60 research outputs found
Gene Flow and Hybridization between Numerically Imbalanced Populations of Two Duck Species in the Falkland Islands
- Author
- AC Fowler
- AP Gray
- C Randler
- C Randler
- CDK Bottema
- CL Hubbs
- CL Pruett
- CL Williams
- CN Balakrishnan
- D Posada
- DC Queller
- DE Wolf
- E Anderson
- E Panov
- EM Calkell
- EM McCarthy
- FC Rohwer
- GG Simpson
- HJ Bandelt
- IV Kulikova
- IV Kulikova
- IV Kulikova
- J Hey
- J Mallet
- J Mallet
- J Rozas
- JBS Haldane
- JC Phillips
- JE Mank
- JK Pritchard
- JL Peters
- JL Peters
- JM Pearce
- JM Rhymer
- JM Rhymer
- K Tamura
- Kevin G. McCracken
- KG McCracken
- KG McCracken
- KM Sefc
- KP Johnson
- L Excoffier
- L Schwacke
- LW Hillier
- M Hasegawa
- M Morando
- M Stephens
- MD Carling
- MJ Donnelly
- MV Lomolino
- MW Weller
- MW Weller
- PA Johnsgard
- PL Tubaro
- PR Grant
- PR Grant
- R Frankham
- R Frankham
- RE Kirby
- RE Kirby
- RH MacArthur
- Robert E. Wilson
- RR Hudson
- RW Woods
- SA Sonsthagen
- SE Masta
- TE Dowling
- TE Steeves
- V Grant
- V Muñoz-Fuentes
- Vincent Laudet
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Interspecific hybridization is common in plants and animals, particularly in waterfowl (Anatidae). One factor shown to contribute to hybridization is restricted mate choice, which can occur when two species occur in sympatry but one is rare. The Hubbs principle, or “desperation hypothesis,” states that under such circumstances the rarer species is more likely to mate with heterospecifics. Here we report interspecific hybridization between two waterfowl species that coexist in broad sympatry and mixed flocks throughout southern South America. Speckled teal (Anas flavirostris) and yellow-billed pintails (Anas georgica) are abundant in continental South America, but in the Falkland Islands speckled teal outnumber yellow-billed pintails approximately ten to one. Using eight genetic loci (mtDNA and 7 nuclear introns) coupled with Bayesian assignment tests and relatedness analysis, we identified a speckled teal x yellow-billed pintail F1 hybrid female and her duckling sired by a male speckled teal. Although our sample in the Falkland Islands was small, we failed to identify unequivocal evidence of hybridization or introgression in a much larger sample from Argentina using a three-population “isolation with migration” coalescent analysis. While additional data are needed to determine if this event in the Falkland Islands was a rare singular occurrence, our results provide further support for the “desperation hypothesis,” which states that scarcity in one population and abundance of another will often lead to hybridization
Biodiversity Trends along the Western European Margin
- Author
- A Brandt
- A Brandt
- A Davies
- A Eleftheriou
- A Jensen
- A Künitzer
- A Longhurst
- A Schroeder
- AE Magurran
- AL Middelboe
- ARG Price
- B Hansen
- B Holte
- B Worm
- BE Narayanaswamy
- BE Narayanaswamy
- BH Corliss
- Bhavani E. Narayanaswamy
- BI Sirenko
- BJ Bett
- BJ Bett
- C Arvanitidis
- C Heip
- C Heip
- C Olabarria
- C Olabarria
- CH Greene
- CL Biles
- CLJ Frid
- CT Stuart
- D Piepenburg
- D Raffaelli
- DG Roberts
- DH Cushing
- Dippner
- DOB Jones
- Duffy
- E Bonsdorff
- E Flach
- E Macpherson
- E Thomas
- E Vanden Berghe
- E Verfaillie
- EN Ieno
- F Beuchel
- F Creutzberg
- F Dyer M
- GA Knox
- GCA Duineveld
- Gerard C. A. Duineveld
- GLJ Paterson
- Golikov
- H Deubel
- H Fosså J
- H Hillebrand
- H Hillebrand
- H Neumann
- H Ojaveer
- H Reiss
- H Reiss
- Henning Reiss
- HJ Lindeboom
- HJ Lindeboom
- HL Rees
- I Kröncke
- I Kröncke
- I Kröncke
- I Kröncke
- I Kröncke
- ICES
- IV Polyakov
- J Berge
- J Gröger
- J Hagberg
- J Hall-Spencer
- J Levinton
- J Svavarsson
- J-C Dauvin
- JA Blake
- JA Craeymeersch
- JC Gering
- JD Gage
- JD Gage
- JD Gage
- JD Gage
- JD Gage
- JD Gage
- JE Hewitt
- JE Wollenburg
- JH Brown
- JL Hernandez-Stefanoni
- JL Leichter
- JL Ruesink
- JM Grebmeier
- JM Guinotte
- JM Roberts
- JM Roberts
- JM Węsławski
- JM Węsławski
- JS Gray
- JS Gray
- JW Thomson
- JW Turrell
- Jørgen Berge
- K Frauenheim
- KE Ellingsen
- KF Drinkwater
- KH Dunton
- KJ Gaston
- KL Howell
- KL Smith
- KN Nesis
- KR Clarke
- LA Levin
- M Coll
- M Glémarec
- M Huston
- M Kottelat
- M Sarnthein
- M Solan
- M Solan
- M Steffens
- M Włodarska-Kowalczuk
- MA Rex
- MA Rex
- MA Rex
- MA Rex
- MA Rex
- MarBEF
- Marc S. S. Lavaleye
- MJ Kaiser
- MJ Kaiser
- MJN Bergman
- MK Walker
- MR Willig
- N Maciolek
- NA Anisimova
- O Gauthier
- OW Brude
- P Kuklinski
- PA Tyler
- Paul E. Renaud
- PB Mortensen
- PC Reid
- PC Reid
- PE Renaud
- PE Renaud
- PE Renaud
- PJ Somerfield
- PJD Lambshead
- PJD Lambshead
- PK Dayton
- PK Dayton
- PRO Barnett
- R Callaway
- R Daan
- R Danovaro
- R Danovaro
- R Danovaro
- R Zühlke
- RC Thompson
- RJ Whittaker
- RK Colwell
- RM Warwick
- RM Warwick
- RM Warwick
- RM Warwick
- RR Hessler
- RR Kirby
- RW Blacker
- S Degraer
- S Degraer
- S Jennings
- S Naeem
- S Naeem
- S Rahmstorf
- S Widdicombe
- SE Gass
- SF Thrush
- SH Hurlbert
- Sibuet
- SJ Culver
- SJ Hawkins
- SKJ Cochrane
- SR Palumbi
- Stuart Humphries
- SV Vassilenko
- T Bekkby
- T Brattegard
- T Brattegard
- TJ Sherwin
- TJ Webb
- Torleiv Brattegard
- U Claussen
- U Stein
- V Escaravage
- V Mokievsky
- W Michaelsen
- W Willems
- WG Ambrose Jr
- Y Herman
- YI Galkin
- Å Husebø
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Short-Lived Trace Gases in the Surface Ocean and the Atmosphere
- Author
- A Bouwman
- A Butler
- A Ekdahl
- A Gabric
- A Guenther
- A Karlsson
- A Khalil
- A Lana
- A Laskin
- A Lupu
- A McCulloch
- A Ooki
- A Ooki
- A Orlikowska
- A Razavi
- A Saiz-Lopez
- A Saiz-Lopez
- A Saiz-Lopez
- A Saiz-Lopez
- A Saiz-Lopez
- A Saiz-Lopez
- A Schmittner
- A Schönhardt
- A Stubbins
- A Stubbins
- A Stubbins
- A Vardi
- AC Lewis
- AD Anbar
- AE Jones
- AJ Beyersdorf
- AJ Gabric
- AJ Kettle
- AJ Kettle
- AJ Kettle
- AJ Kettle
- AJ Kettle
- AL Chuck
- AL Swanson
- Alfonso Saiz-Lopez
- AM Wuosma
- AR Baker
- AR Baker
- AR Bandy
- AR Bandy
- AS Mahajan
- AS Mahajan
- B Alexander
- B Alicke
- B Bonsang
- B Bonsang
- B Bonsang
- B Bonsang
- B Gantt
- B Gantt
- B Quack
- B Quack
- B Quack
- B Stevens
- BA Gray
- BB Ward
- BD Finley
- BG Heikes
- BJ Allan
- BN Duncan
- BS Gilfedder
- BS Gilfedder
- C Bale
- C Hughes
- C Hughes
- C Hughes
- C Hughes
- C Hughes
- C Leck
- C Müller
- C O’Dowd
- C Plass-Dülmer
- C Rinsland
- C Rinsland
- C Shim
- CA Marandino
- Carl J. Palmer
- CD Murphy
- CD O’Dowd
- CD O’Dowd
- CD O’Dowd
- CD O’Dowd
- CE Geen
- CE Jones
- CE Jones
- CG Fichot
- CH Dimmer
- CM Spivakovsky
- CM Trudinger
- CS Law
- CW Fairall
- D Amouroux
- D Helmig
- D Kim
- D Smythe-Wright
- D Smythe-Wright
- D Sprung
- DA Day
- Daniel J. Jacob
- DB King
- DB Millet
- DB Millet
- DD Riemer
- DF Wilson
- DG Capone
- DH Lenschow
- DJ Coffman
- DJ Jacob
- DJ Lary
- DJ Lary
- DK Brownell
- DL Savoie
- DM Joseph
- DR Benson
- E Atlas
- EA Holland
- EA Moelwyn-Hughes
- EC Howard
- ED Hudson
- EE Dahl
- EE Dahl
- EE Dahl
- EE Dahl
- EE Dahl
- EL Atlas
- Elizabeth L. Podowski
- EP Olaguer
- ER Lewis
- ES Saltzman
- EW Bartnicki
- F Dentener
- F Keppler
- F Laturnus
- F Yu
- FC Küpper
- FE Hopkins
- FJ Dentener
- FYB Seto
- G Allen
- G Dufour
- G Luo
- G McFiggans
- G McFiggans
- G McFiggans
- G McFiggans
- G McFiggans
- G Uher
- GA Sturrock
- GJ Derevianko
- GJ Herndl
- GM King
- GO Kirst
- GP Yang
- GP Yang
- GW Schade
- H Fuse
- H Korhonen
- H Mao
- H Sievering
- H Sievering
- H Singh
- H Tsukada
- HB Singh
- HB Singh
- HB Singh
- HB Singh
- HB Singh
- HB Singh
- HC Pumphrey
- HK Tiefenau
- HW Bange
- HX Xie
- HX Xie
- HX Xie
- HX Xie
- I Barnes
- I Barnes
- I Faloona
- I Hense
- I Nagao
- I Obernosterer
- IB Oh
- IR McDonald
- IV Patroescu
- J Aitken
- J Kirkby
- J Lelieveld
- J Lelieveld
- J Sciare
- J Sciare
- J Sciare
- J Sciare
- J Stefels
- J Stefels
- J Stutz
- J Swinnerton
- J Williams
- J Williams
- J-F Mueller
- J-M Kim
- JA Gouw de
- JA Thornton
- JB Nowak
- JC Gómez Martín
- JD Blando
- JE Johnson
- JE Lovelock
- JF Lamarque
- JJ Corbett
- JJ Harrison
- JJ Harrison
- JL Dixon
- JL Dixon
- JL Jimenez
- JL Moyers
- JM Baker
- JM Lobert
- JM Mäkelä
- JMC Plane
- JN Galloway
- JW Bottenheim
- JWH Dacey
- K Ballschmiter
- K Mopper
- K Mopper
- KA Abrahamsson
- KA Read
- KA Read
- KD Goodwin
- L Bariteau
- L Bopp
- L Ganzeveld
- L Hu
- L Wang
- L Whalley
- L Ziolkowski
- LG Wade
- LJ Carpenter
- LJ Carpenter
- LJ Carpenter
- LJ Carpenter
- M Ehrhardt
- M Kulmala
- M Levasseur
- M Martin
- M Martino
- M Martino
- M Martino
- M Mezcua
- M Nemecek-Marshall
- M Prather
- M Ratte
- M Ratte
- M Ratte
- M Vogt
- M Vogt
- M Yang
- MA Moran
- MA Sutton
- MC Facchini
- MG Scarratt
- MG Scarratt
- MG Scarratt
- MH Smith
- MJ Lawler
- MJ Lawler
- MK Sluis
- ML Cox
- ML Wesely
- MO Andreae
- MO Andreae
- MO Andreae
- MP Rayman
- MT Johnson
- MT Johnson
- MT Johnson
- MT Johnson
- MT Johnson
- MT Woodhouse
- MT Woodhouse
- MW Loewus
- N Bell
- N Kaltsoyannis
- N Meskhidze
- N Ohsawa
- N Yassaa
- NJ Blake
- NJ Blake
- NM Donahue
- NV Blough
- NV Blough
- OC Zafiriou
- OC Zafiriou
- OC Zafiriou
- OR Flock
- OW Wingenter
- OW Wingenter
- OW Wingenter
- P Korhonen
- P Williamson
- PC Novelli
- PD Nightingale
- PD Nightingale
- Peter Warneck
- PG Simmonds
- Philip Cameron-Smith
- PK Quinn
- PK Quinn
- PM Gschwend
- PO Wennberg
- PS Liss
- PS Liss
- PS Monks
- Q Li
- QB Li
- R Atkinson
- R Atkinson
- R Beale
- R Conrad
- R Conrad
- R Fischer
- R Glasow
- R Glasow von
- R Glasow Von
- R Glasow von
- R Glasow von
- R Glasow von
- R Glasow von
- R Nadasdi
- R Sander
- R Simo
- R Theiler
- R Tokarczyk
- R Tokarczyk
- R Tokarczyk
- R Toumi
- R Vogt
- R Wada
- RA Duce
- RA Marshall
- RF Troxler
- RG Prinn
- RG Zika
- RJ Charlson
- RJ Flanagan
- RJ Kieber
- RJ Kieber
- RJ Salawitch
- RJ Salawitch
- RL Valentine
- RM Moore
- RM Moore
- RM Moore
- RM Moore
- RM Moore
- RM Moore
- RM Moore
- RM Moore
- RM Moore
- RM Moore
- RP Kiene
- RP Kiene
- RS Russo
- RW Saunders
- RW Saunders
- RW Saunders
- S Amachi
- S Elliott
- S Elliott
- S Elliott
- S Hashimoto
- S Klick
- S Klick
- S Koga
- S Koga
- S O’Doherty
- S Padmaja
- S Punshon
- S Raimund
- S Saemundsdottir
- S Xu
- S. Kloster
- S. M. Vallina
- SA Conley
- SA Yvon-Lewis
- SA Yvon-Lewis
- SD Archer
- SD Archer
- SF Watts
- SJ Oltmans
- SJ Weeks
- SL Manley
- SL Manley
- SL Manley
- SL Manley
- SL Manley
- SL Neidleman
- SL Shaw
- SL Shaw
- SM Kreidenweis
- SM Schauffler
- SM Turner
- SM Vallina
- SM Vallina
- SR Arnold
- SR Arnold
- ST Wilson
- SW Gibb
- T Elias
- T Gravestock
- T Ingham
- T Kurten
- T Tanhua
- TG Bell
- TH Class
- TJ Breider
- TJ Dillon
- TM Vogel
- TN Knepp
- TS Bates
- TS Bates
- TS Rhee
- TW Andreae
- U Gunten von
- U Richter
- U Schmidt
- V Avgoustidi
- V Brüchert
- V Eyring
- V Gros
- V Kitidis
- V Naik
- V Sinha
- VW Truesdale
- W Broadgate
- W Chang
- W Fenical
- W Groszko
- W Grzybowski
- W Mabey
- W Sunda
- WC Keene
- WH Schlesinger
- WJ Bloss
- WJ Bruyn de
- WL Chameides
- WL Chameides
- X Xiao
- X Zhou
- Y Muramatsu
- Y Zuo
- Yvonnick Le Clainche
- Z Zhang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
The two-way exchange of trace gases between the ocean and the atmosphere is important for both the chemistry and physics of the atmosphere and the biogeochemistry of the oceans, including the global cycling of elements. Here we review these exchanges and their importance for a range of gases whose lifetimes are generally short compared to the main greenhouse gases and which are, in most cases, more reactive than them. Gases considered include sulphur and related compounds, organohalogens, non-methane hydrocarbons, ozone, ammonia and related compounds, hydrogen and carbon monoxide. Finally, we stress the interactivity of the system, the importance of process understanding for modeling, the need for more extensive field measurements and their better seasonal coverage, the importance of inter-calibration exercises and finally the need to show the importance of air-sea exchanges for global cycling and how the field fits into the broader context of Earth System Science
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
- Buchanan CC
- Buchholz P
- Buckley DAH
- Buckley-Geer E
- Budnev NM
- Buehler R
- Bueno A
- Bufano F
- Buffa F
- Buikema A
- Buitink S
- Bulgarelli A
- Bulger J
- Bulik T
- Bulik T
- Bulla M
- Bulten HJ
- Buonanno A
- Burgay M
- Burgess JM
- Burgman A
- Burhonov O
- Burke DL
- Burns E
- Burrows DN
- Buscemi M
- Buskulic D
- Buson S
- Bustillo J Caldern
- Busto J
- Butler NR
- Butler RE
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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
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
Search for excited electrons singly produced in proton–proton collisions at \sqrt{s} = 13 TeV with the ALAS experiment at the LHC
- 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
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- Zhemchugov A
- Zheng Z
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- Zhulanov V
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- Zinonos Z
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- Zobernig G
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- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2019
- Field of study
A search for excited electrons produced in pp collisions at s√ = 13 TeV via a contact interaction qq¯→ee∗ is presented. The search uses 36.1 fb −1 of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( eqq¯ ) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a W boson ( νW ) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying W boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the pp→ee∗→eeqq¯ and pp→ee∗→eνW production cross sections as a function of the excited electron mass me∗ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Λ of the model as a function of me∗ . For me∗<0.5 TeV , the lower bound for Λ is 11 TeV . In the special case of me∗=Λ , the values of me∗<4.8 TeV are excluded. The presented limits on Λ are more stringent than those obtained in previous searches
The ATLAS inner detector trigger performance in pp collisions at 13 TeV during LHC Run 2
- Author
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
The design and performance of the inner detector trigger for the high level trigger of the ATLAS experiment at the Large Hadron Collider during the 2016-2018 data taking period is discussed. In 2016, 2017, and 2018 the ATLAS detector recorded 35.6 fb(-1), 46.9 fb(-1), and 60.6 fb(-1) respectively of proton-proton collision data at a centre-of-mass energy of 13TeV. In order to deal with the very high interaction multiplicities per bunch crossing expected with the 13TeV collisions the inner detector trigger was redesigned during the long shutdown of the Large Hadron Collider from 2013 until 2015. An overview of these developments is provided and the performance of the tracking in the trigger for the muon, electron, tau and b-jet signatures is discussed. The high performance of the inner detector trigger with these extreme interaction multiplicities demonstrates how the inner detector tracking continues to lie at the heart of the trigger performance and is essential in enabling the ATLAS physics programme
Guidelines for the use and interpretation of assays for monitoring autophagy (4th edition)1.
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- Abdel-Aziz AK
- Abdelfatah S
- Abdellatif M
- Abdoli A
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- Zimmermann CM
- Ziviani E
- Zoladek T
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- Zorov DB
- Zorzano A
- Zou W
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- Zuryn S
- Zwerschke W
- Álvarez ÉMC
- Ávalos Y
- Önal G
- Üstün S
- Čolić M
- Đokić J
- Žerovnik E
- Publication venue
- 'Informa UK Limited'
- Publication date
- 01/01/2021
- Field of study
In 2008, we published the first set of guidelines for standardizing research in autophagy. Since then, this topic has received increasing attention, and many scientists have entered the field. Our knowledge base and relevant new technologies have also been expanding. Thus, it is important to formulate on a regular basis updated guidelines for monitoring autophagy in different organisms. Despite numerous reviews, there continues to be confusion regarding acceptable methods to evaluate autophagy, especially in multicellular eukaryotes. Here, we present a set of guidelines for investigators to select and interpret methods to examine autophagy and related processes, and for reviewers to provide realistic and reasonable critiques of reports that are focused on these processes. These guidelines are not meant to be a dogmatic set of rules, because the appropriateness of any assay largely depends on the question being asked and the system being used. Moreover, no individual assay is perfect for every situation, calling for the use of multiple techniques to properly monitor autophagy in each experimental setting. Finally, several core components of the autophagy machinery have been implicated in distinct autophagic processes (canonical and noncanonical autophagy), implying that genetic approaches to block autophagy should rely on targeting two or more autophagy-related genes that ideally participate in distinct steps of the pathway. Along similar lines, because multiple proteins involved in autophagy also regulate other cellular pathways including apoptosis, not all of them can be used as a specific marker for bona fide autophagic responses. Here, we critically discuss current methods of assessing autophagy and the information they can, or cannot, provide. Our ultimate goal is to encourage intellectual and technical innovation in the field
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at s√=13TeV
- Author
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- Yao W-M
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- Yildiz HD
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- Yue X
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- Zabinski B
- Zacharis G
- Zaffaroni E
- Zagazeta LFG
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zgubič M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- 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 NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- 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
Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahilo JJL
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barron U
- Barrue RFC
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Baselga M
- Bashta I
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
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- Bauer F
- Bauer P
- Bawa HS
- Bayirli A
- Beacham JB
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- Beauchemin PH
- Becherer F
- Bechtle P
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- Bee CP
- Beermann TA
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- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bello FAD
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- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benhammou Y
- Benjamin DP
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- Bensinger JR
- Bentvelsen S
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- Bergsten LJ
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- Betti A
- Bevan AJ
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Biebel O
- Bielski R
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Bourdarios CA
- 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
- Brener R
- 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
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Brüers B
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Bugge MK
- Bulekov O
- Bullard BA
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Büscher V
- Cabras G
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carlson TI
- Carminati L
- Carnesale M
- Carney RMD
- Caron S
- Carquin E
- Carratta G
- Carrá S
- Carter JWS
- Carter TM
- Casadei D
- Casado MP
- Casha AF
- Castiglia EG
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
- Centonze MS
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Chen Y-H
- Cheng CL
- Cheng HC
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clawson SE
- Clement C
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coelli S
- Cohen H
- Coimbra AEC
- Cole B
- Collot J
- Columbie JMC
- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Coutinho YA
- Cowan G
- Cowley JW
- Cranmer K
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosetti G
- Crépé-Renaudin S
- Cueto A
- Cui H
- Cukierman AR
- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Daalen TRV
- Dabrowski W
- Dado T
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- Zhemchugov A
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- Ziolkowski M
- Zoccoli A
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- EUROPEAN PHYSICAL JOURNAL C
- Publication date
- 01/01/2022
- Field of study
This paper presents the measurement of the electroweak production of two jets
in association with a Zγ pair with the Z boson decaying into two
neutrinos. It also presents the search for invisible or partially invisible
decays of a Higgs boson with a mass of 125 GeV produced through vector-boson
fusion with a photon in the final state. These results use data from LHC
proton-proton collisions at s = 13 TeV collected with the ATLAS
detector corresponding to an integrated luminosity of 139 fb−1. The event
signature, shared by all benchmark processes considered for measurements and
searches, is characterized by a significant amount of unbalanced transverse
momentum and a photon in the final state, in addition to a pair of forward
jets. For electroweak production of Zγ in association with two jets, the
background-only hypothesis is rejected with an observed (expected) significance
of 5.2 (5.1) standard deviations. The measured fiducial cross-section for this
process is 1.31±0.29 fb. Observed (expected) upper limit of 0.37 (0.34) at
95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to
invisible particles, assuming the Standard Model production cross-section. The
signature is also interpreted in the context of decays of a Higgs boson to a
photon and a dark photon. An observed (expected) 95% CL upper limit on the
branching ratio for this decay is set at 0.018 (0.017), assuming the 125 GeV
Standard Model Higgs boson production cross-section
- …