338 research outputs found
Hydrodynamics of R-charged D1-branes
- Author
- A Buchel
- A Buchel
- AW Peet
- C Buragohain
- CL Kane
- CP Herzog
- CP Herzog
- CP Herzog
- CP Herzog
- D Maity
- D Mateos
- DT Son
- DT Son
- G Policastro
- HJ Boonstra
- I Kanitscheider
- I Kanitscheider
- J Mas
- JD Bjorken
- JR David
- Justin R. David
- K Damle
- L Brey
- L-Y Hung
- M Cvetič
- M Rangamani
- Manavendra Mahato
- N Banerjee
- N Iqbal
- N Itzhaki
- O Saremi
- P Kovtun
- PK Kovtun
- S Barrau
- S Jain
- SA Hartnoll
- SA Hartnoll
- Somyadip Thakur
- Spenta R. Wadia
- T Harmark
- VV Deshpande
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 25/08/2010
- Field of study
We study the hydrodynamic properties of strongly coupled SU(N) Yang-Mills
theory of the D1-brane at finite temperature and at a non-zero density of
R-charge in the framework of gauge/gravity duality. The gravity dual
description involves a charged black hole solution of an
Einstein-Maxwell-dilaton system in 3 dimensions which is obtained by a
consistent truncation of the spinning D1-brane in 10 dimensions. We evaluate
thermal and electrical conductivity as well as the bulk viscosity as a function
of the chemical potential conjugate to the R-charges of the D1-brane. We show
that the ratio of bulk viscosity to entropy density is independent of the
chemical potential and is equal to 1/4π. The thermal conductivity and bulk
viscosity obey a relationship similar to the Wiedemann-Franz law. We show that
at the boundary of thermodynamic stability, the charge diffusion mode becomes
unstable and the transport coefficients exhibit critical behaviour. Our method
for evaluating the transport coefficients relies on expressing the second order
differential equations in terms of a first order equation which dictates the
radial evolution of the transport coefficient. The radial evolution equations
can be solved exactly for the transport coefficients of our interest. We
observe that transport coefficients of the D1-brane theory are related to that
of the M2-brane by an overall proportionality constant which sets the
dimensions.Comment: 57 pages, 12 figure
Healing Potential of Picrorhiza kurroa (Scrofulariaceae) rhizomes against indomethacin-induced gastric ulceration: a mechanistic exploration.
- Author
- A Chevallier
- A Krishnamurthy
- A Schmassmann
- B Saraswat
- B Shukla
- Biswanath Maity
- C Hawkins
- D Banerjee
- D Banerjee
- D Dokmeci
- Debashish Banerjee
- F Halter
- J Sedlak
- J Shigeta
- JL Wallace
- JR Avila
- K Biswas
- K Yokoi
- KD Rainsford
- L Ma
- LR Johnson
- M Singh
- M Tariq
- MK Jones
- O Dormond
- PK Visen
- R Pai
- RJ Gryglewski
- S Bhattacharya
- S Hassan
- S Swarnakar
- S Szabo
- S Szabo
- S Szabo
- Sandip K Bandyopadhyay
- Subrata Chattopadhyay
- Subrata K Nag
- T Yoshikawa
- TA Miller
- Y Naito
- Publication venue
- BioMed Central
- Publication date
- 01/01/2008
- Field of study
<p>Abstract</p> <p>Background</p> <p>The present study was undertaken to evaluate the potential of the rhizomes of the Indian medicinal plant, <it>Picrorhiza kurroa </it>in healing indomethacin-induced acute stomach ulceration in mice and examine its capacity to modulate oxidative stress and the levels of prostaglandin (PGE<sub>2</sub>) and EGF during the process.</p> <p>Methods</p> <p>Male swiss albino mice, ulcerated with indomethacin (18 mg/kg, p. o., single dose) were treated up to 7 days with different doses of the methanol extract of <it>P. kurroa </it>rhizomes (designated as PK). The healing capacity of the most effective dose of PK (20 mg/kg, p. o. × 3 d) was compared with that of omeprazole (Omez) (3 mg/kg, p. o. × 3 d). The effects of the drug-treatment for one and three days on the biochemical parameters were assessed by comparing the results with that of untreated mice of the 1<sup>st </sup>and 3<sup>rd </sup>day of ulceration. The stomach tissues of the mice were used for the biochemical analysis.</p> <p>Results</p> <p>The macroscopic indices revealed maximum ulceration on the 3<sup>rd </sup>day after indomethacin administration, which was effectively healed by PK. Under the optimized treatment regime, PK and Omez reduced the ulcer indices by 45.1% (<it>P </it>< 0.01), and 76.3% respectively (<it>P </it>< 0.001), compared to the untreated ulcerated mice.</p> <p>Compared to the ulcerated untreated mice, those treated with PK for 3 days showed decreased the levels of thiobarbituric acid reactive substances (TBARS) (32.7%, <it>P </it>< 0.05) and protein carbonyl (37.7%, <it>P </it>< 0.001), and increased mucin (42.2%, <it>P </it>< 0.01), mucosal PGE<sub>2 </sub>(21.4%, <it>P </it>< 0.05), and expressions of COX-1 and 2 (26.9% and 18.5%, <it>P </it>< 0.05), EGF (149.0%, <it>P </it>< 0.001) and VEGF (56.9%, <it>P </it>< 0.01). Omez reduced the TBARS (29.4%, <it>P </it>< 0.05), and protein carbonyl (38.9%, <it>P </it>< 0.001), and increased mucin (38.3%, <it>P </it>< 0.01), without altering the other parameters significantly.</p> <p>Conclusion</p> <p>PK (20 mg/kg, p. o. × 3 days) could effectively heal indomethacin-induced stomach ulceration in mice by reducing oxidative stress, and promoting mucin secretion, prostaglandin synthesis and augmenting expressions of cyclooxygenase enzymes and growth factors.</p
Characterization of Sn Doped ZnS Thin Films Synthesized by CBD
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Spectral function of the supersymmetry current
- Author
- A Donos
- A Donos
- C Hoyos
- D Maity
- Daniel Waldram
- DF Mross
- DK Brattan
- DR Gulotta
- DZ Freedman
- E Gubankova
- EW Leaver
- F Benini
- F Benini
- F Denef
- F Denef
- F Denef
- G Policastro
- H Liu
- I Bah
- J-W Chen
- Jerome P. Gauntlett
- JP Gauntlett
- JP Gauntlett
- JP Gauntlett
- JP Gauntlett
- JP Wu
- Julian Sonner
- K Kratzert
- L Huijse
- L-Y Hung
- L-Y Hung
- M Ammon
- M Cubrovic
- M Cubrovic
- M Cubrovic
- M Edalati
- M Edalati
- M Edalati
- M Rangamani
- N Iqbal
- N Iqbal
- P Basu
- P Grassi
- P Kovtun
- PK Kovtun
- R Belliard
- S Kachru
- S Kachru
- S Sachdev
- S-S Lee
- SA Hartnoll
- SA Hartnoll
- SA Hartnoll
- SA Hartnoll
- SJ Yamamoto
- SS Gubser
- SS Gubser
- SS Gubser
- T Albash
- T Albash
- T Faulkner
- T Faulkner
- T Faulkner
- T Hartman
- V Lebedev
- V Parente
- X Arsiwalla
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 12/12/2011
- Field of study
We continue our study of the retarded Green's function of the universal
fermionic supersymmetry current ("supercurrent") for the most general class of
d=3 N=2 SCFTs with D=10 or D=11 supergravity duals by studying the propagation
of the Dirac gravitino in the electrically charged AdS-Reissner-Nordstr\"om
black-brane background of N=2 minimal gauged supergravity in D=4. We expand
upon results presented in a companion paper, including the absence of a Fermi
surface and the appearance of a soft power-law gap at zero temperature. We also
present the analytic solution of the gravitino equation in the AdS_2 X R^2
background which arises as the near-horizon limit at zero temperature. In
addition we determine the quasinormal mode spectrum.Comment: 65 pages, 6 Figs; version published in journa
Cytoskeletal control of B cell responses to antigens.
- Author
- A Bergtold
- A Castello
- A Chaudhuri
- A Douglass
- A Leithner
- A Meyer-Bahlburg
- A Noy
- A Saci
- A Stoddart
- A-C Reymann
- AB Verkhovsky
- AE Hauser
- AJ Thrasher
- AT Ritter
- B Liu
- B Treanor
- B Treanor
- BA Heesters
- BE Barnett
- BE Collins
- BF Lillemeier
- C Fu
- C Jurchenko
- C Ketchum
- C Liu
- C Liu
- CD Browne
- CDC Allen
- CJ Staiger
- CR Nowosad
- D Depoil
- D Goswami
- D Li
- D Pore
- D Seo
- D Tischer
- DA Moulding
- DV Köster
- E Arana
- E Evans
- E Janssen
- E Natkanski
- F Baumgart
- F Gasparrini
- F Huang
- F Vascotto
- FD Batista
- G Salbreux
- GD Victora
- GD Victora
- GM Rivera
- GOC Cory
- H Ennomani
- H Park
- H Park
- I Derényi
- I Taniuchi
- IM Antón
- J Derry
- J Heo
- J Lee
- J Müller
- J Prost
- J Yang
- J Yi
- JA Ditlev
- JD Rotty
- JL Maravillas-Montero
- JR Moffitt
- K Gowrishankar
- K Jaqaman
- K Kläsener
- K Kruse
- KG Campellone
- KH Hu
- KL Randall
- KM Eisenmann
- KM Spillane
- KT Roybal
- L Balagopalan
- L Cai
- L Haviv
- L Westerberg
- L Xu
- LS Westerberg
- M Bovellan
- M Burbage
- M Fritzsche
- M Fritzsche
- M Kaksonen
- M Maekawa
- M Murrell
- M Oser
- M Recher
- M Vicente-Manzanares
- M Weber
- M-II Yuseff
- MJ Massaad
- MJ Massaad
- MJ Walmsley
- MK Seeley-Fallen
- MP Blundell
- MP Sheetz
- N Abdul-Manan
- N Billington
- N Billington
- N Bufi
- N Gerasimcik
- N Gupta
- N Morone
- N Parameswaran
- N Ramesh
- N Tomasevic
- NS Kolhatkar
- NS Kolhatkar
- O López-Ortega
- O Thaunat
- OD Weiner
- P Tolar
- P Tolar
- Pavel Tolar
- PC Maity
- PK Mattila
- PK Mattila
- R Basu
- R Basu
- R Hoogeboom
- R Muñoz-Fernández
- R Sarkar
- RA Floto
- RB Birge
- RB Henderson
- RI Ludowyke
- S Becker-Herman
- S Hao
- S Kumari
- S Kühn
- S Malhotra
- S Murugesan
- S Sato
- S Satpathy
- S Seo
- S Sharma
- S Volpi
- S Wolkerstorfer
- S Zhang
- SA Freeman
- SA Freeman
- SB Padrick
- SJ Fleire
- SJ Keppler
- SK Donnelly
- SP Chaki
- SR Brooks
- ST Kim
- T Schnyder
- TA Schwickert
- TA Schwickert
- TD Pollard
- TF Brazão
- TF Tedder
- TS Gomez
- VLJ Tybulewicz
- W Chen
- W-HW Lin
- WJ Polacheck
- X Liu
- X Su
- Y Carrasco
- Y Fang
- Y Harada
- Y Liu
- Y Sawada
- Y Zeng
- Y Zhang
- YR Carrasco
- YR Carrasco
- Z Kalay
- Z Ma
- Z Wan
- Z Wan
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/07/2017
- Field of study
The actin cytoskeleton is essential for cell mechanics and has increasingly been implicated in the regulation of cell signalling. In B cells, the actin cytoskeleton is extensively coupled to B cell receptor (BCR) signalling pathways, and defects of the actin cytoskeleton can either promote or suppress B cell activation. Recent insights from studies using single-cell imaging and biophysical techniques suggest that actin orchestrates BCR signalling at the plasma membrane through effects on protein diffusion and that it regulates antigen discrimination through the biomechanics of immune synapses. These mechanical functions also have a role in the adaptation of B cell subsets to specialized tasks during antibody responses
Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at root s=8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adzic P
- Agapitos A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Al-bataineh A
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alimena J
- Almond J
- Alunni Solestizi L
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Amsler C
- Anagnostou G
- Anderson D
- Anderson I
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Anelli C
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asilar E
- Asin I
- Askew A
- Ata M
- Attikis A
- Aubin A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Awad A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Baber M
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baffioni S
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
- Ball F
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Barbieri R
- Bargassa P
- Baringer P
- Barker A
- Barnes VE
- Barney D
- Baron O
- Barone L
- Barria P
- Bartek R
- Barth C
- Bartosik N
- Bartók M
- Baskakov A
- Battilana C
- Baty A
- Bauerdick LAT
- Baumgartel D
- Baus C
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Beck L
- Beernaert K
- Behera PK
- Behnamian H
- Behnke O
- Behrens U
- Bein S
- Beirão Da Cruz E Silva C
- Belchior Batista Das Chagas E
- Belforte S
- Beliy N
- Belknap DA
- Bell KW
- Bellan R
- Belloni A
- Beluffi C
- Belyaev A
- Belyaev A
- Benato L
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Beni N
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Besancon M
- Betchart B
- Betts RR
- Bhandari R
- Bhardwaj A
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhawandeep U
- Bhopatkar V
- Bhowmik S
- Bi R
- Bialkowska H
- Bian JG
- Bianchini L
- Bianco S
- Bierwagen K
- Biino C
- Bilei GM
- Bilin B
- Bilki B
- Bilmis S
- Bin Anuar AA
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Boccali T
- Bocci A
- Bodek A
- Boimska B
- Boletti A
- Bolla G
- Bonacorsi D
- Bonato A
- Bondu O
- Boos E
- Bornheim A
- Borras K
- Bortignon P
- Borzou A
- Bose S
- Bose T
- Botta C
- Boudoul G
- Bouhali O
- Bourilkov D
- Bouvier E
- Bradmiller-Feld J
- Braghieri A
- Braibant-Giacomelli S
- Brandstetter J
- Brandt S
- Branson JG
- Breedon R
- Breto G
- Brew C
- Brianza L
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Brinson J
- Brito L
- Brivio F
- Brochero Cifuentes JA
- Brochet S
- Brodski M
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brun H
- Bruner C
- Bruno G
- Buchmuller O
- Bucinskaite I
- Bundock A
- Bunin P
- Bunkowski K
- Bunn J
- Buontempo S
- Burkett K
- Burns D
- Burns D
- Burt K
- Burton D
- Busson P
- Busza W
- Butler JN
- Butler PH
- Buttignol M
- Butz E
- Bylsma B
- Byszuk A
- Bäni L
- Cabrera A
- Cabrillo IJ
- Cadamuro L
- Caillol C
- Cakir A
- Calabria C
- Calamba A
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Call K
- Calligaris L
- Calpas B
- Calvelli V
- Calvert B
- Calvo E
- Caminada L
- Campagnari C
- Campanini R
- Campbell A
- Camporesi T
- Candelise V
- Canelli MF
- Cankocak K
- Capiluppi P
- Caputo C
- Carlin R
- Carlson B
- Carnes A
- Carrera Jarrin E
- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho Antunes De Oliveira A
- Carvalho W
- Carver M
- Casal B
- Casarsa M
- Casasso S
- Casimiro Linares E
- Castaldi R
- Castaneda Hernandez A
- Castello R
- Castilla-Valdez H
- Castiñeiras De Saa JR
- Castle J
- Castro A
- Caudron A
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Celik A
- Centis Vignali M
- Cepeda M
- Cerati GB
- Cerminara G
- Cerrada M
- Chabert EC
- Chamizo Llatas M
- Chang P
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Chaparro Sierra LF
- Chapon E
- Charaf O
- Charlot C
- Chasco M
- Chatterjee A
- Chatterjee K
- Chatterjee RM
- Chauhan S
- Chauhan S
- Chaves J
- Chawla R
- Checchia P
- Chen GM
- Chen HS
- Chen KF
- Chen KH
- Chen M
- Chen PH
- Chen Y
- Chen Y
- Chen Z
- Chenarani S
- Cheng T
- Cherepanov V
- Chertok M
- Cheung HWK
- Chhibra SS
- Chierici R
- Chinellato J
- Chiochia V
- Chiorboli M
- Chistov R
- Chlebana F
- Cho S
- Choi M
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury S
- Chtchipounov L
- Chu J
- Chudasama R
- Chwalek T
- Ciangottini D
- Cieri D
- Cihangir S
- Cimmino A
- Ciocci MA
- Cipriani M
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clarke C
- Clement E
- Clerbaux B
- Cockerill DJA
- Cocoros A
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Colombo F
- Connor P
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cornelis T
- Corpe L
- Correa Martins Junior M
- Cossutti F
- Costa M
- Costa S
- Costanza F
- Coubez X
- Couderc F
- Coughlan JA
- Courbon B
- Cousins R
- Covarelli R
- Cowden C
- Cox B
- Cox PT
- Creanza D
- Cremonesi M
- Cristella L
- Cuevas J
- Cuffiani M
- Cumalat JP
- Curras E
- Curry D
- Cussans D
- Custódio A
- Cutts D
- Czellar S
- Da Costa EM
- Da Silveira GG
- Dabrowski A
- Daci N
- Dahmes B
- Dalchenko M
- Dallavalle GM
- Dall’Osso M
- Damarseckin S
- Damgov J
- Danilov M
- Daponte V
- Das S
- Daskalakis G
- Dasu S
- Dauncey P
- David A
- Davies G
- Davignon O
- de Barbaro P
- De Boer W
- De Bruyn I
- De Castro Manzano P
- De Cosa A
- De Filippis N
- De Gruttola M
- De Guio F
- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- De Nardo G
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Trocóniz JF
- De Visscher S
- De Wit A
- De Wolf EA
- Degano A
- Deiters K
- Dejardin M
- Del Re D
- Delaere C
- Delannoy AG
- Delannoy H
- Delcourt M
- Delgado Peris A
- Delgado A
- Della Negra M
- Della Ricca G
- Dell’Orso R
- Demaria N
- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Depasse P
- Derdzinski M
- Dermenev A
- Deroover K
- Dev N
- Devetak D
- Dewanjee RK
- Dey S
- Di Francesco A
- Di Guida S
- Di Marco E
- Di Matteo L
- Di Mattia A
- Diamond B
- Diemoz M
- Dierlamm A
- Dietz C
- Dietz-Laursonn E
- Diez Pardos C
- Dildick S
- Dilsiz K
- Dimitrov A
- Dinardo ME
- Dishaw A
- Dissertori G
- Dittmann J
- Dittmar M
- Dittmer S
- Doan TH
- Dobson M
- Dobur D
- Dodd L
- Dogra S
- Dolen J
- Dolinska G
- Dominguez A
- Donato S
- Donegà M
- Dordevic M
- Dorigo T
- Dorney B
- Doroba K
- Dosselli U
- Dozen C
- Draeger AR
- Dragicevic M
- Dragoiu C
- Dremin I
- Dreyer T
- Driga O
- du Pree T
- Du R
- Duarte J
- Dube S
- Dubinin M
- Duchardt D
- Dudenas V
- Dudero PR
- Dudko L
- Dugad S
- Duggan D
- Duh YT
- Dumanoglu I
- Dunne P
- Dupont N
- Durgut S
- Duric S
- Durkin LS
- Dutt S
- Dutta D
- Dutta S
- Dutta V
- Dünser M
- D’Agnolo RT
- D’Alessandro R
- D’Alfonso M
- d’Enterria D
- D’Hondt J
- D’imperio G
- Eckerlin G
- Ecklund KM
- Eckstein D
- Eerola P
- Eggert N
- Eichhorn T
- El Mamouni H
- Elgammal S
- Eller P
- Elliott-Peisert A
- Ellison J
- Elmer P
- Elumakhov D
- Elvira VD
- Elwood A
- Eminizer N
- Endres M
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erdogan Y
- Erdweg S
- Erfle J
- Ershov A
- Erö J
- Escalante Del Valle A
- Esch T
- Eshaq Y
- Eskandari Tadavani E
- Esposito M
- Etesami SM
- Eusebi R
- Evangelou I
- Evans A
- Evdokimov O
- Everaerts P
- Fabbri F
- Fabbri F
- Fabbro B
- Fabozzi F
- Faccioli P
- Fagot A
- Fahim A
- Fan J
- Fanfani A
- Fang W
- Fangmeier C
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
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- Yumiceva F
- Yusli MN
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- Zahid S
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- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zenaiev O
- Zeuner WD
- Zghiche A
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- Zhokin A
- Zhu DH
- Zhu RY
- Zich J
- Zielinski K
- Ziemons T
- Zientek M
- Zlebcik R
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Österberg K
- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Combination of CMS searches for heavy resonances decaying to pairs of bosons or leptons
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abercrombie D
- Acharya H
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- Verzetti M
- Verzocchi M
- Veszpremi V
- Vesztergombi G
- Vidal R
- Vila I
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- Wiedenbeck S
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- Womersley WJ
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- Wrthwein F
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- Wyslouch B
- Xia F
- Xiao M
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- Xie S
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- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zghiche A
- Zhang A
- Zhang F
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- Publication venue
- Elsevier
- Publication date
- 01/01/2019
- Field of study
CMS Collaboration: et al.A statistical combination of searches for heavy resonances decaying to pairs of bosons or leptons is presented. The data correspond to an integrated luminosity of 35.9 fb collected during 2016 by the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV. The data are found to be consistent with expectations from the standard model background. Exclusion limits are set in the context of models of spin-1 heavy vector triplets and of spin-2 bulk gravitons. For mass-degenerate W′ and Z′ resonances that predominantly couple to the standard model gauge bosons, the mass exclusion at 95% confidence level of heavy vector bosons is extended to 4.5 TeV as compared to 3.8 TeV determined from the best individual channel. This excluded mass increases to 5.0 TeV if the resonances couple predominantly to fermions.Individuals have received support from the Marie-Curie program and the European Research Council and Horizon 2020 Grant, contract Nos. 675440, 752730, and 765710 (European Union); the Programa Estatal de Fomento de la Investigación Científica y Técnica de Excelencia María de Maeztu, grant MDM-2015-0509 and the Programa Severo Ochoa del Principado de Asturias
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