547 research outputs found
Shrike predation on the lizard Mesalina adramitana in Qatar; a review of reported reptile and amphibian prey
- Author
- Arias-Balderas SF
- Baecher JA
- Barone R
- Beven G
- Cade TJ
- Carbajal-Marquez RA
- Chapman BR
- Clark HO
- Duncan R
- Ely E
- Esely J
- Fisher WK
- García-Márquez M
- Hernández A
- Hernández A
- Hernández A
- Hernández A
- Herrera-Bravo de Laguna I
- Hill MT
- Hódar JA
- Jensen JB
- Kopij G
- Lemos-Espinal JA
- Lemos-Espinal JA
- Mahrdt CR
- Martín J
- Morelli F
- Necas J
- Nikolov BP
- Olsson V
- Olsson V
- Pedersen L
- Pujol-Buxó E
- Pérez Padilla D
- Quintero-Diaz GE
- Requena-Aznar C
- Schon M
- Tryjanowski P
- Tsingalia HM
- Tyler JD
- Whyte J
- Yao CT
- Publication venue
- 'Hamad bin Khalifa University Press (HBKU Press)'
- Publication date
- 01/01/2015
- Field of study
We report, for the first time, evidence of predation by a shrike (Lanius sp.) on the lizard Mesalina adramitana. This is the first record of predation by shrikes on lizards in Qatar. Whilst we did not directly observe the event, the presence of shrikes in the area and the method of impalement indicate shrikes as the predator. The lizard was found freshly impaled on a palm tree (Phoenix dactylifera), at 150 cm above ground. Bird species of the genus Lanius are well-known predators of lizards, and in arid environments reptiles are likely common prey for these birds. We provide a review of literature concerning predatory events by shrikes on reptiles and amphibians. We suggest inspection of shrubs for animals impaled by shrikes can improve biodiversity inventories, complementing other commonly used methods
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
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- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
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- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
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- Alshehri AA
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- Alviggi MG
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- Thomson E
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- Tisserant S
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- Tolley E
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- Tong B
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- Toro RC
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- Torres RET
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- Tovey DR
- Traeet A
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- Tricoli A
- Trigger IM
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- Trischuk DA
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- Trocme B
- Trofymov A
- Troncon C
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- Tsai F
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- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
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- Tuts PM
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- Tzovara E
- Ucchielli G
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- Ukegawa F
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- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Usai G
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Vale MAB
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Van Daalen TR
- Van Gemmeren P
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vaniachine A
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vazeille F
- Vazquez Furelos D
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi N
- Vera AMR
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Verzini MJA
- Vetterli MC
- Viaux Maira N
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang AZ
- Wang C
- Wang F
- Wang H
- Wang J
- Wang P
- Wang Q
- Wang R
- Wang R-J
- Wang SM
- Wang W
- Wang WT
- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warrack N
- Washbrook A
- Watson AT
- Watson MF
- Watts G
- Waugh BM
- Webb AF
- Webb S
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
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- Xiao X
- Xiotidis I
- Xu D
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- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
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- Yao W-M
- Yap YC
- Yasu Y
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- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
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- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
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- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 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
The role of open abdomen in non-trauma patient : WSES Consensus Paper
- Author
- A Buter
- A Caro
- A Doyon
- A Eriksson
- A Gurrado
- A Hakkiluoto
- A Khan
- A Lambertz
- A Marinis
- A Pavy-Le Traon
- A Reinisch
- A Reite
- A Schachtrupp
- A Truong
- Addison K. May
- AE Salman
- AE Sharrock
- AH Petter-Puchner
- AI Amin
- AJ Fieger
- AK Leppäniemi
- AL Adkins
- AM Cooper
- Andrew Peitzman
- Andrew W. Kirkpatrick
- Ari Leppaniemi
- AT Gentile
- AW Kirkpatrick
- AW Kirkpatrick
- AW Kirkpatrick
- B Chand
- B Collier
- B Emr
- B Kirshtein
- BD Kubiak
- BH Cuthbertson
- BJ Tsuei
- Boris Sakakushev
- BR Bruns
- Bruno M. Pereira
- C Burtin
- C Haddock
- C Manterola
- C Rubenstein
- C Töns
- CA Bertelsen
- CA Ordóñez
- CC Cothren
- CL Hodgson
- CR Voyles
- D Demetriades
- D Demetriades
- D Gönüllü
- D Lattuada
- D Perez
- D Wondberg
- DE Barker
- DH Wittmann
- DH Wittmann
- DJ Mole
- ED Anderson
- EI Lee
- Ernest E. Moore
- Ewen Griffiths
- F Coccolini
- F Ercan
- F Zingales
- FA Robledo
- Fausto Catena
- FE Primus
- Federico Coccolini
- Fikri M. Abu-Zidan
- FJ Verdam
- Francesco Salvetti
- G Al-Khoury
- G Guyatt
- G Hubens
- G Montori
- G Plantefeve
- GE Leber
- George Velmahos
- Gianmariano Marchesi
- Giulia Montori
- GL Brown
- GL Carlson
- GL Carlson
- GS Hedderich
- Gustavo Pereira Fraga
- H Ozguc
- H Plaudis
- HC Santvoort van
- HJ Lin
- I Pliakos
- I Pliakos
- IA Shaikh
- Ignacio Martin-Loeches
- J Bailey
- J Cipolla
- J Horwood
- J Losanoff
- J Wang
- JA García Iñiguez
- JE Losanoff
- Jeffry L. Kashuk
- JH Booth
- JH Patton
- JJ Atema
- JJ Atema
- JJ Choi
- JJ Diaz
- JJ Waele De
- JL Holihan
- JL Martinez
- JL Martinez-Ordaz
- JL Regner
- John E. Mazuski
- JS Paul
- JVT Tilsed
- JW Wilde
- K Bosscha
- K Kritayakirana
- KG Cornwell
- KI Halonen
- Kjetil Soreide
- L López-Quintero
- L Pérez Domínguez
- LA Smith
- LC Rekstad
- LF Hollender
- LG Koniaris
- LJ Moore
- Luca Ansaloni
- M Björck
- M Björck
- M Giner
- M Rao
- M Sartelli
- M Sartelli
- M Sartelli
- M Schein
- M Schein
- M Singer
- M van ‘t Riet
- MA Moya de
- Manu Malbrain
- Marc De Moya
- Marco Ceresoli
- Marja A. Boermeester
- Massimo Sartelli
- MC Byrnes
- MD Zielinski
- MG Besselink
- Michael Sugrue
- Michele Pisano
- Miklosh Bala
- MJ Bradley
- MJ Pommerening
- ML Cheatham
- ML Cheatham
- ML Konstantinovic
- MM Abdelfatah
- MS Herridge
- MS Petrov
- MW Reimer
- N Ginting
- O Ruler van
- OAA Panel
- OM Ramirez
- Osvaldo Chiara
- P Mentula
- P Mentula
- P Nubiola
- P Oetting
- P Padalino
- PA Banks
- PE Marik
- PGR Teixeira
- PH Navsaria
- Philippe Montravers
- PJ Kim
- PT Engels
- Q Huang
- R Hee Van
- R Kafka-Ritsch
- R Kafka-Ritsch
- R Mofidi
- Rao Ivatury
- Raul Coimbra
- RC Dinsmore
- RF Fansler
- RH Fortelny
- Rita Maria Melotti
- Ron Maier
- RR Ivatury
- RR Ivatury
- S Acosta
- S Acosta
- S Dissanaike
- S Ersryd
- S Karmali
- S Prichayudh
- S Richter
- S Saverio Di
- S Saverio Di
- S Sökmen
- S Yegiyants
- SA McClave
- Salomone Di Saverio
- Sandro Rizoli
- SF Badylak
- SJ Mathes
- SK Rasilainen
- SK Rasilainen
- SM Maurice
- Thomas Scalea
- Tino M. Valetti
- TM Polk
- TS Vries Reilingh de
- UA Dietz
- Vanni Agnoletti
- Vladimir Khokha
- Walter Biffl
- WB Brock
- WP Schecter
- Yoram Kluger
- Publication venue
- Publication date
- 01/01/2017
- Field of study
The open abdomen (OA) is defined as intentional decision to leave the fascial edges of the abdomen un-approximated after laparotomy (laparostomy). The abdominal contents are potentially exposed and therefore must be protected with a temporary coverage, which is referred to as temporal abdominal closure (TAC). OA use remains widely debated with many specific details deserving detailed assessment and clarification. To date, in patients with intra-abdominal emergencies, the OA has not been formally endorsed for routine utilization; although, utilization is seemingly increasing. Therefore, the World Society of Emergency Surgery (WSES), Abdominal Compartment Society (WSACS) and the Donegal Research Academy united a worldwide group of experts in an international consensus conference to review and thereafter propose the basis for evidence-directed utilization of OA management in non-trauma emergency surgery and critically ill patients. In addition to utilization recommendations, questions with insufficient evidence urgently requiring future study were identified.Peer reviewe
Multi-messenger observations of a binary neutron star merger
- Author
- Aab A
- Aartsen MG
- Abbott BP
- Abbott R
- Abbott TD
- Abbott TMC
- Abdalla H
- Abe F
- Abeysekara AU
- Abramo LR
- Abramowski A
- Abreu P
- Acernese F
- Acero F
- Ackermann M
- Ackley K
- Ackley K
- Adams C
- Adams J
- Adams SM
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Afrough M
- Agarwal B
- Agathos M
- Agatsuma K
- Aggarwal N
- Aglietta M
- Agliozzo C
- Agudo I
- Aguiar OD
- Aguilar JA
- Aharonian F
- Ahlers M
- Ahrens M
- Aiello L
- Ain A
- Ajith P
- Akras S
- Al Samarai I
- Albert A
- Albert A
- Albuquerque IFM
- Albury JM
- Alcaniz JS
- Alexander KD
- Alfaro R
- Alighieri S Di Serego
- Allam S
- Allekotte I
- Allen B
- Allen G
- Allison J
- Allison JR
- Allocca A
- Almela A
- Altin PA
- Altmann D
- Alvarez C
- Alvarez JD
- Alvarez M Dovale
- Alvarez-Muiz J
- Amati L
- Amato A
- An T
- Ananyeva A
- Anastasi GA
- Anchordoqui L
- Andeen K
- Anderson JP
- Anderson SB
- Anderson T
- Anderson WG
- Andrada B
- Andre M
- Andreoni I
- Andreoni I
- Andringa S
- Angelova SV
- Anghinolfi M
- Angner EO
- Angus CR
- Annis J
- Ansseau I
- Antier S
- Anton G
- Antonelli LA
- Antonelli LA
- Anupama GC
- Aoki K
- Aoki W
- Appert S
- Aptekar RL
- Arai K
- Arakawa M
- Aramo C
- Araya MC
- Arcavi I
- Arceo R
- Ardid M
- Areeda JS
- Aresu G
- Argan A
- Argelles C
- Arnaud N
- Array LWA Long Wavelength
- Array MWA Murchison Widefield
- Arrieta M
- Arsene N
- Arteaga-Velzquez JC
- Artola R
- Arun KG
- Asakura Y
- Asaoka Y
- Ascenzi S
- Ashall C
- Ashley MCB
- Ashton G
- Asorey H
- Assis P
- Ast M
- Aston SM
- Astone P
- Atallah DV
- ATLAS
- Atwood WB
- Aubert J-J
- Aubert P
- Aublin J
- Auffenberg J
- Aufmuth P
- Aulbert C
- AultONeal K
- Austin C
- Avgitas T
- Avila G
- Avila-Alvarez A
- Awad A Kuotb
- Axani S
- Baar S
- Babak S
- Bachetti M
- Backes M
- Bacon P
- Bader MKM
- Badescu AM
- Bae S
- Bagherpour H
- Bai X
- Bailes M
- Baker PT
- Balaceanu A
- Balanutsa PV
- Balasubramanian A
- Balbinot E
- Baldaccini F
- Baldini L
- Ballardin G
- Ballmer SW
- Bally J
- Balzer A
- Banagiri S
- Banerji M
- Bannister KW
- Barayoga JC
- Barbarino C
- Barbato F
- Barber AS
- Barbiellini G
- Barbiellini G
- Barclay SE
- Baret B
- Barish BC
- Barker D
- Barkett K
- Barnard M
- Barnes J
- Barone F
- Barr B
- Barrios-Marti J
- Barron JP
- Barsotti L
- Barsuglia M
- Barta D
- Barthelmy SD
- Bartlett J
- Bartos I
- Barway S
- Barway S
- Barwick SW
- Basa S
- Bassiri R
- Basti A
- Bastieri D
- Batch JC
- Bauer FE
- Bauer FE
- Baum V
- Bawaj M
- Bay R
- Bayley JC
- Bazzan M
- Bazzano A
- Bchele M
- Beardmore AP
- Beardsley A
- Beatty JJ
- Becerril A
- Becherini Y
- Bechtol K
- Becker KH
- Becsy B
- Beer C
- Bejger M
- Belahcene I
- Belhorma B
- Bell AS
- Bellazzini R
- Bellido JA
- Bellm E
- Belmont-Moreno E
- Benetti S
- Benkhali F Ait
- Benoit-Levy A
- BenZvi SY
- Berat C
- Berenji B
- Berge D
- Berger BK
- Berger E
- Bergmann G
- Berisso M Gomez
- Berley D
- Bernal A
- Bernardini E
- Bernardini MG
- Bernhard S
- Bernrhr K
- Bero JJ
- Beroiz M
- Berry CPL
- Bersanetti D
- Bertaina ME
- Bertin E
- Bertin V
- Bertolini A
- Berton M
- Bertou X
- Bessell MS
- Besson DZ
- Beswick R
- Betzwieser J
- Bhagwat S
- Bhalerao V
- Bhandare R
- Bhattacharya D
- Biagi S
- Biermann PL
- Bilenko IA
- Billingsley G
- Billman CR
- Binder G
- Bindig D
- Birch J
- Birney R
- Birnholtz O
- Biscans S
- Biscoveanu S
- Bisht A
- Bissaldi E
- Bissaldi E
- Biteau J
- Bitossi M
- Biwer C
- Bizouard MA
- Blackburn JK
- Blackburn L
- Blackman J
- Blackwell R
- Blaess SG
- Blagorodnova N
- Blair CD
- Blair DG
- Blair RM
- Blanchard P
- Blanco A
- Bland PA
- Blandford RD
- Blaufuss E
- Blazek J
- Bleve C
- Bloemen S
- Bloom ED
- Blot S
- Bock O
- Bode N
- Boer M
- Bogaert G
- Bohacova M
- Bohe A
- Bohm C
- Boisson C
- Bolmont J
- Bond IA
- Bondu F
- Bonifazi C
- Bonilla E
- Bonino R
- Bonnand R
- Bonnefoy S
- Bonoli S
- Booler T
- Boom BA
- Bordas P
- Bork R
- Bormuth R
- Borner M
- Borodai N
- Bos F
- Boschi V
- Bose D
- Bose S
- Boser S
- Bossie K
- Botner O
- Bottacini E
- Bottcher M
- Botti AM
- Botticella MT
- Bouffanais Y
- Bourbeau E
- Bourbeau J
- Bourret S
- Bouwhuis MC
- Bozzi A
- Bozzo E
- Brack J
- Bradaschia C
- Bradascio F
- Brady PR
- Branchesi M
- Brancus I
- Brandt S
- Brau JE
- Braun J
- Braun J
- Bravo O Martinez
- Brayeur L
- Breeveld AA
- Bregeon J
- Bregeon J
- Brenzke M
- Bretz H-P
- Bretz T
- Briant T
- Bridgeman A
- Briechle FL
- Briggs MS
- Brillet A
- Brinkmann M
- Brisbois C
- Brisson V
- Brnzas H
- Brocato E
- Brockill P
- Broderick JW
- Broida JE
- Bron S
- Brooks AF
- Brooks D
- Brostean-Kaiser J
- Brout D
- Brown DA
- Brown DD
- Brown IS
- Bruijn R
- Brun F
- Brun P
- Brunett S
- Brunner J
- Bruun SH
- Bryan M
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- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
The clinical relevance of oliguria in the critically ill patient : Analysis of a large observational database
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- Field of study
Funding Information: Marc Leone reports receiving consulting fees from Amomed and Aguettant; lecture fees from MSD, Pfizer, Octapharma, 3 M, Aspen, Orion; travel support from LFB; and grant support from PHRC IR and his institution. JLV is the Editor-in-Chief of Critical Care. The other authors declare that they have no relevant financial interests. Publisher Copyright: © 2020 The Author(s). Copyright: Copyright 2020 Elsevier B.V., All rights reserved.Background: Urine output is widely used as one of the criteria for the diagnosis and staging of acute renal failure, but few studies have specifically assessed the role of oliguria as a marker of acute renal failure or outcomes in general intensive care unit (ICU) patients. Using a large multinational database, we therefore evaluated the occurrence of oliguria (defined as a urine output 16 years) patients in the ICON audit who had a urine output measurement on the day of admission were included. To investigate the association between oliguria and mortality, we used a multilevel analysis. Results: Of the 8292 patients included, 2050 (24.7%) were oliguric during the first 24 h of admission. Patients with oliguria on admission who had at least one additional 24-h urine output recorded during their ICU stay (n = 1349) were divided into three groups: transient - oliguria resolved within 48 h after the admission day (n = 390 [28.9%]), prolonged - oliguria resolved > 48 h after the admission day (n = 141 [10.5%]), and permanent - oliguria persisting for the whole ICU stay or again present at the end of the ICU stay (n = 818 [60.6%]). ICU and hospital mortality rates were higher in patients with oliguria than in those without, except for patients with transient oliguria who had significantly lower mortality rates than non-oliguric patients. In multilevel analysis, the need for RRT was associated with a significantly higher risk of death (OR = 1.51 [95% CI 1.19-1.91], p = 0.001), but the presence of oliguria on admission was not (OR = 1.14 [95% CI 0.97-1.34], p = 0.103). Conclusions: Oliguria is common in ICU patients and may have a relatively benign nature if only transient. The duration of oliguria and need for RRT are associated with worse outcome.publishersversionPeer reviewe
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
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- Yildiz HD
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- Zaripovas DR
- Zeissner SV
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- Zeng JC
- Zenin O
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- Zhang Z
- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
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- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aperio Bella L
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
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- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
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- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerradi S
- Zerwas D
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- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou H
- Zhou N
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- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Measurements of W+W−+ ≥ 1 jet production cross-sections in pp collisions at s = 13 TeV with the ATLAS detector
- Author
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- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Abusleme Hoffman AC
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- Zemaityte G
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- Zhang R
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- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou H
- Zhou M
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- Zhu H
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+W− production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fb−1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |�| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+W−+ � 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+W− system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at root s=13 TeV with the ATLAS detector
- Author
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- Abbott B
- Abbott DC
- Abdinov O
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Abraham NL
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- Zhemchugov A
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 13/08/2020
- Field of study
A search for heavy neutral Higgs bosons produced in association with one or two
b
-quarks and decaying to
b
-quark pairs is presented using
27.8
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross section times its branching ratio to
b
¯
b
are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the minimal supersymmetric Standard Model
- …