443 research outputs found
Taming open/closed string duality with a Losev trick
- Author
- A-K Kashani-Poor
- Alessandro Tanzini
- AN Todorov
- Andrea Prudenziati
- C Imbimbo
- D Krefl
- D Krotov
- E Witten
- E Witten
- E Witten
- G Bonelli
- G Bonelli
- Giulio Bonelli
- H Ooguri
- H Ooguri
- J Walcher
- K Hori
- K Kodaira
- L Martucci
- M Alim
- M Bershadsky
- M Henneaux
- N Berkovits
- N Berkovits
- NP Warner
- PLH Cook
- PLH Cook
- R Dijkgraaf
- R Gopakumar
- V Bouchard
- V Bouchard
- V Pestun
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2010
- Field of study
A target space string field theory formulation for open and closed B-model is
provided by giving a Batalin-Vilkovisky quantization of the holomorphic
Chern-Simons theory with off-shell gravity background. The target space
expression for the coefficients of the holomorphic anomaly equation for open
strings are obtained. Furthermore, open/closed string duality is proved from a
judicious integration over the open string fields. In particular, by
restriction to the case of independence on continuous open moduli, the shift
formulas of [7] are reproduced and shown therefore to encode the data of a
closed string dual.Comment: 22 pages, no figures; v.2 Refs. and a comment added
The effect of tightly-bound water molecules on scaffold diversity in computer-aided de novo ligand design of CDK2 inhibitors
- Author
- AC Pierce
- AD Westwell
- AE Gibson
- Alfonso T. GarcĂa-Sosa
- AM Davis
- AT GarcĂa_Sosa
- CS Poornima
- DB Cherbavaz
- DG Lloyd
- E Chung
- GA Breault
- HM Berman
- IR Hardcastle
- J Moravec
- JB Finley
- JF Beattie
- JM Chen
- KL Sayle
- L Shewchuk
- M Anderson
- M Hendlich
- M Knockaert
- M Pastor
- M Rarey
- M Stahl
- MR Wester
- NP Todorov
- NP Todorov
- NS Gray
- P Pospisil
- PA Rejto
- PYS Lam
- Ricardo L. Mancera
- RL Mancera
- RN Misra
- SL McGovern
- TG Davies
- TJ Marrone
- U Schulze-Gahmen
- V Krystof
- V Mikol
- V Schnecke
- WA Metz
- WF Azevedo de
- Z KrĂz
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2006
- Field of study
We have determined the effects that tightly bound water molecules have on the de novo design of cyclin-dependent kinase-2 (CDK2) ligands. In particular, we have analyzed the impact of a specific structural water molecule on the chemical diversity and binding mode of ligands generated through a de novo structure-based ligand generation method in the binding site of CDK2. The tightly bound water molecule modifies the size and shape of the binding site and we have found that it also imposed constraints on the observed binding modes of the generated ligands. This in turn had the indirect effect of reducing the chemical diversity of the underlying molecular scaffolds that were able to bind to the enzyme satisfactorily
The deuteron: structure and form factors
- Author
- A Amghar
- A Buchmann
- A Farkas
- A Gokalp
- A Huber
- A Kobushkin
- A Kobushkin
- A Pellegrino
- AA Logunov
- AY Umnikov
- B Boden
- B Desplanques
- B Grossette
- BB VoÄtsekhovskiÄ
- BD Keister
- C Herberg
- C Ordonez
- C Ordonez
- C Ordonez
- CCD Atti
- CD Buchanan
- CE Carlson
- CE Carlson
- CF Perdrisat
- CW Wong
- D Abbott
- D Abbott
- D Abbott
- D Allasia
- D Benaksas
- D Ganichot
- D Pitz
- D PlĂŒmper
- DB Day
- DB Kaplan
- DB Kaplan
- DB Kaplan
- DB Kaplan
- DG Crabb
- DH Barkhuff
- DJ Beachey
- DJ Drickey
- DM Bishop
- DM Nikolenko
- DO Riska
- DO Riska
- DR Phillips
- DR Phillips
- E Epelbaum
- E Epelbaum
- E Epelbaum
- E Faassen van
- E Faassen van
- E Faassen van
- E Fermi
- E Fermi
- E Fermi
- E Hummel
- E Majorana
- ED Cooper
- EE Salpeter
- EG Kessler
- EM Lev
- EM Lev
- EM Nyman
- EP Wigner
- EP Wigner
- ER Cohen
- F Cardarelli
- F DiFilippo
- F Gross
- F Gross
- F Gross
- F Gross
- F Gross
- F Gross
- F Gross
- F Iachello
- F Martin
- F Villars
- FA Bumiller
- FM Lev
- FM Lev
- FM Lev
- G Breit
- G Höhler
- GE Brown
- GG Simon
- GG Simon
- GM Murphy
- GN Lewis
- GR Farrar
- H Henning
- H Ito
- H Ito
- H Yukawa
- HA Bethe
- HA Bethe
- HA Bethe
- HC Urey
- I Sick
- I The
- II Rabi
- IM Sitnik
- IT Todorov
- J Adam
- J Adam Jr.
- J Arvieux
- J Cameron
- J Carbonell
- J Carbonell
- J Carbonell
- J Carbonell
- J Carbonell
- J Carlson
- J Chadwick
- J Fleischer
- J Fleischer
- J Fleischer
- J Goldemberg
- J Gunion
- J Martorell
- JA McIntyre
- JC Ward
- JE Elias
- JF Mathiot
- JH Bartlett
- JJ Kelly
- JL Forest
- JL Friar
- JL Friar
- JL Friar
- JL Friar
- JL Friar
- JL Friedman
- JMB Kellog
- JMB Kellog
- JS Price
- JW Orden Van
- JW Orden Van
- JW Orden Van
- K Erkelenz
- K Hafidi
- K Kusaka
- K Rith
- K Tamura
- KI Blomqvist
- KL Mitchell
- KP Coulter
- KT Bainbridge
- L Eyraud
- L Hulthén
- LC Alexa
- M Bouwhuis
- M Ferro-Luzzi
- M Garçon
- M Garçon
- M Garçon
- M Garçon
- M Gourdin
- M Lacombe
- M Weitz
- ME Schulze
- MF Gari
- MF Gari
- MF Gari
- MF Gari
- MG Dolidze
- MG Fuda
- MI Strikman
- MI Strikman
- MJ Savage
- MJ Zuilhof
- MK Jones
- MP Rekalo
- MV Mostovoy
- NF Ramsey
- NK Devine
- NK Glendenning
- NL Rodning
- NL Rodning
- NP Aleshin
- P Mergell
- PA Dirac
- PA Dirac
- PA Dirac
- PA Dirac
- PE Bosted
- PG Blunden
- PJ Mohr
- PL Chung
- R Blankenbecler
- R Cramer
- R Dymarz
- R Dymarz
- R Gilman
- R Hofstadter
- R Machleidt
- R Machleidt
- R Machleidt
- R Schiavilla
- R Schiavilla
- RB Wiringa
- RE Arnold
- RE Rand
- RF Code
- RG Arnold
- RG Arnold
- RH Thompson
- RS Suleiman
- RT Birge
- RV Reid
- RW Berard
- S Auffret
- S Frullani
- S Galster
- S Gilad
- S Klarsfeld
- S Kopecky
- S Kox
- S Platchkov
- S Turck-Chieze
- S Weinberg
- S Weinberg
- SG Karshenboim
- SG Popov
- SI Bilenkaya
- SJ Brodsky
- SJ Brodsky
- SJ Brodsky
- SJ Wallace
- SL Belostotski
- SR Beane
- T Aono
- T Forest de Jr.
- T Herrmann
- T Nieuwenhuis
- T-S Park
- TEO Ericson
- TEO Ericson
- TEO Ericson
- TEO Ericson
- TW Allen
- TW Donnelly
- TW Donnelly
- U Kolck van
- V Dmitrosinovic
- V Franco
- VA Karmanov
- VF Dmitriev
- VG Kadychevsky
- VGJ Stoks
- VGJ Stoks
- VGJ Stoks
- VN BoÄtsov
- VZ Jankus
- W Bleakney
- W Heisenberg
- W Heisenberg
- W Turchinetz
- WJ Kasdorp
- WP Sitarski
- WW Buck
- X Zhu
- Y Ko
- Y Takahashi
- YK Akimov
- ZI Zhou
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2001
- Field of study
A brief review of the history of the discovery of the deuteron in provided.
The current status of both experiment and theory for the elastic electron
scattering is then presented.Comment: 80 pages, 33 figures, submited to Advances in Nuclear Physic
Development and validation of an improved algorithm for overlaying flexible molecules
- Author
- AR Leach
- AV Anghelescu
- CM Fonseca
- D Butina
- D CvetkoviÄ
- D Schneidman-Duhovny
- David A. Cosgrove
- DR Koes
- EJ Gardiner
- Eleanor J. Gardiner
- F Zhu
- G Jones
- G Wolber
- G Wolber
- HM Berman
- I Borg
- IJ Bruno
- J Boström
- J Feng
- J Marialke
- J Sadowski
- J Taminau
- J Verma
- Jason C. Cole
- JC Cole
- K Deb
- M Clark
- M Feher
- M Hendlich
- ML Verdonk
- NJ Richmond
- NP Todorov
- O Korb
- Oliver Korb
- P Labute
- PCD Hawkins
- R Taylor
- Robin Taylor
- SJ Cho
- SJ Cottrell
- SJ Cottrell
- SL Dixon
- T Cheeseright
- Valerie J. Gillet
- Publication venue
- Springer Netherlands
- Publication date
- 01/01/2012
- Field of study
A program for overlaying multiple flexible molecules has been developed. Candidate overlays are generated by a novel fingerprint algorithm, scored on three objective functions (union volume, hydrogen-bond match, and hydrophobic match), and ranked by constrained Pareto ranking. A diverse subset of the best ranked solutions is chosen using an overlay-dissimilarity metric. If necessary, the solutions can be optimised. A multi-objective genetic algorithm can be used to find additional overlays with a given mapping of chemical features but different ligand conformations. The fingerprint algorithm may also be used to produce constrained overlays, in which user-specified chemical groups are forced to be superimposed. The program has been tested on several sets of ligands, for each of which the true overlay is known from proteinâligand crystal structures. Both objective and subjective success criteria indicate that good results are obtained on the majority of these sets
Transiting Exoplanet Studies and Community Targets for JWST's Early Release Science Program
- Author
- Agol E
- Angerhausen D
- Barstow JK
- Bean JL
- Beichman C
- Birkmann SM
- Burrows A
- Charbonneau D
- Cowan NB
- Crouzet N
- Cubillos PE
- Curry SM
- Dalba PA
- Deming D
- Desert J-M
- Doyon R
- Dragomir D
- Ehrenreich D
- Fortney JJ
- Fraine J
- Gibson NP
- Gizis JE
- Greene TP
- Harrington J
- Heng K
- Kataria T
- Kempton EM-R
- Kilpatrick BM
- Knutson H
- Kreidberg L
- Krick JE
- Lafreniere D
- Lagage P-O
- Lewis NK
- Line MR
- Lopez-Morales M
- Lothringer JD
- Madhusudhan N
- Mandell AM
- Morley CV
- Munoz AG
- Rocchetto M
- Schlawin E
- Shkolnik EL
- Shporer A
- Sing DK
- Stevenson KB
- Todorov KO
- Tucker GS
- Valenti JA
- Wakeford HR
- Wit JD
- Publication venue
- 'IOP Publishing'
- Publication date
- 23/06/2016
- Field of study
This is a white paper that originated from an open discussion at the Enabling Transiting Exoplanet Science with JWST workshop held November 16 - 18, 2015 at STScI (http://www.stsci.edu/jwst/science/exoplanets). Accepted for publication in PASPThis is the author accepted manuscript. The final version is available from IOP Publishing via the DOI in this record.The James Webb Space Telescope will revolutionize transiting exoplanet atmospheric science due to its capability for continuous, long-duration observations and its larger collecting area, spectral coverage, and spectral resolution compared to existing space-based facilities. However, it is unclear precisely how well JWST will perform and which of its myriad instruments and observing modes will be best suited for transiting exoplanet studies. In this article, we describe a prefatory JWST Early Release Science (ERS) program that focuses on testing specific observing modes to quickly give the community the data and experience it needs to plan more efficient and successful future transiting exoplanet characterization programs. We propose a multi-pronged approach wherein one aspect of the program focuses on observing transits of a single target with all of the recommended observing modes to identify and understand potential systematics, compare transmission spectra at overlapping and neighboring wavelength regions, confirm throughputs, and determine overall performances. In our search for transiting exoplanets that are well suited to achieving these goals, we identify 12 objects (dubbed "community targets") that meet our defined criteria. Currently, the most favorable target is WASP-62b because of its large predicted signal size, relatively bright host star, and location in JWST's continuous viewing zone. Since most of the community targets do not have well-characterized atmospheres, we recommend initiating preparatory observing programs to determine the presence of obscuring clouds/hazes within their atmospheres. Measurable spectroscopic features are needed to establish the optimal resolution and wavelength regions for exoplanet characterization. Other initiatives from our proposed ERS program include testing the instrument brightness limits and performing phase-curve observations.(Abridged)K.B.S. recognizes support from the Sagan Fellowship Program, supported by NASA and administered by the NASA Exoplanet Science Institute (NExScI)
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- 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
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- 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
- Antonelli S
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arms KE
- Armstrong SR
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- 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
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- 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
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- 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 HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bee C
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Belhorma B
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo G
- Bellomo M
- Belloni A
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benedict BH
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- 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
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Bingul A
- Bini C
- Biscarat C
- Bischof R
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Boaretto C
- Bobbink GJ
- Bobrovnikov VB
- Bocci A
- Bock R
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bona M
- Boonekamp M
- Boorman G
- Booth CN
- Booth JRA
- Booth P
- 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
- Boulahouache C
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Braccini S
- Bracinik J
- Braem A
- Brambilla E
- Branchini P
- Branco MDO
- 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
- Brett ND
- Bright-Thomas PG
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brubaker E
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Buescher V
- Bueso XP
- Bugge L
- Buira-Clark D
- Buis EJ
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Byatt T
- Cabrera Urban S
- Caccia M
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camard A
- Camarri P
- Cambiaghi M
- Cameron D
- Camillocci ES
- Cammin J
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepa A
- Cantero J
- Capasso L
- Caprini I
- Caprini M
- Caprio M
- Capriotti D
- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carpentieri C
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo Gimenez V
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavalcanti TP
- Cavallari A
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Cazzato A
- Ceradini F
- Cerna C
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervetto M
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen H
- Chen L
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Cherkaoui El Moursli R
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chevallier F
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Ciocca C
- Ciocio A
- Cirilli M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration A
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coluccia R
- Comune G
- Conde Muino P
- Coniavitis E
- Conidi MC
- Consonni M
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correard S
- Correia AMH
- Corriveau F
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Coura Torres R
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Crepe-Renaudin S
- Cristinziani M
- Crosetti G
- Crupi R
- Cuneo S
- Curatolo M
- Curtis CJ
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- da Costa JBG
- Da Rocha Gesualdi Mello A
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dahlhoff A
- Dai T
- Dallapiccola C
- Dallison SJ
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dankers R
- Dannheim D
- Dao V
- Darbo G
- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies M
- Davison AR
- Dawe E
- Dawson I
- Dawson JW
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- Zeller M
- Zema PF
- Zemla A
- Zendler C
- Zenin AV
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
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- Zhu CG
- Zhu H
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- Zhuang X
- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- 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
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- Anderson KJ
- Andreazza A
- Andrei V
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- Anh TV
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- Antonaki A
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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
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at sâ=8 TeV with the ATLAS detector
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- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- 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
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fbâ1 of protonâproton collision data at âs = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via tËâtÏË01 or tËâ bÏ˱1 âbW(â)ÏË01 , where ÏË01 (Ï˱1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of tË â tÏË01 . For a branching fraction of 100%, top squark masses in the range 270â645 GeV are excluded for ÏË01 masses below 30 GeV. For a branching fraction of 50% to either tË â tÏË01 or tË â bÏ˱1 , and assuming the Ï˱1 mass to be twice the ÏË01 mass, top squark masses in the range 250â550 GeV are excluded for ÏË01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at âs=8TeV
- Author
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- Zinonos Z
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- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fbâ1of data collected in protonâproton collisions at âs=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
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- Yamaguchi H
- Yamamoto A
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- Yamamoto S
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- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
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- Yang UK
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- Yang Z
- Yanush S
- Yao L
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- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
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- Zhang L
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- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- 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 (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) 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<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
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