367 research outputs found
DNA damage by lipid peroxidation products: implications in cancer, inflammation and autoimmunity
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2017
- Field of study
Oxidative stress and lipid peroxidation (LPO) induced by inflammation, excess metal storage and excess caloric intake cause generalized DNA damage, producing genotoxic and mutagenic effects. The consequent deregulation of cell homeostasis is implicated in the pathogenesis of a number of malignancies and degenerative diseases. Reactive aldehydes produced by LPO, such as malondialdehyde, acrolein, crotonaldehyde and 4-hydroxy-2-nonenal, react with DNA bases, generating promutagenic exocyclic DNA adducts, which likely contribute to the mutagenic and carcinogenic effects associated with oxidative stress-induced LPO. However, reactive aldehydes, when added to tumor cells, can exert an anticancerous effect. They act, analogously to other chemotherapeutic drugs, by forming DNA adducts and, in this way, they drive the tumor cells toward apoptosis. The aldehyde-DNA adducts, which can be observed during inflammation, play an important role by inducing epigenetic changes which, in turn, can modulate the inflammatory process. The pathogenic role of the adducts formed by the products of LPO with biological macromolecules in the breaking of immunological tolerance to self antigens and in the development of autoimmunity has been supported by a wealth of evidence. The instrumental role of the adducts of reactive LPO products with self protein antigens in the sensitization of autoreactive cells to the respective unmodified proteins and in the intermolecular spreading of the autoimmune responses to aldehyde-modified and native DNA is well documented. In contrast, further investigation is required in order to establish whether the formation of adducts of LPO products with DNA might incite substantial immune responsivity and might be instrumental for the spreading of the immunological responses from aldehyde-modified DNA to native DNA and similarly modified, unmodified and/or structurally analogous self protein antigens, thus leading to autoimmunity
Coexistence of the spin-density-wave and superconductivity in the (Ba,K)Fe2As2
- Author
- Chen G. F.
- Ding H.
- Dong J.
- G. Wu
- H. Chen
- Liu C. Samolyuk G. D. Lee Y. Ni N. Kondo T. Santander-Syro A. F. Budko S. L. McChesney J. L. Rotenberg E. Valla T.
- Luetkens H. Klauss H.-H. Kraken M. Litterst F. J. Dellmann T. Klingeler R. Hess C. Khasanov R. Amato A. Baines C.
- Margadonna S. Takabayashi Y. McDonald M. T. Brunelli M. Wu G. Liu R. H. Chen X. H. Prassides K.
- Q. Huang
- R. H. Liu
- Ren Z. A.
- Ren Z. A.
- Ren Z.-A.
- Rotter M. Pangerl M. Tegel M. Johrendt D.
- T. Wu
- Takeshita S. Ryosuke Kadono M. H. Miyazaki M. Koda A. Kamihara Y. Hosono H.
- Wang C.
- Wei Bao
- Wu G.
- X. F. Wang
- X. H. Chen
- Y. L. Xie
- Y. Qiu
- Y. Ren
- Yang L. X. Ou H. W. Zhao J. F. Zhang Y. Shen D. W. Zhou B. Wei J. Chen F. Xu M. He C. et al
- Zhao J. Huang Q. de la Cruz C. Li S. Lynn J. W. Chen Y. Green M. A. Chen G. F. Li G. Li Z.
- Zhao L.
- Publication venue
- 'IOP Publishing'
- Publication date
- 24/07/2008
- Field of study
The relation between the spin-density-wave (SDW) and superconducting order is
a central topic in current research on the FeAs-based high Tc superconductors.
Conflicting results exist in the LaFeAs(O,F)-class of materials, for which
whether the SDW and superconductivity are mutually exclusive or they can
coexist has not been settled. Here we show that for the (Ba,K)Fe2As2 system,
the SDW and superconductivity can coexist in an extended range of compositions.
The availability of single crystalline samples and high value of the energy
gaps would make the materials a model system to investigate the high Tc
ferropnictide superconductivity.Comment: 4 pages, 5 figure
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Zhemchugov 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
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Cancer Biomarker Discovery: The Entropic Hallmark
- Author
- A Alcaraz
- A Arabzadeh
- A Bagri
- A Balbin
- A Bantis
- A Ben-Naim
- A Bolander
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- W Weichert
- W Weichert
- WB Isaacs
- WD Dunsmuir
- WE Naugler
- William C. S. Cho
- WK Kaufmann
- WK Lee
- X Chen
- X Cheng
- X Dong
- X Dong
- X Huang
- X Li
- X Liu
- X Liu
- X Meng
- X Ouyang
- X Tang
- X Wu
- X Zhang
- XJ Yang
- XQ Wang
- Y Bu
- Y Cai
- Y Deng
- Y Ito
- Y Katagiri
- Y Kozuka
- Y Lai
- Y Liu
- Y Lu
- Y Lu
- Y Ohyama
- Y Shav-Tal
- Y Sugiyama
- Y Sun
- Y Wang
- Y Wang
- Y Wu
- Y Yamamoto
- Y Yang
- Y Zhou
- YB Lim
- YC Chao
- YJ Ko
- YL Liu
- YN Liu
- YT Sasaki
- YT Sasaki
- YU Katagiri
- Z Jiang
- Z Jiang
- Z Jiang
- Z Jiang
- Z Jiang
- Z Rudzki
- ZA Dotan
- ZR Yurkovetsky
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Background: It is a commonly accepted belief that cancer cells modify their transcriptional state during the progression of the disease. We propose that the progression of cancer cells towards malignant phenotypes can be efficiently tracked using high-throughput technologies that follow the gradual changes observed in the gene expression profiles by employing Shannon's mathematical theory of communication. Methods based on Information Theory can then quantify the divergence of cancer cells' transcriptional profiles from those of normally appearing cells of the originating tissues. The relevance of the proposed methods can be evaluated using microarray datasets available in the public domain but the method is in principle applicable to other high-throughput methods. Methodology/Principal Findings: Using melanoma and prostate cancer datasets we illustrate how it is possible to employ Shannon Entropy and the Jensen-Shannon divergence to trace the transcriptional changes progression of the disease. We establish how the variations of these two measures correlate with established biomarkers of cancer progression. The Information Theory measures allow us to identify novel biomarkers for both progressive and relatively more sudden transcriptional changes leading to malignant phenotypes. At the same time, the methodology was able to validate a large number of genes and processes that seem to be implicated in the progression of melanoma and prostate cancer. Conclusions/Significance: We thus present a quantitative guiding rule, a new unifying hallmark of cancer: the cancer cell's transcriptome changes lead to measurable observed transitions of Normalized Shannon Entropy values (as measured by high-throughput technologies). At the same time, tumor cells increment their divergence from the normal tissue profile increasing their disorder via creation of states that we might not directly measure. This unifying hallmark allows, via the the Jensen-Shannon divergence, to identify the arrow of time of the processes from the gene expression profiles, and helps to map the phenotypical and molecular hallmarks of specific cancer subtypes. The deep mathematical basis of the approach allows us to suggest that this principle is, hopefully, of general applicability for other diseases
Invasive cells in animals and plants: searching for LECA machineries in later eukaryotic life
- Author
- A Abo
- A Berken
- A Das
- A Geitmann
- A Geitmann
- A Gupta
- A Hall
- A Hall
- A Hendrix
- A Kodama
- A Li
- A Lovy-Wheeler
- A Schwarz
- A Tabuchi
- AA Woollard
- AG Simpson
- AH Hutagalung
- AI Prokhnevsky
- AJ Molendijk
- AJ Ridley
- AK Mongiu
- AL Szumlanski
- AM Craig
- AM Pooler
- AM Weaver
- AP Barnes
- AR Strohmaier
- AS Howell
- AY Cheung
- AY Cheung
- B Diaz
- B Kost
- B Kost
- B Leitinger
- BC Gibbon
- BH de Graaf
- BJ Sieberer
- BK McMichael
- BL Goode
- C Albertinazzi
- C Viotti
- CD Moore
- CD Nobes
- CG Dotti
- CG Koh
- CH Woo
- CL Leung
- CL Wymer
- CM Yoo
- CM Yoo
- CW Pak
- D Basu
- D Gianni
- D Gianni
- D Goryunov
- D Lingwood
- D Pommereit
- D Vignjevic
- DA Murphy
- Daniel Rösel
- DB Szymanski
- DB Szymanski
- DH Schott
- DJ Hernandez-Deviez
- DJ Hernandez-Deviez
- E Forster
- E Giannoni
- E Gouin
- E Michard
- E Mucha
- ED Goley
- EE Govek
- EL Ojangu
- EM Lord
- EN Firat-Karalar
- ES Anton
- ET Bowden
- ET Bowden
- F Baluska
- F Bradke
- F Bradke
- F Causeret
- F Cvrckova
- F Cvrckova
- F Cvrckova
- F Korobova
- F Lizarraga
- F Palacios
- F Rivero
- F Simon-Plas
- Fatima Cvrčková
- FB Daher
- FC de Anda
- FC de Anda
- FW Pfrieger
- G Cai
- G Caldieri
- G Caldieri
- G Fishell
- G Gallo
- G Kronenberg
- G Lalli
- G Lalli
- G Wu
- GA Banker
- GA Strasser
- GB Monshausen
- GB Monshausen
- H Kamata
- H Kassai
- H Li
- H Nakahara
- H Nakahara
- H Ren
- H Stenmark
- H Wu
- H Yamaguchi
- H Yamaguchi
- H Yamaguchi
- H Yamaguchi
- HR Bourne
- HR Bourne
- I Ayala
- J Foreman
- J Liu
- J Morel
- J Ng
- J Noritake
- J Peranen
- J Schiefelbein
- J Ye
- Jan Brábek
- JG Donaldson
- JJ Bravo-Cordero
- JK Song
- JR Dickinson
- K Bedard
- K Chae
- K Kikuchi
- K Letinic
- K Suzukawa
- K Vissenberg
- K Yi
- K Zhou
- KA Kennedy
- Katarína Vaškovičová
- KM Valentijn
- L Camacho
- L Camacho
- L Chen
- L Chen
- L Jadeski
- L Luo
- L Shapiro
- L Sosa
- L Synek
- L Vidali
- L Vidali
- L Wang
- L Yakir-Tamang
- L Zhou
- LA Elias
- LJ Pike
- LJ Winship
- M Baldassarre
- M Elias
- M Grunt
- M Hala
- M Iwano
- M Ko
- M Lavy
- M Lorenz
- M Malartre
- M Mazzone
- M Megias
- M Meriane
- M Oser
- M Otsuki
- M Ovecka
- M Potocky
- M Potocky
- M Sagi
- M Sakurai-Yageta
- M Schoumacher
- M Stiess
- M Tsatmali
- M Tsatmali
- M Valiente
- MA del Pozo
- MA Tischfield
- Margaret Nikolič
- ME Nielsen
- MF Hanzal-Bayer
- MF Olson
- MJ Allen
- MJ Deeks
- MJ Deeks
- MJ Kwon
- ML Preuss
- ML Preuss
- N Arimura
- N Asada
- N Balasubramanian
- N Gupta
- N Kebdani
- N Sorek
- N Thapa
- N Xu
- NG Pasteris
- NR Jog
- O Gossot
- O Hazak
- O Reiner
- O Tolde
- P Caroni
- P Liu
- P Niethammer
- P Novick
- PC Coelho
- PT Caswell
- Q Duan
- R Ahuja
- R Buccione
- R Harel
- R Janostiak
- R Pleskot
- R Poincloux
- RA Arkowitz
- RA Cole
- RJ Carol
- RJ Carol
- Roberto Buccione
- S Cappello
- S Corbetta
- S Cudmore
- S Dupraz
- S Etienne-Manneville
- S Hakeda-Suzuki
- S Hashimoto
- S Katoh
- S Katoh
- S Li
- S Linder
- S Linder
- S Locke
- S Muallem
- S Nagawa
- S Rakic
- S Robert
- S Swanson
- S Tahirovic
- S Takeda
- S Wang
- S Yalovsky
- SC Mueller
- SC Mueller
- SC Noctor
- SC Noctor
- SD Harris
- SE Tague
- SH Shiu
- SJ Heasman
- SK Singh
- T Chen
- T Golub
- T Ischebeck
- T Ischebeck
- T Jacobs
- T Kawauchi
- T Kelly
- T Ketelaar
- T Matusek
- T Sapir
- T Shu
- T Tanaka
- T Xu
- TC Spor
- TE Stradal
- TN Bibikova
- TN Bibikova
- U Fischer
- U Fischer
- V Gongidi
- V Munnamalai
- V Muralidharan-Chari
- V Zarsky
- V Zarsky
- Viktor Žárský
- VL Koumandou
- VV Peremyslov
- VV Peremyslov
- VV Peremyslov
- VV Peremyslov
- W Wagner
- W Zheng
- WL Monsky
- WT Chen
- WT Chen
- X Wu
- X Xu
- X Zuo
- XF Song
- Y Bao
- Y Boutte
- Y Fu
- Y Miyamoto
- Y Mori
- Y Wang
- Y Zhang
- Z Kouchi
- Z Xie
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of the cross section for inclusive isolated-photon production in pp collisions at √s=13TeV using the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araya ST
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barajas CAC
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo JT
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becker M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behr JK
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertram IA
- Bertsche C
- Besjes GJ
- Bessner M
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bilokon H
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Bisanz T
- Bittrich C
- Bjergaard DM
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blunier D
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boehler M
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
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- Boscherini D
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- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozson AJ
- Bracinik J
- Brandt A
- Brandt G
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- Brau JE
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- Brennan AJ
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- Bristow TM
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- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
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- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
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- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13TeVis studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2fb−1. The cross section is measured as a function of the photon transverse energy above 125GeVin different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data
Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
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- Acharya BS
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- Adelman J
- Adomeit S
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- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
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- Aielli G
- Akerstedt H
- Akesson TP
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
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- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
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- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
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- Alviggi MG
- Amako K
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- Antonaki A
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- Zhemchugov A
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- Zimmermann C
- Zimmermann R
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- Zobernig G
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- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5 fb[superscript −1] of proton-proton collisions data at √s=7 TeV and 20.3 fb[superscript −1] at √s=8 TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be μ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4 GeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be μ[subscript ggF]=1.32±0.38, μ[subscript VBF]=0.8±0.7, μ[subscript WH]=1.0±1.6, μ[subscript ZH]=0.1[superscript +3.7 subscript −0.1], and μ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript −1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Measurement of W+W− production in association with one jet in proton–proton collisions at sqrt(s) = 8TeV with the ATLAS detector
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- Aad G
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- Abdallah J
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- Zhemchugov A
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- Zibell A
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- Zimmermann C
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- Zinonos Z
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- Zivkovic L
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- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
The production of W boson pairs in association with one jet in pp collisions at View the MathML sources=8 TeV is studied using data corresponding to an integrated luminosity of 20.3 fb−1 collected by the ATLAS detector during 2012 at the CERN Large Hadron Collider. The cross section is measured in a fiducial phase-space region defined by the presence of exactly one electron and one muon, missing transverse momentum and exactly one jet with a transverse momentum above 25 GeV and a pseudorapidity of |η|<4.5|η|<4.5. The leptons are required to have opposite electric charge and to pass transverse momentum and pseudorapidity requirements. The fiducial cross section is found to be View the MathML sourceσWWfid,1-jet=136±6(stat)±14(syst)±3(lumi) fb. In combination with a previous measurement restricted to leptonic final states with no associated jets, the fiducial cross section of WW production with zero or one jet is measured to be View the MathML sourceσWWfid,≤1-jet=511±9(stat)±26(syst)±10(lumi) fb. The ratio of fiducial cross sections in final states with one and zero jets is determined to be 0.36±0.050.36±0.05. Finally, a total cross section extrapolated from the fiducial measurement of WW production with zero or one associated jet is reported. The measurements are compared to theoretical predictions and found in good agreement
Search for dark matter at √s=13 TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb−1 of proton–proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, model-independent limits are set on the fiducial cross section for the production of events in this final state. Exclusion limits are also placed in models where dark-matter candidates are pair-produced. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750–1200 GeV for dark-matter candidate masses below 230–480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale M∗ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to Zγ and the Z boson subsequently decays into neutrinos
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