標(biāo)題: Titlebook: Contemporary Topics in Medium Energy Physics; Klaus Goeke,W-Y. Pauchy Hwang,Josef Speth Book 1994 Springer Science+Business Media New York [打印本頁(yè)] 作者: JOLT 時(shí)間: 2025-3-21 16:31
書(shū)目名稱Contemporary Topics in Medium Energy Physics影響因子(影響力)
書(shū)目名稱Contemporary Topics in Medium Energy Physics影響因子(影響力)學(xué)科排名
書(shū)目名稱Contemporary Topics in Medium Energy Physics網(wǎng)絡(luò)公開(kāi)度
書(shū)目名稱Contemporary Topics in Medium Energy Physics網(wǎng)絡(luò)公開(kāi)度學(xué)科排名
書(shū)目名稱Contemporary Topics in Medium Energy Physics被引頻次
書(shū)目名稱Contemporary Topics in Medium Energy Physics被引頻次學(xué)科排名
書(shū)目名稱Contemporary Topics in Medium Energy Physics年度引用
書(shū)目名稱Contemporary Topics in Medium Energy Physics年度引用學(xué)科排名
書(shū)目名稱Contemporary Topics in Medium Energy Physics讀者反饋
書(shū)目名稱Contemporary Topics in Medium Energy Physics讀者反饋學(xué)科排名
作者: Carcinoma 時(shí)間: 2025-3-21 21:08
Book 1994 of the year of 1992, in the area of medium energy physics. The book is the result of the multi-pronged efforts by the authors who were invited to speak at the Second German- Chinese Symposium on "Medium Energy Physics" (September 7-10, 1992, Bochum, Germany). The premise of the meeting is to invest作者: 傾聽(tīng) 時(shí)間: 2025-3-22 00:28
Packaging and Deploying Your Application,to treat nonleptonic weak interaction problems, including parity-violating ., ., and . couplings, decays of heavy mesons or of heavy baryons, etc. Throughout the present talk, I shall discuss primarily the issues related to the nucleon structure.作者: patella 時(shí)間: 2025-3-22 08:30 作者: 繼而發(fā)生 時(shí)間: 2025-3-22 12:12
Creating Data and Presentation Extensions,ian valid in the limit of large .., one can derive large-.. fourth-order effective chiral Lagrangians for ?. = 1 nonleptonic weak interactions and radiative weak transitions. Applications to . →., . →., and .→. are discussed.作者: Insufficient 時(shí)間: 2025-3-22 16:34 作者: Insufficient 時(shí)間: 2025-3-22 19:49 作者: biosphere 時(shí)間: 2025-3-23 00:52
An Extended Perturbation Theory for QCDesents a pure quantum effect similar to anomalies. An interesting aspect of the scheme is the existence of solutions in which the basic gluon and quark propagators have no stable-particle poles, and describe short-lived elementary excitations, leading to a weak-coupling description of confinement.作者: Lamina 時(shí)間: 2025-3-23 03:08
Large-,, Higher Order Weak Chiral Lagrangians for Nonleptonic and Radiative Kaon Decaysian valid in the limit of large .., one can derive large-.. fourth-order effective chiral Lagrangians for ?. = 1 nonleptonic weak interactions and radiative weak transitions. Applications to . →., . →., and .→. are discussed.作者: 假 時(shí)間: 2025-3-23 07:38 作者: Devastate 時(shí)間: 2025-3-23 12:34 作者: 膝蓋 時(shí)間: 2025-3-23 15:25 作者: 親愛(ài) 時(shí)間: 2025-3-23 20:51 作者: ambivalence 時(shí)間: 2025-3-24 01:46 作者: implore 時(shí)間: 2025-3-24 05:34
Regularization and Renormalization within the Hamiltonian Formulation of QCD the effective Hamiltonian within a primarily regularized framework, only the lattice regularization appears to be consistent. The computation yields then a new check for the equivalence between lattice and dimensional regularization.作者: CRUE 時(shí)間: 2025-3-24 10:32 作者: ARENA 時(shí)間: 2025-3-24 12:18 作者: BUDGE 時(shí)間: 2025-3-24 15:01 作者: faddish 時(shí)間: 2025-3-24 19:06 作者: 野蠻 時(shí)間: 2025-3-25 00:46 作者: 入伍儀式 時(shí)間: 2025-3-25 05:00 作者: savage 時(shí)間: 2025-3-25 09:32 作者: 人類學(xué)家 時(shí)間: 2025-3-25 11:54 作者: 熱烈的歡迎 時(shí)間: 2025-3-25 18:22 作者: infelicitous 時(shí)間: 2025-3-25 20:33
Packaging and Deploying Your Application,ch strong interactions, as described by quantum chromodynamics (QCD) among quarks and gluons, play an important role. The determination of the isovector and isoscalar axial coupling constants, .. and .., via the method of QCD sum rules is used to illustrate the method. The determination of the neutr作者: athlete’s-foot 時(shí)間: 2025-3-26 01:32
Programming Your Own Spreadsheets,expansion (OPE) (Wilson, 1969) for products of local operators. Such an expansion has often been given in terms of local operators of different twists at short or light-like distances. However, as indicated by several calculations (Geyer, 1982; Balitsky, 1983; Braunschweig et al., 1984; Geyer et al.作者: NICHE 時(shí)間: 2025-3-26 05:57
https://doi.org/10.1007/978-1-4302-2526-3icient to describe that most basic of things, the mass spectrum. Although, we may hope one day to gain from the lattice approach numerical confirmation that we have the correct Lagrangian to describe hadronic physics, that day is not at hand. In the meantime it will be argued here, the operator prod作者: 花爭(zhēng)吵 時(shí)間: 2025-3-26 11:30 作者: 緩和 時(shí)間: 2025-3-26 16:09 作者: 帶傷害 時(shí)間: 2025-3-26 20:51 作者: Connotation 時(shí)間: 2025-3-27 00:23
Introducing Silverlight Screen Design,ime thanks to the celebrated asymptotic freedom.. For the static properties of the mesons and baryons, which are described by the rather low energy features of QCD, up to now only the calculations on a lattice could give some crude estimates.. Therefore one was faced with developing some effective t作者: Systemic 時(shí)間: 2025-3-27 04:09
Creating Data and Presentation Extensions,ically from various low-energy hadronic processes. While this scenario works well for strong interactions, it is unsatisfactory for nonleptonic and radiative nonleptonic weak interactions: It is impossible, from the outset, to determine all unknown higher-order chiral couplings by experiment; theory作者: 施加 時(shí)間: 2025-3-27 07:56 作者: amygdala 時(shí)間: 2025-3-27 12:20 作者: CANON 時(shí)間: 2025-3-27 16:52 作者: 有斑點(diǎn) 時(shí)間: 2025-3-27 20:19
Introducing Silverlight Screen Design,quark mass, the strong interactions of a heavy quark become much simplified. Namely, the effective QCD Lagrangian becomes independent of the flavor and spin of the heavy quark. For .. heavy quark flavors, the new spin and flavor symmetries combine to form a .(..) symmetry group (heavy quark symmetry作者: Genetics 時(shí)間: 2025-3-28 02:00 作者: encyclopedia 時(shí)間: 2025-3-28 03:14 作者: 打擊 時(shí)間: 2025-3-28 09:45 作者: 慷慨援助 時(shí)間: 2025-3-28 13:16
https://doi.org/10.1007/978-1-4757-9835-7hadron; lepton; neutron; nuclear physics; nucleon; strong interaction作者: 慢慢啃 時(shí)間: 2025-3-28 15:13 作者: Lumbar-Spine 時(shí)間: 2025-3-28 21:44 作者: Keratectomy 時(shí)間: 2025-3-28 23:56 作者: 熱情贊揚(yáng) 時(shí)間: 2025-3-29 03:44
Regularization and Renormalization within the Hamiltonian Formulation of QCDthod) are discussed within the framework of Lüscher’s small volume Yang Mills theory. If one computes the corresponding folded diagram coefficients of the effective Hamiltonian within a primarily regularized framework, only the lattice regularization appears to be consistent. The computation yields 作者: semiskilled 時(shí)間: 2025-3-29 09:16 作者: 商業(yè)上 時(shí)間: 2025-3-29 13:32 作者: characteristic 時(shí)間: 2025-3-29 15:33
Evolution Equations for Nonlocal Hadron Operatorsexpansion (OPE) (Wilson, 1969) for products of local operators. Such an expansion has often been given in terms of local operators of different twists at short or light-like distances. However, as indicated by several calculations (Geyer, 1982; Balitsky, 1983; Braunschweig et al., 1984; Geyer et al.作者: BROOK 時(shí)間: 2025-3-29 20:54 作者: 淡紫色花 時(shí)間: 2025-3-30 03:00 作者: AVERT 時(shí)間: 2025-3-30 07:29
Solitonic Solutions of the Su(2) Nambu-Jona-Lasinio Model with Vector Mesonsnterpret baryons as solitons of a yet unknown effective mesonic action.. This motivates the use of specific effective models exhibiting one of the most salient features of QCD, dynamical chiral symmetry breaking. The Nambu—Jona-Lasinio model. incorporates this feature and thus has been studied inten作者: GRIEF 時(shí)間: 2025-3-30 08:29
Highlights of the NJL Chiral Solitonmerical results for the static soliton energy are presented for the cases without and with vector and axialvector fields. It is found that the baryon number is carried by the polarized Dirac sea of the quarks if the .. meson is included in contrast to the case without .. where the baryon number resi作者: 稀釋前 時(shí)間: 2025-3-30 15:31 作者: BRUNT 時(shí)間: 2025-3-30 17:00
Large-,, Higher Order Weak Chiral Lagrangians for Nonleptonic and Radiative Kaon Decaysically from various low-energy hadronic processes. While this scenario works well for strong interactions, it is unsatisfactory for nonleptonic and radiative nonleptonic weak interactions: It is impossible, from the outset, to determine all unknown higher-order chiral couplings by experiment; theory作者: Cpr951 時(shí)間: 2025-3-30 20:44 作者: Acupressure 時(shí)間: 2025-3-31 03:46 作者: VICT 時(shí)間: 2025-3-31 08:46
Consequences of the Heavy Quark Symmetry for Semileptonic Decays of Heavy Baryons) that in the formal limit of infinitely large momenta and masses of the heavy quarks, where the momentum-mass ratios, i.e. the velocities, are kept fixed, a new spin-flavour symmetry emerges. In fact it is a .(2). ? .(2). symmetry if we restrict ourselves to c and b quarks. This symmetry is termed 作者: FOR 時(shí)間: 2025-3-31 11:04 作者: Geyser 時(shí)間: 2025-3-31 14:01
Spectator and Non-Spectator Models in the B Meson Systemsatisfy the experimental results. After the contribution from the non-spectator (.-exchange) model is included, the semileptonic branching ratio of . mesons will be within the experimental region, and the sizable lifetime difference between B. and .. mesons is predicted.作者: chondromalacia 時(shí)間: 2025-3-31 19:22
The Electromagnetic Structure of Hadrons and Gauge Invarianceerest was if this interaction is the same as the free interaction or if there are exotic medium modifications of the free mechanism. Reactions that were studied for this purpose were mainly inclusive electron-nucleus scattering and the exclusive (e,e’p) process. The interpretation of these nuclear e作者: achlorhydria 時(shí)間: 2025-3-31 22:04
Book 1994concerning these subjects, as of the year of 1992. As there are many distinctly different research areas in contemporary intermediate energy physics, we could only choose a few topics of current interest, especially those which are related, directly or indirectly, to the structural studies of the nu
