“…The well-known Ξ 0 c baryon consists of the c, s, and d quarks, and has a lifetime of 154.5 AE 1.7 AE 1.6 AE 1.0 fs [3]. The branching fraction BðΞ 0 c → π − Λ þ c Þ has not been previously measured.…”
mentioning
confidence: 99%
“…Based on the measured BðΞ − b → π − Λ 0 b ) [4], and using charmed-baryon lifetimes available at that time, they predict BðΞ 0 c → π − Λ þ c Þ ¼ ð0.19 AE 0.07Þ% for constructive interference and BðΞ 0 c → π − Λ þ c Þ ⪅ 0.01% for destructive interference between the SUUD and WS contributions. We have redone their calculation using updated lifetime measurements [3,7], finding BðΞ 0 c → π − Λ þ c Þ ¼ ð0.14 AE 0.07Þ% for constructive interference and BðΞ 0 c → π − Λ þ c Þ ⪅ ð0.018 AE 0.015Þ% for destructive interference. Faller and Mannel, on the other hand, predict BðΞ 0 c → π − Λ þ c Þ < 0.3%, an upper limit obtained by assuming constructive interference [8].…”
mentioning
confidence: 99%
“…A. Zhelezov, 16 Y. Zheng, 5 X. Zhou, 5 Y. Zhou, 5 X. Zhu, 3 V. Zhukov, 13,39 J. B. Zonneveld,57 S. Zucchelli, 19,e D. Zuliani, 27 and G. Zunica 61 (LHCb Collaboration) 1 Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil…”
The Ξ 0 c baryon is unstable and usually decays into charmless final states by the c → sud transition. It can, however, also disintegrate into a π − meson and a Λ þ c baryon via s quark decay or via cs → dc weak scattering. The interplay between the latter two processes governs the size of the branching fraction BðΞ 0 c → π − Λ þ c Þ, first measured here to be ð0.55 AE 0.02 AE 0.18Þ%, where the first uncertainty is statistical and second systematic. This result is compatible with the larger of the theoretical predictions that connect models of hyperon decays using partially conserved axial currents and SU(3) symmetry with those involving the heavy-quark expansion and heavy-quark symmetry. In addition, the branching fraction of the normalization channel, BðΞ þ c → pK − π þ Þ ¼ ð1.135 AE 0.002 AE 0.387Þ% is measured.
“…The well-known Ξ 0 c baryon consists of the c, s, and d quarks, and has a lifetime of 154.5 AE 1.7 AE 1.6 AE 1.0 fs [3]. The branching fraction BðΞ 0 c → π − Λ þ c Þ has not been previously measured.…”
mentioning
confidence: 99%
“…Based on the measured BðΞ − b → π − Λ 0 b ) [4], and using charmed-baryon lifetimes available at that time, they predict BðΞ 0 c → π − Λ þ c Þ ¼ ð0.19 AE 0.07Þ% for constructive interference and BðΞ 0 c → π − Λ þ c Þ ⪅ 0.01% for destructive interference between the SUUD and WS contributions. We have redone their calculation using updated lifetime measurements [3,7], finding BðΞ 0 c → π − Λ þ c Þ ¼ ð0.14 AE 0.07Þ% for constructive interference and BðΞ 0 c → π − Λ þ c Þ ⪅ ð0.018 AE 0.015Þ% for destructive interference. Faller and Mannel, on the other hand, predict BðΞ 0 c → π − Λ þ c Þ < 0.3%, an upper limit obtained by assuming constructive interference [8].…”
mentioning
confidence: 99%
“…A. Zhelezov, 16 Y. Zheng, 5 X. Zhou, 5 Y. Zhou, 5 X. Zhu, 3 V. Zhukov, 13,39 J. B. Zonneveld,57 S. Zucchelli, 19,e D. Zuliani, 27 and G. Zunica 61 (LHCb Collaboration) 1 Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil…”
The Ξ 0 c baryon is unstable and usually decays into charmless final states by the c → sud transition. It can, however, also disintegrate into a π − meson and a Λ þ c baryon via s quark decay or via cs → dc weak scattering. The interplay between the latter two processes governs the size of the branching fraction BðΞ 0 c → π − Λ þ c Þ, first measured here to be ð0.55 AE 0.02 AE 0.18Þ%, where the first uncertainty is statistical and second systematic. This result is compatible with the larger of the theoretical predictions that connect models of hyperon decays using partially conserved axial currents and SU(3) symmetry with those involving the heavy-quark expansion and heavy-quark symmetry. In addition, the branching fraction of the normalization channel, BðΞ þ c → pK − π þ Þ ¼ ð1.135 AE 0.002 AE 0.387Þ% is measured.
“…LHCb has recently measured the lifetimes of charmed baryons using inclusive semileptonic H b → H c µ − X decays collected during Run 1 [2],where H b represents a Λ 0 b , Ξ 0 b or Ξ − b baryon and H c corresponds to a Λ + c , Ξ + c or Ξ 0 c baryon, respectively. The charmed baryons are reconstructed as Λ + c →pK − π + , Ξ + c →pK − π + and Ξ 0 c →pK − K + π + .…”
Section: Measurement Of Charmed-baryons Lifetimesmentioning
“…The lifetime hierarchy is predicted to be either ( + ) > ( + ) > ( 0 ) > ( 0 ) or ( + ) > ( 0 ) > ( + ) > ( 0 ), depending on the treatment of those higher-order effects. Recently, the LHCb collaboration performed a measurement of charmed baryon lifetimes using semileptonic -hadron decays [3,4], where the lifetime of the 0 was measured to be 268 ± 24 (stat) ± 10 (syst) ± 2( + ) fs, almost four times larger than the world average [5] and inconsistent with it at the level of 7 standard Gaussian deviations ( ), and the lifetime of the 0 baryon was measured to be 54.5 ± 1.7 (stat) ± 1.6 (syst) ± 1.0( + ) fs and in tension with the world average [5] at the level of 3.3 . Additional measurements to confirm or rule out these results and to establish the lifetime hierarchy of the charmed baryons from the experimental side are therefore essential.…”
The LHCb experiment collected the world's largest sample of charmed hadrons during LHC Run 1 and Run 2. With this data set, LHCb is currently providing the world's most precise measurements of properties and production of known charmed baryons, as well as searching for many previously unobserved states. The latest results on the charmed baryons described in this document include the lifetime measurement of the 0 and 0 baryons that are produced directly from proton-proton collisions and reconstructed in the − − + final state. The 0 lifetime is measured to be 276.5 ± 13.4 (stat) ± 4.4 (syst) ± 0.7( 0 ) fs and the 0 lifetime to be 148.0 ± 2.3 (stat) ± 2.2 (syst) ± 0.2( 0 ) fs. Both results are consistent with the previous LHCb measurement based on semileptonic decays of -hadrons. The latest results on the charm baryons from the LHCb collaboration also include searches for the + baryon in the + → + − + decay, the first search for the + baryon in the + → + − + decay, and the searches for the 0 and 0 baryons in the + − and + − final states. No significant signals are found for neither of these decays, therefore upper limits are set on the ratio of production cross-sections times the ratio of branching fractions with respect to their normalisation decay.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.