Titlebook: Hamiltonian Field Theory in the Radiating Regime; Piotr T. Chru?ciel,Jacek Jezierski,Jerzy Kijowski Book 2002 Springer-Verlag Berlin Heide

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書目名稱Hamiltonian Field Theory in the Radiating Regime影響因子(影響力)




書目名稱Hamiltonian Field Theory in the Radiating Regime影響因子(影響力)學(xué)科排名




書目名稱Hamiltonian Field Theory in the Radiating Regime網(wǎng)絡(luò)公開度




書目名稱Hamiltonian Field Theory in the Radiating Regime網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Hamiltonian Field Theory in the Radiating Regime被引頻次




書目名稱Hamiltonian Field Theory in the Radiating Regime被引頻次學(xué)科排名




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書目名稱Hamiltonian Field Theory in the Radiating Regime年度引用學(xué)科排名




書目名稱Hamiltonian Field Theory in the Radiating Regime讀者反饋




書目名稱Hamiltonian Field Theory in the Radiating Regime讀者反饋學(xué)科排名

Mettle

Radiating scalar fields,aOnaaCaaaleqabaGaeqiVd0Ma% eqyVd4gaaOGaeyOaIy7aaSbaaSqaaiabe27aUbqabaGccqWGMbGzcq% GGUaGlaaa!5E49![p^mu = frac{{partial L}}{{partial f_{,mu } }} =- sqrt { - det eta _{alpha eta } } eta ^{mu u } partial _ uf.] The canonical momentum . is defined as in equation (3.18): . Let ? be any piecewise smoot

大火

0940-7677 the case of Einstein gravity. The Hamiltonian role of the Trautman--Bondi mass is exhibited. A Hamiltonian definition of angular momentum at null infinity is derived and analysed.978-3-642-07681-7978-3-540-45604-9Series ISSN 0940-7677

驕傲

Verify

Basilar-Artery

dithiolethione

LIEN

https://doi.org/10.1007/978-3-319-63847-8 to consider motions of hypersurfaces which do not arise from the flow of a vector field; we shall indeed encounter such motions in Sect. 4.5 below. The purpose of this chapter is to generalize the framework of Kijowski and Tulczyjew to allow for such situations.

奇怪

Preliminaries,e following chapters that the dynamics of the massless scalar field in the radiation regime, as well as that of the gravitational field in the radiation regime, satisfies the requirements of the definitions given in this chapter.

Insensate

Hamiltonian flows for geometric field theories, to consider motions of hypersurfaces which do not arise from the flow of a vector field; we shall indeed encounter such motions in Sect. 4.5 below. The purpose of this chapter is to generalize the framework of Kijowski and Tulczyjew to allow for such situations.