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Quantum field theory II[electronic r...
~
Shifman, Mikhail A.
Quantum field theory II[electronic resource] /
紀錄類型:
書目-電子資源 : Monograph/item
杜威分類號:
530.14/3
書名/作者:
Quantum field theory II/ Mikhail Shifman.
其他題名:
Quantum field theory 2
作者:
Shifman, Mikhail A.
出版者:
Singapore : : World Scientific Publishing Co. Pte. Ltd.,, c2019.
面頁冊數:
1 online resource (xvi, 302 p.) : : ill.
標題:
Quantum field theory.
ISBN:
9789813234192
ISBN:
9813234199
書目註:
Includes bibliographical references and index.
內容註:
Lecture 1. Yang-Mills theory -- Lecture 2. Yang-Mills theories (continued) -- Lecture 3. Path integral quantization -- Lecture 4. Path integral in scalar QFT -- Lecture 5. Complex scalar field and finite temperature -- Lecture 6. Calculus of Grassmann numbers and spinor fields -- Lecture 7. Fermion fields in path integrals -- Lecture 8. Gauge fields in path integral : the simplest example of QED -- Lecture 9. Non-abelian gauge fields in path integrals -- Lecture 10. How to calculate charge renormalization -- Lecture 11. Yang-Mills coupling (continued) -- Lecture 12. What if vacuum is not unique -- Lecture 13. Condensed matter week -- Lecture 14. Renormalization group ; RG flow -- Lecture 15. Phases of Yang-Mills theories -- Lecture 16. Anomalous dimensions. Quark mass in QCD -- Lecture 17. More on XSB. Effective Lagrangians -- Lecture 18. Quantum anomalies -- Lecture 19. Quantum anomalies (continued) -- Lecture 20. "External" anomalies : implications -- Lecture 21. Divergence of perturbation theory at high orders -- Lecture 22. Degenerate (pre)vacua and instantons in QM.
摘要、提要註:
"Field Theory II begins with the path integral formulation of quantum field theory. Perturbation theory is generalized beyond tree level, to include radiative corrections (loops). The renormalization procedure and Wilsonean renormalization group are discussed, asymptotic freedom of non-Abelian gauge theories derived, and some applications in Quantum Chromodynamics (QCD) considered, with a brief digression into the Standard Model (SM). Sample higher order corrections are worked out. The SM case requires a study of the spontaneous breaking of the gauge symmetry, a phenomenon which would be more appropriate to call 'Higgsing of the gauge bosons'"--
電子資源:
https://
www.worldscientific.com/worldscibooks/10.1142/10825#t=toc
Quantum field theory II[electronic resource] /
Shifman, Mikhail A.
Quantum field theory II
[electronic resource] /Quantum field theory 2Mikhail Shifman. - 1st ed. - Singapore :World Scientific Publishing Co. Pte. Ltd.,c2019. - 1 online resource (xvi, 302 p.) :ill.
Includes bibliographical references and index.
Lecture 1. Yang-Mills theory -- Lecture 2. Yang-Mills theories (continued) -- Lecture 3. Path integral quantization -- Lecture 4. Path integral in scalar QFT -- Lecture 5. Complex scalar field and finite temperature -- Lecture 6. Calculus of Grassmann numbers and spinor fields -- Lecture 7. Fermion fields in path integrals -- Lecture 8. Gauge fields in path integral : the simplest example of QED -- Lecture 9. Non-abelian gauge fields in path integrals -- Lecture 10. How to calculate charge renormalization -- Lecture 11. Yang-Mills coupling (continued) -- Lecture 12. What if vacuum is not unique -- Lecture 13. Condensed matter week -- Lecture 14. Renormalization group ; RG flow -- Lecture 15. Phases of Yang-Mills theories -- Lecture 16. Anomalous dimensions. Quark mass in QCD -- Lecture 17. More on XSB. Effective Lagrangians -- Lecture 18. Quantum anomalies -- Lecture 19. Quantum anomalies (continued) -- Lecture 20. "External" anomalies : implications -- Lecture 21. Divergence of perturbation theory at high orders -- Lecture 22. Degenerate (pre)vacua and instantons in QM.
"Field Theory II begins with the path integral formulation of quantum field theory. Perturbation theory is generalized beyond tree level, to include radiative corrections (loops). The renormalization procedure and Wilsonean renormalization group are discussed, asymptotic freedom of non-Abelian gauge theories derived, and some applications in Quantum Chromodynamics (QCD) considered, with a brief digression into the Standard Model (SM). Sample higher order corrections are worked out. The SM case requires a study of the spontaneous breaking of the gauge symmetry, a phenomenon which would be more appropriate to call 'Higgsing of the gauge bosons'"--
ISBN: 9789813234192
Standard No.: 99983640706Subjects--Topical Terms:
382693
Quantum field theory.
LC Class. No.: QC174.46 / .S553 2019eb
Dewey Class. No.: 530.14/3
Quantum field theory II[electronic resource] /
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Lecture 1. Yang-Mills theory -- Lecture 2. Yang-Mills theories (continued) -- Lecture 3. Path integral quantization -- Lecture 4. Path integral in scalar QFT -- Lecture 5. Complex scalar field and finite temperature -- Lecture 6. Calculus of Grassmann numbers and spinor fields -- Lecture 7. Fermion fields in path integrals -- Lecture 8. Gauge fields in path integral : the simplest example of QED -- Lecture 9. Non-abelian gauge fields in path integrals -- Lecture 10. How to calculate charge renormalization -- Lecture 11. Yang-Mills coupling (continued) -- Lecture 12. What if vacuum is not unique -- Lecture 13. Condensed matter week -- Lecture 14. Renormalization group ; RG flow -- Lecture 15. Phases of Yang-Mills theories -- Lecture 16. Anomalous dimensions. Quark mass in QCD -- Lecture 17. More on XSB. Effective Lagrangians -- Lecture 18. Quantum anomalies -- Lecture 19. Quantum anomalies (continued) -- Lecture 20. "External" anomalies : implications -- Lecture 21. Divergence of perturbation theory at high orders -- Lecture 22. Degenerate (pre)vacua and instantons in QM.
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"Field Theory II begins with the path integral formulation of quantum field theory. Perturbation theory is generalized beyond tree level, to include radiative corrections (loops). The renormalization procedure and Wilsonean renormalization group are discussed, asymptotic freedom of non-Abelian gauge theories derived, and some applications in Quantum Chromodynamics (QCD) considered, with a brief digression into the Standard Model (SM). Sample higher order corrections are worked out. The SM case requires a study of the spontaneous breaking of the gauge symmetry, a phenomenon which would be more appropriate to call 'Higgsing of the gauge bosons'"--
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https://www.worldscientific.com/worldscibooks/10.1142/10825#t=toc
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