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標題: Titlebook: An introduction to relativistic processes and the standard model of electroweak interactions; Carlo M. Becchi,Giovanni Ridolfi Textbook 20 [打印本頁]

作者: patch-test    時間: 2025-3-21 19:35
書目名稱An introduction to relativistic processes and the standard model of electroweak interactions影響因子(影響力)




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions影響因子(影響力)學科排名




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions網絡公開度




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions網絡公開度學科排名




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions被引頻次




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions被引頻次學科排名




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions年度引用




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions年度引用學科排名




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions讀者反饋




書目名稱An introduction to relativistic processes and the standard model of electroweak interactions讀者反饋學科排名





作者: 邊緣    時間: 2025-3-21 22:47

作者: profligate    時間: 2025-3-22 02:31

作者: 較早    時間: 2025-3-22 07:35

作者: Cryptic    時間: 2025-3-22 11:26
Studien zur politischen Gesellschaftsince the measurement of the muon lifetime provides the most precise determination of the Fermi constant ., and one of the most precise measurements in the whole field of elementary particle physics. In this Section, we describe the calculation of the corresponding decay rate in some detail.
作者: 名次后綴    時間: 2025-3-22 16:36

作者: 甜食    時間: 2025-3-22 19:29

作者: incarcerate    時間: 2025-3-23 01:09
Carlo M. Becchi,Giovanni RidolfiIncludes supplementary material:
作者: Tortuous    時間: 2025-3-23 02:48
UNITEXThttp://image.papertrans.cn/a/image/155721.jpg
作者: ANTH    時間: 2025-3-23 06:33

作者: Osmosis    時間: 2025-3-23 11:05
Studien zur politischen GesellschaftWe present here the full Lagrangian density of the standard model with one Higgs doublet. We have . where
作者: Interstellar    時間: 2025-3-23 14:40
Scattering theory,Before discussing scattering processes in field theory, we briefly recall a few general results in scattering theory in the traditional Lippman-Schwinger formulation.
作者: 離開就切除    時間: 2025-3-23 21:24

作者: RECUR    時間: 2025-3-24 01:09
https://doi.org/10.1007/978-3-662-28931-0regime, a large number of new particles is typically produced, with large momenta, or, equivalently, small wavelengths. For this reason, the scheme of ordinary Quantum Mechanics, based on the Schr?dinger equation for wave functions that depend on a fixed number of variables, is no longer applicable.
作者: 抓住他投降    時間: 2025-3-24 03:21
https://doi.org/10.1007/978-3-658-29331-4he electromagnetic fields, and Dirac and Yukawa fields. The field description of a physical system allows a direct implementation of the principle of covariance, that guarantees the invariance of the equations of motion under changes of reference frame, and of the principle of causality, which is co
作者: Hearten    時間: 2025-3-24 08:14
Lena Schacht,Michael Minkenberg the context of quantum electrodynamics. We define the following symbols: . Equation (3.89) is represented as . while the graphical form of eq. (3.90) is . It is understood that each internal vertex corresponds to a space-time integration.
作者: MEAN    時間: 2025-3-24 13:46
Julia Schwanholz,Patrick Theiner in detail the case of scalar fields, transforming as . under a Lorentz transformation .. A second well-known example (which will be discussed at length in Chapters 7 and 8) is provided by vector fields: . In the general case, we have a system of complex fields ., . = 1, ..., ., with the transformat
作者: 易于出錯    時間: 2025-3-24 16:41
https://doi.org/10.1007/978-3-322-83371-6vide a relativistic description of electrons and photons. The theory is based on a pair of spinor fields of opposite chiralities, . and .; invariance under phase multiplication of the spinor fields is assumed, and the corresponding conserved current is identified with the electromagnetic current. No
作者: 我說不重要    時間: 2025-3-24 20:28
https://doi.org/10.1007/978-3-322-83371-6y of weak interactions. The Fermi Lagrangian density for . and . decays is given by. . From the measured values of muon and neutron lifetimes, . one obtains . while the value . can be extracted from the measurement of baryon semi-leptonic decay rates. The most striking feature of weak interactions,
作者: Senescent    時間: 2025-3-25 00:27
https://doi.org/10.1007/978-3-322-93512-0on field and of the . field; similarly, left-handed quarks with charge ?1/3 enter the weak interaction term as linear combinations of the corresponding mass eigenfields. We show here that these mixing phenomena are consequences of the mechanism of mass generation in the model.
作者: 偏見    時間: 2025-3-25 07:22
Die politische Funktionselite der DDR a chiral transformation, i.e. a transformation that acts differently on left-handed and right-handed components. The gauge transformations of the standard model are precisely of this kind. Again, this difficulty can be circumvented by means of the Higgs mechanism.
作者: Mobile    時間: 2025-3-25 11:22

作者: 傀儡    時間: 2025-3-25 14:17
Abhandlungen zur Mittelstandsforschungby direct experimental upper bounds on neutrino masses: . and even if observations indicate that neutrino masses are in fact non-zero, the approximation . ? ., where . is any fermion in the standard model spectrum, is extremely good for most applications. In view of experimental results, however, it
作者: 休戰(zhàn)    時間: 2025-3-25 17:36

作者: Longitude    時間: 2025-3-25 21:14
Spontaneous breaking of the gauge symmetry,on field and of the . field; similarly, left-handed quarks with charge ?1/3 enter the weak interaction term as linear combinations of the corresponding mass eigenfields. We show here that these mixing phenomena are consequences of the mechanism of mass generation in the model.
作者: GULLY    時間: 2025-3-26 00:17
Breaking of accidental symmetries, a chiral transformation, i.e. a transformation that acts differently on left-handed and right-handed components. The gauge transformations of the standard model are precisely of this kind. Again, this difficulty can be circumvented by means of the Higgs mechanism.
作者: 原諒    時間: 2025-3-26 07:18
Applications,since the measurement of the muon lifetime provides the most precise determination of the Fermi constant ., and one of the most precise measurements in the whole field of elementary particle physics. In this Section, we describe the calculation of the corresponding decay rate in some detail.
作者: osteocytes    時間: 2025-3-26 09:46
2038-5714 dents. The purpose is providing a rigorous and self-contained presentation of the theoretical framework and of the phenomenological aspects of the physics of interactions among fundamental constituents of matter....The first part of the volume is devoted to the description of scattering processes in
作者: invade    時間: 2025-3-26 13:47

作者: 顯而易見    時間: 2025-3-26 20:48
Julia Schwanholz,Patrick Theinerth in Chapters 7 and 8) is provided by vector fields: . In the general case, we have a system of complex fields ., . = 1, ..., ., with the transformation law . where the matrix . obeys the condition . for any two Lorentz transformations .. The vector field is an obvious example; in that case, we have simply . ≡ .).
作者: 凝乳    時間: 2025-3-26 21:23
Abhandlungen zur Mittelstandsforschungon . ? ., where . is any fermion in the standard model spectrum, is extremely good for most applications. In view of experimental results, however, it is interesting to study the possible ways neutrino mass terms can be consistently introduced.
作者: nonradioactive    時間: 2025-3-27 01:25
Relativistic field theory,covariance, that guarantees the invariance of the equations of motion under changes of reference frame, and of the principle of causality, which is connected to the principle of locality, namely, the independence of variables associated to different points in space at the same time.
作者: Glutinous    時間: 2025-3-27 05:36
Spinor fields,th in Chapters 7 and 8) is provided by vector fields: . In the general case, we have a system of complex fields ., . = 1, ..., ., with the transformation law . where the matrix . obeys the condition . for any two Lorentz transformations .. The vector field is an obvious example; in that case, we have simply . ≡ .).
作者: 沒花的是打擾    時間: 2025-3-27 13:14
Neutrino masses and mixing,on . ? ., where . is any fermion in the standard model spectrum, is extremely good for most applications. In view of experimental results, however, it is interesting to study the possible ways neutrino mass terms can be consistently introduced.
作者: concise    時間: 2025-3-27 16:23

作者: ARENA    時間: 2025-3-27 17:54

作者: Diastole    時間: 2025-3-28 00:54

作者: Hemiplegia    時間: 2025-3-28 02:27
Gauge symmetries, where ., . are real constants. Notice that we have inserted a Dirac mass term, which is allowed by the assumed invariance properties, while Majorana mass terms are not, as mentioned in Section 5.2. The conserved current is given by . and the constant e plays the role of elementary charge.
作者: epicardium    時間: 2025-3-28 06:16

作者: 行業(yè)    時間: 2025-3-28 11:23
https://doi.org/10.1007/978-3-322-83371-6the interaction in eq. (7.1) is non-renormalizable, since it contains operators with mass dimension 6; it is an effective theory, in the sense that it can only be used to compute amplitudes in the semi-classical approximation.
作者: climax    時間: 2025-3-28 18:18
The standard model,the interaction in eq. (7.1) is non-renormalizable, since it contains operators with mass dimension 6; it is an effective theory, in the sense that it can only be used to compute amplitudes in the semi-classical approximation.
作者: Ardent    時間: 2025-3-28 21:00
Textbook 20061st editionndard model of electroweak interactions, with special attention to the mechanism of particle mass generation. The extension of the standard model to include neutrino masses is also described....We have included a number of detailed computations of cross sections and decay rates of pedagogical and phenomenological relevance..
作者: 江湖郎中    時間: 2025-3-29 02:58
Introduction,regime, a large number of new particles is typically produced, with large momenta, or, equivalently, small wavelengths. For this reason, the scheme of ordinary Quantum Mechanics, based on the Schr?dinger equation for wave functions that depend on a fixed number of variables, is no longer applicable.
作者: 改革運動    時間: 2025-3-29 03:19
Relativistic field theory,he electromagnetic fields, and Dirac and Yukawa fields. The field description of a physical system allows a direct implementation of the principle of covariance, that guarantees the invariance of the equations of motion under changes of reference frame, and of the principle of causality, which is co
作者: cavity    時間: 2025-3-29 11:02
Feynman diagrams, the context of quantum electrodynamics. We define the following symbols: . Equation (3.89) is represented as . while the graphical form of eq. (3.90) is . It is understood that each internal vertex corresponds to a space-time integration.
作者: 商店街    時間: 2025-3-29 15:09

作者: 推延    時間: 2025-3-29 16:33

作者: 脖子    時間: 2025-3-29 21:11
The standard model,y of weak interactions. The Fermi Lagrangian density for . and . decays is given by. . From the measured values of muon and neutron lifetimes, . one obtains . while the value . can be extracted from the measurement of baryon semi-leptonic decay rates. The most striking feature of weak interactions,




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