1,270 research outputs found
Intubation without muscle relaxation for suspension laryngoscopy: A randomized, controlled study
- Publication venue
- 'African Journals Online (AJOL)'
- Publication date
- 23/06/2014
- Field of study
Objective and Aim: The objective of the following study is to examine the effectiveness and safety of suspension laryngoscopy under intubation with propofol and remifentanil alone for vocal fold nodule (VFN) excision.Materials and Methods: A total of 40 patients were equally and randomly assigned to elective VFN excision using suspension laryngoscopy under intubation with propofol and remifentanil alone (Group A) or with supplementary cisatracurium (Group B).Results: Intubation time was significantly longer in Group A than in Group B (300.0 } 30.0 s vs. 265.2 } 38.7 s, P = 0.003). The two groups showed similar Cormack.Lehane classifications, intubation conditions and ease ofsuspension laryngoscopy. Both groups showed favorable cardiopulmonary safety profiles. Post.anesthesia recovery was significantly more rapid in Group A than in Group B, in terms of times to spontaneous breathing return (7.2 } 1.4 min vs. 10.9 } 1.6 min, P < 0.001), consciousness return (7.4 } 1.5 min vs. 12.3 } 1.8 min, P < 0.001), removal of tracheal intubation (8.1 } 1.5 min vs. 13.2 } 1.7 min, P < 0.001) and operating room discharge (12.7 } 1.4 min vs. 22.1 } 1.3 min, P < 0.001).Conclusion: Use of propofol and remifentanil alone provides favorable intubation and anesthesia conditions for suspension laryngoscopic VFN excision and accelerates post.anesthesia recovery.Key words: Endotracheal intubation, muscle relaxant, propofol, randomized controlled study, remifentanil, suspension laryngoscopy, vocal fold nodul
Observation of a ppb mass threshoud enhancement in \psi^\prime\to\pi^+\pi^-J/\psi(J/\psi\to\gamma p\bar{p}) decay
- Author
- Ablikim M
- Achasov MN
- An L
- An Q
- An ZH
- Bai JZ
- Ban Y
- Berger N
- Bian JM
- Boyko I
- Briere RA
- Bytev V
- Cai X
- Cao GF
- Cao XX
- Chang JF
- Chelkov G
- Chen G
- Chen HS
- Chen JC
- Chen LP
- Chen ML
- Chen P
- Chen SJ
- ChenYB
- Chu YP
- CroninHennessy D
- Dai HL
- Dai JP
- Dedovich D
- Deng ZY
- Denysenko I
- Destefanis M
- Ding Y
- Dong LY
- Dong MY
- Du SX
- Duan MY
- Fang J
- Feng CQ
- Fu CD
- Fu JL
- Gao Y
- Geng C
- Goetzen K
- Gong WX
- Greco M
- Grishin S
- Gu YT
- Guo AQ
- Guo LB
- Guo YP
- Han SQ
- Harris FA
- He KL
- He M
- He ZY
- Heng YK
- Hou ZL
- Hu HM
- Hu JF
- Hu T
- Hu XW
- Huang B
- Huang GM
- Huang JS
- Huang XT
- Huang YP
- Ji CS
- Ji Q
- Ji XB
- Ji XL
- Jia LK
- Jiang LL
- Jiang XS
- Jiao JB
- Jin DP
- Jin S
- Komamiya S
- Kuehn W
- Lange S
- Leung JKC
- Li C
- Li C
- Li DM
- Li F
- Li G
- Li HB
- Li J
- Li JC
- Li L
- Li L
- Li QJ
- Li WD
- Li WG
- Li XL
- Li XN
- Li XQ
- Li XR
- Li YX
- Li ZB
- Liang H
- Liang TR
- Liang YF
- Liang YT
- Liao GR
- Liao XT
- Liu BJ
- Liu CL
- Liu CX
- Liu CY
- Liu F
- Liu F
- Liu FH
- Liu GC
- Liu H
- Liu HB
- Liu HM
- Liu HW
- Liu J
- Liu JP
- Liu K
- Liu KY
- Liu Q
- Liu SB
- Liu XH
- Liu Y
- Liu YB
- Liu YF
- Liu YW
- Liu ZA
- Lu GR
- Lu YP
- Luo CL
- Luo MX
- Luo T
- Luo XL
- LĂŒ JG
- LĂŒ QW
- LĂŒ XR
- Ma CL
- Ma FC
- Ma HL
- Ma QM
- Ma X
- Ma XY
- Maggiora M
- Mao YJ
- Mao ZP
- Min J
- Mo XH
- Muchnoi NYu
- Nefedov Y
- Ning FP
- Olsen SL
- Ouyang Q
- Pelizaeus M
- Peters K
- Ping JL
- Ping RG
- Poling R
- Pun CSJ
- Qi M
- Qian S
- Qiao CF
- Qiu JF
- Rong G
- Ruan XD
- Sarantsev A
- Shao M
- Shen CP
- Shen XY
- Sheng HY
- Sonoda S
- Spataro S
- Spruck B
- Sun DH
- Sun GX
- Sun JF
- Sun SS
- Sun XD
- Sun YJ
- Sun YZ
- Sun ZJ
- Sun ZT
- Tang CJ
- Tang X
- Tang XF
- Tian HL
- Toth D
- Varner GS
- Wan X
- Wang BQ
- Wang JK
- Wang K
- Wang LL
- Wang LS
- Wang P
- Wang PL
- Wang Q
- Wang SG
- Wang XD
- Wang XL
- Wang YD
- Wang YF
- Wang YQ
- Wang Z
- Wang ZG
- Wang ZY
- Wei DH
- Wen SP
- Wiedner U
- Wu LH
- Wu N
- Wu YM
- Wu Z
- Xiao ZJ
- Xie YG
- Xu GF
- Xu GM
- Xu H
- Xu M
- Xu M
- Xu XP
- Xu Y
- Xu ZZ
- Xue Z
- Yan L
- Yan WB
- Yan YH
- Yang HX
- Yang M
- Yang P
- Yang SM
- Yang YX
- Ye M
- Ye MH
- Yu BX
- Yu CX
- Yu L
- Yuan CZ
- Yuan Y
- Zeng Y
- Zhang BX
- Zhang BY
- Zhang CC
- Zhang DH
- Zhang HH
- Zhang HY
- Zhang JW
- Zhang JY
- Zhang JZ
- Zhang L
- Zhang SH
- Zhang XY
- Zhang Y
- Zhang YH
- Zhang ZP
- Zhao C
- Zhao HS
- Zhao JW
- Zhao JW
- Zhao L
- Zhao L
- Zhao MG
- Zhao Q
- Zhao SJ
- Zhao TC
- Zhao XH
- Zhao YB
- Zhao ZG
- Zhemchugov A
- Zheng B
- Zheng JP
- Zheng YH
- Zheng ZP
- Zhong B
- Zhong J
- Zhou L
- Zhou ZL
- Zhu C
- Zhu K
- Zhu KJ
- Zhu QM
- Zhu XW
- Zhu YS
- Zhu ZA
- Zhuang J
- Zou BS
- Zou JH
- Zuo JX
- Zweber P
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
The decay channel ÏâČâÏ+ÏâJ/Ï(J/ÏâÎłppËâ)
is studied using a sample of 1.06Ă108 ÏâČ events collected
by the BESIII experiment at BEPCII. A strong enhancement at threshold is
observed in the ppËâ invariant mass spectrum. The enhancement can be fit
with an S-wave Breit-Wigner resonance function with a resulting peak mass of
M=1861â13+6â(stat)â26+7â(syst)MeV/c2 and a
narrow width that is Î<38MeV/c2 at the 90% confidence level.
These results are consistent with published BESII results. These mass and width
values do not match with those of any known meson resonance.Comment: 5 pages, 3 figures, submitted to Chinese Physics
Shakedown Limits of Slab Track Substructures and Their Implications for Design
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2021
- Field of study
This paper presents an approach to shakedown of slab track substructures subjected to train loads. The train load is converted into a distributed moving load on the substructure surface using a simplified track analysis. Based on the lower-bound dynamic shakedown theorem, shakedown solutions for the slab track substructures are obtained over a range of train speeds between zero and the critical speed of the track. It is found the shakedown limit is largely influenced by the ratio of layer elastic moduli and the ratio of train speed to critical speed rather than their absolute values. An attenuation factor, as a function of the critical speed and the friction angle of subsoil, is proposed to effectively obtain the shakedown limit of the slab track substructure at any train speed. In light of the shakedown solutions, improvements to the existing design and analysis approaches are also suggested
Suppression of PP2A is critical for protection of melanoma cells upon endoplasmic reticulum stress
- Author
- A Ito
- A Mandic
- A Sullivan
- AM Coley
- C Xu
- CC Jiang
- CC Jiang
- CC Jiang
- CC Jiang
- CW Woo
- F Yang
- H Puthalakath
- HP Harding
- JE Vince
- KG Roberts
- KJ Yin
- L Zhang
- L Zhang
- L Zhuang
- LA Fecher
- LH Chen
- M Boyce
- M Deichmann
- M Rahmani
- M Schroder
- MJ Van Kanegan
- P Hersey
- P Hu
- R Ley
- R Ley
- S Gillespie
- S Mannava
- S Strack
- V Christen
- V Janssens
- V Janssens
- VA Nikolaou
- W Hsu
- Y Shi
- YF Wang
- Publication venue
- Nature Publishing Group
- Publication date
- 01/01/2012
- Field of study
Endoplasmic reticulum (ER) stress triggers apoptosis by activating Bim in diverse types of cells, which involves dephosphorylation of BimEL by protein phosphatase 2A (PP2A). However, melanoma cells are largely resistant to ER stress-induced apoptosis, suggesting that Bim activation is suppressed in melanoma cells undergoing ER stress. We show here that ER stress reduces PP2A activity leading to increased ERK activation and subsequent phosphorylation and proteasomal degradation of BimEL. Despite sustained upregulation of Bim at the transcriptional level, the BimEL protein expression was downregulated after an initial increase in melanoma cells subjected to pharmacological ER stress. This was mediated by increased activity of ERK, whereas the phosphatase activity of PP2A was reduced by ER stress in melanoma cells. The increase in ERK activation was, at least in part, due to reduced dephosphorylation by PP2A, which was associated with downregulation of the PP2A catalytic C subunit. Notably, instead of direct dephosphorylation of BimEL, PP2A inhibited its phosphorylation indirectly through dephosphorylation of ERK in melanoma cells. Taken together, these results identify downregualtion of PP2A activity as an important protective mechanism of melanoma cells against ER stress-induced apoptosis
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- 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
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
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- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
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- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
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- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carter JWS
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Cerda Alberich L
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chau CC
- Che S
- Chekanov S
- Chekulaev S
- Chelkov GA
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov M
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Chytka L
- Cieri D
- Ciesla KM
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark MR
- Clark PJ
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Cohen H
- Coimbra AEC
- Cole B
- Colijn AP
- Collot J
- Conde Muino P
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Corga KDV
- Cormier F
- Cormier KJR
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cowan G
- Cowley JW
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cukierman AR
- Cunningham WR
- Czekierda S
- Czodrowski P
- D'amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- da Costa JBG
- Da Fonseca Pinto J
- Da Via C
- Dabrowski W
- Dachs F
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Dann NS
- Danninger M
- Dao V
- Darbo G
- Dartsi O
- Dattagupta A
- Daubney T
- David C
- Davidek T
- Davis DR
- Dawson I
- De Asmundis R
- De Beurs M
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DEF
- De Lima RT
- De Maria A
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Sousa MJDCS
- De K
- Debenedetti C
- Dedovich D
- Deiana AM
- Del Peso J
- Delgove D
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Demontigny G
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Deutsch C
- Devesa MR
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Micco B
- Di Nardo R
- Di Petrillo KF
- Di Sipio R
- Diaconu C
- Dias FA
- Diaz LP
- Diaz MA
- Diaz YD
- Dickinson J
- Diehl EB
- Dietrich J
- Dimitrievska A
- Ding W
- Dingfelder J
- Dittus F
- Djama F
- Djobava T
- Djuvsland J
- Do Vale TD
- Dobre M
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Dominguez LP
- Don MMR
- Donadelli M
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
- Drobac AS
- Du D
- Duan Y
- Dubinin F
- Dubovsky M
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducourthial A
- Ducu OA
- Duda D
- Dudarev A
- Dudder AC
- Duelsen C
- Dueren M
- Duffeld EM
- DuflOt L
- Duhrssen M
- Dumancic M
- Dumitriu AE
- Duncan AK
- Dunford M
- Duperrin A
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dyckes G
- Dyndal M
- Dysch S
- Dziedzic BS
- Ecker KM
- Eggleston MG
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Jarrari H
- El Kossei R
- El Moursli RC
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Epland MB
- Erdmann J
- Ereditato A
- Erland PA
- Errenst M
- Escalier M
- Escobar C
- Estrada Pastor O
- Etzion E
- Evans H
- Ezhilov A
- Fabbri F
- Fabbri L
- Fabiani V
- Facini G
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fbâ1 of â s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
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- Abdelalim AA
- Abdesselam A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
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- Yilmaz M
- Yoosootiniya R
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Zitoun R
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- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Anastopoulos C
- Ancu LS
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- Zaidan R
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- Zambito S
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- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
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- Zhao Z
- Zhemchugov A
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
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- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Yang Z
- Yanush S
- Yao L
- Yao Y
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- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
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- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
- Zhang H
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- Zhang Z
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- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou Y
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fbâ1 of sâ=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan ÎČ < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
- Ahles R
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
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- Apolle R
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- Arguin J-F
- Argyropoulos S
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- Arik M
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- Arutinov D
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- Vannucci F
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vazquez JGP
- Vegni G
- Veillet JI
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- Ventura A
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- Venturi M
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- Vercesi V
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- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
- Virzi J
- Vitells O
- Viti M
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- Volpini G
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorwerk V
- Vos M
- Voss R
- Voss TT
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
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- Wahlen H
- Wahrmund S
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- Warburton A
- Ward CP
- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
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- Waugh AT
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- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Wengler T
- Wengu Z
- Wenig S
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- Werth M
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- Weydert C
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- Whitehead SR
- Whiteson D
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- Wijeratne PA
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- Yamamoto S
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- Yamazaki T
- Yamazaki Y
- Yan Z
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- Yang UK
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- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Ye J
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- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal ZâČ Models
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