650 research outputs found
Road and bridge construction across gypsum karst in England
- Author
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/08/2002
- Field of study
Gypsum karst problems in the Permian and Triassic sequences of England have caused difficult conditions for bridge and road construction. In Northern England, the Ripon Bypass crosses Permian strata affected by active gypsum karst and severe subsidence problems. Here, the initial borehole site investigation for the road was supplemented by resistivity tomography studies. The roadway was reinforced with two layers of tensile membrane material within the earth embankment. This will prevent dangerous catastrophic collapse, but will allow sagging to show where problems exist. The River Ure Bridge was constructed across an area of subsidence pipes filled with alluvial deposits. It was built with extra strength, larger than normal foundations. If one pier fails, the bridge is designed for adjacent arches to span the gap without collapse. The bridge piers are also fitted with electronic load monitoring to warn of failure. In the Midlands area of England, road construction over Triassic gypsum has required a phase of ground improvement on the Derby Southern Bypass. Here, the gypsum caps a hill where it was formerly mined; it dips through a karstic dissolution zone into an area of complete dissolution and collapse. The road and an associated flyover were built across these ground conditions. A major grouting program before the earthworks began treated the cavities in the mine workings and the cavernous margin of the gypsum mass. Within the karstic dissolution zone, gypsum blocks and cavities along the route were identified by conductivity and resistivity geophysical surveys, excavated and backfilled. In the areas of complete dissolution and collapse, the road foundation was strengthened with vibrated stone columns and a reinforced concrete road deck was used
Radio Continuum and Recombination Line Study of UC HII Regions with Extended Envelopes
- Author
- Publication venue
- 'University of Chicago Press'
- Publication date
- 25/10/2000
- Field of study
We have carried out 21 cm radio continuum observations of 16 UC HII regions
using the VLA (D-array) in search of associated extended emission. We have also
observed H76α recombination line towards all the sources and
He76α line at the positions with strong H76α line emission. The
UC HII regions have simple morphologies and large (>10) ratios of single-dish
to VLA fluxes. Extended emission was detected towards all the sources. The
extended emission consists of one to several compact components and a diffuse
extended envelope. All the UC HII regions but two are located in the compact
components, where the UC HII regions always correspond to their peaks. The
compact components with UC HII regions are usually smaller and denser than
those without UC HII regions. Our recombination line observations indicate that
the ultracompact, compact, and extended components are physically associated.
The UC HII regions and their associated compact components are likely to be
ionized by the same sources on the basis of the morphological relations
mentioned above. This suggests that almost all of the observed UC HII regions
are not `real' UC HII regions and that their actual ages are much greater than
their dynamical age (<10000 yr). We find that most of simple UC HII regions
previously known have large ratios of single-dish to VLA fluxes, similar to our
sources. Therefore, the `age problem' of UC HII regions does not seem to be as
serious as earlier studies argued. We present a simple model that explains
extended emission around UC HII regions. Some individual sources are discussed.Comment: 29 pages, 28 postscript figures, Accepted for publication in Ap
The influence of air-sea fluxes on atmospheric aerosols during the summer monsoon over the tropical Indian Ocean
- Author
- Publication venue
- 'Wiley'
- Publication date
- 16/01/2018
- Field of study
During the summer monsoon, the western tropical Indian Ocean is predicted to be a hot spot for dimethylsulfide emissions, the major marine sulfur source to the atmosphere, and an important aerosol precursor. Other aerosol relevant fluxes, such as isoprene and sea spray, should also be enhanced, due to the steady strong winds during the monsoon. Marine air masses dominate the area during the summer monsoon, excluding the influence of continentally derived pollutants. During the SO234-2/235 cruise in the western tropical Indian Ocean from July to August 2014, directly measured eddy covariance DMS fluxes confirm that the area is a large source of sulfur to the atmosphere (cruise average 9.1 μmol m−2 d−1). The directly measured fluxes, as well as computed isoprene and sea spray fluxes, were combined with FLEXPART backward and forward trajectories to track the emissions in space and time. The fluxes show a significant positive correlation with aerosol data from the Terra and Suomi-NPP satellites, indicating a local influence of marine emissions on atmospheric aerosol numbers
Reduced dietary salt for the prevention of cardiovascular disease.
- Author
- Alderman
- Allender
- Alli
- Appel
- Appel
- Appel
- Arroll
- Bahnson
- Bentley
- Borhani
- Brown
- Cappuccio
- Chang
- Cook
- Costa
- Elliot
- Elliott
- Espeland
- Forster
- He
- He
- He
- Hebert
- Higgins
- Hollis
- Hooper
- Hunt
- Jeffery
- Jeffery
- Jürgens
- Knuist
- Koopman
- Kostis
- Lasser
- Licata
- Mackay
- MacMahon
- McHorney
- Meinert
- Morgan
- Morgan
- Post
- Prudhomme
- Schmid
- Shah
- Silman
- Strazzullo
- Thaler
- Velloso
- Whelton
- Whelton
- Whelton
- Publication venue
- Cochrane Collaboration
- Publication date
- 01/01/2011
- Field of study
BACKGROUND: An earlier Cochrane review of dietary advice identified insufficient evidence to assess effects of reduced salt intake on mortality or cardiovascular events. OBJECTIVES: 1. To assess the long term effects of interventions aimed at reducing dietary salt on mortality and cardiovascular morbidity.2. To investigate whether blood pressure reduction is an explanatory factor in any effect of such dietary interventions on mortality and cardiovascular outcomes. SEARCH STRATEGY: The Cochrane Library (CENTRAL, Health Technology Assessment (HTA) and Database of Abstracts of Reviews of Effect (DARE)), MEDLINE, EMBASE, CINAHL and PsycInfo were searched through to October 2008. References of included studies and reviews were also checked. No language restrictions were applied. SELECTION CRITERIA: Trials fulfilled the following criteria: (1) randomised with follow up of at least six-months, (2) intervention was reduced dietary salt (restricted salt dietary intervention or advice to reduce salt intake), (3) adults, (4) mortality or cardiovascular morbidity data was available. Two reviewers independently assessed whether studies met these criteria. DATA COLLECTION AND ANALYSIS: Data extraction and study validity were compiled by a single reviewer, and checked by a second. Authors were contacted where possible to obtain missing information. Events were extracted and relative risks (RRs) and 95% CIs calculated. MAIN RESULTS: Seven studies (including 6,489 participants) met the inclusion criteria - three in normotensives (n=3518), two in hypertensives (n=758), one in a mixed population of normo- and hypertensives (n=1981) and one in heart failure (n=232) with end of trial follow-up of seven to 36 months and longest observational follow up (after trial end) to 12.7 yrs. Relative risks for all cause mortality in normotensives (end of trial RR 0.67, 95% CI: 0.40 to 1.12, 60 deaths; longest follow up RR 0.90, 95% CI: 0.58 to 1.40, 79 deaths) and hypertensives (end of trial RR 0.97, 95% CI: 0.83 to 1.13, 513 deaths; longest follow up RR 0.96, 95% CI; 0.83 to 1.11, 565 deaths) showed no strong evidence of any effect of salt reduction. Cardiovascular morbidity in people with normal blood pressure (longest follow-up RR 0.71, 95% CI: 0.42 to 1.20, 200 events) or raised blood pressure at baseline (end of trial RR 0.84, 95% CI: 0.57 to 1.23, 93 events) also showed no strong evidence of benefit. Salt restriction increased the risk of all-cause death in those with congestive heart failure (end of trial relative risk: 2.59, 95% 1.04 to 6.44, 21 deaths). We found no information on participants health-related quality of life. AUTHORS' CONCLUSIONS: Despite collating more event data than previous systematic reviews of randomised controlled trials (665 deaths in some 6,250 participants), there is still insufficient power to exclude clinically important effects of reduced dietary salt on mortality or cardiovascular morbidity in normotensive or hypertensive populations. Further RCT evidence is needed to confirm whether restriction of sodium is harmful for people with heart failure. Our estimates of benefits from dietary salt restriction are consistent with the predicted small effects on clinical events attributable to the small blood pressure reduction achieved
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- 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
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- Berta P
- Bertella C
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
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- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
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- Bingul A
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- Bitadze A
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- 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
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- 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
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- Bruni LS
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- Bruschi M
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- Buchholz P
- Buckley AG
- Budagov IA
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- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
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- 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
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- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
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- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
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- Camelia EA
- Cameron D
- Camincher C
- Campana S
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- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cantero J
- Cao T
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- Cardillo F
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- Carli I
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- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
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- Carra S
- Carter JWS
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
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- Cavasinni V
- Celebi E
- Cerda Alberich L
- Cerny K
- Cerqueira AS
- Cerri A
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- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
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- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chau CC
- Che S
- Chekanov S
- Chekulaev S
- Chelkov GA
- Chen B
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- Chen X
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
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- Chomont AR
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- Chow YS
- Chu MC
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- Chudoba J
- Chwastowski JJ
- Chytka L
- Cieri D
- Ciesla KM
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
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- Ciungu BM
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- Constantinescu S
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- Cooper-Sarkar AM
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- Cormier KJR
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
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- D'Amico V
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- da Costa JBG
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- Da Via C
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- Dachs F
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- Dahbi S
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- Damazio DO
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- Dandoy JR
- Daneri MF
- Dann NS
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- Dattagupta A
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- de Jong P
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- de Lima DEF
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- De Regie JBDV
- de Renstrom PAB
- De Sa RCL
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- De Sousa MJDCS
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- Debenedetti C
- Dedovich D
- Deiana AM
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- Deliot F
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- Dell'Acqua A
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- Delmastro M
- Delporte C
- Delsart PA
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- Demers S
- Demichev M
- Demontigny G
- Denisov SP
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- Derue F
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- Deterre C
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- Devesa MR
- Deviveiros PO
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- Di Ciaccio A
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- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Gregorio G
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- Di Nardo R
- Di Petrillo KF
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- Dias FA
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- Diehl EB
- Dietrich J
- Dimitrievska A
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- Dubinin F
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- Dubreuil A
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- Duckeck G
- Ducourthial A
- Ducu OA
- Duda D
- Dudarev A
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- Duelsen C
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- Duffeld EM
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- Epland MB
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- Zhemchugov A
- Zheng Z
- Zhong D
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- 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 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Search for chargino-neutralino production with mass splittings near the electroweak scale in three-lepton final states in √s=13 TeV pp collisions with the ATLAS detector
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- Zou R.
- Zu Theenhausen H. Meyer
- Zwalinski L.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 28/05/2019
- Field of study
A search for supersymmetry through the pair production of electroweakinos with mass splittings near the electroweak scale and decaying via on-shell W and Z bosons is presented for a three-lepton final state. The analyzed proton-proton collision data taken at a center-of-mass energy of √s=13 TeV were collected between 2015 and 2018 by the ATLAS experiment at the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. A search, emulating the recursive jigsaw reconstruction technique with easily reproducible laboratory-frame variables, is performed. The two excesses observed in the 2015–2016 data recursive jigsaw analysis in the low-mass three-lepton phase space are reproduced. Results with the full data set are in agreement with the Standard Model expectations. They are interpreted to set exclusion limits at the 95% confidence level on simplified models of chargino-neutralino pair production for masses up to 345 GeV
Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at √s=8 TeV with the ATLAS detector
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- Maxfield SJ
- Maximov DA
- Mazini R
- Maznas I
- Mazza SM
- Mc Fadden NC
- Mc Goldrick G
- Mc Kee SP
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- McCarthy RL
- McCarthy TG
- McClymont LI
- McDonald EF
- Mcfayden JA
- Mchedlidze G
- McMahon SJ
- McNamara PC
- McPherson RA
- Meehan S
- Megy TJ
- Mehlhase S
- Mehta A
- Meideck T
- Meier K
- Meirose B
- Melini D
- Mellenthin JD
- Melo M
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- Meng XT
- Mengarelli A
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- Merino JL
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- Messina A
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- Milov A
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- Minami Y
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- Ming Y
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- Mitsou VA
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- Mizukami A
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- Morgenstern S
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- Nechaeva PY
- Nedden MZ
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- Nitsche I
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- Noguchi Y
- Nomachi M
- Nomidis I
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- Novgorodova O
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- Nurse E
- Nuti F
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- Obermann T
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- Ohm CC
- Ohman H
- Oide H
- Okawa H
- Okumura Y
- Okuyama T
- Olariu A
- Oleiro Seabra LF
- Olszewski A
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- Oreglia MJ
- Oren Y
- Orestano D
- Orlando N
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- Ortiz NGG
- Osculati B
- Ospanov R
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- Otono H
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- Ouraou A
- Oussoren KP
- Outschoorn VIM
- Ouyang Q
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- Pacheco Pages A
- Padilla Aranda C
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- Paige F
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- Palazzo S
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- Panagoulias I
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- Papageorgiou K
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- Pastor ET
- Pastore F
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- Peralva BS
- Perego MM
- Perepelitsa DV
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- Petersen BA
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- Pezoa R
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- Pianori E
- Picazio A
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- Pickering MA
- Piegaia R
- Pilcher JE
- Pilkington AD
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- Pino SAO
- Pirumov H
- Pitt M
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- Plotnikova E
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- Poley A
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- Polifka R
- Polini A
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- Polychronakos V
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- Ponomarenko D
- Pontecorvo L
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- Popeneciu GA
- Poppleton A
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- Potamianos K
- Potrap IN
- Potter CJ
- Poulard G
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- Poveda J
- Pralavorio P
- Pranko A
- Prell S
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- Price LE
- Primavera M
- Prince S
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Puri A
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- Qin G
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- Queitsch-Maitland M
- Quilty D
- Raddum S
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- Radhakrishnan SK
- Radloff P
- Rados P
- Ragusa F
- Rahal G
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- Rashid T
- Raspopov S
- Ratti MG
- Rauch DM
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- Ravinovich I
- Rawling JH
- Raymond M
- Read AL
- Readioff NP
- Reale M
- Rebuzzi DM
- Redelbach A
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- Reiss A
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- Resconi S
- Resseguie ED
- Rettie S
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- Rezanova OL
- Reznicek P
- Rezvani R
- Richter R
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- Rieger J
- Rifki O
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- Rimoldi A
- Rimoldi M
- Rinaldi L
- Ripellino G
- Ristic B
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
- Rizzi C
- Roberts RT
- Robertson SH
- Robichaud-Veronneau A
- Robinson D
- Robinson JEM
- Robson A
- Rocco E
- Roda C
- Rodina Y
- Rodriguez Bosca S
- Rodriguez Perez A
- Rodriguez Rodriguez D
- Rodriguez LP
- Roe S
- Rogan CS
- Rohne O
- Roloff J
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- Rosien N-A
- Rossi E
- Rossi LP
- Rosten JHN
- Rosten R
- Rotaru M
- Roth I
- Rothberg J
- Rousseau D
- Rozanov A
- Rozen Y
- Ruan X
- Rubbo F
- Ruehr F
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rutherfoord JP
- Ruthmann N
- Ryabov YF
- Rybar M
- Rybkin G
- Ryu S
- Ryzhov A
- Rzehorz GF
- Saadi DS
- Saavedra AF
- Sabato G
- Sacerdoti S
- Sadrozinski HF-W
- Sadykov R
- Saez SMR
- Saha P
- Sahinsoy M
- Saimpert M
- Saito M
- Saito T
- Sakamoto H
- Sakurai Y
- Salamanna G
- Salazar Loyola JE
- Salek D
- Salihagic D
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez Martinez V
- Sanchez CAS
- Sanchez FJM
- Sanchez J
- Sandaker H
- Sandbach RL
- Sander CO
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sansoni A
- Santoni C
- Santonico R
- Santos H
- Santurio EV
- Sapronov A
- Saraiva JG
- Sarrazin B
- Sasaki O
- Sato K
- Sauvan E
- Savage G
- Savard P
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- Sawyer C
- Sawyer L
- Saxon J
- Sbarra C
- Sbrizzi A
- Scanlon T
- Scannicchio DA
- Scarcella M
- Scarfone V
- Schaarschmidt J
- Schacht P
- Schachtner BM
- Schaefer D
- Schaefer L
- Schaefer R
- Schaefer U
- Schaeffer J
- Schaepe S
- Schaetzel S
- Schaffer AC
- Schaile D
- Schamberger RD
- Scharf V
- Schegelsky VA
- Scheirich D
- Schernau M
- Schiavi C
- Schier S
- Schildgen LK
- Schillo C
- Schioppa M
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder TV
- Schuh N
- Schulte A
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Searcy J
- Seema P
- Seidel SC
- Seiden A
- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Semprini-Cesari N
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shaikh NW
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shehu CY
- Shen Y
- Sherafati N
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet MJ
- Shojaii S
- Shope DR
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
- Sickles AM
- Sidebo PE
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silverstein SB
- Simak V
- Simic L
- Simion S
- Simioni E
- Simmons B
- Simon M
- Sinervo P
- Sinev NB
- Sioli M
- Siragusa G
- Siral I
- Sivoklokov SY
- Sjolin J
- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Sokhrannyi G
- Solar M
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sopczak A
- Sosa D
- Sotiropoulou CL
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spettel F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spousta M
- Stabile A
- Stamen R
- Stamm S
- Stanecka E
- Stanek RW
- Stanescu C
- Stanitzki MM
- Stapf BS
- Stapnes S
- Starchenko EA
- Stark GH
- Stark J
- Stark SH
- Staroba P
- Starovoitov P
- Starz S
- Staszewski R
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stewart GA
- Stockton MC
- Stoebe M
- Stoicea G
- Stolte P
- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Suchek S
- Sugaya Y
- Suk M
- Sulin VV
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
- Takai H
- Takashima R
- Takasugi EH
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tanaka J
- Tanaka M
- Tanaka R
- Tanaka S
- Tanioka R
- Tannenwald BB
- Tapia Araya S
- Tapprogge S
- Tarem S
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor AC
- Taylor GN
- Taylor PTE
- Taylor W
- Tehrani FS
- Teixeira-Dias P
- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Theenhausen HMZ
- Theveneaux-Pelzer T
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson PD
- Thomsen LA
- Thomson E
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Todome K
- Todorova-Nova S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
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- Tompkins L
- Toms K
- Tong B
- Tornambe P
- Toro RC
- Torrence E
- Torres H
- Torres RET
- Toth J
- Touchard F
- Tovey DR
- Treado CJ
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- Truong L
- Trzebinski M
- Trzupek A
- Tsang KW
- Tseng JC-L
- Tsiareshka PV
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsui KM
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turgeman D
- Turra R
- Tuts PM
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Valderanis C
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallier A
- Valls Ferrer JA
- Van Den Wollenberg W
- van der Graaf H
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez JGP
- Veatch J
- Veeraraghavan V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Verzini MJA
- Vetterli MC
- Viaux Maira N
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
- von der Schmitt H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Walls FMG
- Wang C
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang Q
- Wang R
- Wang SM
- Wang T
- Wang W
- Wang W
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
- Watkins PM
- Watson AT
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb AF
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- Weber MS
- Weber SA
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Werner P
- Wessels M
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong KHY
- Wong VWS
- Worm SD
- Wosiek BK
- Wotschack J
- Wozniak KW
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamatani M
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of √s=8 TeV is presented. The results are based on an integrated luminosity of 20.2 fb−1 recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying |ηγ|40GeV and EγT,2>30 GeV for the two leading photons ordered in transverse energy produced in the interaction. The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is 16.8 ± 0.8 pb . The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%
Measurement of the cross section for inclusive isolated-photon production in pp collisions at √s=13TeV using the ATLAS detector
- Author
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- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Yildiz HD
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- Zakharchuk N
- Zalieckas J
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- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
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- Zenis T
- Zerwas D
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- Zhao Z
- Zhemchugov A
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
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- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13TeVis studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2fb−1. The cross section is measured as a function of the photon transverse energy above 125GeVin different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data
Search for the direct production of charginos and neutralinos in final states with tau leptons in √s=13 TeV collisions with the ATLAS detector
- Author
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- Aad G
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- Abdinov O
- Abeloos B
- Abidi SH
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- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
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- Zemaityte G
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- Zeng JC
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- Zhemchugov A
- Zhou B
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
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- Zobernig G
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- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fb−1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ˜χ+1 ˜χ−1 pair production and of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the ˜ τL state is set to be halfway between the masses of the ˜χ±1 and the ˜χ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ˜χ+1 ˜χ−1 for a massless ˜χ01. Common ˜χ±1 and ˜χ02 masses up to 760 GeV are excluded in the case of production of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 assuming a massless ˜χ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the ˜χ±1 and the ˜χ01 are also studied by varying the ˜ τL mass between the masses of the ˜χ±1 and the ˜χ01
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