1,374 research outputs found
Single-Atom Resolved Fluorescence Imaging of an Atomic Mott Insulator
- Author
- B Capogrosso-Sansone
- B Paredes
- C Zhang
- C-L Hung
- C-L Hung
- Christof Weitenberg
- D Jaksch
- D Jaksch
- F Gerbier
- F Gerbier
- GK Campbell
- I Bloch
- IB Spielman
- Immanuel Bloch
- J-S Bernier
- Jacob F. Sherson
- KD Nelson
- M Greiner
- M Karski
- M Rigol
- Manuel Endres
- Marc Cheneau
- MPA Fisher
- MT DePue
- N Gemelke
- R Jördens
- R Raussendorf
- S Fölling
- Stefan Kuhr
- T Gericke
- T Kinoshita
- T-L Ho
- U Schneider
- W Krauth
- WS Bakr
- WS Bakr
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2010
- Field of study
The reliable detection of single quantum particles has revolutionized the
field of quantum optics and quantum information processing. For several years,
researchers have aspired to extend such detection possibilities to larger scale
strongly correlated quantum systems, in order to record in-situ images of a
quantum fluid in which each underlying quantum particle is detected. Here we
report on fluorescence imaging of strongly interacting bosonic Mott insulators
in an optical lattice with single-atom and single-site resolution. From our
images, we fully reconstruct the atom distribution on the lattice and identify
individual excitations with high fidelity. A comparison of the radial density
and variance distributions with theory provides a precise in-situ temperature
and entropy measurement from single images. We observe Mott-insulating plateaus
with near zero entropy and clearly resolve the high entropy rings separating
them although their width is of the order of only a single lattice site.
Furthermore, we show how a Mott insulator melts for increasing temperatures due
to a proliferation of local defects. Our experiments open a new avenue for the
manipulation and analysis of strongly interacting quantum gases on a lattice,
as well as for quantum information processing with ultracold atoms. Using the
high spatial resolution, it is now possible to directly address individual
lattice sites. One could, e.g., introduce local perturbations or access regions
of high entropy, a crucial requirement for the implementation of novel cooling
schemes for atoms on a lattice
A Rydberg Quantum Simulator
- Author
- A Gaëtan
- A SĂžrensen
- AK Mohapatra
- AV Gorshkov
- AY Kitaev
- AY Kitaev
- B Kraus
- D MĂžller
- D Rokhsar
- D Tong
- E Altman
- E Urban
- G Jackeli
- H Bombin
- H-P Breuer
- Hans Peter BĂŒchler
- Hendrik Weimer
- I Bloch
- Igor Lesanovsky
- J Vidal
- JB Kogut
- K Singer
- KD Nelson
- KD Stokes
- L-M Duan
- M Aguado
- M Fleischhauer
- M Hermele
- M Levin
- M MĂŒller
- Markus MĂŒller
- O Motrunich
- Peter Zoller
- R Heidemann
- R Moessner
- RP Feynman
- S Diehl
- S Fölling
- S Lloyd
- S Whitlock
- T Cubel
- T Vogt
- TF Gallagher
- TG Walker
- W Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 09/04/2012
- Field of study
Following Feynman and as elaborated on by Lloyd, a universal quantum
simulator (QS) is a controlled quantum device which reproduces the dynamics of
any other many particle quantum system with short range interactions. This
dynamics can refer to both coherent Hamiltonian and dissipative open system
evolution. We investigate how laser excited Rydberg atoms in large spacing
optical or magnetic lattices can provide an efficient implementation of a
universal QS for spin models involving (high order) n-body interactions. This
includes the simulation of Hamiltonians of exotic spin models involving
n-particle constraints such as the Kitaev toric code, color code, and lattice
gauge theories with spin liquid phases. In addition, it provides the
ingredients for dissipative preparation of entangled states based on
engineering n-particle reservoir couplings. The key basic building blocks of
our architecture are efficient and high-fidelity n-qubit entangling gates via
auxiliary Rydberg atoms, including a possible dissipative time step via optical
pumping. This allows to mimic the time evolution of the system by a sequence of
fast, parallel and high-fidelity n-particle coherent and dissipative Rydberg
gates.Comment: 8 pages, 4 figure
Recommended conventions for reporting results from direct dark matter searches
- Author
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 15/10/2021
- Field of study
The field of dark matter detection is a highly visible and highly competitive one. In this paper, we propose recommendations for presenting dark matter direct detection results particularly suited for weak-scale dark matter searches, although we believe the spirit of the recommendations can apply more broadly to searches for other dark matter candidates, such as very light dark matter or axions. To translate experimental data into a final published result, direct detection collaborations must make a series of choices in their analysis, ranging from how to model astrophysical parameters to how to make statistical inferences based on observed data. While many collaborations follow a standard set of recommendations in some areas, for example the expected flux of dark matter particles (to a large degree based on a paper from Lewin and Smith in 1995), in other areas, particularly in statistical inference, they have taken different approaches, often from result to result by the same collaboration. We set out a number of recommendations on how to apply the now commonly used Profile Likelihood Ratio method to direct detection data. In addition, updated recommendations for the Standard Halo Model astrophysical parameters and relevant neutrino fluxes are provided. The authors of this note include members of the DAMIC, DarkSide, DARWIN, DEAP, LZ, NEWS-G, PandaX, PICO, SBC, SENSEI, SuperCDMS, and XENON collaborations, and these collaborations provided input to the recommendations laid out here. Wide-spread adoption of these recommendations will make it easier to compare and combine future dark matter results
Orbital excitation blockade and algorithmic cooling in quantum gases
- Author
- A Gaëtan
- C Weitenberg
- D Jaksch
- DC McKay
- DS Weiss
- E Urban
- G Wirth
- GK Campbell
- GM Nikolopoulos
- I Bloch
- J Baugh
- Jonathan Simon
- K Ono
- KD Nelson
- KM Birnbaum
- L Isenhower
- M Greiner
- M Lewenstein
- M Popp
- M. Eric Tai
- MA Kastner
- Markus Greiner
- P Boykin
- P Cheinet
- P Medley
- P Rabl
- P Soltan-Panahi
- Philipp M. Preiss
- Ruichao Ma
- S Will
- T MĂŒller
- T Wilk
- Waseem S. Bakr
- WS Bakr
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 07/10/2011
- Field of study
Interaction blockade occurs when strong interactions in a confined few-body
system prevent a particle from occupying an otherwise accessible quantum state.
Blockade phenomena reveal the underlying granular nature of quantum systems and
allow the detection and manipulation of the constituent particles, whether they
are electrons, spins, atoms, or photons. The diverse applications range from
single-electron transistors based on electronic Coulomb blockade to quantum
logic gates in Rydberg atoms. We have observed a new kind of interaction
blockade in transferring ultracold atoms between orbitals in an optical
lattice. In this system, atoms on the same lattice site undergo coherent
collisions described by a contact interaction whose strength depends strongly
on the orbital wavefunctions of the atoms. We induce coherent orbital
excitations by modulating the lattice depth and observe a staircase-type
excitation behavior as we cross the interaction-split resonances by tuning the
modulation frequency. As an application of orbital excitation blockade (OEB),
we demonstrate a novel algorithmic route for cooling quantum gases. Our
realization of algorithmic cooling utilizes a sequence of reversible OEB-based
quantum operations that isolate the entropy in one part of the system, followed
by an irreversible step that removes the entropy from the gas. This work opens
the door to cooling quantum gases down to ultralow entropies, with implications
for developing a microscopic understanding of strongly correlated electron
systems that can be simulated in optical lattices. In addition, the close
analogy between OEB and dipole blockade in Rydberg atoms provides a roadmap for
the implementation of two-qubit gates in a quantum computing architecture with
natural scalability.Comment: 6 pages, 4 figure
"I'm not being rude, I'd want somebody normal" Adolescents' perception of their peers with Tourette's syndrome; an exploratory study
- Author
- A Strauss
- AJ Cuddy
- AJ Goreczny
- AJ Hutchison
- AK Taylor
- AS Carter
- AS GĂŒler
- AW Fominaya
- B Glaser
- B Weiner
- CM Eddy
- D Cutler
- DA Gorman
- DW Bell
- DW Woods
- DW Woods
- DW Woods
- E Walther
- EA Storch
- F Davis
- H Smith
- HB Bergsieker
- I Katz
- I Krumpal
- J Cohen
- J Garcia
- J Juvonen
- J Kitzinger
- J McCambridge
- JB Pryor
- JM Campbell
- JS Stern
- KD Holtz
- M Bloch
- M Killen
- M Nussbaum
- MA Malli
- Melina Aikaterini Malli
- MH Bloch
- MM Robertson
- MM Robertson
- MM Thompson
- MR Hebl
- N Epley
- PJ Boudjouk
- PJ Hollenbeck
- PW Corrigan
- PW Corrigan
- Rachel Forrester-Jones
- RD Freeman
- RD Freeman
- S Calder-Sprackman
- S Friedrich
- S Horn
- SB Kamenetsky
- SD Lambert
- T Knight
- TA Wills
- WC Thompson
- WM Finlay
- Y Zhu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Background: Touretteâs syndrome (TS) is a highly stigmatised condition, and typically developing adolescentsâ motives and reason for excluding individuals with TS have not been examined.
Aims: The aim of the study was to understand how TS is conceptualised by adolescents and explore how individuals with TS are perceived by their typically developing peers.
Method: Free text writing and focus groups were used to elicit the views of twenty-two year ten students from a secondary school in South East England. Grounded theory was used to develop an analytical framework.
Result: Participantsâ understanding about the condition was construed from misconceptions, unfamiliarity and unanswered questions. Adolescents who conceived TS as a disorder beyond the individualâs control perceived their peers as being deprived of agency and strength and as straying from the boundaries of normalcy. People with TS were viewed as individuals deserving pity, and in need of support. Although participants maintained they had feelings of social politeness towards those with TS, they would avoid initiating meaningful social relationships with them due to fear of âsocial contaminationâ. Intergroup anxiety would also inhibit a close degree of social contact. Participants that viewed those with TS as responsible for their condition expressed a plenary desire for social distance. However, these behavioural intentions were not limited to adolescents that elicited inferences of responsibility to people with TS, indicating that attributional models of stigmatisation may be of secondary importance in the case of TS.
Implications for interventions to improve school belonging among youths with TS are discussed
Field-sensitive addressing and control of field-insensitive neutral-atom qubits
- Author
- A Imamoglu
- C Zhang
- D Hayes
- D Jaksch
- D Jaksch
- D Schrader
- DS Weiss
- E Knill
- GK Brennen
- GK Campbell
- GS Uhrig
- H Katori
- HK Cummins
- I Bloch
- I Deutsch
- I. B. Spielman
- J Beugnon
- J Sebby-Strabley
- J Taylor
- J. M. Obrecht
- J. V. Porto
- KD Nelson
- M Anderlini
- M Levitt
- MJ Biercuk
- MR Matthews
- N Lundblad
- N. Lundblad
- NF Ramsey
- O Mandel
- O Mandel
- P Rosenbusch
- PJ Lee
- VV Flambaum
- W Gerlach
- W Rakreungdet
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 18/02/2009
- Field of study
The establishment of a scalable scheme for quantum computing with addressable
and long-lived qubits would be a scientific watershed, harnessing the laws of
quantum physics to solve classically intractable problems. The design of many
proposed quantum computational platforms is driven by competing needs:
isolating the quantum system from the environment to prevent decoherence, and
easily and accurately controlling the system with external fields. For example,
neutral-atom optical-lattice architectures provide environmental isolation
through the use of states that are robust against fluctuating external fields,
yet external fields are essential for qubit addressing. Here we demonstrate the
selection of individual qubits with external fields, despite the fact that the
qubits are in field-insensitive superpositions. We use a spatially
inhomogeneous external field to map selected qubits to a different
field-insensitive superposition ("optical MRI"), minimally perturbing
unselected qubits, despite the fact that the addressing field is not spatially
localized. We show robust single-qubit rotations on neutral-atom qubits located
at selected lattice sites. This precise coherent control is an important step
forward for lattice-based neutral-atom quantum computation, and is quite
generally applicable to state transfer and qubit isolation in other
architectures using field-insensitive qubits.Comment: press embarg
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at âs = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- Atlay NB
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescua E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartos P
- Bartsch V
- Bassalat A
- Basye A
- Bates RL
- Batkova L
- Batley JR
- Battistin M
- Bauer F
- Bawa HS
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
- Becker S
- Beckingham M
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr K
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belloni A
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
- Benekos N
- Benhammou Y
- Benjamin DP
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernard C
- Bernat P
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertolucci F
- Besana MI
- Besjes GJ
- Bessidskaia O
- Besson N
- Betancourt C
- Bethke S
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
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- Black CW
- Black JE
- Black KM
- Blackburn D
- Blair RE
- Blanchard J-B
- Blazeka T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boek TT
- Boeriu OEV
- Bogaerts JA
- Bogdanchikov AG
- Bogouch A
- Bohm C
- Bohm J
- Boisvert V
- Bold T
- Boldea V
- Boldyrev AS
- Bolnet NM
- Bomben M
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- Boonekamp M
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- Brazzale SF
- Brelier B
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- Brennan AJ
- Brenner R
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- Buat Q
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- Buchholz P
- Buckingham RM
- Buckley AG
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- Buescher V
- Bugge L
- Bugge MK
- Bulekov O
- Bundock AC
- Burckhart H
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- Burmeister I
- Busato E
- Bussey P
- Bustos ACF
- Buszello CP
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- Butt AI
- Buttar CM
- Butterworth JM
- Buttinger W
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- Byszewski M
- Cabrera Urban S
- Caforio D
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- Caminal Armadans R
- Campana S
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- Canelli F
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- Cantero J
- Cantrill R
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- Caprini I
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- Caputo R
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- Carquin E
- Carrillo-Montoya GD
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Castaneda-Miranda E
- Castanheira MTD
- Castelli A
- Castillo Gimenez V
- Castillo IS
- Castillo LRF
- Castillo LRF
- Castro NF
- Catastini P
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavaliere V
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerio B
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cerv M
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chan K
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
- Chen L
- Chen S
- Chen X
- Chen Y
- Cheng HC
- Cheng Y
- Cheplakov A
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiefari G
- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Chouridou S
- Chow BKB
- Christidi IA
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciocio A
- Cirkovic P
- Citron ZH
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Clarke RN
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coffey L
- Cogan JG
- Coggeshall J
- Cole B
- Cole S
- Colijn AP
- Collaboration ATLAS
- Collins-Tooth C
- Collot J
- Colombo T
- Colon G
- Compostella G
- Conde Muino P
- Coniavitis E
- Conidi MC
- Connelly IA
- Consonni SM
- Consorti V
- Constantinescu S
- Conta C
- Conti G
- Conventi F
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
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- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
- Cottin G
- Coutinho YA
- Cowan G
- Cox BE
- Cranmer K
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Cuciuc C-M
- Cummings J
- Curatolo M
- Cuthbert C
- Czirr H
- Czodrowski P
- Czyczula Z
- D'Auria S
- D'Onofrio M
- Da Costa JBG
- Da Costa JGPF
- Da Costa JGPF
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dafinca A
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Daniells AC
- Dao V
- Darbo G
- Darlea GL
- Darmora S
- Dassoulas JA
- Davey W
- David C
- Davidek T
- Davies E
- Davies M
- Davignon O
- Davison AR
- Davison P
- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Asmundis R
- De Bruin PHS
- De Castro S
- De Cecco S
- de Graat J
- De Groot N
- de Jong P
- De la Taille C
- De la Torre H
- de Lima DEF
- de Lima DEF
- De Lorenzi F
- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De Zorzi G
- De K
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Degenhardt J
- Deigaard I
- Del Peso J
- Del Prete T
- Delemontex T
- Deliot F
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demilly A
- Demirkoz B
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
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- Desch K
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Di Valentino D
- Diaz MA
- Diehl EB
- Dietrich J
- Dietzsch TA
- Diglio S
- Dimitrievska A
- Dingfelder J
- Dionisi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- do Vale MAB
- Doan TKO
- Dobos D
- Dobson E
- Doglioni C
- Doherty T
- Dohmae T
- Dolejsi J
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donati S
- Dondero P
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Santos DR
- Dotti A
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- Dris M
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- Dube S
- Dubreuil E
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Dudziak F
- Duehrssen M
- Dueren M
- Duflot L
- Duguid L
- Dunford M
- Dwuznik M
- Ebke J
- Edson W
- Edwards NC
- Ehrenfeld W
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Moursli A
- El Moursli RC
- Ellert M
- Elles S
- Ellinghaus F
- Ellinghaus F
- Ellis N
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- Elmsheuser J
- Elmsheuser J
- Elsing M
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- Emeliyanov D
- Emeliyanov D
- Enari Y
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- Endner OC
- Endner OC
- Endo M
- Endo M
- Engelmann R
- Engelmann R
- Erdmann J
- Erdmann J
- Ereditato A
- Ereditato A
- Eriksson D
- Eriksson D
- Ernis G
- Ernis G
- Ernst J
- Ernst J
- Ernst M
- Ernst M
- Ernwein J
- Ernwein J
- Errede D
- Errede D
- Errede S
- Errede S
- Ertel E
- Ertel E
- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
- Esposito B
- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
- Evans H
- Fabbri L
- Fabbri L
- Facini G
- Facini G
- Fajardo LSG
- Fajardo LSG
- Fakhrutdinov RM
- Fakhrutdinov RM
- Falciano S
- Falciano S
- Faltova J
- Faltova J
- Fang Y
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- Fanti M
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- Farbin A
- Farbin A
- Farilla A
- Farilla A
- Farooque T
- Farooque T
- Farrell S
- Farrell S
- Farrington SM
- Farrington SM
- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
- Fassnacht P
- Fassouliotis D
- Fassouliotis D
- Favareto A
- Favareto A
- Fayard L
- Fayard L
- Federic P
- Federic P
- Fedin OL
- Fedin OL
- Fedorko W
- Fedorko W
- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
- Feigl S
- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
- Feng H
- Fenyuk AB
- Fenyuk AB
- Fernando W
- Fernando W
- Ferrag S
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
- Ferrari P
- Ferrari R
- Ferrari R
- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
- Ferretti C
- Fiascaris M
- Fiascaris M
- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
- Finelli KD
- Fiolhais MCN
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- Fiorini L
- Fiorini L
- Firan A
- Firan A
- Fischer J
- Fischer J
- Fisher MJ
- Fisher MJ
- Fitzgerald EA
- Fitzgerald EA
- Flechl M
- Flechl M
- Fleck I
- Fleck I
- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
- Fletcher GT
- Flick T
- Flick T
- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
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- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
- Franchino S
- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
- Friedrich F
- Froidevaux D
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- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
- Galster G
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- Gandrajula RP
- Gandrajula RP
- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
- Gaur B
- Gauthier L
- Gauthier L
- Gauzzi P
- Gauzzi P
- Gavrilenko IL
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- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
- Gellerstedt K
- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
- Giagu S
- Giangiobbe V
- Giangiobbe V
- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
- Gibbard B
- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
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- Gillberg D
- Gillberg D
- Gillman AR
- Gillman AR
- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
- Giordano R
- Giorgi FM
- Giorgi FM
- Giraud PF
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- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
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- Gkialas I
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- Gladilin LK
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- Glasman C
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- Glatzer J
- Glatzer J
- Glazov A
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- Godfrey J
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- Goncalo R
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- Gonzalez Parra G
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- Gonzalez BA
- Gonzalez-Sevilla S
- Gonzalez-Sevilla S
- Goossens L
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- Gorbounov PA
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- Gordon HA
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- Gorelov I
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- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
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- Gostkin MI
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- Gouighri M
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- Goujdami D
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- Goulette MP
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- Goussiou AG
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- Goy C
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- Gozpinar S
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- Grabas HMX
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- Graber L
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- Grafstroem P
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- Grancagnolo F
- Grancagnolo S
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- Grancagnoloa F
- Grassi V
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- Gratchev V
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- Gray HM
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- Graziani E
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- Grebenyuk OG
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- Greenwood ZD
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- Gregersen K
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- Gregor IM
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- Grenier P
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- Griffiths J
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- Grillo AA
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- Grinstein S
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- Griso SP
- Grivaz J-F
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- Grohs JP
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- Grohsjean A
- Gross AGE
- Gross E
- Grosse-Knetter J
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- Grossi GC
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- Groth-Jensen J
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- Guan L
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- Guescini F
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- Guest D
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- Gueta O
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- Guicheney C
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- Guido E
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- Gutierrez P
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- Gutschow C
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- Guttman N
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- Harenberg T
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- Harris OM
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- Hasegawa Y
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- Kostyukhin VV
- Kotov VM
- Kotwal A
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- Kouskoura V
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- Laplace S
- Lapoire C
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- Laurelli P
- Lavorini V
- Lavrijsen W
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- Le Dortz O
- Le Guirriec E
- Le Menedeu E
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- LeCompte T
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- Loevschall-Jensen AE
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- Long JD
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- Lukas W
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- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of âs = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentreâofâmassframeisusedtosuppressthelargemultiâjetbackground.ThecrossâsectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
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
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Zhemchugov A
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- 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
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
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- Yanush S
- Yao L
- Yao Y
- Yasu Y
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- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
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- Youssef S
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- 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
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- Zhang X
- Zhang Z
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- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou Y
- Zhu CG
- Zhu H
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- 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
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- 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 R
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- 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
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- 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
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Atkinson M
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Avramidou R
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Balek P
- Banas E
- Banerjee P
- Banerjee S
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- Tskhadadze EG
- Tsukerman II
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- Zaidan R
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- Zajacova Z
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- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zerwas D
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- Zhemchugov A
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- Zibell A
- Zieminska D
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- 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
- 23/11/2012
- 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 ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł 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 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ 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 ZâČ Models
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