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From samples of $pp$ collision data collected by the LHCb experiment at $sqrt{s}=7$, $8$ and $13$ TeV corresponding to integrated luminosities of 1.0, 2.0 and 1.5 fb$^{-1}$, respectively, a peak in both the $Lambda_b^0K^-$ and $Xi_b^0pi^-$ invariant mass spectra is observed. In the quark model, radially and orbitally excited $Xi_b^-$ resonances with quark content $bds$ are expected. Referring to this peak as $Xi_b(6227)^-$, the mass and natural width are measured to be $m_{Xi_{b}(6227)^-}=6226.9pm2.0pm0.3pm0.2$ MeV/$c^2$ and $Gamma_{Xi_b(6227)^-}=18.1pm5.4pm1.8$ MeV/$c^2$, where the first uncertainty is statistical, the second is systematic, and the third, on $m_{Xi_b(6227)^-}$, is due to the knowledge of the $Lambda_b^0$ baryon mass. Relative production rates of the ${Xi_b(6227)^-toLambda_b^0K^-}$ and ${Xi_b(6227)^-toXi_b^0pi^-}$ decays are also reported.
Using a proton-proton collision data sample collected by the LHCb experiment, corresponding to an integrated luminosity of 8.5 fb$^{-1}$, the observation of a new excited $Xi_b^0$ resonance decaying to the $Xi_b^-pi^+$ final state is presented. The s
Two structures are observed close to the kinematic threshold in the $Xi_b^0 pi^-$ mass spectrum in a sample of proton-proton collision data, corresponding to an integrated luminosity of 3.0 fb$^{-1}$ recorded by the LHCb experiment. In the quark mode
Decays of the $Xi_b^-$ and $Omega_b^-$ baryons to the charmless final states $p h^{-}h^{prime -}$, where $h^{(prime)}$ denotes a kaon or pion, are searched for with the LHCb detector. The analysis is based on a sample of proton-proton collision data
We report on a high-statistics measurement of the basic double pionic fusion reaction $pn to dpi^0pi^0$ over the energy region of the so-called ABC effect, a pronounced low-mass enhancement in the $pipi$-invariant mass spectrum. The measurements were
We report the observation of a new $D_{sJ}$ meson produced in $B^{+} to bar{D}^{0} D_{sJ} to bar{D}^{0} D^{0} K^{+}$. This state has a mass of $M=2708 pm 9 ^{+11}_{-10} rm{MeV}/{it c}^{2}$, a width $Gamma = 108 pm 23 ^{+36}_{-31} ~rm{MeV}/ {it c}^{2}