理學(xué)家那樣具有深厚的數(shù)學(xué)功底。量子場(chǎng)論讓我們對(duì)物理世界有了一個(gè)截然不同的革命性觀點(diǎn),應(yīng)該讓更多的物理從業(yè)者有機(jī)會(huì)參與其中,所以作者希望為這類人寫(xiě)一本量子場(chǎng)論書(shū)。全書(shū)分十一個(gè)部分,共五十一章(含第零章),前九部分介紹了經(jīng)典場(chǎng)論、量子場(chǎng)論、統(tǒng)計(jì)場(chǎng)論、拓?fù)鋱?chǎng)論等,并間或補(bǔ)充了一些需要用到的量子力學(xué)、統(tǒng)計(jì)力學(xué)等知識(shí);最后兩部分介紹了量子場(chǎng)論在凝聚態(tài)物理和粒子物理中的應(yīng)用。本書(shū)排版錯(cuò)落有致,結(jié)構(gòu)張弛有度,內(nèi)容詳略得當(dāng),文筆精準(zhǔn)優(yōu)雅,插圖生動(dòng)形象,應(yīng)當(dāng)成為每一位量子場(chǎng)論研習(xí)者的案頭讀物。

作者簡(jiǎn)介

  湯姆·蘭卡斯特(Tom Lancaster),曾是牛津大學(xué)物理學(xué)研究員,2012 年加入杜倫大學(xué),目前是物理系和材料物理中心的教授。他曾擔(dān)任國(guó)際μ子光譜學(xué)會(huì)主席,與斯蒂芬·布倫德?tīng)枺⊿tephen J. Blundell)等人合著有Muon Spectroscopy: An Introduction一書(shū)。斯蒂芬·布倫德?tīng)枺⊿tephen J. Blundell),牛津大學(xué)物理系教授,并曾擔(dān)任凝聚態(tài)物理的主任,他還是牛津大學(xué)曼斯菲爾德學(xué)院董事。他另著有Concepts in Thermal Physics,Magnetism in Condensed Matter,Superconductivity: A Very Short Introduction,Magnetism: A Very Short Introduction等書(shū)。

圖書(shū)目錄

Overture The Universe as a set of harmonic oscillators Lagrangians Simple harmonic oscillators Occupation number representation Making second quantization work Writing down Lagrangians Continuous systems A first stab at relativistic quantum mechanics Examples of Lagrangians, or how to write down a theory III. The need for quantum fields The passage of time Quantum mechanical transformations Symmetry Canonical quantization of fields Examples of canonical quantization Fields with many components and massive electromagnetism Gauge fields and gauge theory Discrete transformations Propagators and perturbations Ways of doing quantum mechanics: propagators and Green’s functions Propagators and Fields The S-matrix Expanding the S-matrix: Feynman diagrams Scattering theory Interlude: wisdom from statistical physics Statistical physics: a crash course The generating functional for fields Path Integrals Path Integrals: I said to him, “You’re crazy” Field Integrals Statistical field theory Broken symmetry Coherent states Grassmann numbers: coherent states and the path integral for fermions VII. Topological ideas Topological objects Topological field theory VIII. Renormalization: taming the infinite Renormalization, quasiparticles and the Fermi surface Renormalization: the problem and its solution Renormalization in action: propagators and Feynman diagrams The renormalization group Ferromagnetism: a renormalization group tutorial Putting a spin on QFT The Dirac equation How to transform a spinor The quantum Dirac field A rough guide to quantum electrodynamics QED scattering: three famous cross sections The renormalization of QED and two great results Some applications from the world of condensed matter Superfluids The many-body problem and the metal Superconductors The fractional quantum Hall fluid Some applications from the world of particle physics Non-abelian gauge theory The Weinberg-Salam model Majorana fermions Magnetic monopoles Instantons, tunnelling and the end of the world Appendix A. Further reading
Appendix B. Useful complex analysis               

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