529 research outputs found
Rationing tests for drug-resistant tuberculosis - who are we prepared to miss?
- Author
- A Faustini
- A Pantoja
- A Pooran
- A Vassall
- C Fitzpatrick
- D Martínez
- D Menzies
- DAJ Moore
- DAJ Moore
- David A. J. Moore
- E Tortoli
- EA Kendall
- EL Corbett
- GJ Churchyard
- JC Feres
- Jon S. Friedland
- Jorge Coronel
- K Kliiman
- KAK Angeby
- L Caviedes
- Laura J. Martin
- Louis Grandjean
- Luz Caviedes
- MA Espinal
- Martha H. Roper
- O Oxlade
- P Miotto
- PG Suárez
- PT Kent
- Robert H. Gilman
- SS Shin
- V Boonsarngsuk
- World Health Organization
- World Health Organization
- World Health Organization
- World Health Organization
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 03/02/2016
- Field of study
BACKGROUND: Early identification of patients with drug-resistant tuberculosis (DR-TB) increases the likelihood of treatment success and interrupts transmission. Resource-constrained settings use risk profiling to ration the use of drug susceptibility testing (DST). Nevertheless, no studies have yet quantified how many patients with DR-TB this strategy will miss. METHODS: A total of 1,545 subjects, who presented to Lima health centres with possible TB symptoms, completed a clinic-epidemiological questionnaire and provided sputum samples for TB culture and DST. The proportion of drug resistance in this population was calculated and the data was analysed to demonstrate the effect of rationing tests to patients with multidrug-resistant TB (MDR-TB) risk factors on the number of tests needed and corresponding proportion of missed patients with DR-TB. RESULTS: Overall, 147/1,545 (9.5%) subjects had culture-positive TB, of which 32 (21.8%) had DR-TB (MDR, 13.6%; isoniazid mono-resistant, 7.5%; rifampicin mono-resistant, 0.7%). A total of 553 subjects (35.8%) reported one or more MDR-TB risk factors; of these, 506 (91.5%; 95% CI, 88.9-93.7%) did not have TB, 32/553 (5.8%; 95% CI, 3.4-8.1%) had drug-susceptible TB, and only 15/553 (2.7%; 95% CI, 1.5-4.4%) had DR-TB. Rationing DST to those with an MDR-TB risk factor would have missed more than half of the DR-TB population (17/32, 53.2%; 95% CI, 34.7-70.9). CONCLUSIONS: Rationing DST based on known MDR-TB risk factors misses an unacceptable proportion of patients with drug-resistance in settings with ongoing DR-TB transmission. Investment in diagnostic services to allow universal DST for people with presumptive TB should be a high priority
Ultraspinning instability of anti-de Sitter black holes
- Author
- B Carter
- DJ Gross
- GW Gibbons
- H Elvang
- H Elvang
- H Elvang
- H Iguchi
- H Iguchi
- HK Kunduri
- HS Reall
- IY Park
- J Evslin
- JM Maldacena
- Jorge E. Santos
- K Izumi
- LN Trefethen
- M Shibata
- M Shibata
- MM Caldarelli
- MM Caldarelli
- MM Caldarelli
- MM Caldarelli
- O Aharony
- OJC Dias
- OJC Dias
- OJC Dias
- OJC Dias
- Pau Figueras
- PT Chrusciel
- R Emparan
- R Emparan
- R Emparan
- R Emparan
- R Emparan
- R Emparan
- R Emparan
- R Emparan
- R Gregory
- R Gregory
- R Monteiro
- R Monteiro
- RC Myers
- Ricardo Monteiro
- S Bhardwaj
- S Lahiri
- SS Gubser
- SS Gubser
- SW Hawking
- SW Hawking
- T Prestidge
- T Wiseman
- V Cardoso
- V Cardoso
- V Cardoso
- V Cardoso
- V Cardoso
- V Cardoso
- Y Brihaye
- Óscar J. C. Dias
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/12/2010
- Field of study
Myers-Perry black holes with a single spin in d>5 have been shown to be
unstable if rotating sufficiently rapidly. We extend the numerical analysis
which allowed for that result to the asymptotically AdS case. We determine
numerically the stationary perturbations that mark the onset of the
instabilities for the modes that preserve the rotational symmetries of the
background. The parameter space of solutions is thoroughly analysed, and the
onset of the instabilities is obtained as a function of the cosmological
constant. Each of these perturbations has been conjectured to represent a
bifurcation point to a new phase of stationary AdS black holes, and this is
consistent with our results.Comment: 22 pages, 7 figures. v2: Reference added. Matches published versio
Integrative analyses identify modulators of response to neoadjuvant aromatase inhibitors in patients with early breast cancer
- Author
- A Mackay
- AK Dunbier
- AK Dunbier
- Alan Mackay
- Alexey Larionov
- Anita K Dunbier
- Aradhana Rani
- Ash Nerurkar
- B Weigelt
- BP Coe
- C Curtis
- C Kent
- D Generali
- DG Albertson
- DS Tan
- Elena López-Knowles
- F Kreisel
- Helen Anderson
- HW Cheung
- IE Smith
- IE Smith
- J Hicks
- J Michael Dixon
- Jorge S Reis-Filho
- JS Foster
- K Lundgren
- L Osterberg
- LA Martin
- LA Martin
- LA Martin
- Lesley-Ann Martin
- LG Leon
- Lorna Renshaw
- M Dowsett
- M Mello-Grand
- M Scaltriti
- Mitch Dowsett
- MJ Ellis
- MT Weigel
- N Turner
- P Darbre
- P Lal
- Paul M Wilkerson
- Peter Osin
- PM Wilkerson
- PM Wilkerson
- PT Simpson
- R Beroukhim
- R Duprez
- R Katz-Brull
- R Natrajan
- R Natrajan
- R Natrajan
- Ricardo Ribas
- T Miyake
- T Troiani
- TK Lam
- William R Miller
- WR Miller
- WR Miller
- WR Miller
- WR Miller
- X Huo
- Y Zhao
- Z Ghazoui
- Zara Ghazoui
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Introduction
Aromatase inhibitors (AIs) are a vital component of estrogen receptor positive (ER+) breast cancer treatment. De novo and acquired resistance, however, is common. The aims of this study were to relate patterns of copy number aberrations to molecular and proliferative response to AIs, to study differences in the patterns of copy number aberrations between breast cancer samples pre- and post-AI neoadjuvant therapy, and to identify putative biomarkers for resistance to neoadjuvant AI therapy using an integrative analysis approach.
Methods
Samples from 84 patients derived from two neoadjuvant AI therapy trials were subjected to copy number profiling by microarray-based comparative genomic hybridisation (aCGH, n = 84), gene expression profiling (n = 47), matched pre- and post-AI aCGH (n = 19 pairs) and Ki67-based AI-response analysis (n = 39).
Results
Integrative analysis of these datasets identified a set of nine genes that, when amplified, were associated with a poor response to AIs, and were significantly overexpressed when amplified, including CHKA, LRP5 and SAPS3. Functional validation in vitro, using cell lines with and without amplification of these genes (SUM44, MDA-MB134-VI, T47D and MCF7) and a model of acquired AI-resistance (MCF7-LTED) identified CHKA as a gene that when amplified modulates estrogen receptor (ER)-driven proliferation, ER/estrogen response element (ERE) transactivation, expression of ER-regulated genes and phosphorylation of V-AKT murine thymoma viral oncogene homolog 1 (AKT1).
Conclusions
These data provide a rationale for investigation of the role of CHKA in further models of de novo and acquired resistance to AIs, and provide proof of concept that integrative genomic analyses can identify biologically relevant modulators of AI response
Diagnosis, Genetics, and Therapy of Short Stature in Children: A Growth Hormone Research Society International Perspective
- Author
- Ambler G
- Backeljauw PF
- Bidlingmaier M
- Biller BMK
- Boguszewski MCS
- Cheung PT
- Choong CSY
- Cohen LE
- Cohen P
- Collett-Solberg PF
- Dauber A
- Deal CL
- Gong C
- Hasegawa Y
- Hoffman AR
- Hofman PL
- Horikawa R
- Jorge AAL
- Juul A
- Kamenický P
- Khadilkar V
- Kopchick JJ
- Kriström B
- Lopes ML
- Luo X
- Miller BS
- Misra M
- Netchine
- Radovick S
- Ranke MB
- Rogol AD
- Rosenfeld RG
- Saenger P
- Wit JM
- Woelfle J
- Publication venue
- 'S. Karger AG'
- Publication date
- 01/01/2019
- Field of study
The Growth Hormone Research Society (GRS) convened a Workshop in March 2019 to evaluate the diagnosis and therapy of short stature in children. Forty-six international experts participated at the invitation of GRS including clinicians, basic scientists, and representatives from regulatory agencies and the pharmaceutical industry. Following plenary presentations addressing the current diagnosis and therapy of short stature in children, breakout groups discussed questions produced in advance by the planning committee and reconvened to share the group reports. A writing team assembled one document that was subsequently discussed and revised by participants. Participants from regulatory agencies and pharmaceutical companies were not part of the writing process. Short stature is the most common reason for referral to the pediatric endocrinologist. History, physical examination, and auxology remain the most important methods for understanding the reasons for the short stature. While some long-standing topics of controversy continue to generate debate, including in whom, and how, to perform and interpret growth hormone stimulation tests, new research areas are changing the clinical landscape, such as the genetics of short stature, selection of patients for genetic testing, and interpretation of genetic tests in the clinical setting. What dose of growth hormone to start, how to adjust the dose, and how to identify and manage a suboptimal response are still topics to debate. Additional areas that are expected to transform the growth field include the development of long-acting growth hormone preparations and other new therapeutics and diagnostics that may increase adult height or aid in the diagnosis of growth hormone deficiency.info:eu-repo/semantics/publishedVersio
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boimska B
- Boldizsar L
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondu O
- Bontenackels M
- Boos E
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bortoletto D
- Bose S
- Bose T
- Bostock F
- Botta C
- Boudoul G
- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Broccolo G
- Brochero Cifuentes JA
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmann MA
- Buchmuller O
- Bunkowski K
- Bunn J
- Buontempo S
- Burgmeier A
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
- Campbell A
- Camporesi T
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carrillo Moreno S
- Carroll R
- Cartiglia N
- Carvalho W
- Casal B
- Casimiro Linares E
- Castaldi R
- Castello R
- Castilla-Valdez H
- Castro A
- Castro E
- Caudron J
- Caulfield M
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
- Chen M
- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Cho Y
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cooper W
- Cornelis T
- Correa Martins Junior M
- Cortezon EP
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
- David A
- Davids M
- Davies G
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Troconiz JF
- De Visscher S
- De Wolf EA
- Deisher A
- Deiters K
- Dejardin M
- del Arbol PMR
- Del Re D
- Delaere C
- Delgado Peris A
- Deliomeroglu M
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demortier L
- Denegri D
- Deniz M
- Depasse P
- Dermenev A
- Dero V
- Dhingra N
- Di Giovanni GP
- Di Guida S
- Di Marco E
- Di Matteo L
- Diamond B
- Dias FA
- Diemoz M
- Dierlamm A
- Dietz C
- Dietz-Laursonn E
- Diez Pardos C
- Dimitrov A
- Dinardo ME
- Dirkes G
- Dissertori G
- Dittmar M
- Djordjevic M
- Dobrzynski L
- Dobson M
- Dobur D
- Doesburg R
- Dogangun O
- Dolen J
- Dominguez Vazquez D
- Dominguez A
- Dominik W
- Don CKK
- Dorigo T
- Dorney B
- Doroba K
- Dozen C
- Draeger J
- Dragicevic M
- Dragoiu C
- Drell BR
- Dremin I
- Drouhin F
- Drozdetskiy A
- du Pree T
- Duarte Campderros J
- Duarte J
- Dubinin M
- Dudero PR
- Dudko L
- Duenser M
- Dugad S
- Duggan D
- Dumanoglu I
- Dupont-Sagorin N
- Duric S
- Duris J
- Durkin LS
- Duru F
- Dutta D
- Dutta S
- Dutta V
- Dzelalija M
- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
- Eerola P
- Efron J
- Eggert N
- Ekmedzic M
- El Mamouni H
- Elgammal S
- Elliott-Peisert A
- Ellison J
- Elmer P
- Elvira VD
- Enderle H
- Engh D
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erfle J
- Erhan S
- Ero J
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- Ershov A
- Esen S
- Eshaq Y
- Eskut E
- Etesami SM
- Eugster J
- Eusebi R
- Evangelou I
- Evans D
- Everaerts P
- Everett A
- Evstyukhin S
- Fabbri F
- Fabbri F
- Fabbricatore P
- Fabbro B
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- Fabozzi F
- Faccioli P
- Fahim A
- Falkiewicz A
- Fanelli C
- Fanfani A
- Fano L
- Fantasia C
- Farrell C
- Fasanella D
- Fassi F
- Faure JL
- Favaro C
- Favart D
- Fay J
- Fedi G
- Fehling D
- Feindt M
- Felcini M
- Feld L
- Ferapontov A
- Ferencek D
- Ferguson T
- Ferguson W
- Fernandez Bedoya C
- Fernandez Menendez J
- Fernandez Perez Tomei TR
- Fernandez Ramos JP
- Fernandez M
- Ferrando A
- Ferri F
- Ferro C
- Field RD
- Finger M
- Finger M
- Fiore L
- Fiorendi S
- Fiori F
- Fisher M
- Fisk I
- Flacher H
- Flanagan W
- Flix J
- Florez C
- Flossdorf A
- Flowers K
- Flucke G
- Flugge G
- Foa L
- Focardi E
- Folgueras S
- Fonseca De Souza S
- Fontaine J-C
- Ford WT
- Forthomme L
- Foudas C
- Fouz MC
- Franci D
- Francis B
- Franzoni G
- Frazier R
- Freeman J
- Freudenreich K
- Friedl M
- Friis E
- Frisch B
- Frosali S
- Frueboes T
- Fruhwirth R
- Fu Y
- Fulcher J
- Funk W
- Furic IK
- Futyan D
- Gabathuler K
- Gabella W
- Gabusi M
- Gaddi A
- Galanti M
- Gallinaro M
- Gallo E
- Gamsizkan H
- Ganguly S
- Ganjour S
- Gao Y
- Garcia G
- Garcia-Abia P
- Garcia-Bellido A
- Gardner M
- Garrido RGR
- Gartner J
- Gary JW
- Gascon S
- Gasparini F
- Gataullin M
- Gaultney V
- Gauthier L
- Gavrilov V
- Gay APR
- Gaz A
- Gebbert U
- Geenen H
- Geffert P
- Geiser A
- Geisler M
- Gele D
- Genchev V
- Gennai S
- Georgiou G
- Geralis T
- Gerbaudo D
- Gerber CE
- Gershtein Y
- Gerwig H
- Geurts FJM
- Ghete VM
- Ghezzi A
- Giacomelli P
- Giammanco A
- Giassi A
- Gibbons LK
- Giffels M
- Gigi D
- Gilbert A
- Gill K
- Gilmore J
- Giordano D
- Giordano F
- Girgis S
- Giunta M
- Giurgiu G
- Givernaud A
- Glege F
- Gleyzer SV
- Gninenko S
- Goadhouse S
- Gobbo B
- Godang R
- Godinovic N
- Godshalk A
- Goerlach U
- Goerner M
- Goh J
- Gokbulut G
- Gokieli R
- Goldberg S
- Goldenzweig P
- Goldstein J
- Golf F
- Gollapinni S
- Golovtsov V
- Golubev N
- Golunov A
- Golutvin I
- Gomber B
- Gomez Moreno B
- Gomez G
- Gomez JA
- Goncharov M
- Gonzalez Caballero I
- Gonzalez Lopez O
- Gonzalez Sanchez J
- Gonzalez JS
- Gonzi S
- Goodell J
- Gorbounov N
- Gorski M
- Gotra Y
- Gottschalk E
- Goulianos K
- Gouskos L
- Gouzevitch M
- Govoni P
- Gowdy S
- Goy Lopez S
- Gozzelino A
- Grab C
- Grachov O
- Gramenitski I
- Grandi C
- Gras P
- Grassi M
- Gray L
- Gray R
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- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta MV
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yu I
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
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- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
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- Acosta JG
- Acosta MV
- Adair A
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- Adiguzel A
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- Afanasiev S
- Agostino L
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- Wickramage N
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- Williams G
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- Winer BL
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV 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
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- Zhemchugov A
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- Zobernig G
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- Zur Nedden M
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- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) 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<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Yilmaz Y
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- Yun JC
- Zabel J
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- Zeinali M
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- Zheng Y
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
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- Abbott B
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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 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between 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
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