1,494 research outputs found
Search for CP violation in D0 and D+ decays
- Author
- JM. Link
- VS. Paolone
- M. Reyes
- PM. Yager
- JC. Anjos
- I. Bediaga
- C. Gobel
- J. Magnin
- JM. de Miranda
- IM. Pepe
- AC. dos Reis
- FRA. Simao
- S. Carrillo
- E. Casimiro
- H. Mendez
- A. Sanchez-Hernandez
- C. Uribe
- F. Vazquez
- L. Cinquini
- JP. Cumalat
- JE. Ramirez
- B. O'Reilly
- EW. Vaandering
- JN. Butler
- HWK. Cheung
- I. Gaines
- PH. Garbincius
- LA. Garren
- E. Gottschalk
- SA. Gourlay
- PH. Kasper
- AE. Kreymer
- S. Bianco
- FL. Fabbri
- S. Sarwar
- A. Zallo
- C. Cawlfield
- R. Kutschke
- DY. Kim
- KS. Park
- A. Rahimi
- J. Wiss
- R. Gardner
- YS. Chung
- JS. Kang
- BR. Ko
- JW. Kwak
- KB. Lee
- SS. Myung
- H. Park
- G. Alimonti
- M. Boschini
- D. Brambilla
- B. Caccianiga
- A. Calandrino
- P. D'Angelo
- M. DiCorato
- P. Dini
- M. Giammarchi
- P. Inzani
- F. Leveraro
- S. Malvezzi
- D. Menasce
- M. Mezzadri
- L. Milazzo
- L. Moroni
- D. Pedrini
- F. Prelz
- M. Rovere
- A. Sala
- S. Sala
- TF. Davenport
- V. Arena
- G. Boca
- G. Bonomi
- G. Gianini
- G. Liguori
- M. Merlo
- D. Pantea
- SP. Ratti
- C. Riccardi
- P. Torre
- L. Viola
- P. Vitulo
- H. Hernandez
- AM. Lopez
- L. Mendez
- A. Mirles
- E. Montiel
- D. Olaya
- J. Quinones
- C. Rivera
- Y. Zhang
- N. Copty
- M. Purohit
- JR. Wilson
- K. Cho
- T. Handler
- D. Engh
- WE. Johns
- M. Hosack
- MS. Nehring
- M. Sales
- PD. Sheldon
- K. Stenson
- MS. Webster
- M. Sheaff
- YJ. Kwon
- Publication venue
- Publication date
- 01/01/2000
- Field of study
A high statistics sample of photoproduced charm particles from the FOCUS
(E831) experiment at Fermilab has been used to search for CP violation in the
Cabibbo suppressed decay modes D+ to K-K+pi+, D0 to K-K+ and D0 to pi-pi+. We
have measured the following CP asymmetry parameters: A_CP(K-K+pi+) = +0.006 +/-
0.011 +/- 0.005, A_CP(K-K+) = -0.001 +/- 0.022 +/- 0.015 and A_CP(pi-pi+) =
+0.048 +/- 0.039 +/- 0.025 where the first error is statistical and the second
error is systematic. These asymmetries are consistent with zero with smaller
errors than previous measurements.Comment: 12 pages, 4 figure
A Study of D0 --> K0(S) K0(S) X Decay Channels
- Author
- A. Cerutti
- A. Kryemadhi
- A. Massafferri
- A. Paris
- A. Rahimi
- A. Sanchez-Hernandez
- A. Zallo
- AA. Machado
- AC. dos Reis
- AE. Kreymer
- AM. Lopez
- B. O'Reilly
- BR. Ko
- C. Castromonte
- C. Cawlfield
- C. Gobel
- C. Pontoglio
- C. Riccardi
- C. Uribe
- D. Engh
- D. Menasce
- D. Pantea
- D. Pedrini
- DL. Pegna
- DY. Kim
- E. Casimiro
- E. Cuautle
- E. Gottschalk
- E. Luiggi
- E. Polycarpo
- EW. Vaandering
- F. Leveraro
- F. Prelz
- F. Vazquez
- FL. Fabbri
- G. Alimonti
- G. Boca
- G. Bonomi
- G. Chiodini
- G. Gianini
- G. Liguori
- H. Hernandez
- H. Mendez
- H. Park
- HWK. Cheung
- I. Bediaga
- I. Gaines
- I. Segoni
- IM. Pepe
- J. Magnin
- J. Otalora
- J. Quinones
- J. Wiss
- JC. Anjos
- JE. Ramirez
- JM. de Miranda
- JM. Link
- JN. Butler
- JP. Cumalat
- JR. Wilson
- JS. Kang
- JW. Kwak
- K. Cho
- K. Stenson
- KB. Lee
- L. Agostino
- L. Benussi
- L. Cinquini
- L. Edera
- L. Moroni
- LA. Garren
- M. Boschini
- M. DiCorato
- M. Hosack
- M. Mezzadri
- M. Nehring
- M. Reyes
- M. Rovere
- M. Sheaff
- M. Wang
- M. Webster
- MM. Merlo
- P. D'Angelo
- P. Dini
- P. Inzani
- P. Vitulo
- PD. Sheldon
- PH. Garbincius
- PH. Kasper
- PM. Yager
- R. Gardner
- R. Kutschke
- R. Mitchell
- S. Barberis
- S. Bianco
- S. Carrillo
- S. Erba
- S. Malvezzi
- S. Sala
- SP. Ratti
- T. Handler
- TF. Davenport
- V. Arena
- V. Frisullo
- WE. Johns
- Y. Zhang
- YS. Chung
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2005
- Field of study
Using data from the FOCUS experiment (FNAL-E831), we report on the decay of
D0 mesons into final states containing more than one KS0. We present
evidence for two Cabibbo favored decay modes, D0→KS0KS0K−π+ and
D0→KS0KS0K+π−, and measure their combined branching fraction
relative to D0→Kˉ0π+π− to be Γ(D0→Kˉ0π+π−)Γ(D0→KS0KS0K±π∓) = 0.0106
± 0.0019 ± 0.0010. Further, we report new measurements of
Γ(D0→Kˉ0π+π−)Γ(D0→KS0KS0KS0) =
0.0179 ± 0.0027 ± 0.0026, Γ(D0→Kˉ0π+π−)Γ(D0→K0Kˉ0) = 0.0144 ± 0.0032 ± 0.0016,
and Γ(D0→Kˉ0π+π−)Γ(D0→KS0KS0π+π−) = 0.0208 ± 0.0035 ± 0.0021 where the first error is
statistical and the second is systematic.Comment: 11 pages, 3 figures, typos correcte
Evidence for 6{\Lambda}H
- Author
- Agnello M.
- Benussi L.
- Bertani M.
- Bhang HC.
- Bonomi G.
- Botta E.
- Bregant M.
- Bressani T.
- Bufalino S.
- Busso L.
- Calvo D.
- Camerini P.
- D'Erasmo G.
- Dalena B.
- De Mori F.
- Fabbri FL.
- Feliciello A.
- Filippi A.
- Fiore EM.
- Fontana A.
- Fujioka H.
- Gal A.
- Genova P.
- Gianotti P .
- Grion N.
- Lucherini V.
- Marcello S.
- Mirfakhrai N.
- Moia F.
- Montagna R.
- Morra O.
- Nagae T.
- Outa H.
- Pantaleo A.
- Paticchio V.
- Piano S.
- Rui R.
- Simonetti G.
- Wheadon R.
- Zenoni A.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 19/12/2011
- Field of study
Evidence for the neutron-rich hypernucleus 6{\Lambda}H is presented from the
FINUDA experiment at DA{\Phi}NE, Frascati, studying ({\pi}+, {\pi}-) pairs in
coincidence from the K- +6Li \rightarrow 6 H+{\pi}+ production reaction
followed by 6{\Lambda}H \rightarrow 6He + {\pi}- weak decay. The production
rate of 6{\Lambda}H undergoing this two-body {\pi}- decay is determined to be
(2.9\pm2.0)\cdot10-6/K-. Its binding energy, evaluated jointly from production
and decay, is B{\Lambda}(6{\Lambda}H) = (4.0\pm1.1) MeV with respect to
5H+{\Lambda}. A systematic difference of (0.98 \pm 0.74) MeV between B{\Lambda}
values derived separately from decay and from production is tentatively
assigned to the 6{\Lambda}H 0+g.s. \rightarrow 1+ excitation.Comment: 5 pages, 3 figure
Metabolic syndrome and carotid intima-media thickness in chronic obstructive pulmonary disease
- Author
- A Bourdin
- A Onat
- AG Agusti
- American Thoracic Society
- C Landbo
- DD Sin
- DD Sin
- DD Sin
- DJ Hole
- DM Mannino
- EB Schroeder
- ES Ford
- ES Ford
- FL Fimognari
- G Engström
- G Invernizzi
- H Iwamoto
- H Watz
- HJ Schñnemann
- JD Maclay
- JM Dekker
- JT Salonen
- K Marquis
- KB Lam
- KG Alberti
- KL Ebi-Kryston
- LM Fabbri
- M Torzewski
- M Zureik
- M Zureik
- MA Cornier
- O Kozan
- P Pignoli
- P Poirier
- R Broekhuizen
- RG Barr
- S Ebrahim
- T Ogata
- TG Lohman
- TG Pickering
- YH Lee
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2013
- Field of study
BACKGROUND: The aim of this study is to investigate the prevalence of metabolic syndrome (MetS), carotid intima media thickness (IMT), and serum C-reactive protein (CRP) levels in patients with chronic obstructive pulmonary disease (COPD), and the possible relationships among them. METHODS: Fifty stable COPD patients and 40 healthy controls were included in the study. The participants were further divided into four groups according to their smoking status. Pulmonary function tests were performed in COPD patients. Anthropometric measurements and blood chemistry analysis, serum CRP levels and carotid intima-media thickness (IMT) measurements were performed in all the study population. RESULTS: Prevalence of metabolic syndrome was 43% in COPD patients and 30% in the control group (p = 0.173). FEV(1)% and FEV(1)/FVC were higher in COPD patients with MetS (p = 0.001 and p = 0.014, respectively) compared to those without MetS. Prevalence of MetS was significantly different among the COPD patients with different stages (p = 0.017) with the highest value in stage 2 (59%). Carotid IMT was significantly higher in COPD patients than in control group (1.07 ± 0.25 mm and 0.86 ± 0.18 mm, respectively; p < 0.001). Serum CRP levels were not different in COPD patients and controls, however they were higher in individuals with MetS compared to those without MetS regardless of COPD presence (p = 0.02). CONCLUSIONS: Early markers of atherogenesis, in terms of carotid IMT, were found to be higher in COPD patients than in healthy controls. MetS prevalence was observed to decrease as the severity of airflow obstruction increased. Therefore, screening COPD patients for these cardiovascular risk factors would be a novel approach even in absence of symptoms
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
- Erofeeva M
- 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
- Fabjan C
- 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
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yoo J
- Yoon AS
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- Yumiceva F
- Yun JC
- Zabel J
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- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- 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
Search for the standard model Higgs boson at LEP
- Author
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- Abbaneo D
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- Abdallah J
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- Zobernig G
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- Zupan M
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
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
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yoo J
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- Yumiceva F
- Yun JC
- Zabel J
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- Zanetti M
- Zang J
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- 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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
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- Abbiendi G
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- Czellar S
- D'Agnolo RT
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- Yagil A
- Yan M
- Yang F
- Yang M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- 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
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- 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
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- Alcaraz Maestre J
- Alda Junior WL
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- Aliev T
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- Alves GA
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- Amsler C
- Anagnostou G
- Anastassov A
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- Andreev V
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- Andreev Y
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- CMS Collaboration
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- Villella I
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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
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
- 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
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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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