1,899 research outputs found
Power grip, pinch grip, manual muscle testing or thenar atrophy - which should be assessed as a motor outcome after carpal tunnel decompression? A systematic review
- Author
- AA Gerritsen
- C Dumontier
- C Jerosch-Herold
- C Shum
- CF Leinberry
- Christina Jerosch-Herold
- CS Simpson
- D Moher
- DG Altman
- DJ Mackenzie
- DW Levine
- GD Foulkes
- GR Sennwald
- I Atroshi
- JC MacDermid
- JC MacDermid
- JJ Dias
- JM Agee
- Jo Geere
- JW Brandsma
- K Nakamichi
- KA Kuhlman
- KC Wong
- L Gilbertson
- L Vanderweeën
- LA J. Kazis
- LG Portney
- MC de Krom
- MW Erdmann
- N Borisch
- ND Citron
- NL Saw
- P Brüser
- R Bhattacharya
- RA Brown
- Rachel Chester
- RD Ferdinand
- RH Helm
- RW Bohannon
- S Standring
- S Sunderland
- SE Mackinnon
- Swati Kale
- TA Schreuders
- TA Schreuders
- TA Schreuders
- TE Trumble
- V Mathiowetz
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2007
- Field of study
<p>Abstract</p> <p>Background</p> <p>Objective assessment of motor function is frequently used to evaluate outcome after surgical treatment of carpal tunnel syndrome (CTS). However a range of outcome measures are used and there appears to be no consensus on which measure of motor function effectively captures change. The purpose of this systematic review was to identify the methods used to assess motor function in randomized controlled trials of surgical interventions for CTS. A secondary aim was to evaluate which instruments reflect clinical change and are psychometrically robust.</p> <p>Methods</p> <p>The bibliographic databases Medline, AMED and CINAHL were searched for randomized controlled trials of surgical interventions for CTS. Data on instruments used, methods of assessment and results of tests of motor function was extracted by two independent reviewers.</p> <p>Results</p> <p>Twenty-two studies were retrieved which included performance based assessments of motor function. Nineteen studies assessed power grip dynamometry, fourteen studies used both power and pinch grip dynamometry, eight used manual muscle testing and five assessed the presence or absence of thenar atrophy. Several studies used multiple tests of motor function. Two studies included both power and pinch strength and reported descriptive statistics enabling calculation of effect sizes to compare the relative responsiveness of grip and pinch strength within study samples. The study findings suggest that tip pinch is more responsive than lateral pinch or power grip up to 12 weeks following surgery for CTS.</p> <p>Conclusion</p> <p>Although used most frequently and known to be reliable, power and key pinch dynamometry are not the most valid or responsive tools for assessing motor outcome up to 12 weeks following surgery for CTS. Tip pinch dynamometry more specifically targets the thenar musculature and appears to be more responsive. Manual muscle testing, which in theory is most specific to the thenar musculature, may be more sensitive if assessed using a hand held dynamometer – the Rotterdam Intrinsic Handheld Myometer. However further research is needed to evaluate its reliability and responsiveness and establish the most efficient and psychometrically robust method of evaluating motor function following surgery for CTS.</p
Lambda and Antilambda polarization from deep inelastic muon scattering
- Author
- Adams MR
- Aderholz M
- Aid S
- Anthony PL
- Ashery D
- Averill DA
- Baker MD
- Baller BR
- Banerjee A
- Bhatti AA
- Bratzler U
- Braun HM
- Carroll TJ
- Clark HL
- Conrad JM
- Davisson R
- Derado I
- Dietrich FS
- Dougherty W
- Dreyer T
- Eckardt V
- Ecker U
- Erdmann M
- Fang GY
- Figiel J
- Finlay RW
- Gebauer HJ
- Geesaman DF
- Griffioen KA
- Guo RS
- Haas J
- Halliwell C
- Hantke D
- Hicks KH
- Jackson HE
- Jancso G
- Jansen DM
- Jin Z
- Kadija K
- Kaufmann S
- Kennedy RD
- Kinney ER
- Kobrak HGE
- Kotwal AV
- Kunori S
- Lenski M
- Lord JJ
- Lubatti HJ
- Madden P
- Manz A
- McLeod D
- Melanson H
- Michael DG
- Montgomery HE
- Morfin JG
- Nickerson RB
- Novak J
- Olkiewicz K
- Osborne L
- Otten R
- Papavassiliou V
- Pawlik B
- Pipkin FM
- Pop VT
- Potterveld DH
- Roser A
- Ryan JJ
- Salgado CW
- Schellman H
- Schmitt M
- Schmitz N
- Siegert G
- Skuja A
- Snow GA
- Soldner-Rembold S
- Spentzouris P
- Stopa P
- Swanson RA
- Venkataramania H
- Wilhelm M
- Wilson R
- Wittek W
- Wolbers SA
- Zghiche A
- Zhao T
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 18/11/1999
- Field of study
We report results of the first measurements of Lambda and Antilambda
polarization produced in deep inelastic polarized muon scattering on the
nucleon. The results are consistent with an expected trend towards positive
polarization with increasing x_F. The polarizations of Lambda and Antilambda
appear to have opposite signs. A large negative polarization for Lambda at low
positive x_F is observed and is not explained by existing models.A possible
interpretation is presented.Comment: 9 pages, 2 figure
Common Variants at 10 Genomic Loci Influence Hemoglobin A(1C) Levels via Glycemic and Nonglycemic Pathways
- Author
- Abecasis G
- Altshuler D
- Arking D
- Balkau B
- Barnes D
- Barroso I
- Boehnke M
- Boerwinkle E
- Bonnefond A
- Bonnycastle LL
- Boomsma DI
- Bornstein SR
- Bouatia-Naji N
- Bumpstead S
- Burnett-Miller MS
- Böhm B
- Böttcher Y
- Campbell H
- Cao A
- Chambers J
- Clark R
- Collins FS
- Coresh J
- de Geus EJ
- Dei M
- Deloukas P
- Devaney JM
- Dupuis J
- Döring A
- Egan JM
- Elosua R
- Epstein SE
- Erdmann J
- Ferrucci L
- Fleming MD
- Florez JC
- Forouhi N
- Fox CS
- Franklin C
- Franzosi MG
- Froguel P
- Gallina S
- Gieger C
- Goel A
- Graessler J
- Grallert H
- Greinacher A
- Groop L
- Hadley D
- Hakonarson HH
- Hall A
- Hamsten A
- Hayward C
- Heath S
- Heeney MM
- Herder C
- Homuth G
- Hottenga JJ
- Hunter-Merrill R
- Illig T
- Jackson AU
- Jula A
- Kao WH
- Kathiresan S
- Khaw KT
- Kleber M
- Knouff CW
- Kong A
- Kooner J
- Kovacs P
- Krohn K
- Kuusisto J
- Köttgen A
- Kühnel B
- Laakso M
- Langenberg C
- Lathrop M
- Lecoeur C
- Li M
- Li M
- Loos RJ
- Luan J
- Lyssenko V
- Magnusson PK
- Mangino M
- Martínez-Larrad MT
- McArdle WL
- McCarthy MI
- McPherson R
- Meigs JB
- Meisinger C
- Meitinger T
- Melander O
- Mohlke KL
- Mooser VE
- Morken MA
- Mägi R
- Mälarstig A
- März W
- Narisu N
- Nathan DM
- Nauck M
- O'Donnell C
- Oexle K
- Olla N
- Pankow JS
- Payne F
- Peden JF
- Pedersen NL
- Peltonen L
- Perola M
- Polasek O
- Porcu E
- Prokopenko I
- Rader DJ
- Radke D
- Rathmann W
- Reilly MP
- Ricketts SL
- Ripatti S
- Roberts R
- Rocheleau G
- Roden M
- Rudan I
- Salomaa V
- Samani NJ
- Sandhu MS
- Sanna S
- Saxena R
- Schlessinger D
- Schunkert H
- Schwarz P
- Seedorf U
- Selvin E
- Serrano-Ríos M
- Shrader P
- Silveira A
- Siscovick D
- Sladek R
- Song K
- Soranzo N
- Spector TD
- Stefansson K
- Steinthorsdottir V
- Stewart AF
- Stolerman E
- Strachan DP
- Strawbridge R
- Stumvoll M
- Surakka I
- Swift AJ
- Tanaka T
- Teumer A
- Thorleifsson G
- Thorsteinsdottir U
- Tönjes A
- Uda M
- Usala G
- Vitart V
- Voight BF
- Völzke H
- Wallaschofski H
- Wareham NJ
- Waterworth DM
- Watkins H
- Wheeler E
- Wichmann HE
- Wild SH
- Willemsen G
- Willenborg C
- Williams GH
- Wilson JF
- Winkelmann J
- Wright AF
- Wright B
- WTCCC
- Zabena C
- Zhao JH
- Publication venue
- AMER DIABETES ASSOC
- Publication date
- 01/01/2010
- Field of study
OBJECTIVE Glycated hemoglobin (HbA1c), used to monitor and diagnose diabetes, is influenced by average glycemia over a 2- to 3-month period. Genetic factors affecting expression, turnover, and abnormal glycation of hemoglobin could also be associated with increased levels of HbA1c. We aimed to identify such genetic factors and investigate the extent to which they influence diabetes classification based on HbA1c levels.
RESEARCH DESIGN AND METHODS We studied associations with HbA1c in up to 46,368 nondiabetic adults of European descent from 23 genome-wide association studies (GWAS) and 8 cohorts with de novo genotyped single nucleotide polymorphisms (SNPs). We combined studies using inverse-variance meta-analysis and tested mediation by glycemia using conditional analyses. We estimated the global effect of HbA1c loci using a multilocus risk score, and used net reclassification to estimate genetic effects on diabetes screening.
RESULTS Ten loci reached genome-wide significant association with HbA1c, including six new loci near FN3K (lead SNP/P value, rs1046896/P = 1.6 × 10−26), HFE (rs1800562/P = 2.6 × 10−20), TMPRSS6 (rs855791/P = 2.7 × 10−14), ANK1 (rs4737009/P = 6.1 × 10−12), SPTA1 (rs2779116/P = 2.8 × 10−9) and ATP11A/TUBGCP3 (rs7998202/P = 5.2 × 10−9), and four known HbA1c loci: HK1 (rs16926246/P = 3.1 × 10−54), MTNR1B (rs1387153/P = 4.0 × 10−11), GCK (rs1799884/P = 1.5 × 10−20) and G6PC2/ABCB11 (rs552976/P = 8.2 × 10−18). We show that associations with HbA1c are partly a function of hyperglycemia associated with 3 of the 10 loci (GCK, G6PC2 and MTNR1B). The seven nonglycemic loci accounted for a 0.19 (% HbA1c) difference between the extreme 10% tails of the risk score, and would reclassify ∼2% of a general white population screened for diabetes with HbA1c.
CONCLUSIONS GWAS identified 10 genetic loci reproducibly associated with HbA1c. Six are novel and seven map to loci where rarer variants cause hereditary anemias and iron storage disorders. Common variants at these loci likely influence HbA1c levels via erythrocyte biology, and confer a small but detectable reclassification of diabetes diagnosis by HbA1c
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
- 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
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- 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
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
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- Blumenschein U
- Bobbink GJ
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- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
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- Booth CD
- Borecka-Bielska HM
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- Burgard CD
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- Bussey PJ
- Butler JM
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- Butterworth JM
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- Buzatu A
- Buzykaev AR
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- de Jong P
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- de Lima DEF
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- De Maria A
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- De Regie JBDV
- de Renstrom PAB
- De Sa RCL
- De Salvo A
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- De Santis M
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- De Sousa MJDCS
- De K
- Debenedetti C
- Dedovich D
- Deiana AM
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- 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
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- Dimitrievska A
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- Djama F
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- Djuvsland J
- Do Vale TD
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- Doglioni C
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- Dolezal Z
- Dominguez LP
- Don MMR
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- Dong B
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- Donszelmann TC
- Dopke J
- Doria A
- Dova MT
- Doyle AT
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- Dreyer E
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- Drobac AS
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- Dubreuil A
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zwalinski L
- 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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
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- Abdullin S
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- Yilmaz Y
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- Zanetti M
- Zang J
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- Zeyrek M
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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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- Acosta MV
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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
Transverse electric field dragging of DNA in a nanochannel
- Author
- Publication venue
- Nature Publishing Group
- Publication date
- Field of study
Nanopore analysis is an emerging single-molecule strategy for non-optical and high-throughput DNA sequencing, the principle of which is based on identification of each constituent nucleobase by measuring trans-membrane ionic current blockade or transverse tunnelling current as it moves through the pore. A crucial issue for nanopore sequencing is the fact that DNA translocates a nanopore too fast for addressing sequence with a single base resolution. Here we report that a transverse electric field can be used to slow down the translocation. We find 400-fold decrease in the DNA translocation speed by adding a transverse field of 10 mV/nm in a gold-electrode-embedded silicon dioxide channel. The retarded flow allowed us to map the local folding pattern in individual DNA from trans-pore ionic current profiles. This field dragging approach may provide a new way to control the polynucleotide translocation kinetics
X-ray emission from the Sombrero galaxy: discrete sources
- Author
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- 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
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- Adiguzel A
- Adler V
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- Afanasiev S
- Agostino L
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- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
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- Yilmaz Y
- Yohay R
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- Zumerle G
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- 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
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
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- Zhemchugov A
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- 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 √s = 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 pT≥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 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{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
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