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the Gliozzi-Scherk-Olive (GS0) projection [177]. An alternative light-cone gauge action with manifest spacetime supersymmetry was then proposed by Green and Schwarz [178] and shown by them to be equivalent (by virtue of the triality property of the Spin(8) transverse rotation group) to the light-con
Physics 10 (1974) 363-384. [54] L. Iorio, "Constraints on Galileon-induced precessions from solar system orbital motions" JCAP 07 (2012) 001 [55] R. Jackiw and S.-Y. Pi, "Tutorial on Scale and Conformal Symmetries in Diverse Dimensions" 3. Phys. A44 (2011) 223001, arXiv:1101.4886 [math-ph], and referenc
This fact can perhaps be understood most directly by recalling that the effective action is the generating functional for one- particle irreducible Green's functions, which themselves are gauge dependent [28]. In practice one often neglects this sub- tlety, fixes the gauge at the start of the calculat
okopec and J. Weenink, (2014), arXiv:1403.3219. [26] D. Buttaz2o er at, (2013), arXiv:1307.3536. [27] S. Weinberg, Phys.Rev. D7, 2887 (1973). [28] R. Jackiw. Phys. Rev. D9, 1686 (1974). [29] L. Dolan and R. Jackiw, Phys.Rev. D9. 2904 (1974). 30] J. Kang. Phys.Rev. D10, 3455 (1974). 31] N. K. Nielsen, N
This fact can perhaps be understood most directly by recalling that the effective action is the generating functional for one- particle irreducible Green's functions, which themselves arc gauge dependent [28]. In practice one often neglects this sub- tlety, fixes the gauge at the start of the calculat
Prokopec and J. Weenink, (2014), arXiv:1403.3219. [261 D. Donau° a at, (2013). arXiv:1307.3536. [27] S. Weinberg, Phys.Rev. D7, 2887 (1973). [28] R. Jackiw, Phys. Rev. 139. 1686(1974). [29] L. Dolan and R. Jackiw, Phys.Rev. 139, 2904 (1974). (A10) 1301 J. Kang, Phys.Rev. DIO, 3455 (1974). [311 N. K.
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