-
6
-
-
4243923119
-
-
Heidelberg-Moscow Experiment, A. Balysh, Phys. Lett. B 356, 450 (1995).
-
(1995)
Phys. Lett. B
, vol.356
, pp. 450
-
-
Balysh, A.1
-
8
-
-
0343710604
-
-
Heidelberg- Moscow Experiment, L. Baudis, Phys. Lett. B 407, 219 (1997).
-
(1997)
Phys. Lett. B
, vol.407
, pp. 219
-
-
Baudis, L.1
-
13
-
-
85037231967
-
-
astro-ph/9707285
-
J.R. Primack, presented in the Jerusalem Winter School, 1996, astro-ph/9707285
-
-
-
Primack, J.R.1
-
17
-
-
0346727435
-
-
Super-Kamiohande Collaboration, Y. Fukuda, Phys. Lett. B 433, 9 (1998)
-
(1998)
Phys. Lett. B
, vol.433
, pp. 9
-
-
Fukuda, Y.1
-
24
-
-
0000667291
-
-
K. Zuber, Phys. Rep. 305, 295 (1998) we have corrected some printing errors in the mixing matrix given in this report.
-
(1998)
Phys. Rep.
, vol.305
, pp. 295
-
-
Zuber, K.1
-
25
-
-
85037250453
-
-
H. Päs (private communication).
-
-
-
Päs, H.1
-
29
-
-
85037240457
-
-
Although the observations of high redshift supernovae have been interpreted
-
Although the observations of high redshift supernovae have been interpreted 19 in terms of a nonvanishing cosmological constant (Formula presented) cosmological models with (Formula presented) do not provide good fit to the structure data (CMBR anisotropies and the large-scale structure). Leaving this puzzle to be resolved by the cosmologists, we shall stick to Eq. (6) and deduce the consequences for neutrino physics.
-
-
-
-
33
-
-
85037224572
-
-
astro-ph/9805200
-
B.P. Schmidt, astro-ph/9805200.
-
-
-
Schmidt, B.P.1
-
34
-
-
85037232335
-
-
Although specific value for (Formula presented) is mentioned here as well as below, it must be scaled suitably if the calculated value of the nuclear matrix element in neutrinoless double beta decay changes or if the experimental limit on this decay improves, since only the ratio of the upper limit of (Formula presented) to (Formula presented) enters into our analysis
-
Although specific value for (Formula presented) is mentioned here as well as below, it must be scaled suitably if the calculated value of the nuclear matrix element in neutrinoless double beta decay changes or if the experimental limit on this decay improves, since only the ratio of the upper limit of (Formula presented) to (Formula presented) enters into our analysis.
-
-
-
-
35
-
-
0009821069
-
-
M. Doi, Phys. Lett. 102B, 323 (1981)
-
(1981)
Phys. Lett.
, vol.102
, pp. 323
-
-
Doi, M.1
-
44
-
-
85037179203
-
-
fact this has already happened; according to Reference
-
In fact this has already happened; according to Reference 25, (Formula presented) at 90% C.L.
-
-
-
|