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Study of the charmed baryonic decays $\bar{B}^0\to\Sigma_c^{++}\bar{p}\pi^-$ and $\bar{B}^0\to\Sigma_c^{0}\bar{p}\pi^+$
High Energy Physics - Experiment · Submitted 9 Aug 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We measure the branching fractions ${\cal B} (\bar{B}^0\to\Sigma_c(2455)^{++}\bar{p}\pi^-)$=$(2.1\pm0.2\pm0.3\pm0.5)\times 10^{-4}$, ${\cal B}(\bar{B}^0\to\Sigma_c(2455)^{0}\bar{p}\pi^+)$=$(1.4\pm0.2\pm0.2\pm0.4)\times1 0^{-4}$, ${\cal B}(\bar{B}^0\to\Sigma_c(2520)^{++} \bar{p}\pi^-)$=$(1.2\pm\0.1\pm0.2\pm0.3)\times10^{-4}$ with statistical significances of 13.1, 9.5 and 7.2 standard deviations, respectively.
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The abstract, sentence by sentence
We study the three-body charmed baryonic decays $\bar{B}^0\to\Sigma_c^{++} \bar{p}\pi^-$ and $\bar{B}^0\to\Sigma_c^{0}\bar{p}\pi^+$ in the four-body final state $\bar{B}^0\to\Lambda_c^{+}\bar{p}\pi^+\pi^-$, using a data sample of 357 fb$^{-1}$ accumulated at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider. We measure the branching fractions ${\cal B} (\bar{B}^0\to\Sigma_c(2455)^{++}\bar{p}\pi^-)$=$(2.1\pm0.2\pm0.3\pm0.5)\times 10^{-4}$, ${\cal B}(\bar{B}^0\to\Sigma_c(2455)^{0}\bar{p}\pi^+)$=$(1.4\pm0.2\pm0.2\pm0.4)\times1 0^{-4}$, ${\cal B}(\bar{B}^0\to\Sigma_c(2520)^{++} \bar{p}\pi^-)$=$(1.2\pm\0.1\pm0.2\pm0.3)\times10^{-4}$ with statistical significances of 13.1, 9.5 and 7.2 standard deviations, respectively. The errors are statistical, systematic, and due to the uncertainty in ${\cal B}(\Lambda_c^+\to{p}K^-\pi^+)$, respectively. We also set an upper limit ${\cal B}(\bar{B}^0\to\Sigma_c(2520)^{0}\bar{p}\pi^+)<0.38\times10^{-4}$ at the 90% confidence level. In addition, we obtain a non-resonant branching fraction of $(6.4\pm0.4\pm\0.9\pm1.7)\times10^{-4}$, and a total branching fraction of $(11.2\pm0.5\pm1.4\pm2.9)\times10^{-4}$ for $\bar{B}^0\to\Lambda_c^{+}\bar{p}\pi^+\pi^-$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the three-body charmed baryonic decays $\bar{B}^0\to\Sigma_c^{++} \bar{p}\pi^-$ and $\bar{B}^0\to\Sigma_c^{0}\bar{p}\pi^+$ in the four-body final state $\bar{B}^0\to\Lambda_c^{+}\bar{p}\pi^+\pi^-$, using a data sample of 357 fb$^{-1}$ accumulated at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider. | contribution 0.78 | 0.93 | 0.04 | asserted 0.94 |
| s1 | We measure the branching fractions ${\cal B} (\bar{B}^0\to\Sigma_c(2455)^{++}\bar{p}\pi^-)$=$(2.1\pm0.2\pm0.3\pm0.5)\times 10^{-4}$, ${\cal B}(\bar{B}^0\to\Sigma_c(2455)^{0}\bar{p}\pi^+)$=$(1.4\pm0.2\pm0.2\pm0.4)\times1 0^{-4}$, ${\cal B}(\bar{B}^0\to\Sigma_c(2520)^{++} \bar{p}\pi^-)$=$(1.2\pm\0.1\pm0.2\pm0.3)\times10^{-4}$ with statistical significances of 13.1, 9.5 and 7.2 standard deviations, respectively. | result 1.00 | 0.98 | 0.64 | asserted 1.00 |
| s2 | The errors are statistical, systematic, and due to the uncertainty in ${\cal B}(\Lambda_c^+\to{p}K^-\pi^+)$, respectively. | result 0.35 | 0.45 | 0.03 | asserted 0.99 |
| s3 | We also set an upper limit ${\cal B}(\bar{B}^0\to\Sigma_c(2520)^{0}\bar{p}\pi^+)<0.38\times10^{-4}$ at the 90% confidence level. | result 1.00 | 0.97 | 0.11 | asserted 0.97 |
| s4 | In addition, we obtain a non-resonant branching fraction of $(6.4\pm0.4\pm\0.9\pm1.7)\times10^{-4}$, and a total branching fraction of $(11.2\pm0.5\pm1.4\pm2.9)\times10^{-4}$ for $\bar{B}^0\to\Lambda_c^{+}\bar{p}\pi^+\pi^-$. | result 1.00 | 0.97 | 0.20 | asserted 1.00 |
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The paper
Original abstract
We study the three-body charmed baryonic decays $\bar{B}^0\to\Sigma_c^{++} \bar{p}\pi^-$ and $\bar{B}^0\to\Sigma_c^{0}\bar{p}\pi^+$ in the four-body final state $\bar{B}^0\to\Lambda_c^{+}\bar{p}\pi^+\pi^-$, using a data sample of 357 fb$^{-1}$ accumulated at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider. We measure the branching fractions ${\cal B} (\bar{B}^0\to\Sigma_c(2455)^{++}\bar{p}\pi^-)$=$(2.1\pm0.2\pm0.3\pm0.5)\times 10^{-4}$, ${\cal B}(\bar{B}^0\to\Sigma_c(2455)^{0}\bar{p}\pi^+)$=$(1.4\pm0.2\pm0.2\pm0.4)\times1 0^{-4}$, ${\cal B}(\bar{B}^0\to\Sigma_c(2520)^{++} \bar{p}\pi^-)$=$(1.2\pm\0.1\pm0.2\pm0.3)\times10^{-4}$ with statistical significances of 13.1, 9.5 and 7.2 standard deviations, respectively. The errors are statistical, systematic, and due to the uncertainty in ${\cal B}(\Lambda_c^+\to{p}K^-\pi^+)$, respectively. We also set an upper limit ${\cal B}(\bar{B}^0\to\Sigma_c(2520)^{0}\bar{p}\pi^+)<0.38\times10^{-4}$ at the 90% confidence level. In addition, we obtain a non-resonant branching fraction of $(6.4\pm0.4\pm\0.9\pm1.7)\times10^{-4}$, and a total branching fraction of $(11.2\pm0.5\pm1.4\pm2.9)\times10^{-4}$ for $\bar{B}^0\to\Lambda_c^{+}\bar{p}\pi^+\pi^-$.
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