dc.contributor.author | Aaij, R. | |
dc.contributor.author | Abellán Beteta, C. | |
dc.contributor.author | Adeva, B. | |
dc.contributor.author | Adinolfi, M. | |
dc.contributor.author | Aidala, C. A | |
dc.contributor.author | Ajaltouni, Z. | |
dc.contributor.author | Akar, S. | |
dc.contributor.author | Albicocco, P. | |
dc.contributor.author | Albrecht, J. | |
dc.contributor.author | Alessio, F. | |
dc.contributor.author | Alexander, M. | |
dc.contributor.author | Alfonso Albero, A. | |
dc.contributor.author | Alkhazov, G. | |
dc.contributor.author | Alvarez Cartelle, P. | |
dc.contributor.author | Alves, A. A | |
dc.date.accessioned | 2021-09-20T17:29:38Z | |
dc.date.available | 2021-09-20T17:29:38Z | |
dc.date.issued | 2019-06-21 | |
dc.identifier.uri | https://hdl.handle.net/1721.1/131686 | |
dc.description.abstract | Abstract
The first untagged decay-time-integrated amplitude analysis of B
s
0
→ K
S
0
K±π∓ decays is performed using a sample corresponding to 3.0 fb−1 of pp collision data recorded with the LHCb detector during 2011 and 2012. The data are described with an amplitude model that contains contributions from the intermediate resonances K*(892)0,+, K
2
*
(1430)0,+ and K
0
*
(1430)0,+, and their charge conjugates. Measurements of the branching fractions of the decay modes B
s
0
→ K*(892)±K∓ and
B
s
0
→
K
*
—
892
0
K
0
—
$$ {B}_s^0\to \overset{\left(\hbox{---} \right)}{K^{*}}{(892)}^0\overset{\left(\hbox{---} \right)}{K^0} $$
are in agreement with, and more precise than, previous results. The decays B
s
0
→ K
0
*
(1430)±K∓ and
B
s
0
→
K
0
*
—
1430
0
K
0
—
$$ {B}_s^0\to \overset{\left(\hbox{---} \right)}{K_0^{*}}{(1430)}^0\overset{\left(\hbox{---} \right)}{K^0} $$
are observed for the first time, each with significance over 10 standard deviations. | en_US |
dc.publisher | Springer Berlin Heidelberg | en_US |
dc.relation.isversionof | https://doi.org/10.1007/JHEP06(2019)114 | en_US |
dc.rights | Creative Commons Attribution | en_US |
dc.rights.uri | https://creativecommons.org/licenses/by/4.0/ | en_US |
dc.source | Springer Berlin Heidelberg | en_US |
dc.title | Amplitude analysis of B s 0 → K S 0 K±π∓ decays | en_US |
dc.type | Article | en_US |
dc.identifier.citation | Journal of High Energy Physics. 2019 Jun 21;2019(6):114 | en_US |
dc.contributor.department | Massachusetts Institute of Technology. Department of Physics | |
dc.identifier.mitlicense | PUBLISHER_CC | |
dc.eprint.version | Final published version | en_US |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | en_US |
eprint.status | http://purl.org/eprint/status/PeerReviewed | en_US |
dc.date.updated | 2020-06-26T13:02:34Z | |
dc.language.rfc3066 | en | |
dc.rights.holder | The Author(s) | |
dspace.embargo.terms | N | |
dspace.date.submission | 2020-06-26T13:02:34Z | |
mit.license | PUBLISHER_CC | |
mit.metadata.status | Authority Work and Publication Information Needed | |