scholarly journals Improved lower bounds on partial lifetimes for nucleon decay modes

2019 ◽  
Vol 100 (11) ◽  
Author(s):  
Sudhakantha Girmohanta ◽  
Robert Shrock
1997 ◽  
Vol 411 (3-4) ◽  
pp. 326-329 ◽  
Author(s):  
J-F. Glicenstein
Keyword(s):  

2001 ◽  
Vol 16 (supp01b) ◽  
pp. 855-859 ◽  
Author(s):  
◽  
KENNETH S. GANEZER

We have analyzed 1144 days of Super-Kamiokande data for 13 of the more than 40 possible nucleon decay modes. We have studied p→e+π0, and twelve other two particle B-L conserving decay modes including those with kaons that are preferred in supersymmetric theories. Most modes are currently free of candidate events. In all cases the number of candidates is consistent with atmospheric neutrino induced backgrounds. We have calculated 90% confidence level single sided lower limits on the lifetime of the neutron and proton (divided by the unknown branching ratio) for the studied modes. All of our lower limits are higher than previous best limits by a factor of 2-10. Our limit for p→e+π0 is now 4.4×1033 years.


1989 ◽  
Vol 313 (3) ◽  
pp. 509-540 ◽  
Author(s):  
Ch. Berger ◽  
M. Fröhlich ◽  
H. Mönch ◽  
R. Nisius ◽  
F. Raupach ◽  
...  
Keyword(s):  

Author(s):  
C. Alduino ◽  
K. Alfonso ◽  
D. R. Artusa ◽  
F. T. Avignone III ◽  
O. Azzolini ◽  
...  

Abstract We report on a search for double beta decay of $$^{130}\hbox {Te}$$130Te to the first $$0^{+}$$0+ excited state of $$^{130}\hbox {Xe}$$130Xe using a $$9.8\,\hbox {kg}\cdot \hbox {yr}$$9.8kg·yr exposure of $$^{130}\hbox {Te}$$130Te collected with the CUORE-0 experiment. In this work we exploit different topologies of coincident events to search for both the neutrinoless and two-neutrino double beta decay modes. We find no evidence for either mode and place lower bounds on the half-lives: $$T^{0\nu }_{0^+_1}>7.9\cdot 10^{23}\hbox {yr}$$T01+0ν>7.9·1023yr and $$T^{2\nu }_{0^+_1}>2.4\cdot 10^{23}\hbox {yr}$$T01+2ν>2.4·1023yr ($$90\%\,\hbox {CL}$$90%CL). Combining our results with those obtained by the CUORICINO experiment, we achieve the most stringent constraints available for these processes: $$T^{0\nu }_{0^+_1}>1.4\cdot 10^{24}\hbox {yr}$$T01+0ν>1.4·1024yr and $$T^{2\nu }_{0^+_1}>2.5\cdot 10^{23}\hbox {yr}$$T01+2ν>2.5·1023yr ($$90\%\,\hbox {CL}$$90%CL).


1991 ◽  
Vol 269 (1-2) ◽  
pp. 227-233 ◽  
Author(s):  
C. Berger ◽  
M. Fröhlich ◽  
H. Mönch ◽  
R. Nisius ◽  
F. Raupach ◽  
...  
Keyword(s):  

1991 ◽  
Vol 50 (3) ◽  
pp. 385-394 ◽  
Author(s):  
◽  
Ch. Berger ◽  
M. Fr�hlich ◽  
H. M�nch ◽  
R. Nisius ◽  
...  

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