830 research outputs found
Optimizing Combination Therapies with Existing and Future CML Drugs
- Author
- A Gontarewicz
- A Gontarewicz
- A Quintas-Cardama
- AA Katouli
- AJ Coldman
- AJ Coldman
- Allen A. Katouli
- AS Shet
- B Calabretta
- BJ Druker
- BJ Druker
- C Yoshida
- CB Gambacorti-Passerini
- E Weisberg
- E Weisberg
- EA Gaffney
- EA Gaffney
- F Michor
- FJ Giles
- G Noronha
- H Daub
- H Kantarjian
- HA Bradeen
- HM Byrne
- I Roeder
- J Zhang
- JF Apperley
- JH Goldie
- JH Goldie
- JH Goldie
- JP Jaffrezou
- JV Melo
- KM Shannon
- L Cojocaru
- LE Harnevo
- LE Harnevo
- LG de Pillis
- M Kimmel
- M Kimmel
- M Loriaux
- M Modugno
- M Talpaz
- MW Deininger
- MW Deininger
- N Komarova
- N Vajpai
- Natalia L. Komarova
- NL Komarova
- NL Komarova
- NL Komarova
- NL Komarova
- O Hantschel
- RB Cohen
- RG McKinnell
- Roger Chammas
- S Branford
- S Redaelli
- SH Moolgavkar
- SH Moolgavkar
- SH Moolgavkar
- SN Gardner
- T O'Hare
- T O'Hare
- T Zhou
- TL Jackson
- U Rix
- V Nardi
- WC Moloney
- WS Kendal
- Y Deguchi
- Y Xie
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Small-molecule inhibitors imatinib, dasatinib and nilotinib have been developed to treat Chromic Myeloid Leukemia (CML). The existence of a triple-cross-resistant mutation, T315I, has been a challenging problem, which can be overcome by finding new inhibitors. Many new compounds active against T315I mutants are now at different stages of development. In this paper we develop an algorithm which can weigh different combination treatment protocols according to their cross-resistance properties, and find the protocols with the highest probability of treatment success. This algorithm also takes into account drug toxicity by minimizing the number of drugs used, and their concentration. Although our methodology is based on a stochastic model of CML microevolution, the algorithm itself does not require measurements of any parameters (such as mutation rates, or division/death rates of cells), and can be used by medical professionals without a mathematical background. For illustration, we apply this algorithm to the mutation data obtained in [1], [2]
454 sequencing of pooled BAC clones on chromosome 3H of barley
- Author
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Genome sequencing of barley has been delayed due to its large genome size (ca. 5,000Mbp). Among the fast sequencing systems, 454 liquid phase pyrosequencing provides the longest reads and is the most promising method for BAC clones. Here we report the results of pooled sequencing of BAC clones selected with ESTs genetically mapped to chromosome 3H.</p> <p>Results</p> <p>We sequenced pooled barley BAC clones using a 454 parallel genome sequencer. A PCR screening system based on primer sets derived from genetically mapped ESTs on chromosome 3H was used for clone selection in a BAC library developed from cultivar "Haruna Nijo". The DNA samples of 10 or 20 BAC clones were pooled and used for shotgun library development. The homology between contig sequences generated in each pooled library and mapped EST sequences was studied. The number of contigs assigned on chromosome 3H was 372. Their lengths ranged from 1,230 bp to 58,322 bp with an average 14,891 bp. Of these contigs, 240 showed homology and colinearity with the genome sequence of rice chromosome 1. A contig annotation browser supplemented with query search by unique sequence or genetic map position was developed. The identified contigs can be annotated with barley cDNAs and reference sequences on the browser. Homology analysis of these contigs with rice genes indicated that 1,239 rice genes can be assigned to barley contigs by the simple comparison of sequence lengths in both species. Of these genes, 492 are assigned to rice chromosome 1.</p> <p>Conclusions</p> <p>We demonstrate the efficiency of sequencing gene rich regions from barley chromosome 3H, with special reference to syntenic relationships with rice chromosome 1.</p
The search for transient astrophysical neutrino emission with IceCube-DeepCore
- Author
- Aartsen MG
- Abraham K
- Ackermann M
- Adams J
- Aguilar JA
- Ahlers M
- Ahrens M
- Altmann D
- Anderson T
- Ansseaus I
- Archinger M
- Arguelles C
- Arlen TC
- Auffenberg J
- Bai X
- Barwick SW
- Baum V
- Bay R
- Beatty JJ
- Becker K-H
- Beiser E
- Benzvi S
- Berghaus P
- Berley D
- Bernardini E
- Bernhard A
- Besson DZ
- Binder G
- Bindig D
- Bissoki M
- Blaufuss E
- Blumenthal J
- Boerner M
- Boersma DJ
- Boeser S
- Bohm C
- Bos F
- Bose D
- Botner O
- Braun J
- Brayeur L
- Bretz H-P
- Buzinsky N
- Casey J
- Casier M
- Cheung E
- Chirkin D
- Christov A
- Clark K
- Classen L
- Coenders S
- Cowen DF
- Daughhetee J
- Davis JC
- Day M
- de Andre JPAM
- De Clercq C
- De Ridder S
- de Vries KD
- de Wasseige G
- de With M
- del Pino Rosendo E
- Dembinski H
- Desiati P
- DeYoung T
- di Lorenzo V
- Diaz-Velez JC
- Dumm JP
- Dunkman M
- Eagan R
- Eberhardt B
- Ehrhardt T
- Eichmann B
- Euler S
- Evenson PA
- Fadiran O
- Fahey S
- Fazely AR
- Fedynitch A
- Feintzeig J
- Felde J
- Filimonov K
- Finley C
- Fischer-Wasels T
- Flis S
- Foesig C-C
- Fucus T
- Gaior R
- Gaisser TK
- Gallagher J
- Gerhardt L
- Ghorbani K
- Gier D
- Gladstone L
- Glagla M
- Gluesenkamp T
- Goldschmidt A
- Golup G
- Gonzalez JG
- Gora D
- Grant D
- Groii JC
- Gross A
- Ha C
- Haack C
- Hallgren A
- Halzen F
- Hansen E
- Hansmann B
- Hanson K
- Hebecker D
- Heereman D
- Helbing K
- Hellauer R
- Hickford S
- Hignigiit J
- Hill GC
- Hoffman KD
- Hoffmann R
- Holzapfel K
- Homeier A
- Hoshina K
- Huang F
- Huber M
- Huelsnitz W
- Hulth PO
- Hultqvist K
- IceCube Collaboration
- In S
- Ishihara A
- Ismail AH
- Jacobi E
- Japaridze GS
- Jero K
- Jurkovic M
- Kappes A
- Karg T
- Karle A
- Kauer M
- Keivani A
- Kelley JL
- Kemp J
- Kheirandish A
- Kiryluk J
- Klaes J
- Klein SR
- Koepke L
- Kohnen G
- Koirala R
- Kolanoski H
- Konietz R
- Kopper C
- Kopper S
- Koskinen DJ
- Kowalski M
- Krings K
- Kroll G
- Kroll M
- Kunnen J
- Kurahashi N
- Kuwabara T
- Labare M
- Lanfranchi JL
- Larson MJ
- Lesiak-Bzdak M
- Leuermann M
- Leuner J
- Lu L
- Lunemann J
- Madsen J
- Maggi G
- Mahn KBM
- Maruyama R
- Mase K
- Matis HS
- Maunu R
- McNally F
- Meagher K
- Medici M
- Meli A
- Menne T
- Merino G
- Meuress T
- Miarecki S
- Middell E
- Middlemas E
- Mohrmann L
- Montaruli T
- Morse R
- Nahnhauer R
- Naumann U
- Neer G
- Niederhausen H
- Nowicki SC
- Nygren DR
- O'Murchadha A
- Obertacke A
- Olivas A
- Omairat A
- Palczewski T
- Pandya H
- Pankova DV
- Paul L
- Pepper JA
- Perez de los Heros C
- Pfendner C
- Pieloth D
- Pinat E
- Posselt J
- Price PB
- Przybylski GT
- Puetz J
- Quinnan M
- Raab C
- Raedel L
- Rameez M
- Rawlins K
- Reimann R
- Relich M
- Resconi E
- Rhode W
- Richman M
- Richter S
- Riedel B
- Robertson S
- Rongen M
- Rott C
- Ruhe T
- Ryckbosch D
- Saba SM
- Sabbatini L
- Sander H-G
- Sandrock A
- Sandroos J
- Sarkar Subir
- Schatto K
- Scheriau F
- Schimp M
- Schmidt T
- Schmitz M
- Schoeneberg S
- Schoenen S
- Schoenwald A
- Schulte L
- Seckel D
- Seunarine S
- Silva AHC
- Smith MWE
- Soldin D
- Song M
- Spiczak GM
- Spiering C
- Stahlberg M
- Stamatikos M
- Stanev T
- Stanisha NA
- Stasik A
- Stezelberger T
- Stoessl A
- Stokstad RG
- Strom R
- Strotjohann NL
- Sullivan GW
- Sutherland M
- Taavola H
- Taboada I
- Tatar J
- Ter-Antonyan S
- Terliuk A
- Tesic G
- Tilav S
- Tjus JB
- Toale PA
- Tobin MN
- Toscano S
- Tosi D
- Tselengidou M
- Turcati A
- Unger E
- Usner M
- Vallecorsa S
- van Eundhoven N
- van Santen J
- Vandenbroucke J
- Vanheule S
- Veenkamp J
- Vehring M
- Voge M
- Vraeghe M
- Walck C
- Wallace A
- Wallraff M
- Wandkowsky N
- Weaver C
- Wendt C
- Westerhoff S
- Whelan BJ
- Whitehorn N
- Wiebe K
- Wiebusch CH
- Wille L
- Williams DR
- Wissing H
- Wolf M
- Wood TR
- Woschnagg K
- Xu DL
- Xu XW
- Xu Y
- Yanez JP
- Yodh G
- Yoshida S
- Zoll M
- Publication venue
- Publication date
- 04/12/2015
- Field of study
We present the results of a search for astrophysical sources of brief transient neutrino emission using IceCube and DeepCore data acquired between 2012 May 15 and 2013 April 30. While the search methods employed in this analysis are similar to those used in previous IceCube point source searches, the data set being examined consists of a sample of predominantly sub-TeV muon-neutrinos from the Northern Sky (-5 degrees < delta < 90 degrees) obtained through a novel event selection method. This search represents a first attempt by IceCube to identify astrophysical neutrino sources in this relatively unexplored energy range. The reconstructed direction and time of arrival of neutrino events are used to search for any significant self-correlation in the data set. The data revealed no significant source of transient neutrino emission. This result has been used to construct limits at timescales ranging from roughly 1 s to 10 days for generic soft-spectra transients. We also present limits on a specific model of neutrino emission from soft jets in core-collapse supernovae
Combination of Two but Not Three Current Targeted Drugs Can Improve Therapy of Chronic Myeloid Leukemia
- Author
- A Quintas-Cardama
- AJ Coldman
- Allen A. Katouli
- AS Shet
- B Calabretta
- BJ Druker
- BJ Druker
- C Yoshida
- Cathal Seoighe
- CB Gambacorti-Passerini
- Dominik Wodarz
- E Weisberg
- EA Duncan
- EA Harrington
- GQ Daley
- H Daub
- HA Bradeen
- JH Goldie
- JH Goldie
- JV Melo
- JV Melo
- KM Shannon
- M Talpaz
- MA Young
- ME Gorre
- ME O'Dwyer
- MS Wicha
- MW Deininger
- MW Deininger
- Natalia L. Komarova
- NL Komarova
- NP Shah
- RM Ribeiro
- SK Burley
- T O'Hare
- T Reya
- TA Carter
- V Nardi
- Publication venue
- Public Library of Science
- Publication date
- 10/02/2009
- Field of study
Chronic myeloid leukemia (CML) is a cancer of the hematopoietic system and has been treated with the drug Imatinib relatively successfully. Drug resistance, acquired by mutations, is an obstacle to success. Two additional drugs are now considered and could be combined with Imatinib to prevent resistance, Dasatinib and Nilotinib. While most mutations conferring resistance to one drug do not confer resistance to the other drugs, there is one mutation (T315I) that induces resistance against all three drugs. Using computational methods, the combination of two drugs is found to increase the probability of treatment success despite this cross-resistance. Combining more than two drugs, however, does not provide further advantages. We also explore possible combination therapies using drugs currently under development. We conclude that among the targeted drugs currently available for the treamtent of CML, only the two most effective ones should be used in combination for the prevention of drug resistance
Observation and study of baryonic B decays: B -> D(*) p pbar, D(*) p pbar pi, and D(*) p pbar pi pi
- Author
- Adametz A
- Adye T
- Ahmed S
- Ahmed S
- Alam MS
- Alam MS
- Albert J
- Albert J
- Allen MT
- Alwyn KE
- Anderson J
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Ayad R
- Azzolini V
- Bailey D
- Baldini-Ferroli R
- Band HR
- Band HR
- Banerjee S
- Banerjee S
- Baracchini E
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Battaglia M
- Behera PK
- Bellis M
- Ben-Haim E
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bhuyan B
- Bianchi F
- Bianchi F
- Biasini M
- Biassoni P
- Bingham I
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bomben M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Bozzi C
- Brau J
- Briand H
- Brown DN
- Brown DN
- Bula R
- Burchat PR
- Burchat PR
- Buzykaev AR
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Cartaro C
- Cartaro C
- Casarosa G
- Castelli G
- Cavoto G
- Cecchi A
- Cenci R
- Cervelli A
- Chauveau J
- Chavez CA
- Chen C
- Chen X
- Chen XR
- Cheng CH
- Choi HHF
- Cibinetto G
- Clark PJ
- Cochranz J
- Coleman JP
- Contri R
- Convery MR
- Corwin LA
- Cossutti F
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Curry S
- da Costa JF
- Dallapiccola C
- Dasu S
- Dasu S
- Dauncey PD
- Davier M
- Davis CL
- de Monchenault GH
- De Nardo G
- de Sangro R
- Della Ricca G
- Denig AG
- Derkach D
- Di Lodovico F
- Doll DA
- Dong L
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dubrovin MS
- Dujmic D
- Dunwoodie W
- Ebert M
- Echenard B
- Eckmann R
- Eckmann R
- Edwards AJ
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Ernst JA
- Faccini R
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fioravanti E
- Flanigan JM
- Flood KT
- Flood KT
- Ford WT
- Forti F
- Franchini P
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Gallo F
- Gamba D
- Gamba D
- Gamet R
- Gary JW
- Gaspero M
- Gaz A
- Gershon TJ
- Gioi LL
- Giorgi MA
- Godang R
- Golubev VB
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Gritsan AV
- Grosdidier G
- Guido E
- Guo ZJ
- Guttman N
- Hafner A
- Hamano K
- Hamano K
- Hamon O
- Harrison PF
- Harrison PF
- Hartmann T
- Hast C
- Hawkes CM
- Hearty C
- Heusch CA
- Hitlin DG
- Hollar JJ
- Hong TM
- Honscheid K
- Hooberman B
- Hutchcroft DE
- Igonkina O
- Ilic J
- Innes WR
- Izen JM
- Izen JM
- Jackson G
- Jain V
- Jasper H
- Jawahery A
- Jessop CP
- Karbach TM
- Kass R
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- Kim P
- King GJ
- Kirkby D
- Knoepfel KJ
- Kobel MJ
- Koch H
- Kocian ML
- Kocian ML
- Kolb JA
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kowalewski R
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kutter PE
- Lacker HM
- Lafferty GD
- Lanceri L
- Lanceri L
- Lange DJ
- Lankford AJ
- Latham TE
- Latham TE
- Lazzaro A
- Le Diberder F
- Leddig T
- Lee CL
- Lees JP
- Leith DWGS
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Li S
- Li S
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Lombardo V
- Long O
- Lopez-March N
- Lopez-March N
- LoSecco JM
- Lou XC
- Lou XC
- Lu C
- Lueck T
- Luitz S
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- Lynch HL
- MacFarlane DB
- MacFarlane DB
- Majewski SA
- Malaescu B
- Mallik U
- Mancinelli G
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Marks J
- Marsiske H
- Marsiske H
- Martin EC
- Martinelli M
- Martinez AJ
- Martinez-Vidal F
- Martinez-Vidal F
- Mattison TS
- Mazzoni MA
- McKenna JA
- Meadows BT
- Merkel J
- Messner R
- Meyer WT
- Milanes DA
- Milanes DA
- Miyashita TS
- Miyashita TS
- Mohanty GB
- Monge MR
- Monorchio D
- Morandin M
- Morii M
- Morris JP
- Muller DR
- Muller DR
- Munerato M
- Nagel M
- Nauenberg U
- Neal H
- Neal H
- Negrini M
- Nelson S
- Neri N
- Nguyen X
- Nicolaci M
- Nugent IM
- Nugent IM
- O'Grady CP
- O'Grady CP
- Ocariz J
- Ofte I
- Ofte I
- Olaiya EO
- Olsen J
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Osipenkov IL
- Oyanguren A
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan B
- Pan B
- Pan Y
- Pan Y
- Paoloni E
- Pappagallo M
- Paramesvaran S
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Pelliccioni M
- Pelliccioni M
- Perazzo A
- Perez A
- Perl M
- Perl M
- Peruzzi IM
- Petersen BA
- Petrella A
- Petzold A
- Piccolo M
- Piemontese L
- Pierini M
- Piredda G
- Playfer S
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prendki J
- Prepost R
- Prepost R
- Puccio EMT
- Pulliam T
- Pulliam T
- Purohit MV
- Rahmat R
- Rakitin AY
- Rama M
- Randle-Conde A
- Ratcliff BN
- Ratcliff BN
- Raven G
- Renga F
- Richman JD
- Ritchie JL
- Ritchie JL
- Rizzo G
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roney JM
- Roodman A
- Roodman A
- Rosenberg EI
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
- Ruland AM
- Sacco R
- Saeed MA
- Saeed MA
- Salnikov AA
- Salnikov AA
- Salvati E
- Sanchez PDA
- Santoro V
- Schalk T
- Schilling CJ
- Schilling CJ
- Schindler RH
- Schindler RH
- Schram M
- Schroeder H
- Schroeder T
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwiening J
- Schwierz R
- Schwitters RF
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Serrano J
- Sevilla MF
- Sigamani M
- Simard M
- Simi G
- Simonetto F
- Sinev NB
- Sitt S
- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
- Snyder A
- Snyder A
- Sobie RJ
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Sordini V
- Spaan B
- Spanier SM
- Spanier SM
- Stocchi A
- Stoker DP
- Stracka S
- Stroili R
- Strom D
- Strube J
- Stugu B
- Su D
- Su D
- Sullivan MK
- Sullivan MK
- Summers DJ
- Sun L
- Sun S
- Suzuki K
- Suzuki K
- Swain SK
- Tanabe T
- Taras P
- Telnov AV
- Thompson JM
- Thompson JM
- Tibbetts M
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
- Tosi S
- Touramanis C
- Tuggle JM
- Uwer U
- Va'vra J
- Va'vra J
- Vasseur G
- Verderi M
- Vitale L
- Vitale L
- Vitug GM
- Volk A
- Vuosalo CO
- Wacker K
- Wagner AP
- Wagner AP
- Wagner SR
- Waldi R
- Walsh JJ
- Wang L
- Wang WF
- Wappler FR
- Watson AT
- Watson JE
- Weaver M
- Weaver M
- West C
- West CA
- White RM
- Wilden L
- Wilson FF
- Wilson JR
- Wilson P
- Winer BL
- Winstrom LO
- Wisniewski WJ
- Wisniewski WJ
- Wittgen M
- Wittgen M
- Wittich P
- Wolbers S
- Wolfe H
- Wormser G
- Wray BC
- Wren AC
- Wright DH
- Wright DH
- Wright DM
- Wright T
- Wu SL
- Wu SL
- Wu X
- Wu Z
- Wulsin HW
- Yamamoto K
- Yamato D
- Yang T
- Yang UK
- Yang YC
- Yao WM
- Yarritu AK
- Yarritu AK
- Ye S
- Yeche C
- Yeh GP
- Yi K
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Yushkov AN
- Zain SB
- Zain SB
- Zallo A
- Zanetti A
- Zeng Y
- Zhao M
- Zhou C
- Ziegler V
- Ziegler V
- Zito M
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 15/08/2009
- Field of study
We present a study of ten B-meson decays to a D(*), a proton-antiproton pair,
and a system of up to two pions using BaBar's data set of 455x10^6 BBbar pairs.
Four of the modes (B0bar -> D0 p anti-p, B0bar -> D*0 p anti-p, B0bar -> D+ p
anti-p pi-, B0bar -> D*+ p anti-p pi-) are studied with improved statistics
compared to previous measurements; six of the modes (B- -> D0 p anti-p pi-, B-
-> D*0 p anti-p pi-, B0bar -> D0 p anti-p pi- pi+, B0bar -> D*0 p anti-p pi-
pi+, B- -> D+ p anti-p pi- pi-, B- -> D*+ p anti-p pi- pi-) are first
observations. The branching fractions for 3- and 5-body decays are suppressed
compared to 4-body decays. Kinematic distributions for 3-body decays show
non-overlapping threshold enhancements in m(p anti-p) and m(D(*)0 p) in the
Dalitz plots. For 4-body decays, m(p pi-) mass projections show a narrow peak
with mass and full width of (1497.4 +- 3.0 +- 0.9) MeV/c2, and (47 +- 12 +- 4)
MeV/c2, respectively, where the first (second) errors are statistical
(systematic). For 5-body decays, mass projections are similar to phase space
expectations. All results are preliminary.Comment: 28 pages, 90 postscript figures, submitted to LP0
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
- Author
- A.
- A.
- A.
- A.
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- A.F.
- A.T.
- A.T.
- A.V.
- Aaltonen
- Alvarez González
- Amerio
- Amidei
- Anastassov
- Annovi
- Antos
- Apollinari
- Appel
- Arisawa
- Artikov
- Asaadi
- Ashmanskas
- Auerbach
- Aurisano
- Azfar
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- B.L.
- Badgett
- Bae
- Barbaro-Galtieri
- Barnes
- Barnett
- Barria
- Bartos
- Bauce
- Bedeschi
- Behari
- Bellettini
- Bellinger
- Benjamin
- Beretvas
- Bhatti
- Bisello
- Bizjak
- Bland
- Blumenfeld
- Bocci
- Bodek
- Bortoletto
- Boudreau
- Boveia
- Brigliadori
- Bromberg
- Brucken
- Budagov
- Budd
- Burkett
- Busetto
- Bussey
- Buzatu
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- Calamba
- Calancha
- Camarda
- Campanelli
- Campbell
- Canelli
- Carls
- Carlsmith
- Carosi
- Carrillo
- Carron
- Casal
- Casarsa
- Castro
- Catastini
- Cauz
- Cavaliere
- Cavalli-Sforza
- Cerri
- Cerrito
- Chen
- Chertok
- Chiarelli
- Chlachidze
- Chlebana
- Cho
- Chokheli
- Chung
- Chung
- Ciocci
- Clark
- Clarke
- Compostella
- Convery
- Conway
- Corbo
- Cordelli
- Cox
- Cox
- Crescioli
- Cuevas
- Culbertson
- D'ascenzo
- D'errico
- D'Onofrio
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- Dagenhart
- Datta
- De Barbaro
- Dell'orso
- Demortier
- Deninno
- Devoto
- Di Canto
- Di Ruzza
- Dittmann
- Donati S
- Dong
- Dorigo
- Dorigo
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- Ebina
- Elagin
- Eppig
- Erbacher
- Errede
- Ershaidat
- Eusebi
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- Farrington
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- Freeman
- Funakoshi
- Furic
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- Gallinaro
- Garcia
- Garfinkel
- Garosi
- Gerberich
- Gerchtein
- Giagu
- Giakoumopoulou
- Giannetti
- Gibson
- Ginsburg
- Giokaris
- Giromini
- Giurgiu
- Glagolev
- Glenzinski
- Gold
- Goldin
- Goldschmidt
- Golossanov
- Gomez
- Gomez-Ceballos
- Goncharov
- González
- Gorelov
- Goshaw
- Goulianos
- Grillo
- Grinstein
- Grosso-Pilcher
- Group
- Guimaraes Da Costa
- H.
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- H.S.
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- Hahn
- Halkiadakis
- Hamaguchi
- Han
- Happacher
- Hara
- Hare
- Hare
- Harr
- Hatakeyama
- Hays
- Heck
- Heinrich
- Herndon
- Hewamanage
- Hocker
- Hopkins
- Horn
- Hou
- Hughes
- Hurwitz
- Husemann
- Hussain
- Hussein
- Huston
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- Ivanov
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- J.Y.
- James
- Jang
- Jayatilaka
- Jeon
- Jindariani
- Jones
- Joo
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- Karchin
- Kasmi
- Kato
- Ketchum
- Keung
- Khotilovich
- Kilminster
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- Kimura
- Kirby
- Klimenko
- Knoepfel
- Koh YH
- Koike M
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- Kondo
- Kong
- Kong HJ
- Kong WJ
- Konigsberg
- Korolchuk VI
- Kotake Y
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- Kouri Flores JB
- Kovács AL
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- Trovato
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- Tyagi SC
- Tönges L
- U.
- U.K.
- Uchiyama Y
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- Umekawa M
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- Uozumi
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- V.E.
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- Volpi
- Vázquez
- W.
- W.
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- W.
- W.-M.
- W.C.
- W.H.
- W.K.
- Wagner
- Wagner
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- Wallny
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- Warburton
- Waters
- Wester
- Whiteson
- Wick
- Wicklund
- Wicklund
- Wilbur
- Williams
- Wilson
- Wilson
- Winer
- Wittich
- Wolbers
- Wolfe
- Wright
- Wu
- Wu
- X.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.C.
- Y.C.
- Y.D.
- Y.J.
- Y.K.
- Y.S.
- Yamamoto
- Yamato
- Yang
- Yang
- Yang
- Yao
- Yeh
- Yi
- Yoh
- Yorita
- Yoshida
- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
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- Abajyan T
- Abbott B
- Abdallah J
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- Abramowicz H
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- Allbrooke BMM
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
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- Zobernig G
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- zur Nedden M
- Zutshi V
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
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- Youssef S
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- Zaidan R
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- Zanello L
- Zanzi D
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- Zemla A
- Zengel K
- Zenin O
- Zenis T
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- Zhemchugov A
- Zhong J
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
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