標(biāo)題: Titlebook: An Introduction to Tensors and Group Theory for Physicists; Nadir Jeevanjee Textbook 20111st edition Springer Science+Business Media, LCC [打印本頁] 作者: 珍珠無 時(shí)間: 2025-3-21 16:08
書目名稱An Introduction to Tensors and Group Theory for Physicists影響因子(影響力)
書目名稱An Introduction to Tensors and Group Theory for Physicists影響因子(影響力)學(xué)科排名
書目名稱An Introduction to Tensors and Group Theory for Physicists網(wǎng)絡(luò)公開度
書目名稱An Introduction to Tensors and Group Theory for Physicists網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱An Introduction to Tensors and Group Theory for Physicists被引頻次
書目名稱An Introduction to Tensors and Group Theory for Physicists被引頻次學(xué)科排名
書目名稱An Introduction to Tensors and Group Theory for Physicists年度引用
書目名稱An Introduction to Tensors and Group Theory for Physicists年度引用學(xué)科排名
書目名稱An Introduction to Tensors and Group Theory for Physicists讀者反饋
書目名稱An Introduction to Tensors and Group Theory for Physicists讀者反饋學(xué)科排名
作者: Amendment 時(shí)間: 2025-3-21 21:41
An Introduction to Tensors and Group Theory for Physicists作者: 依法逮捕 時(shí)間: 2025-3-22 02:34 作者: FRET 時(shí)間: 2025-3-22 06:33
Vector Spaceshe component representation of vectors and linear operators from their existence as .. From here we move on to more advanced material, introducing dual spaces as well as non-degenerate Hermitian forms; the latter are the appropriate framework for the various scalar products that occur in physics. We作者: 畸形 時(shí)間: 2025-3-22 12:12 作者: 飛鏢 時(shí)間: 2025-3-22 15:22
Textbook 20111st editionhis material with that of Part I by introducing representation theory.??Exercises andexamples?are provided throughout for good practice in applying the presented definitions and techniques. Advanced undergraduate and graduate students in physics and applied mathematics will find clarity and insight 作者: 夜晚 時(shí)間: 2025-3-22 19:32 作者: 不可磨滅 時(shí)間: 2025-3-22 21:14 作者: 無能力 時(shí)間: 2025-3-23 01:55 作者: 披肩 時(shí)間: 2025-3-23 09:01
Springer Science+Business Media, LCC 2011作者: 造反,叛亂 時(shí)間: 2025-3-23 12:21 作者: 無法治愈 時(shí)間: 2025-3-23 15:28 作者: 打谷工具 時(shí)間: 2025-3-23 19:17
Daniela Schwarzer,Henrik Uterwedder many of the questions students often have when seeing tensors for the first time. In particular, we discuss the meaning of components and the origin of the tensor transformation law (which is taken as the definition of a tensor in the old-fashioned formulation), as well as the difference between a作者: BRIBE 時(shí)間: 2025-3-24 01:44
Daniela Schwarzer,Henrik Uterwedde dual spaces and non-degenerate Hermitian forms) which are also essential but usually are omitted in the standard ‘linear algebra for scientists and engineers’ course. This chapter also takes a more abstract point of view than that usually taken in lower-division linear algebra courses, in that it b作者: inundate 時(shí)間: 2025-3-24 03:11 作者: Ointment 時(shí)間: 2025-3-24 09:06 作者: 博愛家 時(shí)間: 2025-3-24 14:11
Daniela Schwarzer,Henrik Uterwedde. vectors under rotations, or antisymmetric tensors under boosts). We begin by defining a representation of a group as a vector space on which that group acts, and we give many examples, using the vector spaces we met in Chap.?. and the groups we met in Chap.?.. We then discuss how to take tensor pr作者: CHART 時(shí)間: 2025-3-24 16:50 作者: Fermentation 時(shí)間: 2025-3-24 22:18
A Quick Introduction to Tensorsr many of the questions students often have when seeing tensors for the first time. In particular, we discuss the meaning of components and the origin of the tensor transformation law (which is taken as the definition of a tensor in the old-fashioned formulation), as well as the difference between a作者: Vital-Signs 時(shí)間: 2025-3-25 02:48
Vector Spaces dual spaces and non-degenerate Hermitian forms) which are also essential but usually are omitted in the standard ‘linear algebra for scientists and engineers’ course. This chapter also takes a more abstract point of view than that usually taken in lower-division linear algebra courses, in that it b作者: 死貓他燒焦 時(shí)間: 2025-3-25 04:07 作者: pantomime 時(shí)間: 2025-3-25 10:56 作者: CRANK 時(shí)間: 2025-3-25 14:52
Basic Representation Theory. vectors under rotations, or antisymmetric tensors under boosts). We begin by defining a representation of a group as a vector space on which that group acts, and we give many examples, using the vector spaces we met in Chap.?. and the groups we met in Chap.?.. We then discuss how to take tensor pr作者: dialect 時(shí)間: 2025-3-25 15:59
The Wigner–Eckart Theorem and Other Applicationsmatrices and Dirac bilinears. We begin by discussing the perennially confusing concepts of vector operators and spherical tensors, and then unify them using the notion of a representation operator. We then use this framework to derive a generalized selection rule, from which the various quantum-mech作者: 饒舌的人 時(shí)間: 2025-3-25 20:28
Textbook 20111st editiontheoretical physics and applied mathematics. A particular aim is to demystify tensors and provide a unified framework for understanding them in the context of classical and quantum physics. Connecting the component formalism prevalent in physics calculations with the abstract but more conceptual for作者: labile 時(shí)間: 2025-3-26 00:11
Governance der EU-Datenschutzpolitikanical selection rules can be derived, and we also discuss the Wigner–Eckart theorem. We conclude by showing that Dirac’s famous gamma matrices can be understood in terms of representation operators, which then immediately gives the transformation properties of the ‘Dirac bilinears’ of QED.作者: Infuriate 時(shí)間: 2025-3-26 06:14 作者: Inveterate 時(shí)間: 2025-3-26 10:17 作者: 勛章 時(shí)間: 2025-3-26 16:02
s ample exercises for practice of the definitions and techni.An Introduction to Tensors and Group Theory for Physicists.?provides both?an intuitive and rigorous approach to tensors and groups and their role in theoretical physics and applied mathematics. A particular aim is to demystify tensors and 作者: 嘮叨 時(shí)間: 2025-3-26 18:10 作者: 攤位 時(shí)間: 2025-3-27 00:32 作者: 代理人 時(shí)間: 2025-3-27 02:01 作者: 分解 時(shí)間: 2025-3-27 08:29 作者: Extemporize 時(shí)間: 2025-3-27 09:47
Basic Representation Theoryations, which are in a sense the ‘smallest’ ones we can work with, and we compute these representations for .(2). These just end up being the familiar spin . representations, where . is a half-integer. We then use these results to compute the irreducible representations of the Lorentz group as well.作者: 噱頭 時(shí)間: 2025-3-27 15:23
9樓作者: 不如屎殼郎 時(shí)間: 2025-3-27 20:32
9樓作者: Slit-Lamp 時(shí)間: 2025-3-28 01:43
10樓作者: frenzy 時(shí)間: 2025-3-28 04:30
10樓作者: 悄悄移動 時(shí)間: 2025-3-28 06:56
10樓作者: 安定 時(shí)間: 2025-3-28 12:35
10樓