417 research outputs found
Optical kerr effect in supercooled water
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 26/11/2015
- Field of study
We present molecular dynamics simulations of the optical Kerr effect in liquid and supercooled water and compare with recent time-resolved Kerr spectroscopy measurements [R. Torre , Nature (London) 428, 296 (2004)]. The short time features of the Kerr response, characterized by peaks near 15, 60, and 160 fs, are weakly temperature dependent. The long-time decay is well described by a stretched exponential with a nearly constant stretch parameter and relaxation times that follow a power law similar to(T-T-S)(-gamma), with T-S=198.3 K and gamma=2.35. Our findings are discussed in the light of the spectroscopy data and previous simulation analyzes of the structural relaxation in supercooled water.941
Molecular association between water and dimethyl sulfoxide in solution: A molecular dynamics simulation study
- Publication venue
- 'AIP Publishing'
- Publication date
- 26/11/2015
- Field of study
A molecular dynamics simulation study of the local structures and H-bond distribution for water-dimethyl sulfoxide (DMSO) mixtures over the entire composition range is presented. Analysis of several site-site pair distribution functions reveals that two well-defined kinds of aggregates characterize the molecular association between water and DMSO in solution. One of them, already identified through recent neutron diffraction experiments and computer simulations, consists of two water molecules H-bonded to the oxygen atom of a DMSO molecule, such that the angle between the two H-bonds is nearly tetrahedral. The other complex features a central water molecule and two DMSO, making H-bonds to water hydrogens. According to the simulation data, these molecular aggregates coexist with each other in the mixture, but their proportions change with composition. 1DMSO-2water complexes predominate over 2DMSO-1water aggregates for water-rich mixtures (water mole fractions >50%), whereas the opposite is true for DMSO-rich mixtures. The present simulations also seem to indicate that an association between a pair of DMSO molecules through their oxygen atoms is made possible by the formation of the 2DMSO-1water complexes. Implications of the existence of these aggregates to the mobility and other dynamic properties of these mixtures are briefly discussed. (C) 1999 American Institute of Physics. [S0021-9606(99)50511-4].110136412642
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Idealized Carbon-Based Materials Exhibiting Record Deliverable Capacities for Vehicular Methane Storage
- Publication venue
- Journal of Physical Chemistry C
- Publication date
- 01/01/2019
- Field of study
Materials
for vehicular methane storage have been extensively studied,
although no suitable material has been found. In this work, we use
molecular simulation to investigate three types of carbon-based materials,
Schwarzites, layered graphenes, and carbon nanoscrolls, for use in
vehicular methane storage under adsorption conditions of 65 bar and
298 K and desorption conditions of 5.8 bar and 358 K. Ten different
Schwarzites were tested and found to have high adsorption with maximums
at 273 VSTP/V, but middling deliverable capacities of no
more than 131 VSTP/V. Layered graphene and graphene nanoscrolls
were found to have extremely high CH4 adsorption capacities
of 355 and 339 VSTP/V, respectively, when the interlayer
distance was optimized to 11 Å. The deliverable capacities of
perfectly layered graphene and graphene nanoscrolls were also found
to be exceptional with values of 266 and 252 VSTP/V, respectively,
with optimized interlayer distances. These values make idealized graphene
and nanoscrolls the record holders for adsorption and deliverable
capacities under vehicular methane storage conditions
Rotational dynamics and polymerization of C(60) in C(60)-cubane crystals: A molecular dynamics study
- Publication venue
- 'AIP Publishing'
- Publication date
- 26/11/2015
- Field of study
Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)We report classical and tight-binding molecular dynamics simulations of the C(60) fullerene and cubane molecular crystal in order to investigate the intermolecular dynamics and polymerization processes. Our results show that, for 200 and 400 K, cubane molecules remain basically fixed, presenting only thermal vibrations, while C(60) fullerenes show rotational motions. Fullerenes perform "free" rotational motions at short times (less than or similar to 1 ps), small amplitude hindered rotational motions (librations) at intermediate times, and rotational diffusive dynamics at long times (greater than or similar to 10 ps). The mechanisms underlying these dynamics are presented. Random copolymerizations among cubanes and fullerenes were observed when temperature is increased, leading to the formation of a disordered structure. Changes in the radial distribution function and electronic density of states indicate the coexistence of amorphous and crystalline phases. The different conformational phases that cubanes and fullerenes undergo during the copolymerization process are discussed.1296IMMP/MCTIN/MCTTHEO-NANOConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES
SARS-CoV-2 uses CD4 to infect T helper lymphocytes
- Author
- Agrela Marcus V
- Amorim Mariene R
- Bernardes Ana F
- Bispos-dos-Santos Karina
- Bloyet Louis-Marie
- Boldrini Vinicius O
- Brunetti Natalia S
- Buscaratti Lucas I
- Carregari Victor C
- Carvalho Murilo
- Carvalho Robson F
- Castelucci Bianca G
- Castro Icaro MS
- Coimbra Laís D
- Crunfli Fernanda
- Cunha Thiago Mattar
- da Silva Luis LP
- Damasio André
- Davanzo Gustavo G
- de Moraes Diogo
- de Oliveira Eduardo B
- Dias Artur HS
- Dias Marieli MG
- Faca Vitor M
- Farias Alessandro S
- Ferrari Allan JR
- Figueira Ana Carolina M
- Forato Julia
- Gerhardt Jaqueline A
- Gomes Arilson Bernardo SP
- Granja Fabiana
- Knittel Thiago L
- Ludwig Raissa G
- Mansour Eli
- Marques Ana Maria
- Marques Rafael E
- Marques-Souza Henrique
- Martini Matheus Cavalheiro
- Martins-de-Souza Daniel
- Monteiro Lauar B
- Moraes-Vieira Pedro MM
- Moretti Maria Luiza
- Mori Marcelo A
- Munhoz-Alves Natália
- Muraro Stéfanie Primon
- Nakaya Helder I
- Nunes Santos Luana
- Nunes Thyago A
- Palma André C
- Parise Pierina Lorencini
- Pereira Alexandre B
- Pereira Fabricio B
- Pontelli Marjorie C
- Proenca-Modena Jose Luiz
- Profeta Gerson S
- Ribeiro Luciana C
- Rodrigues Patricia B
- Santos Leonilda MB
- Sesti-Costa Renata
- Silva-Costa Lícia C
- Silvestrini Virgínia C
- Simeoni Camila L
- Skaf Munir S
- Souza Gabriela F
- Sposito Andrei C
- Stumpf Spencer
- Tavares Lucas A
- Toledo-Teixeira Daniel A
- Ulaf Raisa G
- Velloso Licio
- Veras Flavio P
- Vieira André S
- Vinolo Marco AR
- Virgílio-da-Silva João Victor
- Wassano Natália S
- Whelan Sean
- Publication venue
- Publication date
- 31/07/2023
- Field of study
The severe acute respiratory syndrome coronavirus 2 (SARS-CoV-2) is the agent of a major global outbreak of respiratory tract disease known as Coronavirus Disease 2019 (COVID-19). SARS-CoV-2 infects mainly lungs and may cause several immune-related complications, such as lymphocytopenia and cytokine storm, which are associated with the severity of the disease and predict mortality. The mechanism by which SARS-CoV-2 infection may result in immune system dysfunction is still not fully understood. Here, we show that SARS-CoV-2 infects human CD4+ T helper cells, but not CD8+ T cells, and is present in blood and bronchoalveolar lavage T helper cells of severe COVID-19 patients. We demonstrated that SARS-CoV-2 spike glycoprotein (S) directly binds to the CD4 molecule, which in turn mediates the entry of SARS-CoV-2 in T helper cells. This leads to impaired CD4 T cell function and may cause cell death. SARS-CoV-2-infected T helper cells express higher levels of IL-10, which is associated with viral persistence and disease severity. Thus, CD4-mediated SARS-CoV-2 infection of T helper cells may contribute to a poor immune response in COVID-19 patients.</p
SARS-CoV-2 uses CD4 to infect T helper lymphocytes
- Author
- Agrela Marcus V
- Amorim Mariene R
- Bernardes Ana F
- Bispos-dos-Santos Karina
- Bloyet Louis-Marie
- Boldrini Vinicius O
- Brunetti Natalia S
- Buscaratti Lucas I
- Carregari Victor C
- Carvalho Murilo
- Carvalho Robson F
- Castelucci Bianca G
- Castro Icaro MS
- Coimbra Laís D
- Crunfli Fernanda
- Cunha Thiago Mattar
- da Silva Luis LP
- Damasio André
- Davanzo Gustavo G
- de Moraes Diogo
- de Oliveira Eduardo B
- Dias Artur HS
- Dias Marieli MG
- Faca Vitor M
- Farias Alessandro S
- Ferrari Allan JR
- Figueira Ana Carolina M
- Forato Julia
- Gerhardt Jaqueline A
- Gomes Arilson Bernardo SP
- Granja Fabiana
- Knittel Thiago L
- Ludwig Raissa G
- Mansour Eli
- Marques Ana Maria
- Marques Rafael E
- Marques-Souza Henrique
- Martini Matheus Cavalheiro
- Martins-de-Souza Daniel
- Monteiro Lauar B
- Moraes-Vieira Pedro MM
- Moretti Maria Luiza
- Mori Marcelo A
- Munhoz-Alves Natália
- Muraro Stéfanie Primon
- Nakaya Helder I
- Nunes Santos Luana
- Nunes Thyago A
- Palma André C
- Parise Pierina Lorencini
- Pereira Alexandre B
- Pereira Fabricio B
- Pontelli Marjorie C
- Proenca-Modena Jose Luiz
- Profeta Gerson S
- Ribeiro Luciana C
- Rodrigues Patricia B
- Santos Leonilda MB
- Sesti-Costa Renata
- Silva-Costa Lícia C
- Silvestrini Virgínia C
- Simeoni Camila L
- Skaf Munir S
- Souza Gabriela F
- Sposito Andrei C
- Stumpf Spencer
- Tavares Lucas A
- Toledo-Teixeira Daniel A
- Ulaf Raisa G
- Velloso Licio
- Veras Flavio P
- Vieira André S
- Vinolo Marco AR
- Virgílio-da-Silva João Victor
- Wassano Natália S
- Whelan Sean
- Publication venue
- Publication date
- 31/07/2023
- Field of study
The severe acute respiratory syndrome coronavirus 2 (SARS-CoV-2) is the agent of a major global outbreak of respiratory tract disease known as Coronavirus Disease 2019 (COVID-19). SARS-CoV-2 infects mainly lungs and may cause several immune-related complications, such as lymphocytopenia and cytokine storm, which are associated with the severity of the disease and predict mortality. The mechanism by which SARS-CoV-2 infection may result in immune system dysfunction is still not fully understood. Here, we show that SARS-CoV-2 infects human CD4+ T helper cells, but not CD8+ T cells, and is present in blood and bronchoalveolar lavage T helper cells of severe COVID-19 patients. We demonstrated that SARS-CoV-2 spike glycoprotein (S) directly binds to the CD4 molecule, which in turn mediates the entry of SARS-CoV-2 in T helper cells. This leads to impaired CD4 T cell function and may cause cell death. SARS-CoV-2-infected T helper cells express higher levels of IL-10, which is associated with viral persistence and disease severity. Thus, CD4-mediated SARS-CoV-2 infection of T helper cells may contribute to a poor immune response in COVID-19 patients.</p
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Appelt C
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahilo JJL
- Bahmani M
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits MS
- Barkeloo J
- Barklow T
- Barnett RM
- Baron P
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barron U
- Barrue RFC
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Baselga M
- Bashta I
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer P
- Bayirli A
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Becot C
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bi R
- Bianchi RM
- Biebel O
- Bielski R
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bjorke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbely AG
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Bourdarios CA
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks WK
- Brost E
- Bruers B
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Bugge MK
- Bulekov O
- Bullard BA
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Buscher V
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Cabras G
- Caforio D
- Cai H
- Cai Y
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carlson TI
- Carminati L
- Carnesale M
- Caron S
- Carquin E
- Carra S
- Carratta G
- Carter JWS
- Carter TM
- Casadei D
- Casado MP
- Casha AF
- Castiglia EG
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
- Centonze MS
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen C
- Chen H
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clawson SE
- Clement C
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Codina EP
- Coelli S
- Cohen H
- Coimbra AEC
- Cole B
- Collot J
- Columbie JMC
- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Coutinho YA
- Cowan G
- Cowley JW
- Cranmer K
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosetti G
- Cueto A
- Cui H
- Cui Z
- Cukierman AR
- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- D'amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'onofrio A
- D'Onofrio M
- D'uffizi M
- Da Costa AMMJ
- da Costa JBG
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dattagupta A
- David C
- Davidek T
- Davis DR
- Davis-Purcell B
- Dawson I
- de Andrade LM
- De Araujo MV
- De Asmundis R
- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- De K
- de la Hoz SG
- De la Torre H
- De Lima RT
- De Maria A
- De Regie JBD
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Sousa MJDS
- De Souza EEP
- Dedovich DV
- Degens J
- Deiana AM
- Del Peso J
- Del Rio F
- Delegido AJG
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delsart PA
- Demers S
- Demichev M
- Denisov SP
- Derendarz D
- Derue F
- Dervan P
- Desch K
- Dette K
- Deutsch C
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
- Di Nardo R
- Diaconu C
- Dias BP
- Dias FA
- Diaz MA
- Didenko M
- Diehl EB
- Dimitriadi C
- Dimitrievska A
- Ding W
- Dingfelder J
- Dinu IM
- Dittmeier SJ
- Dittus F
- Djama F
- Djobava T
- Djuvsland JI
- Do Vale TD
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Dominguez LP
- Donadelli M
- Donaldson CP
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Santos SPA
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Drobac AS
- Du D
- du Pree TA
- Dubinin F
- Dubovsky M
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duflot L
- Duhrssen M
- Dulsen C
- Dumitriu AE
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Duren M
- Durglishvili A
- Dutta B
- Dwyer BL
- Dyckes GI
- Dyndal M
- Dysch S
- Dziedzic BS
- Eckerova B
- Eggleston MG
- Ehrke LF
- Eigen G
- Einsweiler K
- Ekelof T
- El Ghazali Y
- El Jarrari H
- El Moursli RC
- El Moussaouy A
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Ene I
- Erdmann J
- Ereditato A
- Erland PA
- Errenst M
- Escalier M
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- Zhemchugov A
- Zheng Z
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
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- Adamek L
- Addepalli SV
- Addison MJ
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- Zhemchugov A
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- Zhulanov V
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Search for pair production of squarks or gluinos decaying via sleptons or weak bosons in final states with two same-sign or three leptons with the ATLAS detector
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- Zhemchugov A
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 15/02/2024
- Field of study
A search for pair production of squarks or gluinos decaying via sleptons or weak bosons is reported. The search targets a final state with exactly two leptons with same-sign electric charge or at least three leptons without any charge requirement. The analysed data set corresponds to an integrated luminosity of 139 fb−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Multiple signal regions are defined, targeting several SUSY simplified models yielding the desired final states. A single control region is used to constrain the normalisation of the WZ + jets background. No significant excess of events over the Standard Model expectation is observed. The results are interpreted in the context of several supersymmetric models featuring R-parity conservation or R-parity violation, yielding exclusion limits surpassing those from previous searches. In models considering gluino (squark) pair production, gluino (squark) masses up to 2.2 (1.7) TeV are excluded at 95% confidence level
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Yacoob S
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang X
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
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