57 research outputs found
Invasive Plants and Enemy Release: Evolution of Trait Means and Trait Correlations in Ulex europaeus
- Author
- A Atlan
- A Biere
- A Monty
- AA Agrawal
- Anne Atlan
- B Blossey
- B Sinervo
- B Walsh
- Benjamin Hornoy
- CE Lee
- CE Mitchell
- CJE Metcalf
- CM Orians
- CS Kolar
- DA Levin
- DA Roach
- DA Roff
- DA Roff
- DC Lahti
- DJ Futuyma
- DM Blumenthal
- DM Richardson
- DS Falconer
- EA Leger
- EH Chater
- G Bowman
- GP Markin
- GW Gilchrist
- H Liu
- H Müller-Schärer
- J Herrera
- J Joshi
- J Kollmann
- J Zou
- JA Elzinga
- JL Maron
- JL Montague
- JM Alexander
- JM Alexander
- JM Norghauer
- JR Etterson
- LH Millener
- LM Wolfe
- Luc Gigord
- M Barat
- M Barat
- M Hilker
- M Lynch
- M Stastny
- M Tarayre
- Mari Moora
- Maxime Hervé
- Michèle Tarayre
- MTJ Johnson
- MW Blows
- O Bossdorf
- P Alpert
- R Leimu
- RI Colautti
- RL Hill
- RL Hill
- RM Callaway
- RM Keane
- S Lowe
- UA Treier
- W Huang
- WM Davies
- WM Ridenour
- YM Buckley
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Several hypotheses that attempt to explain invasive processes are based on the fact that plants have been introduced without their natural enemies. Among them, the EICA (Evolution of Increased Competitive Ability) hypothesis is the most influential. It states that, due to enemy release, exotic plants evolve a shift in resource allocation from defence to reproduction or growth. In the native range of the invasive species Ulex europaeus, traits involved in reproduction and growth have been shown to be highly variable and genetically correlated. Thus, in order to explore the joint evolution of life history traits and susceptibility to seed predation in this species, we investigated changes in both trait means and trait correlations. To do so, we compared plants from native and invaded regions grown in a common garden. According to the expectations of the EICA hypothesis, we observed an increase in seedling height. However, there was little change in other trait means. By contrast, correlations exhibited a clear pattern: the correlations between life history traits and infestation rate by seed predators were always weaker in the invaded range than in the native range. In U. europaeus, the role of enemy release in shaping life history traits thus appeared to imply trait correlations rather than trait means. In the invaded regions studied, the correlations involving infestation rates and key life history traits such as flowering phenology, growth and pod density were reduced, enabling more independent evolution of these key traits and potentially facilitating local adaptation to a wide range of environments. These results led us to hypothesise that a relaxation of genetic correlations may be implied in the expansion of invasive species
Growth Strategies of Tropical Tree Species: Disentangling Light and Size Effects
- Author
- A Gelman
- A Gelman
- A Gelman
- AJ Kerkhoff
- B Herault
- C Baraloto
- CD Canham
- CD Canham
- CJE Metcalf
- CW Welden
- D Purves
- D Sheil
- DA Clark
- DA Clark
- DA Coomes
- DA King
- DH Dent
- DM Windsor
- DM Windsor
- EGJ Leigh
- EGJ Leigh
- Enrico Scalas
- G Kunstler
- Ghislain Vieilledent
- H Akaike
- HC Muller-Landau
- J Chave
- JB Yavitt
- JMG Bloor
- JS Clark
- JS Clark
- JS Denslow
- JS Denslow
- JS Denslow
- JS Wright
- JW Dalling
- JW Lichstein
- K Kitajima
- KD Coates
- KJ Niklas
- L Poorter
- L Poorter
- L Poorter
- L Sack
- LS Comita
- M Lieberman
- M Uriarte
- M Uriarte
- N Rüger
- N Rüger
- Nadja Rüger
- NCA Pitman
- ND Brown
- OL Phillips
- PH Wyckoff
- PJ van der Meer
- R Condit
- R Condit
- R Condit
- R Condit
- R Wirth
- RA Montgomery
- RB Foster
- RC de Gouvenain
- Richard Condit
- RJW Brienen
- RK Kobe
- S Iriarte Vivar Balderrama
- SA Mangan
- SE Johnson
- SJ Davies
- SJ Wright
- SM McMahon
- SP Hubbell
- Stephen P. Hubbell
- SW Pacala
- T Kohyama
- TB Croat
- Uta Berger
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
An understanding of the drivers of tree growth at the species level is required to predict likely changes of carbon stocks and biodiversity when environmental conditions change. Especially in species-rich tropical forests, it is largely unknown how species differ in their response of growth to resource availability and individual size. We use a hierarchical Bayesian approach to quantify the impact of light availability and tree diameter on growth of 274 woody species in a 50-ha long-term forest census plot in Barro Colorado Island, Panama. Light reaching each individual tree was estimated from yearly vertical censuses of canopy density. The hierarchical Bayesian approach allowed accounting for different sources of error, such as negative growth observations, and including rare species correctly weighted by their abundance. All species grew faster at higher light. Exponents of a power function relating growth to light were mostly between 0 and 1. This indicates that nearly all species exhibit a decelerating increase of growth with light. In contrast, estimated growth rates at standardized conditions (5 cm dbh, 5% light) varied over a 9-fold range and reflect strong growth-strategy differentiation between the species. As a consequence, growth rankings of the species at low (2%) and high light (20%) were highly correlated. Rare species tended to grow faster and showed a greater sensitivity to light than abundant species. Overall, tree size was less important for growth than light and about half the species were predicted to grow faster in diameter when bigger or smaller, respectively. Together light availability and tree diameter only explained on average 12% of the variation in growth rates. Thus, other factors such as soil characteristics, herbivory, or pathogens may contribute considerably to shaping tree growth in the tropics
FXR inhibition may protect from SARS-CoV-2 infection by reducing ACE2
- Author
- Baker S
- Bargehr J
- Barnes E
- Barritt IV AS
- Bastaich DR
- Box H
- Bramwell C
- Brevini T
- Brown ML
- Brown S
- Buczacki SJA
- Buescher G
- Butler AJ
- Clements D
- Consortium UK-PBC
- Corbett G
- Cox H
- Crozier TWM
- Curley P
- Dahman B
- Darvish-Damavandi M
- Davenport AP
- Davies SE
- Dillon S
- Dougan G
- Fear C
- Ferreira RD
- Fisher AJ
- Forrest S
- Fuchs CD
- Galanakis V
- Gelson WTH
- Gibbs P
- Gorgoulis VG
- Griffiths C
- Gupta RK
- Hagstrom H
- Herriott J
- Heslop JA
- Humphreys P
- Illingworth CJR
- John BV
- Kijak E
- Kuc RE
- Lee JH
- Lohse AW
- Maes M
- Marjot T
- Matheson NJ
- Mells GF
- Melum E
- Mlcochova P
- Moon AM
- Mulcahy VL
- Muraro D
- Neary M
- Owen A
- Pereyra-Gerber P
- Pertinez H
- Rossetti D
- Saeb-Parsy K
- Sampaziotis F
- Scott III WE
- Sharp J
- Sinha S
- Stewart J
- Swift L
- Tatham L
- Trauner M
- Tysoe OC
- Upponi SS
- Valentijn A
- Vallier L
- Varankar SS
- Vila-Gonzalez M
- Wang L
- Watson CJE
- Webb GJ
- Wester A
- Williams TL
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- Field of study
Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at √s=8 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TP
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Bagnaia P
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Banerjee S
- Bannoura AAE
- Barajas CAC
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behr JK
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Beringer J
- Berlendis S
- Berlingen JM
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertram IA
- Bertsche C
- Bertsche D
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethani A
- Bethke S
- Bevan AJ
- Beyer J
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bilokon H
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Bisanz T
- Bittrich C
- Bjergaard DM
- Black CW
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blum W
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boehler M
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Bossio Sola JD
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bracinik J
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Bravo AG
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Briglin DL
- Bristow TM
- Britton D
- Britzger D
- Brochu FM
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brosamer J
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
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- Bugge MK
- Bulekov O
- Bullock D
- Burch TJ
- Burckhart H
- Burdin S
- Burgard CD
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- Burmeister I
- Burr JTP
- Busato E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabrera Urban S
- Caforio D
- Cairo VM
- Cakir IT
- Cakir O
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- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
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- Camarda S
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- Camincher C
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- Castillo IS
- Castillo LRF
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- Catmore JR
- Cattai A
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- Celebi E
- Ceradini F
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- Cerqueira AS
- Cerri A
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- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
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- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Che S
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
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- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Chernyatin V
- Cheu E
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- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
- Chizhov MV
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- Chomont AR
- Chouridou S
- Christodoulou V
- Chromek-Burckhart D
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
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- Collaboration ATLAS
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- Crawley SJ
- Creager RA
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cribbs WA
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cukierman AR
- Cummings J
- Curatolo M
- Cuth J
- Czirr H
- Czodrowski P
- D'amen G
- D'Auria S
- D'eramo L
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dado T
- Dai T
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- Dallapiccola C
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- Damazio DO
- Dandoy JR
- Daneri MF
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- De Benedetti A
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- de Jong P
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- de Lima DEF
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- de Renstrom PAB
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- Deigaard I
- Del Gaudio M
- Del Peso J
- Del Prete T
- Delgove D
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- Dell'Orso M
- Della Pietra M
- della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Demilly A
- Denis RDS
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- Di Petrillo KF
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- Di Valentino D
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- Dias FA
- Diaz MA
- Diehl EB
- Dietrich J
- Dimitrievska A
- Dingfelder J
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- Dita S
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- Dudder AC
- Dueren M
- Duffield EM
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- Duhrssen M
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- Dumitriu AE
- Duncan AK
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- Duschinger D
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- Eifert T
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- El Kacimi M
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- Ellajosyula V
- Ellert M
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- Ellinghaus F
- Elliot AA
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- Elmsheuser J
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- Endner OC
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- Erdmann J
- Ereditato A
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- Etienvre AI
- Etzion E
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- Farina EM
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- Farrell S
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Favareto A
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
- Feigl S
- Feligioni L
- Feng C
- Feng EJ
- Feng H
- Fenton MJ
- Fenyuk AB
- Feremenga L
- Fernandez Martinez P
- Fernandez Perez S
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrer A
- Ferrere D
- Ferretti C
- Fiedler F
- Filipcic A
- Filipuzzi M
- Filthaut F
- Fincke-Keeler M
- Finelli KD
- Fiolhais MCN
- Fiorini L
- Fischer A
- Fischer C
- Fischer J
- Fisher WC
- Flaschel N
- Fleck I
- Fleischmann P
- Fletcher RRM
- Flick T
- Flierl BM
- Flowerdew MJ
- Forcolin GT
- Formica A
- Forster FA
- Forti A
- Foster AG
- Fournier D
- Fox H
- Fracchia S
- Francavilla P
- Franchini M
- Franchino S
- Francis D
- Franconi L
- Franklin M
- Frate M
- Fraternali M
- Freeborn D
- Fressard-Batraneanu SM
- Freund B
- Froidevaux D
- Frost JA
- Fukunaga C
- Fusayasu T
- Fuster J
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- Gabizon O
- Gabrielli A
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- Gadatsch S
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- Gagliardi G
- Gagnon LG
- Galea C
- Galhardo B
- Gallas EJ
- Gallop BJ
- Gallus P
- Galster G
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- Ganguly S
- Gao Y
- Gao YS
- Garcia BRM
- Garcia C
- Garcia RFN
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- Gardner RW
- Garelli N
- Garonne V
- Garrido MDMC
- Gasnikova K
- Gatti C
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- Yildirim E
- Yildiz HD
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- Zalieckas J
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- Zanzi D
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- Zemla A
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- Zeng Q
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- Zhang Z
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- Zhao Z
- Zhemchugov A
- Zhou B
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- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of √s=8 TeV is presented. The results are based on an integrated luminosity of 20.2 fb−1 recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying |ηγ|40GeV and EγT,2>30 GeV for the two leading photons ordered in transverse energy produced in the interaction. The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is 16.8 ± 0.8 pb . The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%
Search for dark matter at √s=13 TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam ER
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
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- Alshehri AA
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
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- Amor Dos Santos SP
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- Amundsen G
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- Angelozzi I
- Angerami A
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- Antonelli M
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- Antrim DJ
- Anulli F
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- Araujo Ferraz V
- Araya ST
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- Ardell RE
- Arduh FA
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- Carminati L
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- Carvalho J
- Casadei D
- Casado MP
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- Casper DW
- Castelijn R
- Castillo IS
- Castillo LRF
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- Zivkovic L
- Zobernig G
- Zoccoli
- Zou R
- Zu Theenhausena HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb−1 of proton–proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, model-independent limits are set on the fiducial cross section for the production of events in this final state. Exclusion limits are also placed in models where dark-matter candidates are pair-produced. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750–1200 GeV for dark-matter candidate masses below 230–480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale M∗ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to Zγ and the Z boson subsequently decays into neutrinos
Studies of Zγ production in association with a high-mass dijet system in pp collisions at √s=8 TeV with the ATLAS detector
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- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
The production of a Z boson and a photon in association with a high-mass dijet system is studied using 20.2 fb −1 of proton-proton collision data at a centre-of-mass energy of s=8 TeV recorded with the ATLAS detector in 2012 at the Large Hadron Collider. Final states with a photon and a Z boson decaying into a pair of either electrons, muons, or neutrinos are analysed. Electroweak and total pp → Zγjj cross-sections are extracted in two fiducial regions with different sensitivities to electroweak production processes. Quartic couplings of vector bosons are studied in regions of phase space with an enhanced contribution from pure electroweak production, sensitive to vector-boson scattering processes VV → Zγ. No deviations from Standard Model predictions are observed and constraints are placed on anomalous couplings parameterized by higher-dimensional operators using effective field theory.[Figure not available: see fulltext.]
Ecosystem Services from Small Forest Patches in Agricultural Landscapes
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- A Dobson
- A Hector
- A Jamoneau
- A Kolb
- A Kolb
- A Kolb
- A Montero-Castaño
- A Palo
- A Sourdril
- A Spangenberg
- A Torre De la
- A Troy
- A Valdés
- A Wilby
- A Young
- AB Nielsen
- AC Weibull
- AG Power
- AK Sikka
- AL Reye
- AM Bartuszevige
- AM Klein
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- AR Devlaeminck
- AS Hadley
- B Berg
- B Burkhard
- B Gabrielle
- B Tenhumberg
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- CL Goodale
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- DU Hooper
- E Szabo
- E Virgós
- EB Rastetter
- ES Kasischke
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- G Domínguez
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- GF McCracken
- GJ Nabuurs
- H Calster Van
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- H Gibb
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- I Guerrero
- IA Janssens
- J Abildtrup
- J Boardman
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- L Barbaro
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- L Hörnsten
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- M Christie
- M Crockatt
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- M Kukumägi
- M Lange
- M Lindner
- M Sanctis De
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- M Vellend
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- MC Hansen
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- MJ Schelhaas
- MK Obrist
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- N Stryamets
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- R Aguilar
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- R Bertrand
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- R Devlaeminck
- R Kalda
- R Mäkipää
- R Scarpa
- R Väisänen
- RJ Hobbs
- RL Naylor
- RPC Morgan
- RR Dunn
- RS Groot De
- RS Ostfeld
- S Costard
- S Eriksson
- SG Nilsson
- SM Pawson
- T Brothers
- T Doré
- T Figueiredo de
- T Karjalainen
- T Magura
- T Santos
- T Snäll
- T Tscharntke
- TC Daniel
- TD Heithecker
- TH Ricketts
- UNECE
- VH Dale
- VS Gundersen
- VU Smakhtin
- WE Dramstad
- WH Maes
- Y Paillet
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Performance of the ATLAS Transition Radiation Tracker in Run 1 of the LHC: tracker properties
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- Aad G
- Abbott B
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- Albert J
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- Alexa C
- Alexander G
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- Alhroob M
- Ali B
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- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
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- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
- Amidei D
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- Ardell RE
- Arduh FA
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- Armadans R Caminal
- Armbruster AJ
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2017
- Field of study
he tracking performance parameters of the ATLAS Transition Radiation Tracker (TRT) as part of the ATLAS inner detector are described in this paper for different data-taking conditions in proton-proton, proton-lead and lead-lead collisions at the Large Hadron Collider (LHC). The performance is studied using data collected during the first period of LHC operation (Run 1) and is compared with Monte Carlo simulations. The performance of the TRT, operating with two different gas mixtures (xenon-based and argon-based) and its dependence on the TRT occupancy is presented. These studies show that the tracking performance of the TRT is similar for the two gas mixtures and that a significant contribution to the particle momentum resolution is made by the TRT up to high particle densities.We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently.info:eu-repo/semantics/publishedVersio
Measurement of the cross-section for producing a W boson in association with a single top quark in pp collisions at √s = 13 TeV with ATLAS
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya S
- Adachi S
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
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- Kortner O
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- Kostyukhin VV
- Kotwal A
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- Publication venue
- Springer
- Publication date
- 01/01/2018
- Field of study
The inclusive cross-section for the associated production of a W boson and top
quark is measured using data from proton-proton collisions at √
s = 13 TeV. The dataset
corresponds to an integrated luminosity of 3.2 fb−1
, and was collected in 2015 by the ATLAS
detector at the Large Hadron Collider at CERN. Events are selected requiring two opposite
sign isolated leptons and at least one jet; they are separated into signal and control regions
based on their jet multiplicity and the number of jets that are identified as containing b
hadrons. The W t signal is then separated from the tt¯ background using boosted decision
tree discriminants in two regions. The cross-section is extracted by fitting templates to the
data distributions, and is measured to be σW t = 94±10 (stat.)
+28
−22 (syst.)±2 (lumi.) pb. The
measured value is in good agreement with the SM prediction of σtheory = 71.7±1.8 (scale)±
3.4 (PDF) pb [1]
Determination of the strong coupling constant αs from transverse energy–energy correlations in multijet events at s√=8 TeV using the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/01/2017
- Field of study
Measurements of transverse energy–energy correlations and their associated asymmetries in multi-jet events using the ATLAS detector at the LHC are presented. The data used correspond to s√=8 TeV proton–proton collisions with an integrated luminosity of 20.2 fb−1 . The results are presented in bins of the scalar sum of the transverse momenta of the two leading jets, unfolded to the particle level and compared to the predictions from Monte Carlo simulations. A comparison with next-to-leading-order perturbative QCD is also performed, showing excellent agreement within the uncertainties. From this comparison, the value of the strong coupling constant is extracted for different energy regimes, thus testing the running of αs(μ) predicted in QCD up to scales over 1 TeV . A global fit to the transverse energy–energy correlation distributions yields αs(mZ)=0.1162±0.0011(exp.) +0.0084−0.0070(theo.) , while a global fit to the asymmetry distributions yields a value of αs(mZ)=0.1196±0.0013(exp.) +0.0075−0.0045(theo.)
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