2001
DOI: 10.1103/physrevd.64.076005
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Rephasing-invariantCPviolating parameters with Majorana neutrinos

Abstract: We analyze the dependence of the squared amplitudes on the rephasing-invariant CP-violating parameters of the lepton sector, involving Majorana neutrinos, for various lepton-conserving and lepton-violating processes. We analyze the conditions under which the CP-violating effects in such processes vanish, in terms of the minimal set of rephasing invariants, giving special attention to the dependence on the extra CP-violating parameters that are due to the Majorana nature of the neutrinos.

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Cited by 71 publications
(93 citation statements)
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“…Since both mixing angles θ 13 and θ 23 depend on only one input parameter x. Then we can obtain the following sum rule sin 2 θ 23 = 1 2 ± tan θ 13 2 2 − tan 2 θ 13 1 2 ± √ 2 tan θ 13 2 , (C. 68) where "+" sign in ± is satisfied for x > 0 and "−" for x < 0. Given the experimental 3σ range of θ 13 , we have 0.602 ≤ sin 2 θ 23 ≤ 0.612 or 0.388 ≤ sin 2 θ 23 ≤ 0.398.…”
Section: Other Mixing Patterns With Iomentioning
confidence: 99%
“…Since both mixing angles θ 13 and θ 23 depend on only one input parameter x. Then we can obtain the following sum rule sin 2 θ 23 = 1 2 ± tan θ 13 2 2 − tan 2 θ 13 1 2 ± √ 2 tan θ 13 2 , (C. 68) where "+" sign in ± is satisfied for x > 0 and "−" for x < 0. Given the experimental 3σ range of θ 13 , we have 0.602 ≤ sin 2 θ 23 ≤ 0.612 or 0.388 ≤ sin 2 θ 23 ≤ 0.398.…”
Section: Other Mixing Patterns With Iomentioning
confidence: 99%
“…If this redefinition is performed, the number of phases is reduced to 3, i.e., the 2 Majorana phases on m 2 and m 3 and the Dirac phase δ. Notice that the phase δ is identified easily as the Dirac CP-violating phase from our above parametrization, as can be checked from the calculation of the Jarlskog invariant [41] (see [42][43][44][45][46][47][48][49][50][51][52][53][54] for other possible weak basis invariants).…”
Section: Jhep04(2015)069mentioning
confidence: 99%
“…The Dirac-type phases are determined by the four independent arguments of the quartets arg(V 1i V k j V * 1 j V * ki ), with i = j = k and the Majorana-type phases are given by the six independent arguments of the bilinears arg(V i j V * ik ), with j = k. In the SP, these phases are the minimal CP-violation quantities when neutrinos are Majorana particles [23,24,25,26,27,28,29].…”
Section: Cp Violationmentioning
confidence: 99%