標(biāo)題: Titlebook: Geometry, Particles, and Fields; Bj?rn Felsager Textbook 1998 Springer Science+Business Media New York 1998 Particle Physics.algebra.diffe [打印本頁] 作者: GERD847 時間: 2025-3-21 18:33
書目名稱Geometry, Particles, and Fields影響因子(影響力)
書目名稱Geometry, Particles, and Fields影響因子(影響力)學(xué)科排名
書目名稱Geometry, Particles, and Fields網(wǎng)絡(luò)公開度
書目名稱Geometry, Particles, and Fields網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Geometry, Particles, and Fields被引頻次
書目名稱Geometry, Particles, and Fields被引頻次學(xué)科排名
書目名稱Geometry, Particles, and Fields年度引用
書目名稱Geometry, Particles, and Fields年度引用學(xué)科排名
書目名稱Geometry, Particles, and Fields讀者反饋
書目名稱Geometry, Particles, and Fields讀者反饋學(xué)科排名
作者: 尊嚴(yán) 時間: 2025-3-21 21:39 作者: 滔滔不絕的人 時間: 2025-3-22 03:01
D. Leschi,N. Burais,J. Y. Gaspardve way. The string consists of “atoms.” Each atom interacts with its nearest neighbors. Hence, if one atom is disturbed, this disturbance has influence on its neighbor. But this disturbance of a neighbor has influence on the neighbor of the neighbor, etc.! In this way a traveling wave is created that propagates along the string!作者: adequate-intake 時間: 2025-3-22 05:24
Amplitude and Angle Modulation Systems,3; i.e., do the components ?.(x.…,x.) coincide with the components of some cotensor of rank 3? To investigate this we must try to show that the quantity ?..transforms covariantly. Therefore, we introduce new coordinates (y.…,y.).作者: 突襲 時間: 2025-3-22 08:59 作者: 銼屑 時間: 2025-3-22 13:30
Differential Forms and the Exterior Calculus3; i.e., do the components ?.(x.…,x.) coincide with the components of some cotensor of rank 3? To investigate this we must try to show that the quantity ?..transforms covariantly. Therefore, we introduce new coordinates (y.…,y.).作者: 銼屑 時間: 2025-3-22 18:52
Textbook 1998to the growing number of books that develop geometrical language and use it to describe new developments in particle physics...It provides clear treatment that is accessible to graduate students with a knowledge of advanced calculus and of classical physics...The second half of the book deals with t作者: Observe 時間: 2025-3-22 23:21 作者: 一條卷發(fā) 時間: 2025-3-23 02:24 作者: 替代品 時間: 2025-3-23 07:21
Integral Calculus on Manifolds, say, two variables .,y) defined on a “nice” subset . of?..Then we divide this region.into cells △.with area ∈.and in each cell, △.we choose a point.y.). (See Figure 8.1.) We can now form the Riemann sum:作者: surmount 時間: 2025-3-23 12:02
R. Wollast,M. Hinsenkamp,F. BurnyThe fundamental quantities of the electromagnetic field are the...(t, x) and.(t, x).作者: 情愛 時間: 2025-3-23 14:09 作者: Emmenagogue 時間: 2025-3-23 19:26
Sinusoidal Steady-state Analysis,In the remaining chapter of Part I we would like to include a few aspects of the quantum theory of fields and particles. To simplify the discussion, we begin our considerations with quantum mechanics of a single particle in one space dimension.作者: FLASK 時間: 2025-3-23 22:20 作者: Crayon 時間: 2025-3-24 04:13 作者: MORPH 時間: 2025-3-24 09:27 作者: 嗎啡 時間: 2025-3-24 11:37
Path Integrals and InstantonsIn the remaining chapter of Part I we would like to include a few aspects of the quantum theory of fields and particles. To simplify the discussion, we begin our considerations with quantum mechanics of a single particle in one space dimension.作者: induct 時間: 2025-3-24 16:50
Differentiable Manifolds—Tensor AnalysisTo simplify our discussion, we shall work entirely with subsets of Euclidean spaces! We will assume the reader to be familiar with Euclidean spaces, but to fix notation, some useful properties and definitions are collected in Figure 6.1.作者: Fabric 時間: 2025-3-24 22:38
978-1-4612-6846-8Springer Science+Business Media New York 1998作者: magnate 時間: 2025-3-25 00:05
Geometry, Particles, and Fields978-1-4612-0631-6Series ISSN 0938-037X 作者: Stricture 時間: 2025-3-25 04:59 作者: Confirm 時間: 2025-3-25 08:53 作者: Vital-Signs 時間: 2025-3-25 12:07 作者: 一再困擾 時間: 2025-3-25 16:21 作者: 遣返回國 時間: 2025-3-25 23:18 作者: SLAY 時間: 2025-3-26 02:28 作者: 并入 時間: 2025-3-26 07:18 作者: Spinous-Process 時間: 2025-3-26 09:27 作者: Nuance 時間: 2025-3-26 13:03 作者: Cirrhosis 時間: 2025-3-26 19:42
Origin and Detection of Bioelectric Signals“topological” properties. To keep the discussion as simple as possible, we will only consider classical field theories in (1 + 1)-space—time dimensions.(Although some of the results have suitable generalizations to higher dimensions, these generalizations are by no means trivial.)作者: immunity 時間: 2025-3-27 00:58 作者: Invertebrate 時間: 2025-3-27 04:16
Solitons“topological” properties. To keep the discussion as simple as possible, we will only consider classical field theories in (1 + 1)-space—time dimensions.(Although some of the results have suitable generalizations to higher dimensions, these generalizations are by no means trivial.)作者: 圖表證明 時間: 2025-3-27 09:16 作者: MOAN 時間: 2025-3-27 11:14 作者: single 時間: 2025-3-27 14:38 作者: Magisterial 時間: 2025-3-27 21:41
Dirac Monopolesve survived, although they will be extremely difficult to detect, mainly due to their large mass. Even if magnetic monopoles do not exist, the underlying mathematical model is very interesting, and it has had a great impact on our understanding of gauge theories.作者: Oligarchy 時間: 2025-3-27 23:37 作者: 朋黨派系 時間: 2025-3-28 05:41 作者: 手勢 時間: 2025-3-28 08:55 作者: Gratuitous 時間: 2025-3-28 11:46 作者: Salivary-Gland 時間: 2025-3-28 18:12
Integral Calculus on Manifoldsuld like to give an . feeling of the integral concept we are going to construct. In the familiar theory of Riemann integrals we consider a function of, say, two variables .,y) defined on a “nice” subset . of?..Then we divide this region.into cells △.with area ∈.and in each cell, △.we choose a point.作者: 顯而易見 時間: 2025-3-28 20:09
Dirac Monopolesxperiments, where electric fields are always generated by electrically charged particles, whereas magnetic fields are generated from electric currents. Nevertheless, there is a priori no reason to exclude magnetic charges, and as shown by Dirac (1931) their existence would have interesting theoretic作者: 誘導(dǎo) 時間: 2025-3-29 02:45 作者: 半身雕像 時間: 2025-3-29 05:24
Symmetries and Conservation Lawsntinuity(see (7.88)).The vector field . is interpreted as a “current,” and if Ω is a domain in a space slice, then the flux of . through Ω,given by the integral.is interpreted as a “charge.” (The minus sign is conventional. Compare with (8.53).)
