標題: Titlebook: Geometry of the Fundamental Interactions; On Riemann‘s Legacy M. D. Maia Book 2011 Springer Science+Business Media, LLC 2011 Minkowski‘s s [打印本頁] 作者: Agitated 時間: 2025-3-21 18:52
書目名稱Geometry of the Fundamental Interactions影響因子(影響力)
書目名稱Geometry of the Fundamental Interactions影響因子(影響力)學科排名
書目名稱Geometry of the Fundamental Interactions網絡公開度
書目名稱Geometry of the Fundamental Interactions網絡公開度學科排名
書目名稱Geometry of the Fundamental Interactions被引頻次
書目名稱Geometry of the Fundamental Interactions被引頻次學科排名
書目名稱Geometry of the Fundamental Interactions年度引用
書目名稱Geometry of the Fundamental Interactions年度引用學科排名
書目名稱Geometry of the Fundamental Interactions讀者反饋
書目名稱Geometry of the Fundamental Interactions讀者反饋學科排名
作者: Muffle 時間: 2025-3-21 20:14 作者: arabesque 時間: 2025-3-22 00:42 作者: Heart-Rate 時間: 2025-3-22 07:42
The Physical Manifold,The basic concept of a physical space was formulated by Kant in his Critique of Pure reason 1781, where he used the word . to describe the set of all . [42]. Except for the lack of specification of a geometry and of the measurement conditions, Kant’s concept of physical space is very close to our present notion of space–time.作者: 無能力之人 時間: 2025-3-22 10:50
Herbert Stein,Wolfgang Stein,Andreas Erkensatter, but it is not impossible that some other force will assume such fundamental role in the future. However, not everyone agrees that there are compelling evidences for such assumption, at least within a simple and understandable argument in the Occam sense. Indeed, recent cosmological evidences 作者: 巧思 時間: 2025-3-22 13:58 作者: 巧思 時間: 2025-3-22 18:56
https://doi.org/10.1007/978-3-322-92392-9with the notions of physical space and of symmetry groups, the observables and the conditions of observations complete the basic elements of a physical theory..The observables themselves are usually invariant quantities in the sense that they can be measurable by different observers in different tim作者: MEAN 時間: 2025-3-22 23:06 作者: conscribe 時間: 2025-3-23 03:25
,Das pneumatische Relativl?ngenme?verfahren,dinates are no longer enumerable. A simple but very intuitive example is given in [55, 82]..We emphasize what we have already said in Chapter 1: Point particles do not exist as a physically observable object, carrying mass, charge, momentum, spin, and other attributes in space–time. Regardless of th作者: corn732 時間: 2025-3-23 07:09 作者: 額外的事 時間: 2025-3-23 11:28
Aufbau und Prinzipien der Untersuchung,oether in 1918 [10, 105, 106], showing how to construct the observables of a theory, given its Lagrangian and Lie symmetry groups. Following Lopes, for pedagogical purposes we divide the theorem in three parts, one for each kind of symmetry considered: transformation of coordinates in space–time, gl作者: 定點 時間: 2025-3-23 14:36
Personale Merkmale und Gesundheitsrisiken,as to make the action principle invariant. The invariance of the action means that it must be the same for all observers (when considering coordinate transformations) and for the observable fields (when referring to gauge transformations). It has to be such invariant to fulfill the purposes of Maupe作者: Galactogogue 時間: 2025-3-23 19:48
Ergebnisse der empirischen Untersuchung,rent usages for the designation .. One is the general definition of the Riemann tensor by a displacement of a vector field around a parallelogram as seen in Chapter 2. The other, more common in the applications to Einstein’s equations, is the expression of the Riemann tensor specifically calculated 作者: 準則 時間: 2025-3-24 00:12
Einsatz von Bastfasergarnen in der Wirkereiactions. This apparent paradox exists because gravitation does not seem to fit in the same scheme of the gauge interactions as described in the preceding chapters. Contrarily to the gauge theories, Einstein’s gravitation has not been quantized, either from the canonical, or from the perturbative poi作者: Externalize 時間: 2025-3-24 06:03 作者: 刺耳 時間: 2025-3-24 06:31
Gauge Fields,rent usages for the designation .. One is the general definition of the Riemann tensor by a displacement of a vector field around a parallelogram as seen in Chapter 2. The other, more common in the applications to Einstein’s equations, is the expression of the Riemann tensor specifically calculated for the metric connection.作者: employor 時間: 2025-3-24 11:05 作者: Minutes 時間: 2025-3-24 15:34
https://doi.org/10.1007/978-1-4419-8273-5Minkowski‘s space time; Newton‘s space-time; Yang-Mills theory; coordinate symmetries; fiber bundles; noe作者: 積極詞匯 時間: 2025-3-24 19:19 作者: 烤架 時間: 2025-3-24 23:12 作者: 豐富 時間: 2025-3-25 05:46
https://doi.org/10.1007/978-3-322-88236-3lt of the Michelson–Morley experiment and the subsequent interpretation of the relative motion between observers and observables given by Einstein. This interpretation led us to the emergence of the Poincaré symmetry. From then on, the structure of . has become the essential tool to the understanding of the fundamental interactions.作者: forbid 時間: 2025-3-25 09:54
https://doi.org/10.1007/978-3-322-92392-9l theory..The observables themselves are usually invariant quantities in the sense that they can be measurable by different observers in different times. In this chapter we study the mathematical structure of observables, which may be in general derived from a tensor structure, but which is usually described as scalar, vector, and spinor fields.作者: Nonporous 時間: 2025-3-25 14:10
,Das pneumatische Relativl?ngenme?verfahren, particles do not exist as a physically observable object, carrying mass, charge, momentum, spin, and other attributes in space–time. Regardless of these attributes they always correspond to . in the parameter space .. which is not locally equivalent to the physical manifold.作者: 不適當 時間: 2025-3-25 18:43 作者: POLYP 時間: 2025-3-25 23:26 作者: Consequence 時間: 2025-3-26 03:36 作者: modest 時間: 2025-3-26 05:16
Tilo Pfeifer,Carlos Alberto Schneidertechnology, so that the concept of space–time is not static. In the following we review this process of evolution from Galilei to Einstein’s general relativity. Later on we discuss some future perspectives.作者: VOK 時間: 2025-3-26 12:23
The Fundamental Interactions,the dark component of the universe, composed of dark matter showing attractive gravitation and dark energy showing something like a repulsive gravitation. They are dark because they cannot be seen, like ordinary matter.作者: Bronchial-Tubes 時間: 2025-3-26 13:14 作者: 神刊 時間: 2025-3-26 17:42
Personale Merkmale und Gesundheitsrisiken,rtuis, Euler, Lagrange, and Hamilton. The modification of the derivative is quite intuitive when we are talking about coordinate transformations, but it is less intuitive when we are talking about field theory. In this chapter we will introduce the basic tools to the formal definition of gauge covariant derivatives.作者: Substitution 時間: 2025-3-26 23:54 作者: 注射器 時間: 2025-3-27 02:18
Bundles and Connections,rtuis, Euler, Lagrange, and Hamilton. The modification of the derivative is quite intuitive when we are talking about coordinate transformations, but it is less intuitive when we are talking about field theory. In this chapter we will introduce the basic tools to the formal definition of gauge covariant derivatives.作者: 有其法作用 時間: 2025-3-27 06:16
Gravitation,nts of view [41, 127]. On the side of classical physics the theory can describe the gravitational field of only about 4% of the known universe. The remaining 96% produces a gravitational effect that is not included in Einstein’s theory of gravitation.作者: 有限 時間: 2025-3-27 11:08
Symmetry,lt of the Michelson–Morley experiment and the subsequent interpretation of the relative motion between observers and observables given by Einstein. This interpretation led us to the emergence of the Poincaré symmetry. From then on, the structure of . has become the essential tool to the understanding of the fundamental interactions.作者: overshadow 時間: 2025-3-27 15:55
The Algebra of Observables,l theory..The observables themselves are usually invariant quantities in the sense that they can be measurable by different observers in different times. In this chapter we study the mathematical structure of observables, which may be in general derived from a tensor structure, but which is usually described as scalar, vector, and spinor fields.作者: 善變 時間: 2025-3-27 18:16
Scalar Fields, particles do not exist as a physically observable object, carrying mass, charge, momentum, spin, and other attributes in space–time. Regardless of these attributes they always correspond to . in the parameter space .. which is not locally equivalent to the physical manifold.作者: Macronutrients 時間: 2025-3-27 22:48
Vector, Tensor, and Spinor Fields,oretical and experimental results to the development of gauge theory let us briefly review the basics of the electromagnetic field (for more details, see, e.g., [93]) and some more advanced topics involving its interactions with scalar fields.作者: Anterior 時間: 2025-3-28 02:26 作者: prosperity 時間: 2025-3-28 10:14
Book 2011 fascinating window into the ongoing struggle of mankind to understand nature. The discovery of gauge fields and their properties is the most formidable landmark of modern physics. The expression of the gauge field strength as the curvature associated to a given connection, places quantum field theo作者: AGOG 時間: 2025-3-28 11:21
The Fundamental Interactions,atter, but it is not impossible that some other force will assume such fundamental role in the future. However, not everyone agrees that there are compelling evidences for such assumption, at least within a simple and understandable argument in the Occam sense. Indeed, recent cosmological evidences 作者: 別名 時間: 2025-3-28 17:49
Symmetry,onal structure of nature [59]. However, the awareness of the importance of symmetry in physics became clear only after the debate on the negative result of the Michelson–Morley experiment and the subsequent interpretation of the relative motion between observers and observables given by Einstein. Th作者: Console 時間: 2025-3-28 20:22
The Algebra of Observables,with the notions of physical space and of symmetry groups, the observables and the conditions of observations complete the basic elements of a physical theory..The observables themselves are usually invariant quantities in the sense that they can be measurable by different observers in different tim作者: interior 時間: 2025-3-29 00:46
,Geometry of Space–Times,wing how the physics of space–time determines the geometry. In this, we were much influenced by Penrose’s writings and lectures [71]..As we have detailed in the introduction, we take the physical manifold as the space of perceptions in the sense of Kant. These perceptions are in one way or another a作者: ANTI 時間: 2025-3-29 03:22
Scalar Fields,dinates are no longer enumerable. A simple but very intuitive example is given in [55, 82]..We emphasize what we have already said in Chapter 1: Point particles do not exist as a physically observable object, carrying mass, charge, momentum, spin, and other attributes in space–time. Regardless of th作者: 四目在模仿 時間: 2025-3-29 10:53
Vector, Tensor, and Spinor Fields,ysics, including the emergence of relativity and the relevance of the concept of symmetry in physics. Due to the importance of this combination of theoretical and experimental results to the development of gauge theory let us briefly review the basics of the electromagnetic field (for more details,
