172 results on '"E. J. White"'
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2. Beryllium Probe Neutron Diagnostic for a Gas-Puff Z-Pinch Neutron Source on a 1MA, 100-NS Linear Transformer Driver
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D. E. J. White, A. P. Shah, M. A. Mangan, and R. D. McBride
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- 2022
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3. Pedagogical dialogues with 2 year olds in 'preschool' settings: What do they look like?
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C. Geddes, B. Redder, C. Hjorth, S. Bennett, E. J. White, and B. De Manser
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Early childhood education ,Nonverbal communication ,Younger age ,Teaching method ,Interpersonal communication ,Video technology ,Psychology ,Developmental psychology - Abstract
This article reports on a project midway through a 2-year investigation of the pedagogical interactions that take place for 2 year olds in mixed-age early childhood education (ECE) settings. Teachers slowed down and scrutinised their practice by videoing, analysing, and theorising their dialogue with and about 2 year olds as a central form of teaching and learning. The primary aim of the project was to make explicit the nature of 2 year olds' dialogue in ECE settings traditionally oriented to 3 to 4 year olds. Fine-tuned coding of dialogue and their interpreted meanings by the teachers highlight the impact of different events in the ECE setting on the nature of dialogue that takes place and identified 12 different genre in which 2 year olds were found to engage (or disengage). The insights generated from this project support teachers to re-vision their pedagogy in ways that are inclusive of the specialised genre of this younger age group, and celebrate the many pedagogical provocations for dialogue in preschool settings.
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- 2018
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4. Search for the decay J/ψ→γ+ invisible
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B. Xin, D. L. Kreinick, L. K. Gibbons, B. K. Heltsley, K. Y. Gao, D. Cronin-Hennessy, F. Yang, J. Y. Ge, James E Wiss, N. Lowrey, S. Blusk, D. Cinabro, A. N. Robichaud, K. M. Ecklund, Jing Wang, D. M. Asner, P. Naik, Jonas Rademacker, D. Z. Besson, J. M. Hunt, G. Wilkinson, D. H. Miller, T. K. Pedlar, Juliet Ritchie Patterson, M. Kornicer, V. E. Kuznetsov, D. Riley, X. Ting, C. S. Park, A. Lincoln, R. E. Mitchell, John Yelton, L. Martin, P. Spradlin, J. Hietala, L. Fields, J. Ledoux, R. A. Briere, D. L. Hartill, E. H. Thorndike, A. Powell, J. Libby, H. Muramatsu, R. Mountain, G. S. Adams, G. Bonvicini, E. J. White, S. Stroiney, Jonathan L. Rosner, J. P. Alexander, Amiran Tomaradze, S. Brisbane, H. Mendez, Mark Smith, D. G. Cassel, Anders Ryd, M. R. Shepherd, J. Xavier, J. Zhu, B. Moziak, G. Tatishvili, Werner Sun, J. Napolitano, J. Reed, J. Insler, Lei Zhang, I. P. J. Shipsey, R. Poling, Xin Shi, T. Skwarnicki, P. U. E. Onyisi, K. W. Edwards, S. Ricciardi, Mats A Selen, A. J. Sadoff, S. W. Gray, Ping Zhou, Sadia Khalil, P. Rubin, Z. Metreveli, C. Thomas, Sean A Dobbs, P. Zweber, S. Stone, K. Randrianarivony, D. Hu, R. Ehrlich, H. Mahlke-Krüger, Hans J. Vogel, Marina Artuso, C. M. Tarbert, S. Mehrabyan, K. K. Seth, and D. Peterson
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Nuclear physics ,Physics ,010308 nuclear & particles physics ,0103 physical sciences ,Radiative transfer ,Particle ,High Energy Physics::Experiment ,010306 general physics ,Neutral particle ,01 natural sciences - Abstract
We search for J/psi radiative decays into a weakly interacting neutral particle, namely an invisible particle, using the J/psi produced through the process psi(3686) -> pi(+)pi(-) J/psi in a dat ...
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- 2020
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5. Measurement of the Michel parameters (η‾, ξκ ) in the radiative leptonic decay of τ
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J. E. Fast, D. Dossett, M. Niiyama, L. Pesántez, V. Trusov, Andrey Sokolov, S. Shinomiya, Byeong Rok Ko, M. Feindt, I. Nakamura, V. Babu, Hui Li, Jingxu Wang, T. Aushev, O. Frost, Z. Suzuki, J. Grygier, J. H. Kang, Y. Miyachi, Hikaru Kawai, M. Belhorn, Benjamin Schwenker, T. Zivko, Y. B. Hsiung, K. Neichi, A. Zupanc, C. C. Zhang, E. Nakano, Antonio Limosani, T. Ferber, D. H. Lee, H. Kakuno, H. Shibuya, M. Watanabe, L. S. Peak, C. Niebuhr, O. Nitoh, K. Nishimura, Chawon Park, A. Loos, J. C. Dingfelder, M. V. Purohit, P. Goldenzweig, Rupert Leitner, V. V. Zhulanov, J. Yamaoka, Xiuwan Li, K. Senyo, S. Eidelman, L. Shang, Ihn Sik Seong, S. Sandilya, K. Ueno, M. Heck, M. J. Kim, T. Kawasaki, P. Pakhlov, W. Ostrowicz, U. Tamponi, Anton Poluektov, T. Schlüter, S. Sugihara, M. Starič, Y. Igarashi, M. Masuda, Dipanwita Dutta, A. Sugiyama, T. Kumita, M. Uchida, X. H. He, D. Cinabro, Philip Lewis, G. B. Mohanty, C. H. Li, Massimo Berger, B. H. Kim, Y. Yook, H. Yamamoto, L. K. Li, V.N. Zhilich, Y. Kato, V. Chobanova, Y. Kuroki, Satoshi Tanaka, D. Liventsev, Y. Arita, I. Jaegle, K. Miyabayashi, M. Lubej, G. Inguglia, I. Badhrees, Y. Koga, E. Nedelkovska, F. Breibeck, H. Park, J. Stypula, C. Kiesling, E. J. White, A. Bozek, P. Chang, G. S. Varner, Y.-T. Lai, K. Suzuki, P. Schonmeier, M. Iwabuchi, R. Mussa, H. B. Jeon, O. Grzymkowska, C. H. Wang, M. Grosse Perdekamp, R. Itoh, Jung-Hyun Kim, S. Wehle, T. Keck, S. Paul, L. Li Gioi, Y. Yamashita, C. Z. Yuan, Yukinori Sato, J. G. Shiu, M. Nayak, T. Bloomfield, A. Ishikawa, A. Drutskoy, S. E. Vahsen, A. Bay, C.-L. Hsu, T. Saito, S. Rummel, T. Matsuda, Yu Nakahama, M. Tanaka, T. Peng, G. Schnell, A. Rostomyan, Tsukasa Aso, P. Wang, H. Miyata, Y. Hoshi, M. Barrett, B. Bhuyan, Y.L. Han, A. Frey, H. Ye, P. Križan, T. Iijima, Jun Sasaki, H. G. Moser, M. Bračko, Y. Iwasaki, B. G. Fulsom, Peter Kodys, W. W. Jacobs, T. E. Browder, Y. J. Kwon, K. Nakamura, Ya-Qiu Jin, P. Hamer, K. Hayasaka, A. Bobrov, H. Hayashii, Hyunyong Kim, O. Schneider, K. Prasanth, M. Imamura, T. Nagamine, K. Trabelsi, P. Katrenko, T. Müller, J. Klucar, K. T. Kim, C. P. Shen, S. Di Carlo, Seok Kim, S. Okuno, B. Shwartz, Jamal Rorie, D. Getzkow, C. B. Van Hulse, I. Adachi, A. Ogawa, K. Negishi, T. Kuhr, D. Z. Besson, E. Ribežl, D. Santel, Phillip Urquijo, N. Sasao, Victoria Zhukova, V. Savinov, M. Danilov, H. Nakayama, D. Y. Kim, R. Gillard, R. Mizuk, Eberhard Widmann, J. F. Strube, Matthew Jones, M. Z. Wang, K. Kinoshita, M. Yamauchi, G. Bonvicini, Y. B. Li, Y. Teramoto, I. Tikhomirov, D. Mohapatra, J. B. Singh, A. Chen, K. Hara, S. K. Choi, Sanmay Ganguly, T. Uchida, Y. Ban, N. Zwahlen, Bruce Yabsley, L. Zhao, M. Heider, M. Rozanska, D. Kotchetkov, Y. Yusa, A. Vinokurova, S. Dubey, Rahul Kumar, J. Libby, R. Louvot, Y. Chao, G. N. Taylor, R. Glattauer, V.E. Shebalin, J. Haba, W. Bartel, S. Nishida, S. Al Said, K. Hoshina, Y. Seino, Y. Onuki, K. Vervink, Z. Drásal, Marko Petrič, M. T. Prim, K. Itagaki, Z. Q. Liu, C. Bookwalter, B. G. Cheon, H. J. Hyun, S. Uozumi, P. Smerkol, Tariq Aziz, X. L. Wang, D. Heffernan, T. Morii, C. Boulahouache, J. Hasenbusch, V. Chekelian, J. Li, V. M. Aulchenko, H. Guo, T.-A. Shibata, T. Horiguchi, Y. Ono, S. Koblitz, Seema Bahinipati, Y. Choi, H. Takeichi, K. J. Nath, S. Uno, C. Schwanda, P. Krokovny, M. T. Hedges, Samo Stanič, L.M. Zhang, E. Kurihara, A.E. Bondar, P.A. Lukin, T. Nakano, K. Dutta, A. Garmash, Daniel Greenwald, M. Takizawa, B. Reisert, Y. Sakai, J. Rauch, B. K. Pal, E. L. Barberio, M. Shapkin, Noritaka Shimizu, T. Hara, L. Santelj, J. Dalseno, Robin Wedd, K. M. Williams, V. Bansal, K. Belous, A. M. Bakich, S. Korpar, Jolanta Brodzicka, John Yelton, T. Ohshima, Z. Doležal, K. Chilikin, Y. J. Kim, N. Dash, S. Iwata, H. Ozaki, H. Nakano, C. Ng, K. H. Kang, K. Cho, K. Inami, M. Sumihama, A. Heller, M. D. Peters, Motoki Iwasaki, Y. Ushiroda, N. Taniguchi, Y. M. Goh, S. H. Lee, K. Prothmann, R. Pestotnik, N. Gabyshev, D. Červenkov, A. Abdesselam, M. Steder, M. E. Sevior, I. S. Lee, D. Matvienko, Y. Miyazaki, R. Sinha, P. K. Behera, Yasushi Nagasaka, B. Kronenbitter, Sumio Yamada, E. Kato, M. Leitgab, Tao Luo, K. Tanida, F. Tenchini, T. Sumiyoshi, A. Bala, D. Epifanov, Soumya D. Mohanty, C. Pulvermacher, Martin Ritter, Dmytro Levit, Z. Natkaniec, S. L. Blyth, T. Sanuki, Shigeki Hirose, K. K. Joo, Hirokazu Miyake, R. Seidl, Y. Guan, E. Solovieva, Norihito Muramatsu, M. Huschle, K. Sakai, Y. Watanabe, S. K. Kim, A.L. Sibidanov, H. Kichimi, M. C. Chang, K. S. Park, V. Bhardwaj, T. K. Pedlar, T. Tsuboyama, H. Palka, L. E. Piilonen, G. Pakhlova, J. Wiechczynski, R. Kulasiri, S. U. Kataoka, S. Yashchenko, A. Moll, S. L. Olsen, D. Joffe, T. Julius, Po-Hsun Chen, R. Chistov, A. Vossen, O. Seon, Frank Simon, D. Semmler, Y. Unno, K. F. Chen, R. Ayad, T. Nozaki, S. Uehara, M. N. Wagner, Peter Kvasnicka, A. B. Kaliyar, Sunmin Ryu, C. W. Park, E. Won, C. Oswald, H. Atmacan, P. Vanhoefer, E. Panzenböck, B. Golob, M. Schram, N. K. Nisar, H. K. Moon, J. S. Lange, M. Ziegler, K. Adamczyk, Y. Soloviev, W. S. Hou, K. Arinstein, Y. Mikami, Alexei Kuzmin, V. Vorobyev, Nagao Kobayashi, Y. F. Liu, C. Kleinwort, Z. P. Zhang, H. Sahoo, Tara Nanut, T. Uglov, Yoji Hasegawa, S. Y. Suzuki, Richard T. Kouzes, K. Sumisawa, D. M. Asner, S. Himori, Kevin Varvell, A. Matyja, Jason Crnkovic, T. Mori, H. Aihara, Y. Usov, Jyoti Prakash Biswal, C. Liu, H. Nakazawa, A. J. Schwartz, H. Farhat, J. B. Kim, T. Higuchi, S. Ogawa, V. Gaur, Y. S. Sohn, Ferdinando Giordano, M. Nakao, E. Waheed, S. McOnie, J. MacNaughton, and P. Kapusta
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Maximum likelihood ,Electron–positron annihilation ,01 natural sciences ,law.invention ,Nuclear physics ,KEKB ,law ,0103 physical sciences ,Radiative transfer ,Michel parameters ,Statistical analysis ,010306 general physics ,Collider ,Lepton - Abstract
We present the first measurement of the Michel parameters η ‾ and ξκ in the radiative leptonic decay of the τ lepton using 703 fb-1 of data collected with the Belle detector at the KEKB e + e − collider. The Michel parameters are measured by an unbinned maximum likelihood fit to the kinematic information of e + e − → τ + τ − → ( π + π 0 ν ‾ ) ( l − ν ν ‾ γ ) ( l = e or μ ) . The preliminary values of the measured Michel parameters are η ‾ = − 2.0 ± 1.5 ± 0.8 and ξ κ = 0.6 ± 0.4 ± 0.2 , where the first error is statistical and the second is systematic.
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- 2017
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6. Bildung: Potential and Promise in Early Childhood Education
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E. E. Ødegaard and E. J. White
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05 social sciences ,050301 education ,0501 psychology and cognitive sciences ,0503 education ,050104 developmental & child psychology - Published
- 2017
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7. The potential of 44 native and non-native tree species for woodland creation on a range of contrasting sites in lowland Britain
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Victoria Stokes, Ian Willoughby, Simon J. Hodge, Jane Poole, and John E. J. White
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Leyland cypress ,biology ,Range (biology) ,Agroforestry ,Ecology ,Climate change ,Afforestation ,Forestry ,Introduced species ,Woodland ,Adaptation ,biology.organism_classification ,Woody plant - Abstract
Summary A series of species trials were set up to investigate the establishment and early growth (up to 14 years old) of 44 native and non-native tree species on a variety of different site types in lowland Britain. On good quality lowland afforestation sites, Platanus x hispanica (London plane) established and grew more successfully than the native trees tested, and may be an example of a species that could theoretically be established in anticipation of future climate change. Experiments on a variety of community woodland sites indicated that a range of exotic species, such as X Cupressocyparis leylandii (Leyland cypress), may have the potential for establishing a woodland cover on poorly restored land where few other trees would grow. However, on less challenging, better restored sites, a wide range of native species also grew successfully. Further long-term and larger scale trials on a wider variety of sites are required to confi rm the potential of the species tested for British conditions. The results from these experiments also showed that relative growth rates of different species can vary through time, highlighting the danger in making premature judgements about species suitability based solely on very early tree growth.
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- 2007
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8. Induction of LFA-1-Dependent Neutrophil Rolling on ICAM-1 by Engagement of E-Selectin
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Betsy C. Chesnutt, E. J. White, David F. Smith, Michael L. Smith, Klaus Ley, and Nikolai A. Raffler
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Neutrophils ,Physiology ,Mice, Transgenic ,β2 integrin ,Mice ,Physiology (medical) ,E-selectin ,Animals ,Leukocyte Rolling ,Molecular Biology ,Cells, Cultured ,Inflammation ,ICAM-1 ,biology ,Chemistry ,Extramural ,Adhesion ,Intercellular Adhesion Molecule-1 ,Lymphocyte Function-Associated Antigen-1 ,Cell biology ,Fluorescent labelling ,Immunology ,biology.protein ,Antibody ,E-Selectin ,Cardiology and Cardiovascular Medicine ,Ex vivo - Abstract
To study rolling of mouse neutrophils on E-selectin and ICAM-1 in an ex vivo flow chamber system.The authors developed a small autoperfused flow chamber (20 x 200-microm cross section) that allows direct visualization of cells with and without fluorescent labeling and does not require recirculation of blood.Neutrophils rolled on E-selectin alone, but were unable to interact with immobilized ICAM-1. When ICAM-1 was co-immobilized with E-selectin, the number of cells that rolled was doubled, but no significant firm adhesion was observed. This phenomenon was specific for E-selectin, and no enhancement of rolling was observed when P-selectin was immobilized with ICAM-1. The increased neutrophil rolling seen on E-selectin and ICAM-1 substrates required beta2 integrins. Treating mice with antibodies to the beta2 integrins LFA-1 and Mac-1 showed that LFA-1 was primarily responsible for mediating rolling on ICAM-1 in this model. Increased rolling on E-selectin and ICAM-1 was significantly reduced following administration of a specific p38 mitogen-activated protein kinase (MAPK) inhibitor.The data show that neutrophil rolling on E-selectin leads to partial activation of LFA-1, enabling LFA-1-dependent rolling on ICAM-1. This mechanism is likely to amplify and accelerate neutrophil recruitment in inflammation.
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- 2006
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9. Erratum:J/ψandψ(2S)Radiative Transitions toηc[Phys. Rev. Lett.102, 011801 (2009)]
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R. E. Mitchell, M. R. Shepherd, D. Besson, T. K. Pedlar, D. Cronin-Hennessy, K. Y. Gao, J. Hietala, Y. Kubota, T. Klein, B. W. Lang, R. Poling, A. W. Scott, P. Zweber, S. Dobbs, Z. Metreveli, K. K. Seth, A. Tomaradze, J. Libby, A. Powell, G. Wilkinson, K. M. Ecklund, W. Love, V. Savinov, A. Lopez, H. Mendez, J. Ramirez, J. Y. Ge, D. H. Miller, I. P. J. Shipsey, B. Xin, G. S. Adams, M. Anderson, J. P. Cummings, I. Danko, D. Hu, B. Moziak, J. Napolitano, Q. He, J. Insler, H. Muramatsu, C. S. Park, E. H. Thorndike, F. Yang, M. Artuso, S. Blusk, S. Khalil, J. Li, R. Mountain, S. Nisar, K. Randrianarivony, N. Sultana, T. Skwarnicki, S. Stone, J. C. Wang, L. M. Zhang, G. Bonvicini, D. Cinabro, M. Dubrovin, A. Lincoln, P. Naik, J. Rademacker, D. M. Asner, K. W. Edwards, J. Reed, R. A. Briere, T. Ferguson, G. Tatishvili, H. Vogel, M. E. Watkins, J. L. Rosner, J. P. Alexander, D. G. Cassel, J. E. Duboscq, R. Ehrlich, L. Fields, R. S. Galik, L. Gibbons, R. Gray, S. W. Gray, D. L. Hartill, B. K. Heltsley, D. Hertz, J. M. Hunt, J. Kandaswamy, D. L. Kreinick, V. E. Kuznetsov, J. Ledoux, H. Mahlke-Krüger, D. Mohapatra, P. U. E. Onyisi, J. R. Patterson, D. Peterson, D. Riley, A. Ryd, A. J. Sadoff, X. Shi, S. Stroiney, W. M. Sun, T. Wilksen, S. B. Athar, R. Patel, J. Yelton, P. Rubin, B. I. Eisenstein, I. Karliner, S. Mehrabyan, N. Lowrey, M. Selen, E. J. White, and J. Wiss
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Physics ,Particle physics ,Meson ,010308 nuclear & particles physics ,Hadron ,General Physics and Astronomy ,Elementary particle ,Quarkonium ,01 natural sciences ,Nuclear physics ,Particle decay ,0103 physical sciences ,Radiative transfer ,010306 general physics - Published
- 2011
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10. Branching fractions forχcJ→pp¯π0,pp¯η, andpp¯ω
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J. Libby, L. K. Gibbons, G. Wilkinson, Souvik Das, S. Mehrabyan, I. P. J. Shipsey, D. Cronin-Hennessy, N. Lowrey, E. H. Thorndike, Hans J. Vogel, J. Reed, F. Yang, D. Peterson, S. Adams, Sean A Dobbs, D. Cinabro, Juliet Ritchie Patterson, V. E. Kuznetsov, G. Bonvicini, J. P. Alexander, S. Brisbane, S. Blusk, R. Mountain, Xin Shi, B. Xin, C. M. Tarbert, T. Skwarnicki, Ping Zhou, A. Lincoln, Jonas Rademacker, J. Insler, K. W. Edwards, K. Randrianarivony, D. G. Cassel, John Yelton, J. Hietala, S. W. Gray, D. Hu, A. Powell, R. A. Briere, S. Stone, T. K. Pedlar, A. N. Robichaud, G. Tatishvili, Werner Sun, J. Ledoux, L. Martin, P. Rubin, P. Spradlin, Mark Smith, Lei Zhang, D. M. Asner, E. J. White, Mats A Selen, A. J. Sadoff, H. Mendez, P. Naik, J. Y. Ge, Ting Xiao, James E Wiss, D. Riley, Anders Ryd, P. U. E. Onyisi, D. L. Hartill, M. R. Shepherd, P. Zweber, R. E. Mitchell, J. Zhu, G. S. Adams, Z. Metreveli, C. Thomas, J. Napolitano, Jing Wang, Amiran Tomaradze, D. H. Miller, H. Muramatsu, S. Ricciardi, R. Ehrlich, J. M. Hunt, M. Kornicer, Marina Artuso, K. K. Seth, D. Z. Besson, D. L. Kreinick, B. K. Heltsley, Jonathan L. Rosner, J. Xavier, B. Moziak, C. S. Park, L. Fields, and K. M. Ecklund
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Omega - Abstract
Using a sample of $25.9\ifmmode\times\else\texttimes\fi{}{10}^{6}$ $\ensuremath{\psi}(2S)$ decays acquired with the CLEO-c detector at the CESR ${e}^{+}{e}^{\ensuremath{-}}$ collider, we report branching fractions for the decays ${\ensuremath{\chi}}_{cJ}\ensuremath{\rightarrow}p\overline{p}{\ensuremath{\pi}}^{0}$, $p\overline{p}\ensuremath{\eta}$, and $p\overline{p}\ensuremath{\omega}$, with $J=0$, 1, 2. Our results for $\mathcal{B}({\ensuremath{\chi}}_{cJ}\ensuremath{\rightarrow}p\overline{p}{\ensuremath{\pi}}^{0})$ and $\mathcal{B}({\ensuremath{\chi}}_{cJ}\ensuremath{\rightarrow}p\overline{p}\ensuremath{\eta})$ are consistent with, but more precise than, previous measurements. Furthermore, we include the first measurement of $\mathcal{B}({\ensuremath{\chi}}_{cJ}\ensuremath{\rightarrow}p\overline{p}\ensuremath{\omega})$.
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- 2010
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11. Publisher’s Note: Analysis ofD+→K−π+e+νeandD+→K−π+μ++νμsemileptonic decays [Phys. Rev. DPRVDAQ1550-799881, 112001 (2010)]
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S. Blusk, Ping Zhou, Jonas Rademacker, N. Lowrey, D. Cinabro, Juliet Ritchie Patterson, K. M. Ecklund, G. Wilkinson, Souvik Das, X. Ting, B. K. Heltsley, K. Randrianarivony, C. S. Park, R. Mountain, Amiran Tomaradze, S. Mehrabyan, V. E. Kuznetsov, D. M. Asner, R. A. Briere, Sean A Dobbs, B. Xin, Mats A Selen, A. N. Robichaud, D. Hu, L. Fields, T. K. Pedlar, D. Riley, A. J. Sadoff, J. M. Hunt, J. Napolitano, D. Cronin-Hennessy, L. Martin, F. Yang, M. Kornicer, P. Spradlin, H. Mendez, S. Ricciardi, A. Powell, E. H. Thorndike, J. Reed, P. Rubin, G. Bonvicini, John Yelton, J. Hietala, J. P. Alexander, Z. Metreveli, C. Thomas, Marina Artuso, D. L. Hartill, S. Brisbane, D. Z. Besson, Mark Smith, D. G. Cassel, J. Insler, G. Tatishvili, P. Zweber, Werner Sun, Hans J. Vogel, L. K. Gibbons, P. U. E. Onyisi, K. W. Edwards, R. Ehrlich, C. M. Tarbert, Xin Shi, Lei Zhang, J. Zhu, Jonathan L. Rosner, T. Skwarnicki, D. Peterson, J. Xavier, Jing Wang, J. Y. Ge, B. Moziak, James E Wiss, Sadia Khalil, R. E. Mitchell, Anders Ryd, M. R. Shepherd, D. H. Miller, H. Muramatsu, G. S. Adams, S. Stone, K. K. Seth, J. Libby, A. Lincoln, P. Naik, S. W. Gray, J. Ledoux, E. J. White, I. P. J. Shipsey, and D. L. Kreinick
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Semileptonic decay ,Physics ,Nuclear and High Energy Physics ,Particle decay ,Particle physics ,Pion ,Meson ,Quantum electrodynamics ,Antimatter ,Elementary particle ,Lepton ,Boson - Published
- 2010
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12. Analysis ofD+→K−π+e+νeandD+→K−π+μ++νμsemileptonic decays
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Ping Zhou, Jonathan L. Rosner, Tomasz Skwarnicki, Werner Sun, Lei Zhang, J. Xavier, B. Moziak, R. Mountain, K. Randrianarivony, D. Cronin-Hennessy, F. Yang, G. S. Adams, X. Ting, C. S. Park, L. Fields, T. K. Pedlar, Juliet Ritchie Patterson, L. Martin, Karl Matthew Ecklund, P. Spradlin, P. Rubin, M. Kornicer, L. K. Gibbons, S. Mehrabyan, J. M. Hunt, Marina Artuso, G. Tatishvili, B. Xin, D. G. Cassel, D. Z. Besson, Z. Metreveli, C. Thomas, Anders Ryd, Kamal K. Seth, A. Powell, M. R. Shepherd, S. W. Gray, P. Zweber, Sean A Dobbs, V. E. Kuznetsov, N. Lowrey, J. Ledoux, J. Y. Ge, I. P.J. Shipsey, Amiran Tomaradze, D. Cinabro, Hans J. Vogel, J. Reed, James E Wiss, C. M. Tarbert, David M. Asner, A. N. Robichaud, E. J. White, H. Muramatsu, D. Peterson, R. E. Mitchell, Xin Shi, Sheldon Stone, D. Hu, Mark Smith, K. W. Edwards, John Yelton, D. Riley, J. Hietala, S. Blusk, Peter Onyisi, J. Napolitano, Jing Wang, R. A. Briere, P. Naik, B. K. Heltsley, A. Lincoln, G. Wilkinson, Souvik Das, S. Ricciardi, J. Insler, D. L. Kreinick, R. Ehrlich, A. J. Sadoff, Mats A Selen, J. Libby, David Miller, D. L. Hartill, J. Zhu, Jonas Rademacker, H. Mendez, E. H. Thorndike, S. Khalil, G. Bonvicini, J. P. Alexander, and S. Brisbane
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Semileptonic decay ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Antiparticle ,Muon ,Meson ,010308 nuclear & particles physics ,Branching fraction ,Hadron ,01 natural sciences ,Particle decay ,Crystallography ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,010306 general physics ,Dimensionless quantity - Abstract
Using a large sample ({approx_equal}11800 events) of D{sup +{yields}}K{sup -{pi}+}e{sup +{nu}}{sub e} and D{sup +{yields}}K{sup -{pi}+{mu}+{nu}}{sub {mu}}decays collected by the CLEO-c detector running at the {psi}(3770), we measure the helicity basis form factors free from the assumptions of spectroscopic pole dominance and provide new, accurate measurements of the absolute branching fractions for D{sup +{yields}}K*{sup 0}e{sup +{nu}}{sub e} and D{sup +{yields}}K*{sup 0{mu}+{nu}}{sub {mu}}decays. We find branching fractions which are consistent with previous world averages. Our measured helicity basis form factors are consistent with the spectroscopic pole dominance predictions for the three main helicity basis form factors describing D{sup +{yields}}K*{sup 0}l{sup +{nu}}{sub l} decay. The ability to analyze D{sup +{yields}}K{sup -{pi}+{mu}+{nu}}{sub {mu}}allows us to make the first nonparametric measurements of the mass-suppressed form factor. Our result is inconsistent with existing lattice QCD calculations. Finally, we measure the form factor that controls nonresonant s-wave interference with the D{sup +{yields}}K*{sup 0}l{sup +{nu}}{sub l} amplitude and search for evidence of possible additional nonresonant d- or f-wave interference with the K*{sup 0}.
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- 2010
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13. Search for the decayJ/ψ→γ+invisible
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S. Blusk, Xin Shi, R. A. Briere, K. W. Edwards, F. Yang, J. Insler, J. Libby, Werner Sun, S. Stroiney, D. Z. Besson, Lei Zhang, L. K. Gibbons, Mats A Selen, J. Napolitano, Jonas Rademacker, S. Mehrabyan, Anders Ryd, Jonathan L. Rosner, Tomasz Skwarnicki, M. R. Shepherd, P. Naik, D. Riley, E. H. Thorndike, A. N. Robichaud, D. L. Hartill, J. Hietala, R. Mountain, S. Khalil, E. J. White, J. Xavier, Amiran Tomaradze, J. M. Hunt, G. Bonvicini, J. P. Alexander, B. Moziak, V. E. Kuznetsov, S. Brisbane, J. Zhu, Kamal K. Seth, A. Powell, J. Y. Ge, H. Mendez, Sheldon Stone, James E Wiss, D. Hu, A. Lincoln, I. P.J. Shipsey, P. Rubin, R. E. Mitchell, H. Muramatsu, Daniel P Cronin-Hennessy, Sean A Dobbs, D. Peterson, P. Zweber, Jing Wang, John Yelton, D. G. Cassel, S. W. Gray, J. Reed, X. Ting, Ping Zhou, Karl Matthew Ecklund, N. Lowrey, C. S. Park, D. Cinabro, G. Wilkinson, G. Tatishvili, T. K. Pedlar, L. Fields, K. Randrianarivony, L. Martin, P. Spradlin, J. Ledoux, G. S. Adams, B. Xin, K. Y. Gao, Hans J. Vogel, C. M. Tarbert, David M. Asner, David Miller, R. Ehrlich, Marina Artuso, H. Mahlke-Krüger, M. Kornicer, Z. Metreveli, C. Thomas, S. Ricciardi, Juliet Ritchie Patterson, D. L. Kreinick, A. J. Sadoff, Mark Smith, Peter Onyisi, R. Poling, and B. K. Heltsley
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Physics ,Nuclear and High Energy Physics ,Meson ,010308 nuclear & particles physics ,Branching fraction ,Hadron ,Quarkonium ,01 natural sciences ,Nuclear physics ,Particle decay ,Pion ,0103 physical sciences ,High Energy Physics::Experiment ,Atomic physics ,Cornell Electron Storage Ring ,010306 general physics ,Dimensionless quantity - Abstract
A search for J/{psi} radiative decay to weakly interacting neutral final states was performed using the CLEO-c detector at the Cornell Electron Storage Ring. J/{psi} events were selected by observing the hadronic decay {psi}(2S){yields}{pi}{sup +{pi}-}J/{psi}. A total of 3.7x10{sup 6} J/{psi} events were used to study the decay J/{psi}{yields}{gamma}+X, where X is a narrow state that is invisible to the detector. No significant signal was observed, and upper limits on the branching fraction were set for masses m{sub X} up to 960 MeV/c{sup 2}. The upper limit corresponding to m{sub X}=0 is 4.3x10{sup -6} at the 90% confidence level.
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- 2010
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14. Erratum: Measurement ofσ(e+e−→ψ(3770)→hadrons)atEc.m.=3773 MeV[Phys. Rev. Lett.96, 092002 (2006)]
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R. Ehrlich, C. Cawlfield, T. Skwarnicki, K. Zhang, T. Wilksen, H. Mahlke-Krüger, G. Tatishvili, Juliet Ritchie Patterson, V. Pavlunin, S. Blusk, Werner Sun, K. M. Ecklund, G. S. Adams, Jing Wang, B. W. Lang, D. H. Miller, S. Nisar, S. E. Csorna, A. Lincoln, S. Mehrabyan, K. K. Seth, K. E. Arms, E. A. Phillips, Rishi Patel, P. Rubin, James Mueller, T. O. Meyer, R. Sia, Paul Avery, Karl Berkelman, H. Muramatsu, Horst Severini, R. A. Briere, T. K. Pedlar, Mats A Selen, Radia Redjimi, B. K. Heltsley, J. P. Cummings, Z. Li, A. J. Sadoff, D. Cronin-Hennessy, A. W. Scott, P. Zweber, I. Danko, V. E. Kuznetsov, J. Pivarski, D. Z. Besson, F. Liu, D. Y.J. Kim, E. H. Thorndike, J. Kandaswamy, M. Weinberger, V. Potlia, L. K. Gibbons, Marina Artuso, D. L. Hartill, W. Love, D. L. Kreinick, James E Wiss, P. Naik, T. Klein, D. Hertz, J. A. Ernst, Amiran Tomaradze, G. Bonvicini, J. P. Alexander, Sean A Dobbs, H. Stoeck, S. Stone, N. E. Adam, D. Peterson, K. Randrianarivony, J. Napolitano, V. Savinov, N. Menaa, C. Boulahouache, C. Sedlack, D. T. Gong, Li Jingyuan, E. J. White, Anders Ryd, Z. Metreveli, Q. He, M. R. Shepherd, A. M. Smith, L. Breva-Newell, I. Karliner, Y. S. Gao, J. E. Duboscq, K. W. Edwards, K. Y. Gao, S. A. Dytman, Jamila Bashir Butt, G. S. Huang, H. Mendez, M. E. Watkins, John Yelton, J. Hietala, G. P. Chen, Michael T. Anderson, S. B. Athar, D. G. Cassel, Alan D. Lopez, Hans J. Vogel, Junjie Chen, I. P. J. Shipsey, J. E. Ramirez, R. Poling, C. D. Jones, Xin Shi, B. I. Eisenstein, H. Schwarthoff, Thomas Ferguson, R. Mountain, N. Lowrey, D. Cinabro, B. Sanghi, S. W. Gray, P. U. E. Onyisi, C. S. Park, Richard Gray, L. Fields, T. E. Coan, S. Stroiney, Jonathan L. Rosner, D. M. Asner, D. Riley, M. Dubrovin, and Yuichi Kubota
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Physics ,Particle physics ,Meson ,Spectrometer ,Hadron ,Measuring instrument ,General Physics and Astronomy ,Elementary particle ,Quarkonium ,Particle identification - Published
- 2010
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15. Measurement of absolute branching fractions of inclusive semileptonic decays of charm and charmed-strange mesons
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C. S. Park, Ping Zhou, R. A. Briere, J. Reed, B. Xin, D. Z. Besson, K. Y. Gao, L. Fields, D. G. Cassel, M. Kornicer, P. Zweber, Xin Shi, R. Mountain, Z. Metreveli, C. Thomas, John Yelton, K. W. Edwards, D. Riley, D. Peterson, Kamal K. Seth, A. Powell, S. Stroiney, Jonathan L. Rosner, Tomasz Skwarnicki, S. Blusk, L. K. Gibbons, Werner Sun, D. L. Hartill, G. Wilkinson, J. Xavier, S. Mehrabyan, Souvik Das, B. Moziak, I. P.J. Shipsey, Lei Zhang, Sheldon Stone, A. Lincoln, S. Ricciardi, J. Zhu, A. N. Robichaud, J. Y. Ge, Amiran Tomaradze, R. Ehrlich, Jing Wang, B. K. Heltsley, James E Wiss, H. Mendez, D. L. Kreinick, Anders Ryd, A. J. Sadoff, E. J. White, Marina Artuso, Mats A Selen, V. E. Kuznetsov, J. M. Hunt, M. R. Shepherd, R. E. Mitchell, G. S. Adams, Daniel P Cronin-Hennessy, Sean A Dobbs, Helmut Vogel, L. Martin, C. M. Tarbert, David M. Asner, J. Insler, S. Brisbane, F. Yang, Jonas Rademacker, T. K. Pedlar, P. Spradlin, E. H. Thorndike, S. Khalil, G. Bonvicini, J. P. Alexander, H. Muramatsu, N. Lowrey, D. Cinabro, P. Rubin, J. Libby, K. Randrianarivony, Karl Matthew Ecklund, G. Tatishvili, B. J.Y. Tan, J. Napolitano, David Miller, P. Naik, D. Hu, Mark Smith, Peter Onyisi, R. Poling, Juliet Ritchie Patterson, J. Hietala, S. W. Gray, and J. Ledoux
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Physics ,Semileptonic decay ,Nuclear and High Energy Physics ,Particle physics ,Meson ,010308 nuclear & particles physics ,Branching fraction ,Electron–positron annihilation ,Hadron ,FOS: Physical sciences ,01 natural sciences ,High Energy Physics - Experiment ,3. Good health ,Combinatorics ,High Energy Physics - Experiment (hep-ex) ,Particle decay ,Isospin ,0103 physical sciences ,010306 general physics ,Dimensionless quantity - Abstract
We have measured the inclusive semileptonic branching fractions of $D^0$, $D^+$, and $D^+_s$ mesons. For these measurements, we have used the full CLEO-c open-charm data samples, 818 pb$^{-1}$ at $E_\text{CM} = 3.774$ GeV, giving $D^0 \bar{D}^0$ and $D^+ D^-$ events, and 602 pb$^{-1}$ at $E_\text{CM} = 4.170$ GeV, giving $D^{\ast \pm}_s D^\mp_s$ events. We obtain $\mathcal{B}(D^0 \to X e^+ \nu_e) = (6.46 \pm 0.09 \pm 0.11)$%, $\mathcal{B}(D^+ \to X e^+ \nu_e) = (16.13 \pm 0.10 \pm 0.29)$%, and $\mathcal{B}(D^+_s \to X e^+ \nu_e) = (6.52 \pm 0.39 \pm 0.15)$%, where the first uncertainties are statistical and the second are systematic. From these and lifetimes obtained elsewhere, we obtain the ratios of semileptonic decay widths $\Gamma (D^+ \to X e^+ \nu_e) / \Gamma (D^0 \to X e^+ \nu_e) = 0.985 \pm 0.015 \pm 0.024$ and $\Gamma (D^+_s \to X e^+ \nu_e) / \Gamma (D^0 \to X e^+ \nu_e) = 0.828 \pm 0.051 \pm 0.025$. The ratio of $D^+$ and $D^0$ is consistent with the isospin symmetry prediction of unity, and the ratio of $D^+_s$ and $D^0$ differs from unity, as expected., Comment: 16 pages, available through http://www.lns.cornell.edu/public/CLNS/, published in Physical Review D Vol.81, No.5 (2010).
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- 2010
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16. Search forψ(2S)→γηc(2S)via fully reconstructedηc(2S)decays
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Mark Smith, S. Stroiney, Peter Onyisi, H. Muramatsu, Jonathan L. Rosner, Tomasz Skwarnicki, J. M. Hunt, Mats A Selen, R. Poling, J. Xavier, Q. He, L. K. Gibbons, B. Moziak, D. Hertz, D. G. Cassel, C. S. Park, S. Mehrabyan, D. L. Kreinick, Karl Matthew Ecklund, A. J. Sadoff, D. Z. Besson, T. Wilksen, D. L. Hartill, G. Tatishvili, Jing Wang, L. Fields, J. Hietala, V. E. Kuznetsov, N. Lowrey, D. Hu, D. Cinabro, F. Yang, B. J.Y. Tan, J. Napolitano, Anders Ryd, Xin Shi, T. Klein, M. R. Shepherd, K. W. Edwards, J. Zhu, Marina Artuso, Jonas Rademacker, Juliet Ritchie Patterson, Sheldon Stone, G. S. Adams, Kamal K. Seth, A. Powell, Werner Sun, B. K. Heltsley, Lei Zhang, J. Insler, John Yelton, S. W. Gray, Hans J. Vogel, Daniel P Cronin-Hennessy, I. P.J. Shipsey, Sean A Dobbs, J. Reed, D. Riley, J. Libby, R. Mountain, S. Blusk, M. Dubrovin, R. A. Briere, P. Rubin, K. Randrianarivony, C. M. Tarbert, David M. Asner, J. Y. Ge, James E Wiss, A. N. Robichaud, R. E. Mitchell, R. Gray, Amiran Tomaradze, Yuichi Kubota, J. Kandaswamy, J. Ledoux, P. Zweber, H. Mendez, A. Lincoln, D. Peterson, D. T. Gong, Ping Zhou, T. K. Pedlar, L. Martin, E. H. Thorndike, S. Khalil, G. Bonvicini, J. P. Alexander, R. S. Galik, David Miller, P. Naik, B. Xin, K. Y. Gao, G. Wilkinson, E. J. White, M. Kornicer, Z. Metreveli, C. Thomas, R. Ehrlich, and H. Mahlke-Krüger
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Physics ,Nuclear and High Energy Physics ,Particle decay ,Particle physics ,010308 nuclear & particles physics ,Branching fraction ,Product (mathematics) ,Electron–positron annihilation ,0103 physical sciences ,High Energy Physics::Experiment ,010306 general physics ,01 natural sciences ,Dimensionless quantity - Abstract
We report a search for the decay $\ensuremath{\psi}(2S)\ensuremath{\rightarrow}\ensuremath{\gamma}{\ensuremath{\eta}}_{c}(2S)$ in a sample of $25.9\ifmmode\times\else\texttimes\fi{}{10}^{6}$ $\ensuremath{\psi}(2S)$ events collected with the CLEO-c detector. No signals are observed in any of the 11 exclusive ${\ensuremath{\eta}}_{c}(2S)$ decay modes studied, or in their sum. Product branching fraction upper limits are determined as a function of $\ensuremath{\Gamma}[{\ensuremath{\eta}}_{c}(2S)]$ for the 11 individual modes.
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- 2010
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17. Ornamental uses of willow in Britain
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J. E. J. White
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Artificial environment ,Horticulture ,Willow ,biology ,Agroforestry ,Amenity ,Ornamental plant ,General Medicine ,Business ,biology.organism_classification ,Natural (archaeology) - Abstract
SynopsisThe ornamental use of Salix in Britain must be measured against any detrimental impact introduced plants may have on the natural or artificial environment. Willows in amenity planting have the capacity to be both rewarding and at the same time damaging. Anyone using them should be aware of the constraints that may be imposed by the plants and by any potential site. Existing published plant lists are long and inaccurate, often failing to give proper advice on ornamental use. Commercial plant supply may be wanting. Forty species and cultivars are recommended here for a range of situations, but some require further taxonomic research and others need wider introduction to the trade.
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- 1992
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18. Measurement of the pseudoscalar decay constantfDsusingDs+→τ+ν,τ+→ρ+ν¯decays
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G. S. Adams, X. Shi, Ron Poling, E. H. Thorndike, J. Hietala, C. M. Tarbert, David M. Asner, B. K. Heltsley, Z. Metreveli, M. Kornicer, C. Thomas, Ian Shipsey, A. N. Robichaud, Mark Smith, Peter Onyisi, J. Zhu, L. Fields, B. Xin, A. Lincoln, Marina Artuso, A. Powell, J. M. Hunt, G. Tatishvili, Ping Zhou, L. Gibbons, J. Ledoux, Mats A Selen, J. P. Alexander, Daniel P Cronin-Hennessy, Sean A Dobbs, K. M. Ecklund, H. Mendez, S. Khalil, H. Muramatsu, K. Randrianarivony, J. Napolitano, R. Mountain, D. Cinabro, D. L. Kreinick, A. J. Sadoff, S. Ricciardi, Jonathan L. Rosner, L. Martin, D. Riley, R. A. Briere, E. J. White, S. Blusk, S. Mehrabyan, S. W. Gray, S. Brisbane, J. Xavier, J. Y. Ge, P. Naik, David Miller, R. Ehrlich, P. Spradlin, G. Wilkinson, B. J.Y. Tan, W. M. Sun, J. Wiss, P. Rubin, K. Y. Gao, C. S. Park, T. K. Pedlar, L. M. Zhang, G. Bonvicini, T. Skwarnicki, K. W. Edwards, R. E. Mitchell, J. Insler, S. Stroiney, J. Rademacker, Kamal K. Seth, Helmut Vogel, B. Moziak, Sheldon Stone, J. Reed, J. Yelton, V. E. Kuznetsov, D. Peterson, J. C. Wang, D. Besson, D. L. Hartill, A. Tomaradze, N. Lowrey, D. Hu, F. Yang, A. Ryd, M. R. Shepherd, D. G. Cassel, P. Zweber, J. Libby, and J. R. Patterson
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Muon ,010308 nuclear & particles physics ,Branching fraction ,Cabibbo–Kobayashi–Maskawa matrix ,Electron–positron annihilation ,01 natural sciences ,Particle identification ,Crystallography ,Particle decay ,0103 physical sciences ,Exponential decay ,010306 general physics ,Energy (signal processing) - Abstract
Analyzing 600 pb{sup -1} of e{sup +}e{sup -} collisions at 4170 MeV center-of-mass energy with the CLEO-c detector, we measure the branching fraction B(D{sub s}{sup +}{yields}{tau}{sup +}{nu})=(5.52{+-}0.57{+-}0.21)% using the {tau}{sup +}{yields}{rho}{sup +}{nu} decay mode. Combining with other CLEO measurements of B(D{sub s}{sup +}{yields}{tau}{sup +}{nu}) we determine the pseudoscalar decay constant f{sub D{sub s}}=(259.7{+-}7.8{+-}3.4) MeV consistent with the value obtained from our D{sub s}{sup +}{yields}{mu}{sup +}{nu} measurement of (257.6{+-}10.3{+-}4.3) MeV. Combining these measurements we find a value of f{sub D{sub s}}=(259.0{+-}6.2{+-}3.0) MeV, that differs from the most accurate prediction based on unquenched lattice gauge theory of (241{+-}3) MeV by 2.4 standard deviations. We also present the first measurements of B(D{sub s}{sup +}{yields}K{sup 0}{pi}{sup +}{pi}{sup 0})=(1.00{+-}0.18{+-}0.04)%, and B(D{sub s}{sup +}{yields}{pi}{sup +}{pi}{sup 0}{pi}{sup 0})=(0.65{+-}0.13{+-}0.03)%, and measure a new value for B(D{sub s}{sup +}{yields}{eta}{rho}{sup +})=(8.9{+-}0.6{+-}0.5)%.
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- 2009
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19. Inclusive radiativeψ(2S)decays
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J. Libby, L. Martin, A. Powell, C. Thomas, G. Wilkinson, H. Mendez, J. Y. Ge, D. H. Miller, I. P. J. Shipsey, B. Xin, G. S. Adams, D. Hu, B. Moziak, J. Napolitano, K. M. Ecklund, Q. He, J. Insler, H. Muramatsu, C. S. Park, E. H. Thorndike, F. Yang, M. Artuso, S. Blusk, S. Khalil, R. Mountain, K. Randrianarivony, T. Skwarnicki, S. Stone, J. C. Wang, L. M. Zhang, G. Bonvicini, D. Cinabro, A. Lincoln, M. J. Smith, P. Zhou, J. Zhu, P. Naik, J. Rademacker, D. M. Asner, K. W. Edwards, J. Reed, A. N. Robichaud, G. Tatishvili, E. J. White, R. A. Briere, H. Vogel, P. U. E. Onyisi, J. L. Rosner, J. P. Alexander, D. G. Cassel, R. Ehrlich, L. Fields, R. S. Galik, L. Gibbons, R. Gray, S. W. Gray, D. L. Hartill, B. K. Heltsley, D. Hertz, J. M. Hunt, J. Kandaswamy, D. L. Kreinick, V. E. Kuznetsov, J. Ledoux, H. Mahlke-Krüger, J. R. Patterson, D. Peterson, D. Riley, A. Ryd, A. J. Sadoff, X. Shi, S. Stroiney, W. M. Sun, T. Wilksen, J. Yelton, P. Rubin, N. Lowrey, S. Mehrabyan, M. Selen, J. Wiss, M. Kornicer, R. E. Mitchell, M. R. Shepherd, C. M. Tarbert, D. Besson, T. K. Pedlar, J. Xavier, D. Cronin-Hennessy, K. Y. Gao, J. Hietala, T. Klein, R. Poling, P. Zweber, S. Dobbs, Z. Metreveli, K. K. Seth, B. J. Y. Tan, and A. Tomaradze
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Physics ,Nuclear and High Energy Physics ,Photon ,010308 nuclear & particles physics ,Branching fraction ,Astrophysics::High Energy Astrophysical Phenomena ,Electron ,Photon energy ,01 natural sciences ,Particle identification ,Spectral line ,Gluon ,0103 physical sciences ,High Energy Physics::Experiment ,Atomic physics ,Cornell Electron Storage Ring ,010306 general physics - Abstract
Using e{sup +}e{sup -} collision data taken with the CLEO-c detector at the Cornell Electron Storage Ring, we have investigated the direct photon spectrum in the decay {psi}(2S){yields}{gamma}gg. We determine the ratio of the inclusive direct photon decay rate to that of the dominant three-gluon decay rate {psi}(2S){yields}ggg (R{sub {gamma}}{identical_to}{gamma}({gamma}gg)/{gamma}(ggg)) to be R{sub {gamma}}(z{sub {gamma}}>0.4)=0.070{+-}0.002{+-}0.019{+-}0.011, with z{sub {gamma}} defined as the scaled photon energy relative to the beam energy. The errors shown are statistical, systematic, and that due to the uncertainty in the input branching fractions used to extract the ratio, respectively.
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- 2009
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20. Measurement of charm production cross sections ine+e−annihilation at energies between 3.97 and 4.26 GeV
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M. Dubrovin, E. J. White, M. E. Watkins, J. Y. Ge, K. W. Edwards, R. Patel, K. Y. Gao, T. K. Pedlar, D. Hertz, M. R. Shepherd, R. E. Mitchell, S. Khalil, V. E. Kuznetsov, Yuichi Kubota, J. Wiss, P. Rubin, S. Mehrabyan, Ron Poling, J. Insler, W. M. Sun, P. Naik, Kamal K. Seth, C. S. Park, B. Moziak, J. Kandaswamy, N. Sultana, Peter Onyisi, I. Danko, Alan D. Lopez, G. S. Adams, D. G. Cassel, Daniel P Cronin-Hennessy, J. P. Cummings, B. K. Heltsley, S. Nisar, Q. He, L. M. Zhang, Sean A Dobbs, S. W. Gray, T. Skwarnicki, E. H. Thorndike, R. Ehrlich, H. Muramatsu, N. Lowrey, D. Hu, Jonathan L. Rosner, David M. Asner, Ian Shipsey, F. Yang, A. Ryd, A. W. Scott, X. Shi, Mats A Selen, K. M. Ecklund, S. Blusk, Z. Metreveli, D. Mohapatra, J. E. Duboscq, T. Klein, Brian Lang, J. Yelton, Marina Artuso, A. Powell, G. Bonvicini, H. Mendez, David Miller, D. Cinabro, L. Gibbons, A. J. Sadoff, H. Mahlke-Krüger, A. Lincoln, T. Wilksen, L. Fields, D. Riley, R. Gray, C. D. Jones, J. Napolitano, V. Savinov, D. Peterson, G. Wilkinson, J. C. Wang, D. Besson, D. L. Hartill, Li Jingyuan, B. Xin, J. P. Alexander, Sheldon Stone, Helmut Vogel, R. Mountain, D. L. Kreinick, S. B. Athar, J. Libby, M. Anderson, J. Reed, J. E. Ramirez, Thomas Ferguson, K. Randrianarivony, J. Hietala, R. A. Briere, W. Love, G. Tatishvili, A. Tomaradze, S. Stroiney, J. Rademacker, J. R. Patterson, I. Karliner, P. Zweber, and B. I. Eisenstein
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Annihilation ,Meson ,010308 nuclear & particles physics ,Electron–positron annihilation ,Nuclear Theory ,High Energy Physics::Phenomenology ,01 natural sciences ,Particle identification ,Pion ,0103 physical sciences ,High Energy Physics::Experiment ,Production (computer science) ,Cornell Electron Storage Ring ,Atomic physics ,Nuclear Experiment ,010306 general physics ,Energy (signal processing) - Abstract
Using the CLEO-c detector at the Cornell Electron Storage Ring, we have measured inclusive and exclusive cross sections for the production of ${D}^{+}$, ${D}^{0}$ and ${D}_{s}^{+}$ mesons in ${e}^{+}{e}^{\ensuremath{-}}$ annihilations at 13 center-of-mass energies between 3.97 and 4.26 GeV. Exclusive cross sections are presented for final states consisting of two charm mesons ($D\overline{D}$, ${D}^{*}\overline{D}$, ${D}^{*}{\overline{D}}^{*}$, ${D}_{s}^{+}{D}_{s}^{\ensuremath{-}}$, ${D}_{s}^{*+}{D}_{s}^{\ensuremath{-}}$, and ${D}_{s}^{*+}{D}_{s}^{*\ensuremath{-}}$) and for processes in which the charm-meson pair is accompanied by a pion. No enhancement in any final state is observed at the energy of the $Y(4260)$.
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- 2009
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21. Study of the semileptonic decayDs+→f0(980)e+νand implications forBs0→J/ψf0
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Juliet Ritchie Patterson, M. Kornicer, Z. Metreveli, C. Thomas, D. Z. Besson, Kamal K. Seth, A. Powell, R. Ehrlich, Anders Ryd, M. R. Shepherd, F. Yang, I. P.J. Shipsey, H. Mahlke-Krüger, R. A. Briere, Jonas Rademacker, Marina Artuso, B. K. Heltsley, J. Hietala, V. E. Kuznetsov, H. Muramatsu, S. W. Gray, J. Y. Ge, James E Wiss, J. Ledoux, R. E. Mitchell, Sheldon Stone, B. J.Y. Tan, J. Napolitano, Karl Matthew Ecklund, D. Riley, Werner Sun, G. Tatishvili, J. M. Hunt, Lei Zhang, A. J. Sadoff, J. Insler, P. Rubin, D. L. Kreinick, T. K. Pedlar, Xin Shi, K. W. Edwards, D. G. Cassel, G. S. Adams, S. Khalil, G. Bonvicini, J. P. Alexander, L. Martin, D. Peterson, J. Libby, K. Randrianarivony, John Yelton, S. Mehrabyan, Ron Poling, N. Lowrey, D. Cinabro, Mark Smith, Peter Onyisi, Q. He, J. Zhu, S. Blusk, Mats A Selen, C. S. Park, L. Fields, S. Brisbane, S. Stroiney, Jonathan L. Rosner, Tomasz Skwarnicki, J. Xavier, J. Reed, B. Moziak, E. H. Thorndike, D. Hu, Daniel P Cronin-Hennessy, Sean A Dobbs, P. Zweber, J. C. Wang, D. L. Hartill, A. Lincoln, Amiran Tomaradze, R. Mountain, G. Wilkinson, David Miller, P. Naik, Hans J. Vogel, C. M. Tarbert, David M. Asner, A. N. Robichaud, E. J. White, H. Mendez, Ping Zhou, B. Xin, K. Y. Gao, and L. K. Gibbons
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Semileptonic decay ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Crystallography ,010308 nuclear & particles physics ,Electron–positron annihilation ,0103 physical sciences ,Zero (complex analysis) ,CP violation ,010306 general physics ,01 natural sciences - Abstract
Using ${e}^{+}{e}^{\ensuremath{-}}\ensuremath{\rightarrow}{D}_{s}^{\ensuremath{-}}{D}_{s}^{*+}$ and ${D}_{s}^{*\ensuremath{-}}{D}_{s}^{+}$ interactions at 4170 MeV collected with the CLEO-c detector, we investigate the semileptonic decays ${D}_{s}^{+}\ensuremath{\rightarrow}{f}_{0}(980){e}^{+}\ensuremath{\nu}$ and ${D}_{s}^{+}\ensuremath{\rightarrow}\ensuremath{\phi}{e}^{+}\ensuremath{\nu}$. By examining the decay rates as functions of the four-momentum transfer squared ${q}^{2}$, we measure the ratio $[\frac{d\mathcal{B}}{d{q}^{2}}({D}_{s}^{+}\ensuremath{\rightarrow}{f}_{0}(980){e}^{+}\ensuremath{\nu})\mathcal{B}({f}_{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}})]/[\frac{d\mathcal{B}}{d{q}^{2}}({D}_{s}^{+}\ensuremath{\rightarrow}\ensuremath{\phi}{e}^{+}\ensuremath{\nu})\mathcal{B}(\ensuremath{\phi}\ensuremath{\rightarrow}{K}^{+}{K}^{\ensuremath{-}})]$ at ${q}^{2}$ of zero to be $(42\ifmmode\pm\else\textpm\fi{}11)%$. This ratio has been predicted to equal the rate ratio $[\mathcal{B}({B}_{s}\ensuremath{\rightarrow}J/\ensuremath{\psi}{f}_{0})\mathcal{B}({f}_{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}})]/[\mathcal{B}({B}_{s}\ensuremath{\rightarrow}J/\ensuremath{\psi}\ensuremath{\phi})\mathcal{B}(\ensuremath{\phi}\ensuremath{\rightarrow}{K}^{+}{K}^{\ensuremath{-}})]$, thus indicating that the $CP$ eigenstate $J/\ensuremath{\psi}{f}_{0}$ could be useful for measuring $CP$ violation via ${B}_{s}$ mixing. Assuming a simple pole model for the form factor $|{f}_{+}({q}^{2})|$ in the ${f}_{0}{e}^{+}\ensuremath{\nu}$ decay, we find a pole mass of $({1.7}_{\ensuremath{-}0.7}^{+4.5}\ifmmode\pm\else\textpm\fi{}0.2)\text{ }\text{ }\mathrm{GeV}$. We also determine the ${f}_{0}$ mass and width as $({977}_{\ensuremath{-}9}^{+11}\ifmmode\pm\else\textpm\fi{}1)$ and $({91}_{\ensuremath{-}22}^{+30}\ifmmode\pm\else\textpm\fi{}3)\text{ }\text{ }\mathrm{MeV}$, respectively. In addition, we present updated results for $\mathcal{B}({D}_{s}^{+}\ensuremath{\rightarrow}{f}_{0}(980){e}^{+}\ensuremath{\nu})\mathcal{B}({f}_{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}})=(0.20\ifmmode\pm\else\textpm\fi{}0.03\ifmmode\pm\else\textpm\fi{}0.01)%$ and $\mathcal{B}({D}_{s}^{+}\ensuremath{\rightarrow}\ensuremath{\phi}{e}^{+}\ensuremath{\nu})=(2.36\ifmmode\pm\else\textpm\fi{}0.23\ifmmode\pm\else\textpm\fi{}0.13)%$. Assuming that the ${f}_{0}$ wave function is a combination of strange and nonstrange quark-antiquark components, we use our measurement for $\mathcal{B}({D}_{s}^{+}\ensuremath{\rightarrow}{f}_{0}(980){e}^{+}\ensuremath{\nu})$ to extract a value of the mixing angle that we find consistent with $\ensuremath{\mid}\overline{s}s⟩$ dominance, adding to the mystery as to why the ${f}_{0}$ decays predominantly to two pions rather than two kaons.
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- 2009
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22. Ds+exclusive hadronic decays involvingω
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A. Lincoln, E. J. White, B. Xin, H. Mendez, D. Cinabro, J. Y. Ge, Jonathan L. Rosner, J. Xavier, K. Y. Gao, J. P. Alexander, L. Fields, T. K. Pedlar, J. Wiss, P. Rubin, C. S. Park, M. R. Shepherd, B. J.Y. Tan, P. Zweber, J. Yelton, Sheldon Stone, S. Brisbane, G. Bonvicini, C. M. Tarbert, David M. Asner, V. E. Kuznetsov, Ping Zhou, D. G. Cassel, B. Moziak, K. M. Ecklund, J. Libby, J. Hietala, G. Tatishvili, T. Skwarnicki, K. W. Edwards, D. Peterson, J. Napolitano, J. R. Patterson, J. Insler, R. E. Mitchell, S. Mehrabyan, J. C. Wang, D. Besson, A. J. Sadoff, A. N. Robichaud, D. L. Hartill, T. Wilksen, N. Lowrey, D. Hu, F. Yang, S. Stroiney, W. M. Sun, Ian Shipsey, A. Ryd, P. Naik, D. Riley, J. Rademacker, A. Tomaradze, R. Ehrlich, Ron Poling, L. M. Zhang, G. Wilkinson, Marina Artuso, A. Powell, H. Muramatsu, J. M. Hunt, L. Gibbons, S. Khalil, Kamal K. Seth, X. Shi, B. K. Heltsley, H. Mahlke-Krüger, J. Zhu, David Miller, M. Kornicer, R. Mountain, C. Thomas, D. L. Kreinick, J. Ledoux, K. Randrianarivony, L. Martin, R. A. Briere, G. S. Adams, E. H. Thorndike, S. W. Gray, Daniel P Cronin-Hennessy, Sean A Dobbs, S. Blusk, T. Klein, J. Kandaswamy, Helmut Vogel, Z. Metreveli, J. Reed, Mats A Selen, Mark Smith, Peter Onyisi, and Q. He
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Physics ,Nuclear and High Energy Physics ,010308 nuclear & particles physics ,Electron–positron annihilation ,Hadron ,01 natural sciences ,Omega ,Particle identification ,Crystallography ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,Production (computer science) ,010306 general physics ,Energy (signal processing) - Abstract
Using data collected near the D{sub s}*{sup {+-}}D{sub s}{sup {+-}} peak production energy E{sub cm}=4170 MeV by the CLEO-c detector, we search for D{sub s}{sup +} exclusive hadronic decays involving {omega}. We find B(D{sub s}{sup +}{yields}{pi}{sup +}{omega})=(0.21{+-}0.09{+-}0.01)%, B(D{sub s}{sup +}{yields}{pi}{sup +}{pi}{sup 0}{omega})=(2.78{+-}0.65{+-}0.25)%, B(D{sub s}{sup +}{yields}{pi}{sup +}{pi}{sup +}{pi}{sup -}{omega})=(1.58{+-}0.45{+-}0.09)%, B(D{sub s}{sup +}{yields}{pi}{sup +}{eta}{omega})=(0.85{+-}0.54{+-}0.06)%, B(D{sub s}{sup +}{yields}K{sup +}{omega})
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- 2009
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23. Determination of theD0→K−π+π0andD0→K−π+π+π−coherence factors and average strong-phase differences using quantum-correlated measurements
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D. Hu, S. Stroiney, Jonathan L. Rosner, Tomasz Skwarnicki, Ping Zhou, B. Xin, D. Z. Besson, Neville Harnew, Juliet Ritchie Patterson, K. Y. Gao, J. M. Hunt, B. Moziak, Daniel P Cronin-Hennessy, P. Rubin, J. Ledoux, John Yelton, Sean A Dobbs, G. Wilkinson, R. Gray, S. Mehrabyan, Amiran Tomaradze, A. Powell, S. Khalil, A. J. Sadoff, Karl Matthew Ecklund, S. Blusk, T. Wilksen, Hans J. Vogel, G. Bonvicini, J. P. Alexander, I. P.J. Shipsey, G. Tatishvili, Mats A Selen, David M. Asner, J. E. Duboscq, R. A. Briere, A. N. Robichaud, J. Reed, Ron Poling, B. J.Y. Tan, J. Napolitano, Anders Ryd, M. R. Shepherd, V. E. Kuznetsov, H. Mendez, E. J. White, Marina Artuso, E. H. Thorndike, F. Yang, J. Hietala, L. K. Gibbons, Li Jingyuan, D. Hertz, David Miller, T. Klein, J. Zhu, T. J. Gershon, S. W. Gray, T. K. Pedlar, Jing Wang, Jonas Rademacker, P. Naik, Werner Sun, Mark Smith, Lei Zhang, H. Muramatsu, Peter Onyisi, Kamal K. Seth, Q. He, Z. Metreveli, J. Insler, B. K. Heltsley, J. Kandaswamy, D. L. Kreinick, N. Sultana, Sheldon Stone, R. Ehrlich, J. Y. Ge, James E Wiss, D. Peterson, H. Mahlke-Krüger, R. E. Mitchell, G. S. Adams, L. Martin, D. L. Hartill, A. Lincoln, Xin Shi, K. W. Edwards, D. G. Cassel, D. Riley, M. Dubrovin, P. Zweber, R. Mountain, A. W. Scott, Yuichi Kubota, J. Libby, K. Randrianarivony, N. Lowrey, D. Cinabro, C. S. Park, and L. Fields
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Physics ,Nuclear and High Energy Physics ,Meson ,Unitarity ,010308 nuclear & particles physics ,Electron–positron annihilation ,Analytical chemistry ,Resonance (chemistry) ,01 natural sciences ,Nuclear physics ,Particle decay ,Pair production ,0103 physical sciences ,Pi ,010306 general physics ,Bar (unit) - Abstract
The first measurements of the coherence factors (R-K pi pi 0 and R-K3 pi) and the average strong-phase differences((delta(K pi pi 0)(D) and delta(K3 pi)(D))) for D-0 -> K- pi(+) pi(0) and D-0 -> K- pi(+) pi(+) pi(-) are presented. These parameters can be used to improve the determination of the unitarity triangle angle gamma in B- -> DK- decays, where D is a D-0 or (D) over bar (0) meson decaying to the same final state. The measurements are made using quantum-correlated, fully reconstructed D-0(D) over bar (0) pairs produced in e(+)e(-) collisions at the psi(3770) resonance. The measured values are: R-K pi pi 0 = 0.84 +/- 0.07, delta(K pi pi 0)(D) = (227(-17)(+14))degrees, R-K3 pi = 0.33(-0.23)(+0.20), and delta(K3 pi)(D) = (114(-23)(+26))degrees. These results indicate significant coherence in the decay D-0 -> K- pi(+) pi(0), whereas lower coherence is observed in the decay D-0 -> K- pi(+) pi(+) pi(-). The analysis also results in a small improvement in the knowledge of other D-meson parameters, in particular, the strong-phase difference for D-0 -> K- pi(+), delta(K pi)(D), and the mixing parameter y.
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- 2009
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24. Improved measurements ofDmeson semileptonic decays toπandKmesons
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S. Blusk, Werner Sun, Lei Zhang, Anders Ryd, P. Zweber, M. R. Shepherd, Kamal K. Seth, A. Powell, J. E. Duboscq, T. K. Pedlar, J. Libby, R. Mountain, K. Randrianarivony, D. L. Hartill, D. Riley, A. N. Robichaud, B. Xin, K. Y. Gao, M. Dubrovin, E. J. White, J. Reed, D. G. Cassel, J. Zhu, I. P.J. Shipsey, G. Wilkinson, V. E. Kuznetsov, H. Mendez, S. Mehrabyan, N. Lowrey, D. Cinabro, Daniel P Cronin-Hennessy, Sean A Dobbs, E. H. Thorndike, D. Z. Besson, G. S. Adams, Mark Smith, Karl Matthew Ecklund, Yuichi Kubota, Ping Zhou, B. J.Y. Tan, J. Napolitano, S. Khalil, J. M. Hunt, Sheldon Stone, F. Yang, Peter Onyisi, R. Ehrlich, T. Klein, G. Tatishvili, S. Stroiney, A. Lincoln, Jonathan L. Rosner, Tomasz Skwarnicki, John Yelton, L. Martin, P. Rubin, G. Bonvicini, J. P. Alexander, R. Gray, Amiran Tomaradze, H. Muramatsu, R. Poling, J. Xavier, H. Mahlke-Krüger, Jonas Rademacker, J. Kandaswamy, Jing Wang, J. Insler, D. Hu, Q. He, Z. Metreveli, C. Thomas, B. Moziak, Mats A Selen, N. Sultana, L. K. Gibbons, D. Peterson, D. Hertz, D. L. Kreinick, C. S. Park, A. J. Sadoff, L. Fields, T. Wilksen, Hans J. Vogel, A. W. Scott, David Miller, David M. Asner, Xin Shi, K. W. Edwards, Juliet Ritchie Patterson, J. Y. Ge, James E Wiss, Marina Artuso, R. E. Mitchell, B. K. Heltsley, J. Ledoux, R. A. Briere, J. Hietala, S. W. Gray, and P. Naik
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Semileptonic decay ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Meson ,010308 nuclear & particles physics ,Cabibbo–Kobayashi–Maskawa matrix ,Branching fraction ,Electron–positron annihilation ,Hadron ,01 natural sciences ,Crystallography ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,Lattice (order) ,0103 physical sciences ,D meson ,010306 general physics - Abstract
Using the entire CLEO-c {psi}(3770){yields}DD event sample, corresponding to an integrated luminosity of 818 pb{sup -1} and approximately 5.4x10{sup 6} DD events, we present a study of the decays D{sup 0}{yields}{pi}{sup -}e{sup +}{nu}{sub e}, D{sup 0}{yields}K{sup -}e{sup +}{nu}{sub e}, D{sup +}{yields}{pi}{sup 0}e{sup +}{nu}{sub e}, and D{sup +}{yields}K{sup 0}e{sup +}{nu}{sub e}. Via a tagged analysis technique, in which one D is fully reconstructed in a hadronic mode, partial rates for semileptonic decays by the other D are measured in several q{sup 2} bins. We fit these rates using several form factor parametrizations and report the results, including form factor shape parameters and the branching fractions B(D{sup 0}{yields}{pi}{sup -}e{sup +}{nu}{sub e})=(0.288{+-}0.008{+-}0.003)%, B(D{sup 0}{yields}K{sup -}e{sup +}{nu}{sub e})=(3.50{+-}0.03{+-}0.04)%, B(D{sup +}{yields}{pi}{sup 0}e{sup +}{nu}{sub e})=(0.405{+-}0.016{+-}0.009)%, and B(D{sup +}{yields}K{sup 0}e{sup +}{nu}{sub e})=(8.83{+-}0.10{+-}0.20)%, where the first uncertainties are statistical and the second are systematic. Taking input from lattice quantum chromodynamics, we also find |V{sub cd}|=0.234{+-}0.007{+-}0.002{+-}0.025 and |V{sub cs}|=0.985{+-}0.009{+-}0.006{+-}0.103, where the third uncertainties are from lattice quantum chromodynamics.
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- 2009
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25. First model-independent determination of the relative strong phase betweenD0andD¯0→KS0π+π−and its impact on the CKM angleγ/ϕ3measurement
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Jonathan L. Rosner, D. G. Cassel, D. Mohapatra, J. Kandaswamy, Marina Artuso, B. Sanghi, E. J. White, K. W. Edwards, S. Mehrabyan, Ian Shipsey, J. Y. Ge, R. E. Mitchell, Sheldon Stone, N. Sultana, P. Naik, Ping Zhou, S. Khalil, A. J. Sadoff, T. Wilksen, A. Lincoln, K. Y. Gao, A. Powell, B. J.Y. Tan, J. Yelton, D. Riley, B. Xin, T. K. Pedlar, N. Horwitz, Peter Onyisi, J. M. Hunt, L. Gibbons, Kamal K. Seth, Mats A Selen, D. Hertz, G. Wilkinson, J. Wiss, P. Rubin, S. Blusk, M. Dubrovin, T. Klein, V. E. Kuznetsov, Q. He, V. Pavlunin, C. S. Park, J. P. Alexander, J. E. Duboscq, J. Napolitano, Ron Poling, Li Jingyuan, G. Tatishvili, M. R. Shepherd, B. Moziak, A. N. Robichaud, X. Shi, Yuichi Kubota, J. Ledoux, T. Skwarnicki, N. Lowrey, D. Hu, Z. Metreveli, K. M. Ecklund, B. K. Heltsley, F. Yang, S. B. Athar, J. Zhu, D. Peterson, A. Ryd, H. Mendez, D. Cinabro, A. W. Scott, J. C. Wang, D. Besson, K. Randrianarivony, D. L. Hartill, J. Insler, R. Mountain, R. Ehrlich, S. W. Gray, J. Reed, D. L. Kreinick, Daniel P Cronin-Hennessy, Sean A Dobbs, David M. Asner, H. Mahlke-Krüger, S. Stroiney, J. Rademacker, Helmut Vogel, J. Hietala, L. Martin, R. A. Briere, L. Fields, R. Gray, J. Libby, G. S. Adams, E. H. Thorndike, H. Muramatsu, David Miller, W. M. Sun, L. M. Zhang, J. R. Patterson, P. Zweber, A. Tomaradze, and G. Bonvicini
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Meson ,010308 nuclear & particles physics ,Electron–positron annihilation ,Hadron ,Dalitz plot ,Elementary particle ,01 natural sciences ,Crystallography ,Particle decay ,Pair production ,0103 physical sciences ,B meson ,010306 general physics - Abstract
We exploit the quantum coherence between pair-produced ${D}^{0}$ and ${\overline{D}}^{0}$ in $\ensuremath{\psi}(3770)$ decays to make a first determination of the relative strong phase differences between ${D}^{0}\ensuremath{\rightarrow}{K}_{S}^{0}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ and ${\overline{D}}^{0}\ensuremath{\rightarrow}{K}_{S}^{0}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$, which are of great importance in determining the Cabibbo-Kobayashi-Maskawa angle $\ensuremath{\gamma}/{\ensuremath{\phi}}_{3}$ in ${B}^{\ensuremath{-}}\ensuremath{\rightarrow}{D}^{0}({\overline{D}}^{0}){K}^{\ensuremath{-}}$ decays. Using $818\text{ }\text{ }{\mathrm{pb}}^{\ensuremath{-}1}$ of ${e}^{+}{e}^{\ensuremath{-}}$ collision data collected with the CLEO-c detector at ${E}_{\mathrm{cm}}=3.77\text{ }\text{ }\mathrm{GeV}$, we employ a binned Dalitz-plot analysis of ${K}_{S}^{0}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ and ${K}_{L}^{0}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ decays recoiling against flavor-tagged, $CP$-tagged, and ${K}_{S}^{0}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$-tagged events to determine these strong phase differences.
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- 2009
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26. Search forD0→p¯e+andD0→pe−
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T. Wilksen, K. M. Ecklund, A. N. Robichaud, Amiran Tomaradze, D. L. Kreinick, Jonas Rademacker, H. Mendez, J. Reed, Anders Ryd, M. R. Shepherd, I. P. J. Shipsey, S. Blusk, N. Lowrey, J. Insler, R. Mountain, Ping Zhou, D. L. Hartill, D. G. Cassel, D. Cinabro, R. Poling, Li Jingyuan, K. Randrianarivony, D. Hu, D. Z. Besson, B. Xin, P. U. E. Onyisi, H. Muramatsu, K. Y. Gao, J. Kandaswamy, P. Naik, S. Stone, J. Zhu, Xin Shi, Hans J. Vogel, N. Sultana, C. S. Park, Richard Gray, B. K. Heltsley, S. W. Gray, J. E. Duboscq, K. W. Edwards, D. Peterson, V. E. Kuznetsov, L. K. Gibbons, D. Cronin-Hennessy, F. Yang, A. Powell, D. Hertz, J. Y. Ge, Mats A Selen, R. Ehrlich, James E Wiss, A. J. Sadoff, Sadia Khalil, J. Ledoux, L. Fields, A. W. Scott, T. Klein, S. Mehrabyan, J. Libby, R. E. Mitchell, Mark Smith, Sean A Dobbs, E. J. White, G. Tatishvili, Werner Sun, G. Wilkinson, John Yelton, J. Hietala, Lei Zhang, J. M. Hunt, A. Lincoln, Q. He, H. Mahlke-Krüger, S. Stroiney, Jonathan L. Rosner, Juliet Ritchie Patterson, B. Moziak, K. K. Seth, Z. Metreveli, D. M. Asner, R. A. Briere, T. K. Pedlar, L. Martin, D. Riley, E. H. Thorndike, G. Bonvicini, J. P. Alexander, M. Dubrovin, Yuichi Kubota, B. J.Y. Tan, J. Napolitano, Jing Wang, P. Rubin, D. H. Miller, P. Zweber, T. Skwarnicki, G. S. Adams, and Marina Artuso
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,0103 physical sciences ,010306 general physics ,01 natural sciences - Published
- 2009
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27. Dalitz plot analysis ofDs+→K+K−π+
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Jonas Rademacker, Anders Ryd, A. N. Robichaud, D. Riley, M. Dubrovin, J. Insler, Yuichi Kubota, I. P.J. Shipsey, M. R. Shepherd, H. Mendez, G. Wilkinson, G. S. Adams, V. E. Kuznetsov, A. J. Sadoff, T. Wilksen, Mark Smith, Peter Onyisi, Xin Shi, C. S. Park, K. W. Edwards, Daniel P Cronin-Hennessy, Sean A Dobbs, Q. He, B. Xin, D. G. Cassel, Mats A Selen, T. Klein, L. Fields, F. Yang, P. Rubin, Hans J. Vogel, K. Y. Gao, J. Kandaswamy, J. Ledoux, Ron Poling, Karl Matthew Ecklund, David M. Asner, L. K. Gibbons, Z. Metreveli, C. Thomas, N. Sultana, D. Hertz, J. M. Hunt, J. Y. Ge, Werner Sun, G. Tatishvili, Ping Zhou, D. L. Kreinick, D. Peterson, James E Wiss, Lei Zhang, B. K. Heltsley, D. L. Hartill, A. Lincoln, E. J. White, Marina Artuso, P. Zweber, D. Z. Besson, S. Blusk, R. E. Mitchell, S. Stroiney, Jonathan L. Rosner, Tomasz Skwarnicki, J. Zhu, S. Mehrabyan, Jing Wang, J. E. Duboscq, Kamal K. Seth, A. Powell, H. Muramatsu, J. Hietala, Sheldon Stone, R. Ehrlich, Juliet Ritchie Patterson, J. Xavier, John Yelton, H. Mahlke-Krüger, S. W. Gray, B. Moziak, R. A. Briere, B. J.Y. Tan, J. Napolitano, J. Reed, A. W. Scott, E. H. Thorndike, R. Gray, Amiran Tomaradze, D. Hu, J. Libby, K. Randrianarivony, N. Lowrey, D. Cinabro, T. K. Pedlar, L. Martin, S. Khalil, G. Bonvicini, J. P. Alexander, David Miller, P. Naik, and R. Mountain
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Physics ,Nuclear and High Energy Physics ,Meson ,Branching fraction ,010308 nuclear & particles physics ,Electron–positron annihilation ,Partial wave analysis ,Hadron ,Analytical chemistry ,Resonance ,Dalitz plot ,01 natural sciences ,Particle identification ,Nuclear physics ,Crystallography ,Particle decay ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,010306 general physics ,Dimensionless quantity - Abstract
We perform a Dalitz plot analysis of the decay D{sub s}{sup +}{yields}K{sup +}K{sup -}{pi}{sup +} with the CLEO-c data set of 586 pb{sup -1} of e{sup +}e{sup -} collisions accumulated at {radical}(s)=4.17 GeV. This corresponds to about 0.57x10{sup 6} D{sub s}{sup {+-}}D{sub s}*{sup {+-}} pairs from which we select 14 400 candidates with a background of roughly 15%. In contrast to previous measurements we find good agreement with our data only by including an additional f{sub 0}(1370){pi}{sup +} contribution. We measure the magnitude, phase, and fit fraction of K*(892){sup 0}K{sup +}, {phi}(1020){pi}{sup +}, K{sub 0}{sup *}(1430)K{sup +}, f{sub 0}(980){pi}{sup +}, f{sub 0}(1710){pi}{sup +}, and f{sub 0}(1370){pi}{sup +} contributions and limit the possible contributions of other KK and K{pi} resonances that could appear in this decay.
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- 2009
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28. New measurement of exclusive decays of theχc0andχc2to two-meson final states
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Ian Shipsey, A. Powell, Jonathan L. Rosner, J. Insler, J. M. Hunt, L. Gibbons, Z. Metreveli, E. J. White, J. Y. Ge, J. Kandaswamy, B. Xin, J. Wiss, P. Rubin, C. S. Park, D. Mohapatra, T. Klein, A. Tomaradze, W. M. Sun, N. Sultana, Helmut Vogel, G. Tatishvili, J. P. Alexander, A. J. Sadoff, B. J.Y. Tan, T. Wilksen, G. S. Adams, David M. Asner, Marina Artuso, L. M. Zhang, D. Peterson, J. Yelton, S. Stroiney, E. H. Thorndike, D. Riley, B. Moziak, J. C. Wang, D. Besson, J. Napolitano, J. Rademacker, A. N. Robichaud, H. Muramatsu, J. Hietala, D. L. Hartill, S. Khalil, V. E. Kuznetsov, T. Skwarnicki, A. Lincoln, L. Fields, K. Y. Gao, S. B. Athar, K. W. Edwards, R. Gray, N. Lowrey, D. Hu, R. E. Mitchell, R. Ehrlich, F. Yang, T. K. Pedlar, G. Bonvicini, S. W. Gray, K. M. Ecklund, M. Dubrovin, A. Ryd, J. R. Patterson, A. W. Scott, J. Reed, M. R. Shepherd, S. Mehrabyan, H. Mendez, D. Cinabro, P. Naik, R. S. Galik, H. Mahlke-Krüger, David Miller, Yuichi Kubota, Kamal K. Seth, Ron Poling, J. Libby, Peter Onyisi, P. Zweber, Q. He, V. Pavlunin, Sheldon Stone, L. Martin, G. Wilkinson, R. A. Briere, B. K. Heltsley, R. Mountain, J. Ledoux, K. Randrianarivony, Mats A Selen, D. L. Kreinick, Li Jingyuan, X. Shi, D. G. Cassel, B. Sanghi, Daniel P Cronin-Hennessy, Sean A Dobbs, S. Blusk, J. E. Duboscq, and D. Hertz
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Pseudoscalar ,Physics ,Nuclear and High Energy Physics ,Particle decay ,Particle physics ,Meson ,010308 nuclear & particles physics ,Branching fraction ,0103 physical sciences ,010306 general physics ,01 natural sciences ,Particle identification - Abstract
Using a sample of $2.59\ifmmode\times\else\texttimes\fi{}{10}^{7}$ $\ensuremath{\psi}(2S)$ decays collected by the CLEO-c detector, we present results of a study of ${\ensuremath{\chi}}_{c0}$ and ${\ensuremath{\chi}}_{c2}$ decays into two-meson final states. We present the world's most precise measurements of the ${\ensuremath{\chi}}_{cJ,(J=0,2)}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$, ${\ensuremath{\pi}}^{0}{\ensuremath{\pi}}^{0}$, ${K}^{+}{K}^{\ensuremath{-}}$, ${K}_{S}^{0}{K}_{S}^{0}$, $\ensuremath{\eta}\ensuremath{\eta}$, and ${\ensuremath{\eta}}^{\ensuremath{'}}{\ensuremath{\eta}}^{\ensuremath{'}}$ branching fractions, and a search for ${\ensuremath{\chi}}_{c}$ decays into $\ensuremath{\eta}{\ensuremath{\eta}}^{\ensuremath{'}}$. These results shed light on the mechanism of charmonium decays into pseudoscalar mesons.
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- 2009
- Full Text
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29. Study ofD0→π−e+νe,D+→π0e+νe,D0→K−e+νe, andD+→K¯0e+νein tagged decays of theψ(3770)resonance
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J. Wiss, P. Rubin, S. Mehrabyan, C. S. Park, Sheldon Stone, P. Naik, G. Tatishvili, J. Hietala, B. Moziak, E. J. White, F. Liu, J. Y. Ge, W. M. Sun, T. Skwarnicki, D. Hertz, Ian Shipsey, K. W. Edwards, W. Love, D. Peterson, D. Mohapatra, R. E. Mitchell, A. Lincoln, L. M. Zhang, Mats A Selen, J. C. Wang, D. Besson, A. Tomaradze, K. Y. Gao, V. E. Kuznetsov, L. Martin, T. K. Pedlar, A. Powell, J. M. Hunt, L. Gibbons, Ron Poling, H. Muramatsu, Marina Artuso, R. A. Briere, D. L. Hartill, Kamal K. Seth, Jonathan L. Rosner, G. S. Adams, S. Stroiney, B. K. Heltsley, J. Rademacker, S. Khalil, David Miller, X. Shi, J. Ledoux, K. Randrianarivony, J. Yelton, E. H. Thorndike, Y. S. Gao, Peter Onyisi, L. Fields, A. J. Sadoff, T. Wilksen, Q. He, V. Pavlunin, G. Bonvicini, J. Libby, P. Zweber, R. Gray, R. Ehrlich, D. Riley, V. Savinov, G. Wilkinson, J. Insler, Li Jingyuan, B. Xin, H. Mahlke-Krüger, N. Lowrey, D. Hu, F. Yang, J. R. Patterson, A. Ryd, A. W. Scott, J. P. Alexander, D. G. Cassel, B. Sanghi, S. W. Gray, R. Mountain, T. Klein, D. L. Kreinick, B. J.Y. Tan, K. M. Ecklund, H. Mendez, D. Cinabro, S. Blusk, J. E. Duboscq, Daniel P Cronin-Hennessy, Sean A Dobbs, M. Dubrovin, M. R. Shepherd, J. Napolitano, Yuichi Kubota, Helmut Vogel, S. B. Athar, B. W. Lang, J. Reed, David M. Asner, Z. Metreveli, J. Kandaswamy, and N. Sultana
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Quantum chromodynamics ,Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Cabibbo–Kobayashi–Maskawa matrix ,Branching fraction ,Electron–positron annihilation ,Lattice QCD ,7. Clean energy ,01 natural sciences ,Particle identification ,0103 physical sciences ,D meson ,Atomic physics ,Neutrino ,010306 general physics - Abstract
Using {psi}(3770){yields}DD events collected with the CLEO-c detector at the Cornell e{sup +}e{sup -} storage ring, tagged by fully reconstructing one D meson in a hadronic decay mode, we measure absolute branching fractions and differential decay rates for D{sup 0}{yields}{pi}{sup -}e{sup +}{nu}{sub e}, D{sup +}{yields}{pi}{sup 0}e{sup +}{nu}{sub e}, D{sup 0}{yields}K{sup -}e{sup +}{nu}{sub e}, and D{sup +}{yields}K{sup 0}e{sup +}{nu}{sub e}. The measured decay rates are used to study semileptonic form factors governing these transitions and to test unquenched Lattice QCD (LQCD) calculations. We average our results with previously published CLEO-c measurements of the same quantities using a neutrino reconstruction technique. Combining LQCD calculations of form factor absolute normalizations f{sub +}(0) and measurements of f{sub +}{sup {pi}}(0)|V{sub cd}| and f{sub +}{sup K}(0)|V{sub cs}|, we find |V{sub cd}|=0.222(8)(3)(23) and |V{sub cs}|=1.018(10)(8)(106), where the uncertainties are statistical, experimental systematic, and from LQCD, respectively.
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- 2009
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30. Measurement ofB(Ds+→l+ν)and the decay constantfDs+from600 pb−1ofe+e−annihilation data near 4170 MeV
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Werner Sun, Lei Zhang, D. Riley, G. S. Adams, M. Dubrovin, Xin Shi, K. W. Edwards, B. Sanghi, Jonas Rademacker, D. L. Hartill, N. Lowrey, D. Cinabro, Yuichi Kubota, R. A. Briere, T. K. Pedlar, A. W. Scott, A. Lincoln, A. Powell, D. Hu, D. Mohapatra, V. E. Kuznetsov, L. Martin, D. Z. Besson, S. Mehrabyan, Karl Matthew Ecklund, D. Cronin-Hennessy, F. Yang, Marina Artuso, J. M. Hunt, Jing Wang, G. Tatishvili, J. Y. Ge, T. Klein, S. W. Gray, James E Wiss, L. K. Gibbons, I. P.J. Shipsey, Anders Ryd, E. H. Thorndike, M. R. Shepherd, J. Ledoux, D. Hertz, D. H. Miller, S. Khalil, R. Gray, G. Bonvicini, Amiran Tomaradze, J. P. Alexander, R. E. Mitchell, J. Libby, J. Reed, K. Randrianarivony, John Yelton, J. Hietala, K. K. Seth, J. Kandaswamy, Sean A Dobbs, S. Blusk, R. S. Galik, J. Insler, N. Sultana, J. E. Duboscq, H. Muramatsu, D. Peterson, D. M. Asner, Mats A Selen, Sheldon Stone, S. Stroiney, Jonathan L. Rosner, Tomasz Skwarnicki, B. Moziak, C. S. Park, L. Fields, Hans J. Vogel, Juliet Ritchie Patterson, A. N. Robichaud, B. Xin, P. Naik, K. Y. Gao, H. Mendez, E. J. White, G. Wilkinson, Mark Smith, Peter Onyisi, D. L. Kreinick, A. J. Sadoff, T. Wilksen, R. Poling, Q. He, V. Pavlunin, Li Jingyuan, B. K. Heltsley, R. Mountain, D. G. Cassel, P. Rubin, P. Zweber, B. J.Y. Tan, J. Napolitano, Z. Metreveli, R. Ehrlich, and H. Mahlke-Krüger
- Subjects
Physics ,Nuclear and High Energy Physics ,Antiparticle ,Particle physics ,Annihilation ,Muon ,Meson ,010308 nuclear & particles physics ,Electron–positron annihilation ,Hadron ,Elementary particle ,01 natural sciences ,Particle decay ,Crystallography ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,010306 general physics - Abstract
We examine e{sup +}e{sup -}{yields}D{sub s}{sup -}D{sub s}*{sup +} and D{sub s}*{sup -}D{sub s}{sup +} interactions at 4170 MeV using the CLEO-c detector in order to measure the decay constant f{sub D{sub s}{sup +}} with good precision. Previously our measurements were substantially higher than the most precise lattice based QCD calculation of (241{+-}3) MeV. Here we use the D{sub s}{sup +}{yields}l{sup +}{nu} channel, where the l{sup +} designates either a {mu}{sup +} or a {tau}{sup +}, when the {tau}{sup +}{yields}{pi}{sup +}{nu}. Analyzing both modes independently, we determine B(D{sub s}{sup +}{yields}{mu}{sup +}{nu})=(0.565{+-}0.045{+-}0.017)%, and B(D{sub s}{sup +}{yields}{tau}{sup +}{nu})=(6.42{+-}0.81{+-}0.18)%. We also analyze them simultaneously to find an effective value of B{sup eff}(D{sub s}{sup +}{yields}{mu}{sup +}{nu})=(0.591{+-}0.037{+-}0.018)% and f{sub D{sub s}{sup +}}=(263.3{+-}8.2{+-}3.9) MeV. Combining with the CLEO-c value determined independently using D{sub s}{sup +}{yields}{tau}{sup +}{nu}, {tau}{sup +}{yields}e{sup +}{nu}{nu} decays, we extract f{sub D{sub s}{sup +}}=(259.5{+-}6.6{+-}3.1) MeV. Combining with our previous determination of B(D{sup +}{yields}{mu}{sup +}{nu}), we extract the ratio f{sub D{sub s}{sup +}}/f{sub D{sup +}}=1.26{+-}0.06{+-}0.02. No evidence is found for a CP asymmetry between {gamma}(D{sub s}{sup +}{yields}{mu}{sup +}{nu}) and {gamma}(D{sub s}{sup -}{yields}{mu}{sup -}{nu}); specifically the fractional difference in rates is measured to be (4.8{+-}6.1)%. Finally, we find B(D{sub s}{sup +}{yields}e{sup +}{nu})
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- 2009
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31. Improved measurement of absolute branching fraction ofDs+→τ+ντ
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A. N. Robichaud, I. P.J. Shipsey, V. E. Kuznetsov, H. Mendez, S. B. Athar, T. Klein, Xin Shi, D. Z. Besson, K. W. Edwards, S. Khalil, D. G. Cassel, G. Bonvicini, J. P. Alexander, S. Blusk, J. Insler, J. Kandaswamy, Mats A Selen, J. E. Duboscq, P. Naik, Werner Sun, Lei Zhang, N. Sultana, F. Yang, R. S. Galik, Hans J. Vogel, Ron Poling, Mark Smith, J. Libby, K. Randrianarivony, B. Sanghi, D. Peterson, Peter Onyisi, David M. Asner, D. Hu, B. J.Y. Tan, J. Napolitano, Q. He, V. Pavlunin, J. Y. Ge, James E Wiss, J. Ledoux, Jonas Rademacker, N. Lowrey, D. Cinabro, Kamal K. Seth, A. Powell, Karl Matthew Ecklund, T. K. Pedlar, G. S. Adams, J. M. Hunt, R. E. Mitchell, G. Tatishvili, Juliet Ritchie Patterson, D. Mohapatra, Daniel P Cronin-Hennessy, G. Wilkinson, R. Gray, Anders Ryd, L. Martin, P. Zweber, John Yelton, Amiran Tomaradze, Sean A Dobbs, R. Ehrlich, M. R. Shepherd, S. Mehrabyan, Marina Artuso, J. Reed, R. Mountain, A. W. Scott, P. Rubin, E. H. Thorndike, S. Stroiney, J. Hietala, Jonathan L. Rosner, Tomasz Skwarnicki, Sheldon Stone, H. Muramatsu, D. L. Hartill, A. Lincoln, Jing Wang, H. Mahlke-Krüger, D. H. Miller, B. Moziak, S. W. Gray, C. S. Park, L. Fields, R. A. Briere, D. Riley, E. J. White, M. Dubrovin, Z. Metreveli, Yuichi Kubota, B. Xin, K. Y. Gao, B. K. Heltsley, A. J. Sadoff, T. Wilksen, Li Jingyuan, D. L. Kreinick, L. K. Gibbons, and D. Hertz
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Branching fraction ,Electron–positron annihilation ,01 natural sciences ,Particle identification ,Crystallography ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,High Energy Physics::Experiment ,Production (computer science) ,Exponential decay ,010306 general physics ,Energy (signal processing) - Abstract
We have studied the leptonic decay D{sub s}{sup +}{yields}{tau}{sup +}{nu}{sub {tau}}, via the decay channel {tau}{sup +}{yields}e{sup +}{nu}{sub e}{nu}{sub {tau}}, using a sample of tagged D{sub s}{sup +} decays collected near the D{sub s}*{sup {+-}}D{sub s}{sup {+-}} peak production energy in e{sup +}e{sup -} collisions with the CLEO-c detector. We obtain B(D{sub s}{sup +}{yields}{tau}{sup +}{nu}{sub {tau}})=(5.30{+-}0.47{+-}0.22)% and determine the decay constant f{sub D{sub s}}=(252.5{+-}11.1{+-}5.2) MeV, where the first uncertainties are statistical and the second are systematic.
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- 2009
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32. Observation ofD+→ηe+νe
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Z. Metreveli, R. Ehrlich, H. Mahlke-Krüger, O. Aquines, G. Tatishvili, D. Mohapatra, V. E. Kuznetsov, J. Hietala, Marina Artuso, J. P. Cummings, T. Klein, D. Z. Besson, S. W. Gray, C. S. Park, R. A. Briere, Werner Sun, L. Fields, Alan D. Lopez, Hans J. Vogel, D. L. Kreinick, A. J. Sadoff, T. Wilksen, John Yelton, S. Stroiney, David M. Asner, E. J. White, J. Pivarski, Jonathan L. Rosner, Tomasz Skwarnicki, S. Nisar, G. S. Huang, V. Savinov, B. Moziak, Li Jingyuan, Mats A Selen, E. H. Thorndike, M. E. Watkins, D. Riley, D. H. Kim, B. K. Heltsley, J. Insler, M. Dubrovin, D. L. Hartill, J. Kandaswamy, H. Mendez, S. B. Athar, J. A. Ernst, F. Yang, I. Danko, G. Bonvicini, J. P. Alexander, N. Menaa, Yuichi Kubota, D. Peterson, V. Potlia, B. Xin, L. K. Gibbons, R. Gray, R. Patel, C. Cawlfield, James E Wiss, Sheldon Stone, D. Hertz, K. Y. Gao, Amiran Tomaradze, R. E. Mitchell, A. Smith, R. S. Galik, D. Hu, P. Rubin, R. Sia, J. Butt, K. M. Ecklund, H. Schwarthoff, T. K. Pedlar, J. Napolitano, S. Mehrabyan, D. G. Cassel, Jing Wang, B. W. Lang, D. H. Miller, I. Karliner, G. S. Adams, I. P.J. Shipsey, B. I. Eisenstein, S. Blusk, P. Zweber, J. E. Duboscq, K. Zhang, R. Mountain, Kamal K. Seth, Peter Onyisi, W. Love, A. W. Scott, R. Poling, Q. He, V. Pavlunin, Xin Shi, K. W. Edwards, B. Sanghi, Juliet Ritchie Patterson, N. E. Adam, Daniel P Cronin-Hennessy, Sean A Dobbs, Horst Severini, C. D. Jones, A. Lincoln, J. E. Ramirez, Thomas Ferguson, K. Randrianarivony, M. Anderson, N. Lowrey, D. Cinabro, P. Naik, Anders Ryd, M. R. Shepherd, and H. Muramatsu
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Physics ,010308 nuclear & particles physics ,General Physics and Astronomy ,Resonance ,01 natural sciences ,Particle identification ,Particle decay ,Crystallography ,Nuclear magnetic resonance ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,High Energy Physics::Experiment ,Cornell Electron Storage Ring ,010306 general physics - Abstract
Using a 281 pb{sup -1} data sample collected at the {psi}(3770) resonance with the CLEO-c detector at the Cornell Electron Storage Ring, we report the first observation of D{sup +}{yields}{eta}e{sup +}{nu}{sub e}. We also set upper limits for D{sup +}{yields}{eta}{sup '}e{sup +}{nu}{sub e} and D{sup +}{yields}{phi}e{sup +}{nu}{sub e} that are about 2 orders of magnitude more restrictive than those obtained by previous experiments.
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- 2009
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33. Observation ofη′Decays toπ+π−π0andπ+π−e+e−
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Werner Sun, Lei Zhang, Juliet Ritchie Patterson, J. C. Wang, A. Lincoln, D. Hu, J. M. Hunt, V. E. Kuznetsov, D. Mohapatra, C. S. Park, B. Xin, Jonas Rademacker, J. Libby, R. Gray, Amiran Tomaradze, Marina Artuso, D. Z. Besson, Daniel P Cronin-Hennessy, Sean A Dobbs, L. Fields, S. Blusk, I. P.J. Shipsey, K. Randrianarivony, John Yelton, K. Y. Gao, R. Ehrlich, D. G. Cassel, J. E. Duboscq, D. L. Hartill, Anders Ryd, D. Riley, M. R. Shepherd, D. L. Kreinick, A. J. Sadoff, T. Wilksen, H. Mahlke-Krüger, M. Dubrovin, Mats A Selen, N. Lowrey, D. Cinabro, F. Yang, Z. Metreveli, S. Stroiney, Hans J. Vogel, J. Insler, Jonathan L. Rosner, Tomasz Skwarnicki, S. Mehrabyan, P. Zweber, B. J.Y. Tan, J. Napolitano, Yuichi Kubota, David M. Asner, B. Moziak, A. N. Robichaud, R. Mountain, J. Y. Ge, James E Wiss, H. Mendez, Li Jingyuan, R. E. Mitchell, S. B. Athar, P. Rubin, Kamal K. Seth, A. Powell, B. K. Heltsley, G. Wilkinson, H. Muramatsu, Karl Matthew Ecklund, G. Tatishvili, J. Kandaswamy, Sheldon Stone, N. Sultana, Xin Shi, D. Peterson, K. W. Edwards, T. K. Pedlar, B. Sanghi, E. H. Thorndike, S. Khalil, G. Bonvicini, J. P. Alexander, A. W. Scott, R. S. Galik, R. A. Briere, J. Hietala, S. W. Gray, T. Klein, J. Ledoux, E. J. White, L. K. Gibbons, G. S. Adams, L. Martin, D. Hertz, Peter Onyisi, R. Poling, Q. He, V. Pavlunin, D. H. Miller, P. Naik, and J. Reed
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Physics ,Particle decay ,Crystallography ,Particle physics ,010308 nuclear & particles physics ,Branching fraction ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,Isospin ,Electron–positron annihilation ,0103 physical sciences ,General Physics and Astronomy ,010306 general physics ,01 natural sciences - Abstract
Using {psi}(2S){yields}{pi}{sup +}{pi}{sup -}J/{psi}, J/{psi}{yields}{gamma}{eta}{sup '} events acquired with the CLEO-c detector at the CESR e{sup +}e{sup -} collider, we make the first observations of the decays {eta}{sup '}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup 0} and {eta}{sup '}{yields}{pi}{sup +}{pi}{sup -}e{sup +}e{sup -}, measuring absolute branching fractions (37{sub -9}{sup +11}{+-}4)x10{sup -4} and (25{sub -9}{sup +12}{+-}5)x10{sup -4}, respectively. For {eta}{sup '}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup 0}, this result probes the mechanism of isospin violation and the roles of {pi}{sup 0}/{eta}/{eta}{sup '}-mixing and final state rescattering in strong decays. We also set upper limits on branching fractions for {eta}{sup '} decays to {pi}{sup +}{pi}{sup -}{mu}{sup +}{mu}{sup -}, 2({pi}{sup +}{pi}{sup -}), {pi}{sup +}{pi}{sup -}2{pi}{sup 0}, 2({pi}{sup +}{pi}{sup -}){pi}{sup 0}, 3({pi}{sup +}{pi}{sup -}), and invisible final states.
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- 2009
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34. Observation of eta' decays to pi+pi-pi0 and pi+pi-e+e
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P, Naik, J, Rademacker, D M, Asner, K W, Edwards, J, Reed, A N, Robichaud, G, Tatishvili, R A, Briere, H, Vogel, P U E, Onyisi, J L, Rosner, J P, Alexander, D G, Cassel, J E, Duboscq, R, Ehrlich, L, Fields, R S, Galik, L, Gibbons, R, Gray, S W, Gray, D L, Hartill, B K, Heltsley, D, Hertz, J M, Hunt, J, Kandaswamy, D L, Kreinick, V E, Kuznetsov, J, Ledoux, H, Mahlke-Krüger, D, Mohapatra, J R, Patterson, D, Peterson, D, Riley, A, Ryd, A J, Sadoff, X, Shi, S, Stroiney, W M, Sun, T, Wilksen, S B, Athar, J, Yelton, P, Rubin, S, Mehrabyan, N, Lowrey, M, Selen, E J, White, J, Wiss, R E, Mitchell, M R, Shepherd, D, Besson, T K, Pedlar, D, Cronin-Hennessy, K Y, Gao, J, Hietala, Y, Kubota, T, Klein, R, Poling, A W, Scott, P, Zweber, S, Dobbs, Z, Metreveli, K K, Seth, B J Y, Tan, A, Tomaradze, J, Libby, L, Martin, A, Powell, G, Wilkinson, H, Mendez, J Y, Ge, D H, Miller, V, Pavlunin, B, Sanghi, I P J, Shipsey, B, Xin, G S, Adams, D, Hu, B, Moziak, J, Napolitano, Q, He, J, Insler, H, Muramatsu, C S, Park, E H, Thorndike, F, Yang, M, Artuso, S, Blusk, S, Khalil, J, Li, R, Mountain, K, Randrianarivony, N, Sultana, T, Skwarnicki, S, Stone, J C, Wang, L M, Zhang, G, Bonvicini, D, Cinabro, M, Dubrovin, A, Lincoln, and K M, Ecklund
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High Energy Physics::Experiment ,Nuclear Experiment - Abstract
Using psi(2S)-->pi;{+}pi;{-}J/psi, J/psi-->gammaeta;{'} events acquired with the CLEO-c detector at the CESR e;{+}e;{-} collider, we make the first observations of the decays eta;{'}-->pi;{+}pi;{-}pi;{0} and eta;{'}-->pi;{+}pi;{-}e;{+}e;{-}, measuring absolute branching fractions (37_{-9};{+11}+/-4)x10;{-4} and (25_{-9};{+12}+/-5)x10;{-4}, respectively. For eta;{'}-->pi;{+}pi;{-}pi;{0}, this result probes the mechanism of isospin violation and the roles of pi;{0}/eta/eta;{'}-mixing and final state rescattering in strong decays. We also set upper limits on branching fractions for eta;{'} decays to pi;{+}pi;{-}micro;{+}micro;{-}, 2(pi;{+}pi;{-}), pi;{+}pi;{-}2pi;{0}, 2(pi;{+}pi;{-})pi;{0}, 3(pi;{+}pi;{-}), and invisible final states.
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- 2009
35. Improved measurement of branching fractions forππtransitions amongΥ(nS)states
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J. Libby, John Yelton, K. Randrianarivony, J. Reed, J. Ledoux, Z. Metreveli, M. Anderson, P. Rubin, E. J. White, Mats A Selen, P. Naik, S. R. Bhari, H. Mendez, C. S. Park, S. B. Athar, I. P.J. Shipsey, E. H. Thorndike, F. Yang, Peter Onyisi, Ron Poling, K. M. Ecklund, L. Fields, I. Danko, Daniel P Cronin-Hennessy, Sean A Dobbs, D. Hu, D. L. Kreinick, Hans J. Vogel, R. A. Briere, Jing Wang, Q. He, Thomas Ferguson, J. Y. Ge, W. Love, B. W. Lang, G. Tatishvili, David M. Asner, D. H. Miller, N. Lowrey, James E Wiss, D. Cinabro, J. Napolitano, V. E. Kuznetsov, J. Hietala, G. S. Adams, Juliet Ritchie Patterson, T. K. Pedlar, D. Riley, L. Martin, J. P. Cummings, R. E. Mitchell, S. Stroiney, Jonathan L. Rosner, Tomasz Skwarnicki, T. Klein, M. Dubrovin, S. Blusk, D. Z. Besson, L. K. Gibbons, Kamal K. Seth, A. Powell, R. Patel, S. W. Gray, D. Hertz, A. W. Scott, S. Khalil, J. E. Duboscq, R. Gray, Sheldon Stone, G. Bonvicini, J. P. Alexander, Yuichi Kubota, B. Moziak, J. Insler, Werner Sun, Lei Zhang, E. Engelson, Amiran Tomaradze, I. Karliner, R. S. Galik, D. L. Hartill, A. Lincoln, S. Nisar, B. I. Eisenstein, Xin Shi, P. Zweber, K. W. Edwards, D. G. Cassel, R. Mountain, J. M. Hunt, G. Wilkinson, S. Mehrabyan, M. E. Watkins, Jonas Rademacker, B. Xin, J. Kandaswamy, K. Y. Gao, N. Sultana, D. Peterson, D. Mohapatra, Marina Artuso, H. Muramatsu, Anders Ryd, M. R. Shepherd, R. Ehrlich, H. Mahlke-Krüger, B. K. Heltsley, A. J. Sadoff, T. Wilksen, V. Savinov, and Li Jingyuan
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Physics ,Nuclear and High Energy Physics ,Particle decay ,Crystallography ,010308 nuclear & particles physics ,Branching fraction ,Electron–positron annihilation ,0103 physical sciences ,Atomic physics ,010306 general physics ,Branching (polymer chemistry) ,01 natural sciences ,Particle identification - Abstract
Using samples of (5.93{+-}0.10)x10{sup 6} {upsilon}(3S) decays and (9.11{+-}0.14)x10{sup 6} {upsilon}(2S) decays collected with the CLEO detector, we report improved measurements of the following branching fractions: B({upsilon}(3S){yields}{upsilon}(1S){pi}{sup +}{pi}{sup -})=(4.46{+-}0.01{+-}0.13)%, B({upsilon}(2S){yields}{upsilon}(1S){pi}{sup +}{pi}{sup -})=(18.02{+-}0.02{+-}0.61)%, B({upsilon}(3S){yields}{upsilon}(1S){pi}{sup 0}{pi}{sup 0})=(2.24{+-}0.09{+-}0.11)%, B({upsilon}(2S){yields} {upsilon}(1S){pi}{sup 0}{pi}{sup 0})=(8.43{+-}0.16{+-}0.42)%, and B({upsilon}(3S){yields}{upsilon}(2S){pi}{sup 0}{pi}{sup 0})=(1.82{+-}0.09{+-}0.12)%. In each case, the first uncertainty reported is statistical, while the second is systematic.
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- 2009
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36. J/ψandψ(2S)Radiative Transitions toηc
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Rishi Patel, D. M. Asner, H. Muramatsu, A. Lincoln, D. Mohapatra, Michael T. Anderson, P. Rubin, J. Insler, G. Wilkinson, K. K. Seth, T. K. Pedlar, N. Lowrey, D. Riley, D. Cinabro, Alan D. Lopez, J. E. Duboscq, K. W. Edwards, John Yelton, J. Hietala, D. L. Kreinick, Marina Artuso, R. A. Briere, Sheldon Stone, S. Mehrabyan, R. Ehrlich, M. Dubrovin, J. P. Cummings, M. E. Watkins, G. S. Adams, A. Powell, D. Z. Besson, Anders Ryd, Helmut Vogel, E. H. Thorndike, H. Mahlke-Krüger, M. R. Shepherd, Peter Onyisi, R. Mountain, Yuichi Kubota, Ian Shipsey, V. Savinov, T. Skwarnicki, Mats A Selen, J. E. Ramirez, G. Tatishvili, A. J. Sadoff, H. Mendez, Werner Sun, B. Xin, G. Bonvicini, Q. He, P. Naik, Li Jingyuan, J. P. Alexander, D. G. Cassel, J. Y. Ge, D. L. Hartill, Lei Zhang, K. Y. Gao, I. Karliner, James E Wiss, S. W. Gray, Sean A Dobbs, Peter K. Zweber, J. Ledoux, J. M. Hunt, Thomas Ferguson, R. Poling, Jing Wang, R. E. Mitchell, S. B. Athar, S. Blusk, J. Libby, Juliet Ritchie Patterson, R. S. Galik, B. K. Heltsley, B. W. Lang, B. I. Eisenstein, D. H. Miller, Z. Metreveli, W. Love, E. J. White, J. Kandaswamy, S. Nisar, L. K. Gibbons, D. Hertz, N. Sultana, T. Wilksen, D. Peterson, K. Randrianarivony, J. Napolitano, Amiran Tomaradze, K. M. Ecklund, D. Hu, D. Cronin-Hennessy, F. Yang, I. Danko, J. Reed, Jonas Rademacker, A. W. Scott, C. S. Park, Richard Gray, L. Fields, Xin Shi, Sadia Khalil, S. Stroiney, Jonathan L. Rosner, B. Moziak, V. E. Kuznetsov, and T. Klein
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Physics ,010308 nuclear & particles physics ,Magnetic dipole transition ,Electron–positron annihilation ,High Energy Physics::Phenomenology ,Analytical chemistry ,General Physics and Astronomy ,01 natural sciences ,3. Good health ,Nuclear physics ,0103 physical sciences ,Radiative transfer ,High Energy Physics::Experiment ,010306 general physics ,Magnetic dipole ,Line (formation) - Abstract
Using 24.5 million psi(2S) decays collected with the CLEO-c detector at CESR we present the most precise measurements of magnetic dipole transitions in the charmonium system. We measure B(psi(2S)->gamma eta_c) = (4.32+/-0.16+/-0.60)x10^-3, B(J/psi->gamma eta_c)/B(psi(2S)->gamma eta_c) = 4.59+/-0.23+/-0.64, and B(J/psi->gamma eta_c) = (1.98+/-0.09+/-0.30)%. We observe a distortion in the eta_c line shape due to the photon-energy dependence of the magnetic dipole transition rate. We find that measurements of the eta_c mass are sensitive to the line shape, suggesting an explanation for the discrepancy between measurements of the eta_c mass in radiative transitions and other production mechanisms.
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- 2009
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37. InclusiveχbJ(nP)decays toD0X
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J. E. Ramirez, A. W. Scott, D. Hu, B. W. Lang, Mats A Selen, D. H. Miller, M. E. Watkins, H. Mendez, Werner Sun, S. B. Athar, G. Tatishvili, P. Rubin, Lei Zhang, T. K. Pedlar, D. Riley, Jonas Rademacker, J. Libby, K. Randrianarivony, M. Anderson, N. Lowrey, D. Cinabro, R. Ehrlich, H. Muramatsu, J. P. Cummings, T. Ferguson, M. Dubrovin, K. M. Ecklund, S. Blusk, D. Z. Besson, S. Nisar, H. Mahlke-Krüger, G. Wilkinson, Z. Metreveli, Alan D. Lopez, Hans J. Vogel, G. S. Adams, Anders Ryd, John Yelton, J. Hietala, J. E. Duboscq, M. R. Shepherd, V. E. Kuznetsov, B. Xin, Peter Onyisi, J. Insler, Yuichi Kubota, J. Napolitano, R. Gray, K. Y. Gao, Q. He, Amiran Tomaradze, T. Klein, J. Kandaswamy, J. Reed, K. W. Edwards, D. G. Cassel, S. Khalil, S. Stroiney, P. Zweber, D. M. Asner, J. Y. Ge, F. Yang, G. Bonvicini, I. Danko, J. P. Alexander, James E Wiss, P. Naik, Ron Poling, Juliet Ritchie Patterson, Jonathan L. Rosner, Tomasz Skwarnicki, E. H. Thorndike, R. E. Mitchell, B. K. Heltsley, D. Mohapatra, N. Sultana, A. J. Sadoff, T. Wilksen, Marina Artuso, Daniel P Cronin-Hennessy, Sean A Dobbs, R. Mountain, X. Shi, V. Savinov, L. K. Gibbons, R. Patel, D. Hertz, Li Jingyuan, D. Peterson, D. L. Kreinick, R. S. Galik, Kamal K. Seth, A. Powell, I. Karliner, I. P.J. Shipsey, B. I. Eisenstein, W. Love, B. Moziak, S. Mehrabyan, Sheldon Stone, C. S. Park, L. Fields, J. C. Wang, D. L. Hartill, A. Lincoln, S. W. Gray, R. A. Briere, and E. J. White
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Quantum chromodynamics ,Physics ,Nuclear and High Energy Physics ,Meson ,010308 nuclear & particles physics ,Hadron ,Elementary particle ,01 natural sciences ,Particle identification ,Particle decay ,Pion ,0103 physical sciences ,Production (computer science) ,Atomic physics ,010306 general physics - Abstract
Using {upsilon}(2S) and {upsilon}(3S) data collected with the CLEO III detector we have searched for decays of {chi}{sub bJ} to final states with open charm. We fully reconstruct D{sup 0} mesons with p{sub D{sup 0}}>2.5 GeV/c in three decay modes (K{sup -}{pi}{sup +}, K{sup -}{pi}{sup +}{pi}{sup 0}, and K{sup -}{pi}{sup -}{pi}{sup +}{pi}{sup +}) in coincidence with radiative transition photons that tag the production of one of the {chi}{sub bJ}(nP) states. Significant signals are obtained for the two J=1 states. Recent nonrelativistic QCD (NRQCD) calculations of {chi}{sub bJ}(nP){yields}ccX depend on one nonperturbative parameter per {chi}{sub bJ} triplet. The extrapolation from the observed D{sup 0}X rate over a limited momentum range to a full ccX rate also depends on these same parameters. Using our data to fit for these parameters, we extract results which agree well with NRQCD predictions, confirming the expectation that charm production is largest for the J=1 states. In particular, for J=1, our results are consistent with ccg accounting for about one-quarter of all hadronic decays.
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- 2008
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38. Observation ofχbJ(1P,2P)decays to light hadrons
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K. W. Edwards, J. Yelton, V. Savinov, A. W. Scott, G. Tatishvili, S. Blusk, R. Gray, W. M. Sun, D. Peterson, T. Skwarnicki, Amiran Tomaradze, S. Khalil, L. M. Zhang, V. E. Kuznetsov, Y. Kubota, D. Hu, S. W. Gray, P. U.E. Onyisi, D. G. Cassel, B. Xin, P. Rubin, T. Klein, D. Mohapatra, J. P. Alexander, H. Mendez, J. Libby, S. B. Athar, H. Vogel, P. Zweber, Kamal K. Seth, A. J. Sadoff, K. Y. Gao, R. S. Galik, T. Wilksen, Marina Artuso, Ron Poling, X. Shi, K. Randrianarivony, L. K. Gibbons, K. M. Ecklund, D. M. Asner, J. Y. Ge, James E Wiss, D. Hertz, Daniel P Cronin-Hennessy, Sean A Dobbs, J. Reed, Li Jingyuan, T. K. Pedlar, R. Ehrlich, M. Selen, J. R. Patterson, W. Love, J. E. Duboscq, B. J.Y. Tan, J. Napolitano, H. Mahlke-Krüger, B. I. Eisenstein, A. Ryd, R. E. Mitchell, Brian Heltsley, R. Mountain, E. H. Thorndike, N. Lowrey, J. Hietala, J. M. Hunt, D. L. Kreinick, F. Yang, A. Powell, D. Riley, Q. He, M. Dubrovin, R. A. Briere, J. Insler, S. Mehrabyan, I. Karliner, B. W. Lang, J. Rademacker, G. S. Adams, L. Martin, J. Kandaswamy, D. H. Miller, N. Sultana, G. Bonvicini, P. Naik, M. R. Shepherd, S. Stroiney, Jonathan L. Rosner, Z. Metreveli, B. Moziak, J. Ledoux, H. Muramatsu, E. J. White, C. S. Park, L. Fields, I. P.J. Shipsey, J. C. Wang, Sheldon Stone, D. Besson, D. L. Hartill, A. Lincoln, G. Wilkinson, and D. Cinabro
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Branching fraction ,Hadron ,Radiative decay ,01 natural sciences ,Particle identification ,Dipole ,Electric dipole moment ,Particle decay ,0103 physical sciences ,B meson ,010306 general physics - Abstract
Analyzing {upsilon}(nS) decays acquired with the CLEO detector operating at the CESR e{sup +}e{sup -} collider, we measure for the first time the product branching fractions B[{upsilon}(nS){yields}{gamma}{chi}{sub bJ}((n-1)P)]B[{chi}{sub bJ}(n-1)P){yields}X{sub i}] for n=2 and 3, where X{sub i} denotes, for each i, one of the 14 exclusive light-hadron final states for which we observe significant signals in both {chi}{sub bJ}(1P) and {chi}{sub bJ}(2P) decays. We also determine upper limits for the electric dipole (E1) transitions {upsilon}(3S){yields}{gamma}{chi}{sub bJ}(1P)
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- 2008
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39. First observation of exclusiveχcJdecays to two charged and two neutral hadrons
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T. K. Pedlar, B. K. Heltsley, A. J. Sadoff, T. Wilksen, X. Shi, V. Savinov, Li Jingyuan, L. K. Gibbons, B. Xin, R. Patel, D. Hertz, D. Mohapatra, John Yelton, J. Hietala, Marina Artuso, K. Y. Gao, S. Khalil, G. Bonvicini, J. P. Alexander, S. Stroiney, Jonathan L. Rosner, Tomasz Skwarnicki, M. E. Watkins, Alan D. Lopez, Hans J. Vogel, B. Moziak, C. S. Park, Ron Poling, R. Gray, L. Fields, N. Menaa, J. E. Ramirez, I. P.J. Shipsey, Amiran Tomaradze, T. Ferguson, P. Rubin, R. Sia, J. Y. Ge, James E Wiss, C. D. Jones, D. Hu, N. Lowrey, D. Cinabro, K. M. Ecklund, J. C. Wang, R. A. Briere, D. L. Hartill, A. Lincoln, G. Tatishvili, J. P. Cummings, S. Blusk, R. E. Mitchell, D. Z. Besson, I. Karliner, J. Napolitano, K. Randrianarivony, Mats A Selen, J. E. Duboscq, B. I. Eisenstein, W. Love, M. Anderson, E. J. White, G. S. Adams, Juliet Ritchie Patterson, N. E. Adam, D. M. Asner, E. H. Thorndike, P. Zweber, Z. Metreveli, R. Mountain, S. W. Gray, D. L. Kreinick, H. Mendez, S. B. Athar, Peter Onyisi, B. W. Lang, D. H. Miller, Daniel P Cronin-Hennessy, Sean A Dobbs, Q. He, Kamal K. Seth, R. Ehrlich, J. Kandaswamy, H. Mahlke-Krüger, Werner Sun, Lei Zhang, Anders Ryd, M. R. Shepherd, N. Sultana, Sheldon Stone, S. Nisar, H. Muramatsu, D. Peterson, P. Naik, J. Insler, V. E. Kuznetsov, S. Mehrabyan, T. Klein, D. Riley, F. Yang, I. Danko, M. Dubrovin, K. W. Edwards, D. G. Cassel, Yuichi Kubota, B. Sanghi, and A. W. Scott
- Subjects
Physics ,Nuclear and High Energy Physics ,Particle physics ,Meson ,010308 nuclear & particles physics ,Hadron ,Resonance ,Elementary particle ,01 natural sciences ,Particle identification ,3. Good health ,Particle decay ,Crystallography ,Pion ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,010306 general physics ,Boson - Abstract
We study exclusive {chi}{sub c0,1,2} decays to four-hadron final states involving two charged and two neutral hadrons: {pi}{sup +}{pi}{sup -}{pi}{sup 0}{pi}{sup 0}, K{sup +}K{sup -}{pi}{sup 0}{pi}{sup 0}, pp{pi}{sup 0}{pi}{sup 0}, K{sup +}K{sup -}{eta}{pi}{sup 0}, and K{sup {+-}}{pi}{sup {+-}}K{sup 0}{pi}{sup 0}. The {chi}{sub c} states are produced in radiative decays of 3.08x10{sup 6} {psi}(2S) resonance decays and observed in the CLEO detector. We also measure the largest substructure contributions to the modes {pi}{sup +}{pi}{sup -}{pi}{sup 0}{pi}{sup 0} and K{sup {+-}}{pi}{sup {+-}}K{sup 0}{pi}{sup 0}.
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- 2008
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40. Observation ofΥ(2S)→ηΥ(1S)and Search for Related Transitions
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K. W. Edwards, S. W. Gray, N. Lowrey, S. Mehrabyan, Brian Heltsley, J. M. Hunt, R. Ehrlich, B. I. Eisenstein, G. Tatishvili, G. S. Adams, J. Yelton, P. Zweber, H. Mendez, S. B. Athar, L. M. Zhang, J. Hietala, J. Reed, L. Martin, A. Powell, P. Naik, H. Mahlke-Krüger, W. M. Sun, J. P. Cummings, S. Blusk, J. P. Alexander, I. P.J. Shipsey, M. Selen, D. G. Cassel, Daniel P Cronin-Hennessy, Sean A Dobbs, P. Rubin, S. Nisar, D. H. Miller, J. Libby, H. Vogel, B. Xin, D. Mohapatra, J. Kandaswamy, K. Randrianarivony, J. C. Wang, I. Karliner, J. Y. Ge, A. J. Sadoff, James E Wiss, J. E. Duboscq, B. W. Lang, K. Y. Gao, Marina Artuso, N. Sultana, M. Anderson, V. E. Kuznetsov, R. Mountain, A. Ryd, D. L. Hartill, A. Lincoln, T. Wilksen, X. Shi, E. H. Thorndike, G. Bonvicini, L. K. Gibbons, Sheldon Stone, Ron Poling, R. E. Mitchell, D. Peterson, T. Klein, F. Yang, Y. Kubota, I. Danko, R. Patel, D. Hertz, W. Love, G. Wilkinson, T. K. Pedlar, D. L. Kreinick, Li Jingyuan, Thomas Ferguson, J. R. Patterson, Q. He, P. U.E. Onyisi, D. Besson, Kamal K. Seth, H. Muramatsu, R. Gray, M. E. Watkins, T. Skwarnicki, D. Cinabro, Amiran Tomaradze, D. Riley, D. M. Asner, D. Hu, M. Dubrovin, V. Savinov, A. W. Scott, J. Rademacker, M. R. Shepherd, S. Khalil, K. M. Ecklund, R. S. Galik, J. Napolitano, C. S. Park, L. Fields, S. Stroiney, Jonathan L. Rosner, J. Xavier, Z. Metreveli, B. Moziak, J. Ledoux, E. J. White, R. A. Briere, and J. Insler
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Physics ,Crystallography ,Meson ,010308 nuclear & particles physics ,Branching fraction ,0103 physical sciences ,Hadron ,General Physics and Astronomy ,Elementary particle ,010306 general physics ,01 natural sciences ,Particle identification ,Dimensionless quantity - Abstract
We report the first observation of Y(2S) → ηY(1S), with a branching fraction Β = (2.1 +0.7 -0.6 (stat) ± 0.3(syst)) X 10 -4 and a statistical significance 5.3σ. Data were acquired with the CLEO III detector at the CESR e + e - symmetric collider. This is the first process observed involving a b-quark spin flip. For related transitions, 90% confidence limits in units of 10 -4 are Β(Y(2S) → π 0 Y(1S)) < 1.8, Β(Y(3S) → ηY(1S)) < 1.8, B(Y(3S) →π 0 Y(1S)) < 0.7, and Β(Y(3S) → π 0 Y(2S)) < 5.1.
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- 2008
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41. Search for Lepton Flavor Violation in Upsilon Decays
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Sheldon Stone, G. Tatishvili, G. S. Huang, J. E. Ramirez, H. Mendez, A. J. Sadoff, S. B. Athar, F. Yang, J. P. Cummings, John Yelton, J. Hietala, T. Wilksen, I. Danko, J. Pivarski, Dong-Hyun Kim, W. Love, A. W. Scott, H. Schwarthoff, X. Shi, S. Stroiney, R. A. Briere, Jonathan L. Rosner, Tomasz Skwarnicki, G. S. Adams, D. Z. Besson, Karl Berkelman, D. L. Kreinick, Peter Onyisi, Helmut Vogel, H. Muramatsu, V. Savinov, Ron Poling, N. Lowrey, D. Cinabro, L. K. Gibbons, N. Menaa, B. Moziak, C. D. Jones, Alan D. Lopez, James E Wiss, J. C. Wang, R. Patel, D. Hertz, C. S. Park, D. Mohapatra, P. Zweber, D. L. Hartill, Anders Ryd, M. R. Shepherd, A. Lincoln, E. H. Thorndike, Q. He, V. Pavlunin, L. Fields, V. E. Kuznetsov, Marina Artuso, R. E. Mitchell, R. Mountain, B. W. Lang, Ian Shipsey, D. Hu, B. Xin, S. Khalil, G. Bonvicini, J. P. Alexander, D. H. Miller, K. W. Edwards, P. Rubin, D. G. Cassel, J. Insler, R. Sia, Daniel P Cronin-Hennessy, K. Randrianarivony, Sean A Dobbs, T. Klein, K. Y. Gao, I. Karliner, Juliet Ritchie Patterson, N. E. Adam, B. Sanghi, D. Riley, M. Anderson, Mats A Selen, S. Blusk, Kamal K. Seth, S. Mehrabyan, B. I. Eisenstein, J. E. Duboscq, Z. Metreveli, M. Dubrovin, Werner Sun, R. Gray, Amiran Tomaradze, R. S. Galik, E. J. White, D. M. Asner, N. Horwitz, Yuichi Kubota, M. E. Watkins, P. Naik, S. Nisar, K. M. Ecklund, R. Ehrlich, T. K. Pedlar, H. Mahlke-Krüger, T. Ferguson, S. W. Gray, J. Napolitano, A. Smith, Li Jingyuan, B. K. Heltsley, J. Kandaswamy, D. Peterson, and C. Cawlfield
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Physics ,Particle physics ,Meson ,010308 nuclear & particles physics ,Electron–positron annihilation ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,General Physics and Astronomy ,Probability density function ,01 natural sciences ,High Energy Physics - Experiment ,3. Good health ,Nuclear physics ,High Energy Physics - Experiment (hep-ex) ,0103 physical sciences ,Effective field theory ,High Energy Physics::Experiment ,Statistical analysis ,010306 general physics ,Independent data ,Flavor ,Lepton - Abstract
In this Letter we describe a search for lepton flavor violation (LFV) in the bottomonium system. We search for leptonic decays of Upsilon(nS)(n=1,2, and 3) into muon and tau using the data collected with the CLEO III detector. We identify the tau lepton using its leptonic decay into electron and utilize multidimensional likelihood fitting with PDF shapes measured from independent data samples. We report our estimates of 95% CL upper limits on LFV branching fractions of Upsilon mesons. We interpret our results in terms of the exclusion plot for the energy scale of a hypothetical new interaction versus its effective LFV coupling in the framework of effective field theory., 10 pages, 3 figures, available through http://www.lns.cornell.edu/public/CLNS/, submitted to PRL
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- 2008
42. Observation of Upsilon(2S)-->etaUpsilon(1S) and search for related transitions
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Q, He, J, Insler, H, Muramatsu, C S, Park, E H, Thorndike, F, Yang, M, Artuso, S, Blusk, S, Khalil, J, Li, R, Mountain, S, Nisar, K, Randrianarivony, N, Sultana, T, Skwarnicki, S, Stone, J C, Wang, L M, Zhang, G, Bonvicini, D, Cinabro, M, Dubrovin, A, Lincoln, P, Naik, J, Rademacker, D M, Asner, K W, Edwards, J, Reed, R A, Briere, T, Ferguson, G, Tatishvili, H, Vogel, M E, Watkins, J L, Rosner, J P, Alexander, D G, Cassel, J E, Duboscq, R, Ehrlich, L, Fields, R S, Galik, L, Gibbons, R, Gray, S W, Gray, D L, Hartill, B K, Heltsley, D, Hertz, J M, Hunt, J, Kandaswamy, D L, Kreinick, V E, Kuznetsov, J, Ledoux, H, Mahlke-Krüger, D, Mohapatra, P U E, Onyisi, J R, Patterson, D, Peterson, D, Riley, A, Ryd, A J, Sadoff, X, Shi, S, Stroiney, W M, Sun, T, Wilksen, S B, Athar, R, Patel, J, Yelton, P, Rubin, B I, Eisenstein, I, Karliner, S, Mehrabyan, N, Lowrey, M, Selen, E J, White, J, Wiss, R E, Mitchell, M R, Shepherd, D, Besson, T K, Pedlar, J V, Xavier, D, Cronin-Hennessy, K Y, Gao, J, Hietala, Y, Kubota, T, Klein, B W, Lang, R, Poling, A W, Scott, P, Zweber, S, Dobbs, Z, Metreveli, K K, Seth, A, Tomaradze, J, Libby, L, Martin, A, Powell, G, Wilkinson, K M, Ecklund, W, Love, V, Savinov, H, Mendez, J Y, Ge, D H, Miller, I P J, Shipsey, B, Xin, G S, Adams, M, Anderson, J P, Cummings, I, Danko, D, Hu, B, Moziak, and J, Napolitano
- Abstract
We report the first observation of Upsilon(2S)-->etaUpsilon(1S), with a branching fraction B=(2.1(-0.6)+0.7(stat)+/-0.3(syst)) x 10(-4) and a statistical significance 5.3sigma. Data were acquired with the CLEO III detector at the CESR e+e(-) symmetric collider. This is the first process observed involving a b-quark spin flip. For related transitions, 90% confidence limits in units of 10(-4) are B(Upsilon(2S)-->pi0Upsilon(1S)) < 1.8, B(Upsilon(3S)-->etaUpsilon(1S)) < 1.8, B(Upsilon(3S)-->pi0Upsilon(1S)) < 0.7, and B(Upsilon(3S)-->pi0Upsilon(2S)) < 5.1.
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- 2008
43. Precision Measurement of the Mass of thehc(P11)State of Charmonium
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S. Dobbs, Z. Metreveli, K. K. Seth, A. Tomaradze, J. Libby, A. Powell, G. Wilkinson, K. M. Ecklund, W. Love, V. Savinov, A. Lopez, H. Mendez, J. Ramirez, J. Y. Ge, D. H. Miller, I. P. J. Shipsey, B. Xin, G. S. Adams, M. Anderson, J. P. Cummings, I. Danko, D. Hu, B. Moziak, J. Napolitano, Q. He, J. Insler, H. Muramatsu, C. S. Park, E. H. Thorndike, F. Yang, M. Artuso, S. Blusk, S. Khalil, J. Li, R. Mountain, S. Nisar, K. Randrianarivony, N. Sultana, T. Skwarnicki, S. Stone, J. C. Wang, L. M. Zhang, G. Bonvicini, D. Cinabro, M. Dubrovin, A. Lincoln, P. Naik, J. Rademacker, D. M. Asner, K. W. Edwards, J. Reed, R. A. Briere, T. Ferguson, G. Tatishvili, H. Vogel, M. E. Watkins, J. L. Rosner, J. P. Alexander, D. G. Cassel, J. E. Duboscq, R. Ehrlich, L. Fields, R. S. Galik, L. Gibbons, R. Gray, S. W. Gray, D. L. Hartill, B. K. Heltsley, D. Hertz, J. M. Hunt, J. Kandaswamy, D. L. Kreinick, V. E. Kuznetsov, J. Ledoux, H. Mahlke-Krüger, D. Mohapatra, P. U. E. Onyisi, J. R. Patterson, D. Peterson, D. Riley, A. Ryd, A. J. Sadoff, X. Shi, S. Stroiney, W. M. Sun, T. Wilksen, S. B. Athar, R. Patel, J. Yelton, P. Rubin, B. I. Eisenstein, I. Karliner, S. Mehrabyan, N. Lowrey, M. Selen, E. J. White, J. Wiss, R. E. Mitchell, M. R. Shepherd, D. Besson, T. K. Pedlar, D. Cronin-Hennessy, K. Y. Gao, J. Hietala, Y. Kubota, T. Klein, B. W. Lang, R. Poling, A. W. Scott, and P. Zweber
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Physics ,Hadronic decay ,Particle physics ,Annihilation ,010308 nuclear & particles physics ,0103 physical sciences ,Analytical chemistry ,General Physics and Astronomy ,State (functional analysis) ,010306 general physics ,7. Clean energy ,01 natural sciences ,Gamma gamma - Abstract
A precision measurement of the mass of the h_c(1P1) state of charmonium has been made using a sample of 24.5 million psi(2S) events produced in e+e- annihilation at CESR. The reaction used was psi(2S) -> pi0 h_c, pi0 -> gamma gamma, h_c -> gamma eta_c, and the reaction products were detected in the CLEO-c detector. Data have been analyzed both for the inclusive reaction and for the exclusive reactions in which eta_c decays are reconstructed in fifteen hadronic decay channels. Consistent results are obtained in the two analyses. The averaged results of the present measurements are M(h_c)=3525.28+-0.19 (stat)+-0.12(syst) MeV, and B(psi(2S) -> pi0 h_c)xB(h_c -> gamma eta_c)= (4.19+-0.32+-0.45)x10^-4. Using the 3PJ centroid mass, Delta M_hf(1P)= - M(h_c) = +0.02+-0.19+-0.13 MeV.
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- 2008
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44. Search for Very LightCP-Odd Higgs Boson in Radiative Decays ofΥ(1S)
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D. Riley, N. Lowrey, D. Cinabro, G. Tatishvili, M. Dubrovin, P. Zweber, B. Xin, K. W. Edwards, S. Stroiney, F. Yang, I. Danko, Juliet Ritchie Patterson, Kamal K. Seth, A. Powell, R. Gray, J. P. Cummings, J. Ledoux, R. Mountain, H. Muramatsu, Jonathan L. Rosner, Tomasz Skwarnicki, Yuichi Kubota, K. Y. Gao, Daniel P Cronin-Hennessy, Sean A Dobbs, D. Z. Besson, I. P.J. Shipsey, Amiran Tomaradze, J. Y. Ge, E. J. White, Jonas Rademacker, James E Wiss, Hans J. Vogel, D. G. Cassel, S. Blusk, Anders Ryd, John Yelton, J. Hietala, M. R. Shepherd, D. Hu, J. E. Duboscq, J. M. Hunt, R. E. Mitchell, L. K. Gibbons, R. Patel, D. Hertz, I. Karliner, Sheldon Stone, Thomas Ferguson, B. Moziak, B. W. Lang, J. Kandaswamy, D. H. Miller, Peter Onyisi, J. Reed, B. I. Eisenstein, D. L. Hartill, D. Mohapatra, A. W. Scott, D. M. Asner, W. Love, R. Poling, S. W. Gray, Q. He, C. S. Park, N. Sultana, Marina Artuso, J. Libby, R. A. Briere, G. Wilkinson, L. Fields, K. Randrianarivony, D. Peterson, H. Mendez, S. B. Athar, J. C. Wang, A. Lincoln, M. Anderson, J. Insler, S. Mehrabyan, G. S. Adams, L. Martin, M. E. Watkins, Mats A Selen, Werner Sun, Lei Zhang, S. Nisar, V. E. Kuznetsov, T. Klein, D. L. Kreinick, A. J. Sadoff, T. Wilksen, X. Shi, V. Savinov, Li Jingyuan, B. K. Heltsley, E. H. Thorndike, S. Khalil, G. Bonvicini, J. P. Alexander, R. S. Galik, P. Rubin, Z. Metreveli, R. Ehrlich, T. K. Pedlar, H. Mahlke-Krüger, K. M. Ecklund, J. Napolitano, and P. Naik
- Subjects
Physics ,Particle physics ,010308 nuclear & particles physics ,Branching fraction ,Electron–positron annihilation ,Radiative decay ,General Physics and Astronomy ,Sigma ,Supersymmetry ,01 natural sciences ,Nuclear physics ,Pair production ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,Higgs boson ,Radiative transfer ,High Energy Physics::Experiment ,010306 general physics - Abstract
We search for a non-SM-like CP-odd Higgs boson (a{sub 1}{sup 0}) decaying to {tau}{sup +}{tau}{sup -} or {mu}{sup +}{mu}{sup -} in radiative decays of the {upsilon}(1S). No significant signal is found, and upper limits on the product branching ratios are set. Our {tau}{sup +}{tau}{sup -} results are almost 2 orders of magnitude more stringent than previous upper limits. Our data provide no evidence for a Higgs state with a mass of 214 MeV decaying to {mu}{sup +}{mu}{sup -}, previously proposed as an explanation for 3 {sigma}{sup +}{yields}p{mu}{sup +}{mu}{sup -} events observed by the HyperCP experiment. Our results constrain NMSSM models.
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- 2008
- Full Text
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45. Search forCPviolation in the Dalitz-plot analysis ofD±→K+K−π±
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C. S. Park, L. Fields, E. H. Thorndike, S. Khalil, G. Bonvicini, J. P. Alexander, I. P.J. Shipsey, Jonas Rademacker, L. K. Gibbons, R. Patel, D. Hertz, J. Ledoux, S. Mehrabyan, G. Tatishvili, K. W. Edwards, J. Y. Ge, Daniel P Cronin-Hennessy, Sean A Dobbs, J. M. Hunt, G. S. Adams, James E Wiss, J. Libby, K. Randrianarivony, E. J. White, L. Martin, S. Blusk, P. Naik, W. Love, J. C. Wang, R. E. Mitchell, N. Lowrey, T. K. Pedlar, D. Cinabro, Juliet Ritchie Patterson, A. Lincoln, F. Yang, J. E. Duboscq, Kamal K. Seth, A. Powell, D. Z. Besson, S. Stroiney, Jonathan L. Rosner, Tomasz Skwarnicki, J. Insler, H. Muramatsu, P. Zweber, D. M. Asner, B. W. Lang, D. H. Miller, B. Xin, R. Mountain, D. Mohapatra, B. Moziak, D. G. Cassel, Anders Ryd, J. Kandaswamy, M. R. Shepherd, I. Karliner, N. Sultana, B. I. Eisenstein, D. Peterson, Marina Artuso, Peter Onyisi, A. W. Scott, S. W. Gray, R. Poling, Q. He, R. A. Briere, K. Y. Gao, D. Riley, M. Dubrovin, Yuichi Kubota, H. Mendez, S. B. Athar, G. Wilkinson, Sheldon Stone, Hans J. Vogel, V. E. Kuznetsov, T. Klein, Werner Sun, Lei Zhang, S. Nisar, B. K. Heltsley, D. L. Kreinick, A. J. Sadoff, T. Wilksen, X. Shi, V. Savinov, Li Jingyuan, R. Ehrlich, J. Reed, H. Mahlke-Krüger, D. Hu, D. L. Hartill, R. Gray, Amiran Tomaradze, Z. Metreveli, B. J.Y. Tan, J. Napolitano, Mats A Selen, John Yelton, J. Hietala, P. Rubin, and K. M. Ecklund
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,media_common.quotation_subject ,Resonance ,Dalitz plot ,Two-body problem ,01 natural sciences ,Asymmetry ,Particle identification ,Particle decay ,0103 physical sciences ,CP violation ,Intermediate state ,010306 general physics ,media_common - Abstract
We report on a search for $CP$ asymmetry in the singly Cabibbo-suppressed decay ${D}^{+}\ensuremath{\rightarrow}{K}^{+}{K}^{\ensuremath{-}}{\ensuremath{\pi}}^{+}$ using a data sample of $818\text{ }\text{ }{\mathrm{pb}}^{\ensuremath{-}1}$ accumulated with the CLEO-c detector on the $\ensuremath{\psi}(3770)$ resonance. A Dalitz-plot analysis is used to determine the amplitudes of the intermediate states. We find no evidence for $CP$ violation either in specific two-body amplitudes or integrated over the entire phase space. The $CP$ asymmetry in the latter case is measured to be $(\ensuremath{-}0.03\ifmmode\pm\else\textpm\fi{}0.84\ifmmode\pm\else\textpm\fi{}0.29)%$.
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- 2008
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46. Observation ofχcJRadiative Decays to Light Vector Mesons
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W. Love, G. Tatishvili, N. Lowrey, J. Yelton, M. Selen, J. V. Bennett, Ron Poling, B. I. Eisenstein, S. Blusk, S. Stroiney, L. K. Gibbons, A. Powell, Jonathan L. Rosner, R. Patel, D. Hertz, J. R. Patterson, T. K. Pedlar, P. U.E. Onyisi, B. J.Y. Tan, J. Napolitano, R. Ehrlich, K. W. Edwards, J. Libby, Y. Kubota, P. Rubin, R. A. Briere, J. Insler, V. Savinov, Z. Metreveli, Kamal K. Seth, K. Randrianarivony, H. Mendez, S. B. Athar, A. Ryd, B. Moziak, A. W. Scott, Q. He, H. Mahlke-Krüger, S. Khalil, J. Hietala, F. Yang, W. M. Sun, S. W. Gray, P. Zweber, D. M. Asner, K. M. Ecklund, G. Bonvicini, D. G. Cassel, M. R. Shepherd, I. Karliner, H. Vogel, A. J. Sadoff, T. Wilksen, B. Xin, R. Gray, X. Shi, R. S. Galik, T. Skwarnicki, J. Y. Ge, James E Wiss, K. Y. Gao, R. E. Mitchell, Amiran Tomaradze, Li Jingyuan, Brian Heltsley, J. E. Duboscq, B. W. Lang, J. M. Hunt, C. S. Park, J. Reed, L. Fields, D. Peterson, J. Ledoux, R. Mountain, E. H. Thorndike, E. J. White, D. Hu, D. L. Kreinick, H. Muramatsu, S. Mehrabyan, P. Naik, D. Riley, Daniel P Cronin-Hennessy, Sean A Dobbs, M. Dubrovin, J. Rademacker, J. P. Alexander, G. S. Adams, L. Martin, D. H. Miller, J. Kandaswamy, N. Sultana, D. Besson, S. Nisar, Sheldon Stone, L. M. Zhang, D. Mohapatra, V. E. Kuznetsov, Marina Artuso, T. Klein, G. Wilkinson, D. Cinabro, I. P.J. Shipsey, J. C. Wang, D. L. Hartill, and A. Lincoln
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Physics ,Meson ,Branching fraction ,Astrophysics::High Energy Astrophysical Phenomena ,Electron–positron annihilation ,Radiative decay ,FOS: Physical sciences ,General Physics and Astronomy ,Omega baryon ,Omega ,Particle identification ,High Energy Physics - Experiment ,Nuclear physics ,High Energy Physics - Experiment (hep-ex) ,Radiative transfer ,High Energy Physics::Experiment - Abstract
Using a total of 2.74 x 10^7 decays of the psi(2S) collected with the CLEO-c detector, we present a study of chi_cJ -> gamma V, where V = rho^0, omega, phi. The transitions chi_c1 -> gamma rho^0 and chi_c1 -> gamma omega are observed with B(chi_c1 -> gamma rho^0) = (2.43 +- 0.19 +- 0.22) x 10^-4 and B(chi_c1 -> gamma omega) = (8.3 +- 1.5 +- 1.2) x 10^-5. In the chi_c1 -> gamma rho^0 transition, the final state meson is dominantly longitudinally polarized. Upper limits on the branching fractions of other chi_cJ states to light vector mesons are presented., 10 pages, available through http://www.lns.cornell.edu/public/CLNS/
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- 2008
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47. Precision measurement of the mass of the hc(1P1) state of charmonium
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S, Dobbs, Z, Metreveli, K K, Seth, A, Tomaradze, J, Libby, A, Powell, G, Wilkinson, K M, Ecklund, W, Love, V, Savinov, A, Lopez, H, Mendez, J, Ramirez, J Y, Ge, D H, Miller, I P J, Shipsey, B, Xin, G S, Adams, M, Anderson, J P, Cummings, I, Danko, D, Hu, B, Moziak, J, Napolitano, Q, He, J, Insler, H, Muramatsu, C S, Park, E H, Thorndike, F, Yang, M, Artuso, S, Blusk, S, Khalil, J, Li, R, Mountain, S, Nisar, K, Randrianarivony, N, Sultana, T, Skwarnicki, S, Stone, J C, Wang, L M, Zhang, G, Bonvicini, D, Cinabro, M, Dubrovin, A, Lincoln, P, Naik, J, Rademacker, D M, Asner, K W, Edwards, J, Reed, R A, Briere, T, Ferguson, G, Tatishvili, H, Vogel, M E, Watkins, J L, Rosner, J P, Alexander, D G, Cassel, J E, Duboscq, R, Ehrlich, L, Fields, R S, Galik, L, Gibbons, R, Gray, S W, Gray, D L, Hartill, B K, Heltsley, D, Hertz, J M, Hunt, J, Kandaswamy, D L, Kreinick, V E, Kuznetsov, J, Ledoux, H, Mahlke-Krüger, D, Mohapatra, P U E, Onyisi, J R, Patterson, D, Peterson, D, Riley, A, Ryd, A J, Sadoff, X, Shi, S, Stroiney, W M, Sun, T, Wilksen, S B, Athar, R, Patel, J, Yelton, P, Rubin, B I, Eisenstein, I, Karliner, S, Mehrabyan, N, Lowrey, M, Selen, E J, White, J, Wiss, R E, Mitchell, M R, Shepherd, D, Besson, T K, Pedlar, D, Cronin-Hennessy, K Y, Gao, J, Hietala, Y, Kubota, T, Klein, B W, Lang, R, Poling, A W, Scott, and P, Zweber
- Abstract
A precision measurement of the mass of the h_{c}(1P1) state of charmonium has been made using a sample of 24.5x10;{6} psi(2S) events produced in e;{+}e;{-} annihilation at the Cornell Electron Storage Ring (CESR). The reaction used was psi(2S)-->pi;{0}h_{c}, pi;{0}-->gammagamma, h_{c}-->gammaeta_{c}, and the reaction products were detected in the CLEO-c detector. Data have been analyzed both for the inclusive reaction and for the exclusive reactions in which eta_{c} decays are reconstructed in 15 hadronic decay channels. Consistent results are obtained in the two analyses. The averaged results of the present measurements are M(h_{c})=3525.28+/-0.19(stat.)+/-0.12(syst.) MeV, and B(psi(2S)-->pi;{0}h_{c})xB(h_{c}-->gammaeta_{c})=(4.19+/-0.32+/-0.45)x10;{-4}. Using the ;{3}P_{J} centroid mass, DeltaM_{hf}(1P) identical withM(chi_{cJ})-M(h_{c})=+0.02+/-0.19+/-0.13 MeV.
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- 2008
48. Measurement of the eta'-meson mass using J/psi-->gammaeta'
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J, Libby, L, Martin, A, Powell, G, Wilkinson, K M, Ecklund, W, Love, V, Savinov, H, Mendez, J Y, Ge, D H, Miller, I P J, Shipsey, B, Xin, G S, Adams, M, Anderson, J P, Cummings, I, Danko, D, Hu, B, Moziak, J, Napolitano, Q, He, J, Insler, H, Muramatsu, C S, Park, E H, Thorndike, F, Yang, M, Artuso, S, Blusk, S, Khalil, J, Li, R, Mountain, S, Nisar, K, Randrianarivony, N, Sultana, T, Skwarnicki, S, Stone, J C, Wang, L M, Zhang, G, Bonvicini, D, Cinabro, M, Dubrovin, A, Lincoln, P, Naik, J, Rademacker, D M, Asner, K W, Edwards, J, Reed, R A, Briere, T, Ferguson, G, Tatishvili, H, Vogel, M E, Watkins, J L, Rosner, J P, Alexander, D G, Cassel, J E, Duboscq, R, Ehrlich, L, Fields, R S, Galik, L, Gibbons, R, Gray, S W, Gray, D L, Hartill, B K, Heltsley, D, Hertz, J M, Hunt, J, Kandaswamy, D L, Kreinick, V E, Kuznetsov, J, Ledoux, H, Mahlke-Krüger, D, Mohapatra, P U E, Onyisi, J R, Patterson, D, Peterson, D, Riley, A, Ryd, A J, Sadoff, X, Shi, S, Stroiney, W M, Sun, T, Wilksen, S B, Athar, R, Patel, J, Yelton, P, Rubin, B I, Eisenstein, I, Karliner, S, Mehrabyan, N, Lowrey, M, Selen, E J, White, J, Wiss, R E, Mitchell, M R, Shepherd, D, Besson, T K, Pedlar, D, Cronin-Hennessy, K Y, Gao, J, Hietala, Y, Kubota, T, Klein, B W, Lang, R, Poling, A W, Scott, P, Zweber, S, Dobbs, Z, Metreveli, K K, Seth, and A, Tomaradze
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High Energy Physics::Experiment ,Nuclear Experiment - Abstract
We measure the mass of the eta;{'} meson using psi(2S)-->pi;{+}pi;{-}J/psi, J/psi-->gammaeta;{'} events acquired with the CLEO-c detector operating at the CESR e;{+}e;{-} collider. Using three decay modes, eta;{'}-->rho;{0}gamma, eta;{'}-->pi;{+}pi;{-}eta with eta-->gammagamma, and eta;{'}-->pi;{+}pi;{-}eta with eta-->pi;{+}pi;{-}pi;{0}, we find M_{eta;{'}}=957.793+/-0.054+/-0.036 MeV, in which the uncertainties are statistical and systematic, respectively. This result is consistent with but substantially more precise than the current world average.
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- 2008
49. Precision measurement ofB(D+→μ+ν)and the pseudoscalar decay constantfD+
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Werner Sun, G. Tatishvili, Lei Zhang, G. S. Adams, Anders Ryd, L. Martin, J. Libby, M. R. Shepherd, S. Nisar, J. P. Cummings, K. Randrianarivony, M. Anderson, B. W. Lang, B. Xin, D. H. Miller, D. Z. Besson, K. Y. Gao, Z. Metreveli, V. E. Kuznetsov, N. Lowrey, Peter Onyisi, D. Cinabro, J. C. Wang, Jonas Rademacker, P. Zweber, A. W. Scott, A. Lincoln, R. Poling, D. Mohapatra, T. Klein, S. Stroiney, Sheldon Stone, L. K. Gibbons, Hans J. Vogel, Q. He, Jonathan L. Rosner, Tomasz Skwarnicki, G. Wilkinson, R. Patel, D. Hertz, Daniel P Cronin-Hennessy, Marina Artuso, J. M. Hunt, J. Insler, Sean A Dobbs, K. W. Edwards, R. Mountain, H. Muramatsu, S. Blusk, B. Moziak, B. K. Heltsley, S. Mehrabyan, J. E. Duboscq, D. L. Kreinick, C. S. Park, A. J. Sadoff, T. Wilksen, L. Fields, W. Love, M. E. Watkins, Thomas Ferguson, J. Y. Ge, X. Shi, James E Wiss, R. Ehrlich, D. M. Asner, F. Yang, I. Danko, V. Savinov, D. Riley, H. Mahlke-Krüger, R. E. Mitchell, Li Jingyuan, J. Napolitano, M. Dubrovin, Juliet Ritchie Patterson, P. Rubin, I. P.J. Shipsey, D. G. Cassel, K. M. Ecklund, Yuichi Kubota, J. Kandaswamy, Kamal K. Seth, A. Powell, N. Sultana, I. Karliner, D. Peterson, B. I. Eisenstein, Mats A Selen, T. K. Pedlar, J. Reed, H. Mendez, S. B. Athar, E. H. Thorndike, S. Khalil, G. Bonvicini, J. P. Alexander, D. Hu, John Yelton, J. Hietala, R. S. Galik, D. L. Hartill, N. Menaa, R. Gray, Amiran Tomaradze, P. Naik, S. W. Gray, R. A. Briere, J. Ledoux, and E. J. White
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Muon ,Meson ,010308 nuclear & particles physics ,Branching fraction ,Electron–positron annihilation ,Resonance ,7. Clean energy ,01 natural sciences ,Particle identification ,Crystallography ,TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY ,0103 physical sciences ,CP violation ,Exponential decay ,010306 general physics - Abstract
We measure the branching ratio of the purely leptonic decay of the D{sup +} meson with unprecedented precision as B(D{sup +}{yields}{mu}{sup +}{nu})=(3.82{+-}0.32{+-}0.09)x10{sup -4}, using 818 pb{sup -1} of data taken on the {psi}(3770) resonance with the CLEO-c detector at the CESR collider. We use this determination to derive a value for the pseudoscalar decay constant f{sub D{sup +}}, combining with measurements of the D{sup +} lifetime and assuming |V{sub cd}|=|V{sub us}|. We find f{sub D{sup +}}=(205.8{+-}8.5{+-}2.5) MeV. The decay rate asymmetry ({gamma}(D{sup +}{yields}{mu}{sup +}{nu})-{gamma}(D{sup -}{yields}{mu}{sup -}{nu})/{gamma}(D{sup +}{yields}{mu}{sup +}{nu})+{gamma}(D{sup -}{yields}{mu}{sup -}{nu}))=0.08{+-}0.08, consistent with no CP violation. We also set 90% confidence level upper limits on B(D{sup +}{yields}{tau}{sup +}{nu})
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- 2008
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50. Dalitz plot analysis of theD+→K−π+π+decay
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J. E. Ramirez, V. E. Kuznetsov, Thomas Ferguson, Jonas Rademacker, J. Kandaswamy, Peter Onyisi, B. Xin, T. Klein, Kamal K. Seth, A. Powell, N. Sultana, R. Poling, D. Mohapatra, Marina Artuso, S. Blusk, Q. He, D. Peterson, K. Y. Gao, Sheldon Stone, D. G. Cassel, J. Ledoux, J. E. Duboscq, G. Tatishvili, N. Lowrey, Werner Sun, D. Cinabro, Mats A Selen, S. Stroiney, E. H. Thorndike, Jonathan L. Rosner, Tomasz Skwarnicki, I. P.J. Shipsey, Lei Zhang, S. Mehrabyan, J. M. Hunt, I. Karliner, S. Khalil, J. P. Cummings, E. J. White, J. Y. Ge, D. Riley, G. Bonvicini, J. P. Alexander, James E Wiss, S. Nisar, M. Dubrovin, J. Libby, D. Z. Besson, B. I. Eisenstein, P. Zweber, D. M. Asner, G. Wilkinson, K. Randrianarivony, R. E. Mitchell, B. Moziak, R. Mountain, John Yelton, J. Hietala, M. Anderson, Yuichi Kubota, Juliet Ritchie Patterson, L. K. Gibbons, W. Love, D. L. Hartill, R. Patel, C. S. Park, B. W. Lang, D. H. Miller, D. Hertz, J. Insler, M. E. Watkins, T. K. Pedlar, R. Gray, J. C. Wang, A. Lincoln, L. Fields, S. W. Gray, Amiran Tomaradze, F. Yang, I. Danko, R. A. Briere, G. S. Adams, Daniel P Cronin-Hennessy, Sean A Dobbs, A. W. Scott, J. Reed, K. W. Edwards, D. Hu, H. Mendez, S. B. Athar, Alan D. Lopez, Hans J. Vogel, H. Muramatsu, Anders Ryd, M. R. Shepherd, D. L. Kreinick, A. J. Sadoff, T. Wilksen, R. Ehrlich, X. Shi, V. Savinov, H. Mahlke-Krüger, Li Jingyuan, B. K. Heltsley, Z. Metreveli, P. Rubin, K. M. Ecklund, J. Napolitano, and P. Naik
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Electron–positron annihilation ,Partial wave analysis ,Dalitz plot ,Resonance ,01 natural sciences ,Particle identification ,Particle decay ,Isospin ,0103 physical sciences ,Isobar ,010306 general physics - Abstract
We perform a Dalitz plot analysis of D{sup +}{yields}K{sup -}{pi}{sup +}{pi}{sup +} decay with the CLEO-c data set of 572 pb{sup -1} of e{sup +}e{sup -} collisions accumulated at the {psi}(3770). This corresponds to 1.6x10{sup 6} D{sup +}D{sup -} pairs from which we select 140 793 candidate events with a small background of 1.1%. We compare our results with previous measurements using the isobar model. We modify the isobar model with an improved description of some of the contributing resonances and get better agreement with our data. We also consider a quasi-model-independent approach and measure the magnitude and phase of the contributing K{pi} S wave in the range of invariant masses from the threshold to the maximum in this decay. This gives an improved description of our data over the isobar model. Finally we allow for an isospin-two {pi}{sup +}{pi}{sup +} S wave contribution and find that adding this to both the isobar model and the quasi-model-independent approach gives the best description of our data.
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- 2008
- Full Text
- View/download PDF
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