596 research outputs found
Efficacy of an intensive outpatient rehabilitation program in alcoholism: Predictors of outcome 6 months after treatment
- Author
- Publication venue
- 'S. Karger AG'
- Publication date
- 01/01/2005
- Field of study
Treatment of alcohol-dependent patients was primarily focused on inpatient settings in the past decades. The efficacy of these treatment programs has been evaluated in several studies and proven to be sufficient. However, with regard to the increasing costs in public healthcare systems, questions about alternative treatment strategies have been raised. Meanwhile, there is growing evidence that outpatient treatment might be comparably effective as inpatient treatment, at least for subgroups of alcohol dependents. On that background, the present study aimed to evaluate the efficacy of a high-structured outpatient treatment program in 103 alcohol-dependent patients. 74 patients (72%) terminated the outpatient treatment regularly. At 6 months' follow-up, 95% patients were successfully located and personally re-interviewed. Analyses revealed that 65 patients (64%) were abstinent at the 6-month follow-up evaluation and 37 patients ( 36%) were judged to be non-abstinent. Pretreatment variables which were found to have a negative impact (non-abstinence) on the 6-month outcome after treatment were a higher severity of alcohol dependence measured by a longer duration of alcohol dependence, a higher number of prior treatments and a stronger alcohol craving (measured by the Obsessive Compulsive Drinking Scale). Further patients with a higher degree of psychopathology measured by the Beck Depression Inventory (depression) and State-Trait Anxiety Inventory (anxiety) relapsed more often. In summary, results of this study indicate a favorable outcome of socially stable alcohol-dependent patients and patients with a lower degree of depression, anxiety and craving in an intensive outpatient rehabilitation program
An Intact Kidney Slice Model to Investigate Vasa Recta Properties and Function in situ
- Author
- Agmon Y
- Armulik A
- Bogle RG
- Bratosin D
- C. Crawford
- C. Sprott
- C.M. Peppiatt-Wildman
- Crawford C
- Cupples WA
- Dahlstrom A
- Dietrich HH
- Dunn KW
- Hall AM
- Hamilton NB
- Holliger C
- Horiuchi T
- Hughes S
- J. Munday
- Jans D
- Kawamura H
- L. Sawbridge
- Landis EM
- MacPhee PJ
- Mattson DL
- Mattson DL
- O’Connor PM
- Pallone TL
- Pallone TL
- Pallone TL
- Pallone TL
- Pallone TL
- Park F
- Patzak A
- Peppiatt CM
- Praetorius HA
- R.J. Unwin
- Rhinehart K
- Rhinehart KL
- Roman RJ
- S.S.P. Wildman
- Shepro D
- Silldorff EP
- Silldorff EP
- Silldorff EP
- Sprague RS
- T. Desai
- T. Kennedy-Lydon
- Thiel G
- Whitehouse T
- Wu DM
- Zhang Z
- Zhang Z
- Publication venue
- 'S. Karger AG'
- Publication date
- 20/07/2012
- Field of study
Background: Medullary blood flow is via vasa recta capillaries, which possess contractile pericytes. In vitro studies using isolated descending vasa recta show that pericytes can constrict/dilate descending vasa recta when vasoactive substances are present. We describe a live kidney slice model in which pericyte-mediated vasa recta constriction/dilation can be visualized in situ. Methods: Confocal microscopy was used to image calcein, propidium iodide and Hoechst labelling in ‘live’ kidney slices, to determine tubular and vascular cell viability and morphology. DIC video-imaging of live kidney slices was employed to investigate pericyte-mediated real-time changes in vasa recta diameter. Results: Pericytes were identified on vasa recta and their morphology and density were characterized in the medulla. Pericyte-mediated changes in vasa recta diameter (10–30%) were evoked in response to bath application of vasoactive agents (norepinephrine, endothelin-1, angiotensin-II and prostaglandin E2) or by manipulating endogenous vasoactive signalling pathways (using tyramine, L-NAME, a cyclo-oxygenase (COX-1) inhibitor indomethacin, and ATP release). Conclusions: The live kidney slice model is a valid complementary technique for investigating vasa recta function in situ and the role of pericytes as regulators of vasa recta diameter. This technique may also be useful in exploring the role of tubulovascular crosstalk in regulation of medullary blood flow
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adolphi R
- Adzic P
- Afaq MA
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed W
- Ahuja S
- Aisa D
- Aisa S
- Akchurin N
- Akgun B
- Akgun U
- Akimenko S
- Akin IV
- Alagoz E
- Alampi G
- Albajar C
- Albayrak EA
- Alberdi J
- Albergo S
- Albert E
- Albrow M
- Alexander J
- Alidra M
- Aliev T
- Allfrey P
- Almeida N
- Altenhofer G
- Altsybeev I
- Alver B
- Alverson G
- Alves GA
- Amaglobeli N
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Ananthan B
- Anastassov A
- Andelin D
- Anderson M
- Andrea J
- Andreev V
- Andreev Y
- Anghel IM
- Anguelov T
- Anh T. Vu
- Anisimov A
- Antillon E
- Antipov P
- Antonelli L
- Anttila E
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arnold B
- Arora S
- Artamonov A
- Asaadi J
- Asghar MI
- Ashby S
- Askew A
- Atac M
- Atramentov O
- Auffray E
- Aurisano A
- Autermann C
- Avery P
- Avetisyan A
- Avila C
- Awan MIM
- Ayan AS
- Ayhan A
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babb J
- Babucci E
- Baccaro S
- Bacchetta N
- Bacchi W
- Bachtis M
- Baden D
- Badgett W
- Baechler J
- Baer H
- Baesso P
- Baffioni S
- Bagby L
- Bagliesi G
- Bahk SY
- Bailleux D
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Baldin B
- Ball G
- Ball H
- Ballin J
- Bally SL
- Ban Y
- Bandurin D
- Banerjee S
- Banerjee S
- Banicz K
- Bansal S
- Banzuzi K
- Barashko V
- Barbagli G
- Barberis E
- Barbone L
- Barcala JM
- Barcellan L
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- Baringer P
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Bartalini P
- Bartoloni A
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- Basegmez S
- Battilana C
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- Baud A
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- Bauerdick LAT
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- Bean A
- Beauceron S
- Beaudette F
- Beaumont W
- Bechtel F
- Bedjidian M
- Bedoya CF
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- Bejar JC
- Belforte S
- Beliy N
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Benaglia A
- Bencze G
- Bendavid J
- Bender W
- Benedetti D
- Benelli G
- Benettoni M
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- Benvenuti AC
- Berengueres JOL
- Beretvas A
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- Bitioukov S
- Blaha J
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- Blumenfeld B
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- Bocci A
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- Bodek A
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- Bornheim A
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- Borsato E
- Bortoletto D
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- Botta C
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- Bouhali O
- Bourgeois N
- Bourilkov D
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- Boutemeur M
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- Braibant-Giacomelli S
- Branca A
- Branson JG
- Brauer R
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- Breedon R
- Brett AM
- Breuker H
- Brew C
- Bricola S
- Briggs R
- Brigljevic V
- Broccolo G
- Brom JM
- Brooke JJ
- Brown RM
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- Buchmuller O
- Budd H
- Buege V
- Buehler M
- Bunin P
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- Bylsma B
- Caballero IG
- Cabrillo IJ
- Cafaro VD
- Cai J
- Caiazza SS
- Cakir A
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- Cattai A
- Caudron J
- Cavallari F
- Cavallo FR
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- Ceballos GG
- Cebra D
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- Cerati GB
- Cerci S
- Cerizza G
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- Chabert EC
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- Chandra A
- Chang P
- Chang S
- Chang YH
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chatelain JP
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Chauvey M
- Checchia P
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- Cheung HWK
- Chien CY
- Chierici R
- Chiochia V
- Chiorboli M
- Chipaux R
- Chiumarulo F
- Chlebana F
- Choi M
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- Chou JP
- Choudhary BC
- Choudhury RK
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- Christiansen T
- Chtchipounov L
- Chuang SH
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- Cihangir S
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- Ciulli V
- Civinini C
- Claes DR
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- Clemente A
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- Clerbaux B
- Cline D
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
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- Colling D
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- Contardo D
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- Cooper SI
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- Cortabitarte RV
- Cossutti F
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- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Crawford M
- Creanza D
- Cremaldi LM
- Cripps N
- Crotty I
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cuscela G
- Cushman P
- Cussans D
- Cutts D
- Cwiok M
- Czellar S
- D'Alessandro R
- D'Alfonso M
- D'Angelo P
- D'Antone I
- D'Enterria D
- D'Hondt J
- Dabrowski R
- Dafinei I
- Dagenhart W
- Dahmes B
- Dal Corso F
- Dallavalle GM
- Dambach S
- Damgov J
- Damiao DD
- Dammann D
- Daniel M
- Danielson T
- Darmenov N
- Das S
- Daskalakis G
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- Dattola D
- Daubie E
- David A
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- de Abril IM
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- De Benedetti A
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- de Cassagnac RG
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De La Cruz B
- De Lentdecker G
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- de Monchenault GH
- De Palma M
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- De Roeck A
- De Souza SF
- de Troconiz JF
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- De Wolf EA
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- Debreczeni G
- Deiters K
- Dejardin M
- Del Alamo MB
- del Arbol PMR
- Del Re D
- Delachenal V
- Delaere C
- Deliomeroglu M
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- Della Ricca G
- Dellacasa G
- Delmeire E
- Demaria N
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- Dimitrov A
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- 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
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- 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
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Publication date
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- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
Bioenergetic Consequences of PINK1 Mutations in Parkinson Disease
- Author
- A Grunewald
- A Rakovic
- AC Poole
- AH Schapira
- AH Schapira
- AJ Whitworth
- Andrey Yurevich Abramov
- Anne Grunewald
- Anthony Henry Vernon Schapira
- C Piccoli
- C Scheele
- C Vives-Bauza
- CA Gautier
- Christine Klein
- DP Narendra
- E Ziviani
- EK Tan
- EM Valente
- EM Valente
- HH Hoepken
- IE Clark
- JV Leonard
- K Hedrich
- M Campanella
- Mark P. Mattson
- Matthew Gegg
- ME Gegg
- ME Gegg
- MP Mattson
- N Exner
- Nicholas William Wood
- RK Dagda
- S Gandhi
- S Gispert
- VA Morais
- Y Yang
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
BACKGROUND: Mutations of the gene for PTEN-induced kinase 1 (PINK1) are a cause of familial Parkinson's disease (PD). PINK1 protein has been localised to mitochondria and PINK1 gene knockout models exhibit abnormal mitochondrial function. The purpose of this study was to determine whether cells derived from PD patients with a range of PINK1 mutations demonstrate similar defects of mitochondrial function, whether the nature and severity of the abnormalities vary between mutations and correlate with clinical features. METHODOLOGY: We investigated mitochondrial bioenergetics in live fibroblasts from PINK1 mutation patients using single cell techniques. We found that fibroblasts from PINK1 mutation patients had significant defects of bioenergetics including reduced mitochondrial membrane potential, altered redox state, a respiratory deficiency that was determined by substrate availability, and enhanced sensitivity to calcium stimulation and associated mitochondrial permeability pore opening. There was an increase in the basal rate of free radical production in the mutant cells. The pattern and severity of abnormality varied between different mutations, and the less severe defects in these cells were associated with later age of onset of PD. CONCLUSIONS: The results provide insight into the molecular pathology of PINK1 mutations in PD and also confirm the critical role of substrate availability in determining the biochemical phenotype--thereby offering the potential for novel therapeutic strategies to circumvent these abnormalities
Combined Tevatron upper limit on gg->H->W+W- and constraints on the Higgs boson mass in fourth-generation fermion models
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- Zucchelli SSevior M. E.
- Publication venue
- Publication date
- 01/01/2010
- Field of study
Report number: FERMILAB-PUB-10-125-EWe combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg->H->W+W- in p=pbar collisions at the Fermilab Tevatron Collider at sqrt{s}=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% Confidence Level upper limit on \sigma(gg->H) x B(H->W+W-) is 1.75 pb at m_H=120 GeV, 0.38 pb at m_H=165 GeV, and 0.83 pb at m_H=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% Confidence Level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.We combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg→H→W+W- in pp̅ collisions at the Fermilab Tevatron Collider at √s=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% confidence level upper limit on σ(gg→H)×B(H→W+W-) is 1.75 pb at mH=120 GeV, 0.38 pb at mH=165 GeV, and 0.83 pb at mH=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% confidence level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.Peer reviewe
Identification and Filtering of Uncharacteristic Noise in the CMS Hadron Calorimeter
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- Abbaneo D
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- Publication venue
- INSTITUTE OF PHYSICS PUBLISHING
- Publication date
- 01/01/1
- Field of study
VertaisarvioitupeerReviewe
Performance of CMS hadron calorimeter timing and synchronization using test beam, cosmic ray, and LHC beam data
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
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- Sibille J
- Sidiropoulos G
- Siegrist N
- Siegrist P
- Sierra RV
- Signal T
- Sikler F
- Sill A
- Sillou D
- Silva Do Amaral SM
- Silva J
- Silva P
- Silvestris L
- Sim KS
- Simon S
- Simonetto F
- Simonis HJ
- Sinanis N
- Singh A
- Singh JB
- Singh SP
- Singovsky A
- Sirois Y
- Siroli G
- Sirunyan AM
- Sknar V
- Skuja A
- Skup E
- Slabospitsky S
- Slaunwhite J
- Smiljkovic N
- Smirnov I
- Smirnov V
- Smith J
- Smith K
- Smith RP
- Smith VJ
- Smith WH
- Smolin D
- Smoron A
- Snigirev A
- Snow GR
- Soares D
- Sobol A
- Sobrier T
- Sobron Sanudo M
- Sogut K
- Soha A
- Solano A
- Solin A
- Solovey A
- Solovey A
- Somalwar S
- Son DC
- Song S
- Sonmez N
- Sonnek P
- Sonnenschein L
- Sordini V
- Soroka D
- Sourkov A
- Sousa M
- Souza MHG
- Sowa M
- Spagnolo P
- Spalding WJ
- Spanier S
- Speck J
- Speer T
- Sphicas P
- Spiegel L
- Spiga D
- Spiropulu M
- Sprenger D
- Squires M
- Srivastava AK
- St John J
- Stadie H
- Stahl A
- Staiano A
- Stark R
- Starodumov A
- Stefanovitch R
- Steggemann J
- Steinbrueck G
- Steininger H
- Stenson K
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- Stoykova S
- Stoynev S
- Strang M
- Strauss J
- Stringer R
- Stroiney S
- Stuart D
- Sturdy J
- Sturm P
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
- Sumorok K
- Sun W
- Sung K
- Surat UE
- Suzuki I
- Svintradze I
- Swain J
- Swanson J
- Swartz M
- Sytine A
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- Szabo Z
- Szczesny H
- Szekely G
- Szillasi Z
- Szleper M
- Sznajder A
- Takahashi M
- Tali B
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- Tancini V
- Tanenbaum W
- Tao J
- Tapper A
- Tarakanov V
- Taroni S
- Taurok A
- Tauscher L
- Tavernier S
- Taylor L
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- Teischinger F
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- Tenchini R
- Teng H
- Teo WD
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- Teyssier D
- Thea A
- Themel T
- Theofilatos K
- Thiebaux C
- Thom J
- Thomas M
- Thomas S
- Thomsen J
- Thyssen F
- Tikhonenko E
- Tikhonov A
- Timciuc V
- Timlin C
- Titov M
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- Tomalin IR
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- Toniolo N
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- Tonoiu D
- Tonwar SC
- Toole T
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- Topaksu AK
- Topkar A
- Torassa E
- Tornier D
- Toropin A
- Torre P
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- Toteva Z
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- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
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- Trayanov R
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- Uplegger L
- Uvarov L
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- Vaandering EW
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- Yelton J
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- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
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- Yumiceva F
- Yun JC
- Yuste C
- Zabi A
- Zabolotny W
- Zachariadou A
- Zalewski P
- Zampieri A
- Zanetti M
- Zang SL
- Zarubin A
- Zatzerklyany A
- Zeidler C
- Zeinali M
- Zeise M
- Zelepoukine S
- Zeuner WD
- Zeyrek M
- Zhang J
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- Zheng Y
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- Zhukov V
- Zhukova V
- Ziebarth EB
- Zielinski M
- Zilizi G
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- Zoeller MH
- Zotto P
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- Zumerle G
- Zuranski A
- Zuyeuski R
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- Publication venue
- Institute of Physics Publishing
- Publication date
- 01/01/1
- Field of study
This paper discusses the design and performance of the time measurement technique and of the synchronization systems of the CMS hadron calorimeter. Time measurement performance results are presented from test beam data taken in the years 2004 and 2006. For hadronic showers of energy greater than 100 GeV, the timing resolution is measured to be about 1.2 ns. Time synchronization and out-of-time background rejection results are presented from the Cosmic Run At Four Tesla and LHC beam runs taken in the Autumn of 2008. The inter-channel synchronization is measured to be within ±2 ns
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