629 research outputs found
Rare Z-decay into light CP-odd Higgs bosons: a comparative study in different new physics models
- Author
- A Arhrib
- A Arhrib
- A Belyaev
- A Dedes
- A Djouadi
- A Djouadi
- A Djouadi
- A Djouadi
- A Menon
- AG Akeroyd
- AG Akeroyd
- AG Akeroyd
- ALEPH collaboration
- BA Dobrescu
- C Amsler
- C BalĂĄzs
- C Panagiotakopoulos
- C Panagiotakopoulos
- C Panagiotakopoulos
- D Atwood
- D Buskulic
- D Chang
- D Das
- DJ Miller
- E Keith
- F Borzumati
- F Domingo
- F Franke
- F Larios
- F Larios
- G Abbiendi
- G Abbiendi
- G Abbiendi
- G Abbiendi
- G Altarelli
- G BĂ©langer
- G BĂ©langer
- G BĂ©langer
- G Hiller
- H-S Goh
- HE Logan
- J Abdallah
- J Abdallah
- J Cao
- J Cao
- J Cao
- J Cao
- J Cao
- J Dunkley
- J Kalinowski
- J Kurowska
- JF Gunion
- JF Gunion
- JF Gunion
- JF Gunion
- JI Illana
- Jin Min Yang
- JM Yang
- JR Ellis
- Junjie Cao
- K Cheung
- K Mönig
- K-m Cheung
- M Aoki
- M Davier
- M Drees
- M Krawczyk
- M Krawczyk
- M Krawczyk
- MA Perez
- MA Perez
- ME Peskin
- O Deschamps
- R Barate
- R Dermisek
- R Dermisek
- R Dermisek
- R Dermisek
- R Dermisek
- R Dermisek
- R Dermisek
- RM Barnett
- RM Barnett
- S Andreas
- S Schael
- S Su
- SP Martin
- T Besmer
- TJ Weiler
- U Ellwanger
- U Ellwanger
- U Ellwanger
- U Ellwanger
- V Barger
- V Barger
- X-G He
- X-G He
- Y Grossman
- Z Heng
- Zhaoxia Heng
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 07/11/2010
- Field of study
Various new physics models predict a light CP-odd Higgs boson (labeled as
a) and open up new decay modes for Z-boson, such as ZâfËâfa,
ZâaÎł and Zâaaa, which could be explored at the GigaZ option of
the ILC. In this work we investigate these rare decays in several new physics
models, namely the type-II two Higgs doublet model (type-II 2HDM), the
lepton-specific two Higgs doublet model (L2HDM), the nearly minimal
supersymetric standard model (nMSSM) and the next-to-minimal supersymmetric
standard model (NMSSM). We find that in the parameter space allowed by current
experiments, the branching ratios can reach 10â4 for ZâfËâfa
(f=b,Ï), 10â9 for ZâaÎł and 10â3 for Zâaaa, which
implies that the decays ZâfËâfa and Zâaaa may be accessible
at the GigaZ option. Moreover, since different models predict different
patterns of the branching ratios, the measurement of these rare decays at the
GigaZ may be utilized to distinguish the models.Comment: Version in JHEP (discussions added, errors corrected
Long-lived stops in MSSM scenarios with a neutralino LSP
- Author
- A Arbey
- A Dobrin
- A Heister
- A Riotto
- AC Kraan
- AC Kraan
- AG Cohen
- B Allanach
- C Amsler
- C BalĂĄzs
- D Choudhury
- D. Milstead
- E Komatsu
- GW Bennett
- HP Nilles
- J Abdallah
- J Abraham
- J Edsjo
- J. Edsjö
- JL Diaz-Cruz
- JL Feng
- JL Feng
- JL Hewett
- JR Ellis
- K-i Hikasa
- L Bergstrom
- LA Anchordoqui
- M Fairbairn
- M Muhlleitner
- M. Johansen
- P Abreu
- P Bechtle
- P Gondolo
- R Mackeprang
- R Mackeprang
- S Dawson
- S Kraml
- S. Hellman
- T Aaltonen
- T Aaltonen
- T Adams
- T Sjöstrand
- YR Boer de
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/03/2010
- Field of study
This work investigates the possibility of a long-lived stop squark in
supersymmetric models with the neutralino as the lightest supersymmetric
particle (LSP). We study the implications of meta-stable stops on the sparticle
mass spectra and the dark matter density. We find that in order to obtain a
sufficiently long stop lifetime so as to be observable as a stable R-hadron at
an LHC experiment, we need to fine tune the mass degeneracy between the stop
and the LSP considerably. This increases the stop-neutralino coanihilation
cross section, leaving the neutralino relic density lower than what is expected
from the WMAP results for stop masses ~1.5 TeV/c^2. However, if such scenarios
are realised in nature we demonstrate that the long-lived stops will be
produced at the LHC and that stop-based R-hadrons with masses up to 1 TeV/c^2
can be detected after one year of running at design luminosity
Light dark matter in the NMSSM: upper bounds on direct detection cross sections
- Author
- A Abulencia
- A Bottino
- A Bottino
- A Bottino
- AG Akeroyd
- AJ Buras
- ALEPH DELPHI, L3, OPAL, SLD, LEP Electroweak Working Group, SLD electroweak, heavy flavour groups collaborations
- B Aubert
- B Aubert
- B McElrath
- C Savage
- D Feldman
- D Hooper
- Debottam Das
- DG Cerdeno
- DG Cerdeno
- DS Akerib
- E Aprile
- E Komatsu
- E Kuflik
- F Domingo
- F Domingo
- F Domingo
- F Franke
- G Abbiendi
- G Angloher
- G BĂ©langer
- G BĂ©langer
- G BĂ©langer
- G BĂ©langer
- G BĂ©langer
- GW Bennett
- HK Dreiner
- J Abdallah
- J Angle
- J Cao
- J Cao
- J Kopp
- JF Gunion
- JF Gunion
- M Maniatis
- N Yokozaki
- R Bernabei
- R Dermisek
- R Dermisek
- S Demidov
- S Schael
- ST Lin
- T Aaltonen
- U Ellwanger
- U Ellwanger
- U Nierste
- Ulrich Ellwanger
- V Barger
- V Barger
- W Love
- Z Ahmed
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2010
- Field of study
In the Next-to-Minimal Supersymmetric Standard Model, a bino-like LSP can be
as light as a few GeV and satisfy WMAP constraints on the dark matter relic
density in the presence of a light CP-odd Higgs scalar. We study upper bounds
on the direct detection cross sections for such a light LSP in the mass range
2-20 GeV in the NMSSM, respecting all constraints from B-physics and LEP. The
OPAL constraints on e^+ e^- -> \chi^0_1 \chi^0_i (i > 1) play an important role
and are discussed in some detail. The resulting upper bounds on the
spin-independent and spin-dependent nucleon cross sections are ~ 10^{-42}
cm^{-2} and ~ 4\times 10^{-40} cm^{-2}, respectively. Hence the upper bound on
the spin-independent cross section is below the DAMA and CoGeNT regions, but
could be compatible with the two events observed by CDMS-II.Comment: 17 pages, 3 figure
Combining Anomaly and Z' Mediation of Supersymmetry Breaking
- Author
- A Anisimov
- A Anisimov
- A Manohar
- AD Linde
- AG Cohen
- B Murakami
- C Amsler
- CR Nappi
- DE Kaplan
- DE Kaplan
- DM Pierce
- GF Giudice
- GF Giudice
- Gil Paz
- H Georgi
- H Verlinde
- I Jack
- I Jack
- J Abdallah
- J Alwall
- J Alwall
- J Erler
- Jorge de Blas
- L Randall
- L Ălvarez-GaumĂ©
- Lian-Tao Wang
- M Baumgart
- M Dine
- M Dine
- M Dine
- M Dine
- MA Luty
- MA Luty
- MA Luty
- MA Luty
- P Fayet
- P Langacker
- P Langacker
- P Langacker
- P Langacker
- Paul Langacker
- R Blumenhagen
- R Sundrum
- S Kachru
- S Kachru
- SP Martin
- SP Martin
- SR Coleman
- T Gherghetta
- T Hahn
- T Kikuchi
- T Kikuchi
- TW Grimm
- V Barger
- Y Yamada
- Y Yamada
- Z Chacko
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 19/01/2010
- Field of study
We propose a scenario in which the supersymmetry breaking effect mediated by
an additional U(1)' is comparable with that of anomaly mediation. We argue that
such a scenario can be naturally realized in a large class of models. Combining
anomaly with Z' mediation allows us to solve the tachyonic slepton problem of
the former and avoid significant fine tuning in the latter. We focus on an
NMSSM-like scenario where U(1)' gauge invariance is used to forbid a tree-level
mu term, and present concrete models, which admit successful dynamical
electroweak symmetry breaking. Gaugino masses are somewhat lighter than the
scalar masses, and the third generation squarks are lighter than the first two.
In the specific class of models under consideration, the gluino is light since
it only receives a contribution from 2-loop anomaly mediation, and it decays
dominantly into third generation quarks. Gluino production leads to distinct
LHC signals and prospects of early discovery. In addition, there is a
relatively light Z', with mass in the range of several TeV. Discovering and
studying its properties can reveal important clues about the underlying model.Comment: Minor changes: references added, typos corrected, journal versio
A New Era in the Quest for Dark Matter
- Author
- A Arvanitaki
- A Boyarsky
- A Caldwell
- A GouvĂȘa de
- A Robertson
- A Robertson
- AG Riess
- B Abbott
- B Carr
- BC Lacki
- BJ Kavanagh
- BP Abbott
- CS Frenk
- D Erkal
- D Gaggero
- D George
- D Harvey
- D Harvey
- D Merritt
- Daniel Gilman
- DN Spergel
- E Bulbul
- EP Verlinde
- EW Kolb
- G Bertone
- G Bertone
- G Bertone
- G Bertone
- G Bertone
- G Despali
- GG Ross
- Gianfranco Bertone
- H Silverwood
- H Wang
- J Abdallah
- J Billard
- J Bovy
- J Goodman
- J Sakstein
- JD Bekenstein
- JG Swart de
- JH Yoon
- JW Moffat
- KN Abazajian
- L Berezhiani
- L Hui
- LF Abbott
- M Beekveld van
- M Beltran
- M Dine
- M Drewes
- M Kaplinghat
- M Laine
- M Milgrom
- M Oguri
- M Ricotti
- M Sasaki
- N Banik
- N Dalal
- N Du
- P Athron
- P Gondolo
- PAR Ade
- PW Graham
- R Brito
- R Essig
- R Essig
- RB Metcalf
- RG Carlberg
- S Bird
- S Boran
- S Caron
- S Clesse
- S Knapen
- S Mao
- S Tulin
- S Vegetti
- SM Koushiappas
- SW Randall
- T Brinckmann
- T Daylan
- TE Jeltema
- Tim M. P. Tait
- V IrĆĄiÄ
- V IrĆĄiÄ
- VK Narayanan
- X-D Shi
- Y Ali-HaĂŻmoud
- Y Hochberg
- Y Hochberg
- Y Kahn
- YD Hezaveh
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/10/2018
- Field of study
There is a growing sense of `crisis' in the dark matter community, due to the
absence of evidence for the most popular candidates such as weakly interacting
massive particles, axions, and sterile neutrinos, despite the enormous effort
that has gone into searching for these particles. Here, we discuss what we have
learned about the nature of dark matter from past experiments, and the
implications for planned dark matter searches in the next decade. We argue that
diversifying the experimental effort, incorporating astronomical surveys and
gravitational wave observations, is our best hope to make progress on the dark
matter problem.Comment: Published in Nature, online on 04 Oct 2018. 13 pages, 1 figur
Ferritins: furnishing proteins with iron
- Author
- A Crow
- A Treffry
- AG Frey
- CC Philpott
- DM Lawson
- DM Lawson
- E Wajnberg
- EC Theil
- EC Theil
- EC Theil
- EC Theil
- EI Stiefel
- ER Bauminger
- F BarcelĂł
- F Bou-Abdallah
- FA Fischbach
- FA Fischbach
- FH Kadir
- FHA Kadir
- GC Ford
- GC Papaefthymiou
- GD Watt
- GD Watt
- Geoffrey R. Moore
- GR Moore
- H Abdul-Tehrani
- H Aitken-Rogers
- H Shi
- H Yao
- H Yao
- H Yao
- J Yariv
- J-F Ma
- JD LĂłpez-Castro
- JD Mancias
- JM Bradley
- JM Bradley
- JS Rohrer
- Justin M. Bradley
- L Swartz
- L Toussaint
- MA Quail
- MJ OâConnell
- ML Vasil
- MR Cheesman
- ND Chasteen
- NE Brun Le
- NE Brun Le
- NE Brun Le
- Nick E. Le Brun
- NM Reid
- O Sadeghi
- P Arosio
- P Doig
- PD Hempstead
- PL Ringeling
- PM Harrison
- PM Harrison
- RF Boyer
- RJ Ward
- RK Behera
- RP Garg
- S Bereswill
- S Granick
- S Granick
- S Levi
- S Macedo
- S Mann
- S Mann
- S Pfaffen
- SC Andrews
- SC Andrews
- SG Wong
- SK Weeratunga
- T Asano
- T Douglas
- T Jones
- T Tosha
- TJ Stillman
- TV OâHalloran
- TZ Kidane
- V Laufberger
- VJ Wade
- WH Massover
- X Liu
- X Yang
- Y Ha
- Y Wang
- YH Pan
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Ferritins are a superfamily of iron oxidation, storage and mineralization proteins found throughout the animal, plant, and microbial kingdoms. The majority of ferritins consist of 24 subunits that individually fold into 4-α-helix bundles and assemble in a highly symmetric manner to form an approximately spherical protein coat around a central cavity into which an iron-containing mineral can be formed. Channels through the coat at inter-subunit contact points facilitate passage of iron ions to and from the central cavity, and intrasubunit catalytic sites, called ferroxidase centers, drive Fe2+ oxidation and O2 reduction. Though the different members of the superfamily share a common structure, there is often little amino acid sequence identity between them. Even where there is a high degree of sequence identity between two ferritins there can be major differences in how the proteins handle iron. In this review we describe some of the important structural features of ferritins and their mineralized iron cores and examine in detail how three selected ferritins oxidise Fe2+ in order to explore the mechanistic variations that exist amongst ferritins. We suggest that the mechanistic differences reflect differing evolutionary pressures on amino acid sequences, and that these differing pressures are a consequence of different primary functions for different ferritins
Testing new physics with the electron g-2
- Author
- A Czarnecki
- A Czarnecki
- A Lusiani
- A Masiero
- A Masiero
- A Petermann
- A Petermann
- AG Cohen
- B Aubert
- B Aubert
- B Aubert
- B Aubert
- B Aubert
- B Aubert
- B Aubert
- B Aubert
- B Bellazzini
- B Keren-Zur
- B Krause
- C Lazzeroni
- CM Sommerfield
- CM Sommerfield
- D Britton
- D Hanneke
- D Hanneke
- D MaĂźtre
- E Remiddi
- F Jegerlehner
- G Bennett
- G Bennett
- G Czapek
- G. F. Giudice
- GA Gonzalez-Sprinberg
- GF Giudice
- H Brown
- I Masina
- J Abdallah
- J Adam
- J Beringer
- J Bernabeu
- J Bernabeu
- J Girrbach
- J Hisano
- J Hisano
- J Lees
- JP Leveille
- JS Schwinger
- K Hagiwara
- K Hayasaka
- K Hayasaka
- M Antonelli
- M Cadoret
- M Leurer
- M Passera
- M Passera
- M Raidal
- M. Passera
- P Clade
- P Krawczyk
- P Mohr
- P Paradisi
- P. Paradisi
- PH Chankowski
- PH Chankowski
- R Bouchendira
- R Dyck Van
- S Dimopoulos
- S Eidelman
- S Laporta
- S Laporta
- S Laporta
- S Laporta
- S Schael
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Aoyama
- T Gehrmann
- T Gehrmann
- T Kinoshita
- U Ellwanger
- V Gerginov
- Y Grossman
- Y Miyazaki
- Y Miyazaki
- Y Miyazaki
- Y Miyazaki
- Y Miyazaki
- Y Nir
- Y Nishio
- YK Semertzidis
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
We argue that the anomalous magnetic moment of the electron (a_e) can be used
to probe new physics. We show that the present bound on new-physics
contributions to a_e is 8*10^-13, but the sensitivity can be improved by about
an order of magnitude with new measurements of a_e and more refined
determinations of alpha in atomic-physics experiments. Tests on new-physics
effects in a_e can play a crucial role in the interpretation of the observed
discrepancy in the anomalous magnetic moment of the muon (a_mu). In a large
class of models, new contributions to magnetic moments scale with the square of
lepton masses and thus the anomaly in a_mu suggests a new-physics effect in a_e
of (0.7 +- 0.2)*10^-13. We also present examples of new-physics theories in
which this scaling is violated and larger effects in a_e are expected. In such
models the value of a_e is correlated with specific predictions for processes
with violation of lepton number or lepton universality, and with the electric
dipole moment of the electron.Comment: 34 pages, 7 figures. Minor changes and references adde
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
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros 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
- Anh TV
- Anjos N
- Annovi A
- 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
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- 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
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou 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 F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck GA
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- 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
- Boeriu OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Bracinik J
- Braem A
- Branchini P
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brown H
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- BScher V
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
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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 âs = 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 pTâ„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 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{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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- Zitoun R
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- 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 of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at âs = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- Atlay NB
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescua E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bailey DC
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- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
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- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
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- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
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- Bartsch V
- Bassalat A
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- Batley JR
- Battistin M
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- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
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- Beckingham M
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
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- Castillo IS
- Castillo LRF
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- Castro NF
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- Cortes-Gonzalez A
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- Da Via C
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- De Nooij L
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- De Regie JBDV
- de Renstrom PAB
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- Delsart PA
- Deluca C
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- Demilly A
- Demirkoz B
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- Derue F
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- Deviveiros PO
- Dewhurst A
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
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- Di Simone A
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- Djama F
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- Dueren M
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- Dwuznik M
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- Ehrenfeld W
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- Ekelof T
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- El Moursli A
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- Emeliyanov D
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- Enari Y
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- Engelmann R
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- Erdmann J
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- Ereditato A
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- Eriksson D
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- Ernis G
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- Ernst J
- Ernst J
- Ernst M
- Ernst M
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- Errede D
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- Errede S
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- Ertel E
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- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
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- Fabbri L
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- Facini G
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- Fakhrutdinov RM
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- Faltova J
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- Fang Y
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- Farooque T
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- Farrell S
- Farrell S
- Farrington SM
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- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
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- Fassouliotis D
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- Favareto A
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- Fayard L
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- Federic P
- Federic P
- Fedin OL
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- Fedorko W
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- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
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- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
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- Fenyuk AB
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- Fernando W
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- Ferrag S
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- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
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- Ferrari A
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- Ferrari P
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- Ferretti C
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- Fiascaris M
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- Fiedler F
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- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
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- Fincke-Keeler M
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- Fiolhais MCN
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- Fiorini L
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- Firan A
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- Fisher MJ
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- Fitzgerald EA
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- Fleck I
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- Fleischmann P
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- Fleischmann S
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- Fletcher G
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- Fletcher GT
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- Floderus A
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- Florez Bustos AC
- Flowerdew MJ
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- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
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- Fournier D
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- Francavilla P
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- Francis D
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- Franklin M
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- Franz S
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- Fraternali M
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- French ST
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- Friedrich C
- Friedrich F
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- Fulsom BG
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- Gabizon O
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- Gabrielli A
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- Gadatsch S
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- Gadomski S
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- Gagliardi G
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- Gagnon P
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- Galea C
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- Galhardo B
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- Gallas EJ
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- Gallo V
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- Gallop BJ
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- Gallus P
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- Gao J
- Gao YS
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- Gaob J
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- Garcia Navarro JE
- Garcia BRM
- Garcia C
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- Garcia JAB
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- Gardner RW
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- Garelli N
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- Garonne V
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- Garrido MDMC
- Gatti C
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- Gaudio G
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- Gaur B
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- Gauzzi P
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- Gavrilenko IL
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- Gay C
- Gay C
- Gaycken G
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- Gazis EN
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- Ge P
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- Gecse Z
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- Gee CNP
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- Geerts DAA
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- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
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- Gemme C
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- Gemmell A
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- Genest MH
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- Gentile S
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- George M
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- George S
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- Gerbaudo D
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- Gershon A
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- Ghazlane H
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- Ghodbane N
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- Giacobbe B
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- Giagu S
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- Giangiobbe V
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- Giannetti P
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- Gillam TPS
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- Gingrich DM
- Gingrich M
- Giokaris N
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- Giordani MP
- Giordani MP
- Giordano R
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- Giraud PF
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- Giugni D
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- Giuliani C
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- Giunta M
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- Gjelsten BK
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- Gordon HA
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- Gorelov I
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- Gorini B
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- Gorini E
- Gorini E
- Gorisek A
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of âs = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentreâofâmassframeisusedtosuppressthelargemultiâjetbackground.ThecrossâsectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
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