TY - JOUR
T1 - Fine structure of beta decay end point spectrum
AU - Masood, Samina S.
AU - Nasri, Salah
AU - Schechter, Joseph
N1 - Funding Information:
We are grateful to Mariam Tortola for checking our equations and correcting an overall factor in Eq. (6). S. S. Masood would like to thank the Physics Department at Syracuse University for their hospitality. The work of S. Nasri is supported by National Science foundation grant No. PHY-0099. The work of J. Schechter is supported in part by the U.S. DOE under Contract No. DE-FG-02-85ER 40231.
PY - 2006/1/30
Y1 - 2006/1/30
N2 - We note that the fine structure at the end point region of the beta decay spectrum is now essentially known using neutrino oscillation data, if the mass of one neutrino is specified. This may help to identify the effects of nonzero neutrino masses in future experiments. We also give a compact description of the entire range of allowed neutrino masses as a function of the third neutrino mass, m3. A three neutrino assumption is being made. An exact treatment of phase space kinematics is used, in contrast to the conventional approximate formula. This work is independent of theoretical models; however, additional restrictions due to the assumption of a "complementary ansatz" for the neutrino mass matrix are also discussed. The ansatz implies that the values of the three neutrino masses should approximately be able to form a triangle. It is noted that most of the presently allowed neutrino mass sets have this triangular property.
AB - We note that the fine structure at the end point region of the beta decay spectrum is now essentially known using neutrino oscillation data, if the mass of one neutrino is specified. This may help to identify the effects of nonzero neutrino masses in future experiments. We also give a compact description of the entire range of allowed neutrino masses as a function of the third neutrino mass, m3. A three neutrino assumption is being made. An exact treatment of phase space kinematics is used, in contrast to the conventional approximate formula. This work is independent of theoretical models; however, additional restrictions due to the assumption of a "complementary ansatz" for the neutrino mass matrix are also discussed. The ansatz implies that the values of the three neutrino masses should approximately be able to form a triangle. It is noted that most of the presently allowed neutrino mass sets have this triangular property.
KW - Complementary ansatz
KW - Neutrino masses
KW - Neutrino oscillation constraints
KW - Tritium beta decay
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U2 - 10.1142/S0217751X06028552
DO - 10.1142/S0217751X06028552
M3 - Article
AN - SCOPUS:33644635787
SN - 0217-751X
VL - 21
SP - 517
EP - 531
JO - International Journal of Modern Physics A
JF - International Journal of Modern Physics A
IS - 3
ER -