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First evidence for the two-body charmless baryonic decay $ {B^0}\to p\overline{p} $
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Abstract
The results of a search for the rare two-body charmless baryonic decays
$ {B^0}\to p\overline{p} $
and
$ B_s^0\to p\overline{p} $
are reported. The analysis uses a data sample, corresponding to an integrated luminosity of 0.9 fb−1, of pp collision data collected by the LHCb experiment at a centre-of-mass energy of 7 TeV. An excess of
$ {B^0}\to p\overline{p} $
candidates with respect to background expectations is seen with a statistical significance of 3.3 standard deviations. This is the first evidence for a two-body charmless baryonic B
0 decay. No significant
$ B_s^0\to p\overline{p} $
signal is observed, leading to an improvement of three orders of magnitude over previous bounds. If the excess events are interpreted as signal, the 68.3% confidence level intervals on the branching fractions are
$ \begin{array}{*{20}{c}} {\mathcal{B}\left( {{B^0}\to p\overline{p}} \right)=1.47_{-0.51-0.14}^{+0.62+0.35}\times {10^{-8 }},} \hfill \\ {\mathcal{B}\left( {{B^s}\to p\overline{p}} \right)=2.84_{-1.68-0.18}^{+2.03+0.85}\times {10^{-8 }},} \hfill \\ \end{array} $
where the first uncertainty is statistical and the second is systematic.
Springer Science and Business Media LLC
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Title: First evidence for the two-body charmless baryonic decay $ {B^0}\to p\overline{p} $
Description:
Abstract
The results of a search for the rare two-body charmless baryonic decays
$ {B^0}\to p\overline{p} $
and
$ B_s^0\to p\overline{p} $
are reported.
The analysis uses a data sample, corresponding to an integrated luminosity of 0.
9 fb−1, of pp collision data collected by the LHCb experiment at a centre-of-mass energy of 7 TeV.
An excess of
$ {B^0}\to p\overline{p} $
candidates with respect to background expectations is seen with a statistical significance of 3.
3 standard deviations.
This is the first evidence for a two-body charmless baryonic B
0 decay.
No significant
$ B_s^0\to p\overline{p} $
signal is observed, leading to an improvement of three orders of magnitude over previous bounds.
If the excess events are interpreted as signal, the 68.
3% confidence level intervals on the branching fractions are
$ \begin{array}{*{20}{c}} {\mathcal{B}\left( {{B^0}\to p\overline{p}} \right)=1.
47_{-0.
51-0.
14}^{+0.
62+0.
35}\times {10^{-8 }},} \hfill \\ {\mathcal{B}\left( {{B^s}\to p\overline{p}} \right)=2.
84_{-1.
68-0.
18}^{+2.
03+0.
85}\times {10^{-8 }},} \hfill \\ \end{array} $
where the first uncertainty is statistical and the second is systematic.
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