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The production rate of bottom quarks at hadron colliders exceeds the expectations of next-to-leading order perturbative quantum chromodynamics. An additional contribution from pair-production of light gluinos, of mass 12 to 16 GeV, with…

High Energy Physics - Phenomenology · Physics 2014-11-17 Edmond L. Berger

A new contribution from pair-production of light gluinos, of mass 12 to 16 GeV, with two-body decays into bottom quarks and light bottom squarks, helps to obtain a bottom-quark production rate in better agreement with hadron collider data.…

High Energy Physics - Phenomenology · Physics 2016-11-23 Edmond L. Berger

A long-standing discrepancy between the bottom-quark production cross section and predictions of perturbative quantum chromodynamics is addressed. We show that pair production of light gluinos, of mass 12 to 16 GeV, with two-body decays…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. L. Berger , B. W. Harris , D. E. Kaplan , Z. Sullivan , T. M. P. Tait , C. E. M. Wagner

In this talk, I describe a supersymmetric solution to the long-standing discrepancy between the bottom-quark production cross section and predictions of perturbative quantum chromodynamics. Pair production of light gluinos, of mass 12-16…

High Energy Physics - Phenomenology · Physics 2007-05-23 Z. Sullivan

Agreement of theoretical calculations with the observed production rate of bottom quarks at hadron colliders is improved by the introduction of a contribution from pair-production of light gluinos, of mass 12 to 16 GeV, having two-body…

High Energy Physics - Phenomenology · Physics 2009-11-07 Edmond L Berger

At hadron colliders, one of the most important channels for sparticle production is expected to be the gluino pair production. In the scenario where the sbottom is lighter than the gluino, gluinos can decay into sbottom and bottom quarks.…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. Mahmoudi , A. Deandrea

Light bottom squarks and gluinos have been invoked to explain the b quark pair production excess at the Tevatron. We investigate the associated production of ttbb at hadron colliders in this scenario, and find that the rates for this…

High Energy Physics - Phenomenology · Physics 2014-11-17 Adam K. Leibovich , David Rainwater

The minimal supersymmetric model with light sbottom ($\sim m_b$) and light gluino (12 $\sim$ 16 GeV) can explain the excess of bottom quark production cross section at hadron colliders and has drawn much attention. We calculate one-loop…

High Energy Physics - Phenomenology · Physics 2008-11-26 Seungwon Baek

We report on a search for the supersymmetric partner of the bottom quark produced from gluino decays in data from 2.5 fb-1 of integrated luminosity collected by the Collider Detector at Fermilab at sqrt(s)=1.96 TeV. Candidate events are…

High Energy Physics - Experiment · Physics 2009-08-26 CDF Collaboration , T. Aaltonen

The cross section of top pair production in hadronic collisions to O(alpha \alpha_s^2) is calculated within the General 2-Higgs-Doublet Model and the Minimal Supersymmetric Standard Model. At the parton level the O(alpha) one-loop…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Hollik , W. M. Moesle , D. Wackeroth

The production and decay of supersymmetric particles is presented. The dependence of the hadro-production cross section for weakly and strongly interacting yields an improvement of derived mass bounds or the measurement of the masses,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tilman Plehn

The scalar partners of top and bottom quarks are expected to be the lightest squarks in supersymmetric theories, with potentially large cross sections at hadron colliders. We present predictions for the production of top and bottom squarks…

High Energy Physics - Phenomenology · Physics 2014-11-21 Wim Beenakker , Silja Brensing , Michael Krämer , Anna Kulesza , Eric Laenen , Irene Niessen

We have determined the theoretical predictions for the cross-sections of squark and gluino production at $\ppb$ and $pp$ colliders (Tevatron and LHC) in next-to-leading order of supersymmetric QCD. By reducing the dependence on the…

High Energy Physics - Phenomenology · Physics 2011-07-19 W. Beenakker , R. H"opker , M. Spira , P. M. Zerwas

The cross section of bottom quark-antiquark ($b\bar{b}$) production in $p$+$p$ collisions at $\sqrt{s}=510$ GeV is measured with the PHENIX detector at the Relativistic Heavy Ion Collider. The results are based on the yield of high mass,…

High Energy Physics - Experiment · Physics 2020-11-18 U. Acharya , A. Adare , C. Aidala , N. N. Ajitanand , Y. Akiba , R. Akimoto , M. Alfred , N. Apadula , Y. Aramaki , H. Asano , E. T. Atomssa , T. C. Awes , B. Azmoun , V. Babintsev , M. Bai , N. S. Bandara , B. Bannier , K. N. Barish , S. Bathe , A. Bazilevsky , M. Beaumier , S. Beckman , R. Belmont , A. Berdnikov , Y. Berdnikov , L. Bichon , D. Black , B. Blankenship , J. S. Bok , V. Borisov , K. Boyle , M. L. Brooks , J. Bryslawskyj , H. Buesching , V. Bumazhnov , S. Campbell , V. Canoa Roman , C. -H. Chen , C. Y. Chi , M. Chiu , I. J. Choi , J. B. Choi , T. Chujo , Z. Citron , M. Connors , M. Csanád , T. Csörgő , A. Datta , M. S. Daugherity , G. David , K. DeBlasio , K. Dehmelt , A. Denisov , A. Deshpande , E. J. Desmond , L. Ding , A. Dion , J. H. Do , A. Drees , K. A. Drees , J. M. Durham , A. Durum , A. Enokizono , H. En'yo , R. Esha , S. Esumi , B. Fadem , W. Fan , N. Feege , D. E. Fields , M. Finger , M. Finger, , D. Firak , D. Fitzgerald , S. L. Fokin , J. E. Frantz , A. Franz , A. D. Frawley , C. Gal , P. Gallus , P. Garg , H. Ge , F. Giordano , A. Glenn , Y. Goto , N. Grau , S. V. Greene , M. Grosse Perdekamp , Y. Gu , T. Gunji , H. Guragain , T. Hachiya , J. S. Haggerty , K. I. Hahn , H. Hamagaki , S. Y. Han , J. Hanks , S. Hasegawa , X. He , T. K. Hemmick , J. C. Hill , A. Hodges , R. S. Hollis , K. Homma , B. Hong , T. Hoshino , J. Huang , S. Huang , Y. Ikeda , K. Imai , Y. Imazu , M. Inaba , A. Iordanova , D. Isenhower , D. Ivanishchev , B. V. Jacak , S. J. Jeon , M. Jezghani , Z. Ji , J. Jia , X. Jiang , B. M. Johnson , E. Joo , K. S. Joo , D. Jouan , D. S. Jumper , J. H. Kang , J. S. Kang , D. Kawall , A. V. Kazantsev , J. A. Key , V. Khachatryan , A. Khanzadeev , A. Khatiwada , K. Kihara , C. Kim , D. H. Kim , D. J. Kim , E. -J. Kim , H. -J. Kim , M. Kim , Y. K. Kim , D. Kincses , E. Kistenev , J. Klatsky , D. Kleinjan , P. Kline , T. Koblesky , M. Kofarago , J. Koster , D. Kotov , B. Kurgyis , K. Kurita , M. Kurosawa , Y. Kwon , R. Lacey , J. G. Lajoie , D. Larionova , M. Larionova , A. Lebedev , K. B. Lee , S. H. Lee , M. J. Leitch , M. Leitgab , N. A. Lewis , X. Li , S. H. Lim , M. X. Liu , S. Lökös , D. Lynch , T. Majoros , Y. I. Makdisi , M. Makek , A. Manion , V. I. Manko , E. Mannel , M. McCumber , P. L. McGaughey , D. McGlinchey , C. McKinney , A. Meles , M. Mendoza , B. Meredith , W. J. Metzger , Y. Miake , A. C. Mignerey , A. J. Miller , A. Milov , D. K. Mishra , J. T. Mitchell , Iu. Mitrankov , S. Miyasaka , S. Mizuno , P. Montuenga , T. Moon , D. P. Morrison , S. I. Morrow , T. V. Moukhanova , B. Mulilo , T. Murakami , J. Murata , A. Mwai , S. Nagamiya , J. L. Nagle , M. I. Nagy , I. Nakagawa , H. Nakagomi , K. Nakano , C. Nattrass , S. Nelson , P. K. Netrakanti , M. Nihashi , T. Niida , R. Nouicer , N. Novitzky , A. S. Nyanin , E. O'Brien , C. A. Ogilvie , J. D. Orjuela Koop , J. D. Osborn , A. Oskarsson , K. Ozawa , R. Pak , V. Pantuev , V. Papavassiliou , S. Park , S. F. Pate , L. Patel , M. Patel , J. -C. Peng , W. Peng , D. V. Perepelitsa , G. D. N. Perera , D. Yu. Peressounko , C. E. PerezLara , J. Perry , R. Petti , C. Pinkenburg , R. Pinson , R. P. Pisani , A. Pun , M. L. Purschke , P. V. Radzevich , J. Rak , N. Ramasubramanian , I. Ravinovich , K. F. Read , D. Reynolds , V. Riabov , Y. Riabov , D. Richford , T. Rinn , N. Riveli , D. Roach , S. D. Rolnick , M. Rosati , Z. Rowan , J. G. Rubin , J. Runchey , N. Saito , T. Sakaguchi , H. Sako , V. Samsonov , M. Sarsour , S. Sato , S. Sawada , B. Schaefer , B. K. Schmoll , K. Sedgwick , J. Seele , R. Seidl , A. Sen , R. Seto , P. Sett , A. Sexton , D. Sharma , I. Shein , T. -A. Shibata , K. Shigaki , M. Shimomura , P. Shukla , A. Sickles , C. L. Silva , D. Silvermyr , B. K. Singh , C. P. Singh , V. Singh , M. Slunečka , K. L. Smith , R. A. Soltz , W. E. Sondheim , S. P. Sorensen , I. V. Sourikova , P. W. Stankus , M. Stepanov , S. P. Stoll , T. Sugitate , A. Sukhanov , T. Sumita , J. Sun , X. Sun , Z. Sun , J. Sziklai , A. Takahara , A. Taketani , K. Tanida , M. J. Tannenbaum , S. Tarafdar , A. Taranenko , A. Timilsina , T. Todoroki , M. Tomášek , H. Torii , M. Towell , R. Towell , R. S. Towell , I. Tserruya , Y. Ueda , B. Ujvari , H. W. van Hecke , M. Vargyas , J. Velkovska , M. Virius , V. Vrba , E. Vznuzdaev , X. R. Wang , D. Watanabe , Y. Watanabe , Y. S. Watanabe , F. Wei , S. Whitaker , S. Wolin , C. P. Wong , C. L. Woody , Y. Wu , M. Wysocki , B. Xia , Q. Xu , L. Xue , S. Yalcin , Y. L. Yamaguchi , A. Yanovich , I. Yoon , I. Younus , I. E. Yushmanov , W. A. Zajc , A. Zelenski , Y. Zhai , S. Zharko , L. Zou

A low-energy supersymmetry scenario with a light gluino of mass 12 - 16 GeV and light sbottom (b1) of mass 2 - 6 GeV has been used to explain the apparent overproduction of b quarks at the Tevatron. In this scenario the other mass…

High Energy Physics - Phenomenology · Physics 2011-01-27 Rahul Malhotra

The discrepancy between the measured and theoretical production cross section of $b$ quarks at the Tevatron can probably be explained by the recently proposed scenario of light gluinos of mass 12-16 GeV and light sbottoms of mass $2-5.5$…

High Energy Physics - Phenomenology · Physics 2009-09-01 kingman Cheung , Wai-Yee Keung

We argue that it is possible to make a consistent picture of FNAL data including the production and decay of gluinos and squarks. The additional cross section is several pb, about the size of that for Standard Model (SM) top quark pair…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. L. Kane , S. Mrenna

We review the status of the QCD corrected cross sections and kinematic distributions for the production of a Higgs boson in association with top quark or bottom quark pairs at the Fermilab Tevatron and at the LHC. Results for b-bbar-H…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Dawson , C. B. Jackson , L. Reina , D. Wackeroth

Due to the enhancement of the couplings between Higgs boson and bottom quarks in the minimal sypersymmetric standard model (MSSM), the cross section of the process pp(p\bar{p}) \to h^0b(h^0\bar{b})+X at hadron colliders can be considerably…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hou Hong-Sheng , Ma Wen-Gan , Wu Peng , Wang Lei , Zhang Ren-You

We present cross sections for the reactions p pbar --> H gamma and pp --> H\gamma arising from the subprocess q qbar --> H gamma. The calculation includes the complete one-loop contribution from all light quarks as well as the tree…

High Energy Physics - Phenomenology · Physics 2011-01-13 A. Abbasabadi , D. Bowser-Chao , D. A. Dicus , W. W. Repko
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