196 research outputs found
Some distorted thoughts about ketamine as a psychedelic and a novel hypothesis based on NMDA receptor-mediated synaptic plasticity.
- Publication venue
- 'Elsevier BV'
- Publication date
- 06/06/2018
- Field of study
Ketamine, a channel blocking NMDA receptor antagonist, is used off-label for its psychedelic effects, which may arise from a combination of several inter-related actions. Firstly, reductions of the contribution of NMDA receptors to afferent information from external and internal sensory inputs may distort sensations and their processing in higher brain centres. Secondly, reductions of NMDA receptor-mediated excitation of GABAergic interneurons can result in glutamatergic overactivity. Thirdly, limbic cortical disinhibition may indirectly enhance dopaminergic and serotonergic activity. Fourthly, inhibition of NMDA receptor mediated synaptic plasticity, such as short-term potentiation (STP) and long-term potentiation (LTP), could lead to distorted memories. Here, for the first time, we compared quantitatively the effects of ketamine on STP and LTP. We report that ketamine inhibits STP in a double sigmoidal fashion with low (40 nM) and high (5.6 μM) IC50 values. In contrast, ketamine inhibits LTP in a single sigmoidal manner (IC50 value ∼ 15 μM). A GluN2D-subunit preferring NMDA receptor antagonist, UBP145, has a similar pharmacological profile. We propose that the psychedelic effects of ketamine may involve the inhibition of STP and, potentially, associated forms of working memory. This article is part of the Special Issue entitled 'Psychedelics: New Doors, Altered Perceptions'
Regulation of Kainate Receptor Subunit mRNA by Stress and Corticosteroids in the Rat Hippocampus
- Author
- A Contractor
- A Munck
- AE Autry
- AM Magarinos
- Ana Costa
- AS Clark
- Bernhard Baune
- Bruce S. McEwen
- BS McEwen
- C de Montigny
- C Mulle
- CA Frye
- CS Woolley
- D Schmitz
- DH Blackwood
- DM Kullmann
- E Gould
- EJ Calabrese
- Erik Bloss
- F Han
- G Laje
- G Paxinos
- HH Schiffer
- J Raudensky
- JA Van Eekelen
- JV Nadler
- JV Nadler
- Katharine McCarthy
- LP Reagan
- M Beneyto
- M Darstein
- M Hollmann
- M Joels
- M Nishi
- MT Lowy
- N Strutz-Seebohm
- R Chittajallu
- RG Hunter
- RG Hunter
- Richard G. Hunter
- RS Sloviter
- Rudy Bellani
- S Paddock
- SE Lauri
- SJ Lupien
- U Wullner
- VN Luine
- W Wisden
- Y Watanabe
- Y Watanabe
- ZA Bortolotto
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
Kainate receptors are a class of ionotropic glutamate receptors that have a role in the modulation of glutamate release and synaptic plasticity in the hippocampal formation. Previous studies have implicated corticosteroids in the regulation of these receptors and recent clinical work has shown that polymorphisms in kainate receptor subunit genes are associated with susceptibility to major depression and response to anti-depressant treatment. In the present study we sought to examine the effects of chronic stress and corticosteroid treatments upon the expression of the mRNA of kainate receptor subunits GluR5-7 and KA1-2. Our results show that, after 7 days, adrenalectomy results in increased expression of hippocampal KA1, GluR6 and GluR7 mRNAs, an effect which is reversed by treatment with corticosterone in the case of KA1 and GluR7 and by aldosterone treatment in the case of GluR6. 21 days of chronic restraint stress (CRS) elevated the expression of the KA1 subunit, but had no effect on the expression of the other subunits. Similarly, 21 days of treatment with a moderate dose of corticosterone also increased KA1 mRNA in the dentate gyrus, whereas a high corticosterone dose has no effect. Our results suggest an interaction between hippocampal kainate receptor composition and the hypothalamic-pituitary-adrenal (HPA) axis and show a selective chronic stress induced modulation of the KA1 subunit in the dentate gyrus and CA3 that has implications for stress-induced adaptive structural plasticity
Convergence among Non-Sister Dendritic Branches: An Activity-Controlled Mean to Strengthen Network Connectivity
- Author
- A Mason
- A Ostling
- A Polsky
- A Roxin
- A van Ooyen
- A van Ooyen
- AI Gulyás
- B Lin
- BL Chen
- CF Olson
- D Baranes
- D Baranes
- Danny Baranes
- DB Chklovskii
- Eshel Ben-Jacob
- ET Kavalali
- G Liu
- GA Chauvet
- H Hasegawa
- J van Pelt
- JC López-García
- JG Jefferys
- JH Kong
- JL Krichmar
- Joshua Cove
- JQ Zheng
- JZ Parrish
- L Lovmar
- LF Lago-Fernandes
- LS Furtado
- M Kohrmann
- M Maletic-Savatic
- M Migliore
- Maytal Foox
- N Kalisman
- N Masuda
- O Shefi
- P Rousseeuw
- P Vetter
- Pablo Blinder
- PB Sargent
- Q Wen
- R Condit
- R Criado
- S Dudoit
- S Konur
- SD Washington
- SE Grebenyuk
- TS Skoglund
- V Latora
- V Latora
- V Sytnyk
- ZA Bortolotto
- ZF Mainen
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
The manner by which axons distribute synaptic connections along dendrites remains a fundamental unresolved issue in neuronal development and physiology. We found in vitro and in vivo indications that dendrites determine the density, location and strength of their synaptic inputs by controlling the distance of their branches from those of their neighbors. Such control occurs through collective branch convergence, a behavior promoted by AMPA and NMDA glutamate receptor activity. At hubs of convergence sites, the incidence of axo-dendritic contacts as well as clustering levels, pre- and post-synaptic protein content and secretion capacity of synaptic connections are higher than found elsewhere. This coupling between synaptic distribution and the pattern of dendritic overlapping results in ‘Economical Small World Network’, a network configuration that enables single axons to innervate multiple and remote dendrites using short wiring lengths. Thus, activity-mediated regulation of the proximity among dendritic branches serves to pattern and strengthen neuronal connectivity
Successful Cognitive Aging in Rats: A Role for mGluR5 Glutamate Receptors, Homer 1 Proteins and Downstream Signaling Pathways
- Author
- A Bikbaev
- A Serge
- B Monti
- B Xiao
- B Xiao
- BJ Williams
- C Romano
- CA Barnes
- Caroline Ménard
- CE Benoit
- CJ Westmark
- CM Alberini
- CM Bird
- CR Bramham
- D Manahan-Vaughan
- DD Krueger
- DS Bredt
- EK Osterweil
- F Bertaso
- F Nicoletti
- F Roselli
- G Dolen
- G Page
- GG Turrigiano
- HK Lee
- I Aubert
- IA Wilson
- J Brouillette
- J Brouillette
- J Nithianantharajah
- J Xu
- JA Moron
- JA Ronesi
- JC Beique
- JC Lauterborn
- JH Hu
- JJ Brightwell
- JM Henley
- JW Rowe
- JX Liu
- K Boric
- K Van Keuren-Jensen
- L Fagni
- L Hou
- L Mao
- L Yang
- M Gallagher
- M Klugmann
- M Kollen
- M Renner
- Mark P. Mattson
- MD Antion
- MJ Palmer
- MM Nicolle
- MW Jones
- N Saito
- PJ Colombo
- PJ Colombo
- PJ Kammermeier
- PR Brakeman
- PW Frankland
- R Gong
- R Kim
- R Lamprecht
- R Morris
- RG Parsons
- RP Haberman
- RS Duncan
- Rémi Quirion
- S Blum
- S Neyman
- SM Gallagher
- SN Burke
- T Celikel
- VJ Collett
- W Xu
- WB Rowe
- WB Rowe
- WQ Zhang
- Y Ge
- YS Lee
- ZA Bortolotto
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
Normal aging is associated with impairments in cognition, especially learning and memory. However, major individual differences are known to exist. Using the classical Morris Water Maze (MWM) task, we discriminated a population of 24-months old Long Evans aged rats in two groups - memory-impaired (AI) and memory-unimpaired (AU) in comparison with 6-months old adult animals. AI rats presented deficits in learning, reverse memory and retention. At the molecular level, an increase in metabotropic glutamate receptors 5 (mGluR5) was observed in post-synaptic densities (PSD) in the hippocampus of AU rats after training. Scaffolding Homer 1b/c proteins binding to group 1 mGluR facilitate coupling with its signaling effectors while Homer 1a reduces it. Both Homer 1a and 1b/c levels were up-regulated in the hippocampus PSD of AU animals following MWM task. Using immunohistochemistry we further demonstrated that mGluR5 as well as Homer 1b/c stainings were enhanced in the CA1 hippocampus sub-field of AU animals. In fact mGluR5 and Homer 1 isoforms were more abundant and co-localized in the hippocampal dendrites in AU rats. However, the ratio of Homer 1a/Homer 1b/c bound to mGluR5 in the PSD was four times lower for AU animals compared to AI rats. Consequently, AU animals presented higher PKCγ, ERK, p70S6K, mTOR and CREB activation. Finally the expression of immediate early gene Arc/Arg3.1 was shown to be higher in AU rats in accordance with its role in spatial memory consolidation. On the basis of these results, a model of successful cognitive aging with a critical role for mGluR5, Homer 1 proteins and downstream signalling pathways is proposed here
Ubiquitous molecular substrates for associative learning and activity-dependent neuronal facilitation.
- Author
- Abeliovich A
- Abrams TW
- Abrams TW
- Acosta-Urquidi J
- Akaike T
- Akers RF
- Alger BE
- Alkon DL
- Alkon DL
- Alkon DL
- Alkon DL
- Alkon DL
- Alkon DL
- Alkon DL
- Alkon DL
- Alkon DL
- Alkon DL
- Alkon DL
- Ambros-Ingerson J.
- Andersen P
- Andrade R
- Angenstein F
- Angestein F
- Annau Z
- Auerbach SB
- Axelrod J
- Bailey CH
- Bailey CH
- Bailey CH
- Bannerman DM
- Bao JX
- Barrionuevo G
- Baxter DA
- Baxter DA
- Bernier L
- Berridge MJ
- Bliss TV
- Bliss TV
- Bliss TVP
- Boenhoffer T
- Bortolotto ZA
- Bortolotto ZA
- Bortolotto ZA
- Boyle MB
- Braha O
- Bramham C R
- Breakwell NA
- Brown AM
- Burch RM
- Byrne JH
- Byrne JH
- Byrne JH
- Byrne JH.
- Carew TJ
- Carew TJ
- Carew TJ
- Castellucci V
- Chapouthier G
- Chavez-Noriega LE
- Chavez-Noriega LE
- Chavez-Noriega LE.
- Clapham DE.
- Clark GA
- Clark GA.
- Coffey ET
- Colebrook E
- Collin C
- Collingridge GL
- Colwill RM
- Connor J
- Critz SD
- Crow T
- Crow T
- Crow T
- Crow T
- Crow T.
- Crow TJ
- Crow TJ
- Davis RJ
- Dennis MJ
- Detwiler PB
- Detwiler PB
- Deutsch JA
- Dutar P
- Dutar P
- Eakin RM
- Edmonds B
- Edstrom JP
- Eliot LS
- Exton JH
- Exton JH
- Falk-Vairant J
- Farley J
- Farley J
- Farley J
- Farley J
- Farley J
- Farley J
- Farley J
- Fein A
- Finch EA
- Frenguelli BG
- Frey U
- Frey U
- Frysztak RJ
- Gage PW
- Ghirardi M.
- Ghosh A
- Glanzman DL
- Goh Y
- Goh Y
- Grover LM
- Grover LM
- Grover LM
- Hanse
- Hargreaves EL
- Harrigan JF
- Harris EW
- Hawkins RD
- Hawkins RD
- Hawkins RD
- Hawkins RD
- Hawkins RD
- Hochner B
- Homayouni R
- Huang YY
- Isaac JT
- Jaffe D
- Johnston D
- Kandel ER
- Kandel ER
- Kandel ER
- Kandel ER
- Khan WA
- Khan WA
- Klann E
- Klann E
- Klein M
- Klein M
- Krasne FB
- Kruger KE
- Kullmann DM
- Kupfermann I
- Kuzirian AM
- Land PW
- Lavond DG
- Lederhendler II
- Lester DS
- Lester DS
- Levy WB
- Liao D
- Lin XY
- Lisman J
- Lockery SR
- Lukowiak K
- Mackey SL
- Magee JC
- Malenka RC
- Malenka RC
- Malenka RC
- Malenka RC
- Malenka RC
- Malinow R
- Malinow R. LTP
- Manseau F
- Marder
- Martinez JL
- Massicotte G
- Matzel LD
- Matzel LD
- Matzel LD
- Matzel LD
- Matzel LD
- Matzel LD
- Matzel LD
- Matzel LD
- Matzel LD
- Mayford M
- McEachern JC
- McPhie D
- Meissner G.
- Miller RR
- Miller RR
- Murphy GG
- Murphy GG
- Muzzio I
- Muzzio IA
- Nakamura S
- Neary JT
- Nelson J
- Nelson TJ
- Nguyen PV
- Nishizuka Y
- Nosten-Bertrand M
- O'Dell TJ
- Ocorr KA
- Ogita K
- Okada D
- Olds J
- Osten
- Papini MR
- Payne R
- Perkins CC
- Pettit DL
- Pinsker H
- Publicover SJ
- Qi M
- Rasmussen H
- Rescorla RA
- Rescorla RA
- Rescorla RA
- Reymann KG
- Richards WG
- Roberson ED
- Rogers RF
- Rogers RF
- Rogers RF
- Rogers RF
- Sacktor TC
- Sacktor TC
- Sakakibara M
- Salin PA
- Saucier D
- Schneiderman N
- Schreurs BG
- Schuman EM
- Schuman EM
- Schwartzkroin P
- Scoville WB
- Sellers JR
- Shinomura T
- Shors TJ
- Shuster MJ
- Silva AJ
- Silva AJ
- Smirnova T
- Soderling TR
- Sossin WW
- Staubli U
- Steinmetz JE
- Stephane HRO
- Stevens CF
- Steward O
- Sugita S
- Susswein AJ
- Sweatt JD
- Talk AC
- Talk AC
- Taube JS
- Tesauro G
- Tsau Y
- Turkkan JS.
- Walters ET
- Walters ET
- Walters ET
- Wasserman EA
- Weinstein IB
- Weiss S
- West A
- Wu JY
- Yamamoto C
- Yamoah E
- Yanow SK
- Yin JC
- Yovell Y
- Yovell Y
- Zhuo M
- Publication venue
- 'Walter de Gruyter GmbH'
- Publication date
- 05/11/1998
- Field of study
Recent evidence suggests that many of the molecular cascades and substrates that contribute to learning-related forms of neuronal plasticity may be conserved across ostensibly disparate model systems. Notably, the facilitation of neuronal excitability and synaptic transmission that contribute to associative learning in Aplysia and Hermissenda, as well as associative LTP in hippocampal CA1 cells, all require (or are enhanced by) the convergence of a transient elevation in intracellular Ca2+ with transmitter binding to metabotropic cell-surface receptors. This temporal convergence of Ca2+ and G-protein-stimulated second-messenger cascades synergistically stimulates several classes of serine/threonine protein kinases, which in turn modulate receptor function or cell excitability through the phosphorylation of ion channels. We present a summary of the biophysical and molecular constituents of neuronal and synaptic facilitation in each of these three model systems. Although specific components of the underlying molecular cascades differ across these three systems, fundamental aspects of these cascades are widely conserved, leading to the conclusion that the conceptual semblance of these superficially disparate systems is far greater than is generally acknowledged. We suggest that the elucidation of mechanistic similarities between different systems will ultimately fulfill the goal of the model systems approach, that is, the description of critical and ubiquitous features of neuronal and synaptic events that contribute to memory induction
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlas Collaboration
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Bakshi Gupta D
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães Da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- 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
- Behera A
- Behr JK
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bellomo M
- Bellos P
- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertram IA
- Besjes GJ
- Bessidskaia Bylund O
- 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
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Bisanz T
- Biswal JP
- 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
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt A
- Brandt G
- Brandt O
- Braren F
- Bratzler U
- Brau B
- Brau JE
- Breaden Madden WD
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brost E
- Broughton JH
- Bruckman De Renstrom PA
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Bugge MK
- Bulekov O
- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Burr JTP
- Buschmann E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Büscher D
- Büscher V
- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cairo VMM
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarri P
- Cameron D
- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido MDM
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carrá S
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Che S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Cinca D
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
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- Mikuž M
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- Milic A
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- Perepelitsa DV
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- Ristić B
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- Schäfer U
- Sciandra A
- Sciolla G
- Scornajenghi M
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- Sebastiani CD
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- Sharma A
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- Shaw SM
- Shcherbakova A
- Shen Y
- Sherafati N
- Sherman AD
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shoaleh Saadi D
- Shochet MJ
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- Sjölin J
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- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
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- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Soffa AM
- Soffer A
- Soh DA
- Sokhrannyi G
- Solans Sanchez CA
- Solar M
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
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- Sopkova F
- Sosa D
- Sotiropoulou CL
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spanò F
- Sperlich D
- Spettel F
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- Spighi R
- Spigo G
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- Svatos M
- Swiatlowski M
- Swift SP
- Sydorenko A
- Sykora I
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- Sánchez J
- Søgaard A
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- Taenzer J
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- Talyshev AA
- Tanaka J
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- Tarem S
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
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- Tayalati Y
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- Thomsen LA
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- Tian Y
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- Torrence E
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- Torró Pastor E
- Tosciri C
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- Tsukerman II
- Tsulaia V
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- Tuna AN
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- Ungaro FC
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- Urban J
- Urquijo P
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- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valdes Santurio E
- Valente M
- Valentinetti S
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- Vallance RA
- Vallier A
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- Van Gemmeren P
- Van Nieuwkoop J
- Van Vulpen I
- Van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vari R
- Varnes EW
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- Varouchas D
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- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Vergel Infante CM
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vetterli MC
- Viaux Maira N
- Viazlo O
- Vichou I
- Vickey Boeriu OE
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
- Vokac P
- Volpi G
- Von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vranjes Milosavljevic M
- Vranjes N
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- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakamiya K
- Walbrecht VM
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Wang AM
- Wang C
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- Wanotayaroj C
- Warburton A
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- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
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- Wenig S
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- Werner MD
- Werner P
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- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
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- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Wilkins LJ
- Williams HH
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- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Woźniak KW
- Wraight K
- Wu M
- Wu SL
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- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
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- Xu H
- Xu L
- Xu T
- Xu W
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yue X
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
- Zgubič M
- Zhang D
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- Zhang F
- Zhang G
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- Zhang J
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- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
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- Yu J
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- Yuen SPY
- Yusuff I
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- Zaidan R
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- Zalieckas J
- Zambito S
- Zanzi D
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- Zemaityte G
- Zeng JC
- Zeng Q
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- Zhao X
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- Zhao Z
- Zhemchugov A
- Zhou B
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- Zhu CG
- Zhu H
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Operation and performance of the ATLAS Tile Calorimeter in Run 1
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouelfadl 
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez 
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor 
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Argos FC
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- Argyropoulos S
- Armadans R
- Armbruster AJ
- Armitage LJ
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- Artamonov A
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- Buzatu A
- Buzykaev AR
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- Caforio D
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- Calafiura P
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- Calderini G
- Calfayan P
- Callea G
- Caloba LP
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- Canale V
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- Cantero J
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- Capeans Garrido MDM
- Caprini I
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- Capua M
- Carbone RM
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- Cardillo FC
- Carli I
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- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carrá S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
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- Catmore JR
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- Caudron J
- Cavaliere V
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- Cavalli-Sforza M
- Cavasinni V
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- Charlton DG
- Chau CC
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- De Benedetti A
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- De Cecco S
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- de Jong P
- De la Torre H
- De Lorenzi F
- De Maria A
- De Moura 
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- De Santo A
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- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Gaudio M
- Del Peso J
- Delgado A
- Delgove D
- Deliot F
- Delitzsch CM
- Della Pietra M
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- Denysiuk D
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- Do 
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- Zhemchugov A
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- Zobernig G
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- Zorbas TG
- Zou R
- Zur 
- Zwalinski L
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeter’s performance during the years 2008–2012 using cosmic-ray muon events and proton–proton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fb−1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from proton–proton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
Search for large missing transverse momentum in association with one top-quark in proton-proton collisions at √s = 13 TeV with the ATLAS detector
- Author
- Aaboud M.
- Aad G.
- Abbott B.
- Abdinov O.
- Abeloos B.
- Abhayasinghe D. K.
- Abidi S. H.
- Abouzeid O. S.
- Abraham N. L.
- Abramowicz H.
- Abreu H.
- Abulaiti Y.
- Acharya B. S.
- Adachi S.
- Adam L.
- Adamczyk L.
- Adelman J.
- Adersberger M.
- Adiguzel A.
- Adye T.
- Affolder A. A.
- Aguilar-Saavedra J. A.
- Ahmadov F.
- Aielli G.
- Akatsuka S.
- Akesson T. P. A.
- Akilli E.
- Akimov A.
- Alberghi G. L.
- Albert J.
- Albicocco P.
- Alconada Verzini M. J.
- Alderweireldt S.
- Aleksa M.
- Aleksandrov I. N.
- Alexa C.
- Alexopoulos T.
- Alhroob M.
- Ali B.
- Alimonti G.
- Alison J.
- Alkire S. P.
- Allaire C.
- Allbrooke B. M. M.
- Allen B. W.
- Allport P. P.
- Aloisio A.
- Alonso A.
- Alonso F.
- Alpigiani C.
- Alshehri A. A.
- Alstaty M.
- Alvarez Piqueras D.
- Alviggi M. G.
- Amadio B. T.
- Amaral Coutinho Y.
- Ambler A.
- Ambroz L.
- Amelung C.
- Amidei D.
- Amor Dos Santos S. P.
- Amoroso S.
- Amrouche C. S.
- An F.
- Anastopoulos C.
- Anchez J. S.
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/12/2018
- Field of study
This paper describes a search for events with one top-quark and large missing transverse momentum in the final state. Data collected during 2015 and 2016 by the ATLAS experiment from 13 TeV proton–proton collisions at the LHC corresponding to an integrated luminosity of 36.1 fb−1 are used. Two channels are considered, depending on the leptonic or the hadronic decays of the W boson from the top quark. The obtained results are interpreted in the context of simplified models for dark-matter production and for the single production of a vector-like T quark. In the absence of significant deviations from the Standard Model background expectation, 95% confidence-level upper limits on the corresponding production cross-sections are obtained and these limits are translated into constraints on the parameter space of the models considered
Performance of missing transverse momentum reconstruction with the ATLAS detector using proton–proton collisions at √s = 13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
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- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
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- Arabidze G
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- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
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- Arslan O
- Artamonov A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying τ -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fb−1
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