標(biāo)題: Titlebook: BMS Particles in Three Dimensions; Blagoje Oblak Book 2017 Springer International Publishing AG 2017 BMS Symmetry.BMS Group.Three-dimensio [打印本頁(yè)] 作者: patch-test 時(shí)間: 2025-3-21 19:50
書(shū)目名稱BMS Particles in Three Dimensions影響因子(影響力)
書(shū)目名稱BMS Particles in Three Dimensions影響因子(影響力)學(xué)科排名
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書(shū)目名稱BMS Particles in Three Dimensions被引頻次
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書(shū)目名稱BMS Particles in Three Dimensions讀者反饋
書(shū)目名稱BMS Particles in Three Dimensions讀者反饋學(xué)科排名
作者: 遠(yuǎn)足 時(shí)間: 2025-3-21 20:56 作者: Ascribe 時(shí)間: 2025-3-22 02:44 作者: 刪減 時(shí)間: 2025-3-22 06:01 作者: ASTER 時(shí)間: 2025-3-22 10:46 作者: 碎石頭 時(shí)間: 2025-3-22 14:12
NDE 4.0: Image and Sound Recognitionthe opposite phenomenon: starting from a . of a group ., we will obtain a representation by . the orbit. This construction will further explain why orbits of momenta classify representations of semi-direct products. In addition it will turn out to be a tool for understanding gravity in parts II and III.作者: 注入 時(shí)間: 2025-3-22 18:48
Springer Series in Optical Sciencesly these tools to the BMS. group in three dimensions. Accordingly, in this chapter and the two next ones we address a necessary prerequisite for these considerations by studying the central extension of the group of diffeomorphisms of the circle, i.e. the Virasoro group.作者: optional 時(shí)間: 2025-3-23 00:41
Handbook of Nonlinear Optical Crystalsal for our purposes because they will turn out to coincide with the supermomentum orbits that classify BMS. particles. As we shall see, despite being infinite-dimensional, these orbits behave very much like the finite-dimensional coadjoint orbits of ..作者: EXPEL 時(shí)間: 2025-3-23 05:24 作者: 能量守恒 時(shí)間: 2025-3-23 08:20
Semi-direct Productsunitary representations, which are induced from representations of their translation subgroup combined with a so-called .. We interpret these representations as . propagating in space-time and having definite transformation properties under the corresponding symmetry group. This picture will be instrumental in our study of the BMS. group.作者: NATAL 時(shí)間: 2025-3-23 11:18
Coadjoint Orbits and Geometric Quantizationthe opposite phenomenon: starting from a . of a group ., we will obtain a representation by . the orbit. This construction will further explain why orbits of momenta classify representations of semi-direct products. In addition it will turn out to be a tool for understanding gravity in parts II and III.作者: 殘酷的地方 時(shí)間: 2025-3-23 17:19 作者: 蔑視 時(shí)間: 2025-3-23 20:59
Virasoro Coadjoint Orbitsal for our purposes because they will turn out to coincide with the supermomentum orbits that classify BMS. particles. As we shall see, despite being infinite-dimensional, these orbits behave very much like the finite-dimensional coadjoint orbits of ..作者: 克制 時(shí)間: 2025-3-23 23:11
Madhuja Tanya Mitra,K. Ray ChaudhuriIn this short chapter we discuss the implementation of symmetries in a quantum-mechanical context.作者: 狗窩 時(shí)間: 2025-3-24 06:02 作者: compassion 時(shí)間: 2025-3-24 10:09
Properties of Nonlinear Optical Crystals,The Bondi–Metzner–Sachs (BMS) group is an infinite-dimensional symmetry group of asymptotically flat gravity at null infinity, that extends Poincaré symmetry.作者: Ferritin 時(shí)間: 2025-3-24 11:39
https://doi.org/10.1007/978-3-540-46793-9This chapter is devoted to irreducible unitary representations of the BMS. group, i.e. BMS. particles, which we classify and interpret. As we shall see, the classification is provided by supermomentum orbits that coincide with coadjoint orbits of the Virasoro group.作者: canvass 時(shí)間: 2025-3-24 16:13 作者: Flagging 時(shí)間: 2025-3-24 20:21 作者: Provenance 時(shí)間: 2025-3-24 23:32
Quantum Mechanics and Central ExtensionsIn this short chapter we discuss the implementation of symmetries in a quantum-mechanical context.作者: Thymus 時(shí)間: 2025-3-25 04:24
Symmetries of Gravity in AdS,In this chapter we explore a physical model where the Virasoro group plays a key role, namely three-dimensional gravity on Anti-de Sitter (AdS) backgrounds and its putative dual two-dimensional conformal field theory (CFT). These considerations will be a basis and a guide for our study of asymptotically flat space-times in part III.作者: 吞下 時(shí)間: 2025-3-25 08:26
Classical BMS, SymmetryThe Bondi–Metzner–Sachs (BMS) group is an infinite-dimensional symmetry group of asymptotically flat gravity at null infinity, that extends Poincaré symmetry.作者: 貨物 時(shí)間: 2025-3-25 11:57 作者: LIMIT 時(shí)間: 2025-3-25 18:25 作者: EPT 時(shí)間: 2025-3-25 21:01
ConclusionWe have now completed our survey of the group-theoretic aspects of three-dimensional gravity, and in particular of BMS symmetry in three dimensions.作者: 轎車 時(shí)間: 2025-3-26 00:51
Charles X. Wang,Scott Webster,Sidong Zhangproblem that can be studied on the sole basis of symmetries, without any assumptions on the underlying microscopic theory. In this introduction we describe this strategy in some more detail, starting in Sect.?. with a broad overview of asymptotic symmetries in general and Bondi-Metzner-Sachs (BMS) s作者: CAJ 時(shí)間: 2025-3-26 04:32 作者: Amnesty 時(shí)間: 2025-3-26 12:10
NDE 4.0: Image and Sound Recognitionunitary representations, which are induced from representations of their translation subgroup combined with a so-called .. We interpret these representations as . propagating in space-time and having definite transformation properties under the corresponding symmetry group. This picture will be inst作者: 上漲 時(shí)間: 2025-3-26 16:18 作者: 改良 時(shí)間: 2025-3-26 18:54 作者: 宿醉 時(shí)間: 2025-3-26 21:35 作者: Console 時(shí)間: 2025-3-27 04:40
Blagoje OblakNominated as an outstanding PhD thesis by the Brussels Universities, Belgium and University of Cambridge, UK.Offers a self-contained and pedagogical presentation with numerous schematic drawings illus作者: 共和國(guó) 時(shí)間: 2025-3-27 07:53
Springer Theseshttp://image.papertrans.cn/b/image/180129.jpg作者: commensurate 時(shí)間: 2025-3-27 12:48 作者: VEN 時(shí)間: 2025-3-27 14:09
https://doi.org/10.1007/978-1-908517-60-9e remaining problem then is to write down explicit representations, so our goal in this chapter is to build Hilbert spaces of wavefunctions acted upon by a group of unitary transformations. Guided by group actions on homogeneous spaces, we will be led to the method of ..作者: 來(lái)自于 時(shí)間: 2025-3-27 21:16
Induced Representationse remaining problem then is to write down explicit representations, so our goal in this chapter is to build Hilbert spaces of wavefunctions acted upon by a group of unitary transformations. Guided by group actions on homogeneous spaces, we will be led to the method of ..作者: grandiose 時(shí)間: 2025-3-27 22:38
2190-5053 the field along the way. This makes it a highly rewarding read and a perfect starting point for anybody with a serious interest in the four-dimensional problem.978-3-319-87184-4978-3-319-61878-4Series ISSN 2190-5053 Series E-ISSN 2190-5061 作者: Employee 時(shí)間: 2025-3-28 05:06
Book 2017riginal results that have been obtained while learning a number of fundamental concepts in the field along the way. This makes it a highly rewarding read and a perfect starting point for anybody with a serious interest in the four-dimensional problem.作者: 圓木可阻礙 時(shí)間: 2025-3-28 09:04 作者: regale 時(shí)間: 2025-3-28 12:36 作者: 有害 時(shí)間: 2025-3-28 14:39 作者: Entreaty 時(shí)間: 2025-3-28 21:01
Semi-direct Productsunitary representations, which are induced from representations of their translation subgroup combined with a so-called .. We interpret these representations as . propagating in space-time and having definite transformation properties under the corresponding symmetry group. This picture will be inst作者: 推遲 時(shí)間: 2025-3-28 23:01
Coadjoint Orbits and Geometric Quantizationthe opposite phenomenon: starting from a . of a group ., we will obtain a representation by . the orbit. This construction will further explain why orbits of momenta classify representations of semi-direct products. In addition it will turn out to be a tool for understanding gravity in parts II and 作者: 夜晚 時(shí)間: 2025-3-29 05:24 作者: BROTH 時(shí)間: 2025-3-29 09:35
Virasoro Coadjoint Orbitsal for our purposes because they will turn out to coincide with the supermomentum orbits that classify BMS. particles. As we shall see, despite being infinite-dimensional, these orbits behave very much like the finite-dimensional coadjoint orbits of ..作者: 突襲 時(shí)間: 2025-3-29 11:54
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