402 research outputs found
Transcriptome-based polygenic score links depression-related corticolimbic gene expression changes to sex-specific brain morphology and depression risk
- Author
- Adams MJ
- Baune BT
- Boomsma DI
- Byrne EM
- Castelao E
- Dos Santos FC
- Hamilton SP
- Hariri AR
- Jones I
- Jones LA
- Levinson DF
- Lewis CM
- Lewis G
- Major Depressive Disorder Working Group of the Psychiatric Genom
- McIntosh AM
- Miles AE
- Nikolova YS
- Penninx BWJH
- Perlis RH
- Pistis G
- Potash JB
- Preisig M
- Renteria ME
- Schubert KO
- Shi J
- Sibille E
- Smoller JW
- Uher R
- Weissman MM
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Studies in post-mortem human brain tissue have associated major depressive disorder (MDD) with cortical transcriptomic changes, whose potential in vivo impact remains unexplored. To address this translational gap, we recently developed a transcriptome-based polygenic risk score (T-PRS) based on common functional variants capturing ‘depression-like’ shifts in cortical gene expression. Here, we used a non-clinical sample of young adults (n = 482, Duke Neurogenetics Study: 53% women; aged 19.8 ± 1.2 years) to map T-PRS onto brain morphology measures, including Freesurfer-derived subcortical volume, cortical thickness, surface area, and local gyrification index, as well as broad MDD risk, indexed by self-reported family history of depression. We conducted side-by-side comparisons with a PRS independently derived from a Psychiatric Genomics Consortium (PGC) MDD GWAS (PGC-PRS), and sought to link T-PRS with diagnosis and symptom severity directly in PGC-MDD participants (n = 29,340, 59% women; 12,923 MDD cases, 16,417 controls). T-PRS was associated with smaller amygdala volume in women (t = −3.478, p = 0.001) and lower prefrontal gyrification across sexes. In men, T-PRS was associated with hypergyrification in temporal and occipital regions. Prefrontal hypogyrification mediated a male-specific indirect link between T-PRS and familial depression (b = 0.005, p = 0.029). PGC-PRS was similarly associated with lower amygdala volume and cortical gyrification; however, both effects were male-specific and hypogyrification emerged in distinct parietal and temporo-occipital regions, unassociated with familial depression. In PGC-MDD, T-PRS did not predict diagnosis (OR = 1.007, 95% CI = [0.997–1.018]) but correlated with symptom severity in men (rho = 0.175, p = 7.957 × 10−4) in one cohort (N = 762, 48% men). Depression-like shifts in cortical gene expression have sex-specific effects on brain morphology and may contribute to broad depression vulnerability in men
Graphene membranes for water desalination
- Author
- A Aghigh
- A Akbari
- A Buchsteiner
- A Lee
- A Nicolaï
- AA Balandin
- AK Geim
- B Corry
- B Mi
- B Van der Bruggen
- C Fritzmann
- CJ Russo
- CN Yeh
- D An
- D Cohen-Tanugi
- D Cohen-Tanugi
- D Cohen-Tanugi
- DA Dikin
- DL Gin
- DR Dreyer
- EN Wang
- F Perreault
- G Eda
- G Romanos
- H He
- H Huang
- H Huang
- HM Hegab
- I Jung
- J Abraham
- J Chang
- J Schaep
- J Wang
- J Zhao
- JD Renteria
- JS Bunch
- JW Burress
- K Sint
- K Xu
- KA Mahmoud
- KO Agenson
- KP Lee
- KS Lee
- L Huang
- L Huang
- L Huang
- L Liu
- M Coleman
- M Elimelech
- M Hu
- M Thomas
- MA Shannon
- ME Suk
- MSH Boutilier
- N Wei
- N Wei
- P Goh
- P Sun
- P Sun
- P Sun
- Q Schiermeier
- R Joshi
- R Nair
- R Semiat
- R Tkacz
- S Bae
- S Garaj
- S Homaeigohar
- S Homaeigohar
- S Hong
- S Wu
- S Zhao
- SC O’Hern
- SC O’Hern
- SC O’Hern
- SK Kannam
- SP Koenig
- SP Surwade
- T Carlsson
- T Darden
- V Berry
- W Wang
- WW Liu
- Y Cheng
- Y Han
- Z He
- Z Zheng
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 25/08/2017
- Field of study
Extensive environmental pollution caused by worldwide industrialization and population growth has led to a water shortage. This problem lowers the quality of human life and wastes a large amount of money worldwide each year due to the related consequences. One main solution for this challenge is water purification. State-of-the-art water purification necessitates the implementation of novel materials and technologies that are cost and energy efficient. In this regard, graphene nanomaterials, with their unique physicochemical properties, are an optimum choice. These materials offer extraordinarily high surface area, mechanical durability, atomic thickness, nanosized pores and reactivity toward polar and non-polar water pollutants. These characteristics impart high selectivity and water permeability, and thus provide excellent water purification efficiency. This review introduces the potential of graphene membranes for water desalination. Although literature reviews have mostly concerned graphene's capability for the adsorption and photocatalysis of water pollutants, updated knowledge related to its sieving properties is quite limited.Peer reviewe
Human subcortical brain asymmetries in 15,847 people worldwide reveal effects of age and sex
- Author
- A Abedelahi
- A Colombo
- A Glenthoj
- A Roos
- A Wyciszkiewicz
- A. Marten H. Onnink
- Aiden Corvin
- AL Foundas
- Alejandro Arias-Vásquez
- AM Zimmerman
- Andre F. Marquand
- Andrea Gonzalez Suarez
- Andreas Heinz
- Anna Cattrell
- Anne Uhlmann
- Annerine Roos
- Annette Conzelmann
- Anushree Bose
- Arun L.W. Bokde
- B Fischl
- B Mazoyer
- B Patenaude
- Barbara Franke
- BD Mitchell
- Benedicto Crespo-Facorro
- Benjamin S. Aribisala
- Benson Mwangi
- Bernard Mazoyer
- Bernd Ittermann
- Bernd Kraemer
- Bernhard T. Baune
- C Francks
- CA Szabo
- Carles Soriano-Mas
- Chaim Huyser
- Christian Büchel
- Christine Lochner
- Christopher D. Whelan
- Clyde Francks
- Colm McDonald
- Dan J. Stein
- Daniella Vuletic
- Dara M. Cannon
- David C. Glahn
- David Mataix-Cols
- Dennis van der Meer
- Derek W. Morris
- Derrek P. Hibar
- Dick J. Veltman
- Dimitri Papadopoulos Orfanos
- Dominik Grotegerd
- DP Hibar
- DR McKay
- E Maltbie
- E Mellet
- Elena Shumskaya
- Eric Artiges
- Erik G. Jönsson
- Erlend S. Dørum
- Esther Walton
- F Cendes
- F Chouinard-Decorte
- F Shi
- Fabrice Crivello
- Fleur M. Howells
- Frauke Nees
- FX Castellanos
- G Karlebach
- Ganesan Venkatasubramanian
- Gareth Barker
- Gary Donohoe
- GD Ruxton
- Greig I. de Zubicaray
- Guillén Fernández
- Gunter Schumann
- GW Hynd
- Hans J. Grabe
- Hao Hu
- Harald Kugel
- HE Hulshoff Pol
- Henrik Walter
- Henry Brodaty
- Herta Flor
- Herve Lemaitre
- Hilleke E. Hulshoff Pol
- HS Singer
- HS Soininen
- Hugh Garavan
- I Altarelli
- I Vernaleken
- Ian J. Deary
- Ignacio Martínez-Zalacaín
- Ingrid Agartz
- J Jovicich
- J Willford
- J Xia
- Jair C. Soares
- Jan Buitelaar
- Jan E. Nordvik
- Janardhan YC. Reddy
- Janardhanan C. Narayanaswaamy
- Je-Yeon Yun
- Jean-Luc Martinot
- Jean-Paul Fouche
- Jessica A. Turner
- Jian Xu
- JingJing Zhao
- JL Stein
- JN Giedd
- Joanna Wardlaw
- John Blangero
- José M. Menchón
- JS Lee
- Jun Soo Kwon
- Jürgen Gallinat
- K Amunts
- K Niemann
- K Yamashita
- Karen Mather
- Katharina Wittfeld
- Katie L. McMahon
- Klaus-Peter Lesch
- KY Haaland
- L Almasy
- L Niu
- Lachlan T. Strike
- Lars T. Westlye
- LE DeLisi
- Lianne Schmaal
- LT Eyler
- LT Eyler
- Lucija Abramovic
- Luise Poustka
- M Balconi
- M Borenstein
- Marcel P. Zwiers
- Margaret J. Wright
- Maria Valdés Hernández
- Marie-Laure Paillère Martinot
- Mark E. Bastin
- Martine Hoogman
- Masaki Fukunaga
- MC Corballis
- ME Koran
- Michael Gill
- Michael N. Smolka
- Michelle Luciano
- Miguel E. Renteria
- ML Concha
- MP Bryden
- MR Herbert
- MS Rosenberg
- N Makris
- N Raz
- Natalie A. Royle
- Nathalie Tzourio-Mazoyer
- Neda Jahanshad
- Neeltje E.M . van Haren
- Nhat Trung Doan
- Nicholas G. Martin
- Nicola J. Armstrong
- Nils Opel
- Nora C. Vetter
- Odile A. van den Heuvel
- OE Titova
- Ole A. Andreassen
- Oliver Gruber
- Omar Mothersill
- Pascual Sánchez-Juan
- Patricia J. Conrod
- Paul M. Thompson
- Paul Pauli
- Penny Gowland
- Perminder Sachdev
- PG Hepper
- Pieter J. Hoekstra
- PR Szeszko
- Premika S.W. Boedhoe
- RA Morey
- Rene S. Kahn
- RM Willems
- Robert Whelan
- Roberto Roiz-Santiáñez
- Roberto Toro
- Roel Ophoff
- Rosa Ayesa-Arriola
- Ryota Hashimoto
- S Kloppel
- Samantha Brooks
- Samuel R. Mathias
- Sarah E. Medland
- Sarah Jurk
- Saskia Hagenaars
- Silvia Brem
- Simon E. Fisher
- Sinead Kelly
- Sonja M.C. de Zwarte
- Stefan Ehrlich
- Susana Munoz Maniega
- Susanne Walitza
- SY Zhou
- Sylvane Desrivières
- T Guadalupe
- T Guadalupe
- Takashi Nakamae
- Theo G. M. vanErp
- Thomas Espeseth
- Thomas Wolfers
- Tobias Banaschewski
- Tobias U. Hauser
- Tomohiro Nakao
- Tomáš Paus
- Tulio Guadalupe
- Udo Dannlowski
- Uli Bromberg
- V Oertel-Knochel
- VA Kovalev
- Vatche G. Baboyan
- Vince D. Calhoun
- Vincent Frouin
- Volker Arolt
- VS Caviness Jr.
- WD Hopkins
- Wei Wen
- X Han
- Xiufeng Xu
- Yoshinari Abe
- Yuqi Cheng
- Zhen Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
The two hemispheres of the human brain differ functionally and structurally. Despite over a century of research, the extent to which brain asymmetry is influenced by sex, handedness, age, and genetic factors is still controversial. Here we present the largest ever analysis of subcortical brain asymmetries, in a harmonized multi-site study using meta-analysis methods. Volumetric asymmetry of seven subcortical structures was assessed in 15,847 MRI scans from 52 datasets worldwide. There were sex differences in the asymmetry of the globus pallidus and putamen. Heritability estimates, derived from 1170 subjects belonging to 71 extended pedigrees, revealed that additive genetic factors influenced the asymmetry of these two structures and that of the hippocampus and thalamus. Handedness had no detectable effect on subcortical asymmetries, even in this unprecedented sample size, but the asymmetry of the putamen varied with age. Genetic drivers of asymmetry in the hippocampus, thalamus and basal ganglia may affect variability in human cognition, including susceptibility to psychiatric disorders
Exploration of Shared Genetic Architecture Between Subcortical Brain Volumes and Anorexia Nervosa
- Author
- Abramovic L
- Adams HHH
- Adan R
- Agartz I
- Alfredsson L
- Alhusaini S
- Almasy L
- Ames D
- Andersson M
- Ando T
- Andreassen O
- Andreassen OA
- Anttila V
- Arepalli S
- Arias-Vasquez A
- Aribisala BS
- Armstrong NJ
- Aschauer H
- Ashbrook DG
- Assareh AA
- Athanasiu L
- Baker J
- Barrett J
- Bastin ME
- Batury V-L
- Becker JT
- Bencko V
- Bergen A
- Bernard M
- Berrettini W
- Birgegard A
- Bis JC
- Blangero J
- Bohlken MM
- Boks MP
- Boni C
- Boomsma DI
- Bralten J
- Brandt H
- Breen G
- Brodaty H
- Brouwer RM
- Brown AA
- Brunner HG
- Buckner RL
- Buitelaar JK
- Bulayeva KB
- Bulik CM
- Bulik CM
- Bulik-Sullivan B
- Burghardt R
- Cahn W
- Calhoun VD
- Cannon DM
- Carlberg L
- Carless MA
- Cassina M
- Cavalleri GL
- Chakravarty MM
- Chauhan G
- Chen Q
- Cheung J
- Ching CRK
- Cichon CCS
- Cichon S
- Clementi M
- Cohen-Woods S
- Coleman J
- Cone R
- Cookson MR
- Corvin A
- Courtet P
- Crawford S
- Crespo-Facorro B
- Crow S
- Crowley J
- Cuellar-Partida G
- Curran JE
- Czisch M
- Dale AM
- Danner U
- Davies GE
- Davis O
- de Geus EJC
- de Zubicaray GI
- de Zwaan M
- Deary IJ
- Dedoussis G
- Degortes D
- Delanty N
- Den Braber A
- Depondt C
- DeSocio J
- Desrivieres S
- Dick D
- Dikeos D
- Dillman A
- Dina C
- Ding B
- Djurovic S
- Dmitrzak-Weglarz M
- Docampo E
- Donohoe G
- Drevets WC
- Duggirala R
- Duncan L
- Dyer TD
- Ebling M
- Egberts K
- Ehrlich S
- Ehrlich S
- Ehrlich S
- Erk S
- Escaramis G
- Esko T
- Espeseth T
- Espeseth T
- Estivill X
- Favaro A
- Fedko IO
- Fernandez G
- Fernandez-Aranda F
- Ferrucci L
- Fichter M
- Finan C
- Fischer K
- Fischl B
- Fisher SE
- Floyd J
- Focker M
- Foretova L
- Foroud TM
- Forzan M
- Fox C
- Fox PT
- Francks C
- Franke B
- Franklin C
- Fukunaga M
- Gallinger VGS
- Gambaro G
- Gaspar H
- Gibbs JR
- Giddaluru S
- Giegling I
- Glahn DC
- Goldman AL
- Goldstein J
- Gollub RL
- Gonidakis F
- Goring HHH
- Gorwood P
- Grabe HJ
- Gratacos M
- Green RC
- Greve D
- Grimm O
- Gruber O
- Guadalupe T
- Gudnason V
- Guelfi S
- Guillaume S
- Guo Y
- Hager R
- Hakobjan MMH
- Hakonarson H
- Halmi K
- Hansell NK
- Hardy J
- Harrison R
- Hartberg CB
- Hartman CA
- Hashimoto R
- Hass J
- Hatzikotoulas K
- Haukvik UK
- Hauser J
- Hebebrand J
- Hegenscheid K
- Heinz A
- Heister AJGAM
- Helder S
- Hendriks J
- Herms S
- Hernandez DG
- Hernandez MCV
- Herpertz-Dahlmann B
- Herzog W
- Heslenfeld DJ
- Hibar D
- Hibar DP
- Hilliard C
- Hinney A
- Ho B-C
- Hoekstra PJ
- Hoffmann W
- Hohn D
- Holmes AJ
- Holsboer F
- Homuth G
- Hoogman M
- Hosten N
- Hottenga J-J
- Huckins L
- Hudson J
- Huemer J
- Ikeda M
- Ikram MA
- Imgart H
- Inoko H
- Jack CR
- Jahanshad N
- Jahanshad N
- Jamain SJS
- Janout V
- Janowitz D
- Jenkinson M
- Jia T
- Jimenez-Murcia S
- Johnson C
- Johnson R
- Jonsson EG
- Jordan J
- Julia A
- Jureus A
- Kahn RS
- Kalsi G
- Kaminska D
- Kanai R
- Kaplan A
- Kaprio J
- Karhunen L
- Karwautz A
- Kas M
- Kasperaviciute D
- Kaye W
- Keil M
- Kennedy J
- Kennedy M
- Kent JW
- Keski-Rahkonen A
- Kiezebrink K
- Kim S
- Kim Y-R
- Klareskog L
- Klein M
- Kloszewska I
- Klump K
- Knudsen GP
- Kochunov P
- Koeleman B
- Koubek D
- Kraemer B
- Kwok JB
- La Via M
- Landen M
- Launer LJ
- Lawrie SM
- Le Hellard S
- Le Hellard S
- Leboyer M
- Lee PH
- Levitan R
- Li D
- Lichtenstein P
- Liewald DCM
- Lilenfeld L
- Lissowska J
- Liu X
- Longo DL
- Longstreth WT
- Loohuis LMO
- Lopez LM
- Lovestone S
- Lu L
- Luciano M
- Lundervold A
- Macare C
- Magistretti P
- Maj M
- Makkinje RRR
- Mannik K
- Marsal S
- Martin N
- Martin NG
- Matarin M
- Mather KA
- Mattay VS
- Mattheisen M
- Mattingsdal M
- Mazoyer B
- McDevitt S
- McDonald C
- McGuffin P
- McIntosh AM
- Mckay DR
- McMahon FJ
- McMahon KL
- Mecocci P
- Medland SE
- Meisenzahl E
- Melle I
- Merl E
- Metspalu A
- Meulenbelt I
- Meyer-Lindenberg A
- Micali N
- Milaneschi Y
- Mitchell J
- Mitchell K
- Mohnke S
- Monteleone AM
- Monteleone P
- Montgomery G
- Montgomery GW
- Morris DW
- Mortensen P
- Mostert JC
- Mueller T
- Mueller-Myhsok B
- Muhleisen TW
- Munn-Chernoff M
- Naber MAM
- Nacmias B
- Nalls MA
- Nauck M
- Navratilova M
- Needham M
- Nho K
- Nichols TE
- Nilsson I
- Nilsson LG
- Norring C
- Nothen MM
- Ntalla I
- Nugent AC
- Nyberg L
- Nyquist P
- O'Toole J
- Ohi K
- Olvera RL
- Ophoff R
- Ophoff RA
- Palotie A
- Pandolfo M
- Pantel J
- Papezova H
- Papmeyer M
- Paus T
- Pausova Z
- Penninx BWJH
- Perez-Iglesias R
- Perica VB
- Pike GB
- Pinto RPD
- Pol HEH
- Potkin SG
- Putz B
- Rabionet R
- Raevuori A
- Rajewski A
- Ramasamy A
- Ramoz N
- Rayner NW
- Reichborn-Kjennerud T
- Reinvang I
- Renteria ME
- Reppermund S
- Ricca V
- Rietschel M
- Ripatti S
- Ripke S
- Risacher SL
- Ritschel F
- Roberts M
- Roffman JL
- Roiz-Santianez R
- Romanczuk-Seiferth N
- Rose EJ
- Rosen GD
- Rotondo A
- Rujescu D
- Rujescu D
- Rybakowski F
- Ryten M
- Sachdev PS
- Salami A
- Samann PG
- Santonastaso P
- Satizabal CL
- Saykin AJ
- Scherag A
- Scherer S
- Schmaal L
- Schmidt H
- Schmidt R
- Schmidt U
- Schnell K
- Schofield PR
- Schork AJ
- Schork N
- Schosser A
- Schumann G
- Scott L
- Seiler S
- Seitz J
- Seitz J
- Seshadri S
- Shen L
- Shin J
- Simmons A
- Singleton A
- Sisodiya SM
- Slachtova L
- Sladek R
- Slagboom PE
- Slof-Op't Landt M
- Slopien A
- Smith C
- Smith T
- Smoller JW
- Soininen H
- Soranzo N
- Sorbi S
- Southam L
- Sprooten E
- Steen V
- Steen VM
- Stein JL
- Strengman E
- Strike LT
- Strober M
- Sussmann JE
- Szatkiewicz J
- Szeszenia-Dabrowska N
- Tachmazidou I
- Tenconi E
- Teumer A
- Thalamuthu A
- Thompson PM
- Thompson PM
- Thornton L
- Toga AW
- Toro R
- Tortorella A
- Tozzi F
- Trabzuni D
- Traynor BJ
- Treasure J
- Troncoso J
- Tschop M
- Tsitsika A
- Turner JA
- Tziouvas K
- van Bokhoven H
- van der Brug M
- van der Lee SJ
- van der Marel SSL
- van der Wee NJA
- van Donkelaar MMJ
- van Duijn CM
- van Eijk KR
- van Elburg A
- van Furth E
- van Haren NEM
- van Hulzen KJE
- van Tol M-J
- van't Ent D
- Veltman DJ
- Vinke LN
- Volzke H
- Wade T
- Wagner G
- Walter H
- Walters R
- Walters RK
- Walton E
- Walton E
- Walton E
- Wardlaw JM
- Wassink TH
- Watson H
- Weale ME
- Weinberger DR
- Weiner MW
- Wen W
- Westlye LT
- Westman E
- Whelan CD
- White T
- Wichmann H-E
- Widen E
- Williams RW
- Winkler AM
- Wittfeld K
- Woldehawariat G
- Wolf C
- Woodside DB
- Wright MJ
- Xue L
- Yanek LR
- Yanovski J
- Yao S
- Yilmaz Z
- Yilmaz Z
- Zerwas S
- Zielke RH
- Zipfel S
- Zonderman AB
- Zwiers MP
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/07/2019
- Field of study
In MRI scans of patients with anorexia nervosa (AN), reductions in brain volume are often apparent. However, it is unknown whether such brain abnormalities are influenced by genetic determinants that partially overlap with those underlying AN. Here, we used a battery of methods (LD score regression, genetic risk scores, sign test, SNP effect concordance analysis, and Mendelian randomization) to investigate the genetic covariation between subcortical brain volumes and risk for AN based on summary measures retrieved from genome-wide association studies of regional brain volumes (ENIGMA consortium, n = 13,170) and genetic risk for AN (PGC-ED consortium, n = 14,477). Genetic correlations ranged from − 0.10 to 0.23 (all p > 0.05). There were some signs of an inverse concordance between greater thalamus volume and risk for AN (permuted p = 0.009, 95% CI: [0.005, 0.017]). A genetic variant in the vicinity of ZW10, a gene involved in cell division, and neurotransmitter and immune system relevant genes, in particular DRD2, was significantly associated with AN only after conditioning on its association with caudate volume (pFDR = 0.025). Another genetic variant linked to LRRC4C, important in axonal and synaptic development, reached significance after conditioning on hippocampal volume (pFDR = 0.021). In this comprehensive set of analyses and based on the largest available sample sizes to date, there was weak evidence for associations between risk for AN and risk for abnormal subcortical brain volumes at a global level (that is, common variant genetic architecture), but suggestive evidence for effects of single genetic markers. Highly powered multimodal brain- and disorder-related genome-wide studies are needed to further dissect the shared genetic influences on brain structure and risk for AN
Altered structural brain asymmetry in autism spectrum disorder in a study of 54 datasets
- Author
- A Christakou
- A Retico
- AK Lindell
- AL Rysstad
- AS Nunes
- AW Toga
- B Fischl
- B Tick
- Boedhoe
- Boedhoe
- C Ecker
- C Francks
- C Lord
- C Lord
- CC Dougherty
- CO Carlisi
- CO Carlisi
- D Li
- D van Rooij
- DL Floris
- E Conti
- E Courchesne
- E Courchesne
- E Loth
- F Kurth
- F Leroy
- G Xu
- H Watanabe
- HG Trontel
- I Gori
- JA Nielsen
- JM Chambers
- KS Button
- L Gabard-Durnam
- L Schmaal
- L Schmaal
- L Wei
- LJ Rogers
- LQ Uddin
- M Elsabbagh
- M Hoogman
- M Hoogman
- M Langen
- ME Raichle
- ME Renteria
- MR Munafo
- MS Panizzon
- MW Logue
- N Geschwind
- N Rommelse
- NM Kleinhans
- P Markou
- R Adolphs
- RA Carper
- RC Cardinale
- RM Joseph
- RS Desikan
- S Haar
- S Lucibello
- SG Costafreda
- SR Sharma
- SS Jeste
- T Guadalupe
- TA Knaus
- TA Knaus
- TGM van Erp
- V Biberacher
- V Duboc
- XZ Kong
- Y Benjamini
- Y Jiao
- Y Kawasaki
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Altered structural brain asymmetry in autism spectrum disorder (ASD) has been reported. However, findings have been inconsistent, likely due to limited sample sizes. Here we investigated 1,774 individuals with ASD and 1,809 controls, from 54 independent data sets of the ENIGMA consortium. ASD was significantly associated with alterations of cortical thickness asymmetry in mostly medial frontal, orbitofrontal, cingulate and inferior temporal areas, and also with asymmetry of orbitofrontal surface area. These differences generally involved reduced asymmetry in individuals with ASD compared to controls. Furthermore, putamen volume asymmetry was significantly increased in ASD. The largest case-control effect size was Cohen’s d = −0.13, for asymmetry of superior frontal cortical thickness. Most effects did not depend on age, sex, IQ, severity or medication use. Altered lateralized neurodevelopment may therefore be a feature of ASD, affecting widespread brain regions with diverse functions. Large-scale analysis was necessary to quantify subtle alterations of brain structural asymmetry in ASD
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
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- Zhemchugov A
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Search for pair production of squarks or gluinos decaying via sleptons or weak bosons in final states with two same-sign or three leptons with the ATLAS detector
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- Zenger DT
- Zenin O
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- Zerwas D
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- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 15/02/2024
- Field of study
A search for pair production of squarks or gluinos decaying via sleptons or weak bosons is reported. The search targets a final state with exactly two leptons with same-sign electric charge or at least three leptons without any charge requirement. The analysed data set corresponds to an integrated luminosity of 139 fb−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Multiple signal regions are defined, targeting several SUSY simplified models yielding the desired final states. A single control region is used to constrain the normalisation of the WZ + jets background. No significant excess of events over the Standard Model expectation is observed. The results are interpreted in the context of several supersymmetric models featuring R-parity conservation or R-parity violation, yielding exclusion limits surpassing those from previous searches. In models considering gluino (squark) pair production, gluino (squark) masses up to 2.2 (1.7) TeV are excluded at 95% confidence level
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- 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
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
- 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
- Alunno Camelia E
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Aranzabal N
- Araujo Ferraz V
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
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- Zhemchugov A
- Zheng Z
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
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- Zenger DT
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- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
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- Zhou Y
- Zhu CG
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- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
HE-LHC: The High-Energy Large Hadron Collider: Future Circular Collider Conceptual Design Report Volume 4
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abelleira Fernandez J
- Abramov A
- Aburaia M
- Acar AO
- Adzic PR
- Agrawal P
- Aguilar-Saavedra JA
- Aguilera-Verdugo JJ
- Aiba M
- Aichinger I
- Aielli G
- Akay A
- Akhundov A
- Aksakal H
- Albacete JL
- Albergo S
- Alekou A
- Aleksa M
- Aleksan R
- Alemany Fernandez RM
- Alexahin Y
- Alia RG
- Alioli S
- Alipour Tehrani N
- Allanach BC
- Allport PP
- Altinli M
- Altmannshofer W
- Ambrosio G
- Amorim D
- Amstutz O
- Anderlini L
- Andreazza A
- Andreini M
- Andriatis A
- Andris C
- Andronic A
- Angelucci M
- Antinori F
- Antipov SA
- Antonelli M
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- Anulli F
- Apolinario L
- Apollinari G
- Apollonio A
- Appeloe D
- Appleby RB
- Apyan A
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- Arbey A
- Arbuzov A
- Arduini G
- Ari V
- Arias S
- Armesto N
- Arnaldi R
- Arsenyev SA
- Arzeo M
- Asai S
- Aslanides E
- Assmann RW
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- Atieh S
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- Auchmann B
- Audurier A
- Aull S
- Aumon S
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- Avino F
- Avrillaud G
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- Azatov A
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- Publication venue
- SPRINGER HEIDELBERG
- Publication date
- 01/07/2019
- Field of study
In response to the 2013 Update of the European Strategy for Particle Physics (EPPSU), the Future Circular Collider (FCC) study was launched as a world-wide international collaboration hosted by CERN. The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the third volume of the FCC Conceptual Design Report, devoted to the hadron collider FCC-hh. It summarizes the FCC-hh physics discovery opportunities, presents the FCC-hh accelerator design, performance reach, and staged operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation. Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the FCC-hh design aims at significantly extending the energy frontier to 100 TeV. Its unprecedented centre-of-mass collision energy will make the FCC-hh a unique instrument to explore physics beyond the Standard Model, offering great direct sensitivity to new physics and discoveries
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