標(biāo)題: Titlebook: Gauge Theory of Weak Interactions; Walter Greiner,Berndt Müller Textbook 2009Latest edition Springer-Verlag Berlin Heidelberg 2009 Element [打印本頁(yè)] 作者: EXTRA 時(shí)間: 2025-3-21 17:16
書(shū)目名稱(chēng)Gauge Theory of Weak Interactions影響因子(影響力)
書(shū)目名稱(chēng)Gauge Theory of Weak Interactions影響因子(影響力)學(xué)科排名
書(shū)目名稱(chēng)Gauge Theory of Weak Interactions網(wǎng)絡(luò)公開(kāi)度
書(shū)目名稱(chēng)Gauge Theory of Weak Interactions網(wǎng)絡(luò)公開(kāi)度學(xué)科排名
書(shū)目名稱(chēng)Gauge Theory of Weak Interactions被引頻次
書(shū)目名稱(chēng)Gauge Theory of Weak Interactions被引頻次學(xué)科排名
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書(shū)目名稱(chēng)Gauge Theory of Weak Interactions年度引用學(xué)科排名
書(shū)目名稱(chēng)Gauge Theory of Weak Interactions讀者反饋
書(shū)目名稱(chēng)Gauge Theory of Weak Interactions讀者反饋學(xué)科排名
作者: 團(tuán)結(jié) 時(shí)間: 2025-3-21 23:25 作者: 不能平靜 時(shí)間: 2025-3-22 04:16
Limitations of Fermi Theory,ould – up to now – be classified and understood within this scheme. Nevertheless, as we shall see, the Fermi theory contains severe difficulties and is therefore unsatisfactory. In order to reveal these difficulties we shall discuss first another phenomenon of weak interactions, i.e. the neutral cur作者: Digitalis 時(shí)間: 2025-3-22 05:11
,The Salam–Weinberg Theory,ractions, and incorporating charged and neutral currents in a unified way. First we have to learn how to convert a theory involving massless vector bosons into a theory of massive particles, without disturbing the favorable high-energy behavior of a massless propagator. We shall proceed by discussin作者: Crumple 時(shí)間: 2025-3-22 10:28
,Some Properties of the Salam–Weinberg Theory?of?Leptons,he neutral current. This made a specific experimental search for these particles possible, to which end it is important to know the possible creation and decay mechanisms. We see immediately that in an electron–positron storage ring it is considerably easier to produce the neutral Z. bosons than the作者: CAMEO 時(shí)間: 2025-3-22 14:26 作者: CAMEO 時(shí)間: 2025-3-22 18:47 作者: Canyon 時(shí)間: 2025-3-23 00:49 作者: Palter 時(shí)間: 2025-3-23 02:08
Unified Gauge Theories,treats leptons and quarks on the same footing. However, the fact that leptons carry integer charge while the charge of quarks is 1/3 is needed as a basic input. On the other hand, there are indications that this fact is due to some superior principle, that is a larger symmetry. This leads to the hyp作者: Perceive 時(shí)間: 2025-3-23 08:06 作者: 微粒 時(shí)間: 2025-3-23 11:39 作者: Laconic 時(shí)間: 2025-3-23 14:51 作者: heirloom 時(shí)間: 2025-3-23 19:59
Leptonic Interactions,no each. The charged particles are the electron, the muon, and the tau lepton, the corresponding neutrinos the electron neutrino, the muon neutrino, and the tau neutron. Muons and tau leptons decay into electrons via the weak interactions, and we discuss these processes in detail.作者: Commission 時(shí)間: 2025-3-23 23:06 作者: 付出 時(shí)間: 2025-3-24 02:21
Nuclear Beta Decay, In order to describe the weak interactions of the hadrons themselves we must in addition know how the hadrons are made up of quarks, that is, we must know the wave functions of the quarks within the hadrons. This problem has not yet been completely solved, but there are a number of models which reflect some properties of the hadrons quite well.作者: 宿醉 時(shí)間: 2025-3-24 09:03
https://doi.org/10.1007/978-3-540-87843-8Elementary Particle Physics; Gauge Theory; Kaon; Lepton; Nuclear Physics; Weak Interactions; hadron作者: Mitigate 時(shí)間: 2025-3-24 13:36
Deutschland: Ein Auswanderungsland?,, these are: the strong (nuclear) interaction, electromagnetism, the weak (nuclear) interaction, and gravity. The interaction strength varies with distance between the force centers..In contrast to the strong interaction, the weak interaction operates between all particles. It causes reactions which作者: bourgeois 時(shí)間: 2025-3-24 16:06 作者: 輕觸 時(shí)間: 2025-3-24 22:00 作者: THE 時(shí)間: 2025-3-25 01:53
Senta Pfaff-Rüdiger,Maria L?blichractions, and incorporating charged and neutral currents in a unified way. First we have to learn how to convert a theory involving massless vector bosons into a theory of massive particles, without disturbing the favorable high-energy behavior of a massless propagator. We shall proceed by discussin作者: Optic-Disk 時(shí)間: 2025-3-25 05:08 作者: RENAL 時(shí)間: 2025-3-25 09:32
https://doi.org/10.1007/978-3-662-29339-3ys have integer spin. The lightest hadrons, with equal spin (and equal parity), can be arranged in simple multiplets, where two further quantum numbers serve as order criteria: the isospin ., and its third component .., and the strangeness ., or alternatively the so-called strong hypercharge .=.+.. 作者: Conspiracy 時(shí)間: 2025-3-25 15:35
https://doi.org/10.1007/978-3-663-04720-9 In order to describe the weak interactions of the hadrons themselves we must in addition know how the hadrons are made up of quarks, that is, we must know the wave functions of the quarks within the hadrons. This problem has not yet been completely solved, but there are a number of models which ref作者: 散布 時(shí)間: 2025-3-25 15:53
https://doi.org/10.1007/978-3-662-35318-9ent shows that K. and K. form a conjugate particle–antiparticle pair, as does the pair K. and .. While both K. and . are neutral, they differ in the signs of isospin and strangeness. We know that isospin and strangeness conservation are violated by the weak interaction. Thus, despite the fact that K作者: nauseate 時(shí)間: 2025-3-25 20:39
https://doi.org/10.1007/978-3-663-07096-2treats leptons and quarks on the same footing. However, the fact that leptons carry integer charge while the charge of quarks is 1/3 is needed as a basic input. On the other hand, there are indications that this fact is due to some superior principle, that is a larger symmetry. This leads to the hyp作者: 討好女人 時(shí)間: 2025-3-26 01:43
978-3-540-87842-1Springer-Verlag Berlin Heidelberg 2009作者: Salivary-Gland 時(shí)間: 2025-3-26 06:25
Walter Greiner,Berndt MüllerCarefully developed and well introduced text.Part of the Greiner lectures and its educational standards.Accessible introduction to the field.Now available as a newly revised edition.Includes supplemen作者: Herd-Immunity 時(shí)間: 2025-3-26 10:02 作者: 俗艷 時(shí)間: 2025-3-26 15:38 作者: BUDGE 時(shí)間: 2025-3-26 17:51 作者: 凌辱 時(shí)間: 2025-3-27 00:36
.Now available as a newly revised edition.Includes supplemen"Gauge Theory of Weak Interactions" treats the unification of electromagnetic and weak interactions and considers related phenomena. First, the Fermi theory of beta decay is presented, followed by a discussion of parity violation, clarifyin作者: 600 時(shí)間: 2025-3-27 03:24 作者: Biomarker 時(shí)間: 2025-3-27 05:48
https://doi.org/10.1007/978-3-662-35318-9igns of isospin and strangeness. We know that isospin and strangeness conservation are violated by the weak interaction. Thus, despite the fact that K. and . are different particles at the level of the strong interaction, there is no reason why they should not be able to transform into each other under the influence of the weak interaction.作者: Accomplish 時(shí)間: 2025-3-27 11:25
https://doi.org/10.1007/978-3-663-04440-6rticular, decays involving a neutrino are experimentally characteristic, because a large fraction of the energy present in the scattering is transferred to the neutrino and is therefore not seen in the detectors.作者: 哪有黃油 時(shí)間: 2025-3-27 14:03
https://doi.org/10.1007/978-3-663-07096-2mmetry. The simplest group that incorporates the product SU(3)×SU(2)×SU(1) as a subgroup is SU(5). A model for the unification of the three interactions based on the group SU(5) was proposed by Georgi and Glashow.作者: Subdue 時(shí)間: 2025-3-27 19:29 作者: BOOST 時(shí)間: 2025-3-27 23:56 作者: lymphoma 時(shí)間: 2025-3-28 02:11 作者: Exposition 時(shí)間: 2025-3-28 10:03 作者: 執(zhí) 時(shí)間: 2025-3-28 13:46 作者: 同謀 時(shí)間: 2025-3-28 14:52
Textbook 2009Latest editionnteractions is thoroughly discussed including current developments. The final chapter contains an introduction to unified theories of strong and electroweak interactions. Numerous solved examples and problems make this volume uniquely suited as a text for an advanced course. This fourth edition has been carefully revised.作者: Ligneous 時(shí)間: 2025-3-28 22:47
,The Salam–Weinberg Theory,sons into a theory of massive particles, without disturbing the favorable high-energy behavior of a massless propagator. We shall proceed by discussing the methodical approach first, before performing a detailed calculation.作者: CHAFE 時(shí)間: 2025-3-28 23:35
The Neutral Kaon System,igns of isospin and strangeness. We know that isospin and strangeness conservation are violated by the weak interaction. Thus, despite the fact that K. and . are different particles at the level of the strong interaction, there is no reason why they should not be able to transform into each other under the influence of the weak interaction.作者: phytochemicals 時(shí)間: 2025-3-29 05:27
