512 research outputs found
Frequency-dependent parameterized macromodeling of integrated inductors
- Publication venue
- Publication date
- 01/01/2016
- Field of study
Intravenous leiomyomatosis of the uterus with extension to the right heart
- Author
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
A 42-year-old woman admitted with debilitation and engorgement both lower extremities. Transthoracic two-dimensional echocardiography, abdominal ultrasound and computerized tomography revealed a lobulated pelvic mass, a mass within right internal iliac vein, both common iliac vein, as well as the inferior vena cava, extending into the right atrium. In addition, echocardiography and abdominal ultrasound showed the tumor of right atrium and inferior vena cave has no stalk and has well-demarcated borders with the wall of right atrium and inferior vena cave. Hence, the presumptive diagnosis of IVL was made by echocardiography and abdominal ultrasound and the presumptive diagnosis of sarcoma with invasion in right internal iliac vein, both common iliac vein, the inferior vena cava, as well as the right atrium was made by multi-detector-row computerized tomography. The patient underwent a one-stage combined multidisciplinary thoraco-abdominal operation under general anaesthetic. Subsequently the pathologic report confirmed IVL
Green-to-red photoconvertible fluorescent proteins: tracking cell and protein dynamics on standard wide-field mercury arc-based microscopes
- Author
- A Muller-Taubenberger
- DM Chudakov
- DM Chudakov
- DM Chudakov
- DW Piston
- FF Bukauskas
- FV Subach
- G Gaietta
- K Jordan
- KA Lukyanov
- L Zhang
- M Falk
- M Mavrakis
- M Piehl
- MA Beardslee
- Matthias M Falk
- MM Falk
- MM Falk
- MM Falk
- NC Shaner
- NG Gurskaya
- P Lopez
- RF Fallon
- Robert W Buckheit
- S Habuchi
- S Nowotschin
- SA McKinney
- Susan M Baker
- U Lauf
- U Lauf
- VM Berthoud
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>Green fluorescent protein (GFP) and other FP fusions have been extensively utilized to track protein dynamics in living cells. Recently, development of photoactivatable, photoswitchable and photoconvertible fluorescent proteins (PAFPs) has made it possible to investigate the fate of discrete subpopulations of tagged proteins. Initial limitations to their use (due to their tetrameric nature) were overcome when monomeric variants, such as Dendra, mEos, and mKikGR were cloned/engineered.</p> <p>Results</p> <p>Here, we report that by closing the field diaphragm, selective, precise and irreversible green-to-red photoconversion (330-380 nm illumination) of discrete subcellular protein pools was achieved on a wide-field fluorescence microscope equipped with standard DAPI, Fluorescein, and Rhodamine filter sets and mercury arc illumination within 5-10 seconds. Use of a DAPI-filter cube with long-pass emission filter (LP420) allowed the observation and control of the photoconversion process in real time. Following photoconversion, living cells were imaged for up to 5 hours often without detectable phototoxicity or photobleaching.</p> <p>Conclusions</p> <p>We demonstrate the practicability of this technique using Dendra2 and mEos2 as monomeric, photoconvertible PAFP representatives fused to proteins with low (histone H2B), medium (gap junction channel protein connexin 43), and high (α-tubulin; clathrin light chain) dynamic cellular mobility as examples. Comparable efficient, irreversible green-to-red photoconversion of selected portions of cell nuclei, gap junctions, microtubules and clathrin-coated vesicles was achieved. Tracking over time allowed elucidation of the dynamic live-cycle of these subcellular structures. The advantage of this technique is that it can be performed on a standard, relatively inexpensive wide-field fluorescence microscope with mercury arc illumination. Together with previously described laser scanning confocal microscope-based photoconversion methods, this technique promises to further increase the general usability of photoconvertible PAFPs to track the dynamic movement of cells and proteins over time.</p
A genetic algorithm-Bayesian network approach for the analysis of metabolomics and spectroscopic data: application to the rapid detection of Bacillus spores and identification of Bacillus species
- Author
- A Atrih
- AD Warth
- AP Snyder
- CD Havey
- D Heckerman
- DE Goldberg
- DE Goldberg
- DH Wolpert
- DM Chickering
- E Ghiamati
- EC Lopez-Diez
- Elon Correa
- FV Jensen
- IH Witten
- J Opitz
- J Pearl
- JF Hair
- JH Holland
- L Breiman
- LA Shute
- LA Shute
- M Barker
- M Mitchell
- M Seasholtz
- MB Beverly
- MW Tabor
- N Sproch
- NA Karp
- P Zhang
- R Goodacre
- RE Neapolitan
- Royston Goodacre
- RR Bouckaert
- SH Pendukar
- SJ DeLuca
- SL Lauritzen
- Ss Huang
- TV Inglesby
- W Barnaby
- X Zeng
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
Background
The rapid identification of Bacillus spores and bacterial identification are paramount because of their implications in food poisoning, pathogenesis and their use as potential biowarfare agents. Many automated analytical techniques such as Curie-point pyrolysis mass spectrometry (Py-MS) have been used to identify bacterial spores giving use to large amounts of analytical data. This high number of features makes interpretation of the data extremely difficult We analysed Py-MS data from 36 different strains of aerobic endospore-forming bacteria encompassing seven different species. These bacteria were grown axenically on nutrient agar and vegetative biomass and spores were analyzed by Curie-point Py-MS.
Results
We develop a novel genetic algorithm-Bayesian network algorithm that accurately identifies sand selects a small subset of key relevant mass spectra (biomarkers) to be further analysed. Once identified, this subset of relevant biomarkers was then used to identify Bacillus spores successfully and to identify Bacillus species via a Bayesian network model specifically built for this reduced set of features.
Conclusions
This final compact Bayesian network classification model is parsimonious, computationally fast to run and its graphical visualization allows easy interpretation of the probabilistic relationships among selected biomarkers. In addition, we compare the features selected by the genetic algorithm-Bayesian network approach with the features selected by partial least squares-discriminant analysis (PLS-DA). The classification accuracy results show that the set of features selected by the GA-BN is far superior to PLS-DA
Exosomes derived from mesenchymal stem cells enhance radiotherapy-induced cell death in tumor and metastatic tumor foci
- Author
- A Dietrich
- Ana Nieto
- Ana Santos
- C Thery
- D Hanahan
- D Klein
- D Kumar
- DJ Prockop
- E Lopez
- E Lopez
- E Siles
- Eduardo Andrés
- EJ van der Vlist
- F Valeriote
- F. Javier Oliver
- Francisco Martín
- Francisco O’Valle
- FV de Araujo
- GG Steel
- GL Nicolson
- H Peinado
- H Weyd
- Isabel Tovar
- J Gomez-Millan
- JE Scaife
- Jesús López-Peñalver
- José Expósito
- José Mariano Ruiz de Almodóvar
- JW Shin
- K Shah
- L Claret
- M Villalobos
- MB Barton
- ML Maitland
- MR Loebinger
- MR Loebinger
- NH Nicolay
- Per Anderson
- Q Zhao
- R Atun
- R Cojocneanu Petric
- RC Lai
- Santiago Serrano-Saenz
- SE Haynesworth
- SM Kim
- TH Tran
- TM Rager
- VA Farias
- VA Farias
- Virgínea de Araujo Farias
- W Zhou
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/08/2018
- Field of study
We have recently shown that radiotherapy may not only be a successful local and regional treatment
but, when combined with MSCs, may also be a novel systemic cancer therapy. This study aimed to investigate the
role of exosomes derived from irradiated MSCs in the delay of tumor growth and metastasis after treatment with
MSC + radiotherapy (RT). The tumor cell loss rates found after treatment with the combination of MSC and RT and for exclusive RT, were:
44.4% % and 12,1%, respectively. Concomitant and adjuvant use of RT and MSC, increased the mice surviving time 22,5%
in this group, with regard to the group of mice treated with exclusive RT and in a 45,3% respect control group. Moreover,
the number of metastatic foci found in the internal organs of the mice treated with MSC + RT was 60% less than the
mice group treated with RT alone. We reasoned that the exosome secreted by the MSC, could be implicated in tumor
growth delay and metastasis control after treatment. Our results show that exosomes derived form MSCs, combined with radiotherapy, are determinant in
the enhancement of radiation effects observed in the control of metastatic spread of melanoma cells and suggest that
exosome-derived factors could be involved in the bystander, and abscopal effects found after treatment of the tumors
with RT plus MSC. Radiotherapy itself may not be systemic, although it might contribute to a systemic effect when used
in combination with mesenchymal stem cells owing the ability of irradiated MSCs-derived exosomes to increase the
control of tumor growth and metastasis.This work was supported by CNPq, Conselho Nacional de
Desenvolvimento Científico e Tecnológico – Brasil, Junta de Andalucía,
project of Excellence from Junta de Andalucía P12-CTS-383 to FJO, Spanish
Ministry of Economy and Competitiveness SAF2015-70520-R to FJO and
JMRdA, RTICC RD12/0036/0026 and CIBER Cáncer ISCIII CB16/12/00421 to
FJO
Precise measurement of the W-boson mass with the CDF II detector
- Author
- Aaltonen T.
- Abbaneo D
- Adzic P
- Aguilar-Benitez M
- Ahmad M
- Ahmed I
- Albajar C
- Allfrey P
- Almeida N
- Alvarez Gonzalez B.
- Amerio S.
- Amidei D.
- Anastassov A.
- Andreev V
- Andreev Y
- Annovi A.
- Antos J.
- Apollinari G.
- Appel J. A.
- Arce P
- Arisawa T.
- Artikov A.
- Asaadi J.
- Asghar MI
- Ashmanskas W.
- Auerbach B.
- Auffray E
- Aurisano A.
- Auzinger G
- Azarkin M
- Azfar F.
- Azhgirey I
- Badgett W.
- Bae T.
- Baillon P
- Ball AH
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- Barnes V. E.
- Barnett B. A.
- Barney D
- Barria P.
- Bartos P.
- Battilana C
- Bauce M.
- Bedeschi F.
- Bedoya CF
- Beecher D.
- Behari S.
- Bell AJ
- Bellettini G.
- Bellinger J.
- Belotelov I
- Benedetti D
- Benjamin D.
- Beretvas A.
- Bernet C
- Bhatti A.
- Bialas W
- Bilinskas MJ
- Binkley M.
- Bisello D.
- Bitioukov S
- Bizjak I.
- Bland K. R.
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- Burelo ED
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- Busetto G.
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- Wilbur S.
- Wilbur S.
- Williams H. H.
- Williams H. H.
- Willmott C
- Wilson J. S.
- Wilson J. S.
- Wilson P.
- Wilson P.
- Winer B. L.
- Winer B. L.
- Wittich P.
- Wittich P.
- Wohri HK
- Wolbers S.
- Wolbers S.
- Wolfe H.
- Wolfe H.
- Wright T.
- Wright T.
- Wrochna G
- Wu X.
- Wu X.
- Wu Z.
- Wu Z.
- Yamamoto K.
- Yamamoto K.
- Yamaoka J.
- Yamato D.
- Yang T.
- Yang T.
- Yang U. K.
- Yang U. K.
- Yang Y. C.
- Yang Y. C.
- Yao W. -M.
- Yao W. -M.
- Yeh G. P.
- Yeh G. P.
- Yi K.
- Yi K.
- Yoh J.
- Yoh J.
- Yorita K.
- Yorita K.
- Yoshida T.
- Yoshida T.
- Yu G. B.
- Yu G. B.
- Yu I
- Yu I.
- Yu I.
- Yu S. S.
- Yu S. S.
- Yun J. C.
- Yun J. C.
- Zalewski R
- Zanetti A.
- Zanetti A.
- Zarubin A
- Zeng Y.
- Zeng Y.
- Zhokin A
- Zhou C.
- Zucchelli S..
- Zucchelli S..ng S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We have measured the W-boson mass MW using data corresponding to 2.2/fb of
integrated luminosity collected in proton-antiproton collisions at 1.96 TeV
with the CDF II detector at the Fermilab Tevatron collider. Samples consisting
of 470126 W->enu candidates and 624708 W->munu candidates yield the measurement
MW = 80387 +- 12 (stat) +- 15 (syst) = 80387 +- 19 MeV. This is the most
precise measurement of the W-boson mass to date and significantly exceeds the
precision of all previous measurements combined
Evidence for the h_b(1P) meson in the decay Upsilon(3S) --> pi0 h_b(1P)
- Author
- Adametz A.
- Adye T.
- Ahmed H.
- Alam M. S.
- Albert J.
- Allen M. T.
- Alwyn K. E.
- Andreassen R.
- Angelini C.
- Anh TV
- Anulli F.
- Arnaud N.
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini-Ferroli R.
- Band H. R.
- Banerjee Sw.
- Bard D. J.
- Barlow R. J.
- Bartoldus R.
- Batignani G.
- Behera P. K.
- Bellis M.
- Ben-Haim E.
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
- Bettarini S.
- Bettoni D.
- Bevan A. J.
- Bhuyan B.
- Bianchi F.
- Biasini M.
- Biassoni P.
- Bingham I.
- Blinov V. E.
- Bloom P. C.
- Blount N. L.
- Bomben M.
- Bondioli M.
- Bonneaud G. R.
- Bozzi C.
- Brau J.
- Briand H.
- Brown D. N.
- Brown D. N.
- Buenger C.
- Burchat P. R.
- Buzykaev A. R.
- Cakir IT
- Calabrese R.
- Calcaterra A.
- Calderini G.
- Campagnari C.
- Carpinelli M.
- Cartaro C.
- Casarosa G.
- Castanheira MTD
- Castelli G.
- Cavoto G.
- Cenci R.
- Cervelli A.
- Chauveau J.
- Chavez C. A.
- Chen C.
- Chen X. R.
- Cheng C. H.
- Choi H. H. F.
- Cibinetto G.
- Clark P. J.
- Cochran J.
- Coleman J. P.
- Contri R.
- Convery M. R.
- Corwin L. A.
- Cowan G.
- Cowan R.
- Crawley H. B.
- Cremaldi L.
- Curry S.
- Dallapiccola C.
- Dasu S.
- Dauncey P. D.
- Davier M.
- Davis C. L.
- de Monchenault G. Hamel
- De Nardo G.
- de Sangro R.
- Denig A. G.
- Derkach D.
- Di Lodovico F.
- Doll D. A.
- Dorfan J.
- Druzhinin V. P.
- Dubois-Felsmann G. P.
- Dubrovin M. S.
- Dujmic D.
- Dunwoodie W.
- Ebert M.
- Echenard B.
- Eckmann R.
- Edwards A. J.
- Eigen G.
- Eisner A. M.
- Emery S.
- Ernst J. A.
- Faccini R.
- Feltresi E.
- Ferrarotto F.
- Ferrer JAV
- Ferroni F.
- Field R. C.
- Finocchiaro G.
- Fioravanti E.
- Firmino da Costa J.
- Flood K. T.
- Ford W. T.
- Forti F.
- Frey R.
- Fritsch M.
- Fry J. R.
- Fulsom B. G.
- Gabareen A. M.
- Gabathuler E.
- Gagliardi N.
- Gallego EV
- Gamba D.
- Garra Tico J.
- Gary J. W.
- Garzia I.
- Gaspero M.
- Gaz A.
- Gershon T. J.
- Gioi L. Li
- Giorgi M. A.
- Godang R.
- Golubev V. B.
- Gradl W.
- Graham M. T.
- Grauges E.
- Grenier P.
- Gritsan A. V.
- Grosdidier G.
- Guido E.
- Guo Z. J.
- Guttman N.
- Hafner A.
- Hamano K.
- Hamilton B.
- Hamon O.
- Harrison P. F.
- Hartmann T.
- Hast C.
- Hearty C.
- Hitlin D. G.
- Hong T. M.
- Honscheid K.
- Hutchcroft D. E.
- Innes W. R.
- Izen J. M.
- Jackson G.
- Jasper H.
- Jawahery A.
- Jessop C. P.
- Kass R.
- Kelsey M. H.
- Kerth L. T.
- Khan A.
- Kim H.
- Kim P.
- King G. J.
- Kirkby D.
- Knoepfel K. J.
- Kobel M. J.
- Koch H.
- Kocian M. L.
- Kolb J. A.
- Kolomensky Yu. G.
- Kovalskyi D.
- Kowalewski R.
- Kravchenko E. A.
- Kroeger R.
- Kroseberg J.
- Lacker H. M.
- Lafferty G. D.
- Lanceri L.
- Lange D. J.
- Lankford A. J.
- Latham T. E.
- Lazzaro A.
- Le Diberder F.
- Leddig T.
- Lee C. L.
- Lees J. P.
- Leith D. W. G. S.
- Leruste Ph.
- Lewczuk M. J.
- Lewis P.
- Li S.
- Lindemann D.
- Lindquist B.
- Lindsay C.
- Liu F.
- Lo Vetere M.
- Lockman W. S.
- Lombardo V.
- Long O.
- Lopez-March N.
- LoSecco J. M.
- Lou X. C.
- Lu C.
- Lueck T.
- Luitz S.
- Lund P.
- Luppi E.
- Lusiani A.
- Luth V.
- Lutz A. M.
- Lynch G.
- Lynch H. L.
- MacFarlane D. B.
- Malaescu B.
- Mallik U.
- Mandelkern M.
- Manoni E.
- Marchiori G.
- Margoni M.
- Marks J.
- Martinelli M.
- Martinez A. J.
- Martinez-Vidal F.
- Mattison T. S.
- Mazzoni M. A.
- McKenna J. A.
- Meadows B. T.
- Meyer W. T.
- Milanes D. A.
- Milosavljevic MV
- Miyashita T. S.
- Monge M. R.
- Monorchio D.
- Morandin M.
- Morii M.
- Muller D. R.
- Munerato M.
- Nagel M.
- Nauenberg U.
- Neal H.
- Negrini M.
- Nelson S.
- Neri N.
- Nguyen X.
- Nicolaci M.
- Nugent I. M.
- O'Grady C. P.
- Ocariz J.
- Ofte I.
- Olaiya E. O.
- Olsen J.
- Ongmongkolkul P.
- Onorato G.
- Onuchin A. P.
- Osipenkov I. L.
- Oyanguren A.
- Pacetti S.
- Palano A.
- Palombo F.
- Pan Y.
- Paoloni E.
- Pappagallo M.
- Paramesvaran S.
- Park W.
- Passaggio S.
- Pastor ET
- Patel P. M.
- Patrignani C.
- Patteri P.
- Payne D. J.
- Pegna D. Lopes
- Pelliccioni M.
- Perez A.
- Perez MV
- Perl M.
- Peruzzi I. M.
- Petzold A.
- Piccolo M.
- Piemontese L.
- Piredda G.
- Playfer S.
- Poireau V.
- Porter F. C.
- Posocco M.
- Prasad V.
- Prell S.
- Prencipe E.
- Prepost R.
- Puccio E. M. T.
- Pulliam T.
- Purohit M. V.
- Rahmat R.
- Rakitin A. Y.
- Rama M.
- Randle-Conde A.
- Ratcliff B. N.
- Raven G.
- Richman J. D.
- Ritchie J. L.
- Rizzo G.
- Roberts D. A.
- Robertson S. H.
- Robertson S. H.
- Robutti E.
- Rodriguez FV
- Roney J. M.
- Roodman A.
- Rosenberg E. I.
- Rossi A.
- Rotondo M.
- Roudeau P.
- Rubin A. E.
- Ruland A. M.
- Sacco R.
- Salnikov A. A.
- Salvati E.
- Sanchez J
- Santoro V.
- Schalk T.
- Schilling C. J.
- Schindler R. H.
- Schram M.
- Schroeder H.
- Schroeder T.
- Schubert K. R.
- Schumm B. A.
- Schune M. H.
- Schwiening J.
- Schwierz R.
- Schwitters R. F.
- Sciacca C.
- Sciolla G.
- Seiden A.
- Sekula S. J.
- Serednyakov S. I.
- Sevilla M. Franco
- Sigamani M.
- Simi G.
- Simonetto F.
- Sinev N. B.
- Sitt S.
- Skovpen Yu. I.
- Smith A. J. S.
- Smith J. G.
- Snoek H. L.
- Snyder A.
- Sobie R. J.
- Soffer A.
- Soh DA
- Sokoloff M. D.
- Solodov E. P.
- Sonnek P.
- Spaan B.
- Spanier S. M.
- Stocchi A.
- Stoker D. P.
- Stracka S.
- Straessner A
- Strandberg J
- Strandberg S
- Strandlie A
- Strang M
- Strauss E
- Strauss M
- Strizenec P
- Strohmer R
- Stroili R.
- Strom D.
- Strom DM
- Strong JA
- Stroynowski R
- Strube J
- Strube J.
- Stugu B
- Stugu B.
- Stumer O
- Stupak J
- Sturm P
- Su D
- Su D.
- Subramania HS
- Sugaya Y
- Sugimoto T
- Suhr C
- Suita K
- Suk M
- Sulin VV
- Sullivan M. K.
- Sultansoy S
- Sumida T
- Summers D. J.
- Sun L.
- Sun S.
- Sun X
- Sundermann JE
- Suruliz K
- Sushkov S
- Susinno G
- Sutton MR
- Suzuki K.
- Suzuki Y
- Sviridov YM
- Swedish S
- Sykora I
- Sykora T
- Szeless B
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taga A
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Talby M
- Talyshev A
- Tamsett MC
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanaka Y
- Tani K
- Tannoury N
- Tappern GP
- Tapprogge S
- Taras P.
- Tardif D
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tatarkhanov M
- Taylor C
- Taylor FE
- Taylor GN
- Taylor W
- Teixeira-Dias P
- Telnov A. V.
- Temming KK
- Ten Kate H
- Teng PK
- Tenon J
- Terada S
- Terashi K
- Terwort M
- Testa M
- Teuscher RJ
- Tevlin CM
- Thadome J
- Therhaag J
- Theveneaux-Pelzer T
- Thioye M
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson J. M.
- Thompson PD
- Thompson PD
- Thomson E
- Thomson M
- Thun RP
- Tibbetts M.
- Tic T
- Tikhomirov V
- Tikhonov YA
- Timmermans CJWP
- Tipton P
- Tisserand V.
- Tisserant S
- Tobias J
- Toczek B
- Todorov T
- Todorova-Nova S
- Todyshev K. Yu.
- Toggerson B
- Tojo J
- Tokar S
- Toki W. H.
- Tokunaga K
- Tokushuku K
- Tollefson K
- Tomoto M
- Tompkins L
- Toms K
- Tonazzo A
- Tong G
- Tonoyan A
- Topfel C
- Topilin ND
- Torchiani I
- Torrence E
- Torrence E.
- Toth J
- Touchard F
- Touramanis C.
- Tovey DR
- Traynor D
- Trefzger T
- Treis J
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trinh TN
- Tripiana MF
- Triplett N
- Trischuk W
- Trivedi A
- Trocme B
- Troncon C
- Trottier-McDonald M
- Trzupek A
- Tsarouchas C
- Tseng JCL
- Tsialciris M
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman O
- Tsulaia V
- Tsung JW
- Tsuno S
- Tsybychev D
- Tua A
- Tuggle JM
- Turala M
- Turecek D
- Turlay E
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Typaldos D
- Tyrvainen H
- Tzanakos G
- Uchida K
- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
- Ukegawa F
- Unal G
- Underwood DG
- Undnis A
- Unel G
- Unno Y
- Urbaniec D
- Urkovsky E
- Urrejola P
- Usai G
- Uslenghi M
- Uwer U.
- Va'vra J.
- Vacavant L
- Vacek V
- Vachon B
- Vague FV
- Vahsen S
- Valderanis C
- Valenta J
- Valente P
- Valentinetti S
- Valkar S
- Vallecorsa S
- van der Graaf H
- van der Kraaij E
- Van Der Leeuw R
- van der Poel E
- van der Ster D
- Van Eijk B
- van Eldik N
- van Gemmeren P
- van Kesteren Z
- van Vulpen I
- Vandelli W
- Vandoni G
- Vaniachine A
- Vankov P
- Vannucci F
- Vari R
- Varnes EW
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasseur G.
- Vassilakopoulos VI
- Vazeille F
- Vegni G
- Veillet JJ
- Velev G.
- Vellidis C
- Vellidis C.
- Veloso F
- Veness R
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Vercesi V
- Verderi M.
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vichou I
- Vickey T
- Vidal M.
- Viegas FJTA
- Viehhauser GHA
- Viel S
- Vila I.
- Vilar R.
- Villa M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
- Viret S
- Virzi J
- Vitale A
- Vitale L.
- Vitells O
- Viti M
- Vitug G. M.
- Vivarelli I
- Vizan J.
- Vlachos S
- Vlasak M
- Vlasov N
- Vogel A
- Vogel M.
- Vokac P
- Volpi G
- Volpi G.
- Volpi M
- Volpini G
- von der Schmitt H
- von Loeben J
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorobiev AP
- Vorwerk V
- Vos M
- Voss R
- Voss TT
- Vossebeld JH
- Vovenko AS
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vuosalo C. O.
- Wagner A. P.
- Wagner P
- Wagner P.
- Wagner R. L.
- Wagner S. R.
- Wagner W
- Wahlen H
- Wakabayashi J
- Wakisaka T.
- Walbersloh J
- Walch S
- Walder J
- Waldi R.
- Walker R
- Wallny R.
- Walsh J. J.
- Wang L.
- Wang S M
- Wang S. M.
- Wang W. F.
- Warburton A
- Warburton A.
- Waters D
- Waters D.
- Watson J. E.
- Weaver M.
- Weinberger M
- Weinberger M.
- West C. A.
- Wester W C 3rd
- Wester W. C. III
- White R. M.
- Whitehouse B
- Whitehouse B.
- Whiteson D
- Whiteson D.
- Wick F
- Wick F.
- Wicklund A B
- Wicklund A. B.
- Wicklund E
- Wicklund E.
- Wilbur S
- Wilbur S.
- Williams H H
- Williams H. H.
- Wilson F. F.
- Wilson J S
- Wilson J. R.
- Wilson J. S.
- Wilson P
- Wilson P.
- Winer B L
- Winer B. L.
- Wisniewski W. J.
- Wittgen M.
- Wittich P
- Wittich P.
- Wolbers S
- Wolbers S.
- Wolfe H
- Wolfe H.
- Wormser G.
- Wray B. C.
- Wren A. C.
- Wright D. H.
- Wright D. M.
- Wright T
- Wright T.
- Wu S. L. Wallny R
- Wu X
- Wu X.
- Wu Z
- Wu Z.
- Wulsin H. W.
- Yamamoto K
- Yamamoto K.
- Yamaoka J
- Yamaoka J.
- Yang T
- Yang T.
- Yang U K
- Yang U. K.
- Yang Y C
- Yang Y. C.
- Yao W-M
- Yao W. -M.
- Yarritu A. K.
- Yeche Ch.
- Yeh G P
- Yeh G. P.
- Yi K
- Yi K.
- Yoh J
- Yoh J.
- Yorita K
- Yorita K.
- Yoshida T
- Yoshida T.
- Young C. C.
- Yu G B
- Yu G. B.
- Yu I
- Yu I.
- Yu S S
- Yu S. S.
- Yun J C
- Yun J. C.
- Yun J. C.
- Yushkov A. N.
- Zallo A.
- Zanetti A
- Zanetti A.
- Zanetti A.
- Zeng Y
- Zeng Y.
- Zeng Y.
- Ziegler V.
- Zucchelli S.
- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Using a sample of 122 million Upsilon(3S) events recorded with the BaBar
detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we search for
the hb(1P) spin-singlet partner of the P-wave chi_{bJ}(1P) states in the
sequential decay Upsilon(3S) --> pi0 h_b(1P), h_b(1P) --> gamma eta_b(1S). We
observe an excess of events above background in the distribution of the recoil
mass against the pi0 at mass 9902 +/- 4(stat.) +/- 2(syst.) MeV/c^2. The width
of the observed signal is consistent with experimental resolution, and its
significance is 3.1sigma, including systematic uncertainties. We obtain the
value (4.3 +/- 1.1(stat.) +/- 0.9(syst.)) x 10^{-4} for the product branching
fraction BF(Upsilon(3S)-->pi0 h_b) x BF(h_b-->gamma eta_b).Comment: 8 pages, 4 postscript figures, submitted to Phys. Rev. D (Rapid
Communications
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
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- Atlay NB
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescua E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartos P
- Bartsch V
- Bassalat A
- Basye A
- Bates RL
- Batkova L
- Batley JR
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- Castillo IS
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- de Renstrom PAB
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- Enari Y
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- Eriksson D
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- Escalier M
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- Esch H
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- Escobar C
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- Espinal Curull X
- Espinal Curull X
- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
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- Etzion E
- Etzion E
- Evans H
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- Fabbri L
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- Facini G
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- Farrell S
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- Farrington SM
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- Farthouat P
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- Fassi F
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- Fassnacht P
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- Fassouliotis D
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- Favareto A
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- Fayard L
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- Federic P
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- Fedin OL
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- Fedorko W
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- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
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- Feligioni L
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- Feng C
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- Feng EJ
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- Fenyuk AB
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- Fernando W
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- Ferrando BMS
- Ferrando J
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- Ferrara V
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- Ferrari A
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- Fiedler F
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- Filipcic A
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- Filipuzzi M
- Filipuzzi M
- Filthaut F
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- Fincke-Keeler M
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- Fitzgerald EA
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- Fleck I
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- Fleischmann S
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- Fletcher G
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- Floderus A
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- Florez Bustos AC
- Flowerdew MJ
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- Formica A
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- Forti A
- Forti A
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- French ST
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- Gabizon O
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- Gabrielli A
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- Gadatsch S
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- Gadomski S
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- Gagnon P
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- Galhardo B
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- Gallas EJ
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- Gallo V
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- Gallop BJ
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- Gallus P
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- Gao J
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- Garcia BRM
- Garcia C
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- Gardner RW
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- Garelli N
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- Garonne V
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- Garrido MDMC
- Gatti C
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- Gaudio G
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- Gaur B
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- Gauzzi P
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- Gavrilenko IL
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- Gay C
- Gay C
- Gaycken G
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- Gazis EN
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- Ge P
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- Gecse Z
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- Gee CNP
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- Geerts DAA
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- Geich-Gimbel C
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- Gellerstedt K
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- Gemme C
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- Gemmell A
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- Genest MH
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- Gentile S
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- George M
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- Gerbaudo D
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- Gershon A
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- Ghazlane H
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- Ghodbane N
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- Giacobbe B
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- Giangiobbe V
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- Giannetti P
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- Giokaris N
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- Giordani MP
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- Giordano R
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- Giraud PF
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- Giugni D
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- Giuliani C
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- Giunta M
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- Gjelsten BK
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- Gordon HA
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- Gorini B
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- Gorini E
- Gorini E
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Zhemchugov A
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- Zurzolo G
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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 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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- Yao W-M
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- Yildiz HD
- Yilmaz M
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- Young CJS
- Youssef S
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- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhang H
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- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou N
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- 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 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
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Atkinson M
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen A
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
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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
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