Titlebook: Journey to the Bound States; Paul Hoyer Book 2021 The Author(s), under exclusive license to Springer Nature Switzerland AG 2021 QCD bound

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書目名稱Journey to the Bound States影響因子(影響力)




書目名稱Journey to the Bound States影響因子(影響力)學科排名




書目名稱Journey to the Bound States網(wǎng)絡公開度




書目名稱Journey to the Bound States網(wǎng)絡公開度學科排名




書目名稱Journey to the Bound States被引頻次




書目名稱Journey to the Bound States被引頻次學科排名




書目名稱Journey to the Bound States年度引用




書目名稱Journey to the Bound States年度引用學科排名




書目名稱Journey to the Bound States讀者反饋




書目名稱Journey to the Bound States讀者反饋學科排名

賞錢

Features of Hadrons,g and bound states (Sect. 2.2). The .-dependence of Deep Inelastic Scattering distinguishes partons that are intrinsic to the hadron from those that are created by the hard scattering (Sect. 2.3). Data is consistent with a QCD coupling . which “freezes” at low scales (Sect. 2.4).

FEAS

Brief Survey of Present QED Approaches to Atoms,ethe-Salpeter bound state equation is sketched, and its non-uniqueness noted (Sect. 3.3). The non-relativistic effective field theory method NRQED is introduced (Sect. 3.4). The corresponding heavy quark effective theories HQET, NRQCD and pNRQCD are noted (Sect. 3.5).

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召集

Fock Expansion of Bound States in Temporal (,) Gauge,oral gauges in QED (Sect. 5.2). The vanishing of the color octet electric field . for color singlet states allows to include a homogeneous solution of Gauss’ constraint for each color component of the state. This corresponds to a boundary condition which introduces a universal constant . (Sect. 5.3).

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內(nèi)部

Book 2021t recalls the usual quantum electrodynamics (QED) approach to atoms in terms of Feynman diagrams, which assume free states at asymptotic times. Motivated by general principles and data, he then develops a novel method based on a Fock expansion of bound states in temporal gauge. The properties of rel

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緊張過度

Applications to QCD Bound States,arton model, string breaking and duality (Sect. 8.4). The glueball (.) spectrum has features similar to that of . mesons (Sect. 8.5). There is a massless . . state which has vanishing four-momentum in all frames. It may mix with the vacuum without violating Poincaré invariance, giving rise to a spontaneous breaking of chiral symmetry (Sect. 8.6).

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