436 research outputs found
The stellar and sub-stellar IMF of simple and composite populations
- Author
- A Duquennoy
- A Maeder
- A Parravano
- A Sollima
- A Sollima
- A Stolte
- A Vazdekis
- A Vazdekis
- AA Muench
- AE Piskunov
- AJ Cenarro
- AN Belikov
- AP Whitworth
- AR Boss
- AS Eddington
- AT Myers
- B Binggeli
- B García
- B Reipurth
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- C Briceño
- C Esteban
- C Flynn
- C Grillo
- C Hayashi
- C Koen
- C Low
- C Reylé
- C Soubiran
- C Weidner
- C Weidner
- C Weidner
- C Weidner
- C Weidner
- C Weidner
- C Weidner
- C Yasui
- CA Tout
- CJ Clarke
- CJ Grillmair
- CJ Lada
- CJ Lonsdale
- CL Slesnick
- CM Baugh
- CM Boily
- D Calzetti
- D Gouliermis
- D Gouliermis
- D Stamatellos
- D Stamatellos
- D Stamatellos
- D Stamatellos
- D Vanbeveren
- DA Fischer
- DA Forbes
- DA Tilley
- DA Tilley
- DC Heggie
- DF Figer
- DJ Pinfield
- DJ Price
- DR Weisz
- E Brocato
- E Casuso
- E Corbelli
- E Moraux
- E Schilbach
- E Vesperini
- E Vesperini
- EA Evstigneeva
- EA Hoversten
- EE Salpeter
- F D’Antona
- F Egusa
- F Motte
- F Najarro
- F Palla
- F Paresce
- F Selman
- FC Adams
- FC Adams
- FD Kahn
- G Basri
- G Bosch
- G Chabrier
- G Chabrier
- G Chabrier
- G Chabrier
- G Chabrier
- G Chabrier
- G Duchêne
- G Garcia-Segura
- G Garcia-Segura
- G Marchi de
- G Marchi de
- G Marchi De
- G Piotto
- G Weigelt
- G Wuchterl
- G Wuchterl
- GE Miller
- GR Blumenthal
- GR Meurer
- H Bartko
- H Baumgardt
- H Baumgardt
- H Bouy
- H Jahreiss
- H Kirk
- H Sana
- H Zinnecker
- H Zinnecker
- HT Janka
- I Baraffe
- I Misgeld
- I Thies
- I Thies
- I Thies
- I Thies
- IA Bonnell
- IA Bonnell
- IA Bonnell
- IA Bonnell
- IA Bonnell
- IA Bonnell
- IN Reid
- IN Reid
- IN Reid
- IN Reid
- J Binney
- J Bouvier
- J Dabringhausen
- J Dabringhausen
- J Dabringhausen
- J Jijina
- J Köppen
- J Maíz Apellániz
- J Maíz Apellániz
- J Maíz Apellániz
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Strader
- JB Lamb
- JC Tan
- JD Neill
- JE Dale
- JE Gizis
- JH Jeans
- JJ Bochanski
- JL Beuzit
- JL Halbwachs
- JM Kirk
- JM Oliveira
- JM Scalo
- JN Bahcall
- JP Anderson
- JS Kalirai
- JS Ulvestad
- K Fuhrmann
- K Kuijken
- KD Finkelstein
- KL Luhman
- KL Luhman
- KS Boer de
- L Siess
- L Testi
- LA Hillenbrand
- LA Hillenbrand
- LJ Smith
- LM Close
- LR Penny
- M Andersen
- M Andersen
- M Beech
- M Dominik
- M Fellhauer
- M Fellhauer
- M Fellhauer
- M Fellhauer
- M Fumagalli
- M Haywood
- M Mac Low
- M Marks
- M Marks
- M Marks
- M Marks
- M Marks
- M Marks
- M Nagashima
- M Ramspeck
- M Schmalzl
- M Schwarzschild
- M Sirianni
- MA Pérez-Torres
- MG Wolfire
- MJ Disney
- MN Machida
- MN Machida
- MR Bate
- MR Bate
- MR Bate
- MR Krumholz
- MR Krumholz
- MR Krumholz
- MS Oey
- MS Oey
- N Bastian
- N Ivanova
- N Kevlahan
- N Lodieu
- N McCrady
- N Moeckel
- N Murray
- N Phan-Bao
- N Reid
- N Rio Da
- NC Hambly
- NC Hambly
- O Malkov
- OY Malkov
- P Girichidis
- P Hennebelle
- P Hennebelle
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Massey
- P Massey
- P Padoan
- P Padoan
- P Wang
- PA Crowther
- PC Clark
- PC Myers
- PFL Maxted
- PG Dokkum van
- PG Dokkum van
- PJE Peebles
- PP Papadopoulos
- PP Papadopoulos
- PR Allen
- R Chini
- R Fuente Marcos de La
- R Kudritzki
- R Parra
- R Wojtak
- R Wünsch
- RB Larson
- RB Larson
- RB Stothers
- RC Kennicutt Jr
- RJ Parker
- RJ Parker
- RJ Parker
- RJ Smith
- RJ White
- RS Klessen
- RS Klessen
- RS Stobie
- S Banerjee
- S Basu
- S Basu
- S Bontemps
- S Dib
- S Dib
- S Djorgovski
- S Feltzing
- S Hocuk
- S Mieske
- S Mieske
- S Nayakshin
- S Recchi
- S Roychowdhury
- S Röser
- S Shen
- S Zucker
- SD Murray
- SF Portegies Zwart
- SJ Aarseth
- SLW McMillan
- SM Wilkins
- SP Goodwin
- SP Goodwin
- SP Goodwin
- SP Goodwin
- SP Goodwin
- SS Kim
- SS Vogt
- ST Megeath
- T Chlebowski
- T Hippel von
- T Maschberger
- T Maschberger
- T Maschberger
- T Onishi
- T Peters
- T Peters
- T Preibisch
- T Tsujimoto
- TE Lutz
- TJ Henry
- TV Veltchev
- U Löckmann
- V Bromm
- V Joergens
- V Weidemann
- VV Gvaramadze
- VV Gvaramadze
- W Jao
- W-H Hsu
- WJ Wit de
- WJ Wit de
- X Delfosse
- X Delfosse
- Y Li
- Z-Y Li
- Å Nordlund
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 04/11/2012
- Field of study
The current knowledge on the stellar IMF is documented. It appears to become
top-heavy when the star-formation rate density surpasses about 0.1Msun/(yr
pc^3) on a pc scale and it may become increasingly bottom-heavy with increasing
metallicity and in increasingly massive early-type galaxies. It declines quite
steeply below about 0.07Msun with brown dwarfs (BDs) and very low mass stars
having their own IMF. The most massive star of mass mmax formed in an embedded
cluster with stellar mass Mecl correlates strongly with Mecl being a result of
gravitation-driven but resource-limited growth and fragmentation induced
starvation. There is no convincing evidence whatsoever that massive stars do
form in isolation. Various methods of discretising a stellar population are
introduced: optimal sampling leads to a mass distribution that perfectly
represents the exact form of the desired IMF and the mmax-to-Mecl relation,
while random sampling results in statistical variations of the shape of the
IMF. The observed mmax-to-Mecl correlation and the small spread of IMF
power-law indices together suggest that optimally sampling the IMF may be the
more realistic description of star formation than random sampling from a
universal IMF with a constant upper mass limit. Composite populations on galaxy
scales, which are formed from many pc scale star formation events, need to be
described by the integrated galactic IMF. This IGIMF varies systematically from
top-light to top-heavy in dependence of galaxy type and star formation rate,
with dramatic implications for theories of galaxy formation and evolution.Comment: 167 pages, 37 figures, 3 tables, published in Stellar Systems and
Galactic Structure, Vol.5, Springer. This revised version is consistent with
the published version and includes additional references and minor additions
to the text as well as a recomputed Table 1. ISBN 978-90-481-8817-
Evolution of ligand specificity in vertebrate corticosteroid receptors
- Author
- A Koide
- A Stevens
- A Sturm
- Adam S Arterbery
- AH Bass
- AK Greenwood
- Andrew H Bass
- AS Arterbery
- C Robin-Jagerschmidt
- CRW Edwards
- D Alsop
- Daniel J Fergus
- David L Deitcher
- DW Ray
- EA Ortlund
- EH Stolte
- EH Stolte
- Elizabeth A Fogarty
- FM Rogerson
- FM Rogerson
- FM Rogerson
- H Gronemeyer
- HA Bern
- JA Sisneros
- JMHM Reul
- John Mayberry
- JP Huelsenbeck
- JQ Jiang
- JS Nelson
- JT Bridgham
- JT Bridgham
- JW Funder
- JW Thornton
- JW Thornton
- K Arnold
- K Maruska
- L Colombe
- M Einstein
- M Proszkowiec-Weglarz
- MC Peitsch
- MD Taves
- ME Baker
- ME Baker
- MJM Schaaf
- MY Kim
- N Guex
- NR Bury
- NR Bury
- P Bentley
- P Porcu
- P Porcu
- PM Forlano
- R Development Core Team
- RK Bledsoe
- RK Bledsoe
- S Milla
- SCP Renn
- SH Meijsing
- SM Carroll
- T Osterwalder
- V Giguere
- VN Parikh
- W Lee Kraus
- WV Welshons
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Corticosteroid receptors include mineralocorticoid (MR) and glucocorticoid (GR) receptors. Teleost fishes have a single MR and duplicate GRs that show variable sensitivities to mineralocorticoids and glucocorticoids. How these receptors compare functionally to tetrapod MR and GR, and the evolutionary significance of maintaining two GRs, remains unclear.</p> <p>Results</p> <p>We used up to seven steroids (including aldosterone, cortisol and 11-deoxycorticosterone [DOC]) to compare the ligand specificity of the ligand binding domains of corticosteroid receptors between a mammal (<it>Mus musculus</it>) and the midshipman fish (<it>Porichthys notatus</it>), a teleost model for steroid regulation of neural and behavioral plasticity. Variation in mineralocorticoid sensitivity was considered in a broader phylogenetic context by examining the aldosterone sensitivity of MR and GRs from the distantly related daffodil cichlid (<it>Neolamprologus pulcher</it>), another teleost model for neurobehavioral plasticity. Both teleost species had a single MR and duplicate GRs. All MRs were sensitive to DOC, consistent with the hypothesis that DOC was the initial ligand of the ancestral MR. Variation in GR steroid-specificity corresponds to nine identified amino acid residue substitutions rather than phylogenetic relationships based on receptor sequences.</p> <p>Conclusion</p> <p>The mineralocorticoid sensitivity of duplicate GRs in teleosts is highly labile in the context of their evolutionary phylogeny, a property that likely led to neo-functionalization and maintenance of two GRs.</p
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=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
- 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
- Akesson TPA
- 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
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- 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
- 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
- Araque JP
- Arce ATH
- Arguin J-F
- 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
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Baas A
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bannoura AAE
- Bansal V
- Bansil HS
- Barajas CAC
- 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 F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartos P
- Bartsch V
- Bassalat A
- Basye A
- Bates RL
- Batkova L
- Batley JR
- Battaglia M
- Battistin M
- Bauer F
- Bawa HS
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
- Becker S
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr K
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
- Benekos N
- Benhammou Y
- Benjamin DP
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Beringer J
- Bernard C
- Bernat P
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertsche D
- Besana MI
- Besjes GJ
- Bessidskaia O
- Bessner MF
- Besson N
- Betancourt C
- Bethke S
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Black CW
- Black JE
- Black KM
- Blackburn D
- Blair RE
- Blanchard J-B
- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boddy CR
- Boehler M
- Boek TT
- Boeriu OEV
- Bogaerts JA
- Bogdanchikov AG
- Bogouch A
- Bohm C
- Bohm J
- Boisvert V
- Bold T
- Boldea V
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Borri M
- Borroni S
- Bortfeldt J
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Bousson N
- Boutouil S
- Boveia A
- Boyd J
- Boyko IR
- Bracinik J
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brazzale SF
- Brelier B
- Brendlinger K
- Brennan AJ
- Brenner R
- Bressler S
- Bret MC
- Bristow K
- Bristow TM
- Britton D
- Brochu FM
- Brock I
- Brock R
- Bromberg C
- Bronner J
- Brooijmans G
- Brooks T
- Brooks WK
- Brosamer J
- Brost E
- Brown J
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- Bryngemark L
- Buanes T
- Buat Q
- Bucci F
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Buehrer F
- Bugge L
- Bugge MK
- Bulekov O
- Bundock AC
- Burckhart H
- Burdin S
- Burghgrave B
- Burke S
- Burmeister I
- Busato E
- Buscher D
- Buscher V
- Bussey P
- Bustos ACF
- Buszello CP
- Butler B
- Butler JM
- Butt AI
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Byszewski M
- Cabrera Urban S
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Calvet D
- Calvet S
- Camarda S
- Cameron D
- Camillocci ES
- Caminada LM
- Caminal Armadans R
- Campana S
- Campanelli M
- Campoverde A
- Canale V
- Canepa A
- Cantero J
- Cantrill R
- Cao T
- Caprini I
- Caprini M
- Capua M
- Caputo R
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Casolino M
- Castaneda-Miranda E
- Castanheira MTD
- Castelli A
- Castillo Gimenez V
- Castillo IS
- Castillo LRF
- Castro NF
- Catastini P
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavaliere V
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerio B
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cerv M
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
- Chen L
- Chen S
- Chen X
- Chen Y
- Cheng HC
- Cheng Y
- Cheplakov A
- Cherkaoui El Moursli R
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiefari G
- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Chouridou S
- Chow BKB
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Chwastowski JJ
- Chytka L
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciocio A
- Cirkovic P
- Citron ZH
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Clarke RN
- Cleland W
- Clemens JC
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coffey L
- Cogan JG
- Coggeshall J
- Cole B
- Cole S
- Colijn AP
- Collaboration ATLAS
- Collot J
- Colombo T
- Colon G
- Compostella G
- Conde Muino P
- Coniavitis E
- Conidi MC
- Connell SH
- Connelly IA
- Consonni SM
- Consorti V
- Constantinescu S
- Conta C
- Conti G
- Conventi F
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
- Cottin G
- Cowan G
- Cox BE
- Cranmer K
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cribbs WA
- Cristinziani M
- Croft V
- Crosetti G
- Cuciuc C-M
- Cummings J
- Curatolo M
- Cuthbert C
- Czirr H
- Czodrowski P
- Czyczula Z
- D'Auria S
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dafinca A
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Daniells AC
- Dao V
- Darbo G
- Darmora S
- Dassoulas JA
- Dattagupta A
- Davey W
- David C
- Davidek T
- Davies E
- Davies M
- Davignon O
- Davison AR
- Davison P
- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Asmundis R
- De Bruin PHS
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DEF
- De Lorenzi F
- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De K
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Deigaard I
- Del Peso J
- Del Prete T
- Deliot F
- Delitzsch CM
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Dell'Orso M
- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demilly A
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Di Valentino D
- Dias FA
- Diaz MA
- Diehl EB
- Dietrich J
- Dietzsch TA
- Diglio S
- Dimitrievska A
- Dingfelder J
- Dionisi C
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- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
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- Zhemchugov A
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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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
- '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 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±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 t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- 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
- Akesson TP
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- 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
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
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- Anders CF
- Anders G
- Anderson KJ
- Andrade Filho LMD
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- Angelozzi I
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- Angerami A
- Anghinolfi F
- Anisenkov AV
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- Annovi A
- Antonaki A
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- Winklmeier F
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- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
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- Yoshihara K
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- Youssef S
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- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
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- Zanello L
- Zanzi D
- 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
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- 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
- '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 20.3fb−1of data collected in proton–proton collisions at √s=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
Rydberg-Stark deceleration of atoms and molecules
- Author
- A Anderson
- A Kellerbauer
- A Osterwalder
- A Osterwalder
- A Osterwalder
- A Reinhard
- A Tauschinsky
- A Wallraff
- AB Henson
- AH Al-Ramadhan
- AP Mills Jr
- C Baxter
- C Foot
- C Hermann-Avigliano
- C Zener
- CH Greene
- Ch Seiler
- Ch Seiler
- Ch Seiler
- Ch Seiler
- CH Storry
- D Kleppner
- D Sprecher
- D Townsend
- DB Cassidy
- DB Cassidy
- DF Gray
- DH Parker
- DP Comparat
- E Narevicius
- E So
- E Vliegen
- E Vliegen
- E Vliegen
- E Vliegen
- E Vliegen
- E Vliegen
- E Vliegen
- EA Hinds
- EJ Beiting
- ES Shuman
- F Merkt
- F Merkt
- G Santambrogio
- GB Andresen
- GB Andresen
- GR Lloyd
- H Ko
- H Kübler
- H Walther
- HA Bethe
- HG Bennewitz
- HH Fielding
- HL Bethlem
- HL Bethlem
- I Mourachko
- II Beterov
- J Chiaverini
- J Liu
- J Liu
- JA Gibbard
- JD Carter
- JD Pritchard
- JH Choi
- JK Messer
- JM Doyle
- JP Gordon
- JP Home
- JR Hiskes
- JR Rydberg
- JW Humberston
- JZ Zhang
- JZ Zhang
- K Qin
- KA Smith
- KP Ziock
- L Hollberg
- L Isenhower
- LC Carr
- LD Landau
- M Amoretti
- M Charlton
- M Mandel
- M Saffman
- MF Riedel
- MJ Englefield
- MJ Vrakking
- ML Zimmerman
- MT Bell
- N Vanhaecke
- NF Ramsey
- O Cherry
- P Allmendinger
- P Allmendinger
- P Crivelli
- P Lancuba
- P Lancuba
- P Rabl
- PF Staanum
- PR Brooks
- R Folman
- R Fulton
- RJ Damburg
- RN Zare
- RP Wayne
- RS Vallery
- S Stolte
- S Willitsch
- S Willitsch
- SA Meek
- SA Meek
- SA Meek
- SB Hill
- SD Hogan
- SD Hogan
- SD Hogan
- SD Hogan
- SD Hogan
- SD Hogan
- SD Hogan
- SD Hogan
- SE Anderson
- SG Karshenboim
- SR Procter
- SV Stepkin
- SYT van de Meerakker
- T Breeden
- T Nirrengarten
- T Thiele
- T Vogt
- T Vogt
- T Wilk
- TE Wall
- TE Wall
- TF Gallagher
- TF Gallagher
- TF Gallagher
- TP Softley
- V Bendkowsky
- V Sandoghdar
- V Zhelyazkova
- V Zhelyazkova
- V Zhelyazkova
- W Gerlach
- W Gerlach
- W Gerlach
- W Pauli
- WH Wing
- WP Spencer
- WR Anderson
- Y Shagam
- Y Yamakita
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at root s = 8 TeV with the ATLAS detector (vol 75, 299, 2015)
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
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- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alhroob M
- Alimonti G
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- Allbrooke BMM
- Allison LJ
- Allport PP
- Aloisio A
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- Alviggi MG
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- Castillo Gimenez V
- Castillo IS
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- Cerqueira AS
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- Chalupkova I
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
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- Chen L
- Chen S
- Chen X
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- Cheng HC
- Cheng Y
- Cheplakov A
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- Chernyatin V
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- Childers JT
- Chilingarov A
- Chiodini G
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- Chromek-Burckhart D
- Chu ML
- Chudoba J
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- Ciftci AK
- Cinca D
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- Ciocio A
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- Coffey L
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- Cole B
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- Colijn AP
- Collaboration ATLAS
- Collot J
- Colombo T
- Compostella G
- Coniavitis E
- Connell SH
- Connelly IA
- Consonni SM
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- Da Via C
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- Dafinca A
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- Dallapiccola C
- Dam M
- Damazio DO
- Dandoy JR
- Daniells AC
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- Davey W
- David C
- Davidek T
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- Davies M
- Davignon O
- Davison P
- Davygora Y
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- Dawson I
- Daya-Ishmukhametova RK
- de Asmundis R
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- de Lima DEF
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- Zhemchugov A
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- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √s=8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT>120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between EmissT>150 GeV and EmissT>700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presented
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at root s = 8 TeV with the ATLAS detector (vol 75, 299, 2015)
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- 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
- Akesson TPA
- 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
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- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
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- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang J
- Zhang L
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- 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
- 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
- 01/01/2015
- Field of study
Measurement of the transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at √s=7 TeV using the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- 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
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- 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
- Alonso F
- Alpigiani C
- Altheimer A
- 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
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- Anderson KJ
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- Angelidakis S
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- Aoki M
- Arabidze G
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- Arce ATH
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- Argyropoulos S
- Arik M
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- Zhemchugov A
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2014
- Field of study
The transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760 μb−1 of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5×10−5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is −0.010±0.005(stat)±0.004(syst) for Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement
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
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- Zhemchugov A
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- Zimmermann C
- Zimmermann R
- Zimmermann S
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- 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
Measurements of normalized differential cross sections for tt̄ production in pp collisions at √(s)=7 TeV using 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
- Abulaiti Y
- Acharya BS
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- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
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- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Albert J
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- 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
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- Youssef S
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- Zanzi D
- Zaytsev A
- Zeitnitz C
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- Zemla A
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- Zhemchugov A
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
Measurements of normalized differential cross sections for top-quark pair production are presented as a function of the top-quark transverse momentum, and of the mass, transverse momentum, and rapidity of the t¯t system, in proton–proton collisions at a center-of-mass energy of √s=7 TeV. The data set corresponds to an integrated luminosity of 4.6 fb−1, recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one lepton and at least four jets with at least one of the jets tagged as originating from a b-quark. The measured spectra are corrected for detector efficiency and resolution effects and are compared to several Monte Carlo simulations and theory calculations. The results are in fair agreement with the predictions in a wide kinematic range. Nevertheless, data distributions are softer than predicted for higher values of the mass of the t¯t system and of the top-quark transverse momentum. The measurements can also discriminate among different sets of parton distribution functions
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