953 research outputs found
Observation of the Baryonic Flavor-Changing Neutral Current Decay Lambda_b -> Lambda mu+ mu-
- Author
- Aaltonen T
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report the first observation of the baryonic flavor-changing neutral
current decay Lambda_b -> Lambda mu+ mu- with 24 signal events and a
statistical significance of 5.8 Gaussian standard deviations. This measurement
uses ppbar collisions data sample corresponding to 6.8fb-1 at sqrt{s}=1.96TeV
collected by the CDF II detector at the Tevatron collider. The total and
differential branching ratios for Lambda_b -> Lambda mu+ mu- are measured. We
find B(Lambda_b -> Lambda mu+ mu-) = [1.73+-0.42(stat)+-0.55(syst)] x 10^{-6}.
We also report the first measurement of the differential branching ratio of B_s
-> phi mu+ mu- using 49 signal events. In addition, we report branching ratios
for B+ -> K+ mu+ mu-, B0 -> K0 mu+ mu-, and B -> K*(892) mu+ mu- decays.Comment: 8 pages, 2 figures, 4 tables. Submitted to Phys. Rev. Let
Search for the standard model Higgs boson at LEP
- Author
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- Abbaneo D
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- Anderson KJ
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- von Wimmersperg-Toeller JH
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- Vorobyov AA
- Voss H
- Vossebeld J
- Vrba V
- Waananen A
- Wachsmuth H
- Wadhwa M
- Wahlen H
- Waller D
- Wallraff W
- Wang M
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- Wang XL
- Wang ZM
- Ward CP
- Ward DR
- Ward JJ
- Washbrook AJ
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- Watkins PM
- Watson AT
- Watson NK
- Weber M
- Weiser C
- Well PS
- Wengler T
- Wermes N
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- Wetterling D
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- Wicke D
- Wickens J
- Wiedenmann W
- Wienemann P
- Wilkens H
- Wilkinson G
- Wilson GW
- Wilson JA
- Winter M
- Witek M
- Wolf G
- Wolf G
- Wu J
- Wu SL
- Wu SX
- Wu X
- Wunsch M
- Wyatt TR
- Wynhoff S
- Xia L
- Xie Y
- Xu R
- Xu ZZ
- Xue S
- Yamamoto J
- Yamashita S
- Yang BZ
- Yang CG
- Yang HJ
- Yang M
- Yeh SC
- Yuan C
- Yushchenko O
- Zachariadou K
- Zalewska A
- Zalewski P
- Zalite A
- Zalite Y
- Zavrtanik D
- Zeitnitz C
- Zer-Zion D
- Zhang J
- Zhang L
- Zhang ZP
- Zhao J
- Zhao W
- Zhu GY
- Zhu RY
- Zhuang HL
- Zhuravlov V
- Zichichi A
- Ziegler T
- Zilizi G
- Zimin NI
- Zimmermann B
- Zintchenko A
- Zito G
- Zivkovic L
- Zobernig G
- Zoller M
- Zupan M
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fbâ1 of â s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at sâ=8 TeV with the ATLAS detector
- Author
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- Zhemchugov A
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- 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 20.1fbâ1 of protonâproton collision data at âs = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via tËâtÏË01 or tËâ bÏ˱1 âbW(â)ÏË01 , where ÏË01 (Ï˱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 tË â tÏË01 . For a branching fraction of 100%, top squark masses in the range 270â645 GeV are excluded for ÏË01 masses below 30 GeV. For a branching fraction of 50% to either tË â tÏË01 or tË â bÏ˱1 , and assuming the Ï˱1 mass to be twice the ÏË01 mass, top squark masses in the range 250â550 GeV are excluded for ÏË01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at âs=8TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
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- Acharya BS
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- Adomeit S
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- Aguilar-Saavedra JA
- Agustoni M
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- Aielli G
- Akerstedt H
- Akesson TP
- Akimoto G
- Akimov AV
- Alberghi GL
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- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
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- Zhemchugov A
- Zhong J
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
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- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- 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 20.3fbâ1of data collected in protonâproton collisions at âs=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
Combined Tevatron upper limit on gg->H->W+W- and constraints on the Higgs boson mass in fourth-generation fermion models
- Author
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- Publication venue
- Publication date
- 01/01/2010
- Field of study
Report number: FERMILAB-PUB-10-125-EWe combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg->H->W+W- in p=pbar collisions at the Fermilab Tevatron Collider at sqrt{s}=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% Confidence Level upper limit on \sigma(gg->H) x B(H->W+W-) is 1.75 pb at m_H=120 GeV, 0.38 pb at m_H=165 GeV, and 0.83 pb at m_H=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% Confidence Level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.We combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process ggâHâW+W- in ppÌ
collisions at the Fermilab Tevatron Collider at âs=1.96ââTeV. With 4.8ââfb-1 of integrated luminosity analyzed at CDF and 5.4ââfb-1 at D0, the 95% confidence level upper limit on Ï(ggâH)ĂB(HâW+W-) is 1.75 pb at mH=120ââGeV, 0.38 pb at mH=165ââGeV, and 0.83 pb at mH=200ââGeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% confidence level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.Peer reviewe
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
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- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
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- Benjamin DP
- Bensinger JR
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- Suruliz K
- Susinno G
- Sutton MR
- Suzuki S
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- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
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- Taenzer J
- Taffard A
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- Vivarelli I
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- von der Schmitt H
- von Toerne E
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- Vuillermet R
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- Wagner P
- Wagner W
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- Wahrmund S
- Wakabayashi J
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- Wallangen V
- Walls FM Garay
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- Wanotayaroj C
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- Wardrope DR
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- Watson IJ
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- White R
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- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
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- Wiik-Fuchs LAM
- Wildauer A
- Wilkens HG
- Williams HH
- Williams S
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- Wingerter-Seez I
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KH Yau
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wu M
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- Wyatt TR
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- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yuen SPY
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particleâhole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Synthesis of 2-azidoethyl α-d-mannopyranoside orthogonally protected and selective deprotections
- Author
- Acciarri M
- Adriani O
- Aguilar-Benitez M
- Ahlen S
- Alcaraz J
- Alemanni G
- Allaby J
- Aloisio A
- Alverson G
- Alviggi MG
- Ambrosi G
- Anderhub H
- Andreev VP
- Angelescu T
- Anselmo F
- Arefiev A
- Azemoon T
- Aziz T
- Bagnaia P
- Baksay L
- Ball RC
- Banerjee S
- Banerjee S
- Banicz K
- Barczyk A
- Barillere R
- Barone L
- Bartalini P
- Baschirotto A
- Basile M
- Battiston R
- Bay A
- Becattini F
- Becker U
- Behner F
- Berdugo J
- Berges P
- Bertucci B
- Betev BL
- Bhattacharya S
- Biasini M
- Biland A
- BIlei GM
- Blaising JJ
- Blyth SC
- Bobbink GJ
- Bock R
- Bohm A
- Boldizsar L
- Borgia B
- Boucham A
- Bourilkov D
- Bourquin M
- Boutigny D
- Braccini S
- Branson JG
- Brigljevic V
- Brock IC
- Buffini A
- Buijs A
- Burger JD
- Burger WJ
- Busenitz J
- Cai XD
- Campanelli M
- Capell M
- Carlino G
- Cartacci AM
- Casaus J
- Castellini G
- Cavallari F
- Cavallo N
- Cecchi C
- Cerrada M
- Cesaroni F
- Chamizo M
- Chang YH
- Chaturvedi UK
- Chekanov SV
- Chemarin M
- Chen A
- Chen G
- Chen GM
- Chen HF
- Chen HS
- Chen M
- Chiefari G
- Chien CY
- Cifarelli L
- Cindolo F
- Civinini C
- Clare I
- Clare R
- Cohn HO
- Coignet G
- Colijn AP
- Colino N
- Collaboration L
- Commichau V
- Costantini S
- Cotorobai F
- Csilling A
- D'Alessandro R
- Dai TS
- de Asmundis R
- de Guevara PL
- de Jong P
- de la Cruz B
- Degre A
- Deiters K
- Denes P
- DeNotaristefani F
- Di Lodovico F
- DiBitonto D
- Diemoz M
- Dionisi C
- Dittmar M
- Dominguez A
- Doria A
- Dorne I
- Dova MT
- Drago E
- Duchesneau D
- Duinker P
- Duran I
- Dutta S
- Easo S
- Efremenko Y
- El Mamouni H
- Engler A
- Eppling FJ
- Erne FC
- Ernenwein JP
- Extermann P
- Fabre M
- Faccini R
- Falciano S
- Favara A
- Fay J
- Fedin O
- Felcini M
- Fenyi B
- Ferguson T
- Ferroni F
- Fesefeldt H
- Fiandrini E
- Field JH
- Filthaut F
- Fisher PH
- Fisk I
- Forconi G
- Fredj L
- Freudenreich K
- Furetta C
- Galaktionov Y
- Ganguli SN
- Garica-Abia P
- Gau SS
- Gentile S
- Gerald J
- Gheordanescu N
- Giagu S
- Goldfarb S
- Goldstein J
- Gong ZF
- Gougas A
- Gratta G
- Gruenewald MW
- Gupta VK
- Gurtu A
- Gutay LJ
- Hartmann B
- Hasan A
- Hatzifotiadou D
- Hebbeker T
- Herve A
- Hofer H
- Hong SJ
- Hoorani H
- Hou SR
- Hu G
- Innocente V
- Janssen H
- Jenkes K
- Jin BN
- Jones LW
- Josa-Mutuberria I
- Kamrad D
- Kamyshkov Y
- Kapustinsky JS
- Karyotakis Y
- Kasser A
- Kaur M
- Khan RA
- Kienzle-Focacci MN
- Kim D
- Kim DH
- Kim JK
- Kim SC
- Kim YG
- Kinnison WW
- Kirkby A
- Kirkby D
- Kirkby J
- Kiss D
- Kittel W
- Klimentov A
- Konig AC
- Kopp A
- Korolko I
- Koutsenko V
- Kraemer RW
- Krenz W
- Kunin A
- Landi G
- Lapoint C
- Lassila-Perini K
- Laurikainen P
- Le Coultre P
- Le Goff JM
- Lebeau M
- Lebedev A
- Lebrun P
- Lecomte P
- Lecoq P
- Leggett C
- Leiste R
- Leonardi E
- Levtchenko P
- Li C
- Lin CH
- Lin WT
- Linde FL
- Lista L
- Liu ZA
- Lohmann W
- Longo E
- Lu W
- Lu YS
- Lubelsmeyer K
- Luci C
- Luckey D
- Luminari L
- Lustermann W
- Ma WG
- Maity M
- Majumder G
- Malgeri L
- Malinin A
- Mana C
- Mangeol D
- Mangla S
- Marchesini P
- Marin A
- Martin JP
- Marzano F
- Massaro GGG
- McNally D
- Mele S
- Merola L
- Meschini M
- Metzger WJ
- Mi Y
- Mihul A
- Mirabelli G
- Mnich J
- Molnar P
- Monteleoni B
- Moore R
- Morganti S
- Moulik T
- Mount R
- Muheim F
- Muijs AJM
- Muller S
- Nahn S
- Napolitano M
- Nessi-Tedaldi F
- Newman H
- Niessen T
- Nippe A
- Nisati A
- Nowak H
- Oh YD
- Opitz H
- Organtini G
- Ostonen R
- Palomares C
- Pandoulas D
- Paoletti S
- Paolucci P
- Park HK
- Park IH
- Pascale G
- Passaleva G
- Patricelli S
- Paul T
- Pauluzzi M
- Paus C
- Pauss F
- Peach D
- Pei YJ
- Pensotti S
- Perret-Gallix D
- Petersen B
- Petrak S
- Pevsner A
- Piccolo D
- Pieri M
- Pinto JC
- Piroue PA
- Pistolesi E
- Plyaskin V
- Pohl M
- Pojidaev V
- Postema H
- Produit N
- Prokofiev D
- Rahal-Callot G
- Raja N
- Rancoita PG
- Rattaggi M
- Raven G
- Razis P
- Read K
- Ren D
- Rescigno M
- Reucroft S
- Riemann S
- Riles K
- Rind O
- Robohm A
- Rodin J
- Roe BP
- Romeo GC
- Romero L
- Rosier-Lees S
- Rosselet P
- Roth S
- Rubio JA
- Ruschmeier D
- Rykaczewski H
- Salicio J
- Sanchez E
- Sanders MP
- Sarakinos ME
- Sarkar S
- Sassowsky M
- Sauvage G
- Schafer C
- Schegelsky V
- Schmidt-Kaerst S
- Schmitz D
- Schmitz P
- Schneegans M
- Scholz N
- Schopper H
- Schotanus DJ
- Schwenke J
- Schwering G
- Sciacca C
- Sciarrino D
- Servoli L
- Shevchenko S
- Shivarov N
- Shoutko V
- Shukla J
- Shumilov E
- Shvorob A
- Siedenburg T
- Smith B
- Son D
- Sopczak A
- Soulimov V
- Spillantini P
- Steuer M
- Stickland DP
- Stone H
- Stoyanov B
- Straessner A
- Strauch K
- Sudhakar K
- Sultanov G
- Sun LZ
- Susinno GF
- Suter H
- Swain JD
- Tang XW
- Tauscher L
- Taylor L
- Ting SCC
- Ting SM
- Tonutti M
- Tonwar SC
- Toth J
- Tuchscherer H
- Tully C
- Tung KL
- Uchida Y
- Ulbricht J
- Uwer U
- Valente E
- Van de Walle RT
- van Dierendonck D
- van Hoek WC
- van Mil AJW
- van Rhee T
- van Rossum W
- Vesztergombi G
- Vetlitsky I
- Viertel G
- Vivargent M
- Vogel H
- Vogt H
- Volkert R
- von der Mey M
- Vorobiev I
- Vorobyov AA
- Vorvolakos A
- Wadhwa M
- Wallraff W
- Wang JC
- Wang XL
- Wang ZM
- Weber A
- Wittgenstein F
- Wu SX
- Wynhoff S
- Xu J
- Xu ZZ
- Yang BZ
- Yang CG
- Yao XY
- Ye JB
- Yeh SC
- You JM
- Zalite A
- Zalite Y
- Zemp P
- Zeng Y
- Zhang Z
- Zhang ZP
- Zhou B
- Zhou Y
- Zhu GY
- Zhu RY
- Zichichi A
- Ziegler F
- Publication venue
- Elsevier
- Publication date
- 01/01/1998
- Field of study
4 pĂĄginas, 1 figura, 2 esquemas.We present the synthesis of a fully orthogonally protected mannosyl glycoside 1 and the corresponding methods for selective deprotections. Mannosyl glycoside 1 contains a functionalized linker at the anomeric position to allow for the attachment of carbohydrate units to scaffolds in order to prepare carbohydrate multivalent systems.We would like to thank FIS (PI030093), for financial supportPeer reviewe
Measurement of the W±Z boson pair-production cross section in pp collisions at âs=13TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- AlconadaVerzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos CN
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baak MA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Bagiacchi P
- Bagnaia P
- Bai Y
- Baines JT
- Baker OK
- Baldin EM
- Balek P
- Balestri T
- Balli F
- Balunas WK
- Banas E
- Banerjee S
- Bannoura AAE
- Barajas CAC
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Baw HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Beringer J
- Berlendis S
- Berlingen JM
- Bernard NR
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertram IA
- Bertsche C
- Bertsche D
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bevan AJ
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Biedermann D
- Bielski R
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biondi S
- Bjergaard DM
- Black CW
- Black JE
- Black KM
- Blackburn D
- Blair RE
- Blanchard J-B
- Blanco JE
- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boehler M
- Boeriu OEV
- Boerner D
- Bogaerts JA
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Bossio Sola JD
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bracinik J
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- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wittkowski J
- Wolf TMH
- Wolter MW
- Wolters H
- Wong KHY
- Worm SD
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wu M
- Wu M
- Wu SL
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- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
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- Yan Z
- Yang H
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- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
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- Yuen SPY
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- Netherlands
- Publication date
- 01/01/2016
- Field of study
published_or_final_versio
Measurement of W+Wâ production in association with one jet in protonâproton collisions at sqrt(s) = 8TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Ahlen SP
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- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
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- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
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- Alstaty M
- Alviggi MG
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- Amako K
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- Arce ATH
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- Argyropoulos S
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- Armadans RC
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- Arnaez O
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- Arslan O
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
The production of W boson pairs in association with one jet in pp collisions at View the MathML sources=8 TeV is studied using data corresponding to an integrated luminosity of 20.3 fbâ1 collected by the ATLAS detector during 2012 at the CERN Large Hadron Collider. The cross section is measured in a fiducial phase-space region defined by the presence of exactly one electron and one muon, missing transverse momentum and exactly one jet with a transverse momentum above 25 GeV and a pseudorapidity of |η|<4.5|η|<4.5. The leptons are required to have opposite electric charge and to pass transverse momentum and pseudorapidity requirements. The fiducial cross section is found to be View the MathML sourceÏWWfid,1-jet=136±6(stat)±14(syst)±3(lumi) fb. In combination with a previous measurement restricted to leptonic final states with no associated jets, the fiducial cross section of WW production with zero or one jet is measured to be View the MathML sourceÏWWfid,â€1-jet=511±9(stat)±26(syst)±10(lumi) fb. The ratio of fiducial cross sections in final states with one and zero jets is determined to be 0.36±0.050.36±0.05. Finally, a total cross section extrapolated from the fiducial measurement of WW production with zero or one associated jet is reported. The measurements are compared to theoretical predictions and found in good agreement
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