Abstract
The Cabibbo-suppressed decay $$ {\Lambda}_{\mathrm{b}}^0 $$
Λ
b
0
→ χc1pπ− 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 $$ {\Lambda}_{\mathrm{b}}^0 $$
Λ
b
0
→ χc2pπ− decay is also found. Using the $$ {\Lambda}_{\mathrm{b}}^0 $$
Λ
b
0
→ χc1pK− decay as normalisation channel, the ratios of branching fractions are measured to be$$ {\displaystyle \begin{array}{c}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\uppi}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\mathrm{K}}^{-}\right)}=\left(6.59\pm 1.01\pm 0.22\right)\times {10}^{-2},\\ {}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}2}{\mathrm{p}\uppi}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\uppi}^{-}\right)}=0.95\pm 0.30\pm 0.04\pm 0.04,\\ {}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}2}{\mathrm{p}\mathrm{K}}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\mathrm{K}}^{-}\right)}=1.06\pm 0.05\pm 0.04\pm 0.04,\end{array}} $$
B
Λ
b
0
→
χ
c
1
pπ
−
B
Λ
b
0
→
χ
c
1
pK
−
=
6.59
±
1.01
±
0.22
×
10
−
2
,
B
Λ
b
0
→
χ
c
2
pπ
−
B
Λ
b
0
→
χ
c
1
pπ
−
=
0.95
±
0.30
±
0.04
±
0.04
,
B
Λ
b
0
→
χ
c
2
pK
−
B
Λ
b
0
→
χ
c
1
pK
−
=
1.06
±
0.05
±
0.04
±
0.04
,
where the first uncertainty is statistical, the second is systematic and the third is due to the uncertainties in the branching fractions of χc1,2→ J/ψγ decays.
Measurement of the Double-Differential Inclusive Jet Cross Section in Proton–Proton Collisions at 13 TeV Centre-of-Mass Energy with the Compact Muon Solenoid Detector
