135 research outputs found
Subjective social status predicts long-term smoking abstinence
- Author
- A Agresti
- A Singh-Manoux
- Carlos A Mazas
- CJ Gwaltney
- D Operario
- Darla E Kendzor
- David W Wetter
- DW Wetter
- DW Wetter
- JI Vidrine
- JM Ostrove
- L Franzini
- L Radloff
- Lorraine R Reitzel
- LR Reitzel
- LR Reitzel
- LR Reitzel
- Ludmila Cofta-Woerpel
- M Fiore
- Michael S Businelle
- MJ McGowan
- MS Businelle
- N Adler
- N Adler
- NE Adler
- P Demakakos
- Paul M Cinciripini
- PD Allison
- PJ Gianaros
- S Shiffman
- S Shiffman
- S Shiffman
- SG Ghaed
- T Mendelson
- USDHHS
- Yessenia Castro
- Yisheng Li
- Yumei Cao
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
Design of a randomized controlled trial for multiple cancer risk behaviors among Spanish-speaking Mexican-origin smokers
- Author
- A Bandura
- A Bandura
- A Chiolero
- AD Goode
- AH Glassman
- AH Mokdad
- AS Hagler
- AV Wilkinson
- BH Marcus
- BL Burke
- C Greaves
- C MCCulloch
- C Ross
- CC DiClemente
- Centers for Disease Control and Prevention
- Centers for Disease Control and Prevention
- Centers for Disease Control and Prevention
- Centers for Disease Control and Prevention
- CJ Heckman
- CM Friedenreich
- CN Sciamanna
- D Watson
- David W Wetter
- DE Kendzor
- DP MacKinnon
- DW Wetter
- DW Wetter
- DW Wetter
- DW Wetter
- DW Wetter
- EG Eakin
- Elizabeth G Eakin
- ES Burgess
- FE Thompson
- G Block
- G Danaei
- G Verbeke
- GA Colditz
- GA Marlatt
- Group USCSW
- J Davis
- J Mata
- J Mirowsky
- J Mirowsky
- J Richert
- J Wardle
- JA Marrero
- JB McClure
- JO Prochaska
- JO Prochaska
- JO Prochaska
- JR Hughes
- JR Hughes
- K Basen-Engquist
- K Witkiewitz
- Karen Basen-Engquist
- Ken Resnicow
- KJ Palmer
- KM Carroll
- KM Carroll
- KM Emmons
- KM Emmons
- KM Emmons
- KM Emmons
- L Ries
- Larkin L Strong
- LC Gallo
- LC Larabie
- LR Reitzel
- M Fiore
- M Koring
- M Wu
- Maria E Fernandez
- MB Steinberg
- MK Hunt
- MN Silva
- MS Donaldson
- MS Fortier
- MS Webb
- N Mier
- National Heart L and Blood Institute
- NE Adler
- P Kreausukon
- P Westfall
- PM Cinciripini
- Prevention CfDCa
- R Diggle
- R Doll
- R Little
- R Ramirez
- R West
- RA Carels
- RE Glasgow
- RE Glasgow
- RE Glasgow
- RJ Shephard
- RK Martins
- S Cohen
- S Eldridge
- S Pocock
- S Pocock
- S Rubak
- S Shiffman
- S Thomas
- Services USDoHaH
- Services USDoHaH
- SM Hall
- SS Smith
- SY Lee
- T Bodenheimer
- T Bodenheimer
- United States Department of Health and Human Services
- W Miller
- W Miller
- W Miller
- WF Velicer
- WF Velicer
- WL Heppner
- Yessenia Castro
- Yisheng Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
Background: Smoking, poor diet, and physical inactivity account for as much as 60% of cancer risk. Latinos experience profound disparities in health behaviors, as well as the cancers associated with them. Currently, there is a dearth of controlled trials addressing these health behaviors among Latinos. Further, to the best of our knowledge, no studies address all three behaviors simultaneously, are culturally sensitive, and are guided by formative work with the target population. Latinos represent 14% of the U. S. population and are the fastest growing minority group in the country. Efforts to intervene on these important lifestyle factors among Latinos may accelerate the elimination of cancer-related health disparities
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- 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
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- 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
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aperio Bella L
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce AT
- Arfaoui S
- Arguin JF
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- ATLAS Collaboration The
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Backus Mayes J
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
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- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro Guimarães da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartsch V
- Basye A
- 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
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- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behar Harpaz S
- Belanger-Champagne C
- Bell PJ
- Bell WH
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- Beloborodova O
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
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- 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
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- Bernat P
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- Bernius C
- Bernlochner FU
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- Bertella C
- Bertin A
- Bertolucci F
- Besana MI
- Besjes GJ
- Besson N
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- Bhimji W
- Bianchi RM
- Bianchini L
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- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
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- Blair RE
- Blanchard JB
- Blazek T
- Bloch I
- Blocker C
- Blocki J
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boek TT
- Boelaert N
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Bohm J
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bomben M
- Bona M
- Boonekamp M
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borri M
- Borroni S
- Bortfeldt J
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
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- Bouchami J
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- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
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- Bozovic-Jelisavcic I
- Bracinik J
- Branchini P
- Brandt A
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- Brau B
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- Brazzale SF
- Brelier B
- Bremer J
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- Britton D
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- Brock I
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- Buckingham RM
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- Buda SI
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- Bundock AC
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
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- Butterworth JM
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- Caforio D
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- Calafiura P
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- Capeans Garrido MD
- Caprini I
- Caprini M
- Capriotti D
- Capua M
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- Cardarelli R
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- Carrillo-Montoya GD
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- Castillo Gimenez V
- Castro NF
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- Catastini P
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- Cattai A
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- Caughron S
- Cavaliere V
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chan K
- Chang P
- Chapleau B
- Chapman JD
- Chapman JW
- Charlton DG
- Chavda V
- Chavez Barajas CA
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen X
- Chen Y
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- Cheplakov A
- Cherkaoui El Moursli R
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
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- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Choudalakis G
- Chouridou S
- Chow BK
- Christidi IA
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- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
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- Coniavitis E
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- Czodrowski P
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- Côté D
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- Dabrowski W
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- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Asmundis R
- De Castro S
- De Cecco S
- de Graat J
- De Groot N
- de Jong P
- De La Taille C
- De la Torre H
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- De Nooij L
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- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demirkoz B
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deviveiros PO
- Dewhurst A
- Dewilde B
- Dhaliwal S
- Dhullipudi R
- Di Ciaccio A
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- Di Donato C
- Di Girolamo A
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- Diehl EB
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- Dionisi C
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- Djama F
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- do Vale MA
- Do Valle Wemans A
- Doan TK
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- Dodd J
- Doglioni C
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- Ferreira de Lima DE
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- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
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- Yildiz H Duran
- Yorita K
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- Yoshihara K
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- Youssef S
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- Yusuff I
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- Zaidan R
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- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
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- Zanzi D
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- Zeman M
- Zemla A
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- Zeng Q
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- Zenis T
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- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particle–hole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Performance of the ATLAS muon trigger in pp collisions at [Formula: see text] TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akimoto G
- Akimov AV
- Alberghi GL
- 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 BM
- Allison LJ
- Allport PP
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- 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
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aperio Bella L
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Araque JP
- Arce AT
- Arguin JF
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- ATLAS Collaboration
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Baas AE
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Backus Mayes J
- Badescu E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bannoura AA
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro Guimarães da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Bartsch V
- Bassalat A
- Basye A
- Bates RL
- Batley JR
- Battaglia M
- Battistin M
- Bauer F
- Bawa HS
- Beattie MD
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
- Becker S
- Beckingham M
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- Zurzolo G
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- Åkesson TP
- Åsman B
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- Publication venue
- Publication date
- 01/03/2015
- Field of study
The performance of the ATLAS muon trigger system is evaluated with proton-proton collision data collected in 2012 at the Large Hadron Collider at a centre-of-mass energy of 8 TeV. It is primarily evaluated using events containing a pair of muons from the decay of [Formula: see text] bosons. The efficiency of the single-muon trigger is measured for muons with transverse momentum [Formula: see text] GeV, with a statistical uncertainty of less than 0.01 % and a systematic uncertainty of 0.6 %. The [Formula: see text] range for efficiency determination is extended by using muons from decays of [Formula: see text] mesons, [Formula: see text] bosons, and top quarks. The muon trigger shows highly uniform and stable performance. The performance is compared to the prediction of a detailed simulation
Search for light top squark pair production in final states with leptons and b -jets with the ATLAS detector in s=7 TeV proton-proton collisions
- Author
- Aad G
- Abajyan T
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- Abdallah J
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- Publication venue
- Publication date
- 01/12/2012
- Field of study
The results of a search for pair production of light top squarks are presented, using 4.7 fb^-1 of sqrt(s) = 7 TeV proton-proton collisions collected with the ATLAS detector at the Large Hadron Collider. This search targets top squarks with masses similar to, or lighter than, the top quark mass. Final states containing exclusively one or two leptons (e, mu), large missing transverse momentum, light-jets and b-jets are used to reconstruct the top squark pair system. Global mass scale variables are used to separate the signal from a large ttbar background. No excess over the Standard Model expectations is found. The results are interpreted in the framework of the Minimal Supersymmetric Standard Model, assuming the top squark decays exclusively to a chargino and a b-quark. Light top squarks with masses between 123-167 GeV are excluded for neutralino masses around 55 GeV
Electron reconstruction and identification efficiency measurements with the ATLAS detector using the 2011 LHC proton–proton collision data
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
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- Alconada Verzini MJ
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- Alexa C
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- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yildirim E
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
Many of the interesting physics processes to be measured at the LHC have a signature involving one or more isolated electrons. The electron reconstruction and identification efficiencies of the ATLAS detector at the LHC have been evaluated using proton–proton collision data collected in 2011 at s√=7 TeV and corresponding to an integrated luminosity of 4.7 fb −1. Tag-and-probe methods using events with leptonic decays of W and Z bosons and J/ψ mesons are employed to benchmark these performance parameters. The combination of all measurements results in identification efficiencies determined with an accuracy at the few per mil level for electron transverse energy greater than 30 GeV
Search for Higgs and Z Boson Decays to J/ψγ and ϒ(nS)γ with the ATLAS Detector.
- Author
- (ATLAS Collaboration)
- Aad G
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akimoto G
- Akimov AV
- Alberghi GL
- 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
- Aloisio A
- Alonso A
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- Alpigiani C
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
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- Amidei D
- Amor Dos Santos SP
- Amorim A
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- Amundsen G
- Anastopoulos C
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- Andari N
- Andeen T
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- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
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- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
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- Armbruster AJ
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- Artamonov A
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- Asai S
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- Asquith L
- Assamagan K
- Astalos R
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- Atlay NB
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- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
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- Chernyatin V
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- Zurzolo G
- Zwalinski L
- Åkesson TPA
- Åsman B
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
A search for the decays of the Higgs and Z bosons to J/ψγ and ϒ(nS)γ (n=1,2,3) is performed with pp collision data samples corresponding to integrated luminosities of up to 20.3 fb^{-1} collected at sqrt[s]=8 TeV with the ATLAS detector at the CERN Large Hadron Collider. No significant excess of events is observed above expected backgrounds and 95% C.L. upper limits are placed on the branching fractions. In the J/ψγ final state the limits are 1.5×10^{-3} and 2.6×10^{-6} for the Higgs and Z boson decays, respectively, while in the ϒ(1S,2S,3S)γ final states the limits are (1.3,1.9,1.3)×10^{-3} and (3.4,6.5,5.4)×10^{-6}, respectively.We acknowledge the support of ANPCyT,
Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI,
Canada; CERN; CONICYT, Chile; CAS, MOST and
NSFC, China; COLCIENCIAS, Colombia; MSMT CR,MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/ IRFU, France; GNSF, Georgia; BMBF, DFG, HGF,
MPG and AvH Foundation, Germany; GSRT and
NSRF, Greece; ISF, MINERVA, GIF, I-CORE and
Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS,
Japan; CNRST, Morocco; FOM and NWO, Netherlands;BRF and RCN, Norway; MNiSW and NCN, Poland;GRICES and FCT, Portugal; MNE/IFA, Romania; MES of Russia and ROSATOM, Russian Federation; JINR;MSTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain;SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC,Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America
Search for resonances in diphoton events at √s = 13 TeV with the ATLAS detector
- Author
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- Zalieckas J
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- Zhemchugov A
- Zhong J
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- Zieminska D
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- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Searches for new resonances decaying into two photons in the ATLAS experiment at the CERN Large Hadron Collider are described. The analysis is based on proton-proton collision data corresponding to an integrated luminosity of 3.2 fb−1 at s√=13 TeV recorded in 2015. Two searches are performed, one targeted at a spin-2 particle of mass larger than 500 GeV, using Randall-Sundrum graviton states as a benchmark model, and one optimized for a spin-0 particle of mass larger than 200 GeV. Varying both the mass and the decay width, the most significant deviation from the background-only hypothesis is observed at a diphoton invariant mass around 750 GeV with local significances of 3.8 and 3.9 standard deviations in the searches optimized for a spin-2 and spin-0 particle, respectively. The global significances are estimated to be 2.1 standard deviations for both analyses. The consistency between the data collected at 13 TeV and 8 TeV is also evaluated. Limits on the production cross section times branching ratio to two photons for the two resonance types are reported
Measurements of top-quark pair differential cross-sections in the lepton plus jets channel in pp collisions at root s=8 TeV using the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam E Romero
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich L Cerda
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Aranda C Padilla
- Araque JP
- Araya S Tapia
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Measurements of normalized differential cross-sections of top-quark pair production are presented as a function of the top-quark, tt¯tt¯ system and event-level kinematic observables in proton–proton collisions at a centre-of-mass energy of s√=8TeVs=8TeV . The observables have been chosen to emphasize the tt¯tt¯ production process and to be sensitive to effects of initial- and final-state radiation, to the different parton distribution functions, and to non-resonant processes and higher-order corrections. The dataset corresponds to an integrated luminosity of 20.3 fb −1−1 , recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of the jets tagged as originating from a b-quark. The measured spectra are corrected for detector effects and are compared to several Monte Carlo simulations. The results are in fair agreement with the predictions over a wide kinematic range. Nevertheless, most generators predict a harder top-quark transverse momentum distribution at high values than what is observed in the data. Predictions beyond NLO accuracy improve the agreement with data at high top-quark transverse momenta. Using the current settings and parton distribution functions, the rapidity distributions are not well modelled by any generator under consideration. However, the level of agreement is improved when more recent sets of parton distribution functions are used
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