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Search for double-beta decay of $$\mathrm {^{130}Te}$$ to the $$0^+$$ states of $$\mathrm {^{130}Xe}$$ with CUORE
The CUORE experiment is a large bolometric array searching for the lepton number violating neutrino-less double beta decay ( $$0\nu \beta \beta $$ 0 ν β β ) in the isotope $$\mathrm {^{130}Te}$$ 130 Te . In this work we present the latest results on two searches for the double beta decay (DBD) of $$...
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Published in: | The European physical journal. C, Particles and fields Particles and fields, 2021-07, Vol.81 (7), Article 567 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
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Summary: | The CUORE experiment is a large bolometric array searching for the lepton number violating neutrino-less double beta decay (
$$0\nu \beta \beta $$
0
ν
β
β
) in the isotope
$$\mathrm {^{130}Te}$$
130
Te
. In this work we present the latest results on two searches for the double beta decay (DBD) of
$$\mathrm {^{130}Te}$$
130
Te
to the first
$$0^{+}_2$$
0
2
+
excited state of
$$\mathrm {^{130}Xe}$$
130
Xe
: the
$$0\nu \beta \beta $$
0
ν
β
β
decay and the Standard Model-allowed two-neutrinos double beta decay (
$$2\nu \beta \beta $$
2
ν
β
β
). Both searches are based on a 372.5 kg
$$\times $$
×
yr TeO
$$_2$$
2
exposure. The de-excitation gamma rays emitted by the excited Xe nucleus in the final state yield a unique signature, which can be searched for with low background by studying coincident events in two or more bolometers. The closely packed arrangement of the CUORE crystals constitutes a significant advantage in this regard. The median limit setting sensitivities at 90% Credible Interval (C.I.) of the given searches were estimated as
$$\mathrm {S^{0\nu }_{1/2} = 5.6 \times 10^{24} \, \mathrm {yr}}$$
S
1
/
2
0
ν
=
5.6
×
10
24
yr
for the
$${0\nu \beta \beta }$$
0
ν
β
β
decay and
$$\mathrm {S^{2\nu }_{1/2} = 2.1 \times 10^{24} \, \mathrm {yr}}$$
S
1
/
2
2
ν
=
2.1
×
10
24
yr
for the
$${2\nu \beta \beta }$$
2
ν
β
β
decay. No significant evidence for either of the decay modes was observed and a Bayesian lower bound at
$$90\%$$
90
%
C.I. on the decay half lives is obtained as:
$$\mathrm {(T_{1/2})^{0\nu }_{0^+_2} > 5.9 \times 10^{24} \, \mathrm {yr}}$$
(
T
1
/
2
)
0
2
+
0
ν
>
5.9
×
10
24
yr
for the
$$0\nu \beta \beta $$
0
ν
β
β
mode and
$$\mathrm {(T_{1/2})^{2\nu }_{0^+_2} > 1.3 \times 10^{24} \, \mathrm {yr}}$$
(
T
1
/
2
)
0
2
+
2
ν
>
1.3
×
10
24
yr
for the
$$2\nu \beta \beta $$
2
ν
β
β
mode. These represent the most stringent limits on the DBD of
$$^{130}$$
130
Te to excited states and improve by a factor
$$\sim 5$$
∼
5
the previous results on this process. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-021-09317-z |