152 research outputs found
Magnetic phase evolution and particle size estimation study on nanocrystalline Mg–Mn ferrites
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Investigation of the Ni3Al-Fe alloys by resistivity measurements and differential thermal analysis
- Author
- Publication venue
- 'Allerton Press'
- Publication date
- Field of study
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
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- Allwood-Spiers SE
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
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- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
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- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Measurement of the cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
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- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Alam MA
- Alam MS
- 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
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
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- Searcy J
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- Shan LY
- Shank JT
- Shao QT
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- Shatalov PB
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- Sherman D
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- Short D
- Shupe MA
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- Sidoti A
- Siebel A
- Siegert F
- Siegrist J
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- Silva J
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- Silverstein SB
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- Simard O
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- Simonyan M
- Sinervo P
- Sinev NB
- Sipica V
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjolin J
- Sjursen TB
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- Skubic P
- Skvorodnev N
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- Slavicek T
- Sliwa K
- Sloan TJ
- Sloper J
- Smakhtin V
- Smirnov SY
- Smirnova LN
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- Smit GVY
- Smith BC
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- Snesarev AA
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- Solovyanov OV
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- Stekl I
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- Sulin VV
- Sultansoy S
- Sumida T
- Sun X
- Sundermann JE
- Suruliz K
- Sushkov S
- Susinno G
- Sutton MR
- Suzuki Y
- Suzuki Y
- Svatos M
- Sviridov YM
- Swedish S
- Sykora I
- Sykora T
- Szeless B
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- 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
- Tardif D
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tatarkhanov M
- Tayalati Y
- Taylor C
- Taylor FE
- Taylor GN
- Taylor W
- Tehrani FS
- Teinturier M
- Teixeira-Dias P
- Temming KK
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- Teng PK
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- Teuscher RJ
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- Therhaag J
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- Thompson EN
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- Thompson PD
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- Tikhonov YA
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- Tokar S
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- Torchiani I
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- Traynor D
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- Tricoli A
- Trigger IM
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- Trischuk W
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- Tseng JC-L
- Tsiakiris M
- Tsiareshka PV
- Tsionou D
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- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
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- Turlay E
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- Tykhonov A
- Tylmad M
- Tyndel M
- Tyrvainen H
- Tzanakos G
- Uchida K
- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
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- Underwood DG
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- Unno Y
- Urbaniec D
- Urkovsky E
- Urrejola P
- Usai G
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- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
- 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 Huysduynen LH
- van Kesteren Z
- van Vulpen I
- Vandelli W
- Vandoni G
- Vaniachine A
- Vankov P
- Vannucci F
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- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vegni G
- Veillet JJ
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- Venturi M
- Venturi N
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- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vichou I
- Vickey T
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- Viehhauser GHA
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- Vilucchi E
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- Virzi J
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- Vivarelli I
- Vlachos S
- Vlasak M
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- Vogel A
- Vokac P
- 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
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wahlen H
- Wakabayashi J
- Walbersloh J
- Walch S
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- Wang JC
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- Wang SM
- Warburton A
- Ward CP
- Wardrope DR
- Warsinsky M
- Watkins PM
- Watson AT
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- Watts S
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- Waugh BM
- Weber J
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- Weber MS
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- Weidberg AR
- Weigell P
- Weingarten JJ
- Weiser C
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- Wells PS
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- Wenig S
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- Werner P
- Werth M
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- Weydert C
- Whalen K
- Wheeler-Ellis SJ
- Whitaker SP
- White A
- White MJ
- Whitehead SR
- Whiteson D
- Whittington D
- Wicek F
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Willis W
- Willocq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wraight K
- Wright C
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wunstorf R
- Wynne BM
- Xaplanteris L
- Xella S
- Xie S
- Xie Y
- Xu C
- Xu D
- Xu G
- Yabsley B
- Yacoob S
- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A measurement is presented of the inclusive cross-section for b-jet production in association with a Z boson in pp collisions at a centre-of-mass energy of root s = 7 TeV. The analysis uses the data sample collected by the ATLAS experiment in 2010, corresponding to an integrated luminosity of approximately 36 pb(-1). The event selection requires a Z boson decaying into high P-T electrons or muons, and at least one b-jet, identified by its displaced vertex, with transverse momentum p(T) > 25 GeV and rapidity vertical bar y vertical bar < 2.1. After subtraction of background processes, the yield is extracted from the vertex mass distribution of the candidate b-jets. The ratio of this cross-section to the inclusive Z cross-section (the average number of b-jets per Z event) is also measured. Both results are found to be in good agreement with perturbative QCD predictions at next-to-leading order
Design and baseline characteristics of the finerenone in reducing cardiovascular mortality and morbidity in diabetic kidney disease trial
- Author
- Abdel-Rahman Emaad
- Abhayaratna Walter
- Abramof Ness Rosane
- Acosta Idalia
- Adams Atoya
- Adawi Faiad
- Adler Sharon
- Ahmed Fayzal
- Aizenberg Diego
- Ajani Dilawar
- Al-Karadsheh Amer
- Albota Adrian
- Alferi Dino
- Alicic Radica
- Alla Sreedhara
- Allison D
- Almeida Edgar
- Alpizar Salazar Melchor
- Amer Joseph
- Amod Aslam
- Andrawis Nabil
- Antonio Bossi Carlo
- Antsiferov Mikhail
- Antunes Daniela
- Araki Hideo
- Arango Clara
- Arcos Edgar
- Arif Ahmed
- Arif Imrozia
- Arkhipov Mikhail
- Armaly Zaher
- Aroca Gustavo
- Asprusten Emil
- Atar Shaul
- Avila Pardo Sandro
- Awad Ahmed
- Axthelm Christoph
- Azizad Masoud
- Azizah Aziz Nor
- B Brouwer C
- Babikova Jana
- Babkin Andrey
- Badak Ozer
- Bahrami Michael
- Bajcsi Dora
- Baker John
- Bala Cornelia
- Ballesteros Rosa
- Bansal Shweta
- Barag Steven
- Barakzoy Ahmad
- Baranov Vitaliy
- Barbarash Olga
- Barbonta Hortensia
- Barney Mark
- Barre Paul
- Barrera Sandra
- Barreto Carlos
- Barreto Germ\ue1n
- Bartolacci In\ue9s
- Bashir Khalid
- Bashkin Amir
- Bastidas Adrian Miriam
- Bautista Albert
- Bautista Jose
- Bech Jesper
- Beddhu Srinivasan
- Beltr\ue1n L\uf3pez Nelly
- Ben Chetrit Sydney
- Benitez Diego
- Benjamin Sabrina
- Berar Yanay Noa
- Berenji Ramin
- Bertram Pitt
- Bertsch John
- Besada Diego
- Bhana Sindeep
- Bhargava Anuj
- Bilz Stefan
- Birkenfeld Andreas
- Birriel Jose
- Bittar Julio
- Blanco Guillermo
- Bleich David
- Boletis Ioannis
- Bondarets Iryna
- Bonora Enzo
- Bornfreund Jonathan
- Boshnyashka Radostina
- Botelho Roberto
- Botero Rodrigo
- Botsyurko Volodymyr
- Bouarich Hanane
- Brada Michal
- Brandao Ilidio
- Brar Harjeet
- Braun Hermann
- Brezina Jiri
- Brian Susan
- Brietzke Stephen
- Brito Claudia
- Bruchfeld Annette
- Bruno Giorda Carlo
- Brusco Osvaldo
- Bu Ruifang
- Bucek Petr
- Buganova Ingrid
- Burgner Anna
- Busch Klaus
- Busch Robert
- Butrymowicz Patrycja
- C Bakker R
- C\ue1rdenas Tatiana
- Caceaune Elena
- Cai Hanqing
- Calabr\uf2 Paolo
- Calero Francesca
- Canadas Rafael
- Canani Luis
- Caramori Maria
- Cardona Jose
- Cariou Bertrand
- Carlo Maggi Davide
- Carlos Palma Juan
- Carlos Prieto Juan
- Carlson Brian
- Carpio Jose
- Carvalho Rui
- Case Christopher
- Castro Cristina
- Catindig Elizabeth
- Catrinoiu Doina
- Cayli Murat
- Cereto Castro Fernando
- Cerqueira Maria
- Chahin Mariano
- Chang Chiz-Tzung
- Chantrel Fran\ue7ois
- Chen Dejun
- Chen Nan
- Chen Qinkai
- Cheng Jinluo
- Chernikova Viktoriia
- Chernin Gil
- Chernyavskaya Elena
- Chew Wong Alfredo
- Christina Nowack
- Chuang Lee-Ming
- Chung ChoonHee
- Ciechanowski Kazimierz
- Cieslik Grazyna
- Cigarr\ue1n Guldris Secundino
- Cimino Roberto
- Clavel Sylvaine
- Clodi Martin
- Cobos Jorge
- Colman Peter
- Colquhoun David
- Constantin Ciprian
- Contzen Christel
- Conway James
- Coronel Julian
- Cortes-Maisonet Gregorio
- Cortes-Maisonet Gregorio
- Cournoyer Serge
- Crawford Veronica
- Cristina Gregorini Maria
- Cruz Humberto
- Cruzado Garrit Josep
- Cure Carlos
- Curiac Dan
- Cutfield Rick
- Dandillaya Ramprasad
- Dang Cuong
- Danos Peter
- Darawsha Mahmud
- de \uc1lvaro Fernando
- de Paula Rogerio
- Deerochanawong Chaicharn
- Degenhardt Stefan
- Demko Arkadiy
- Derwahl Karl
- Dhanireddy Soni
- Din Zia
- Distiller Larry
- Dixon Bradley
- Dolores Mart\uednez Esteban M\uaa
- Donath Marc
- Donets Oleksandra
- Dong Junwu
- Dong Youping
- Doshi Ankur
- Doubel Peter
- Dreval Alexander
- Drexel Heinz
- Du Yuming
- Dumas Richard
- Dumitrescu Adriana
- Dunn Peter
- Dur\ue1n Carlos
- Duyck Francis
- Dzupina Andrej
- E Costa Fernando Teixeira
- Ebenbichler Christoph
- Ebisui Osamu
- Edelsberger Tomas
- Edin Anton
- Eduardo Figueiredo Carlos
- Eduardo Salles Joao
- Efrati Shai
- Ekinci Elif
- El Shahawy Mahfouz
- El-Shahawy Mohammed
- Elbert Alicia
- Elias Mazen
- Eliaschewitz Freddy
- Eliasson Ken
- Emdin Michele
- Engelen Wendy
- Eren Necmi
- Eriksen Erik
- Ermakova Polina
- Escalada San Mart\uedn Javier
- Escobedo de la Pe\uf1a Jorge
- Esteves Cesar
- Eugenia Canziani Maria
- Eustace Joe
- Evans John
- Faber Jens
- Fadda George
- Fang Sum Chee
- Fang Yi
- Fangh\ue4nel Salm\uf3n Guillermo
- Farah Ghassan
- Farber Evgeny
- Farooq Umar
- Fauvel Jean-Pierre
- Fernando Roland
- Fiaccadori Enrico
- Fikry Sameh
- Fink Raymond
- Finnes Trine
- Fiorina Paolo
- First Brian
- Fitz-Patrick David
- Flack John
- Fliesser-G\uf6rzer Evelyn
- Fluck Patrick
- Fogelfeld Leon
- Fonseca Vivian
- Forti Adriana
- Franek Edward
- Frank Malin
- Frias Juan
- Fujita Naruhiro
- Furuya Ryuichi
- Fushtey Ivan
- G Lieverse A
- Galcer\ue1n Josep
- Gallouj Karim
- Galphin Claude
- Galyavich Albert
- Gansevoort Ron
- Garc\ueda Hern\ue1ndez Pedro
- Garc\ueda Luis
- Garcia-Mayol Luis
- Gaysina Leyla
- Gelersztein Elizabeth
- George L Bakris
- Georgiev Dimitar
- Gerasimos Filippatos
- Giebel Thomas
- Gillard Pieter
- Giorgio Battaglia Giovanni
- Gislason Gunnar
- Glandt Mariela
- Goldstein Gary
- Goluch Richard
- Gonz\ue1lez Albarr\ue1n Olga
- Gonz\ue1lez G\ue1lvez Guillermo
- Gonz\ue1lez Gonz\ue1lez Jos\ue9
- Gonz\ue1lez Fernando
- Gonzalez Edgar
- Gonzalez-Abreu Francisco
- Gordeev Ivan
- Gore Ashwini
- Gouet Didier
- Grachova Mariia
- Grant David
- Grossman Ehud
- Guan Tianjun
- Guerci Bruno
- Guerrot Dominique
- Guia Jose
- Gul Ibrahim
- Gulakova Drahomira
- Gumprecht Janusz
- Guo Weiying
- Guron Gregor
- Gushterova Valentina
- Guti\ue9rrez Ochoa Ramiro
- Guzm\ue1n Gustavo
- H Boonstra A
- H\uf8ivik Hans
- Habwe Violet
- Hagemeier Robert
- Hagenow Andreas
- Halabi Majdi
- Haller Hermann
- Halpern Stephen
- Hamamoto Yoshiyuki
- Hamasaki Akihiro
- Hamet Pavel
- Hamilton Maxine
- Hammoud Jamal
- Handelsman Stuart
- Hangaard J\uf8rgen
- Hanna Fahmy
- Hanusch Ursula
- Hao Chuanming
- Harcsa Eleonora
- Hart Randolph
- Hartman Israel
- Hasalova Zapletalova Jitka
- Hasnul Halimi Bin Wan Hasan Wan
- Hasslacher Christoph
- Hatazaki Masahiro
- Hatunic Mensud
- Hatziagelaki Erifili
- Hayashi Terumasa
- Heigerick Glenn
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- Ujihara Makoto
- Ukhanova Olga
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- Urina Miguel
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- Valdez Ortiz Rafael
- Valika Shujauddin
- Vallejos Augusto
- van Buren M
- van den Born Bert-Jan
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- van Zyl Louis
- Vanbelleghem Hilde
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- Wainstein Julio
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- Wang Lihua
- Wang Xinjun
- Wanner Christoph
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- Wassermann Alfredo
- Wei Jiali
- Weisnagel Stanley
- Weissman Peter
- Whaley-Connell Adam
- Wierusz-Wysocka Bogna
- Wilderman Igor
- Winston Jonathan
- Wise Jonathan
- Wittert Gary
- Wnetrzak-Michalska Renata
- Wong Yuk-Ki
- Wu Chaoqing
- Wu Mai-Szu
- Wu Ming-Ju
- Wu Tianfeng
- Wudi Krisztina
- Wuerzner Gregoire
- Wynne Katie-Jane
- Xing Changying
- Xiong Fei
- Xu Ning
- Xu Xudong
- Yagil Yoram
- Yajima Ken
- Yakhontov Davyd
- Yale Jean-Francois
- Yamada Daishiro
- Yamada Masayo
- Yamagata Kazuo
- Yamakawa Fumiko
- Yamakawa Ken
- Yamasaki Yoshimitsu
- Yambe Yuko
- Yanai Hidekatsu
- Yang Jinkui
- Yasuda Tetsuyuki
- Yenicerioglu Yavuz
- Yeung Vincent
- Yilmaz Huseyin
- Yin Aiping
- Yoncheva-Mihaylova Mariana
- Young Park Cheol
- Yuan Lee Li
- Yupanqui Hern\ue1n
- Yuryev Michael
- Zakharova Elena
- Zalevskaya Alsu
- Zanozina Olga
- Zaoui Philippe
- Zeig Steven
- Zeng Longyi
- Zhang Hao
- Zhang Yanlin
- Zhang Ying
- Zhao Zhiquan
- Zhdanova Elena
- Zheng Hongguang
- Zhong Ling
- Zhong Liyong
- Zhu Dalong
- Zhukova Larisa
- Zilahi Zsolt
- Zsom Marianna
- Zukermann Robert
- Zykova Tatyana
- Publication venue
- 'S. Karger AG'
- Publication date
- 01/01/2019
- Field of study
Background: Among people with diabetes, those with kidney disease have exceptionally high rates of cardiovascular (CV) morbidity and mortality and progression of their underlying kidney disease. Finerenone is a novel, nonsteroidal, selective mineralocorticoid receptor antagonist that has shown to reduce albuminuria in type 2 diabetes (T2D) patients with chronic kidney disease (CKD) while revealing only a low risk of hyperkalemia. However, the effect of finerenone on CV and renal outcomes has not yet been investigated in long-term trials.
Patients and Methods: The Finerenone in Reducing CV Mortality and Morbidity in Diabetic Kidney Disease (FIGARO-DKD) trial aims to assess the efficacy and safety of finerenone compared to placebo at reducing clinically important CV and renal outcomes in T2D patients with CKD. FIGARO-DKD is a randomized, double-blind, placebo-controlled, parallel-group, event-driven trial running in 47 countries with an expected duration of approximately 6 years. FIGARO-DKD randomized 7,437 patients with an estimated glomerular filtration rate >= 25 mL/min/1.73 m(2) and albuminuria (urinary albumin-to-creatinine ratio >= 30 to <= 5,000 mg/g). The study has at least 90% power to detect a 20% reduction in the risk of the primary outcome (overall two-sided significance level alpha = 0.05), the composite of time to first occurrence of CV death, nonfatal myocardial infarction, nonfatal stroke, or hospitalization for heart failure.
Conclusions: FIGARO-DKD will determine whether an optimally treated cohort of T2D patients with CKD at high risk of CV and renal events will experience cardiorenal benefits with the addition of finerenone to their treatment regimen.
Trial Registration: EudraCT number: 2015-000950-39; ClinicalTrials.gov identifier: NCT02545049
Constraining the magnitude of the chiral magnetic effect with event shape engineering in Pb-Pb collisions at root s(NN)=2.76 TeV
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- Publication venue
- 'Elsevier BV'
- Publication date
- 13/02/2020
- Field of study
CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOIn ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow v(2) reflects fluctuations in the shape of the initial state of the system. This allows to select events with the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two-and three-particle correlations in Pb-Pb collisions at root s(NN) = 2.76 TeV. The two-particle correlator < cos(phi(alpha) - phi(ss))gt;, calculated for different combinations of charges alpha and beta, is almost independent of v(2) (for a given centrality), while the three-particle correlator < cos(phi(alpha) + phi(beta) - 2 Psi(2))gt; scales almost linearly both with the event v(2) and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on v(2) points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.777151162CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOCNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOSem informaçãoSem informaçãoSem informaçãoAgências de fomento estrangeiras apoiaram essa pesquisa, mais informações acesse artig
Abstracts from the 8th International Conference on cGMP Generators, Effectors and Therapeutic Implications
- Author
- Adam Snook
- Adrian J. Hobbs
- Aikaterini I. Argyriou
- Albert Smolenski
- Albert T. Profy
- Alessandro Cataliotti
- Alexander Froese
- Alexander Kollau
- Alexander Kollau
- Alexander Vincent
- Alexandre Dumoulin
- Ali Banijamali
- Alisa Kamynina
- Amie J. Moyes
- Amrita Ahluwalia
- Andrea Gerling
- Andrea Hembre Ulsund
- Andrea Neubauer
- Andreas Friebe
- Andreas Friebe
- Andreas Friebe
- Andreas Friebe
- Andreas Friebe
- Andreas Friebe
- Andreas Friebe
- Andreas Friebe
- Andreas Friebe
- Andreas Güldner
- Andreas Papapetropoulos
- Andrew Tobin
- Andriana Stamopoulou
- Andrzej Weichsel
- Angela McLaughlin
- Angelos Vachaviolos
- Annemarie Aue
- Annemarie Aue
- Annemarie Aue
- Antonius C. F. Gorren
- Arnab Ghosh
- Arno Fritsch
- Astrid Schrammel
- Astrid Schrammel
- Astrid Schrammel
- Astrid Weiss
- Athanassios Giannis
- Atsuko Okamoto
- Attila Oláh
- Axel Gödecke
- B. Selin Kenet
- Balázs Tamás Németh
- Banumathi Sankaran
- Barbara Voussen
- Barbara Voussen
- Barbara Wilhelm
- Bernd J. Pichler
- Bernd Mayer
- Bernd Mayer
- Bernd Mayer
- Bernd Wissinger
- Boris Tchernychev
- Béla Merkely
- Camila B. Almeida
- Carine M. Boustany
- Carla F. F. Penteado
- Catherine Mansfield
- Cheng-Yu Chen
- Chieri Takeuchi
- Choel Kim
- Choel Kim
- Choel Kim
- Choel Kim
- Chris Sarko
- Christian Dees
- Christian Meier
- Christian Schön
- Christine E. Gee
- Christopher Newton-Cheh
- Claire Poulet
- Clara D. Ledsky
- Cor de Wit
- Cor de Witt
- Corina Russwurm
- Cornelia Virus
- Courtney Shea
- Csaba Mátyás
- César Ibarra-Alvarado
- Damian Brockschnieder
- Daniel P. Zimmer
- Daniel Richards
- Daniela Bertinetti
- Dante Merlino
- Darren Casteel
- Darren E. Casteel
- David A. Kass
- David Kilpatrick
- David Langleben
- David Langleben
- Deborah M. Dickey
- Dennis Busse
- Dennis J. Stuehr
- Diane Wong
- Dianna M. Milewicz
- Dieter Groneberg
- Dieter Groneberg
- Dieter Groneberg
- Ditta Zobor
- Dominik M. Fischer
- Donald B. Bloch
- Dong I. Lee
- Dongjian Hu
- Donté A. Stevens
- Doris Koesling
- Doris Koesling
- Doris Koesling
- Doris Koesling
- Doris Koesling
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- Sonia Donzelli
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- Stefan Hell
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- Stepan Gambaryan
- Stephan Rosenkranz
- Steven S. Pullen
- Stylianos Michalakis
- Susanne Feil
- Susanne Feil
- Susanne Kohl
- Susanne Krasemann
- Sylvia Nikkho
- Sylvie Bernier
- Sylvie G. Bernier
- Takashi Nojiri
- Takashi Nojiri
- Takashi Nojiri
- Takeshi Tokudome
- Takeshi Tokudome
- Tamás Radovits
- Thomas G. Oertner
- Thorsten Kessler
- Timothy Calamaras
- Tobias Bauch
- Tobias Peters
- Ulrich Walter
- Ulrike Scheib
- Ulrike Zimmermann
- V. Kaila
- Viacheslav O. Nikolaev
- Viacheslav O. Nikolaev
- Viacheslav O. Nikolaev
- Viacheslav O. Nikolaev
- Vikas Kapil
- Vineet Agrawal
- Vu Thao-Vi Dao
- Walter E. Haefeli
- Wendy Baur
- William R. Montfort
- Wilson A. Ferreira
- Wolfgang F. Graier
- Yasutake Tanaka
- Yigao Huang
- Ying-Ju Sung
- Yue Dai
- Yusu Gu
- Yutaka Suzuki
- Zhi Cheng Jing
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
This work was supported by a restricted research grant of Bayer AG
Search for the standard model Higgs boson in the diphoton decay channel with 4.9fb -1 of pp collision data at √s=7TeV with atlas
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- Zutshi V
- Zwalinski L
- Åkesson TPA
- Åsman B
- Publication venue
- Publication date
- 01/01/2012
- Field of study
A search for the standard model Higgs boson is performed in the diphoton decay channel. The data used correspond to an integrated luminosity of 4.9 fb-1 collected with the ATLAS detector at the Large Hadron Collider in proton-proton collisions at a center-of-mass energy of √s=7 TeV. In the diphoton mass range 110–150 GeV, the largest excess with respect to the background-only hypothesis is observed at 126.5 GeV, with a local significance of 2.8 standard deviations. Taking the look-elsewhere effect into account in the range 110–150 GeV, this significance becomes 1.5 standard deviations. The standard model Higgs boson is excluded at 95% confidence level in the mass ranges of 113–115 GeV and 134.5–136 GeV
Search for the standard model Higgs boson in the diphoton decay channel with 4.9fb -1 of pp collision data at √s=7TeV with atlas
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aenia T
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Aivković L
- Akdogan T
- Akimoto G
- Akimov AV
- Akiyama A
- Alam MA
- Alam MS
- 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
- Aliyev M
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amorós G
- 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
- Angerami A
- Anghinolfi F
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Aperio Bella L
- Apolle R
- Arabidze G
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- Åkesson TPA
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- Publication venue
- Publication date
- 01/01/2012
- Field of study
A search for the standard model Higgs boson is performed in the diphoton decay channel. The data used correspond to an integrated luminosity of 4.9 fb-1 collected with the ATLAS detector at the Large Hadron Collider in proton-proton collisions at a center-of-mass energy of √s=7 TeV. In the diphoton mass range 110–150 GeV, the largest excess with respect to the background-only hypothesis is observed at 126.5 GeV, with a local significance of 2.8 standard deviations. Taking the look-elsewhere effect into account in the range 110–150 GeV, this significance becomes 1.5 standard deviations. The standard model Higgs boson is excluded at 95% confidence level in the mass ranges of 113–115 GeV and 134.5–136 GeV
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