Study of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="italic">Υ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>3</mml:mn><mml:mi>S</mml:mi><mml:mo>,</mml:mo><mml:mn>2</mml:mn><mml:mi>S</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>→</mml:mo><mml:mi>η</mml:mi><mml:mi mathvariant="italic">Υ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mi>S</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math>and<mml:math xmlns:mml="http://www.w3.

Lees, J. P.; Poireau, V.; Tisserand, V.; Tico, J. Garra; Graugés, E.; Martinelli, M.; Milanés, D. A.; Palano, A.; Pappagallo, M.; Eigen, G.; Stugu, B.; Brown, D. N.; Kerth, L. T.; Kolomensky, Yu. G.; Lynch, G.; Koch, H.; Schroeder, T. Vazquez; Asgeirsson, D. J.; Hearty, C.; Mattison, T. S.; McKenna, J. A.; Khan, A.; Blinov, V.; Бузыкаев, А. Р.; Дружинин, В. П.; Голубев, В. Б.; Kravchenko, E. A.; Onuchin, A. P.; Serednyakov, S. I.; Skovpen, Yu. I.; Solodov, E. P.; Todyshev, K. Yu; Yushkov, A. N.; Bondioli, M.; Kirkby, D.; Lankford, A. J.; Mandelkern, M.; Stoker, D. P.; Atmacan, H.; Gary, J. W.; Liu, F.; Long, O. R.; Vitug, G. M.; Campagnari, C.; Hong, T. M.; Kovalskyi, D.; Richman, J.; West, C.; Eisner, A. M.; Kroseberg, J.; Lockman, W. S.; Martínez, A. J.; Schalk, T.; Schumm, B. A.; Seiden, A.; Cheng, C. H.; Doll, D. A.; Echenard, B.; Flood, K. T.; Hitlin, D. G.; Ongmongkolkul, P.; Porter, F. C.; Rakitin, A. Y.; Andreassen, R.; Dubrovin, M.; Huard, Z.; Meadows, B.; Sokoloff, M. D.; Sun, Liang; Bloom, P. C.; Ford, W. T.; Gaz, A.; Nagel, M.; Nauenberg, U.; Smith, J. G.; Wagner, S. R.; Ayad, R.; Toki, W. H.; Spaan, B.; Kobel, M.; Schubert, K. R.; Schwierz, R.; Bernard, D.; Verderi, M.; Clark, P. J.; Playfer, S.; Bettoni, D.; Bozzi, C.; Calabrese, R.; Cibinetto, G.; Fioravanti, E.; Garzia, I.; Luppi, E.; Munerato, M.; Negrini, M.; Piemontese, L.; Santoro, V.; Baldini-Ferroli, R.; Calcaterra, A.; Sangro, R. de; Finocchiaro, G.; Nicolaci, M.; Patterí, P.; Peruzzi, I. M.; Piccolo, M.; Rama, M.; Zallo, A.; Contri, R.; Guido, E.; Vetere, M. Lo; Monge, M. R.; Passaggio, S.; Patrignani, C.; Robutti, E.; Bhuyan, B.; Prasad, V.; Lee, C. L.; Morii, M.; Edwards, A. J.; Adametz, A.; Marks, J.; Uwer, U.; Bernlochner, F. U.; Ebert, M.; Lacker, H.; Lueck, T.; Dauncey, P.; Tibbetts, M. J.; Behera, P. K.; Mallik, U.; Chen, C.; Cochran, J.; Meyer, W. T.; Prell, S.; Rosenberg, E. I.; Rubin, A. E.; Gritsan, A. V.; Guo, Z.; Arnaud, N.; Davier, M.; Grosdidier, G.; Diberder, F. Le; Lutz, A. M.; Malaescu, B.; Roudeau, P.; Schune, M. H.; Stocchi, A.; Wormser, G.; Lange, D. J.; Wright, D.; Bingham, I.; Chavez, C. A.; Coleman, J. P.; Fry, J. R.; Gabathuler, E.; Hutchcroft, D.; Payne, D. J.; Touramanis, C.; Bevan, A. J.; Lodovico, F. Di; Sacco, R.; Sigamani, M.; Cowan, G.; Davis, C. L.; Denig, A.; Fritsch, M.; Gradl, W.; Hafner, A.; Prencipe, E.; Alwyn, K. E.; Bailey, D.; Barlow, R. J.; Jackson, G.; Lafferty, G. D.; Behn, E.; Cenci, R.; Hamilton, B.; Jawahery, A.; Roberts, D. A.; Simi, G.; Dallapiccola, C.; Cowan, R.; Dujmić, D.; Sciolla, G.; Lindemann, D.; Patel, P. M.; Robertson, S. H.; Schram, M.; Biassoni, P.; Lazzaro, A.; Lombardo, V.; Neri, N.; Palombo, F.; Stracka, S.; Cremaldi, L.; Godang, R.; Kroeger, R.; Sonnek, P.; Summers, D. J.; Nguyen, X.; Taras, P.; Nardo, G. De; Monorchio, D.; Onorato, G.; Sciacca, C.; Raven, G.; Snoek, H. L.; Jessop, C.; Knoepfel, K. J.; LoSecco, J. M.; Wang, W. F.; Honscheid, K.; Kass, R.; Brau, J.; Frey, R.; Sinev, N. B.; Strom, D.; Torrence, E.; Feltresi, E.; Gagliardi, N.; Margoni, M.; Morandin, M.; Posocco, M.; Rotondo, M.; Simonetto, F.; Stroili, R.; Akar, S.; Ben-Haim, E.; Bomben, M.; Bonneaud, G. R.; Briand, H.; Calderini, G.; Chauveau, J.; Hamon, O.; Leruste, Ph; Marchiori, G.; Ocariz, J.; Sitt, S.; Biasini, M.; Manoni, E.; Pacetti, S.; Rossi, A.; Angelini, C.; Batignani, G.; Bettarini, S.; Carpinelli, M.; Casarosa, G.; Cervelli, A.; Forti, F.; Giorgi, M. A.; Lusiani, A.; Oberhof, B.; Paoloni, E.; Pérez, A.; Rizzo, G.; Walsh, J.; Pegna, D. Lopes; Lu, Chih-Ting; Olsen, J.; Smith, A. J. S.; Telnov, A. V.; Anulli, F.; Cavoto, G.; Faccini, R.; Ferrarotto, F.; Ferroni, F.; Gaspero, M.; Gioi, L. Li; Mazzoni, M. A.; Piredda, G.; Bünger, C.; Grünberg, O.; Hartmann, T.; Leddig, T.; Schröder, H.; Waldi, R.; Adye, T.; Olaiya, E.; Wilson, F. F.; Emery, S.; Monchenault, G. Hamel de; Vasseur, G.; Yèche, Ch; Aston, D.; Bard, D. J.; Bartoldus, R.; Cartaro, C.; Convery, M. R.; Dorfan, J.; Dubois-Felsmann, G. P.; Dunwoodie, W.; Field, R. C.; Sevilla, M. Franco; Fulsom, B. G.; Gabareen, A. M.; Graham, M. T.; Grenier, P.; Hast, C.; Innes, W. R.; Kelsey, M.; Kim, H.; Kim, P.; Kocian, M. L.; Leith, D. W. G. S.; Lewis, P.; Li, S.; Lindquist, B.; Luitz, S.; Lüth, V.; Lynch, H. L.; MacFarlane, D. B.; Müller, D.; Neal, H. A.; Nelson, S.; Ofte, I.; Perl, M.; Pulliam, T.; Ratcliff, B. N.; Roodman, A.; Salnikov, A.; Schindler, R. H.; Snyder, A.; Su, D.; Sullivan, M. K.; Va’vra, J.; Wagner, A.; Weaver, M.; Wisniewski, W. J.; Wittgen, M.; Wright, D. H.; Wulsin, H. W.; Yarritu, A. K.; Young, C.; Ziegler, V.; Park, W.; Purohit, M.; White, R. M.; Wilson, J. R.; Randle-Conde, A.; Sekula, S. J.; Bellis, M.; Benitez, J. F.; Burchat, P. R.; Miyashita, T. S.; Alam, M. S.; Ernst, J.; Gorodeisky, R.; Guttman, N.; Peimer, D. R.; Soffer, A.; Lund, P.; Spanier, S.; Eckmann, R.; Ritchie, J. L.; Ruland, A. M.; Schilling, C. J.; Schwitters, R. F.; Wray, B. C.; Izen, J. M.; Lou, X.; Bianchi, F.; Gamba, D.; Lanceri, L.; Vitale, L.; Martínez-Vidal, F.; Oyanguren, A.; Ahmed, H.; Albert, J.; Banerjee, S.; Choi, H. H. F.; King, G. J.; Kowalewski, R.; Lewczuk, M. J.; Nugent, I. M.; Roney, J. M.; Sobie, R. J.; Tasneem, N.; Gershon, T.; Harrison, P. F.; Latham, T.; Puccio, E. M. T.; Band, H. R.; Dasu, S.; Pan, Y.; Prepost, R.; Wu, S. L.

doi:10.1103/physrevd.84.092003

Cited by 15 publications

(2 citation statements)

References 17 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…Therefore the ratios between the η and ππ transitions among Υ(3S ), Υ(2S ) and Υ(1S ), R . This QCDME prediction meets, at least qualitatively the experimental measurements in the sector of narrow bottomonia, indicating that the HQSS is indeed a good symmetry: R 2S →1S η,ππ = (1.6 ± 0.2) × 10 −3 [20,21,22] and R 3S →1S η,ππ < 2.1 × 10 −3 [21]. At the Υ(4S ) energy however the situation is completely reversed.…”

Section: New Hadronic Transitionssupporting

confidence: 78%

Bottomonium physics above BB¯ thresholds with the Belle experiment

Tamponi

2016

AIP Conference Proceedings

View full text Add to dashboard Cite

Abstract. The structure of heavy mesons located above the thresholds for the open flavor production has been largely discussed in the recent years. Their conventional description as pure BB bound state has been called into question by the study of the hadronic transitions to the lower states, and the observation of charged exotic states has highlighted the importance of the light quark degrees of freedom in the description of both charmonia and bottomonia. We will report the most recent experimental measurements performed by the Belle collaboration in the Y(4S), Y(5S) and Y(6S) regions, including the measurement of the ratio, the search for neutral states near the B 0B0 threshold, the first observation of the transition Υ(4S ) → ηh b (1P) and the study of the η transitions at the Υ(5S ) energy. The contribution to the study of the structure of these states coming from the measurement of hadronic transitions will be discussed.

show abstract

Section: New Hadronic Transitionssupporting

confidence: 78%

Bottomonium physics above BB¯ thresholds with the Belle experiment

Tamponi

2016

AIP Conference Proceedings

View full text Add to dashboard Cite

show abstract

“…where hm recoil i is the expected location of the Çð1SÞ peak, determined by the mass difference between the Çð2SÞ and Çð1SÞ mesons [21]. The final signal selection efficiency varies between 1% and 4.5% (Fig.…”

mentioning

confidence: 99%

Search for a low-mass scalar Higgs boson decaying to a tau pair in single-photon decays ofΥ(1S)

Lees¹,

Poireau²,

Tisserand³

et al. 2013

Phys. Rev. D

Self Cite

View full text Add to dashboard Cite

We search for a low-mass scalar CP-odd Higgs boson, A 0 , produced in the radiative decay of the Upsilon resonance and decaying into a τ + τ − pair: Υ (1S) → γA 0 . The production of Υ (1S) mesons is tagged by Υ (2S) → π + π − Υ (1S) transitions, using a sample of (98.3 ± 0.9) × 10 6 Υ (2S) mesons collected by the BABAR detector. We find no evidence for a Higgs boson in the mass range 3.5 GeV ≤ m A 0 ≤ 9.2 GeV, and combine these results with our previous search for the tau decays of the light Higgs in radiative Υ (3S) decays, setting limits on the coupling of A 0 to the b b quarks in the range 0.09 − 1.9. Our measurements improve the constraints on the parameters of the Nextto-Minimal-Supersymmetric Standard Model and similar theories with low-mass scalar degrees of freedom.

show abstract