122 research outputs found
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- 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
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
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- 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
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
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
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- Aloisio A
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- Yilmaz M
- Yoosootiniya R
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- Zhemchugov A
- Zheng S
- Zhong J
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- Zhu CG
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- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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- Zsenei A
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- Zwalinski L
- 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 cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Zanello L
- Zarzhitsky P
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- Zhemchugov A
- Zheng S
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- Zhu H
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- 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
FCC Physics Opportunities: Future Circular Collider Conceptual Design Report Volume 1
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abramov A
- Aburaia M
- Acar AO
- Adzic PR
- Agrawal P
- Aguilar-Saavedra JA
- Aguilera-Verdugo JJ
- Ahnen JV
- Aiba M
- Aichinger I
- Aielli G
- Akay A
- Akhundov A
- Aksakal H
- Alaniz EC
- Albacete JL
- Albergo S
- Alekou A
- Aleksa M
- Aleksan R
- Alexahin Y
- Alia RG
- Alioli S
- Allanach BC
- Allport PP
- Altinli M
- Altmannshofer W
- Amann RW
- Ambrosio G
- Amorim D
- Amstutz O
- Anderlini L
- Andreazza A
- Andreini M
- Andriatis A
- Andris C
- Andronic A
- Angelucci M
- Antinori F
- Antipov SA
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- Appleby RB
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- Asai S
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- Astapovych D
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- Chaikovska I
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- de Vivie de Regie JB
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- Deghaye S
- Delikaris D
- Deliot F
- Dell'Acqua A
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- Demarteau M
- Denegri D
- Deniau L
- Denisov D
- Denizli H
- Denner A
- Derue F
- Deschamps O
- Descotes-Genon S
- Dev PSB
- Dewanjee RK
- Di Cicco A
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- Diaz VG
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- Doblhammer A
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- Dordei F
- Drago A
- Draper P
- Drasal Z
- Drewes M
- Duarte L
- Dubovyk I
- Duca VD
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- Dziewit B
- Eisenhardt S
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- Ellis J
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- Weiland C
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- Widorski M
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- Wienands H-U
- Wilkinson G
- Williams PH
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- Wojton T
- Wollmann D
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- Woog D
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- Wulzer A
- Yanehsari MK
- Yanehsari MK
- Yang G
- Yang HJ
- Yao W-M
- Yazgan E
- Yermolchik V
- Yildiz HD
- Yilmaz A
- Yilmaz A
- Yoo H-D
- Yost SA
- You T
- Young C
- Yu F
- Yu T-T
- Zaborowska A
- Zadeh SG
- Zadeh SG
- Zahnd M
- Zanetti M
- Zanotto L
- Zawiejski L
- Zeiler P
- Zerlauth M
- Zernov SM
- Zevi Dell Porta G
- Zhang C
- Zhang H
- Zhang Y
- Zhang Z
- Zhao Z
- Zhong Y-M
- Zhou D
- Zhou J
- Zhuang P
- Zick G
- Zimmermann F
- Zinn-Justin J
- Zivkovic L
- Zlobin AV
- Zobov M
- Zupan J
- Zurita J
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/06/2019
- Field of study
We review the physics opportunities of the Future Circular Collider, covering its e+e-, pp, ep and heavy ion programmes. We describe the measurement capabilities of each FCC component, addressing the study of electroweak, Higgs and strong interactions, the top quark and flavour, as well as phenomena beyond the Standard Model. We highlight the synergy and complementarity of the different colliders, which will contribute to a uniquely coherent and ambitious research programme, providing an unmatchable combination of precision and sensitivity to new physics
HE-LHC: The High-Energy Large Hadron Collider: Future Circular Collider Conceptual Design Report Volume 4
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abelleira Fernandez J
- Abramov A
- Aburaia M
- Acar AO
- Adzic PR
- Agrawal P
- Aguilar-Saavedra JA
- Aguilera-Verdugo JJ
- Aiba M
- Aichinger I
- Aielli G
- Akay A
- Akhundov A
- Aksakal H
- Albacete JL
- Albergo S
- Alekou A
- Aleksa M
- Aleksan R
- Alemany Fernandez RM
- Alexahin Y
- Alia RG
- Alioli S
- Alipour Tehrani N
- Allanach BC
- Allport PP
- Altinli M
- Altmannshofer W
- Ambrosio G
- Amorim D
- Amstutz O
- Anderlini L
- Andreazza A
- Andreini M
- Andriatis A
- Andris C
- Andronic A
- Angelucci M
- Antinori F
- Antipov SA
- Antonelli M
- Antonello M
- Antonioli P
- Antusch S
- Anulli F
- Apolinario L
- Apollinari G
- Apollonio A
- Appeloe D
- Appleby RB
- Apyan A
- Apyan A
- Arbey A
- Arbuzov A
- Arduini G
- Ari V
- Arias S
- Armesto N
- Arnaldi R
- Arsenyev SA
- Arzeo M
- Asai S
- Aslanides E
- Assmann RW
- Astapovych D
- Atanasov M
- Atieh S
- Attie D
- Auchmann B
- Audurier A
- Aull S
- Aumon S
- Aune S
- Avino F
- Avrillaud G
- Aydin G
- Azatov A
- Azuelos G
- Azzi P
- Azzolini O
- Azzurri P
- Bacchetta N
- Bacchiocchi E
- Bachacou H
- Baek YW
- Baglin V
- Bai Y
- Baird S
- Baker MJ
- Baldwin MJ
- Ball AH
- Ballarino A
- Banerjee S
- Barber DP
- Barducci D
- Barjhoux P
- Barna D
- Barnafoldi GG
- Barnes MJ
- Barr A
- Barranco Garcia J
- Barreiro Guimaraes da Costa J
- Bartmann W
- Baryshevsky V
- Barzi E
- Bass SA
- Bastianin A
- Baudouy B
- Bauer F
- Bauer M
- Baumgartner T
- Bautista-Guzman I
- Bayindir C
- Beaudette F
- Bedeschi F
- Beguin M
- Bellafont I
- Bellagamba L
- Bellegarde N
- Belli E
- Bellingeri E
- Bellini F
- Bellomo G
- Belomestnykh S
- Bencivenni G
- Benedikt M
- Bernardi G
- Bernardi J
- Bernet C
- Bernhardt JM
- Bernini C
- Berriaud C
- Bertarelli A
- Bertolucci S
- Besana MI
- Besancon M
- Beznosov O
- Bhat C
- Bhat P
- Biagini ME
- Biarrotte J-L
- Bibet Chevalier A
- Bielert ER
- Biglietti M
- Bilei GM
- Bilki B
- Biscari C
- Bishara F
- Blanco-Garcia OR
- Blanquez FR
- Blekman F
- Blondel A
- Bluemlein J
- Boccali T
- Boels R
- Bogacz SA
- Bogomyagkov A
- Boine-Frankenheim O
- Boland MJ
- Bologna S
- Bolukbasi O
- Bomben M
- Bondarenko S
- Bonvini M
- Boos E
- Bordini B
- Bordry F
- Borghello G
- Borgonovi L
- Borowka S
- Bortoletto D
- Boscherini D
- Boscolo M
- Boselli S
- Bosley RR
- Bossu F
- Botta C
- Bottura L
- Boughezal R
- Boutin D
- Bovone G
- Bozbey A
- Bozovic Jelisavic I
- Bozzi C
- Bozzini D
- Braccini V
- Braibant-Giacomelli S
- Bramante J
- Braun-Munzinger P
- Briffa JA
- Britzger D
- Brodsky SJ
- Brooke JJ
- Bruce R
- Bruckman De Renstrom P
- Bruna E
- Bruning O
- Brunner K
- Brunner O
- Bruzzone P
- Buffat X
- Bulyak E
- Burkart F
- Burkhardt H
- Burnet J-P
- Butin F
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- Caccia M
- Cai Y
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- Cairo V
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- Caliskan A
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- Carra F
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- Casas J
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- Chaikovska I
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- Chevalier L
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- Childers JT
- Chmielinska A
- Cholakian A
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- Dubovyk I
- Duda P
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- Hernandez-Sanchez J
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- Honorato CG
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- Iconomidou-Fayard L
- Ilyina-Brunner K
- Incandela J
- Infantino A
- Ippolito V
- Ishino M
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- Ita H
- Ivanovs A
- Iwamoto S
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- Izquierdo Bermudez S
- Jadach S
- Jamin DO
- Janot P
- Jarry P
- Jeff A
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- Jensen E
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- Jiang X
- Jimenez JM
- Jones MA
- Jones OR
- Jowett JM
- Jung S
- Kaabi W
- Kado M
- Kahle K
- Kalinovskaya L
- Kalinowski J
- Kamenik JF
- Kannike K
- Kara SO
- Karadeniz H
- Karaventzas V
- Karpov I
- Kartal S
- Karyukhin A
- Kashikhin V
- Katharina Behr J
- Kaya U
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- Keinz PA
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- Kershaw K
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- Khatiri Yanehsari M
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- Kieseler J
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- Kolomiets AA
- Komppula J
- Koop I
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- Korjik M
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- Kuhlmann G
- Kulesza A
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- Landsberg G
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- Lenzi P
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- Leon-Monzon I
- Leonidopoulos C
- Lerner G
- Leroy O
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- Leveratto A
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- Locci E
- Logothetis Agaliotis E
- Lombardo MP
- Long AJ
- Lorin C
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- Louzguiti A
- Low I
- Lucchesi D
- Lucchini MT
- Luciani A
- Lueckhof M
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- Lyubimtsev DA
- Maggiora M
- Magnin N
- Mahmoud MA
- Mahmoudi F
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- Makarenko V
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- Malyshev OB
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- Mandrik P
- Manfrinetti P
- Mangano M
- Manil P
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- Marchiori G
- Marhauser F
- Mariani V
- Marinozzi V
- Mariotto S
- Marquard P
- Marquet C
- Marriott-Dodington T
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- Martin O
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- Martinez-Hernandez MI
- Martins DE
- Marzani S
- Marzocca D
- Marzola L
- Masciocchi S
- Masina I
- Massimiliano A
- Massironi A
- Masubuchi T
- Matveev VA
- Mazzoni MA
- McCullough M
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- Meade P
- Medina L
- Meier A
- Meignan J
- Mele B
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- Mertens V
- Mether L
- Metral E
- Migliorati M
- Milanese A
- Milardi C
- Milhano G
- Militsyn BL
- Millet F
- Minashvili I
- Minervini JV
- Miralles LS
- Mirarchi D
- Mishima S
- Missiaen DP
- Mitselmakher G
- Mitshuhashi T
- Mnich J
- Mohammadi Najafabadi M
- Mohapatra RN
- Mokhov N
- Molson JG
- Monge R
- Montag C
- Montagna G
- Monteil S
- Montenero G
- Montesinos E
- Moortgat F
- Morange N
- Morello G
- Moreno Llacer M
- Moretti M
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- Morley AK
- Moros A
- Morozov I
- Morretta V
- Morrone M
- Mostacci A
- Muanza S
- Muchnoi N
- Mueller A-S
- Mueller F
- Muhlegger M
- Mulder M
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- Muller B
- Munilla J
- Murray MJ
- Muttoni Y
- Myers S
- Mylona M
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- Nakamoto T
- Nardecchia M
- Nardini G
- Nason P
- Nergiz Z
- Nesterenko AV
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- Neubuser C
- Neundorf J
- Niccoli F
- Nicrosini O
- Nie Y
- Niedermayer U
- Niedziela J
- Niemi A
- Nikitin SA
- Nisati A
- No JM
- Nonis M
- Nosochkov Y
- Novak M
- Novokhatski A
- O'Callaghan JM
- Ochando C
- Ogur S
- Ohmi K
- Oide K
- Okorokov VA
- Okumura Y
- Oleari C
- Olness FI
- Onel Y
- Ortino M
- Osborne J
- Osland P
- Otto T
- Oyulmaz KY
- Ozansoy A
- Ozcan V
- Ozdemir K
- Pagliarone CE
- Pais da Silva HF
- Palmieri E
- Palumbo L
- Pampaloni A
- Pan R-Q
- Panareo M
- Panella O
- Panico G
- Panizzo G
- Pankov AA
- Pantsyrny V
- Papadopoulos CG
- Papaefstathiou A
- Papaphilippou Y
- Parker MA
- Parma V
- Pasquali M
- Patra SK
- Patterson R
- Paukkunen H
- Pauss F
- Peggs S
- Penttinen J-P
- Peon G
- Perepelkin EE
- Perez Codina E
- Perez Morales J
- Perez E
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- Perez JC
- Perfilov M
- Pernegger H
- Peruzzi M
- Pes C
- Peters K
- Petracca S
- Petriello F
- Pezzotti L
- Pfeiffer S
- Piccinini F
- Pieloni T
- Pierini M
- Pikhartova H
- Pikurs G
- Pilicer E
- Piminov P
- Pira C
- Pittau R
- Placzek W
- Plagge M
- Plehn T
- Pleier M-A
- Ploskon M
- Podeur M
- Podlech H
- Podzorny T
- Poggioli L
- Poiron A
- Polesello G
- Poli Lener M
- Polini A
- Polinski J
- Polozov SM
- Ponce L
- Pont M
- Pontecorvo L
- Portaluri T
- Potamianos K
- Prasse C
- Prausa M
- Preinerstorfer A
- Premat E
- Price T
- Primavera M
- Prino F
- Prioli M
- Proudfoot J
- Provino A
- Pugnat T
- Pukhaeva N
- Pulawski S
- Pulikowski D
- Punzi G
- Putti M
- Pyarelal A
- Quack H
- Quispe M
- Racioppi A
- Rafique H
- Raginel V
- Raidal M
- Ramirez-Uribe NS
- Ramsey-Musolf MJ
- Rata R
- Ratoff P
- Ravotti F
- Rebello Teles P
- Reboud M
- Redaelli S
- Renner E
- Renteria-Olivo AE
- Rescigno M
- Reuter J
- Ribon A
- Ricci AM
- Riegler W
- Riemann B
- Riemann S
- Riemann T
- Rifflet JM
- Rimmer RA
- Rinaldesi R
- Rinolfi L
- Rios Rubiras O
- Risselada T
- Rivetti A
- Rivkin L
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- Romanov A
- Roncarolo F
- Rosado Sanchez A
- Rosaz G
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- Rossmanith R
- Rousset B
- Royon C
- Ruan X
- Ruehl I
- Ruhlmann-Kleider V
- Ruiz R
- Rumyantsev L
- Ruprecht R
- Ryazanov AI
- Saba A
- Sadykov R
- Saez de Jauregui D
- Sahin M
- Sailer B
- Saito M
- Sala F
- Salam GP
- Salfeld-Nebgen J
- Salgado CA
- Salini S
- Sallese JM
- Salmi T
- Salzburger A
- Sampayo OA
- Sanfilippo S
- Santiago J
- Santopinto E
- Santoro R
- Sanz Ull A
- Sarasola X
- Sarpun IH
- Sauvain M
- Savelyeva S
- Sawada R
- Sborlini GFR
- Schaffer A
- Schaumann M
- Schenk M
- Scheuerlein C
- Schienbein I
- Schlenga K
- Schmickler H
- Schmidt R
- Schoerling D
- Schoerner-Sadenius T
- Schoning A
- Schott M
- Schulte D
- Schwaller P
- Schwanenberger C
- Schwemling P
- Schwerg N
- Scibile L
- Sciuto A
- Scomparin E
- Sebastiani C
- Seeber B
- Segreti M
- Selva P
- Selvaggi M
- Senatore C
- Senol A
- Serin L
- Serluca M
- Serra N
- Seryi A
- Sestini L
- Sfyrla A
- Shaposhnikov M
- Shaposhnikova E
- Sharkov BY
- Shatilov D
- Shelton J
- Shiltsev V
- Shipsey IP
- Shirkov GD
- Shivaji A
- Shwartz D
- Sian T
- Sidorov S
- Siemko A
- Silvestrini L
- Simand N
- Simon F
- Singh BK
- Siodmok A
- Sirois Y
- Sirtori E
- Sirvinskaite R
- Sitar B
- Sjostrand T
- Skands P
- Skordis E
- Skovpen K
- Skrzypek M
- Slade E
- Slavich P
- Slovak R
- Smaluk V
- Smirnov V
- Snoeys W
- Soffi L
- Sollander P
- Solovyanov O
- Soltveit HK
- Song H
- Sopicki P
- Sorbi M
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- Spiesberger H
- Spiller P
- Spira M
- Srivastava T
- Stachel J
- Stakia A
- Stanyard JL
- Starchenko E
- Starikov AY
- Stasto AM
- Statera M
- Steerenberg R
- Steggemann J
- Stenvall A
- Stivanello F
- Stoeckinger D
- Stoeger-Pollach M
- Stoel LS
- Strauss B
- Stuart M
- Stupakov G
- Su S
- Sublet A
- Sugita K
- Sulak L
- Sullivan MK
- Sultansoy S
- Sumida T
- Suzuki K
- Sylva G
- Syphers MJ
- Sznajder A
- Taborelli M
- Tahir NA
- Takeuchi M
- Tal Hod E
- Tambasco C
- Tanaka J
- Tang K
- Tapan I
- Taroni S
- Tartarelli GF
- Tassielli G
- Tavian L
- Taylor GN
- Taylor TM
- Teixeira AM
- Tejeda-Munoz G
- Telnov VI
- ten Kate HHJ
- Tenchini R
- Terashi K
- Tesi A
- Testa M
- Tetrel C
- Teytelman D
- Thaler J
- Thamm A
- The FCC Collaboration
- Thomas S
- Tiirakari MT
- Tikhomirov V
- Tikhonov D
- Timko H
- Tisserand V
- Tkachenko LM
- Tkaczuk J
- Tock JP
- Todd B
- Todesco E
- Tomas Garcia R
- Tommasini D
- Tonelli G
- Toral F
- Torims T
- Torre R
- Townsend Z
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- Tricomi A
- Trischuk W
- Tropin IS
- Tuchming B
- Tudora AA
- Turbiarz B
- Turk Cakir I
- Turri M
- Tydecks T
- Usovitsch J
- Uythoven J
- Vaglio R
- Valassi A
- Valchkova F
- Valdivia Garcia MA
- Vale Silva L
- Valente P
- Valente RU
- Valente-Feliciano A-M
- Valentino G
- Valet JM
- Valizadeh R
- Valle JWF
- Vallecorsa S
- Vallone G
- van Leeuwen M
- van Rienen UH
- van Riesen-Haupt L
- Varasteh M
- Vecchi L
- Vedrine P
- Velev G
- Veness R
- Ventura A
- Venturini Delsolaro W
- Verducci M
- Verhaaren CB
- Vernieri C
- Verweij AP
- Verwilligen O
- Viazlo O
- Vicini A
- Viehhauser G
- Vignaroli N
- Vignolo M
- Vitrano A
- Vivarelli I
- Vlachos S
- Voelkl V
- Vogel M
- Vogt DM
- Volkov P
- Volpini G
- von Ahnen J
- Vorotnikov G
- Voutsinas GG
- Vysotsky V
- Wagner U
- Wallny R
- Wang K
- Wang L-T
- Wang R
- Ward BFL
- Watson NK
- Watson TP
- Weiland C
- Weinzierl S
- Welsch CP
- Wenninger J
- Widorski M
- Wiedemann UA
- Wienands H-U
- Wilkinson G
- Williams PH
- Winter A
- Wohlfahrt A
- Wojton T
- Wollmann D
- Womersley J
- Woog D
- Ws Z
- Wu X
- Wulzer A
- Yanehsari MK
- Yang G
- Yang HJ
- Yao W-M
- Yazgan E
- Yermolchik V
- Yilmaz A
- Yilmaz A
- Yoo H-D
- Yost SA
- You T
- Young C
- Yu F
- Yu T-T
- Zaborowska A
- Zadeh SG
- Zahnd M
- Zanetti M
- Zanotto L
- Zawiejski L
- Zeiler P
- Zerlauth M
- Zernov SM
- Zevi Dell Porta G
- Zhang C
- Zhang H
- Zhang Y
- Zhang Z
- Zhao Z
- Zhong Y-M
- Zhou D
- Zhou J
- Zhuang P
- Zick G
- Zimmermann F
- Zinn-Justin J
- Zivkovic L
- Zlobin AV
- Zobov M
- Zupan J
- Zurita J
- Publication venue
- SPRINGER HEIDELBERG
- Publication date
- 01/07/2019
- Field of study
In response to the 2013 Update of the European Strategy for Particle Physics (EPPSU), the Future Circular Collider (FCC) study was launched as a world-wide international collaboration hosted by CERN. The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the third volume of the FCC Conceptual Design Report, devoted to the hadron collider FCC-hh. It summarizes the FCC-hh physics discovery opportunities, presents the FCC-hh accelerator design, performance reach, and staged operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation. Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the FCC-hh design aims at significantly extending the energy frontier to 100 TeV. Its unprecedented centre-of-mass collision energy will make the FCC-hh a unique instrument to explore physics beyond the Standard Model, offering great direct sensitivity to new physics and discoveries
FCC-ee: The Lepton Collider: Future Circular Collider Conceptual Design Report Volume 2
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abramov A
- Aburaia M
- Acar AO
- Adzic PR
- Agaliotis EL
- Agrawal P
- Aguilar-Saavedra JA
- Aguilera-Verdugo JJ
- Aiba M
- Aichinger I
- Aielli G
- Akay A
- Akhundov A
- Aksakal H
- Alaniz EC
- Albacete JL
- Albergo S
- Alekou A
- Aleksa M
- Aleksan R
- Alexahin Y
- Alia RG
- Alioli S
- Allanach BC
- Allport PP
- Altinli M
- Altmannshofer W
- Ambrosio G
- Amorim D
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- Andreazza A
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- Andriatis A
- Andris C
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- Yang G
- Yang HJ
- Yao W-M
- Yazgan E
- Yermolchik V
- Yildiz HD
- Yilmaz A
- Yilmaz A
- Yoo H-D
- Yost SA
- You T
- Young C
- Yu F
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- Zaborowska A
- Zadeh SG
- Zadeh SG
- Zahnd M
- Zanetti M
- Zanotto L
- Zawiejski L
- Zeiler P
- Zerlauth M
- Zernov SM
- Zhang C
- Zhang H
- Zhang Y
- Zhang Z
- Zhao Z
- Zhong Y-M
- Zhou D
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- Zhuang P
- Zick G
- Zimmermann F
- Zinn-Justin J
- Zivkovic L
- Zlobin AV
- Zobov M
- Zupan J
- Zurita J
- Publication venue
- SPRINGER HEIDELBERG
- Publication date
- 01/06/2019
- Field of study
In response to the 2013 Update of the European Strategy for Particle Physics, the Future Circular Collider (FCC) study was launched, as an international collaboration hosted by CERN. This study covers a highest-luminosity high-energy lepton collider (FCC-ee) and an energy-frontier hadron collider (FCC-hh), which could, successively, be installed in the same 100 km tunnel. The scientific capabilities of the integrated FCC programme would serve the worldwide community throughout the 21st century. The FCC study also investigates an LHC energy upgrade, using FCC-hh technology. This document constitutes the second volume of the FCC Conceptual Design Report, devoted to the electron-positron collider FCC-ee. After summarizing the physics discovery opportunities, it presents the accelerator design, performance reach, a staged operation scenario, the underlying technologies, civil engineering, technical infrastructure, and an implementation plan. FCC-ee can be built with today’s technology. Most of the FCC-ee infrastructure could be reused for FCC-hh. Combining concepts from past and present lepton colliders and adding a few novel elements, the FCC-ee design promises outstandingly high luminosity. This will make the FCC-ee a unique precision instrument to study the heaviest known particles (Z, W and H bosons and the top quark), offering great direct and indirect sensitivity to new physics
FCC-hh: The Hadron Collider: Future Circular Collider Conceptual Design Report Volume 3
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abelleira Fernandez J
- Abramov A
- Aburaia M
- Acar AO
- Adzic PR
- Agrawal P
- Aguilar-Saavedra JA
- Aguilera-Verdugo JJ
- Aiba M
- Aichinger I
- Aielli G
- Akay A
- Akhundov A
- Aksakal H
- Albacete JL
- Albergo S
- Alekou A
- Aleksa M
- Aleksan R
- Alemany Fernandez RM
- Alexahin Y
- Alia RG
- Alioli S
- Alipour Tehrani N
- Allanach BC
- Allport PP
- Altinli M
- Altmannshofer W
- Ambrosio G
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- Andreazza A
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- Andriatis A
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- Andronic A
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- Bellini F
- Bellomo G
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- Fernandez-Tellez A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 18/12/2018
- Field of study
In response to the 2013 Update of the European Strategy for Particle Physics (EPPSU), the Future Circular Collider (FCC) study was launched as a world-wide international collaboration hosted by CERN. The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the third volume of the FCC Conceptual Design Report, devoted to the hadron collider FCC-hh. It summarizes the FCC-hh physics discovery opportunities, presents the FCC-hh accelerator design, performance reach, and staged operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation. Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the FCC-hh design aims at significantly extending the energy frontier to 100 TeV. Its unprecedented centre of-mass collision energy will make the FCC-hh a unique instrument to explore physics beyond the Standard Model, offering great direct sensitivity to new physics and discoveries
HE-LHC: The High-Energy Large Hadron Collider
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abelleira Fernandez J
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 18/12/2018
- Field of study
In response to the 2013 Update of the European Strategy for Particle Physics (EPPSU), the Future Circular Collider (FCC) study was launched as a world-wide international collaboration hosted by CERN. The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the third volume of the FCC Conceptual Design Report, devoted to the hadron collider FCC-hh. It summarizes the FCC-hh physics discovery opportunities, presents the FCC-hh accelerator design, performance reach, and staged operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation. Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the FCC-hh design aims at significantly extending the energy frontier to 100 TeV. Its unprecedented centre-of-mass collision energy will make the FCC-hh a unique instrument to explore physics beyond the Standard Model, offering great direct sensitivity to new physics and discoveries
FCC-hh: The Hadron Collider: Future Circular Collider Conceptual Design Report Volume 3
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abelleira Fernandez J
- Abramov A
- Aburaia M
- Acar AO
- Adzic PR
- Agrawal P
- Aguilar-Saavedra JA
- Aguilera-Verdugo JJ
- Aiba M
- Aichinger I
- Aielli G
- Akay A
- Akhundov A
- Aksakal H
- Albacete JL
- Albergo S
- Alekou A
- Aleksa M
- Aleksan R
- Alemany Fernandez RM
- Alexahin Y
- Alia RG
- Alioli S
- Alipour Tehrani N
- Allanach BC
- Allport PP
- Altinli M
- Altmannshofer W
- Ambrosio G
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- Amstutz O
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- Andriatis A
- Andris C
- Andronic A
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- Publication venue
- SPRINGER HEIDELBERG
- Publication date
- 01/07/2019
- Field of study
In response to the 2013 Update of the European Strategy for Particle Physics (EPPSU), the Future Circular Collider (FCC) study was launched as a world-wide international collaboration hosted by CERN. The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the third volume of the FCC Conceptual Design Report, devoted to the hadron collider FCC-hh. It summarizes the FCC-hh physics discovery opportunities, presents the FCC-hh accelerator design, performance reach, and staged operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation. Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the FCC-hh design aims at significantly extending the energy frontier to 100 TeV. Its unprecedented centre of-mass collision energy will make the FCC-hh a unique instrument to explore physics beyond the Standard Model, offering great direct sensitivity to new physics and discoveries
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
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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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