The investigation of CP violation through the decay of polarized tau leptons

Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics

Volumn 378, Issue 1-4, 1996, Pages 272-278

  Tsai, Yung Su ^a  

^a SLAC NATIONAL ACCELERATOR LABORATORY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0001690539     PISSN: 03702693     EISSN: None     Source Type: Journal    
DOI: 10.1016/0370-2693(96)00403-0     Document Type: Article

References (21)

1. Y.S. Tsai, Phys. Rev. D51 (1995) 3172.
2. Y.S. Tsai, "Test of T and CP violation in Leptonic Decay of tau" in the Proceedings of the Workshop on the Tau/Charm Factory, Argonne National Laboratory, June 21-23, 1995, Edited by Jose Repond, AIP Press, New York (1995).
3. ∓" in the Proceedings of the Workshop on the Tau/Charm Factory, Argonne National Laboratory, June 21-23, 1995, Edited by Jose Repond, AIP Press, New York (1995).
4. 2 ... are independent of spin of the exchanged particle.
5. S. Goozovat and C.A. Nelson, Phys. Lett. B267 (1991) 128.
6. Kaoru Yokoya, private communication made during the Tau/Charm Factory Workshop, February 5-9, 1996 Beijing.
7. ∓" in the Proceedings of the Tau/Charm Factory Workshop, SLAC, May 23-27, 1989, edited by Lydia V. Beers, SLAC Report 343, SLAC (1989).
8. Vera Luth, a speech made at SLAC 2000 on February 24, 1996.
9. T.D. Lee, Phys. Rev. D8 (1973) 1226; Phys. Rep. 9C (1974) 143.
10. T.D. Lee, Phys. Rev. D8 (1973) 1226; Phys. Rep. 9C (1974) 143.
11. Y.S. Tsai, Phys. Rev. 120 (1960) 269, Eq. (7).
12. F. Hoogeveen and L. Stodolsky, Phys. Lett. B 212 (1988) 505; G. Couture, ibid. B272 (1991) 404; W. Bernreuther and O. Nachtmann, Phys. Rev. Lett. 63 (1989) 2787; W. Bernreuther, G.W. Botz, O. Nachtmann and P. Overmann, Z. Phys. C 52 (1991) 567; W. Bernreuther, O. Nachtmann, P. Overmann, Phys. Rev. D48 (1993) 78; B. Aranthanarayan and S.D. Rindani, Phys. Rev. Lett. 73 (1994) 1215.
13. F. Hoogeveen and L. Stodolsky, Phys. Lett. B 212 (1988) 505; G. Couture, ibid. B272 (1991) 404; W. Bernreuther and O. Nachtmann, Phys. Rev. Lett. 63 (1989) 2787; W. Bernreuther, G.W. Botz, O. Nachtmann and P. Overmann, Z. Phys. C 52 (1991) 567; W. Bernreuther, O. Nachtmann, P. Overmann, Phys. Rev. D48 (1993) 78; B. Aranthanarayan and S.D. Rindani, Phys. Rev. Lett. 73 (1994) 1215.
14. F. Hoogeveen and L. Stodolsky, Phys. Lett. B 212 (1988) 505; G. Couture, ibid. B272 (1991) 404; W. Bernreuther and O. Nachtmann, Phys. Rev. Lett. 63 (1989) 2787; W. Bernreuther, G.W. Botz, O. Nachtmann and P. Overmann, Z. Phys. C 52 (1991) 567; W. Bernreuther, O. Nachtmann, P. Overmann, Phys. Rev. D48 (1993) 78; B. Aranthanarayan and S.D. Rindani, Phys. Rev. Lett. 73 (1994) 1215.
15. F. Hoogeveen and L. Stodolsky, Phys. Lett. B 212 (1988) 505; G. Couture, ibid. B272 (1991) 404; W. Bernreuther and O. Nachtmann, Phys. Rev. Lett. 63 (1989) 2787; W. Bernreuther, G.W. Botz, O. Nachtmann and P. Overmann, Z. Phys. C 52 (1991) 567; W. Bernreuther, O. Nachtmann, P. Overmann, Phys. Rev. D48 (1993) 78; B. Aranthanarayan and S.D. Rindani, Phys. Rev. Lett. 73 (1994) 1215.
16. F. Hoogeveen and L. Stodolsky, Phys. Lett. B 212 (1988) 505; G. Couture, ibid. B272 (1991) 404; W. Bernreuther and O. Nachtmann, Phys. Rev. Lett. 63 (1989) 2787; W. Bernreuther, G.W. Botz, O. Nachtmann and P. Overmann, Z. Phys. C 52 (1991) 567; W. Bernreuther, O. Nachtmann, P. Overmann, Phys. Rev. D48 (1993) 78; B. Aranthanarayan and S.D. Rindani, Phys. Rev. Lett. 73 (1994) 1215.
17. F. Hoogeveen and L. Stodolsky, Phys. Lett. B 212 (1988) 505; G. Couture, ibid. B272 (1991) 404; W. Bernreuther and O. Nachtmann, Phys. Rev. Lett. 63 (1989) 2787; W. Bernreuther, G.W. Botz, O. Nachtmann and P. Overmann, Z. Phys. C 52 (1991) 567; W. Bernreuther, O. Nachtmann, P. Overmann, Phys. Rev. D48 (1993) 78; B. Aranthanarayan and S.D. Rindani, Phys. Rev. Lett. 73 (1994) 1215.
18. -8 cm e that does not have anything to do with T and P violations. The water molecule is not rotationally symmetric, hence the usual argument that the electrical dipole moment being a vector must be proportional to the spin of the particle does not apply. Hence it violates neither P nor T. Tau being an elementary particle can no have this kind of dipole moment.
19. -5 and thus cannot be detected even with the future Tau/Charm Factory. It can barely detect this kind of correlation of the magnitude α/π due to the final state electromagnetic interaction.
20. -5 and thus cannot be detected even with the future Tau/Charm Factory. It can barely detect this kind of correlation of the magnitude α/π due to the final state electromagnetic interaction.
21. -5 and thus cannot be detected even with the future Tau/Charm Factory. It can barely detect this kind of correlation of the magnitude α/π due to the final state electromagnetic interaction.