Academic literature on the topic 'Leptonic CP Violation'

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Journal articles on the topic "Leptonic CP Violation"

1

LIU, YONG, and UTPAL SARKAR. "CP VIOLATION IN NEUTRINO MIXING MATRIX AND LEPTOGENESIS." Modern Physics Letters A 16, no. 09 (2001): 603–13. http://dx.doi.org/10.1142/s0217732301003528.

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The CP violation required in leptogenesis may have different origin, but in an effective theory they are all related to the rephasing invariant CP violating measures in the mixing matrix of the leptonic sector. We point out that with our present knowledge of the mixing angles it is possible to estimate the maximum allowed value for all the rephasing invariant measures of CP violation in the leptonic sector. In the effective three-generation scenario there are three CP violating rephasing invariant measures. We show that only one rephasing invariant measure enters the lepton number conserving processes while the other two enter the lepton number violating processes. In the bimaximal mixing case, the lepton number conserving measure of CP violation vanishes while the two lepton number violating rephasing invariant measures of CP violation remain nonzero, which could contribute to the lepton asymmetry of the universe.
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2

Maalampi, J., and K. Mursula. "Leptonic CP-violation and mirror leptons." Nuclear Physics B 269, no. 1 (1986): 109–18. http://dx.doi.org/10.1016/0550-3213(86)90368-8.

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3

Petcov, S. T. "Leptonic CP violation and leptogenesis." International Journal of Modern Physics A 29, no. 11n12 (2014): 1430028. http://dx.doi.org/10.1142/s0217751x14300282.

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The phenomenology of 3-neutrino mixing, the current status of our knowledge about the 3-neutrino mixing parameters, including the absolute neutrino mass scale, and of the Dirac and Majorana CP violation in the lepton sector, are reviewed. The problems of CP violation in neutrino oscillations and of determining the nature — Dirac or Majorana — of massive neutrinos, are discussed. The seesaw mechanism of neutrino mass generation and the related leptogenesis scenario of generation of the baryon asymmetry of the universe, are considered. The results showing that the CP violation necessary for the generation of the baryon asymmetry of the universe in leptogenesis can be due exclusively to the Dirac and/or Majorana CP-violating phase(s) in the neutrino mixing matrix U, are briefly reviewed.
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4

Hagedorn, C. "Leptonic CP violation theory." Journal of Physics: Conference Series 888 (September 2017): 012027. http://dx.doi.org/10.1088/1742-6596/888/1/012027.

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5

NASRI, S., J. SCHECHTER, and S. MOUSSA. "STUDY OF LEPTONIC CP VIOLATION." International Journal of Modern Physics A 19, no. 31 (2004): 5367–75. http://dx.doi.org/10.1142/s0217751x04022608.

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The "complementary" Ansatz, Tr (Mν)=0, where Mν is the prediagonal neutrino mass matrix, seems a plausible approximation for capturing in a self contained way some of the content of Grand Unification. We study its consequences in the form of relations between the neutrino masses and CP violation phases.
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6

Grossman, Yuval. "Leptonic flavor and CP violation." Pramana 62, no. 2 (2004): 269–81. http://dx.doi.org/10.1007/bf02705088.

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7

Zeen Devi, H. "Correlations between low energy leptonic CP violation and leptogenesis in the light of recent experiments." International Journal of Modern Physics A 29, no. 20 (2014): 1450104. http://dx.doi.org/10.1142/s0217751x14501048.

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Leptogenesis is the most favorable mechanism for generating the observed baryon asymmetry of the universe (BAU) which implies CP violation in the high energy scale. The low energy leptonic CP violation is expected to be observed in the neutrino oscillations and 0ν2β decay experiments. Generally, it is not possible to connect both the CP violations. Here we revisit the issue of connecting the two in flavored leptogenesis scenario within the Type I seesaw in the light of recent neutrino oscillation and Planck data. With the recent precise measurements of θ13 and BAU, we are able to find new correlations between the low and high energy CP violating phases when leptogenesis occurs at temperature between 109 to 1012 GeV and there is no contribution to CP violation from the heavy neutrino sector.
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8

Ahuja, Gulsheen, and Samandeep Sharma. "Texture zero mass matrices and CP violation." International Journal of Modern Physics A 32, no. 16 (2017): 1742005. http://dx.doi.org/10.1142/s0217751x17420052.

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Within the Standard Model, using the facility of making Weak Basis transformations, attempt has been made to examine the most general mass matrices within the texture zero approach. For the case of quarks, interestingly, one finds a particular set of texture four zero quark mass matrices emerging out to be a unique viable option for the description of quark mixing data as well as for accommodation of CP violation. Similarly, general lepton mass matrices, essentially considered as texture zero mass matrices, yield interesting bounds on the CP violating Jarlskog’s rephasing invariant parameter in the leptonic sector.
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9

Tandean, Jusak, and G. Valencia. "CP violation in non-leptonic decays." Physics Letters B 451, no. 3-4 (1999): 382–87. http://dx.doi.org/10.1016/s0370-2693(99)00173-2.

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10

Minakata, Hisakazu, and Shinji Watanabe. "Solar neutrinos and leptonic CP violation." Physics Letters B 468, no. 3-4 (1999): 256–60. http://dx.doi.org/10.1016/s0370-2693(99)01224-1.

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