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W, Gilmore J, Kamon T, Khotilovich V, Montalvo R, Osipenkov I, Pakhotin Y, Perloff A, Roe J, Safonov A, Sakuma T, Sengupta S, Suarez I, Tatarinov A, Toback D, Akchurin N, Damgov J, Dragoiu C, Dudero PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Roh Y, Volobouev I, Appelt E, Delannoy AG, Florez C, Greene S, Gurrola A, Johns W, Johnston C, Kurt P, Maguire C, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Yohay R, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sakharov A, Anderson M, Belknap DA, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Gray L, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Leonard J, Loveless R, Mohapatra A, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Search for physics beyond the standard model in events with τ leptons, jets, and large transverse momentum imbalance in pp collisions at [Formula: see text]. THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS 2013; 73:2493. [PMID: 25814865 PMCID: PMC4370880 DOI: 10.1140/epjc/s10052-013-2493-8] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 01/16/2013] [Revised: 06/11/2013] [Indexed: 06/04/2023]
Abstract
A search for physics beyond the standard model is performed with events having one or more hadronically decaying τ leptons, highly energetic jets, and large transverse momentum imbalance. The data sample corresponds to an integrated luminosity of 4.98 fb-1 of proton-proton collisions at [Formula: see text] collected with the CMS detector at the LHC in 2011. The number of observed events is consistent with predictions for standard model processes. Lower limits on the mass of the gluino in supersymmetric models are determined.
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Khotilovich V, Montalvo R, Osipenkov I, Pakhotin Y, Perloff A, Roe J, Safonov A, Sakuma T, Suarez I, Tatarinov A, Toback D, Akchurin N, Damgov J, Dragoiu C, Dudero PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Volobouev I, Appelt E, Delannoy AG, Greene S, Gurrola A, Johns W, Maguire C, Mao Y, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sakharov A, Anderson M, Belknap DA, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Loveless R, Mohapatra A, Mozer MU, Ojalvo I, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Measurement of masses in the [Formula: see text] system by kinematic endpoints in pp collisions at [Formula: see text]. THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS 2013; 73:2494. [PMID: 25814866 PMCID: PMC4371053 DOI: 10.1140/epjc/s10052-013-2494-7] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 04/21/2013] [Revised: 06/18/2013] [Indexed: 06/04/2023]
Abstract
A simultaneous measurement of the top-quark, W-boson, and neutrino masses is reported for [Formula: see text] events selected in the dilepton final state from a data sample corresponding to an integrated luminosity of 5.0 fb-1 collected by the CMS experiment in pp collisions at [Formula: see text]. The analysis is based on endpoint determinations in kinematic distributions. When the neutrino and W-boson masses are constrained to their world-average values, a top-quark mass value of [Formula: see text] is obtained. When such constraints are not used, the three particle masses are obtained in a simultaneous fit. In this unconstrained mode the study serves as a test of mass determination methods that may be used in beyond standard model physics scenarios where several masses in a decay chain may be unknown and undetected particles lead to underconstrained kinematics.
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Search for a standard-model-like Higgs boson with a mass in the range 145 to 1000 GeV at the LHC. THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS 2013; 73:2469. [PMID: 25814864 PMCID: PMC4370850 DOI: 10.1140/epjc/s10052-013-2469-8] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 03/31/2013] [Revised: 05/04/2013] [Indexed: 06/04/2023]
Abstract
A search for a standard-model-like Higgs boson in the H→WW and H→ZZ decay channels is reported, for Higgs boson masses in the range 145
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Liu B, Zhou S, Song S. SU-E-T-613: A Multi-Isocenter IMRT Approach of Large Fields to Reduce the Hot Or Cold Spots Caused by Setup Error. Med Phys 2013. [DOI: 10.1118/1.4815041] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/07/2022] Open
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Dogan N, Sleeman W, Asher D, Fatyga M, Schutzer M, Song S. SU-E-J-94: Assessment of Dose Accumulation with Different Deformable Image Registration Algorithms for Image-Guided Radiotherapy of Head and Neck Cancer. Med Phys 2013. [DOI: 10.1118/1.4814306] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/07/2022] Open
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PC, Bloch I, Burkett K, Butler JN, Chetluru V, Cheung HWK, Chlebana F, Elvira VD, Fisk I, Freeman J, Gao Y, Green D, Gutsche O, Hanlon J, Harris RM, Hirschauer J, Hooberman B, Jindariani S, Johnson M, Joshi U, Kilminster B, Klima B, Kunori S, Kwan S, Leonidopoulos C, Linacre J, Lincoln D, Lipton R, Lykken J, Maeshima K, Marraffino JM, Maruyama S, Mason D, McBride P, Mishra K, Mrenna S, Musienko Y, Newman-Holmes C, O’Dell V, Prokofyev O, Sexton-Kennedy E, Sharma S, Spalding WJ, Spiegel L, Taylor L, Tkaczyk S, Tran NV, Uplegger L, Vaandering EW, Vidal R, Whitmore J, Wu W, Yang F, Yumiceva F, Yun JC, Acosta D, Avery P, Bourilkov D, Chen M, Cheng T, Das S, De Gruttola M, Di Giovanni GP, Dobur D, Drozdetskiy A, Field RD, Fisher M, Fu Y, Furic IK, Gartner J, Hugon J, Kim B, Konigsberg J, Korytov A, Kropivnitskaya A, Kypreos T, Low JF, Matchev K, Milenovic P, Mitselmakher G, Muniz L, Park M, Remington R, Rinkevicius A, Sellers P, Skhirtladze N, Snowball M, Yelton J, Zakaria M, Gaultney V, 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Sakuma T, Sengupta S, Suarez I, Tatarinov A, Toback D, Akchurin N, Damgov J, Dragoiu C, Dudero PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Roh Y, Volobouev I, Appelt E, Delannoy AG, Florez C, Greene S, Gurrola A, Johns W, Kurt P, Maguire C, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sakharov A, Anderson M, Belknap DA, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Gray L, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Leonard J, Loveless R, Mohapatra A, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Search for supersymmetry in pp collisions at [Formula: see text] TeV in events with a single lepton, jets, and missing transverse momentum. THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS 2013; 73:2404. [PMID: 25814857 PMCID: PMC4370766 DOI: 10.1140/epjc/s10052-013-2404-z] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/28/2012] [Revised: 03/02/2013] [Indexed: 05/30/2023]
Abstract
Results are reported from a search for new physics processes in events containing a single isolated high-transverse-momentum lepton (electron or muon), energetic jets, and large missing transverse momentum. The analysis is based on a 4.98 fb-1 sample of proton-proton collisions at a center-of-mass energy of 7 TeV, obtained with the CMS detector at the LHC. Three separate background estimation methods, each relying primarily on control samples in the data, are applied to a range of signal regions, providing complementary approaches for estimating the background yields. The observed yields are consistent with the predicted standard model backgrounds. The results are interpreted in terms of limits on the parameter space for the constrained minimal supersymmetric extension of the standard model, as well as on cross sections for simplified models, which provide a generic description of the production and decay of new particles in specific, topology based final states. ELECTRONIC SUPPLEMENTARY MATERIAL The online version of this article (doi:10.1140/epjc/s10052-013-2404-z) contains supplementary material, which is available to authorized users.
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Lee H, Song S, Lim K, Han S, Kim W, Oh Y, Lee J. 30P DIFFERENTIAL MICRORNA EXPRESSION AND TARGET GENES BETWEEN LUNG CANCER AND NORMAL TISSUE. Lung Cancer 2013. [DOI: 10.1016/s0169-5002(13)70251-4] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/26/2022]
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MU, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Measurement of associated production of vector bosons and top quark-antiquark pairs in pp collisions at sqrt[s]=7 TeV. PHYSICAL REVIEW LETTERS 2013; 110:172002. [PMID: 23679709 DOI: 10.1103/physrevlett.110.172002] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/13/2013] [Indexed: 06/02/2023]
Abstract
The first measurement of vector-boson production associated with a top quark-antiquark pair in proton-proton collisions at sqrt[s] = 7 TeV is presented. The results are based on a data set corresponding to an integrated luminosity of 5.0 fb(-1), recorded by the CMS detector at the LHC in 2011. The measurement is performed in two independent channels through a trilepton analysis of ttZ events and a same-sign dilepton analysis of ttV (V = W or Z) events. In the trilepton channel a direct measurement of the ttZ cross section σ(ttZ) = 0.28(-0.11)(+0.14) (stat)(-0.03)(+0.06) (syst) pb is obtained. In the dilepton channel a measurement of the ttV cross section yields σ(ttV) = 0.43(-0.15)(+0.17) (stat)(-0.07)(+0.09) (syst) pb. These measurements have a significance, respectively, of 3.3 and 3.0 standard deviations from the background hypotheses and are compatible, within uncertainties, with the corresponding next-to-leading order predictions of 0.137(-0.016)(+0.012) and 0.306(-0.053)(+0.031) pb.
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Search for new physics in final states with a lepton and missing transverse energy inppcollisions at the LHC. Int J Clin Exp Med 2013. [DOI: 10.1103/physrevd.87.072005] [Citation(s) in RCA: 10] [Impact Index Per Article: 0.9] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/07/2022]
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Vaughan J, Weng Y, Winstrom L, Wittich P, Winn D, Abdullin S, Albrow M, Anderson J, Bauerdick LAT, Beretvas A, Berryhill J, Bhat PC, Burkett K, Butler JN, Chetluru V, Cheung HWK, Chlebana F, Cihangir S, Elvira VD, Fisk I, Freeman J, Gao Y, Green D, Gutsche O, Hanlon J, Harris RM, Hirschauer J, Hooberman B, Jindariani S, Johnson M, Joshi U, Klima B, Kunori S, Kwan S, Leonidopoulos C, Linacre J, Lincoln D, Lipton R, Lykken J, Maeshima K, Marraffino JM, Martinez Outschoorn VI, Maruyama S, Mason D, McBride P, Mishra K, Mrenna S, Musienko Y, Newman-Holmes C, O'Dell V, Prokofyev O, Sexton-Kennedy E, Sharma S, Spalding WJ, Spiegel L, Taylor L, Tkaczyk S, Tran NV, Uplegger L, Vaandering EW, Vidal R, Whitmore J, Wu W, Yang F, Yun JC, Acosta D, Avery P, Bourilkov D, Chen M, Cheng T, Das S, De Gruttola M, Di Giovanni GP, Dobur D, Drozdetskiy A, Field RD, Fisher M, Fu Y, Furic IK, Gartner J, Hugon J, Kim B, Konigsberg J, Korytov A, Kropivnitskaya A, Kypreos T, Low JF, Matchev K, Milenovic P, Mitselmakher G, Muniz L, Park M, Remington R, Rinkevicius A, Sellers P, Skhirtladze N, Snowball M, Yelton J, Zakaria M, Gaultney V, Hewamanage S, Lebolo LM, Linn S, Markowitz P, Martinez G, Rodriguez JL, Adams T, Askew A, Bochenek J, Chen J, Diamond B, Gleyzer SV, Haas J, Hagopian S, Hagopian V, Jenkins M, Johnson KF, Prosper H, Veeraraghavan V, Weinberg M, Baarmand MM, Dorney B, Hohlmann M, Kalakhety H, Vodopiyanov I, Yumiceva F, Adams MR, Anghel IM, Apanasevich L, Bai Y, Bazterra VE, Betts RR, Bucinskaite I, Callner J, Cavanaugh R, Evdokimov O, Gauthier L, Gerber CE, Hofman DJ, Khalatyan S, Lacroix F, O'Brien C, Silkworth C, Strom D, Turner P, Varelas N, Akgun U, Albayrak EA, Bilki B, Clarida W, Duru F, Griffiths S, Merlo JP, Mermerkaya H, Mestvirishvili A, Moeller A, Nachtman J, Newsom CR, Norbeck E, Onel Y, Ozok F, Sen S, Tan P, Tiras E, Wetzel J, Yetkin T, Yi K, Barnett BA, Blumenfeld B, Bolognesi S, Fehling D, Giurgiu G, Gritsan AV, Guo ZJ, Hu G, Maksimovic P, Swartz M, Whitbeck A, Baringer P, Bean A, Benelli G, Kenny Iii RP, Murray M, Noonan D, Sanders S, Stringer R, Tinti G, Wood JS, Barfuss AF, Bolton T, Chakaberia I, Ivanov A, Khalil S, Makouski M, Maravin Y, Shrestha S, Svintradze I, Gronberg J, Lange D, Rebassoo F, Wright D, Baden A, Calvert B, Eno SC, Gomez JA, Hadley NJ, Kellogg RG, Kirn M, Kolberg T, Lu Y, Marionneau M, Mignerey AC, Pedro K, Peterman A, Skuja A, Temple J, Tonjes MB, Tonwar SC, Apyan A, Bauer G, Bendavid J, Busza W, Butz E, Cali IA, Chan M, Dutta V, Gomez Ceballos G, Goncharov M, Kim Y, Klute M, Krajczar K, Levin A, Luckey PD, Ma T, Nahn S, Paus C, Ralph D, Roland C, Roland G, Rudolph M, Stephans GSF, Stöckli F, Sumorok K, Sung K, Velicanu D, Wenger EA, Wolf R, Wyslouch B, Yang M, Yilmaz Y, Yoon AS, Zanetti M, Zhukova V, Cooper SI, Dahmes B, De Benedetti A, Franzoni G, Gude A, Kao SC, Klapoetke K, Kubota Y, Mans J, Pastika N, Rusack R, Sasseville M, Singovsky A, Tambe N, Turkewitz J, Cremaldi LM, Kroeger R, Perera L, Rahmat R, Sanders DA, Avdeeva E, Bloom K, Bose S, Claes DR, Dominguez A, Eads M, Keller J, Kravchenko I, Lazo-Flores J, Malik S, Snow GR, Godshalk A, Iashvili I, Jain S, Kharchilava A, Kumar A, Rappoccio S, Wan Z, Alverson G, Barberis E, Baumgartel D, Chasco M, Haley J, Nash D, Orimoto T, Trocino D, Wood D, Zhang J, Anastassov A, Hahn KA, Kubik A, Lusito L, Mucia N, Odell N, Ofierzynski RA, Pollack B, Pozdnyakov A, Schmitt M, Stoynev S, Velasco M, Won S, Berry D, Brinkerhoff A, Chan KM, Hildreth M, Jessop C, Karmgard DJ, Kolb J, Lannon K, Luo W, Lynch S, Marinelli N, Morse DM, Pearson T, Planer M, Ruchti R, Slaunwhite J, Valls N, Wayne M, Wolf M, Antonelli L, Bylsma B, Durkin LS, Hill C, Hughes R, Kotov K, Ling TY, Puigh D, Rodenburg M, Vuosalo C, Williams G, Winer BL, Berry E, Elmer P, Halyo V, Hebda P, Hegeman J, Hunt A, Jindal P, Koay SA, Lopes Pegna D, Lujan P, Marlow D, Medvedeva T, Mooney M, Olsen J, Piroué P, Quan X, Raval A, Saka H, Stickland D, Tully C, Werner JS, Zenz SC, Zuranski A, Brownson E, Lopez A, Mendez H, Ramirez Vargas JE, Alagoz E, Barnes VE, Benedetti D, Bolla G, Bortoletto D, De Mattia M, Everett A, Hu Z, Jones M, Koybasi O, Kress M, Laasanen AT, Leonardo N, Maroussov V, Merkel P, Miller DH, Neumeister N, Shipsey I, Silvers D, Svyatkovskiy A, Vidal Marono M, Yoo HD, Zablocki J, Zheng Y, Guragain S, Parashar N, Adair A, Akgun B, Boulahouache C, Ecklund KM, Geurts FJM, Li W, Padley BP, Redjimi R, Roberts J, Zabel J, Betchart B, Bodek A, Chung YS, Covarelli R, de Barbaro P, Demina R, Eshaq Y, Ferbel T, Garcia-Bellido A, Goldenzweig P, Han J, Harel A, Miner DC, Vishnevskiy D, Zielinski M, Bhatti A, Ciesielski R, Demortier L, Goulianos K, Lungu G, Malik S, Mesropian C, Arora S, Barker A, Chou JP, Contreras-Campana C, Contreras-Campana E, Duggan D, Ferencek D, Gershtein Y, Gray R, Halkiadakis E, Hidas D, Lath A, Panwalkar S, Park M, Patel R, Rekovic V, Robles J, Rose K, Salur S, Schnetzer S, Seitz C, Somalwar S, Stone R, Thomas S, Walker M, Cerizza G, Hollingsworth M, Spanier S, Yang ZC, York A, Eusebi R, Flanagan W, Gilmore J, Kamon T, Khotilovich V, Montalvo R, Osipenkov I, Pakhotin Y, Perloff A, Roe J, Safonov A, Sakuma T, Sengupta S, Suarez I, Tatarinov A, Toback D, Akchurin N, Damgov J, Dragoiu C, Dudero PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Volobouev I, Appelt E, Delannoy AG, Florez C, Greene S, Gurrola A, Johns W, Kurt P, Maguire C, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sakharov A, Anderson M, Belknap DA, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Gray L, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Loveless R, Mohapatra A, Mozer MU, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Search for pair-produced dijet resonances in four-jet final states in pp collisions at sqrt[s] = 7 TeV. PHYSICAL REVIEW LETTERS 2013; 110:141802. [PMID: 25166980 DOI: 10.1103/physrevlett.110.141802] [Citation(s) in RCA: 8] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/03/2013] [Indexed: 06/03/2023]
Abstract
A search for the pair production of a heavy, narrow resonance decaying into two jets has been performed using events collected in sqrt[s] = 7 TeV pp collisions with the CMS detector at the LHC. The data sample corresponds to an integrated luminosity of 5.0 fb(-1). Events are selected with at least four jets and two dijet combinations with similar dijet mass. No resonances are found in the dijet mass spectrum. The upper limit at 95% confidence level on the product of the resonance pair production cross section, the branching fractions into dijets, and the acceptance varies from 0.22 to 0.005 pb, for resonance masses between 250 and 1200 GeV. Pair-produced colorons decaying into qq are excluded for coloron masses between 250 and 740 GeV.
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Jeong J, Cho I, Kong E, Chun K, Jang B, Kim T, Kim S, Song S. Evaluation of hybrid PET/CT gastrography in gastric cancer. Nuklearmedizin 2013; 52:107-12. [PMID: 23681152 DOI: 10.3413/nukmed-0504-12-05] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/11/2012] [Accepted: 10/28/2012] [Indexed: 01/25/2023]
Abstract
AIM With the recent advances in multidetector-row CT, a fusion of functional PET with three dimensional (3D) CT gastrography may provide enhanced diagnostic capability and help surgeons during preoperative planning. The diagnostic value of hybrid PET/CT gastrography was compared with that of conventional PET/CT alone in gastric cancer staging. PATIENTS, METHODS Patients with gastric cancer (n = 101) confirmed by endoscopic biopsy specimens underwent conventional PET/CT and regional PET with contrast enhanced CT, followed by gastrectomy with lymphadenectomy at our institution from November 2007 to November 2008. These images were fused into a hybrid PET/CT gastrography using the cardiac IQ fusion software. Conventional PET/CT and hybrid PET/CT gastrography were evaluated for staging of gastric cancer. After gastrectomy, these were compared with pathologic reports respectively. RESULTS Gastric cancer was diagnosed as 50 early gastric cancer (EGC) and 51 advanced gastric cancer (AGC) on pathologic examination. In EGC, hybrid PET/CT gastrography and PET/CT identified 36 (72%) and 7 (14%) tumours, respectively. Hybrid PET/CT gastrography correctly delineated the subtype of 25 EGC. In AGC, all 51 (100%) tumours were identified on the hybrid PET/CT gastrography compared to 39 (76.5%) tumours on PET/CT. Hybrid PET/CT gastrography correctly classified the morphology of 42 AGC using the Bormann classification. Additionally, depth of invasion was correctly presented in 38 of 51 AGC. Hybrid PET/CT gastrography for regional lymph node (LN) metastasis in the EGC and AGC showed the sensitivity of 75% and 83.9%, and specificity 90.5% and 55%, respectively. CONCLUSION Hybrid PET/CT gastrography is the more intuitive and comprehensive method for the preoperative evaluation of gastric cancer than conventional PET/CT.
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Robert A, Curtis R, Flath D, Gray A, Sikorski M, Song S, Srinivasan V, Stefanescu D. The X-ray Correlation Spectroscopy instrument at the Linac Coherent Light Source. ACTA ACUST UNITED AC 2013. [DOI: 10.1088/1742-6596/425/21/212009] [Citation(s) in RCA: 11] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
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Xiang Q, Wang CL, Song S, Shi TJ. WITHDRAWN: Highly efficient agonist-induced internalization of somatostatin SST2 receptor in mouse dorsal root ganglion and spinal cord: Molecular evidence for mechanism of somatostatin inhibits neuropathic pain. REGULATORY PEPTIDES 2013:S0167-0115(13)00042-6. [PMID: 23507148 DOI: 10.1016/j.regpep.2013.03.013] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/18/2012] [Revised: 11/29/2012] [Accepted: 03/03/2013] [Indexed: 06/01/2023]
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Shi Y, Zhang L, Song S, Teves ME, Li H, Wang Z, Hess RA, Jiang G, Zhang Z. The mouse transcription factor-like 5 gene encodes a protein localized in the manchette and centriole of the elongating spermatid. Andrology 2013; 1:431-9. [PMID: 23444080 DOI: 10.1111/j.2047-2927.2013.00069.x] [Citation(s) in RCA: 13] [Impact Index Per Article: 1.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/27/2012] [Revised: 01/05/2013] [Accepted: 01/11/2013] [Indexed: 12/17/2022]
Abstract
Spermiogenesis is the final phase of spermatogenesis. During this process, haploid round spermatids differentiate into spermatozoa, with dramatic morphological changes, including elongation and condensation of the nuclei, and formation of the flagella. Meig1 is one of many genes involved in the regulation of this process. Male mice deficient in MEIG1 are sterile with a severe defect in spermiogenesis, associated with dramatic disruption of the spermatid manchette and failure of flagellogenesis. A yeast two-hybrid screen using full-length MEIG1 as bait identified transcription factor-like 5 protein (TCFL5) as a putative interacting proteins. Interestingly, this protein was also identified as a potential binding partner of SPAG16, another protein essential for spermatogenesis, and also a binding partner of MEIG1. The interaction between TCFL5 and MEIG1 was confirmed in cultured cells over-expressing the two proteins. The mouse Tcfl5 transcript is present only in the testis, and its expression is significantly increased during spermiogenesis. However, little is known about TCFL5 protein and its role in male germ cells. A rabbit polyclonal antibody was generated against the C-terminal region of TCFL5. Mouse TCFL5 protein was expressed in the testis but not in mature spermatozoa. During the first wave of spermatogenesis, TCFL5 expression was dramatically increased at day 30 after birth. In the testis and a mixture of dispersed testicular cells, the protein co-localized with α-tubulin, a manchette marker in early elongating spermatids. The protein also localized in the centrioles of late elongating spermatids. No obvious differences in TCFL5 epitope abundance and localization were observed between wild type and the Meig1-deficient mice. These findings suggest that TCFL5 may play a role upstream of MEIG1 action, and based on putative binding partners and localization is likely to be involved in spermiogenesis and formation of the sperm flagella.
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I, Burkett K, Butler JN, Chetluru V, Cheung HWK, Chlebana F, Elvira VD, Fisk I, Freeman J, Gao Y, Green D, Gutsche O, Hanlon J, Harris RM, Hirschauer J, Hooberman B, Jindariani S, Johnson M, Joshi U, Kilminster B, Klima B, Kunori S, Kwan S, Leonidopoulos C, Linacre J, Lincoln D, Lipton R, Lykken J, Maeshima K, Marraffino JM, Maruyama S, Mason D, McBride P, Mishra K, Mrenna S, Musienko Y, Newman-Holmes C, O'Dell V, Prokofyev O, Sexton-Kennedy E, Sharma S, Spalding WJ, Spiegel L, Taylor L, Tkaczyk S, Tran NV, Uplegger L, Vaandering EW, Vidal R, Whitmore J, Wu W, Yang F, Yumiceva F, Yun JC, Acosta D, Avery P, Bourilkov D, Chen M, Cheng T, Das S, De Gruttola M, Di Giovanni GP, Dobur D, Drozdetskiy A, Field RD, Fisher M, Fu Y, Furic IK, Gartner J, Hugon J, Kim B, Konigsberg J, Korytov A, Kropivnitskaya A, Kypreos T, Low JF, Matchev K, Milenovic P, Mitselmakher G, Muniz L, Park M, Remington R, Rinkevicius A, Sellers P, Skhirtladze N, Snowball M, Yelton J, Zakaria M, Gaultney V, Hewamanage S, 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Safonov A, Sakuma T, Sengupta S, Suarez I, Tatarinov A, Toback D, Akchurin N, Damgov J, Dragoiu C, Dudero PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Roh Y, Volobouev I, Appelt E, Delannoy AG, Florez C, Greene S, Gurrola A, Johns W, Johnston C, Kurt P, Maguire C, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Yohay R, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sakharov A, Anderson M, Belknap D, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Gray L, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Leonard J, Loveless R, Mohapatra A, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Search for pair production of third-generation leptoquarks and top squarks in pp collisions at sqrt[s] = 7 TeV. PHYSICAL REVIEW LETTERS 2013; 110:081801. [PMID: 23473129 DOI: 10.1103/physrevlett.110.081801] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/22/2012] [Indexed: 06/01/2023]
Abstract
Results are presented from a search for the pair production of third-generation scalar and vector leptoquarks, as well as for top squarks in R-parity-violating supersymmetric models. In either scenario, the new, heavy particle decays into a τ lepton and a b quark. The search is based on a data sample of pp collisions at sqrt[s] = 7 TeV, which is collected by the CMS detector at the LHC and corresponds to an integrated luminosity of 4.8 fb(-1). The number of observed events is found to be in agreement with the standard model prediction, and exclusion limits on mass parameters are obtained at the 95% confidence level. Vector leptoquarks with masses below 760 GeV are excluded and, if the branching fraction of the scalar leptoquark decay to a τ lepton and a b quark is assumed to be unity, third-generation scalar leptoquarks with masses below 525 GeV are ruled out. Top squarks with masses below 453 GeV are excluded for a typical benchmark scenario, and limits on the coupling between the top squark, τ lepton, and b quark, λ(333)(') are obtained. These results are the most stringent for these scenarios to date.
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Zheng Y, Guragain S, Parashar N, Adair A, Akgun B, Boulahouache C, Ecklund KM, Geurts FJM, Li W, Padley BP, Redjimi R, Roberts J, Zabel J, Betchart B, Bodek A, Chung YS, Covarelli R, de Barbaro P, Demina R, Eshaq Y, Ferbel T, Garcia-Bellido A, Goldenzweig P, Han J, Harel A, Miner DC, Vishnevskiy D, Zielinski M, Bhatti A, Ciesielski R, Demortier L, Goulianos K, Lungu G, Malik S, Mesropian C, Arora S, Barker A, Chou JP, Contreras-Campana C, Contreras-Campana E, Duggan D, Ferencek D, Gershtein Y, Gray R, Halkiadakis E, Hidas D, Lath A, Panwalkar S, Park M, Patel R, Rekovic V, Robles J, Rose K, Salur S, Schnetzer S, Seitz C, Somalwar S, Stone R, Thomas S, Walker M, Cerizza G, Hollingsworth M, Spanier S, Yang ZC, York A, Eusebi R, Flanagan W, Gilmore J, Kamon T, Khotilovich V, Montalvo R, Osipenkov I, Pakhotin Y, Perloff A, Roe J, Safonov A, Sakuma T, Sengupta S, Suarez I, Tatarinov A, Toback D, Akchurin N, Damgov J, Dragoiu C, Dudero PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Roh Y, Volobouev I, Appelt E, Delannoy AG, Florez C, Greene S, Gurrola A, Johns W, Kurt P, Maguire C, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sakharov A, Anderson M, Belknap D, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Gray L, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Loveless R, Mohapatra A, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Measurement of the Υ1S, Υ2S, and Υ3S polarizations in pp collisions at sqrt[s] = 7 TeV. PHYSICAL REVIEW LETTERS 2013; 110:081802. [PMID: 23473130 DOI: 10.1103/physrevlett.110.081802] [Citation(s) in RCA: 9] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/13/2012] [Indexed: 06/01/2023]
Abstract
The polarizations of the Υ(1S), Υ(2S), and Υ(3S) mesons are measured in proton-proton collisions at sqrt[s] = 7 TeV, using a data sample of Υ(nS) → μ +μ- decays collected by the CMS experiment, corresponding to an integrated luminosity of 4.9 fb(-1). The dimuon decay angular distributions are analyzed in three different polarization frames. The polarization parameters λ[symbol see text], λ(φ), and λ([symbol see text]φ), as well as the frame-invariant quantity λ, are presented as a function of the Υ(nS) transverse momentum between 10 and 50 GeV, in the rapidity ranges |y|<0.6 and 0.6<|y|<1.2. No evidence of large transverse or longitudinal polarizations is seen in the explored kinematic region.
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Swanson J. Study of the mass and spin-parity of the Higgs boson candidate via its decays to Z boson pairs. PHYSICAL REVIEW LETTERS 2013; 110:081803. [PMID: 23473131 DOI: 10.1103/physrevlett.110.081803] [Citation(s) in RCA: 33] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/29/2012] [Indexed: 06/01/2023]
Abstract
A study is presented of the mass and spin-parity of the new boson recently observed at the LHC at a mass near 125 GeV. An integrated luminosity of 17.3 fb(-1), collected by the CMS experiment in proton-proton collisions at center-of-mass energies of 7 and 8 TeV, is used. The measured mass in the ZZ channel, where both Z bosons decay to e or μ pairs, is 126.2 ± 0.6(stat) ± 0.2(syst) GeV. The angular distributions of the lepton pairs in this channel are sensitive to the spin-parity of the boson. Under the assumption of spin 0, the present data are consistent with the pure scalar hypothesis, while disfavoring the pure pseudoscalar hypothesis.
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PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Roh Y, Volobouev I, Appelt E, Delannoy AG, Florez C, Greene S, Gurrola A, Johns W, Kurt P, Maguire C, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Mcgee K, Sakharov A, Siehl K, Anderson M, Belknap D, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Gray L, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Leonard J, Loveless R, Mohapatra A, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Measurement of the sum of WW and WZ production with W+dijet events in pp collisions at [Formula: see text]. THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS 2013; 73:2283. [PMID: 25814853 PMCID: PMC4370803 DOI: 10.1140/epjc/s10052-013-2283-3] [Citation(s) in RCA: 8] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/29/2012] [Revised: 12/20/2012] [Indexed: 06/02/2023]
Abstract
A measurement of the inclusive WW+WZ diboson production cross section in proton-proton collisions is reported, based on events containing a leptonically decaying W boson and exactly two jets. The data sample, collected at [Formula: see text] with the CMS detector at the LHC, corresponds to an integrated luminosity of 5.0 fb-1. The measured value of the sum of the inclusive WW and WZ cross sections is σ(pp→WW+WZ)=68.9±8.7 (stat.)±9.7 (syst.)±1.5 (lum.) pb, consistent with the standard model prediction of 65.6±2.2 pb. This is the first measurement of WW+WZ production in pp collisions using this signature. No evidence for anomalous triple gauge couplings is found and upper limits are set on their magnitudes.
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Vanelderen L, Barth C, Berger J, Böser C, Chwalek T, De Boer W, Descroix A, Dierlamm A, Feindt M, Guthoff M, Hackstein C, Hartmann F, Hauth T, Heinrich M, Held H, Hoffmann KH, Honc S, Katkov I, Komaragiri JR, Lobelle Pardo P, Martschei D, Mueller S, Müller T, Niegel M, Nürnberg A, Oberst O, Oehler A, Ott J, Quast G, Rabbertz K, Ratnikov F, Ratnikova N, Röcker S, Scheurer A, Schilling FP, Schott G, Simonis HJ, Stober FM, Troendle D, Ulrich R, Wagner-Kuhr J, Wayand S, Weiler T, Zeise M, Daskalakis G, Geralis T, Kesisoglou S, Kyriakis A, Loukas D, Manolakos I, Markou A, Markou C, Mavrommatis C, Ntomari E, Gouskos L, Mertzimekis TJ, Panagiotou A, Saoulidou N, Evangelou I, Foudas C, Kokkas P, Manthos N, Papadopoulos I, Patras V, Bencze G, Hajdu C, Hidas P, Horvath D, Sikler F, Veszpremi V, Vesztergombi G, Beni N, Czellar S, Molnar J, Palinkas J, Szillasi Z, Karancsi J, Raics P, Trocsanyi ZL, Ujvari B, Beri SB, Bhatnagar V, Dhingra N, Gupta R, Kaur M, Mehta MZ, Nishu N, Saini LK, Sharma A, Singh JB, Kumar A, Kumar A, Ahuja S, Bhardwaj A, Choudhary BC, Malhotra S, Naimuddin M, Ranjan K, Sharma V, Shivpuri RK, Banerjee S, Bhattacharya S, Dutta S, Gomber B, Jain S, Jain S, Khurana R, Sarkar S, Sharan M, Abdulsalam A, Choudhury RK, Dutta D, Kailas S, Kumar V, Mehta P, Mohanty AK, Pant LM, Shukla P, Aziz T, Ganguly S, Guchait M, Maity M, Majumder G, Mazumdar K, Mohanty GB, Parida B, Sudhakar K, Wickramage N, Banerjee S, Dugad S, Arfaei H, Bakhshiansohi H, Etesami SM, Fahim A, Hashemi M, Hesari H, Jafari A, Khakzad M, Mohammadi Najafabadi M, Paktinat Mehdiabadi S, Safarzadeh B, Zeinali M, Abbrescia M, Barbone L, Calabria C, Chhibra SS, Colaleo A, Creanza D, De Filippis N, De Palma M, Fiore L, Iaselli G, Lusito L, Maggi G, Maggi M, Marangelli B, My S, Nuzzo S, Pacifico N, Pompili A, Pugliese G, Selvaggi G, Silvestris L, Singh G, Venditti R, Zito G, Abbiendi G, Benvenuti AC, Bonacorsi D, Braibant-Giacomelli S, Brigliadori L, Capiluppi P, Castro A, Cavallo FR, Cuffiani M, Dallavalle GM, Fabbri F, Fanfani A, Fasanella D, Giacomelli P, Grandi C, Guiducci L, Marcellini S, Masetti G, Meneghelli M, Montanari A, Navarria FL, Odorici F, Perrotta A, Primavera F, Rossi AM, Rovelli T, Siroli GP, Travaglini R, Albergo S, Cappello G, Chiorboli M, Costa S, Potenza R, Tricomi A, Tuve C, Barbagli G, Ciulli V, Civinini C, D’Alessandro R, Focardi E, Frosali S, Gallo E, Gonzi S, Meschini M, Paoletti S, Sguazzoni G, Tropiano A, Benussi L, Bianco S, Colafranceschi S, Fabbri F, Piccolo D, Fabbricatore P, Musenich R, Tosi S, Benaglia A, De Guio F, Di Matteo L, Fiorendi S, Gennai S, Ghezzi A, Malvezzi S, Manzoni RA, Martelli A, Massironi A, Menasce D, Moroni L, Paganoni M, Pedrini D, Ragazzi S, Redaelli N, Sala S, Tabarelli de Fatis T, Buontempo S, Carrillo Montoya CA, Cavallo N, De Cosa A, Dogangun O, Fabozzi F, Iorio AOM, Lista L, Meola S, Merola M, Paolucci P, Azzi P, Bacchetta N, Bisello D, Branca A, Carlin R, Checchia P, Gasparini F, Gasparini U, Gozzelino A, Kanishchev K, Lacaprara S, Lazzizzera I, Margoni M, Meneguzzo AT, Pazzini J, Pozzobon N, Ronchese P, Simonetto F, Torassa E, Tosi M, Triossi A, Vanini S, Ventura S, Zotto P, Gabusi M, Ratti SP, Riccardi C, Torre P, Vitulo P, Biasini M, Bilei GM, Fanò L, Lariccia P, Lucaroni A, Mantovani G, Menichelli M, Nappi A, Romeo F, Saha A, Santocchia A, Spiezia A, Taroni S, Azzurri P, Bagliesi G, Bernardini J, Boccali T, Broccolo G, Castaldi R, D’Agnolo RT, Dell’Orso R, Fiori F, Foà L, Giassi A, Kraan A, Ligabue F, Lomtadze T, Martini L, Messineo A, Palla F, Rizzi A, Serban AT, Spagnolo P, Squillacioti P, Tenchini R, Tonelli G, Venturi A, Verdini PG, Barone L, Cavallari F, Del Re D, Diemoz M, Fanelli C, Grassi M, Longo E, Meridiani P, Micheli F, Nourbakhsh S, Organtini G, Paramatti R, Rahatlou S, Sigamani M, Soffi L, Amapane N, Arcidiacono R, Argiro S, Arneodo M, Biino C, Cartiglia N, Costa M, Demaria N, Mariotti C, Maselli S, Migliore E, Monaco V, Musich M, Obertino MM, Pastrone N, Pelliccioni M, Potenza A, Romero A, Ruspa M, Sacchi R, Solano A, Staiano A, Vilela Pereira A, Belforte S, Candelise V, Cossutti F, Della Ricca G, Gobbo B, Marone M, Montanino D, Penzo A, Schizzi A, Heo SG, Kim TY, Nam SK, Chang S, Kim DH, Kim GN, Kong DJ, Park H, Ro SR, Son DC, Son T, Kim JY, Kim ZJ, Song S, Choi S, Gyun D, Hong B, Jo M, Kim H, Kim TJ, Lee KS, Moon DH, Park SK, Choi M, Kim JH, Park C, Park IC, Park S, Ryu G, Cho Y, Choi Y, Choi YK, Goh J, Kim MS, Kwon E, Lee B, Lee J, Lee S, Seo H, Yu I, Bilinskas MJ, Grigelionis I, Janulis M, Juodagalvis A, Castilla-Valdez H, De La Cruz-Burelo E, Heredia-de La Cruz I, Lopez-Fernandez R, Magaña Villalba R, Martínez-Ortega J, Sanchez-Hernandez A, Villasenor-Cendejas LM, Carrillo Moreno S, Vazquez Valencia F, Salazar Ibarguen HA, Casimiro Linares E, Morelos Pineda A, Reyes-Santos MA, Krofcheck D, Bell AJ, Butler PH, Doesburg R, Reucroft S, Silverwood H, Ahmad M, Ansari MH, Asghar MI, Hoorani HR, Khalid S, Khan WA, Khurshid T, Qazi S, Shah MA, Shoaib M, Bialkowska H, Boimska B, Frueboes T, Gokieli R, Górski M, Kazana M, Nawrocki K, Romanowska-Rybinska K, Szleper M, Wrochna G, Zalewski P, Brona G, Bunkowski K, Cwiok M, Dominik W, Doroba K, Kalinowski A, Konecki M, Krolikowski J, Almeida N, Bargassa P, David A, Faccioli P, Ferreira Parracho PG, Gallinaro M, Seixas J, Varela J, Vischia P, Belotelov I, Bunin P, Golutvin I, Gorbunov I, Kamenev A, Karjavin V, Kozlov G, Lanev A, Malakhov A, Moisenz P, Palichik V, Perelygin V, Savina M, Shmatov S, Smirnov V, Volodko A, Zarubin A, Evstyukhin S, Golovtsov V, Ivanov Y, Kim V, Levchenko P, Murzin V, Oreshkin V, Smirnov I, Sulimov V, Uvarov L, Vavilov S, Vorobyev A, Vorobyev A, Andreev Y, Dermenev A, Gninenko S, Golubev N, Kirsanov M, Krasnikov N, Matveev V, Pashenkov A, Tlisov D, Toropin A, Epshteyn V, Erofeeva M, Gavrilov V, Kossov M, Lychkovskaya N. Search for contact interactions inμ+μ−events inppcollisions ats=7 TeV. Int J Clin Exp Med 2013. [DOI: 10.1103/physrevd.87.032001] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/07/2022]
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Li S, Li W, Yang Z, Song S, Yang J, Gong P, Zhang W, Liu K, Li J, Zhang G, Zhang X. Infection of cattle with Cryptosporidium parvum: mast cell accumulation in small intestine mucosa. Vet Pathol 2013; 50:842-8. [PMID: 23370094 DOI: 10.1177/0300985813476055] [Citation(s) in RCA: 7] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/16/2022]
Abstract
Mast cells might play an important role as the major effector cells in the immune response against Cryptosporidium parvum. C. parvum is a protozoan parasite that causes cryptosporidiosis in animals and humans worldwide. To investigate the interaction between C. parvum and mast cells during infection, nine 3-day-old male calves were orally challenged with 10(6) oocysts of C. parvum per calf. The distribution of mast cells in the mucosa of the small intestine was analyzed by toluidine blue staining. The concentrations of histamine and the cytokines interferon-γ, interleukin-4, interleukin-2, and interleukin-12 were measured in the serum, and the histamine levels were also determined from the intestinal contents. The following clinical signs were monitored: nausea, watery diarrhea, dehydration, and weight loss. Oocysts were shed in the feces during the infection period. C. parvum infection induced an increase in mast cell numbers in the mucosa of the small intestine in distinct temporal and spatial patterns. Infection with C. parvum can induce mastocytosis in the entire small intestinal mucosa in immune-competent calves, and the presence of the parasites influences the distribution profile of the mast cells.
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Chatrchyan S, Khachatryan V, Sirunyan AM, Tumasyan A, Adam W, Aguilo E, Bergauer T, Dragicevic M, Erö J, Fabjan C, Friedl M, Frühwirth R, Ghete VM, Hammer J, Hörmann N, Hrubec J, Jeitler M, Kiesenhofer W, Knünz V, Krammer M, Krätschmer I, Liko D, Mikulec I, Pernicka M, Rahbaran B, Rohringer C, Rohringer H, Schöfbeck R, Strauss J, Taurok A, Waltenberger W, Walzel G, Widl E, Wulz CE, Mossolov V, Shumeiko N, Suarez Gonzalez J, Bansal S, Cornelis T, De Wolf EA, Janssen X, Luyckx S, Mucibello L, Ochesanu S, Roland B, Rougny R, Selvaggi M, Staykova Z, Van Haevermaet H, Van Mechelen P, Van Remortel N, Van Spilbeeck A, Blekman F, Blyweert S, D'Hondt J, Gonzalez Suarez R, Kalogeropoulos A, Maes M, Olbrechts A, Van Doninck W, Van Mulders P, Van Onsem GP, Villella I, Clerbaux B, De Lentdecker G, Dero V, Gay APR, Hreus T, Léonard A, Marage PE, Reis T, Thomas L, Vander Marcken G, Vander Velde C, Vanlaer P, Wang J, Adler V, Beernaert K, Cimmino A, Costantini S, Garcia G, Grunewald M, Klein B, 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Wickramage N, Banerjee S, Dugad S, Arfaei H, Bakhshiansohi H, Etesami SM, Fahim A, Hashemi M, Hesari H, Jafari A, Khakzad M, Mohammadi Najafabadi M, Paktinat Mehdiabadi S, Safarzadeh B, Zeinali M, Abbrescia M, Barbone L, Calabria C, Chhibra SS, Colaleo A, Creanza D, De Filippis N, De Palma M, Fiore L, Iaselli G, Lusito L, Maggi G, Maggi M, Marangelli B, My S, Nuzzo S, Pacifico N, Pompili A, Pugliese G, Selvaggi G, Silvestris L, Singh G, Venditti R, Zito G, Abbiendi G, Benvenuti AC, Bonacorsi D, Braibant-Giacomelli S, Brigliadori L, Capiluppi P, Castro A, Cavallo FR, Cuffiani M, Dallavalle GM, Fabbri F, Fanfani A, Fasanella D, Giacomelli P, Grandi C, Guiducci L, Marcellini S, Masetti G, Meneghelli M, Montanari A, Navarria FL, Odorici F, Perrotta A, Primavera F, Rossi AM, Rovelli T, Siroli G, Travaglini R, Albergo S, Cappello G, Chiorboli M, Costa S, Potenza R, Tricomi A, Tuve C, Barbagli G, Ciulli V, Civinini C, D'Alessandro R, Focardi E, Frosali S, Gallo E, Gonzi S, Meschini M, 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Roe J, Safonov A, Sakuma T, Sengupta S, Suarez I, Tatarinov A, Toback D, Akchurin N, Damgov J, Dudero PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Roh Y, Volobouev I, Appelt E, Delannoy AG, Florez C, Greene S, Gurrola A, Johns W, Johnston C, Kurt P, Maguire C, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Yohay R, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sakharov A, Anderson M, Bachtis M, Belknap D, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Gray L, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Leonard J, Loveless R, Mohapatra A, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Measurement of the azimuthal anisotropy of neutral pions in Pb-Pb collisions at sqrt[s](NN)] = 2.76 TeV. PHYSICAL REVIEW LETTERS 2013; 110:042301. [PMID: 25166155 DOI: 10.1103/physrevlett.110.042301] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/12/2012] [Indexed: 06/03/2023]
Abstract
First measurements of the azimuthal anisotropy of neutral pions produced in Pb-Pb collisions at a center-of-mass energy of sqrt[s(NN)] = 2.76 TeV are presented. The amplitudes of the second Fourier component (v(2)) of the π(0) azimuthal distributions are extracted using an event-plane technique. The values of v(2) are studied as a function of the neutral pion transverse momentum (p(T)) for different classes of collision centrality in the kinematic range 1.6<p(T) <8.0 GeV/c, within the pseudorapidity interval |η|<0.8. The CMS measurements of v(2) (p(T)) are similar to previously reported π(0) azimuthal anisotropy results from sqrt[s(NN)] = 200 GeV Au-Au collisions at RHIC, despite a factor of ∼ 14 increase in the center-of-mass energy. In the momentum range 2.5<p(T)<5.0 GeV/c, the neutral pion anisotropies are found to be smaller than those observed by CMS for inclusive charged particles.
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Berryhill J, Bhat PC, Bloch I, Burkett K, Butler JN, Chetluru V, Cheung HWK, Chlebana F, Elvira VD, Fisk I, Freeman J, Gao Y, Green D, Gutsche O, Hanlon J, Harris RM, Hirschauer J, Hooberman B, Jindariani S, Johnson M, Joshi U, Kilminster B, Klima B, Kunori S, Kwan S, Leonidopoulos C, Linacre J, Lincoln D, Lipton R, Lykken J, Maeshima K, Marraffino JM, Maruyama S, Mason D, McBride P, Mishra K, Mrenna S, Musienko Y, Newman-Holmes C, O'Dell V, Prokofyev O, Sexton-Kennedy E, Sharma S, Spalding WJ, Spiegel L, Taylor L, Tkaczyk S, Tran NV, Uplegger L, Vaandering EW, Vidal R, Whitmore J, Wu W, Yang F, Yumiceva F, Yun JC, Acosta D, Avery P, Bourilkov D, Chen M, Cheng T, Das S, De Gruttola M, Di Giovanni GP, Dobur D, Drozdetskiy A, Field RD, Fisher M, Fu Y, Furic IK, Gartner J, Hugon J, Kim B, Konigsberg J, Korytov A, Kropivnitskaya A, Kypreos T, Low JF, Matchev K, Milenovic P, Mitselmakher G, Muniz L, Park M, Remington R, Rinkevicius A, Sellers P, Skhirtladze N, Snowball M, Yelton J, Zakaria 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Safonov A, Sakuma T, Sengupta S, Suarez I, Tatarinov A, Toback D, Akchurin N, Damgov J, Dragoiu C, Dudero PR, Jeong C, Kovitanggoon K, Lee SW, Libeiro T, Roh Y, Volobouev I, Appelt E, Delannoy AG, Florez C, Greene S, Gurrola A, Johns W, Kurt P, Maguire C, Melo A, Sharma M, Sheldon P, Snook B, Tuo S, Velkovska J, Arenton MW, Balazs M, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Lin C, Neu C, Wood J, Gollapinni S, Harr R, Karchin PE, Kottachchi Kankanamge Don C, Lamichhane P, Sakharov A, Anderson M, Belknap D, Borrello L, Carlsmith D, Cepeda M, Dasu S, Friis E, Gray L, Grogg KS, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Klukas J, Lanaro A, Lazaridis C, Leonard J, Loveless R, Mohapatra A, Ojalvo I, Palmonari F, Pierro GA, Ross I, Savin A, Smith WH, Swanson J. Evidence for associated production of a single top quark and W boson in pp collisions at sqrt[s]=7 TeV. PHYSICAL REVIEW LETTERS 2013; 110:022003. [PMID: 23383893 DOI: 10.1103/physrevlett.110.022003] [Citation(s) in RCA: 10] [Impact Index Per Article: 0.9] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/16/2012] [Indexed: 06/01/2023]
Abstract
Evidence is presented for the associated production of a single top quark and W boson in pp collisions at sqrt[s]=7 TeV with the CMS experiment at the LHC. The analyzed data correspond to an integrated luminosity of 4.9 fb(-1). The measurement is performed using events with two leptons and a jet originated from a b quark. A multivariate analysis based on kinematic properties is utilized to separate the tt background from the signal. The observed signal has a significance of 4.0σ and corresponds to a cross section of 16(-4)(+5) pb, in agreement with the standard model expectation of 15.6±0.4(-1.2)(+1.0) pb.
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Song S, Huo J, Li D, Yuan Y, Yuan F, Miao Y. Molecular cloning, sequence characterization, and gene expression profiling of a novel water buffalo (Bubalus bubalis) gene, AGPAT6. GENETICS AND MOLECULAR RESEARCH 2013; 12:4116-26. [DOI: 10.4238/2013.october.1.2] [Citation(s) in RCA: 8] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/03/2022]
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Search for heavy neutrinos and W(R) bosons with right-handed couplings in a left-right symmetric model in pp collisions at sqrt[s]=7 TeV. PHYSICAL REVIEW LETTERS 2012; 109:261802. [PMID: 23368549 DOI: 10.1103/physrevlett.109.261802] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/08/2012] [Indexed: 06/01/2023]
Abstract
Results are presented from a search for heavy, right-handed muon neutrinos, N(μ), and right-handed W(R) bosons, which arise in the left-right symmetric extensions of the standard model. The analysis is based on a 5.0 fb(-1) sample of proton-proton collisions at a center-of-mass energy of 7 TeV, collected by the CMS detector at the Large Hadron Collider. No evidence is observed for an excess of events over the standard model expectation. For models with exact left-right symmetry, heavy right-handed neutrinos are excluded at 95% confidence level for a range of neutrino masses below the W(R) mass, dependent on the value of M(W(R)). The excluded region in the two-dimensional (M(W(R)), M(N(μ)) mass plane extends to M(W(R))=2.5 TeV.
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