-
2
-
-
85038347534
-
-
Our space-time metric is (Formula presented) while (Formula presented) designates a generic element of the two-dimensional antisymmetric unit matrix (Formula presented)
-
Our space-time metric is (Formula presented) while (Formula presented) designates a generic element of the two-dimensional antisymmetric unit matrix (Formula presented).
-
-
-
-
5
-
-
25744468395
-
-
Phys. Rev. D52, R4277 (1995).
-
(1995)
Phys. Rev. D
, vol.52
-
-
-
6
-
-
0003425766
-
-
Belfer Graduate School on Science, Yeshiva University, New York
-
P. A. M. Dirac, Lectures on Quantum Mechanics (Belfer Graduate School on Science, Yeshiva University, New York, 1964).
-
(1964)
Lectures on Quantum Mechanics
-
-
Dirac, P.A.M.1
-
9
-
-
85038332145
-
-
H. O. Girotti, Classical and Quantum Dynamics of Constrained Systems, Lectures in Proceedings of the (Formula presented) Jorge Andre Swieca Summer School, edited by O. J. P. Eboli, M. Gomes, and A. Santoro (World Scientific, Singapore, 1990), pp. 1–77
-
H. O. Girotti, Classical and Quantum Dynamics of Constrained Systems, Lectures in Proceedings of the (Formula presented) Jorge Andre Swieca Summer School, edited by O. J. P. Eboli, M. Gomes, and A. Santoro (World Scientific, Singapore, 1990), pp. 1–77.
-
-
-
-
10
-
-
36149005338
-
-
Also see C. Itzykson and J-B. Zuber, Quantum Field Theory (McGraw-Hill, Singapore, 1985)
-
J. Schwinger, Phys. Rev.127, 324 (1962). Also see C. Itzykson and J-B. Zuber, Quantum Field Theory (McGraw-Hill, Singapore, 1985).
-
(1962)
Phys. Rev.
, vol.127
, pp. 324
-
-
Schwinger, J.1
-
11
-
-
85038279262
-
-
J. Schwinger, Particles, Sources and Fields (Addison-Wesley, New York, 1970), Vol. I
-
J. Schwinger, Particles, Sources and Fields (Addison-Wesley, New York, 1970), Vol. I.
-
-
-
-
13
-
-
85038313197
-
-
The time label in the arguments of the fields will be omitted whenever it does not lead to confusion
-
The time label in the arguments of the fields will be omitted whenever it does not lead to confusion.
-
-
-
-
14
-
-
85038325414
-
-
We shall not distinguish between a quantum field operator and its classical counterpart
-
We shall not distinguish between a quantum field operator and its classical counterpart.
-
-
-
-
15
-
-
85038313906
-
-
Recall that (Formula presented) is not Lorentz scalar and that a set of four quantities (Formula presented), obeying the Coulomb condition do not transform as components of a four-vector under Lorentz boosts
-
Recall that (Formula presented) is not Lorentz scalar and that a set of four quantities (Formula presented), obeying the Coulomb condition do not transform as components of a four-vector under Lorentz boosts.
-
-
-
|