171 research outputs found
Performance of the 2017 and 2010 Revised McDonald Criteria in Predicting MS Diagnosis After a Clinically Isolated Syndrome: A MAGNIMS Study
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- Publication venue
- Publication date
- 04/01/2022
- Field of study
BACKGROUND AND OBJECTIVES: To compare the performance of the 2017 revisions to the McDonald criteria with the 2010 McDonald criteria in establishing MS diagnosis and predicting prognosis in patients with clinically isolated syndrome (CIS) suggestive of multiple sclerosis (MS). METHODS: CSF examination, brain and spinal cord MRI obtained ≤5 months from CIS onset, and a follow-up brain MRI acquired within 15 months from CIS onset were evaluated in 785 CIS patients from 9 European centers. Date of second clinical attack and of reaching Expanded Disability Status Score (EDSS) ≥ 3.0, if they occurred, were also collected. Performance of the 2017 and 2010 McDonald criteria for dissemination in space (DIS), time (DIT) (including oligoclonal bands assessment) and DIS + DIT for predicting a second clinical attack (clinically definite [CD] MS) and EDSS ≥ 3.0 at follow-up was evaluated. Time to MS diagnosis for the different criteria was also estimated. RESULTS: At follow-up (median = 69.1 months), 406/785 CIS patients developed CDMS. At 36 months, the 2017 DIS + DIT criteria had higher sensitivity (0.83 vs 0.66), lower specificity (0.39 vs 0.60) and similar area under the curve values (0.61 vs 0.63). Median time to MS diagnosis was shorter with the 2017 vs the 2010 or CDMS criteria (2017 revision = 3.2; 2010 revision = 13.0; CDMS = 58.5 months). The 2 sets of criteria similarly predicted EDSS ≥ 3.0 milestone. Three periventricular lesions improved specificity in patients ≥45 years. DISCUSSION: The 2017 McDonald criteria showed higher sensitivity, lower specificity and similar accuracy in predicting CDMS compared to 2010 McDonald criteria, while shortening time to diagnosis of MS. CLASSIFICATION OF EVIDENCE: This study provides Class II evidence that the 2017 McDonald Criteria more accurately distinguish CDMS in patients early after a CIS when compared to the 2010 McDonald criteria
Search for the standard model Higgs boson at LEP
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- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbiendi G
- Abdallah J
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- Trochimczuk M
- Trocme B
- Trocsanyi Z
- Troncon C
- Tsur E
- Tuchming B
- Tully C
- Tung KL
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- Tyapkin IA
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- Wyatt TR
- Wynhoff S
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- Xie Y
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- 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
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- 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
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
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- Adelman J
- Aderholz M
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- Aharrouche M
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- 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
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- 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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- Amako K
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- Anderson KJ
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- Angerami A
- Anghinolfi F
- Anh TV
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- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
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- Artamonov A
- Artoni G
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- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
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- Chikovani L
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- Chilingarov A
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- Chu ML
- Chudoba J
- Ciapetti G
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- Ciobotaru MD
- Cioccaa C
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- Codina EP
- Coe P
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- Coggeshall J
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- Cojocaru CD
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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
Short-stem reconstruction for megaendoprostheses in case of an ultrashort proximal femur
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
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
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- 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
All-sky search for gravitational-wave bursts in the second joint LIGO-Virgo run
- Author
- Abadie J
- Abbott BP
- Abbott R
- Abbott TD
- Abernathy M
- Accadia T
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- Zweizig Jang H
- Zweizig Jkiforov A.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We present results from a search for gravitational-wave bursts in the data
collected by the LIGO and Virgo detectors between July 7, 2009 and October 20,
2010: data are analyzed when at least two of the three LIGO-Virgo detectors are
in coincident operation, with a total observation time of 207 days. The
analysis searches for transients of duration < 1 s over the frequency band
64-5000 Hz, without other assumptions on the signal waveform, polarization,
direction or occurrence time. All identified events are consistent with the
expected accidental background. We set frequentist upper limits on the rate of
gravitational-wave bursts by combining this search with the previous LIGO-Virgo
search on the data collected between November 2005 and October 2007. The upper
limit on the rate of strong gravitational-wave bursts at the Earth is 1.3
events per year at 90% confidence. We also present upper limits on source rate
density per year and Mpc^3 for sample populations of standard-candle sources.
As in the previous joint run, typical sensitivities of the search in terms of
the root-sum-squared strain amplitude for these waveforms lie in the range 5
10^-22 Hz^-1/2 to 1 10^-20 Hz^-1/2. The combination of the two joint runs
entails the most sensitive all-sky search for generic gravitational-wave bursts
and synthesizes the results achieved by the initial generation of
interferometric detectors.Comment: 15 pages, 7 figures: data for plots and archived public version at
https://dcc.ligo.org/cgi-bin/DocDB/ShowDocument?docid=70814&version=19, see
also the public announcement at
http://www.ligo.org/science/Publication-S6BurstAllSky
Verticillium wilt of olive: a case study to implement an integrated strategy to control a soil-borne pathogen
- Author
- A Angiolillo
- A Collins
- A Collins
- A Gamliel
- A Hamblin
- A Klimes
- A Klimes
- A Matta
- A Morton
- A Morton
- A Porras-Soriano
- A Porras-Soriano
- A Porta-Puglia
- A Rodríguez-Lizana
- A Saeedizadeh
- A Saeedizadeh
- A Tantaoui
- A Trapero
- A Trapero
- A Vigouroux
- A Yildiz
- AE Arnold
- AG Baídez
- AG Levin
- AG Levin
- AG Levin
- AHC Van Bruggen
- AJ Termorshuizen
- AJM Rijkers
- AK Uppal
- AL Shigo
- AM Emechebe
- B Morera
- B Paul
- BA Latorre
- BA McDonald
- BJJ Lugtenberg
- BW Pennypacker
- C Colella
- C Eynck
- C Gayoso
- C Kalbe
- C Martos-Moreno
- C Navarro
- C Saydam
- CA Strausbaugh
- CA Strausbaugh
- CAN Okoli
- CC Thanassoulopoulos
- CC Thanassoulopoulos
- CC Thanassoulopoulos
- CH Beckman
- CL Xiao
- CL Xiao
- CR Howell
- D Haas
- D Rodríguez-Jurado
- D Zohary
- DC Harris
- DF Antonopoulos
- DG Zachos
- DJ Barbara
- DJ O’Sullivan
- DM Benson
- DM Huber
- DM Weller
- DR Duncan
- DR Fravel
- E Pérez-Artés
- E Pérez-Artés
- E Rodríguez
- E Rodríguez
- EA Markakis
- EA Markakis
- EC Tjamos
- EC Tjamos
- EC Tjamos
- EC Tjamos
- EC Tjamos
- EC Tjamos
- EC Tjamos
- EC Tjamos
- EF Fradin
- EJ Butterfield
- EK Ligoxigakis
- F Daayf
- F Nigro
- F Pérez-Jiménez
- FB Abeles
- FJ Gallego-Álvarez
- FJ López-Escudero
- FJ López-Escudero
- FJ López-Escudero
- FJ López-Escudero
- FJ López-Escudero
- FJ López-Escudero
- FJ López-Escudero
- FJ López-Escudero
- FJ López-Escudero
- Francisco Javier López-Escudero
- G Berg
- G Berg
- G Berg
- G Evans
- G Lazarovits
- G Ruggieri
- G Ruggieri
- GD Easton
- GE Harman
- GE Vallad
- GE Vallad
- GF Pegg
- GF Pegg
- GF Pegg
- GS Mahuku
- GS Mahuku
- H Dan
- H Hartman
- H Klebahn
- H Meschke
- H Saremi
- I Garmendia
- I Garmendia
- I Uremis
- J Bejarano-Alcázar
- J Bejarano-Alcázar
- J Bejarano-Alcázar
- J Fahleson
- J Frankowski
- J Huang
- J Katan
- J Katan
- J Levy
- J Mercado-Blanco
- J Mercado-Blanco
- J Mercado-Blanco
- J Mercado-Blanco
- J Mercado-Blanco
- J Mercado-Blanco
- J Robb
- J Robb
- J Robb
- JA Gómez
- JA Hiemstra
- JA Hiemstra
- JA Hiemstra
- JA Morillo
- JA Navas-Cortés
- JB Heale
- JB Taylor
- JC Goud
- JC Goud
- JC Goud
- JE DeVay
- JE Fernández
- Jesús Mercado-Blanco
- JF Leslie
- JH Carder
- JH Carder
- JM Caballero
- JM Caballero
- JM Raaijmakers
- JM Whipps
- JS Gerik
- JT Tippett
- JW Perry
- JW Perry
- K Elena
- K Elena
- K Hameed
- K Lachquer
- K Narisawa
- K Narisawa
- K Zeise
- KF Dobinson
- KF Dobinson
- KM El-Zik
- KN Li
- KN Li
- KV Subbarao
- L Civantos
- L Madi
- L Schena
- L Schena
- L Tsror
- L Tsror
- L Tsror
- L Zhou
- LC Mejía
- LE Datnoff
- LJ Toit
- LR Schreiber
- LS Thomashow
- LX Ran
- M Abu-Qamar
- M Arbogast
- M Bellahcene
- M Bellahcene
- M Bellahcene
- M Cherrab
- M Cherrab
- M Cirulli
- M Cirulli
- M Cirulli
- M Cirulli
- M Collado-Romero
- M Collado-Romero
- M Collado-Romero
- M Collado-Romero
- M Kamensky
- M Koike
- M Nagtzaam
- M Sarwar
- MA Al-Ahmad
- MA Blanco-López
- MA Blanco-López
- MA Blanco-López
- MA Typas
- MD García-Pedrajas
- ME Sánchez-Hernández
- MLV Resende
- MLV Resende
- MN Serrhini
- MR Karajeh
- MS Reddy
- MZ Tawil
- N Goicoechea
- N Ioannou
- N Karagiannidis
- N Kobra
- N Korolev
- N Korolev
- N Korolev
- N Korolev
- N Saitou
- O Erdogan
- O Manluk
- OC Huisman
- OC Huisman
- P Castillo
- P Prieto
- P Prieto
- P Rauyaree
- PP Antoniou
- PV Pramateftaki
- R Aragüés
- R Aragüés
- R Costa
- R Faggian
- R Hall
- R Heinz
- R Heinz
- R Messner
- R Moukhamedov
- R Vargas-Machuca
- RG Bhat
- RG Bhat
- RG Bhat
- RH Garber
- RH Garber
- RJ Cook
- RJ Green Jr
- RJ Rodríguez
- RJ Scheffer
- RJ Scheffer
- RM Jiménez-Díaz
- RM Jiménez-Díaz
- RM Jiménez-Díaz
- RN Nazar
- RS Utkhede
- S Alström
- S Dervis
- S Dervis
- S Dervis
- S Radišek
- S Wilhelm
- S Wilhelm
- S Wilhelm
- SA Deepak
- SD Leben
- SE Tjamos
- SG Edwards
- SJ Klosterman
- SJ Sanei
- SJ Sanei
- T Benítez
- T Volossiouk
- TB Morrison
- TC Paulitz
- TR Joaquim
- TR Joaquim
- VO Sadras
- VWL Jordan
- W Chen
- WA Sinclair
- WC Schnathorst
- WC Schnathorst
- WC Schnathorst
- WC Schnathorst
- WC Schnathorst
- WC Snyder
- WJ Blok
- X Hu
- X Zhengjun
- YL Tsai
- ZH Ma
- ZK Atallah
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
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
- Aracena I
- Arai Y
- Arce ATH
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barashkou A
- Barbaro Galtieri A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro Guimarães Da Costa J
- Barreiro F
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Bauer F
- Bawa HS
- Beale S
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker S
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behar Harpaz S
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Bell PJ
- Bell WH
- Bella G
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez Garcia JA
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertella C
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek T
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Bohm J
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bomben M
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borri M
- Borroni S
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
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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
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
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- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdesselam A
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- 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
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