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21.
In a vacuum spacetime equipped with the Bondi’s radiating metric which is asymptotically flat at spatial infinity including
gravitational radiation (Condition D), we establish the relation between the ADM total energy-momentum and the Bondi energy-momentum
for perturbed radiative spatial infinity. The perturbation is given by defining the “real” time as the sum of the retarded
time, the Euclidean distance and certain function f.
This work is partially supported by the National Natural Science Foundation of China (Grant Nos. 10231050, 10421001), the
National Key Basic Research Project of China (Grant No. 2006CB805905) and the Innovation Project of Chinese Academy of Sciences 相似文献
22.
Sebastiano Carpi 《Letters in Mathematical Physics》1998,45(3):259-267
We show that if A is the Haag–Kastler net generated by the energy-momentum tensor in a chiral quantum field theory, then every subsystem B A which is covariant under the action of SL(2,R given on A must coincide with A. The result is valid for all the allowed values of the central charge and is obtained using scaling limit techniques. 相似文献
23.
24.
Dan Solomon 《Central European Journal of Physics》2006,4(3):380-392
A common assumption in quantum field theory is that the energy-momentum 4-vector of any quantum state must be time-like. It
will be proven that this is not the case for a Dirac-Maxwell field. In this case quantum states can be shown to exist whose
energy-momentum is space-like. 相似文献
25.
In the light of the local Lorentz transformations and the general Noether theorem, a new formulate of the general covariant energy-momentum conservation law in f(R) gravity is obtained, which does not depend on the coordinative choice. 相似文献
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27.
利用半度规λ(α)μ表象的数学工具定义一个对广义坐标具有协变形式的重力场矢势函数ω(α)μ≡-cλ(α)μ,给出一个具有广义协变的包含重力场贡献的重力场方程Rμν-gμνR/2+Λgμν=8πG(T(Ⅰ)μν+T(Ⅱ)μν)
关键词:
重力场方程
协变形式
能量-动量张量
量子化 相似文献
28.
《Journal of Nonlinear Mathematical Physics》2013,20(4):580-594
The Lorentz-group of transformations usually consists of linear transformations of the coordinates, keeping as invariant the norm of the four-vector in (Minkowski) space-time. Besides those linear transformations, one may construct different forms of nonlinear transformations of the coordinates keeping unchanged that respective invariant. In this paper we explore nonlinear transformations of second-order which have a natural interpretation within the framework of Yamaleev's concept of the counterpart of rapidity (co-rapidity). The purpose of developed concept is to show that the formulae for energy and momentum of the relativistic particle become regular near the zero-mass and speed of light states. Furthermore, in a covariant formulation, the co-rapidity is presented as a four-vector which admits an extension of the Lorentz-group of transformations. In this paper we additionally show, that in the same way as the rapidity is related to the electromagnetic field, the co-rapidity is related to the field of strengths, which are given by a four-vector. The corresponding equations of such a field are also constructed. 相似文献
29.
In this paper we generalize the results of Part I to the submanifoldDirac operator. In particular, we give optimal lower bounds for thesubmanifold Dirac operator in terms of the mean curvature and othergeometric invariants as the Yamabe number or the energy-momentum tensor.In the limiting case, we prove that the submanifold is Einstein if thenormal bundle is flat. 相似文献
30.
Gamal G.L. Nashed 《中国物理 B》2011,20(11):110401-110401
We compute the total energy and the spatial momentum of four charged rotating (Kerr-Newman) frames by using the gravitational energy-momentum 3-form within the framework of the tetrad formulation of the general relativity theory. We show how the effect of the inertial always makes the total energy divergent. We use a natural regularization method, which yields the physical value for the total energy of the system. We show how the regularization method works on a number of different rotating frames that are related to each other by the local Lorentz transformation. We also show that the inertial has no effect on the spatial momentum components. 相似文献