1,305 research outputs found
Neural correlates of sexual cue reactivity in individuals with and without compulsive sexual behaviours
- Author
- A Ferretti
- A Galvan
- A Kor
- A Shenhav
- AJ Shackman
- AR Childress
- AS Euser
- AT Beck
- BA Arnow
- BL Odlaug
- BL Odlaug
- BY Hayden
- CA McGahuey
- CA Warren
- D Martinez
- D Weintraub
- DC Perry
- DE Linden
- DG Smith
- DI Lubman
- DL Delmonico
- DV Sheehan
- ER Sowell
- G Sescousse
- GJ Meerkerk
- GK Murray
- H Kataoka
- H Mouras
- IH Franken
- IH Franken
- J Redoute
- JA Maldjian
- JB Saunders
- JD Wallis
- JE Grant
- JE Grant
- JP Dunning
- Judy Karr
- KS Young
- Laura Porter
- Laurel Morris
- LH Somerville
- M Bocher
- M Heinze
- M Politis
- Marc N. Potenza
- MC van de Laar
- MF Rushworth
- MH Miner
- Michael Irvine
- MP Kafka
- Neil A. Harrison
- NM Petry
- Paula Banca
- PH Rudebeck
- RA Chambers
- RA Poldrack
- RC Reid
- RC Reid
- S Hamann
- S Kuhn
- S Kuhn
- S Kuhn
- S Stoleru
- Simon Mitchell
- SM Williams
- SP Whiteside
- T Paul
- Tatyana R. Lapa
- TE Robinson
- Thomas B. Mole
- TW Fong
- V Voon
- Valerie Voon
- Veronique Sgambato-Faure
- VR Steele
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 11/07/2014
- Field of study
Although compulsive sexual behaviour (CSB) has been conceptualized as a "behavioural" addiction and common or overlapping neural circuits may govern the processing of natural and drug rewards, little is known regarding the responses to sexually explicit materials in individuals with and without CSB. Here, the processing of cues of varying sexual content was assessed in individuals with and without CSB, focusing on neural regions identified in prior studies of drug-cue reactivity. 19 CSB subjects and 19 healthy volunteers were assessed using functional MRI comparing sexually explicit videos with non-sexual exciting videos. Ratings of sexual desire and liking were obtained. Relative to healthy volunteers, CSB subjects had greater desire but similar liking scores in response to the sexually explicit videos. Exposure to sexually explicit cues in CSB compared to non-CSB subjects was associated with activation of the dorsal anterior cingulate, ventral striatum and amygdala. Functional connectivity of the dorsal anterior cingulate-ventral striatum-amygdala network was associated with subjective sexual desire (but not liking) to a greater degree in CSB relative to non-CSB subjects. The dissociation between desire or wanting and liking is consistent with theories of incentive motivation underlying CSB as in drug addictions. Neural differences in the processing of sexual-cue reactivity were identified in CSB subjects in regions previously implicated in drug-cue reactivity studies. The greater engagement of corticostriatal limbic circuitry in CSB following exposure to sexual cues suggests neural mechanisms underlying CSB and potential biological targets for interventions
Non-Hodgkin lymphoma response evaluation with MRI texture classification
- Author
- A Skoch
- BD Cheson
- BD Cheson
- BJ Woods
- D Jirák
- D Mahmoud-Ghoneim
- FA Hampson
- G Chen
- G Collewet
- H Kato
- Hannu J Eskola
- Hannu Pertovaara
- JM Mathias
- K Jafari-Khouzani
- L Bonilha
- L Harrison
- Lara CV Harrison
- LCV Harrison
- LH Sehn
- ME Mayerhoefer
- O Weingart
- O Yu
- P Gibbs
- P Therasse
- P Therasse
- PA Freeborough
- Pirkko-Liisa I Kellokumpu-Lehtinen
- PM Szczypinski
- PM Szczypiński
- Prasun Dastidar
- R Krug
- Ritva Järvenpää
- S Herlidou
- S Herlidou
- S Herlidou-Meme
- S Sinha
- SB Antel
- Seppo Soimakallio
- SM Ansell
- T Heinonen
- T Saarinen
- T Sankar
- Tiina Luukkaala
- Tomi T Heinonen
- Tuomas O Saarinen
- VR Anderson
- W Chen
- X Zhang
- Publication venue
- BioMed Central
- Publication date
- 01/01/2009
- Field of study
<p>Abstract</p> <p>Background</p> <p>To show magnetic resonance imaging (MRI) texture appearance change in non-Hodgkin lymphoma (NHL) during treatment with response controlled by quantitative volume analysis.</p> <p>Methods</p> <p>A total of 19 patients having NHL with an evaluable lymphoma lesion were scanned at three imaging timepoints with 1.5T device during clinical treatment evaluation. Texture characteristics of images were analyzed and classified with MaZda application and statistical tests.</p> <p>Results</p> <p>NHL tissue MRI texture imaged before treatment and under chemotherapy was classified within several subgroups, showing best discrimination with 96% correct classification in non-linear discriminant analysis of T2-weighted images.</p> <p>Texture parameters of MRI data were successfully tested with statistical tests to assess the impact of the separability of the parameters in evaluating chemotherapy response in lymphoma tissue.</p> <p>Conclusion</p> <p>Texture characteristics of MRI data were classified successfully; this proved texture analysis to be potential quantitative means of representing lymphoma tissue changes during chemotherapy response monitoring.</p
Sexual Plasticity and Self-Fertilization in the Sea Anemone Aiptasia diaphana
- Author
- A Burt
- A Schlesinger
- A Schlesinger
- A Weismann
- AJ Heyward
- Ami Schlesinger
- B Rinkevich
- B Rinkevich
- C Darwin
- C Tang
- CL Littlefield
- CLA Chen
- CLA Chen
- D Carre
- DA Brazeau
- DB Carlon
- DG Fautin
- DG Fautin
- DG Fautin
- E Kramarsky-Winter
- Esti Kramarsky-Winter
- Hanna Rosenfeld
- IB Baums
- JL Hamrick
- JM Shick
- JM Shick
- K Soong
- KM Bassim
- LH Hyman
- LW Buss
- MT Ghiselin
- N Colegrave
- NE Chadwick-Furman
- NH Putnam
- PL Harrison
- PL Harrison
- R Grosberg
- Rachel Armoza-Zvoloni
- Ryan L. Earley
- S Kalisz
- SV Vollmer
- T Hunter
- TA Stephenson
- U Frank
- VR Hall
- W Clayton
- Y Fukui
- Y Loya
- Y Loya
- Yossi Loya
- Publication venue
- Public Library of Science
- Publication date
- 01/07/2010
- Field of study
Traits that influence reproductive success and contribute to reproductive isolation in animal and plant populations are a central focus of evolutionary biology. In the present study we used an experimental approach to demonstrate the occurrence of environmental effects on sexual and asexual reproduction, and provide evidence for sexual plasticity and inter-clonal fertilization in laboratory-cultured lines of the sea anemone Aiptasia diaphana. We showed that in A. diaphana, both asexual reproduction by pedal laceration, and sexual reproduction have seasonal components. The rate of pedal laceration was ten-fold higher under summer photoperiod and water temperature conditions than under winter conditions. The onset of gametogenesis coincided with the rising water temperatures occurring in spring, and spawning occurred under parameters that emulated summer photoperiod and temperature conditions. In addition, we showed that under laboratory conditions, asexually produced clones derived from a single founder individual exhibit sexual plasticity, resulting in the development of both male and female individuals. Moreover, a single female founder produced not only males and females but also hermaphrodite individuals. We further demonstrated that A. diaphana can fertilize within and between clone lines, producing swimming planula larvae. These diverse reproductive strategies may explain the species success as invader of artificial marine substrates. We suggest that these diverse reproductive strategies, together with their unique evolutionary position, make Aiptasia diaphana an excellent model for studying the evolution of sex
Search for CP violation in D+→ϕπ+ and D+s→K0Sπ+ decays
- Author
- Aaij R
- Adeva B
- Adinolfi M
- Adrover C
- Affolder A
- Ajaltouni Z
- Akiba KC
- Albor VF
- Albrecht J
- Alessio F
- Alexander M
- Ali S
- Alkhazov G
- Altarelli MP
- Alvarez AP
- Alves AA
- Amato S
- Amerio S
- Amhis Y
- Anderlini L
- Anderson J
- Andreassen R
- Appleby RB
- Archilli F
- Artamonov A
- Artuso M
- Aslanides E
- Auriemma G
- Bachmann S
- Back JJ
- Baesso C
- Balagura V
- Baldini W
- Barlow RJ
- Barschel C
- Barsuk S
- Barter W
- Bauer T
- Bay A
- Beddow J
- Bedeschi F
- Bediaga I
- Belogurov S
- Belous K
- Belyaev I
- Ben-Haim E
- Benayoun M
- Bencivenni G
- Benson S
- Benton J
- Berezhnoy A
- Bernet R
- Beteta CA
- Bettler M-O
- Bien A
- Bifani S
- Bird T
- Bizzeti A
- Bjørnstad PM
- Blake T
- Blanc F
- Blouw J
- Blusk S
- Bocci V
- Bondar A
- Bondar N
- Bonivento W
- Borghi S
- Borgia A
- Bowcock TJV
- Bowen E
- Bozzi C
- Brambach T
- Bressieux J
- Brett D
- Britsch M
- Britton T
- Brook NH
- Brown H
- Burducea I
- Bursche A
- Busetto G
- Buytaert J
- Cadeddu S
- Callot O
- Calvi M
- Camboni A
- Campana P
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LAG
- Carranza-Mejia H
- Carson L
- Cartelle PA
- Casasus MP
- Casse G
- Cattaneo M
- Cauet C
- Charles M
- Charpentier P
- Chen P
- Chiapolini N
- Chrzaszcz M
- Ciba K
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Coca C
- Coco V
- Cogan J
- Cogneras E
- Collins P
- Comerma-Montells A
- Contu A
- Cook A
- Coombes M
- Coquereau S
- Corti G
- Coutinho RS
- Couturier B
- Cowan GA
- Craik D
- Cunliffe S
- Currie R
- David P
- David PNY
- De Bonis I
- De Bruyn K
- De Capua S
- De Cian M
- De Miranda JM
- De Oyanguren Campos M
- De Paula L
- De Silva W
- De Simone P
- Decamp D
- Deckenhoff M
- Del Buono L
- Derkach D
- Deschamps O
- Dettori F
- Di Canto A
- Diaz RG
- Dijkstra H
- Dogaru M
- Donleavy S
- Dordei F
- dos Reis AC
- Dossett D
- Dovbnya A
- Dupertuis F
- Dzhelyadin R
- Dziurda A
- Dzyuba A
- D’Ambrosio C
- Easo S
- Egede U
- Egorychev V
- Eidelman S
- Eisenhardt S
- Eitschberger U
- Ekelhof R
- Eklund L
- El Rifai I
- Elsasser C
- Elsby D
- Falabella A
- Fardell G
- Farinelli C
- Farry S
- Fave V
- Ferguson D
- Ferro-Luzzi M
- Filippov S
- Fitzpatrick C
- Fontana M
- Fontanelli F
- Forty R
- Francisco O
- Frank M
- Frei C
- Frosini M
- Furcas S
- Furfaro E
- Färber C
- Galli D
- Gandelman M
- Gandini P
- Gao Y
- Garofoli J
- Garosi P
- Garrido L
- Gaspar C
- Gauld R
- Gersabeck E
- Gersabeck M
- Gershon T
- Ghez P
- Gibson V
- Gioi LL
- Gligorov VV
- Goicochea JMO
- Golubkov D
- Golutvin A
- Gomes A
- Gomez MC
- Gordon H
- Graugés E
- Graziani G
- Grecu A
- Greening E
- Gregson S
- Grünberg O
- Gui B
- Gushchin E
- Gutierrez OA
- Guz Y
- Gys T
- Gándara MG
- Göbel C
- Hadjivasiliou C
- Haefeli G
- Haen C
- Haines SC
- Hall S
- Hampson T
- Hansmann-Menzemer S
- Harnew N
- Harnew ST
- Harrison J
- Hartmann T
- He J
- Heijne V
- Hennessy K
- Henrard P
- Hicks E
- Hill D
- Hoballah M
- Hombach C
- Hopchev P
- Hulsbergen W
- Hunt P
- Huse T
- Hussain N
- Hutchcroft D
- Hynds D
- Iakovenko V
- Idzik M
- Ilten P
- Jacobsson R
- Jaeger A
- Jans E
- Jaton P
- Jing F
- John M
- Johnson D
- Jones CR
- Jost B
- Kaballo M
- Kandybei S
- Karacson M
- Karbach TM
- Kenyon IR
- Kerzel U
- Ketel T
- Keune A
- Khanji B
- Kochebina O
- Komarov I
- Koopman RF
- Koppenburg P
- Korolev M
- Kozlinskiy A
- Kravchuk L
- Kreplin K
- Kreps M
- Krocker G
- Krokovny P
- Kruse F
- Kucharczyk M
- Kudryavtsev V
- Kvaratskheliya T
- La Thi VN
- Lacarrere D
- Lafferty G
- Lai A
- Lambert D
- Lambert RW
- Lanciotti E
- Lanfranchi G
- Langenbruch C
- Latham T
- Lazzeroni C
- Le Gac R
- Lees J-P
- Leflat A
- Lefrançois J
- Lefèvre R
- Leo S
- Leroy O
- Leverington B
- Li Y
- Liles M
- Lindner R
- Linn C
- Liu B
- Liu G
- Lohn S
- Lopes JH
- Lopez Asamar E
- Lopez-March N
- Lu H
- Lucchesi D
- Luisier J
- Luo H
- Machefert F
- Machikhiliyan IV
- Maciuc F
- Maev O
- Malde S
- Manca G
- Mancinelli G
- Marconi U
- Marks J
- Martellotti G
- Martens A
- Martin L
- Martinelli M
- Massafferri A
- Matev R
- Mathe Z
- Matteuzzi C
- Maurice E
- Mazurov A
- McCarthy J
- Mcnab A
- McNulty R
- Meadows B
- Meier F
- Meissner M
- Merk M
- Milanes DA
- Minard M-N
- Molina VR
- Monteil S
- Moran D
- Morata JAH
- Morawski P
- Morello MJ
- Mountain R
- Mous I
- Muheim F
- Muresan R
- Muryn B
- Muster B
- Märki R
- Müller K
- Naik P
- Nakada T
- Nandakumar R
- Nasteva I
- Needham M
- Neufeld N
- Nguyen AD
- Nguyen TD
- Nguyen-Mau C
- Nicol M
- Niess V
- Niet R
- Nikitin N
- Nikodem T
- Nomerotski A
- Novoselov A
- Oblakowska-Mucha A
- Obraztsov V
- Oggero S
- Ogilvy S
- Okhrimenko O
- Oldeman R
- Orlandea M
- Owen P
- Pal BK
- Palano A
- Palutan M
- Panman J
- Papanestis A
- Pappagallo M
- Parkes C
- Parkinson CJ
- Passaleva G
- Patel GD
- Patel M
- Patrick GN
- Patrignani C
- Pavel-Nicorescu C
- Pellegrino A
- Penso G
- Perazzini S
- Perego DL
- Perez Trigo E
- Perret P
- Perrin-Terrin M
- Pessina G
- Petridis K
- Petrolini A
- Phan A
- Picatoste Olloqui E
- Pietrzyk B
- Pilař T
- Pinci D
- Playfer S
- Polci F
- Polok G
- Poluektov A
- Polycarpo E
- Popov D
- Popovici B
- Potterat C
- Powell A
- Prisciandaro J
- Pugatch V
- Puig Navarro A
- Punzi G
- Qian W
- Rademacker JH
- Rakotomiaramanana B
- Rangel MS
- Raniuk I
- Rauschmayr N
- Raven G
- Redford S
- Reid MM
- Ricciardi S
- Richards A
- Rinnert K
- Roa Romero DA
- Robbe P
- Rodrigues E
- Rodrigues FF
- Rodriguez Perez P
- Rodriguez JM
- Roiser S
- Romanovsky V
- Romero Vidal A
- Rouvinet J
- Ruf T
- Ruffini F
- Ruiz Valls P
- Ruiz H
- Sabatino G
- Saborido Silva JJ
- Sagidova N
- Sail P
- Saitta B
- Salzmann C
- Sanmartin Sedes B
- Sannino M
- Santacesaria R
- Santamarina Rios C
- Santos DM
- Santovetti E
- Sapunov M
- Sarti A
- Satriano C
- Satta A
- Savrie M
- Savrina D
- Schaack P
- Schiller M
- Schindler H
- Schlupp M
- Schmelling M
- Schmidt B
- Schneider O
- Schopper A
- Schune M-H
- Schwemmer R
- Sciascia B
- Sciubba A
- Seco M
- Semennikov A
- Senderowska K
- Sepp I
- Serra N
- Serrano J
- Seyfert P
- Shapkin M
- Shapoval I
- Shatalov P
- Shcheglov Y
- Shears T
- Shekhtman L
- Shevchenko O
- Shevchenko V
- Shires A
- Skwarnicki T
- Smith E
- Smith M
- Smith NA
- Sokoloff MD
- Soler FJP
- Soomro F
- Souza De Paula B
- Souza D
- Spaan B
- Sparkes A
- Spradlin P
- Stagni F
- Stahl S
- Steinkamp O
- Stoica S
- Stone S
- Storaci B
- Straticiuc M
- Straumann U
- Subbiah VK
- Suárez AD
- Swientek S
- Syropoulos V
- Szczekowski M
- Szczypka P
- Szumlak T
- Sánchez AM
- Teklishyn M
- Teodorescu E
- Teubert F
- The LHCb collaboration
- Thomas C
- Thomas E
- Tico JG
- Tisserand V
- Tobin M
- Tolk S
- Tonelli D
- Topp-Joergensen S
- Torr N
- Torreira AG
- Tostes DM
- Tournefier E
- Tourneur S
- Tran MT
- Tresch M
- Tsaregorodtsev A
- Tsopelas P
- Tuning N
- T’Jampens S
- Ubeda Garcia M
- Ukleja A
- Urner D
- Uwer U
- Vagnoni V
- Valenti G
- van Beuzekom M
- van den Brand J
- van Eijk D
- van Herwijnen E
- van Leerdam J
- van Tilburg J
- Vazquez Gomez R
- Vazquez Regueiro P
- Vecchi S
- Velthuis JJ
- Veltri M
- Veneziano G
- Vesterinen M
- Viaud B
- Vidal XC
- Vieira D
- Vilasis-Cardona X
- Vollhardt A
- Volyanskyy D
- von Loeben J
- Voong D
- Vorobyev A
- Vorobyev V
- Voss H
- Voß C
- Waldi R
- Wallace R
- Wandernoth S
- Wang J
- Ward DR
- Watson NK
- Webber AD
- Websdale D
- Whitehead M
- Wicht J
- Wiechczynski J
- Wiedner D
- Wiggers L
- Wilkinson G
- Williams M
- Williams MP
- Wilson FF
- Wishahi J
- Witek M
- Wotton SA
- Wright S
- Wu S
- Wyllie K
- Xie Y
- Xing F
- Xing Z
- Yang Z
- Young R
- Yuan X
- Yushchenko O
- Yzquierdo AP-C
- Zangoli M
- Zavertyaev M
- Zhang F
- Zhang L
- Zhang WC
- Zhang Y
- Zhelezov A
- Zhokhov A
- Zhong L
- Zvyagin A
- Publication venue
- Springer
- Publication date
- 01/01/2013
- Field of study
A search for CP violation in D + → ϕπ + decays is performed using data collected in 2011 by the LHCb experiment corresponding to an integrated luminosity of 1.0 fb−1 at a centre of mass energy of 7 TeV. The CP -violating asymmetry is measured to be (−0.04 ± 0.14 ± 0.14)% for candidates with K − K + mass within 20 MeV/c 2 of the ϕ meson mass. A search for a CP -violating asymmetry that varies across the ϕ mass region of the D + → K − K + π + Dalitz plot is also performed, and no evidence for CP violation is found. In addition, the CP asymmetry in the D+s→K0Sπ+ decay is measured to be (0.61 ± 0.83 ± 0.14)%
TRY plant trait database - enhanced coverage and open access
- Author
- Aakala T
- Abedi M
- Acosta ATR
- Adamidis GC
- Adamson K
- Aiba M
- Albert CH
- Alcantara JM
- Alcazar CC
- Aleixo I
- Ali H
- Amiaud B
- Ammer C
- Amoroso MM
- Anand M
- Anderson C
- Anh TDL
- Anten N
- Antos J
- Apgaua DMG
- Ashman TL
- Asmara DH
- Asner GP
- Aspinwall M
- Atkin O
- Aubin I
- Baastrup-Spohr L
- Bahalkeh K
- Bahn M
- Baker T
- Baker WJ
- Bakker JP
- Baldocchi D
- Baltzer J
- Banerjee A
- Baranger A
- Barlow J
- Barneche DR
- Baruch Z
- Bastianelli D
- Battles J
- Bauerle W
- Bauters M
- Bazzato E
- Beckmann M
- Beeckman H
- Beierkuhnlein C
- Bekker R
- Belfry G
- Belluau M
- Beloiu M
- Benavides R
- Benomar L
- Berdugo-Lattke ML
- Berenguer E
- Bergamin R
- Bergmann J
- Berner L
- Bernhardt-Romermann M
- Bigler C
- Bjorkman AD
- Blackman C
- Blanco C
- Blonder B
- Blumenthal D
- Bocanegra-Gonzalez KT
- Boeckx P
- Bohlman S
- Bohning-Gaese K
- Boisvert-Marsh L
- Bond W
- Bond-Lamberty B
- Bonisch G
- Boom A
- Boonman CCF
- Bordin K
- Boughton EH
- Boukili V
- Bowman DMJS
- Bravo S
- Brendel MR
- Broadley MR
- Brown KA
- Bruelheide H
- Brumnich F
- Bruun HH
- Bruy D
- Buchanan SW
- Bucher SF
- Buchmann N
- Buitenwerf R
- Bunker DE
- Burger J
- Burrascano S
- Burslem DFRP
- Butterfield BJ
- Byun C
- Caccianiga M
- Cadotte M
- Cailleret M
- Camac J
- Camarero JJ
- Campany C
- Campetella G
- Campos JA
- Cano-Arboleda L
- Canullo R
- Carbognani M
- Carlucci MB
- Carvalho F
- Casanoves F
- Castagneyrol B
- Catford JA
- Cavender-Bares J
- Cerabolini BEL
- Cervellini M
- Chacon-Madrigal E
- Chapin FS
- Chapin K
- Chelli S
- Chen AP
- Chen SC
- Cherubini P
- Chianucci F
- Choat B
- Chung KS
- Chytry M
- Ciccarelli D
- Coll L
- Collins CG
- Conti L
- Coomes D
- Cornelissen JHC
- Cornwell WK
- Corona P
- Coyea M
- Craine J
- Craven D
- Cromsigt JPGM
- Csecserits A
- Cufar K
- Cuntz M
- da Silva AC
- Dahlin KM
- Dainese M
- Dalke I
- Dalle Fratte M
- Danihelka J
- Dannoura M
- Dawson S
- de Beer AJ
- de Dios VR
- De Frutos A
- de Gasper AL
- De Long JR
- Dechant B
- Delagrange S
- Delpierre N
- Derroire G
- Dias AS
- Diaz S
- Diaz-Toribio MH
- Dimitrakopoulos PG
- Dobrowolski M
- Doktor D
- Domingues TF
- Dong N
- Dransfield J
- Dressler S
- Drevojan P
- Duarte L
- Ducouret E
- Dullinger S
- Durka W
- Duursma R
- Dymova O
- E-Vojtko A
- Eckstein RL
- Ejtehadi H
- Elser J
- Emilio T
- Engemann K
- Erfanian MB
- Erfmeier A
- Esquivel-Muelbert A
- Esser G
- Estiarte M
- Fagan WF
- Fagundez J
- Falster DS
- Fan Y
- Fang JY
- Farris E
- Fazlioglu F
- Feng YH
- Fernandez-Mendez F
- Ferrara C
- Ferreira J
- Fidelis A
- Finegan B
- Firn J
- Flowers TJ
- Flynn DFB
- Fontana V
- Forey E
- Forgiarini C
- Francois L
- Frangipani M
- Frank D
- Frenette-Dussault C
- Freschet GT
- Fry EL
- Fyllas NM
- Gachet S
- Gallagher R
- Ganade G
- Ganga F
- Garcia-Palacios P
- Gargaglione V
- Garnier E
- Garrido JL
- Garvizu GS
- Gea-Izquierdo G
- Gibson D
- Gillison AN
- Giroldo A
- Glasenhardt MC
- Gleason S
- Gliesch M
- Goldberg E
- Goldel B
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- Zotz G
- Publication venue
- 'Royal College of Obstetricians & Gynaecologists (RCOG)'
- Publication date
- 01/01/2020
- Field of study
Plant traits-the morphological, anatomical, physiological, biochemical and phenological characteristics of plants-determine how plants respond to environmental factors, affect other trophic levels, and influence ecosystem properties and their benefits and detriments to people. Plant trait data thus represent the basis for a vast area of research spanning from evolutionary biology, community and functional ecology, to biodiversity conservation, ecosystem and landscape management, restoration, biogeography and earth system modelling. Since its foundation in 2007, the TRY database of plant traits has grown continuously. It now provides unprecedented data coverage under an open access data policy and is the main plant trait database used by the research community worldwide. Increasingly, the TRY database also supports new frontiers of trait-based plant research, including the identification of data gaps and the subsequent mobilization or measurement of new data. To support this development, in this article we evaluate the extent of the trait data compiled in TRY and analyse emerging patterns of data coverage and representativeness. Best species coverage is achieved for categorical traits-almost complete coverage for 'plant growth form'. However, most traits relevant for ecology and vegetation modelling are characterized by continuous intraspecific variation and trait-environmental relationships. These traits have to be measured on individual plants in their respective environment. Despite unprecedented data coverage, we observe a humbling lack of completeness and representativeness of these continuous traits in many aspects. We, therefore, conclude that reducing data gaps and biases in the TRY database remains a key challenge and requires a coordinated approach to data mobilization and trait measurements. This can only be achieved in collaboration with other initiatives
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
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- 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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
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- Asner D
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- Assamagan K
- Astbury A
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- Atoian G
- Aubert B
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- Avramidou R
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- Ay C
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- Azuma Y
- Baak MA
- Baccaglioni G
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- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
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- AbouZeid OS
- Abramowicz H
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- Zurzolo G
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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- Musheghyan H
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- Schorlemmer ALS
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- Schroeder TV
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- Schwanenberger C
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- Selbach KE
- Seliverstov DM
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- Serfon C
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- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
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- Shabalina E
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- Shan LY
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- Sjursen TB
- Skottowe HP
- Skovpen KY
- Skubic P
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- Slavicek T
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
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- Smizanska M
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- Subramaniam R
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- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Svatos M
- Swedish S
- Swiatlowski M
- Sykora I
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- Ta D
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- Talyshev AA
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- Tanasijczuk AJ
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- Teoh JJ
- Terada S
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- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thomas JP
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- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
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- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
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- Tisserant S
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- Tsionou D
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turra R
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- Ueda I
- Ueno R
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- Ugland M
- Uhlenbrock M
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- Undrus A
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- Ungaro FC
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- Urbaniec D
- Urquijo P
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- Vacavant L
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- Vachon B
- Valencic N
- Valentinetti S
- Valero A
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- Valladolid Gallego E
- Vallecorsa S
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- van der Geer R
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- van Huysduynen LH
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- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
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- Vermeulen JC
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- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
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- Virzi J
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
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- Vokac P
- Volpi G
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- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
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- Weidberg AR
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- Weingarten J
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- Wells PS
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- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
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- Wilkens HG
- Will JZ
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- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wittig T
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wright M
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- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wyatt TR
- Wynne BM
- Xella S
- Xiao M
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamada M
- Yamaguchi H
- Yamaguchi Y
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
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