1,251 research outputs found
Electrophysiological Heterogeneity of Fast-Spiking Interneurons: Chandelier versus Basket Cells
- Author
- A Woodruff
- Aleksey V. Zaitsev
- AM Thomson
- AR Woodruff
- AV Zaitsev
- AV Zaitsev
- B Rudy
- C Constantinidis
- CR Yang
- D Guan
- DA Lewis
- DA McCormick
- David A. Lewis
- DJ Simons
- F Conde
- FA Wilson
- G Gonzalez-Burgos
- GA Ascoli
- Gianmaria Maccaferri
- Guillermo Gonzalez-Burgos
- H Taniguchi
- HC Pape
- J Szabadics
- JF Sauer
- JK Seamans
- JS Lund
- L Massi
- LL Glickfeld
- LS Krimer
- LS Krimer
- M Bartos
- M Inan
- M Steriade
- MV Sanchez-Vives
- MW Jung
- Nadezhda V. Povysheva
- NV Povysheva
- P Sah
- PA Glazebrook
- PL Gabbott
- RB Robinson
- RJ Douglas
- T Dugladze
- VF Descalzo
- VS Sohal
- X Xu
- Y Aponte
- Y Kawaguchi
- Y Kawaguchi
- Y Kawaguchi
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/08/2013
- Field of study
In the prefrontal cortex, parvalbumin-positive inhibitory neurons play a prominent role in the neural circuitry that subserves working memory, and alterations in these neurons contribute to the pathophysiology of schizophrenia. Two morphologically distinct classes of parvalbumin neurons that target the perisomatic region of pyramidal neurons, chandelier cells (ChCs) and basket cells (BCs), are generally thought to have the same "fast-spiking" phenotype, which is characterized by a short action potential and high frequency firing without adaptation. However, findings from studies in different species suggest that certain electrophysiological membrane properties might differ between these two cell classes. In this study, we assessed the physiological heterogeneity of fast-spiking interneurons as a function of two factors: species (macaque monkey vs. rat) and morphology (chandelier vs. basket). We showed previously that electrophysiological membrane properties of BCs differ between these two species. Here, for the first time, we report differences in ChCs membrane properties between monkey and rat. We also found that a number of membrane properties differentiate ChCs from BCs. Some of these differences were species-independent (e.g., fast and medium afterhyperpolarization, firing frequency, and depolarizing sag), whereas the differences in the first spike latency between ChCs and BCs were species-specific. Our findings indicate that different combinations of electrophysiological membrane properties distinguish ChCs from BCs in rodents and primates. Such electrophysiological differences between ChCs and BCs likely contribute to their distinctive roles in cortical circuitry in each species. © 2013 Povysheva et al
Ion implantation in nanodiamonds: Size effect and energy dependence
- Author
- A Magyar
- AA Shiryaev
- AB Verchovsky
- AM Zaitsev
- AM Zaitsev
- AP Koscheev
- AS Barnard
- AV Fisenko
- BA Fairchild
- D Saada
- DN Batuk
- F Valencia
- F Valencia
- G Greaves
- G Stan
- GK Ustinova
- GR Huss
- HO Funsten
- II Vlasov
- II Vlasov
- J Stursa
- J Tersoff
- J Vondele Van de
- J Vondele Van de
- JA Hinks
- JD Gilmour
- JP Perdew
- JT Buchan
- L Himics
- L Jamison
- L Pastewka
- MJ Demkowicz
- N Marks
- OA Shenderova
- RS Lewis
- S Goedecker
- S Gupta
- V Liechtenstein
- YV Martynenko
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
Nanoparticles are ubiquitous in nature and are increasingly important for technology. They are subject to bombardment by ionizing radiation in a diverse range of environments. In particular, nanodiamonds represent a variety of nanoparticles of significant fundamental and applied interest. Here we present a combined experimental and computational study of the behaviour of nanodiamonds under irradiation by xenon ions. Unexpectedly, we observed a pronounced size effect on the radiation resistance of the nanodiamonds: particles larger than 8 nm behave similarly to macroscopic diamond (i.e. characterized by high radiation resistance) whereas smaller particles can be completely destroyed by a single impact from an ion in a defined energy range. This latter observation is explained by extreme heating of the nanodiamonds by the penetrating ion. The obtained results are not limited to nanodiamonds, making them of interest for several fields, putting constraints on processes for the controlled modification of nanodiamonds, on the survival of dust in astrophysical environments, and on the behaviour of actinides released from nuclear waste into the environment
Photochromism in single nitrogen-vacancy defect in diamond
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 12/08/2005
- Field of study
Photochromism in single nitrogen-vacancy optical centers in diamond is
demonstrated. Time-resolved optical spectroscopy shows that intense irradiation
at 514 nm switches the nitrogen-vacancy defects to the negative form. This
defect state relaxes back to the neutral form under dark conditions. Temporal
anticorrelation of photons emitted by the different charge states of the
optical center unambiguously indicates that the nitrogen-vacancy defect
accounts for both 575 nm and 638 nm emission bands. Possible mechanism of
photochromism involving nitrogen donors is discussed.Comment: 11 pages, 3 figures, submitted to Applied Physics B: Lasers and
Optic
Benchmarking of cell type deconvolution pipelines for transcriptomics data
- Author
- A Sharma
- AM Newman
- AM Newman
- AT L. Lun
- B Jew
- B Li
- B Li
- BM Bolstad
- C Evans
- C Hafemeister
- C Soneson
- CW Law
- D Risso
- D Tsoucas
- DC Hoyle
- DJ McCarthy
- F Avila Cobos
- F Elloumi
- F Finotello
- F Vallania
- FW Townes
- G Monaco
- G Sturm
- GJ Hunt
- GXY Zheng
- I Zwiener
- J Friedman
- J Racle
- JH Bullard
- K Zaitsev
- M Baron
- M Enge
- M Hoffmann
- M Schelker
- M-A Dillies
- MD Robinson
- MD Robinson
- P Darvin
- R Gaujoux
- R Gaujoux
- S Anders
- S Hendry
- SH Yip
- T Abdelaal
- T Gong
- X Wang
- Y Hao
- Y Zhong
- Y Zhong
- Z Altboum
- Ă Segerstolpe
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2020
- Field of study
Many computational methods have been developed to infer cell type proportions from bulk transcriptomics data. However, an evaluation of the impact of data transformation, pre-processing, marker selection, cell type composition and choice of methodology on the deconvolution results is still lacking. Using five single-cell RNA-sequencing (scRNA-seq) datasets, we generate pseudo-bulk mixtures to evaluate the combined impact of these factors. Both bulk deconvolution methodologies and those that use scRNA-seq data as reference perform best when applied to data in linear scale and the choice of normalization has a dramatic impact on some, but not all methods. Overall, methods that use scRNA-seq data have comparable performance to the best performing bulk methods whereas semi-supervised approaches show higher error values. Moreover, failure to include cell types in the reference that are present in a mixture leads to substantially worse results, regardless of the previous choices. Altogether, we evaluate the combined impact of factors affecting the deconvolution task across different datasets and propose general guidelines to maximize its performance. Inferring cell type proportions from transcriptomics data is affected by data transformation, normalization, choice of method and the markers used. Here, the authors use single-cell RNAseq datasets to evaluate the impact of these factors and propose guidelines to maximise deconvolution performance
The Hubbard model within the equations of motion approach
- Author
- Abrikosov A
- Abrikosov AA
- Aksenov V
- Alexandrov A
- Allega AM
- Alvarez J
- Alvarez J
- Anderson P
- Anderson P
- Andrei EY
- Anlage S
- Annett J
- Ashcroft N
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Avella A
- Bak M
- Bak M
- Bala J
- Barnes SE
- Barrett S
- Becca F
- Becker KW
- Beenen J
- Belkhir L
- Bickers N
- Bickers N
- Bickers N
- Birgenau R
- Boer JD
- Boer JD
- Bogoliubov N
- Bogoliubov N
- Bogolubov N
- Bonca J
- Bonner J
- Bosse J
- Brenig W
- Brewer DF
- Brinkman WF
- Brodale GE
- Bruus H
- Bulla R
- Bulut N
- Bulut N
- Bulut N
- Buzatu FD
- BĂ©nard P
- BĂ©nard P
- Calandra M
- Callen H
- Canali C
- Cannon J
- Carmelo J
- Carter SA
- Carter SA
- Carter SA
- Chao KA
- Chatterji T
- Chattopadhyay B
- Chen CH
- Chen H
- Chen YC
- Cheong SW
- Chitra R
- Chow DS
- Coldea R
- Coleman P
- Cooper S
- Dagotto E
- Dagotto E
- Dagotto E
- Dagotto E
- Dai P
- Dai P
- Damascelli A
- Dancoff SM
- Deguchi T
- Dessau D
- Dessau DS
- Dho J
- Di Matteo T
- DI Matteo T
- DI Matteo T
- Dongen PV
- Dongen PV
- Dorneich A
- Dover RV
- Duffy D
- Duffy D
- Duffy D
- Duffy D
- Emery V
- Eskes H
- Fano G
- Fazekas P
- Fazekas P
- Fazekas P
- Fedro AJ
- Feiner LF
- Feng S
- Fernandez J
- Ferrer J
- Fetter A
- Fiorentino V
- Fischer J
- Fleck M
- Fong H
- Friedel J
- Fujimori A
- Fulde P
- Fulde P
- Furukawa N
- Furukawa N
- Furukawa N
- Gebhard F
- Gebhard F
- Geipel G
- Georges A
- Georges A
- Georges A
- Germann A
- Gofron K
- Gonzalez J
- Gooding R
- Gradshteyn IS
- Grewe N
- Greywall DS
- Grilli M
- Gutzwiller M
- Halboth C
- Hardy W
- Harlingen DV
- Hashimoto K
- Heeger AJ
- Hellberg C
- Herrmann T
- Herrmann T
- Hewson AC
- Hirsch J
- Hirsch JE
- Hirsch JE
- Hirsch JE
- Hirsch JE
- Hirsch JE
- Hoang A
- Horbach M
- Horbach M
- Howell RH
- Huang Z
- Hubbard J
- Hubbard J
- Hubbard J
- Huber DL
- Imada M
- Imada M
- Imada M
- Imada M
- Ino A
- Ino A
- Ino A
- Ino A
- Ioffe L
- Irkhin V
- Ishihara S
- Izyumov Y
- Izyumov Y
- Izyumov Y
- JakliÄ J
- Janner A
- Japaridze G
- Jarrell M
- Jarrell M
- Jeckelmann E
- Jelitto R
- Johnston D
- JĂŒttner G
- K. J.
- Kalashnikov OK
- Kalashnikov OK
- Kampf A
- Kampf A
- Kampf AP
- Kanamori J
- Kawakami N
- Kellen SB
- Kim C
- King DM
- Kohn W
- Kotliar G
- Kotliar G
- Kotliar G
- KrĂŒger P
- Kubo K
- Kubo R
- Kumagai K
- Kuramoto Y
- Kwork P
- Langer W
- Lee PA
- Lenck S
- Leplae L
- Liang W
- Lieb E
- Lieb E
- Lieb EH
- Lieb EH
- Lilly L
- Lin H
- Littlewood P
- Littlewood P
- Lonke A
- Loram J
- Loram J
- Loram J
- Loram JW
- Loram JW
- Luttinger JM
- MacDonald A
- MacDonald A
- Maier T
- Maier T
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Mancini F
- Manske D
- Mao J
- Markiewicz R
- Markiewicz R
- Markiewicz RS
- Martindale J
- Martindale J
- Mason T
- Mason TE
- Matsuda M
- Matsumoto H
- Matsumoto H
- Matsumoto H
- Matsumoto H
- Matsumoto H
- Matsumoto H
- Matsumoto H
- Mattis D
- Mattis D
- McKenzie RH
- McWhan DB
- McWhan DB
- Mehlig B
- Merino J
- Metzner W
- Metzner W
- Metzner W
- Micnas R
- Millis A
- Millis AJ
- Mills R
- Monien H
- Monthoux P
- Monthoux P
- Monthoux P
- Monthoux P
- Monthoux P
- Monthoux P
- Monthoux P
- Moreo A
- Moreo A
- Moreo A
- Moreo A
- Moreo A
- Mori H
- Mori H
- Morita T
- Moriya T
- Mott N
- Mott NF
- MĂŒnzner R
- Nagaoka Y
- Nakamura M
- Newns D
- Newns D
- Newns DM
- Nolting W
- Nolting W
- NoziĂšres P
- NoziĂšres P
- NĂ©lisse H
- Ochiai A
- Ogata M
- Ohama T
- Okajima Y
- Okamoto T
- OleĆ A
- Onoda S
- Onoda S
- Onoda S
- Ovchinnikov A
- Pao C-H
- Pao C-H
- Park SK
- Peres N
- Peters C
- Phillips NE
- Pietig R
- Pines D
- Plakida N
- Plakida N
- Plakida N
- Plakida N
- Plakida N
- Plakida N
- Plakida NM
- Plekhanov E
- Potthoff M
- Pruschke T
- Pruschke T
- Pruschke T
- Putikka WO
- Qin S
- Raimondi R
- Randeria M
- Randeria M
- Randeria M
- Randeria M
- Robaszkiewicz S
- Roger M
- Roth LM
- Rowe DJ
- Rozenberg MJ
- Rozenberg MJ
- Rozenberg MJ
- RĂžnnow H
- Salamon M
- Sato M
- Scalapino D
- Scalapino DJ
- Schlager HG
- Schneider T
- Schulte J
- Sengupta P
- Seo H
- Shafer M
- Shastry B
- Shen S-Q
- Shen Z
- Shen Z
- Shen Z-X
- Shiba H
- Shiba H
- Shimahara H
- Shirane G
- Shirane G
- Si Q
- Sigrist M
- SimĂłn M
- Singh R
- Sonier J
- Sorella S
- Sorella S
- SpaĆek J
- SpaĆek J
- SpaĆek J
- SpaĆek J
- Stanescu T
- Stanescu T
- Stanescu T
- Steglich F
- Stephan W
- Stephan W
- Stevens K
- Strack R
- Suzuki M
- SyljuÄsen O
- SĂĄnchez-Lopez M
- SĂĄnchez-Lopez M
- SĂĄnchez-Lopez M
- Takahashi M
- Takahashi M
- Takahashi M
- Takahashi Y
- Takigawa M
- Tamasaku K
- Tanamoto T
- Tasaki H
- Tasaki H
- Tasaki H
- Tasaki H
- Tasaki H
- Thomas GA
- Thurston T
- Thurston T
- Tian G
- Tohyama T
- Tokura Y
- Tomioka Y
- Torrance J
- Torrance J
- Tranquada J
- Trapper U
- Trapper U
- Tserkovnikov YA
- Tserkovnikov YA
- Tsuchiizu M
- Tsuei C
- Tutuc E
- Tyablikov S
- Uchida S
- Ueda K
- Ueda Y
- Usuki T
- Vaks V
- van den Brink J
- van den Brink J
- Varma C
- Varma C
- Varma C
- Vilk YM
- Villani D
- Visser AD
- Vojta M
- Vollhardt D
- Vollhardt D
- Vollhardt D
- Von Der Linden W
- Wada N
- Ward J
- Wells B
- Wermbter S
- Westerholt K
- White SR
- Wigner E
- Xu JH
- Xu JH
- Yamada K
- Yamada K
- Yamaji K
- Yang CN
- Yokohama H
- Yoon J
- Yu R
- Yushankhai V
- Yushankhai V
- Zaitsev R
- Zhang F
- Zhang W
- Zhang W
- Zhang XY
- Zhang XY
- Zhou Y
- Zubarev D
- Zubarev DN
- Publication venue
- 'Informa UK Limited'
- Publication date
- 01/01/2004
- Field of study
The Hubbard model has a special role in Condensed Matter Theory as it is
considered as the simplest Hamiltonian model one can write in order to describe
anomalous physical properties of some class of real materials. Unfortunately,
this model is not exactly solved except for some limits and therefore one
should resort to analytical methods, like the Equations of Motion Approach, or
to numerical techniques in order to attain a description of its relevant
features in the whole range of physical parameters (interaction, filling and
temperature). In this manuscript, the Composite Operator Method, which exploits
the above mentioned analytical technique, is presented and systematically
applied in order to get information about the behavior of all relevant
properties of the model (local, thermodynamic, single- and two- particle ones)
in comparison with many other analytical techniques, the above cited known
limits and numerical simulations. Within this approach, the Hubbard model is
shown to be also capable to describe some anomalous behaviors of the cuprate
superconductors.Comment: 232 pages, more than 300 figures, more than 500 reference
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â 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
- Bellos P
- 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
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- 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 fbâ1 of â 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
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
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- Zarzhitsky P
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- Zhemchugov A
- Zheng S
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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 âs = 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 pTâ„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 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{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
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
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- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
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- Yao L
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- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- Yurkewicz A
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- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
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- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- 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
- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Zitoun R
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- 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
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- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wynne BM
- Xella S
- Xiao M
- Xie S
- Xu C
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
- Ye S
- 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
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- 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
- 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 fbâ1 of sâ=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 ÎČ < 40
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