320 research outputs found
Estimation of Fish Biomass Using Environmental DNA
- Author
- A Valentini
- CL Jerde
- CS Goldberg
- GF Ficetola
- GG Mittelbach
- H Akaike
- Hideyuki Doi
- Hiroki Yamanaka
- J Person-Le Ruyet
- J Roberts
- Jack Anthony Gilbert
- JE Titus
- K Andersen
- K Mabuchi
- K Matsui
- KP Burnham
- L Zambrano
- L Zambrano
- M Begon
- MY Engelsma
- RG Wetzel
- SA Miller
- T Dejean
- T Minamoto
- T Minamoto
- T Minamoto
- T Takahara
- Teruhiko Takahara
- TK Pitt
- TL Beitinger
- Toshifumi Minamoto
- V Barus
- WN Venables
- Zen'ichiro Kawabata
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
Environmental DNA (eDNA) from aquatic vertebrates has recently been used to estimate the presence of a species. We hypothesized that fish release DNA into the water at a rate commensurate with their biomass. Thus, the concentration of eDNA of a target species may be used to estimate the species biomass. We developed an eDNA method to estimate the biomass of common carp (Cyprinus carpio L.) using laboratory and field experiments. In the aquarium, the concentration of eDNA changed initially, but reached an equilibrium after 6 days. Temperature had no effect on eDNA concentrations in aquaria. The concentration of eDNA was positively correlated with carp biomass in both aquaria and experimental ponds. We used this method to estimate the biomass and distribution of carp in a natural freshwater lagoon. We demonstrated that the distribution of carp eDNA concentration was explained by water temperature. Our results suggest that biomass data estimated from eDNA concentration reflects the potential distribution of common carp in the natural environment. Measuring eDNA concentration offers a non-invasive, simple, and rapid method for estimating biomass. This method could inform management plans for the conservation of ecosystems
Phase I Study of Safety and Immunogenicity of an Escherichia coli-Derived Recombinant Protective Antigen (rPA) Vaccine to Prevent Anthrax in Adults
- Author
- Anita Gillis
- BE Ivins
- BE Ivins
- Bruce K. Brown
- CP Quinn
- CP Quinn
- David Joseph Diemert
- Deborah Birx
- DL Doolan
- FC Belton
- GJ Gorse
- GJ Gorse
- JA Young
- JD Campbell
- Josephine Cox
- JS Allen
- Karen Metcalfe
- Kelly T. McKee
- Lindsay Wieczorek
- Mark Milazzo
- Mary Marovich
- Merlin L. Robb
- ML Pitt
- MT Niu
- PC Turnbull
- PF Fellows
- PR Pittman
- PS Brachman
- Raburn M. Mallory
- S Ratto-Kim
- S Reuveny
- SF Little
- Tanya Santelli Antonille
- Thomas C. VanCott
- TK Zink
- Victoria R. Polonis
- WA Keitel
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
The fatal disease caused by Bacillus anthracis is preventable with a prophylactic vaccine. The currently available anthrax vaccine requires a lengthy immunization schedule, and simpler and more immunogenic options for protection against anthrax are a priority for development. In this report we describe a phase I clinical trial testing the safety and immunogenicity of an anthrax vaccine using recombinant Escherichia coli-derived, B. anthracis protective antigen (rPA).A total of 73 healthy adults ages 18-40 were enrolled and 67 received 2 injections separated by 4 weeks of either buffered saline placebo, or rPA formulated with or without 704 ”g/ml AlhydrogelŸ adjuvant in increasing doses (5, 25, 50, 100 ”g) of rPA. Participants were followed for one year and safety and immunologic data were assessed. Tenderness and warmth were the most common post-injection site reactions. No serious adverse events related to the vaccine were observed. The most robust humoral immune responses were observed in subjects receiving 50 ”g of rPA formulated with AlhydrogelŸ with a geometric mean concentration of anti-rPA IgG antibodies of 283 ”g/ml and a toxin neutralizing geometric 50% reciprocal geometric mean titer of 1061. The highest lymphoproliferative peak cellular response (median Lymphocyte Stimulation Index of 29) was observed in the group receiving 25 ”g AlhydrogelŸ-formulated rPA.The vaccine was safe, well tolerated and stimulated a robust humoral and cellular response after two doses.ClinicalTrials.gov NCT00057525
Monosodium urate crystals promote innate anti-mycobacterial immunity and improve BCG efficacy as a vaccine against tuberculosis
- Author
- AC Hesseling
- BM Babior
- C Conforti-Andreoni
- CF von Reyn
- CJ Chen
- DB Young
- DE Hu
- DE Hu
- E Greco
- E Greco
- Emanuela Greco
- F Martinon
- F Martinon
- F Martinon
- Francesco Taus
- Giovanni Delogu
- I Sakamaki
- Ivana Palucci
- J Kleinnijenhuis
- J Quintin
- J Quintin
- JD Bieber
- JM Pitt
- JM Rybicka
- K Pethe
- KD Mayer-Barber
- KL Rock
- M Kool
- M Sali
- Marilina B. Santucci
- Matteo Morandi
- Maurizio Fraziano
- Noemi Poerio
- P Desaulniers
- P Nunes
- Roberto Nisini
- S Abramson
- S Sturgill-Koszycki
- S Swaminathan
- Sabrina Mariotti
- Thomas Jens Scriba
- TK Mak
- XJ Ma
- Y Arai
- Y Shi
- Y Shi
- Y Zhang
- ZA Malik
- Publication venue
- Publication date
- 01/01/2015
- Field of study
A safer and more effective anti-Tuberculosis vaccine is still an urgent need. We probed the effects of monosodium urate crystals (MSU) on innate immunity to improve the Bacille Calmette-Guerin (BCG) vaccination. Results showed that in vitro MSU cause an enduring macrophage stimulation of the anti-mycobacterial response, measured as intracellular killing, ROS production and phagolysosome maturation. The contribution of MSU to anti-mycobacterial activity was also shown in vivo. Mice vaccinated in the presence of MSU showed a lower number of BCG in lymph nodes draining the vaccine inoculation site, in comparison to mice vaccinated without MSU. Lastly, we showed that MSU improved the efficacy of BCG vaccination in mice infected with Mycobacterium tuberculosis (MTB), measured in terms of lung and spleen MTB burden. These results demonstrate that the use of MSU as adjuvant may represent a novel strategy to enhance the efficacy of BCG vaccination
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at sâ=8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- 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
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- 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
- Angelozzi I
- 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
- Araque JP
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Baas A
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bannoura AAE
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Barnovska Z
- 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
- Battaglia M
- Battistin M
- Bauer F
- Bawa HS
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
- Becker S
- Beckingham M
- Becot C
- 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
- 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
- Beringer J
- Bernard C
- Bernat P
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertsche D
- Besana MI
- Besjes GJ
- Bessidskaia O
- Bessner MF
- Besson N
- Betancourt C
- Bethke S
- Bhimji W
- Bianchi RM
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- Bieniek SP
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- Biglietti M
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- Blanchard J-B
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- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boddy CR
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- Boeriu OEV
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- Bogdanchikov AG
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- Bortolotto V
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- Caminal Armadans R
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- da Costa JBG
- Da Costa JGPF
- Da Cunha Sargedas De Sousa MJ
- Da Via C
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- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fbâ1 of protonâproton collision data at âs = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via tËâtÏË01 or tËâ bÏ˱1 âbW(â)ÏË01 , where ÏË01 (Ï˱1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of tË â tÏË01 . For a branching fraction of 100%, top squark masses in the range 270â645 GeV are excluded for ÏË01 masses below 30 GeV. For a branching fraction of 50% to either tË â tÏË01 or tË â bÏ˱1 , and assuming the Ï˱1 mass to be twice the ÏË01 mass, top squark masses in the range 250â550 GeV are excluded for ÏË01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at âs=8TeV
- Author
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- Rosenthal O
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- Rossi LP
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- Royon CR
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- Rozen Y
- Ruan X
- Rubbo F
- Rubinskiy I
- Rud VI
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- Rudolph MS
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- Rurikova Z
- Rusakovich NA
- Ruschke A
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- Schorlemmer ALS
- Schott M
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- Schramm S
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- Schroeder TV
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- Schultz-Coulon H-C
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- Schune P
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- Schwartzman A
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- Schwemling P
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- Sekula SJ
- Selbach KE
- Seliverstov DM
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- Serfon C
- Serin L
- Serkin L
- Serre T
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shamim M
- Shan LY
- Shang R
- Shank JT
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- Shatalov PB
- Shaw K
- Shehu CY
- Sherwood P
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- Shimizu S
- Shimmin CO
- Shimojima M
- Shiyakova M
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- Shochet MJ
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- Sinev NB
- Sipica V
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjoelin J
- Sjursen TB
- Skottowe HP
- Skovpen KY
- Skubic P
- Slater M
- Slavicek T
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith KM
- Smizanska M
- Smolek K
- Snesarev AA
- Snidero G
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Solans CA
- Solar M
- Solc J
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Song HY
- Soni N
- Sood A
- Sopczak A
- Sopko B
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- Sorin V
- Sosebee M
- Soualah R
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- Soukharev AM
- South D
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- Spreitzer T
- Spurlock B
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- Staerz S
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- Stanecka E
- Stanek RW
- Stanescu C
- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Stavina P
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
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- Stonjek S
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- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strandlie A
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- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Svatos M
- Swedish S
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
- Taccini C
- Tackmann K
- Taenzer J
- Taffard A
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- Taiblum N
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tam JYC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tannenwald BB
- Tannoury N
- Tapprogge S
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
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- Tashiro T
- Tassi E
- Tayalati Y
- Taylor FE
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- Teoh JJ
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- Terzo S
- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thomas JP
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- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thompson RJ
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
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- Tiouchichine E
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- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
- Tolley E
- Tomlinson L
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- Trigger IM
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- Tripiana MF
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- Trocme B
- Troncon C
- Trottier-McDonald M
- Trovatelli M
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- Trzebinski M
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- Tsarouchas C
- Tseng JC-L
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman I
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Uchida K
- Ueda I
- Ueno R
- Ughetto M
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urbaniec D
- Urquijo P
- Usai G
- Usanova A
- Vacavant L
- Vacek V
- Vachon B
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallecorsa S
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- Van Der Deijl PC
- van der Geer R
- van der Graaf H
- Van Der Leeuw R
- van der Ster D
- Van Eldik N
- Van Gemmeren P
- van Huysduynen LH
- Van Nieuwkoop J
- van Vulpen I
- Van Woerden MC
- Vanadia M
- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloso F
- Velz T
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Verzini MJA
- Vest A
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigne R
- Villa M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Virzi J
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuanh T
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
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- Walkowiak W
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- Walls FMG
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- Wanotayaroj C
- Warburton A
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- Washbrook A
- Wasicki C
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- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weigell P
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
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- Werner P
- Wessels M
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- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilkens HG
- Will JZ
- Williams HH
- Williams S
- Willis C
- Willocq S
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- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wittig T
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wright M
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wyatt TR
- Wynne BM
- Xella S
- Xiao M
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamada M
- Yamaguchi H
- Yamaguchi Y
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- 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
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fbâ1of data collected in protonâproton collisions at âs=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Biomass of Scyphozoan Jellyfish, and Its Spatial Association with 0-Group Fish in the Barents Sea
- Author
- A Hylen
- A Roohi
- AC Utne-Palm
- AJ Richardson
- Aleksandr Trofimov
- B Ă dlandsvik
- CE Mills
- CP Lynam
- CP Lynam
- CP Lynam
- CP Lynam
- CP Lynam
- D Pauly
- Daniel Howell
- DB Spangenberg
- Dmitry Prozorkevich
- DV Naumov
- DĂ Hjermann
- E Eriksen
- E Eriksen
- E Eriksen
- E Eriksen
- E Johannesen
- EA Zelickman
- EA Zelickman
- EH Hallfredsson
- EL Orlova
- Elena Eriksen
- F Gröndahl
- FAO
- FS Russell
- G Ottersen
- G Schneider
- G SĂŠtersdal
- GE DingsĂžr
- GM Daskalov
- Graeme Clive Hays
- H GjĂžsĂŠter
- H Loeng
- ICES
- ICES
- ICES
- J Hamre
- JDR Houghton
- JE Purcell
- JE Purcell
- JE Purcell
- JE Purcell
- JE Purcell
- JE Purcell
- JE Purcell
- JE Stiansen
- KA Pitt
- KHP Stromberg
- KT Frank
- MKS Lilley
- MN Arai
- NA Arai
- O Lindahl
- OA Bergstad
- P Dalpadado
- P Dalpadado
- R Ingvaldsen
- R Mansueti
- RD Brodeur
- RD Brodeur
- RH Brewer
- S Hay
- S Hay
- S Holst
- SN Wood
- T Kogovsek
- TA SĂžrnes
- TK Doyle
- V Ozhigin
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
An 0-group fish survey is conducted annually in the Barents Sea in order to estimate fish population abundance. Data on jellyfish by-catch have been recorded since 1980, although this dataset has never been analysed. In recent years, however, the ecological importance of jellyfish medusae has become widely recognized. In this paper the biomass of jellyfish (medusae) in 0â60 m depths is calculated for the period 1980â2010. During this period the climate changed from cold to warm, and changes in zooplankton and fish distribution and abundance were observed. This paper discusses the less well known ecosystem component; jellyfish medusae within the Phylum Cnidaria, and their spatial and temporal variation. The long term average was ca. 9Ă108 kg, with some years showing biomasses in excess of 5Ă109 kg. The biomasses were low during 1980s, increased during 1990s, and were highest in early 2000s with a subsequent decline. The bulk of the jellyfish were observed in the central parts of the Barents Sea, which is a core area for most 0-group fishes. Jellyfish were associated with haddock in the western area, with haddock and herring in the central and coastal area, and with capelin in the northern area of the Barents Sea. The jellyfish were present in the temperature interval 1°C<T<10°C, with peak densities at ca. 5.5°C, and the greatest proportion of the jellyfish occurring between 4.0â7.0°C. It seems that the ongoing warming trend may be favourable for Barents Sea jellyfish medusae; however their biomass has showed a recent moderate decline during years with record high temperatures in the Barents Sea. Jellyfish are undoubtedly an important component of the Barents Sea ecosystem, and the data presented here represent the best summary of jellyfish biomass and distribution yet published for the region
Measurement of the transverse polarization of Î and ÎÂŻ hyperons produced in proton-proton collisions at âs=7ââTeV using the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- 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
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- 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
- Angelozzi I
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- Anghinolfi F
- Anh TV
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- Arabidze G
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- Argyropoulos S
- Arik M
- Armbruster AJ
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- Arnal V
- Arnold H
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- Artamonov A
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- Atlay NB
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- Avolio G
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- Baker OK
- Balek P
- Balli F
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- Banerjee S
- Bannoura AAE
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- Zhemchugov A
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- Zobernig G
- Zoccoli A
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2014
- Field of study
The transverse polarization of Î and ÎÂŻ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760ââÎŒbâ1 of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5Ă10â5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is â0.010±0.005(stat)±0.004(syst) for Î and 0.002±0.006(stat)±0.004(syst) for ÎÂŻ. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement
Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
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- Zanzi D
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- Zhemchugov A
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- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5ââfb[superscript â1] of proton-proton collisions data at âs=7ââTeV and 20.3ââfb[superscript â1] at âs=8ââTeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be ÎŒ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4ââGeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be ÎŒ[subscript ggF]=1.32±0.38, ÎŒ[subscript VBF]=0.8±0.7, ÎŒ[subscript WH]=1.0±1.6, ÎŒ[subscript ZH]=0.1[superscript +3.7 subscript â0.1], and ÎŒ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript â1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Global patient outcomes after elective surgery: prospective cohort study in 27 low-, middle- and high-income countries.
- Author
- Ab Majid MA
- Ab Rahman AS
- Ab Rahman R
- Abayasinghe C
- Abbott T
- Abdullah NH
- Abdur-Rahman L
- Abeloos J
- Abernethy C
- Abidin UN
- Abrunhosa A
- Absar M
- Adam S
- Adams D
- Adams G
- Adamson M
- Adekola O
- Adelaja Y
- Ademola A
- Adenekan A
- Adenike O
- Adeolu AA
- Adetoye A
- Adewale B
- Adigun T
- Adolfsson A
- Aflori L
- Africander C
- Afshari A
- Agarwal V
- Agodirin O
- Aguero Vera M
- Aguzzoli C
- Ahmad A
- Ahmad N
- Ahmad T
- Ahmad T
- Ahmad Y
- Ahmed A
- Ahmed J
- Ai Y
- Aignatoaie M
- Aimoniotou-Georgiou E
- Akanmu O
- Akerman N
- Akinwale M
- Akring I
- Al 'Amri K
- Al Anizi M
- Al hussaini S
- Al-Soudaine Y
- Aladin H
- Alagbe-Briggs O
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- Zhao S
- Zhao T
- Zhao W
- Zhao W
- Zhao X
- Zhen J
- Zheng K
- Zheng L
- Zheng T
- Zhong Y
- Zhou C
- Zhou D
- Zhou H
- Zhou H
- Zhou J
- Zhou J
- Zhou J
- Zhou X-J
- Zhu X
- Zhu X
- Zhu Y
- Zhu Z
- Zhuang X
- Zilis G
- Zin NHM
- Zingerle N
- Zingg U
- Zoerner F
- Zonneveldt H
- Zou X
- Zoulamoglou M
- Zsisku L
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/01/2016
- Field of study
BACKGROUND: As global initiatives increase patient access to surgical treatments, there remains a need to understand the adverse effects of surgery and define appropriate levels of perioperative care. METHODS: We designed a prospective international 7-day cohort study of outcomes following elective adult inpatient surgery in 27 countries. The primary outcome was in-hospital complications. Secondary outcomes were death following a complication (failure to rescue) and death in hospital. Process measures were admission to critical care immediately after surgery or to treat a complication and duration of hospital stay. A single definition of critical care was used for all countries. RESULTS: A total of 474 hospitals in 19 high-, 7 middle- and 1 low-income country were included in the primary analysis. Data included 44Â 814 patients with a median hospital stay of 4 (range 2-7) days. A total of 7508 patients (16.8%) developed one or more postoperative complication and 207 died (0.5%). The overall mortality among patients who developed complications was 2.8%. Mortality following complications ranged from 2.4% for pulmonary embolism to 43.9% for cardiac arrest. A total of 4360 (9.7%) patients were admitted to a critical care unit as routine immediately after surgery, of whom 2198 (50.4%) developed a complication, with 105 (2.4%) deaths. A total of 1233 patients (16.4%) were admitted to a critical care unit to treat complications, with 119 (9.7%) deaths. Despite lower baseline risk, outcomes were similar in low- and middle-income compared with high-income countries. CONCLUSIONS: Poor patient outcomes are common after inpatient surgery. Global initiatives to increase access to surgical treatments should also address the need for safe perioperative care. STUDY REGISTRATION: ISRCTN5181700
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- Abdallah J
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- Snidero G
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Solans CA
- Solar M
- Solc J
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Song HY
- Soni N
- Sood A
- Sopczak A
- Sopko B
- Sopko V
- Sorin V
- Sosebee M
- Soualah R
- Soueid P
- Soukharev AM
- South D
- Spagnolo S
- Spano F
- Spearman WR
- Spighi R
- Spigo G
- Spousta M
- Spreitzer T
- Spurlock B
- Staerz S
- Stahlman J
- Stamen R
- Stanecka E
- Stanek RW
- Stanescu C
- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Stavina P
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stern S
- Stewart GA
- Stillings JA
- Stockton MC
- Stoebe M
- Stoicea G
- Stolte P
- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strandlie A
- Strauss E
- Strauss M
- Strizenec P
- Strohmer R
- Strom DM
- Stroynowski R
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Subramania HS
- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Svatos M
- Swedish S
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tam JYC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tani K
- Tannoury N
- Tapprogge S
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tayalati Y
- Taylor FE
- Taylor GN
- Taylor W
- Tehrani FS
- Teischinger FA
- Teixeira-Dias P
- Temming KK
- Ten Kate H
- Teng PK
- Teoh JJ
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
- Tomlinson L
- Tomoto M
- Tompkins L
- Toms K
- Topilin ND
- Toro RC
- Torregrosa EF
- Torrence E
- Torres H
- Torro Pastor E
- Toth J
- Touchard F
- Tovey DR
- Tran HL
- Trefzger T
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Triplett N
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- True P
- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Uchida K
- Ueda I
- Ueno R
- Ughetto M
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Urbaniec D
- Urquijo P
- Usai G
- Usanova A
- Vacavant L
- Vacek V
- Vachon B
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
- Van Der Deijl PC
- Van der Geer R
- Van der Graaf H
- Van der Leeuw R
- Van der Ster D
- van Eldik N
- van Gemmeren P
- van Huysduynen LH
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloso F
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigne R
- Villa M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Virzi J
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
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- Walkowiak W
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- Waller P
- Walls FMG
- Walsh B
- Wang C
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- Wang SM
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- Wanotayaroj C
- Warburton A
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- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
- Watkins PM
- Watson AT
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- Watson MF
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- Waugh BM
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- Webster JS
- Weidberg AR
- Weigell P
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Weng Z
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- Wessels M
- Wetter J
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- White R
- White S
- Whiteson D
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilkens HG
- Will JZ
- Williams HH
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- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wittig T
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wright M
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- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wyatt TR
- Wynne BM
- Xella S
- Xiao M
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamada M
- Yamaguchi H
- Yamaguchi Y
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- 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
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to dielectron or dimuon final states. Results are presented from an analysis of proton-proton (pp) collisions at a center-of-mass energy of 8 TeV corresponding to an integrated luminosity of 20.3ââfbâ1 in the dimuon channel. A narrow resonance with Standard Model Z couplings to fermions is excluded at 95% confidence level for masses less than 2.79 TeV in the dielectron channel, 2.53 TeV in the dimuon channel, and 2.90 TeV in the two channels combined. Limits on other model interpretations are also presented, including a grand-unification model based on the E6 gauge group, Zâ bosons, minimal Z' models, a spin-2 graviton excitation from Randall-Sundrum models, quantum black holes, and a minimal walking technicolor model with a composite Higgs boson
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