429 research outputs found
Interactive Rhythmic Auditory Stimulation Reinstates Natural 1/f Timing in Gait of Parkinson's Patients
- Author
- A Graybiel
- A Nieuwboer
- AL Goldberger
- BH Repp
- BH Repp
- BH Repp
- C-K Peng
- CT Buhusi
- CT Kello
- D Delignieres
- DJ O'Boyle
- DL Gilden
- EAF Ihlen
- EW Large
- GC McIntosh
- Hirotaka Uchitomi
- I Lim
- JA Grahn
- JA Grahn
- JAS Kelso
- JM Hausdorff
- JM Hausdorff
- JM Hausdorff
- JM Hausdorff
- K Jordan
- K Torre
- Kazuki Suzuki
- M Schwartze
- ME Morris
- MEJ Newman
- MH Thaut
- MH Thaut
- Michael J. Hove
- MR Pierrynowski
- N Scafetta
- NI Fisher
- P Arias
- P Bak
- P Brotchie
- R Bartsch
- R Cunnington
- RC Schmidt
- SA Kotz
- Satoshi Orimo
- SK Rankin
- T Herman
- T Muto
- TC Rubinstein
- Wing-ho Yung
- Y Chen
- Y Miyake
- Y Miyake
- Y Miyake
- Y Miyake
- Yoshihiro Miyake
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Parkinson's disease (PD) and basal ganglia dysfunction impair movement timing, which leads to gait instability and falls. Parkinsonian gait consists of random, disconnected stride timesβrather than the 1/f structure observed in healthy gaitβand this randomness of stride times (low fractal scaling) predicts falling. Walking with fixed-tempo Rhythmic Auditory Stimulation (RAS) can improve many aspects of gait timing; however, it lowers fractal scaling (away from healthy 1/f structure) and requires attention. Here we show that interactive rhythmic auditory stimulation reestablishes healthy gait dynamics in PD patients. In the experiment, PD patients and healthy participants walked with a) no auditory stimulation, b) fixed-tempo RAS, and c) interactive rhythmic auditory stimulation. The interactive system used foot sensors and nonlinear oscillators to track and mutually entrain with the human's step timing. Patients consistently synchronized with the interactive system, their fractal scaling returned to levels of healthy participants, and their gait felt more stable to them. Patients and healthy participants rarely synchronized with fixed-tempo RAS, and when they did synchronize their fractal scaling declined from healthy 1/f levels. Five minutes after removing the interactive rhythmic stimulation, the PD patients' gait retained high fractal scaling, suggesting that the interaction stabilized the internal rhythm generating system and reintegrated timing networks. The experiment demonstrates that complex interaction is important in the (re)emergence of 1/f structure in human behavior and that interactive rhythmic auditory stimulation is a promising therapeutic tool for improving gait of PD patients
At-risk elementary school children with one year of classroom music instruction are better at keeping a beat
- Author
- A Tierney
- Adam Tierney
- AT Tierney
- B Repp
- BH Repp
- BH Repp
- BH Repp
- C Drake
- C Drake
- C Woerner
- D Levitin
- DL Strait
- E Large
- E Skoe
- EE Hannon
- EE Hannon
- EE Hannon
- EW Large
- G Aschersleben
- G Buzsaki
- G Dellatolas
- G Schlaug
- H Ben-Pazi
- H Ben-Pazi
- J Gromko
- J Hornickel
- J Phillips-Silver
- J Phillips-Silver
- J Reifinger
- J Standley
- JA Grahn
- JA HΓ€mΓ€lΓ€inen
- JD McAuley
- Jessica Slater
- JM Thomson
- Joel Snyder
- K Bugaj
- K Drewing
- K Grieshaber
- KH Corriveau
- L Gooding
- LJ Trainor
- M Huss
- M Schwartze
- N Kraus
- Nina Kraus
- P Janata
- P Tallal
- R Dauer
- RJ Ellis
- S Keele
- S Lipscomb
- S Nozaradan
- SH Anvari
- T Fujioka
- T Fujioka
- T Fujioka
- U Goswami
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2013
- Field of study
Temporal processing underlies both music and language skills. There is increasing evidence that rhythm abilities track with reading performance and that language disorders such as dyslexia are associated with poor rhythm abilities. However, little is known about how basic time-keeping skills can be shaped by musical training, particularly during critical literacy development years. This study was carried out in collaboration with Harmony Project, a non-profit organization providing free music education to children in the gang reduction zones of Los Angeles. Our findings reveal that elementary school children with just one year of classroom music instruction perform more accurately in a basic finger-tapping task than their untrained peers, providing important evidence that fundamental time-keeping skills may be strengthened by short-term music training. This sets the stage for further examination of how music programs may be used to support the development of basic skills underlying learning and literacy, particularly in at-risk populations which may benefit the most
Targeted analysis of four breeds narrows equine Multiple Congenital Ocular Anomalies locus to 208 kilobases
- Author
- A Komaromy
- A Watanabe
- AC Karlsson
- AC Theos
- AV Das
- B Duncan
- BH Grahn
- BjΓΆrn Ekesten
- BS Kwon
- C Kuehn
- CA Hodgkinson
- CM Wade
- David T. Ramsey
- DT Ramsey
- DT Ramsey
- DT Ramsey
- E Brunberg
- EK Shin
- EM Santschi
- G Benson
- Gabriella Lindgren
- Gus Cothran
- HB Schonthaler
- JA Rudolph
- JL Johnson
- Katarina Lyberg
- L Corbeel
- L Wang
- LA Clark
- Lisa S. Andersson
- LS Andersson
- ML Dechassa
- R Hu
- R Liu
- RC Tryon
- Rytis Juras
- S Kerje
- S Rozen
- SL Ewart
- Sofia Mikko
- Susan Ewart
- Y Nobukuni
- Z Liu
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2011
- Field of study
The syndrome Multiple Congenital Ocular Anomalies (MCOA) is the collective name ascribed to heritable congenital eye defects in horses. Individuals homozygous for the disease allele (MCOA phenotype) have a wide range of eye anomalies, while heterozygous horses (Cyst phenotype) predominantly have cysts that originate from the temporal ciliary body, iris, and/or peripheral retina. MCOA syndrome is highly prevalent in the Rocky Mountain Horse but the disease is not limited to this breed. Affected horses most often have a Silver coat color; however, a pleiotropic link between these phenotypes is yet to be proven. Locating and possibly isolating these traits would provide invaluable knowledge to scientists and breeders. This would favor maintenance of a desirable coat color while addressing the health concerns of the affected breeds, and would also provide insight into the genetic basis of the disease. Identical-by-descent mapping was used to narrow the previous 4.6-Mb region to a 264-kb interval for the MCOA locus. One haplotype common to four breeds showed complete association to the disease (Cyst phenotype, nΒ =Β 246; MCOA phenotype, nΒ =Β 83). Candidate genes from the interval, SMARCC2 and IKZF4, were screened for polymorphisms and genotyped, and segregation analysis allowed the MCOA syndrome region to be shortened to 208Β kb. This interval also harbors PMEL17, the gene causative for Silver coat color. However, by shortening the MCOA locus by a factor of 20, 176 other genes have been unlinked from the disease and only 15 genes remain
Cortical Plasticity Induced by Short-Term Multimodal Musical Rhythm Training
- Author
- A Petacchi
- AJ Shahin
- AJ Shahin
- B Haslinger
- BH Repp
- C Gaser
- C Lappe
- C Oldfield R
- C Pantev
- C Pantev
- CD Tesche
- Christo Pantev
- CJ Limb
- Claudia Lappe
- DB Polley
- DJ Bosnyak
- E Brattico
- E Geiser
- G Schlaug
- G Schlaug
- H Platel
- I Cross
- J Chen
- J Fritz
- J Phillips-Silver
- J Phillips-Silver
- J RΓΌsseler
- JA Grahn
- JA Grahn
- JR Zatorre
- KL Hyde
- Laurel J. Trainor
- Li I. Zhang
- LJ Trainor
- LJ Trainor
- M Atienza
- M Bangert
- M Bangert
- M Bangert
- M Kasia
- M Marinoni
- M Proksch
- M Schulz
- M SchΓΆnwiesner
- M Zentner
- ML Jongsma
- ML Jongsma
- P Bermudez
- P Janata
- P Schneider
- P Vuust
- Patel
- PQ Pfordrescher
- R NÀÀtÀnen
- RJ Zatorre
- RJ Zatorre
- S Baumann
- S Brown
- S Brown
- S Evers
- S Hutchinson
- S Koelsch
- SC Herholz
- SC Herholz
- Sibylle C. Herholz
- T Elbert
- T Fujioka
- T Fujioka
- T Kujala
- TW Picton
- Y Hirata
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Performing music is a multimodal experience involving the visual, auditory, and somatosensory modalities as well as the motor system. Therefore, musical training is an excellent model to study multimodal brain plasticity. Indeed, we have previously shown that short-term piano practice increase the magnetoencephalographic (MEG) response to melodic material in novice players. Here we investigate the impact of piano training using a rhythmic-focused exercise on responses to rhythmic musical material. Musical training with non musicians was conducted over a period of two weeks. One group (sensorimotor-auditory, SA) learned to play a piano sequence with a distinct musical rhythm, another group (auditory, A) listened to, and evaluated the rhythmic accuracy of the performances of the SA-group. Training-induced cortical plasticity was evaluated using MEG, comparing the mismatch negativity (MMN) in response to occasional rhythmic deviants in a repeating rhythm pattern before and after training. The SA-group showed a significantly greater enlargement of MMN and P2 to deviants after training compared to the A- group. The training-induced increase of the rhythm MMN was bilaterally expressed in contrast to our previous finding where the MMN for deviants in the pitch domain showed a larger right than left increase. The results indicate that when auditory experience is strictly controlled during training, involvement of the sensorimotor system and perhaps increased attentional recources that are needed in producing rhythms lead to more robust plastic changes in the auditory cortex compared to when rhythms are simply attended to in the auditory domain in the absence of motor production
A Method to Quantify Mouse Coat-Color Proportions
- Author
- A Bradley
- A Castilho
- A Visel
- AG Smith
- AL Brunner
- BH Koller
- CA Cooney
- CA Cooney
- CB Ware
- Craig A. Cooney
- DC Dolinoy
- DJ Schuirmann
- DM Duhl
- Eric R. Siegel
- Erik A. Nilsson
- F Gaudet
- G Van Belle
- GL Wolff
- GL Wolff
- GL Wolff
- HD Morgan
- JE Cropley
- JM Bland
- JM Bland
- K Hochedlinger
- Kristin L. Wheeler
- Leszek Wojnowski
- LN Trut
- M Buehr
- M Wu
- P Li
- PE Shrout
- PL Schwartzberg
- PM Fayers
- PS Yan
- RA Grahn
- RA Waterland
- Rachel E. McDonald-Phillips
- RL Mynatt
- Songthip Ounpraseuth
- T Koji
- TI Leakey
- TM Badger
- Tonya M. Rafferty
- VM Komashko
- Whitney M. Gammill
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
Coat-color proportions and patterns in mice are used as assays for many processes such as transgene expression, chimerism, and epigenetics. In many studies, coat-color readouts are estimated from subjective scoring of individual mice. Here we show a method by which mouse coat color is quantified as the proportion of coat shown in one or more digital images. We use the yellow-agouti mouse model of epigenetic variegation to demonstrate this method. We apply this method to live mice using a conventional digital camera for data collection. We use a raster graphics editing program to convert agouti regions of the coat to a standard, uniform, brown color and the yellow regions of the coat to a standard, uniform, yellow color. We use a second program to quantify the proportions of these standard colors. This method provides quantification that relates directly to the visual appearance of the live animal. It also provides an objective analysis with a traceable record, and it should allow for precise comparisons of mouse coats and mouse cohorts within and between studies
Cyclic and Sleep-Like Spontaneous Alternations of Brain State Under Urethane Anaesthesia
- Author
- A Carlsson
- A Ocampo_Garces
- A Rechtschaffen
- A Rechtschaffen
- A Rechtschaffen
- A Shafer
- A Tung
- A Tung
- A Tung
- A Tung
- A Tung
- A Tung
- A Ylinen
- AA BorbΓ©ly
- AA Nomeir
- AG Siapas
- Alby Richard
- BE Jones
- BE Jones
- BH Bland
- BH Bland
- C Dickson
- C Dickson
- CH Vanderwolf
- Clayton T. Dickson
- CM Sinton
- D Contreras
- DA Grahn
- DD Koblin
- E Aserinsky
- E Aserinsky
- EF Pace_Schott
- Elizabeth A. Clement
- Ernest Greene
- GG Kinney
- HC Dringenberg
- J Lee
- J Lu
- JA Hobson
- JA Hobson
- JD Hunter
- JM Siegel
- Jonathan Ailon
- JR Bueno
- K Hara
- L DΓ©tΓ‘ri
- LE Nelson
- LE Nelson
- LE Nelson
- M Chaput
- M Ferrara
- M Molle
- M Murakami
- M Steriade
- M Steriade
- M Steriade
- Megan Thwaites
- MN Shouse
- MP Sceniak
- O Eschenko
- PJ Whelan
- RC Carvalho
- RE Sotomayor
- RL Horner
- RP Vertes
- RW McCarley
- S Datta
- Steven Peters
- T Wolansky
- TE Robinson
- TE Robinson
- W Dement
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
Background: Although the induction of behavioural unconsciousness during sleep and general anaesthesia has been shown to involve overlapping brain mechanisms, sleep involves cyclic fluctuations between different brain states known as active (paradoxical or rapid eye movement: REM) and quiet (slow-wave or non-REM: nREM) stages whereas commonly used general anaesthetics induce a unitary slow-wave brain state. Methodology/Principal Findings: Long-duration, multi-site forebrain field recordings were performed in urethaneanaesthetized rats. A spontaneous and rhythmic alternation of brain state between activated and deactivated electroencephalographic (EEG) patterns was observed. Individual states and their transitions resembled the REM/nREM cycle of natural sleep in their EEG components, evolution, and time frame (,11 minute period). Other physiological variables such as muscular tone, respiration rate, and cardiac frequency also covaried with forebrain state in a manner identical to sleep. The brain mechanisms of state alternations under urethane also closely overlapped those of natural sleep in their sensitivity to cholinergic pharmacological agents and dependence upon activity in the basal forebrain nuclei that are the major source of forebrain acetylcholine. Lastly, stimulation of brainstem regions thought to pace state alternations in sleep transiently disrupted state alternations under urethane. Conclusions/Significance: Our results suggest that urethane promotes a condition of behavioural unconsciousness tha
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonelli S
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arms KE
- Armstrong SR
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bee C
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Belhorma B
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo G
- Bellomo M
- Belloni A
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benedict BH
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Bingul A
- Bini C
- Biscarat C
- Bischof R
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Boaretto C
- Bobbink GJ
- Bobrovnikov VB
- Bocci A
- Bock R
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bona M
- Boonekamp M
- Boorman G
- Booth CN
- Booth JRA
- Booth P
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Boulahouache C
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Braccini S
- Bracinik J
- Braem A
- Brambilla E
- Branchini P
- Branco MDO
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Brett ND
- Bright-Thomas PG
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brubaker E
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Buescher V
- Bueso XP
- Bugge L
- Buira-Clark D
- Buis EJ
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Byatt T
- Cabrera Urban S
- Caccia M
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camard A
- Camarri P
- Cambiaghi M
- Cameron D
- Camillocci ES
- Cammin J
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepa A
- Cantero J
- Capasso L
- Caprini I
- Caprini M
- Caprio M
- Capriotti D
- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carpentieri C
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo Gimenez V
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavalcanti TP
- Cavallari A
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Cazzato A
- Ceradini F
- Cerna C
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervetto M
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen H
- Chen L
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Cherkaoui El Moursli R
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chevallier F
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Ciocca C
- Ciocio A
- Cirilli M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration A
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coluccia R
- Comune G
- Conde Muino P
- Coniavitis E
- Conidi MC
- Consonni M
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correard S
- Correia AMH
- Corriveau F
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Coura Torres R
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Crepe-Renaudin S
- Cristinziani M
- Crosetti G
- Crupi R
- Cuneo S
- Curatolo M
- Curtis CJ
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- da Costa JBG
- Da Rocha Gesualdi Mello A
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dahlhoff A
- Dai T
- Dallapiccola C
- Dallison SJ
- Dam M
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- Yoosoofmiya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zdrazil M
- Zeitnitz C
- Zeller M
- Zema PF
- Zemla A
- Zendler C
- Zenin AV
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MS
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Gonzalez BA
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amram N
- Anastopoulos C
- Ancu LS
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- Anderson KJ
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- Angelidakis S
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- Anghinolfi F
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- Yilmaz M
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- Yorita K
- Yoshida R
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- Zeitnitz C
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- Zenin O
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- Zerwas D
- della Porta GZ
- Zhang D
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fbβ1 of sβ=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan Ξ² < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at sβ=7 TeV with the ATLAS detector
- Author
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- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Aben R
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- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
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- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang H
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- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Zβ² gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Ξ³ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbβ1 in the e + e β channel and 5.0 fbβ1 in the ΞΌ + ΞΌ βchannel. A Z β² boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Zβ² Models
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami 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 βs = 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 pTβ₯20 GeV and pseudorapidities {pipe}Ξ·{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}Ξ·{pipe}<0. 8) for jets with 60β€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2β€{pipe}Ξ·{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. Β© 2013 CERN for the benefit of the ATLAS collaboration
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