TY  - JOUR
AU  - LHCb Collaboration (Aaij, R. et al
AU  - Henry, L.
AU  - Jashal, B. K.
AU  - Martinez-Vidal, F.
AU  - Oyanguren, A.
AU  - Remon Alepuz, C.
AU  - Ruiz Vidal, J.
PY  - 2021
DA  - 2021//
TI  - Observation of the decay Lambda b0 -> chi(c1)p pi(-)
T2  - J. High Energy Phys.
JO  - Journal of High Energy Physics
SP  - 095
EP  - 21pp
VL  - 05
IS  - 5
PB  - Springer
KW  - B physics
KW  - Branching fraction
KW  - Hadron-Hadron scattering (experiments)
KW  - QCD
KW  - Quarkonium
AB  - The Cabibbo-suppressed decay Lambda b0</mml:msubsup>-> chi (c1)p(-) is observed for the first time using data from proton-proton collisions corresponding to an integrated luminosity of 6 fb(-1), collected with the LHCb detector at a centre-of-mass energy of 13 TeV. Evidence for the Lambda b0</mml:msubsup>-> chi (c2)p(-) decay is also found. Using the Lambda b0</mml:msubsup>-> chi (c1)pK(-) decay as normalisation channel, the ratios of branching fractions are measured to be<disp-formula id="Equa"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mfrac>B<mml:mfenced close=")" open="(">Lambda b0</mml:msubsup>-> chi c1p pi-</mml:mfenced>B<mml:mfenced close=")" open="(">Lambda b0</mml:msubsup>-> <mml:msub>chi c1pK-</mml:mfenced></mml:mfrac>=<mml:mfenced close=")" open="(">6.59 +/- 1.01 +/- 0.22</mml:mfenced>x10-2,</mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mfrac>B<mml:mfenced close=")" open="(">Lambda b0 -> <mml:msub>chi c2p pi-</mml:mfenced>B<mml:mfenced close=")" open="(">Lambda b0 -> <mml:msub>chi c1p pi-</mml:mfenced></mml:mfrac>=0.95 +/- 0.30 +/- 0.04 +/- 0.04,</mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mfrac>B<mml:mfenced close=")" open="(">Lambda b0 -> <mml:msub>chi c2pK-</mml:mfenced>B<mml:mfenced close=")" open="(">Lambda b0 -> <mml:msub>chi c1pK-</mml:mfenced></mml:mfrac>=1.06 +/- 0.05 +/- 0.04 +/- 0.04,</mml:mtd></mml:mtr></mml:mtable><graphic position="anchor" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="13130_2021_15658_Article_Equa.gif"></graphic></disp-formula><p id="Par2">where the first uncertainty is statistical, the second is systematic and the third is due to the uncertainties in the branching fractions of chi (c1,2)-> J/psi gamma decays.<fig id="Figa" position="anchor"><graphic position="anchor" specific-use="HTML" mime-subtype="JPEG" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="MediaObjects/13130_2021_15658_Figa_HTML.jpg" id="MO1"></graphic
SN  - 1029-8479
UR  - https://arxiv.org/abs/2103.04949
UR  - https://doi.org/10.1007/JHEP05(2021)095
DO  - 10.1007/JHEP05(2021)095
LA  - English
N1  - WOS:000651537500001
ID  - LHCbCollaborationAaij_etal2021
ER  -