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Measurements of branching fractions of leptonic and hadronic $ D_s^{+} $ meson decays and extraction of the $ D_s^{+} $ meson decay constant

We present measurements of absolute branching fractions of hadronic and lep-tonic $ D_s^{+} $ decays to K − K + π + , $ {{\overline{K}}^0} $ K + , ηπ + , μ + ν μ and τ + ν τ and report a search for the leptonic $ D_s^{+} $ → e + ν e decays. The results are obtained from a data sample of 913 fb −1 co...

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Published in:The journal of high energy physics 2013-09, Vol.2013 (9), Article 139
Main Authors: Zupanc, A., Adachi, I., Aihara, H., Arinstein, K., Asner, D. M., Aushev, T., Bakich, A. M., Bala, A., Bhuyan, B., Bonvicini, G., Bozek, A., Bračko, M., Brodzicka, J., Browder, T. E., Chang, M.-C., Chang, P., Chekelian, V., Chen, A., Chen, P., Cheon, B. G., Chilikin, K., Chistov, R., Cho, K., Chobanova, V., Choi, S.-K., Choi, Y., Cinabro, D., Dalseno, J., Danilov, M., Doležal, Z., Drásal, Z., Dutta, D., Eidelman, S., Farhat, H., Fast, J. E., Ferber, T., Gaur, V., Gabyshev, N., Ganguly, S., Gillard, R., Goh, Y. M., Golob, B., Haba, J., Hara, T., Hayasaka, K., Hayashii, H., Horii, Y., Hoshi, Y., Hou, W.-S., Hsiung, Y. B., Hyun, H. J., Iijima, T., Inami, K., Ishikawa, A., Itoh, R., Iwasaki, Y., Iwashita, T., Jaegle, I., Julius, T., Kato, E., Kawai, H., Kawasaki, T., Kichimi, H., Kiesling, C., Kim, D. Y., Kim, H. O., Kim, J. B., Kim, J. H., Kim, M. J., Kim, Y. J., Kinoshita, K., Klucar, J., Ko, B. R., Kodyš, P., Korpar, S., Križan, P., Krokovny, P., Kronenbitter, B., Kuhr, T., Kumita, T., Kuzmin, A., Kwon, Y.-J., Lange, J. S., Lee, S.-H., Li, J., Libby, J., Liu, Z. Q., Liventsev, D., Lukin, P., Miyata, H., Mizuk, R., Mohanty, G. B., Moll, A., Mussa, R., Nakano, E., Nakao, M., Nedelkovska, E., Nisar, N. K., Nishida, S., Nitoh, O.
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cited_by cdi_FETCH-LOGICAL-c1549-b0ffa7e8e87e82e718db9144fc26cb758ac89991d5148fb1a950a376005370673
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container_title The journal of high energy physics
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creator Zupanc, A.
Adachi, I.
Aihara, H.
Arinstein, K.
Asner, D. M.
Aushev, T.
Bakich, A. M.
Bala, A.
Bhuyan, B.
Bonvicini, G.
Bozek, A.
Bračko, M.
Brodzicka, J.
Browder, T. E.
Chang, M.-C.
Chang, P.
Chekelian, V.
Chen, A.
Chen, P.
Cheon, B. G.
Chilikin, K.
Chistov, R.
Cho, K.
Chobanova, V.
Choi, S.-K.
Choi, Y.
Cinabro, D.
Dalseno, J.
Danilov, M.
Doležal, Z.
Drásal, Z.
Dutta, D.
Eidelman, S.
Farhat, H.
Fast, J. E.
Ferber, T.
Gaur, V.
Gabyshev, N.
Ganguly, S.
Gillard, R.
Goh, Y. M.
Golob, B.
Haba, J.
Hara, T.
Hayasaka, K.
Hayashii, H.
Horii, Y.
Hoshi, Y.
Hou, W.-S.
Hsiung, Y. B.
Hyun, H. J.
Iijima, T.
Inami, K.
Ishikawa, A.
Itoh, R.
Iwasaki, Y.
Iwashita, T.
Jaegle, I.
Julius, T.
Kato, E.
Kawai, H.
Kawasaki, T.
Kichimi, H.
Kiesling, C.
Kim, D. Y.
Kim, H. O.
Kim, J. B.
Kim, J. H.
Kim, M. J.
Kim, Y. J.
Kinoshita, K.
Klucar, J.
Ko, B. R.
Kodyš, P.
Korpar, S.
Križan, P.
Krokovny, P.
Kronenbitter, B.
Kuhr, T.
Kumita, T.
Kuzmin, A.
Kwon, Y.-J.
Lange, J. S.
Lee, S.-H.
Li, J.
Libby, J.
Liu, Z. Q.
Liventsev, D.
Lukin, P.
Miyata, H.
Mizuk, R.
Mohanty, G. B.
Moll, A.
Mussa, R.
Nakano, E.
Nakao, M.
Nedelkovska, E.
Nisar, N. K.
Nishida, S.
Nitoh, O.
description We present measurements of absolute branching fractions of hadronic and lep-tonic $ D_s^{+} $ decays to K − K + π + , $ {{\overline{K}}^0} $ K + , ηπ + , μ + ν μ and τ + ν τ and report a search for the leptonic $ D_s^{+} $ → e + ν e decays. The results are obtained from a data sample of 913 fb −1 collected at or near the $ \varUpsilon $ (4 S ) and $ \varUpsilon $ (5 S ) resonances with the Belle detector at the KEKB asymmetric-energy e + e − collider. The branching fractions of hadronic decays are measured to be $ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {K^{-}}{K^{+}}{\pi^{+}}} \right) = \left( {5.06\pm 0.15\pm 0.21} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ {{\overline{K}}^0}{K^{+}}} \right) = \left( {2.95\pm 0.11\pm 0.09} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ \eta {\pi^{+}}} \right) = \left( {1.82\pm 0.14\pm 0.07} \right)\%,} \\ \end{array} $ where the first and second uncertainties are statistical and systematic, respectively. The branching fractions of leptonic decays are measured to be $ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {\mu^{+}}{\nu_{\mu }}} \right)=\left( {0.531\pm 0.028\pm 0.020} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\to {\tau^{+}}{\nu_{\tau }}} \right)=\left( {5.70\pm 0.21_{-0.30}^{-0.31 }} \right)\%,} \\ \end{array} $ which are combined to determine the $ D_s^{+} $ meson decay constant $ {f_{{{D_s}}}=\left( {255.5\pm 4.2\pm 5.1} \right)\ \mathrm{MeV}. $ We find no significant signal for $ D_s^{+} $ → e + ν e decays and set an upper limit of $ \mathcal{B}\left( {D_s^{+}\ \to\ {e^{+}}{\nu_e}} \right) $ < 1 . 0(0 . 83) × 10 −4 at 95% (90%) confidence level.
doi_str_mv 10.1007/JHEP09(2013)139
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M. ; Aushev, T. ; Bakich, A. M. ; Bala, A. ; Bhuyan, B. ; Bonvicini, G. ; Bozek, A. ; Bračko, M. ; Brodzicka, J. ; Browder, T. E. ; Chang, M.-C. ; Chang, P. ; Chekelian, V. ; Chen, A. ; Chen, P. ; Cheon, B. G. ; Chilikin, K. ; Chistov, R. ; Cho, K. ; Chobanova, V. ; Choi, S.-K. ; Choi, Y. ; Cinabro, D. ; Dalseno, J. ; Danilov, M. ; Doležal, Z. ; Drásal, Z. ; Dutta, D. ; Eidelman, S. ; Farhat, H. ; Fast, J. E. ; Ferber, T. ; Gaur, V. ; Gabyshev, N. ; Ganguly, S. ; Gillard, R. ; Goh, Y. M. ; Golob, B. ; Haba, J. ; Hara, T. ; Hayasaka, K. ; Hayashii, H. ; Horii, Y. ; Hoshi, Y. ; Hou, W.-S. ; Hsiung, Y. B. ; Hyun, H. J. ; Iijima, T. ; Inami, K. ; Ishikawa, A. ; Itoh, R. ; Iwasaki, Y. ; Iwashita, T. ; Jaegle, I. ; Julius, T. ; Kato, E. ; Kawai, H. ; Kawasaki, T. ; Kichimi, H. ; Kiesling, C. ; Kim, D. Y. ; Kim, H. O. ; Kim, J. B. ; Kim, J. H. ; Kim, M. J. ; Kim, Y. J. ; Kinoshita, K. ; Klucar, J. ; Ko, B. R. ; Kodyš, P. ; Korpar, S. ; Križan, P. ; Krokovny, P. ; Kronenbitter, B. ; Kuhr, T. ; Kumita, T. ; Kuzmin, A. ; Kwon, Y.-J. ; Lange, J. S. ; Lee, S.-H. ; Li, J. ; Libby, J. ; Liu, Z. Q. ; Liventsev, D. ; Lukin, P. ; Miyata, H. ; Mizuk, R. ; Mohanty, G. B. ; Moll, A. ; Mussa, R. ; Nakano, E. ; Nakao, M. ; Nedelkovska, E. ; Nisar, N. K. ; Nishida, S. ; Nitoh, O.</creator><creatorcontrib>Zupanc, A. ; Adachi, I. ; Aihara, H. ; Arinstein, K. ; Asner, D. M. ; Aushev, T. ; Bakich, A. M. ; Bala, A. ; Bhuyan, B. ; Bonvicini, G. ; Bozek, A. ; Bračko, M. ; Brodzicka, J. ; Browder, T. E. ; Chang, M.-C. ; Chang, P. ; Chekelian, V. ; Chen, A. ; Chen, P. ; Cheon, B. G. ; Chilikin, K. ; Chistov, R. ; Cho, K. ; Chobanova, V. ; Choi, S.-K. ; Choi, Y. ; Cinabro, D. ; Dalseno, J. ; Danilov, M. ; Doležal, Z. ; Drásal, Z. ; Dutta, D. ; Eidelman, S. ; Farhat, H. ; Fast, J. E. ; Ferber, T. ; Gaur, V. ; Gabyshev, N. ; Ganguly, S. ; Gillard, R. ; Goh, Y. M. ; Golob, B. ; Haba, J. ; Hara, T. ; Hayasaka, K. ; Hayashii, H. ; Horii, Y. ; Hoshi, Y. ; Hou, W.-S. ; Hsiung, Y. B. ; Hyun, H. J. ; Iijima, T. ; Inami, K. ; Ishikawa, A. ; Itoh, R. ; Iwasaki, Y. ; Iwashita, T. ; Jaegle, I. ; Julius, T. ; Kato, E. ; Kawai, H. ; Kawasaki, T. ; Kichimi, H. ; Kiesling, C. ; Kim, D. Y. ; Kim, H. O. ; Kim, J. B. ; Kim, J. H. ; Kim, M. J. ; Kim, Y. J. ; Kinoshita, K. ; Klucar, J. ; Ko, B. R. ; Kodyš, P. ; Korpar, S. ; Križan, P. ; Krokovny, P. ; Kronenbitter, B. ; Kuhr, T. ; Kumita, T. ; Kuzmin, A. ; Kwon, Y.-J. ; Lange, J. S. ; Lee, S.-H. ; Li, J. ; Libby, J. ; Liu, Z. Q. ; Liventsev, D. ; Lukin, P. ; Miyata, H. ; Mizuk, R. ; Mohanty, G. B. ; Moll, A. ; Mussa, R. ; Nakano, E. ; Nakao, M. ; Nedelkovska, E. ; Nisar, N. K. ; Nishida, S. ; Nitoh, O. ; The BELLE collaboration ; Virginia Polytechnic Inst. and State Univ. (Virginia Tech), Blacksburg, VA (United States)</creatorcontrib><description>We present measurements of absolute branching fractions of hadronic and lep-tonic $ D_s^{+} $ decays to K − K + π + , $ {{\overline{K}}^0} $ K + , ηπ + , μ + ν μ and τ + ν τ and report a search for the leptonic $ D_s^{+} $ → e + ν e decays. The results are obtained from a data sample of 913 fb −1 collected at or near the $ \varUpsilon $ (4 S ) and $ \varUpsilon $ (5 S ) resonances with the Belle detector at the KEKB asymmetric-energy e + e − collider. The branching fractions of hadronic decays are measured to be $ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {K^{-}}{K^{+}}{\pi^{+}}} \right) = \left( {5.06\pm 0.15\pm 0.21} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ {{\overline{K}}^0}{K^{+}}} \right) = \left( {2.95\pm 0.11\pm 0.09} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ \eta {\pi^{+}}} \right) = \left( {1.82\pm 0.14\pm 0.07} \right)\%,} \\ \end{array} $ where the first and second uncertainties are statistical and systematic, respectively. The branching fractions of leptonic decays are measured to be $ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {\mu^{+}}{\nu_{\mu }}} \right)=\left( {0.531\pm 0.028\pm 0.020} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\to {\tau^{+}}{\nu_{\tau }}} \right)=\left( {5.70\pm 0.21_{-0.30}^{-0.31 }} \right)\%,} \\ \end{array} $ which are combined to determine the $ D_s^{+} $ meson decay constant $ {f_{{{D_s}}}=\left( {255.5\pm 4.2\pm 5.1} \right)\ \mathrm{MeV}. $ We find no significant signal for $ D_s^{+} $ → e + ν e decays and set an upper limit of $ \mathcal{B}\left( {D_s^{+}\ \to\ {e^{+}}{\nu_e}} \right) $ &lt; 1 . 0(0 . 83) × 10 −4 at 95% (90%) confidence level.</description><identifier>ISSN: 1029-8479</identifier><identifier>EISSN: 1029-8479</identifier><identifier>DOI: 10.1007/JHEP09(2013)139</identifier><language>eng</language><publisher>United States: Springer Berlin</publisher><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><ispartof>The journal of high energy physics, 2013-09, Vol.2013 (9), Article 139</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1549-b0ffa7e8e87e82e718db9144fc26cb758ac89991d5148fb1a950a376005370673</citedby><cites>FETCH-LOGICAL-c1549-b0ffa7e8e87e82e718db9144fc26cb758ac89991d5148fb1a950a376005370673</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27903,27904</link.rule.ids><backlink>$$Uhttps://www.osti.gov/servlets/purl/1594506$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Zupanc, A.</creatorcontrib><creatorcontrib>Adachi, I.</creatorcontrib><creatorcontrib>Aihara, H.</creatorcontrib><creatorcontrib>Arinstein, K.</creatorcontrib><creatorcontrib>Asner, D. 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(Virginia Tech), Blacksburg, VA (United States)</creatorcontrib><title>Measurements of branching fractions of leptonic and hadronic $ D_s^{+} $ meson decays and extraction of the $ D_s^{+} $ meson decay constant</title><title>The journal of high energy physics</title><description>We present measurements of absolute branching fractions of hadronic and lep-tonic $ D_s^{+} $ decays to K − K + π + , $ {{\overline{K}}^0} $ K + , ηπ + , μ + ν μ and τ + ν τ and report a search for the leptonic $ D_s^{+} $ → e + ν e decays. The results are obtained from a data sample of 913 fb −1 collected at or near the $ \varUpsilon $ (4 S ) and $ \varUpsilon $ (5 S ) resonances with the Belle detector at the KEKB asymmetric-energy e + e − collider. The branching fractions of hadronic decays are measured to be $ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {K^{-}}{K^{+}}{\pi^{+}}} \right) = \left( {5.06\pm 0.15\pm 0.21} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ {{\overline{K}}^0}{K^{+}}} \right) = \left( {2.95\pm 0.11\pm 0.09} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ \eta {\pi^{+}}} \right) = \left( {1.82\pm 0.14\pm 0.07} \right)\%,} \\ \end{array} $ where the first and second uncertainties are statistical and systematic, respectively. The branching fractions of leptonic decays are measured to be $ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {\mu^{+}}{\nu_{\mu }}} \right)=\left( {0.531\pm 0.028\pm 0.020} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\to {\tau^{+}}{\nu_{\tau }}} \right)=\left( {5.70\pm 0.21_{-0.30}^{-0.31 }} \right)\%,} \\ \end{array} $ which are combined to determine the $ D_s^{+} $ meson decay constant $ {f_{{{D_s}}}=\left( {255.5\pm 4.2\pm 5.1} \right)\ \mathrm{MeV}. $ We find no significant signal for $ D_s^{+} $ → e + ν e decays and set an upper limit of $ \mathcal{B}\left( {D_s^{+}\ \to\ {e^{+}}{\nu_e}} \right) $ &lt; 1 . 0(0 . 83) × 10 −4 at 95% (90%) confidence level.</description><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><issn>1029-8479</issn><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNp1kE9LAzEQxYMoWKtnr0E8KLJ2Znez2RylVqtU9KBXQzab2JU2W5IIFvEb-KHd_jl48TLzZvjxZniEHCNcIgAf3I9HTyDOUsDsHDOxQ3oIqUjKnIvdP3qfHITwDoAMBfTIz4NR4cObuXEx0NbSyiunp417o9YrHZvWrdczs4itazRVrqZTVfv1cEqvZXj9uvju1NyE1tHaaLUMa8p8xq3DyiBOzX841d2RqFw8JHtWzYI52vY-ebkZPQ_HyeTx9m54NUk0slwkFViruClN2ZXUcCzrSmCeW50WuuKsVLoUQmDNMC9thUowUBkvAFjGoeBZn5xsfNsQGxl0E42edk84o6NEJnIGRQcNNpD2bQjeWLnwzVz5pUSQq8TlJnG5Slx2iWe_4adzkw</recordid><startdate>20130925</startdate><enddate>20130925</enddate><creator>Zupanc, A.</creator><creator>Adachi, I.</creator><creator>Aihara, H.</creator><creator>Arinstein, K.</creator><creator>Asner, D. 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K.</creator><creator>Nishida, S.</creator><creator>Nitoh, O.</creator><general>Springer Berlin</general><scope>AAYXX</scope><scope>CITATION</scope><scope>OIOZB</scope><scope>OTOTI</scope></search><sort><creationdate>20130925</creationdate><title>Measurements of branching fractions of leptonic and hadronic $ D_s^{+} $ meson decays and extraction of the $ D_s^{+} $ meson decay constant</title><author>Zupanc, A. ; Adachi, I. ; Aihara, H. ; Arinstein, K. ; Asner, D. M. ; Aushev, T. ; Bakich, A. M. ; Bala, A. ; Bhuyan, B. ; Bonvicini, G. ; Bozek, A. ; Bračko, M. ; Brodzicka, J. ; Browder, T. E. ; Chang, M.-C. ; Chang, P. ; Chekelian, V. ; Chen, A. ; Chen, P. ; Cheon, B. G. ; Chilikin, K. ; Chistov, R. ; Cho, K. ; Chobanova, V. ; Choi, S.-K. ; Choi, Y. ; Cinabro, D. ; Dalseno, J. ; Danilov, M. ; Doležal, Z. ; Drásal, Z. ; Dutta, D. ; Eidelman, S. ; Farhat, H. ; Fast, J. E. ; Ferber, T. ; Gaur, V. ; Gabyshev, N. ; Ganguly, S. ; Gillard, R. ; Goh, Y. M. ; Golob, B. ; Haba, J. ; Hara, T. ; Hayasaka, K. ; Hayashii, H. ; Horii, Y. ; Hoshi, Y. ; Hou, W.-S. ; Hsiung, Y. B. ; Hyun, H. J. ; Iijima, T. ; Inami, K. ; Ishikawa, A. ; Itoh, R. ; Iwasaki, Y. ; Iwashita, T. ; Jaegle, I. ; Julius, T. ; Kato, E. ; Kawai, H. ; Kawasaki, T. ; Kichimi, H. ; Kiesling, C. ; Kim, D. Y. ; Kim, H. O. ; Kim, J. B. ; Kim, J. H. ; Kim, M. J. ; Kim, Y. J. ; Kinoshita, K. ; Klucar, J. ; Ko, B. R. ; Kodyš, P. ; Korpar, S. ; Križan, P. ; Krokovny, P. ; Kronenbitter, B. ; Kuhr, T. ; Kumita, T. ; Kuzmin, A. ; Kwon, Y.-J. ; Lange, J. S. ; Lee, S.-H. ; Li, J. ; Libby, J. ; Liu, Z. Q. ; Liventsev, D. ; Lukin, P. ; Miyata, H. ; Mizuk, R. ; Mohanty, G. B. ; Moll, A. ; Mussa, R. ; Nakano, E. ; Nakao, M. ; Nedelkovska, E. ; Nisar, N. K. ; Nishida, S. ; Nitoh, O.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1549-b0ffa7e8e87e82e718db9144fc26cb758ac89991d5148fb1a950a376005370673</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zupanc, A.</creatorcontrib><creatorcontrib>Adachi, I.</creatorcontrib><creatorcontrib>Aihara, H.</creatorcontrib><creatorcontrib>Arinstein, K.</creatorcontrib><creatorcontrib>Asner, D. M.</creatorcontrib><creatorcontrib>Aushev, T.</creatorcontrib><creatorcontrib>Bakich, A. 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B.</creatorcontrib><creatorcontrib>Moll, A.</creatorcontrib><creatorcontrib>Mussa, R.</creatorcontrib><creatorcontrib>Nakano, E.</creatorcontrib><creatorcontrib>Nakao, M.</creatorcontrib><creatorcontrib>Nedelkovska, E.</creatorcontrib><creatorcontrib>Nisar, N. K.</creatorcontrib><creatorcontrib>Nishida, S.</creatorcontrib><creatorcontrib>Nitoh, O.</creatorcontrib><creatorcontrib>The BELLE collaboration</creatorcontrib><creatorcontrib>Virginia Polytechnic Inst. and State Univ. (Virginia Tech), Blacksburg, VA (United States)</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>The journal of high energy physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zupanc, A.</au><au>Adachi, I.</au><au>Aihara, H.</au><au>Arinstein, K.</au><au>Asner, D. M.</au><au>Aushev, T.</au><au>Bakich, A. M.</au><au>Bala, A.</au><au>Bhuyan, B.</au><au>Bonvicini, G.</au><au>Bozek, A.</au><au>Bračko, M.</au><au>Brodzicka, J.</au><au>Browder, T. E.</au><au>Chang, M.-C.</au><au>Chang, P.</au><au>Chekelian, V.</au><au>Chen, A.</au><au>Chen, P.</au><au>Cheon, B. G.</au><au>Chilikin, K.</au><au>Chistov, R.</au><au>Cho, K.</au><au>Chobanova, V.</au><au>Choi, S.-K.</au><au>Choi, Y.</au><au>Cinabro, D.</au><au>Dalseno, J.</au><au>Danilov, M.</au><au>Doležal, Z.</au><au>Drásal, Z.</au><au>Dutta, D.</au><au>Eidelman, S.</au><au>Farhat, H.</au><au>Fast, J. E.</au><au>Ferber, T.</au><au>Gaur, V.</au><au>Gabyshev, N.</au><au>Ganguly, S.</au><au>Gillard, R.</au><au>Goh, Y. M.</au><au>Golob, B.</au><au>Haba, J.</au><au>Hara, T.</au><au>Hayasaka, K.</au><au>Hayashii, H.</au><au>Horii, Y.</au><au>Hoshi, Y.</au><au>Hou, W.-S.</au><au>Hsiung, Y. B.</au><au>Hyun, H. J.</au><au>Iijima, T.</au><au>Inami, K.</au><au>Ishikawa, A.</au><au>Itoh, R.</au><au>Iwasaki, Y.</au><au>Iwashita, T.</au><au>Jaegle, I.</au><au>Julius, T.</au><au>Kato, E.</au><au>Kawai, H.</au><au>Kawasaki, T.</au><au>Kichimi, H.</au><au>Kiesling, C.</au><au>Kim, D. Y.</au><au>Kim, H. O.</au><au>Kim, J. B.</au><au>Kim, J. H.</au><au>Kim, M. J.</au><au>Kim, Y. J.</au><au>Kinoshita, K.</au><au>Klucar, J.</au><au>Ko, B. R.</au><au>Kodyš, P.</au><au>Korpar, S.</au><au>Križan, P.</au><au>Krokovny, P.</au><au>Kronenbitter, B.</au><au>Kuhr, T.</au><au>Kumita, T.</au><au>Kuzmin, A.</au><au>Kwon, Y.-J.</au><au>Lange, J. S.</au><au>Lee, S.-H.</au><au>Li, J.</au><au>Libby, J.</au><au>Liu, Z. Q.</au><au>Liventsev, D.</au><au>Lukin, P.</au><au>Miyata, H.</au><au>Mizuk, R.</au><au>Mohanty, G. B.</au><au>Moll, A.</au><au>Mussa, R.</au><au>Nakano, E.</au><au>Nakao, M.</au><au>Nedelkovska, E.</au><au>Nisar, N. K.</au><au>Nishida, S.</au><au>Nitoh, O.</au><aucorp>The BELLE collaboration</aucorp><aucorp>Virginia Polytechnic Inst. and State Univ. (Virginia Tech), Blacksburg, VA (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Measurements of branching fractions of leptonic and hadronic $ D_s^{+} $ meson decays and extraction of the $ D_s^{+} $ meson decay constant</atitle><jtitle>The journal of high energy physics</jtitle><date>2013-09-25</date><risdate>2013</risdate><volume>2013</volume><issue>9</issue><artnum>139</artnum><issn>1029-8479</issn><eissn>1029-8479</eissn><abstract>We present measurements of absolute branching fractions of hadronic and lep-tonic $ D_s^{+} $ decays to K − K + π + , $ {{\overline{K}}^0} $ K + , ηπ + , μ + ν μ and τ + ν τ and report a search for the leptonic $ D_s^{+} $ → e + ν e decays. The results are obtained from a data sample of 913 fb −1 collected at or near the $ \varUpsilon $ (4 S ) and $ \varUpsilon $ (5 S ) resonances with the Belle detector at the KEKB asymmetric-energy e + e − collider. The branching fractions of hadronic decays are measured to be $ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {K^{-}}{K^{+}}{\pi^{+}}} \right) = \left( {5.06\pm 0.15\pm 0.21} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ {{\overline{K}}^0}{K^{+}}} \right) = \left( {2.95\pm 0.11\pm 0.09} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ \eta {\pi^{+}}} \right) = \left( {1.82\pm 0.14\pm 0.07} \right)\%,} \\ \end{array} $ where the first and second uncertainties are statistical and systematic, respectively. The branching fractions of leptonic decays are measured to be $ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {\mu^{+}}{\nu_{\mu }}} \right)=\left( {0.531\pm 0.028\pm 0.020} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\to {\tau^{+}}{\nu_{\tau }}} \right)=\left( {5.70\pm 0.21_{-0.30}^{-0.31 }} \right)\%,} \\ \end{array} $ which are combined to determine the $ D_s^{+} $ meson decay constant $ {f_{{{D_s}}}=\left( {255.5\pm 4.2\pm 5.1} \right)\ \mathrm{MeV}. $ We find no significant signal for $ D_s^{+} $ → e + ν e decays and set an upper limit of $ \mathcal{B}\left( {D_s^{+}\ \to\ {e^{+}}{\nu_e}} \right) $ &lt; 1 . 0(0 . 83) × 10 −4 at 95% (90%) confidence level.</abstract><cop>United States</cop><pub>Springer Berlin</pub><doi>10.1007/JHEP09(2013)139</doi><oa>free_for_read</oa></addata></record>
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title Measurements of branching fractions of leptonic and hadronic $ D_s^{+} $ meson decays and extraction of the $ D_s^{+} $ meson decay constant
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