420 research outputs found
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adolphi R
- Adzic P
- Afaq MA
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed W
- Ahuja S
- Aisa D
- Aisa S
- Akchurin N
- Akgun B
- Akgun U
- Akimenko S
- Akin IV
- Alagoz E
- Alampi G
- Albajar C
- Albayrak EA
- Alberdi J
- Albergo S
- Albert E
- Albrow M
- Alexander J
- Alidra M
- Aliev T
- Allfrey P
- Almeida N
- Altenhofer G
- Altsybeev I
- Alver B
- Alverson G
- Alves GA
- Amaglobeli N
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Ananthan B
- Anastassov A
- Andelin D
- Anderson M
- Andrea J
- Andreev V
- Andreev Y
- Anghel IM
- Anguelov T
- Anh T. Vu
- Anisimov A
- Antillon E
- Antipov P
- Antonelli L
- Anttila E
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arnold B
- Arora S
- Artamonov A
- Asaadi J
- Asghar MI
- Ashby S
- Askew A
- Atac M
- Atramentov O
- Auffray E
- Aurisano A
- Autermann C
- Avery P
- Avetisyan A
- Avila C
- Awan MIM
- Ayan AS
- Ayhan A
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babb J
- Babucci E
- Baccaro S
- Bacchetta N
- Bacchi W
- Bachtis M
- Baden D
- Badgett W
- Baechler J
- Baer H
- Baesso P
- Baffioni S
- Bagby L
- Bagliesi G
- Bahk SY
- Bailleux D
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- Bainbridge R
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- Bakken JA
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- Baldin B
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- Banerjee S
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- Bansal S
- Banzuzi K
- Barashko V
- Barbagli G
- Barberis E
- Barbone L
- Barcala JM
- Barcellan L
- Bard R
- Bargassa P
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- Barnett BA
- Barney D
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- Bartalini P
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- Battilana C
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- Belforte S
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- Bellinger JN
- Belotelov I
- Benaglia A
- Bencze G
- Bendavid J
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- Benedetti D
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- Benvenuti AC
- Berengueres JOL
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- Besson A
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- Beuselinck R
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- Bhatti A
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- Bornheim A
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- Calderon A
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- Calvo E
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- Camanzi B
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- Campderros JD
- Campi D
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- Capiluppi P
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- Castello R
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- Cattai A
- Caudron J
- Cavallari F
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- Cebra D
- Cepeda M
- Cerati GB
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- Cerizza G
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- Ceron C
- Cerrada M
- Chabert EC
- Chan M
- Chandra A
- Chang P
- Chang S
- Chang YH
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chatelain JP
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Chauvey M
- Checchia P
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- Chekhovsky V
- Chen EA
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- Chertok M
- Chetluru V
- Cheung HWK
- Chien CY
- Chierici R
- Chiochia V
- Chiorboli M
- Chipaux R
- Chiumarulo F
- Chlebana F
- Choi M
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- Choudhary BC
- Choudhury RK
- Christian G
- Christiansen T
- Chtchipounov L
- Chuang SH
- Chung J
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- Chung YS
- Churin I
- Chwalek T
- Cihangir S
- Cimmino A
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- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
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- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
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- Colling D
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- Contardo D
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- Cooper SI
- Cordonnier AM
- Cortabitarte RV
- Cossutti F
- Costa M
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- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
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- Creanza D
- Cremaldi LM
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- Crotty I
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- Cumalat JP
- Cuplov V
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- Cuscela G
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- D'Angelo P
- D'Antone I
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- Di Giovanni GP
- Di Marco E
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- Dimitrov A
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- Djordjevic M
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- Dutta D
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- Dvornikov O
- Dykstra D
- Dyulendarova M
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- Zachariadou A
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Genome-wide association study identifies six new loci influencing pulse pressure and mean arterial pressure.
- Author
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- Vasan Ramachandran S.
- Verwoert GC
- Verwoert Germaine C.
- Viikari Jorma
- Vita JA
- Vitart V
- Vitart Veronique
- Voight BF
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- Voight Benjamin F
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- Vollenweider P
- Vollenweider Peter
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- Waeber Gérard
- Wagner AK
- Wain Louise V.
- Waksman R
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- Wallace C
- Wallace C
- Wang TJ
- Wang TJ
- Wang W
- Wang Thomas J.
- Wareham NJ
- Wareham Nicholas J.
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- Watkins Hugh
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- Webster Rebecca J.
- Wells GA
- Wells GA
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- Whitteman J
- Wichmann HE
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- Wichmann HE
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- Witteman JC
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- Witteman Jacqueline C. M.
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- Wright Alan F.
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- Yasmin
- Zaboli G
- Zeginigg Marion
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- Zeller T
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- Zerres K
- Zgaga L
- Zhang W
- Zhang Feng
- Zhang Weihua
- Zhao Jing Hua
- Ziegler A
- Ziegler A
- Ziegler A
- Ziegler A
- Ziegler A
- Ziegler A
- Zillikens MC
- Zitting Paavo
- Zweiker R
- Publication venue
- Nat Genet
- Publication date
- 01/01/2011
- Field of study
Numerous genetic loci have been associated with systolic blood pressure (SBP) and diastolic blood pressure (DBP) in Europeans. We now report genome-wide association studies of pulse pressure (PP) and mean arterial pressure (MAP). In discovery (N = 74,064) and follow-up studies (N = 48,607), we identified at genome-wide significance (P = 2.7 × 10(-8) to P = 2.3 × 10(-13)) four new PP loci (at 4q12 near CHIC2, 7q22.3 near PIK3CG, 8q24.12 in NOV and 11q24.3 near ADAMTS8), two new MAP loci (3p21.31 in MAP4 and 10q25.3 near ADRB1) and one locus associated with both of these traits (2q24.3 near FIGN) that has also recently been associated with SBP in east Asians. For three of the new PP loci, the estimated effect for SBP was opposite of that for DBP, in contrast to the majority of common SBP- and DBP-associated variants, which show concordant effects on both traits. These findings suggest new genetic pathways underlying blood pressure variation, some of which may differentially influence SBP and DBP
Mean-field transport theory for the two-flavour NJL model
- Author
- Abbiendi G
- Abe T
- Abramowicz H
- Acosta D
- Adamczyk L
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- Amelung C
- Anselmo F
- Antonioli P
- Arneodo M
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- Bashkirov V
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- Bauerdick LAT
- Bednarek B
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- Bertolin A
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- Bienlein JK
- Blaikley HE
- Bohnet I
- Bokel C
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- Botje M
- Breitweg J
- Briskin G
- Brock I
- Bromley JT
- Brook NH
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- Brümmer N
- Bukowy M
- Bulmahn J
- Burow BD
- Bussey PJ
- Butterworth I
- Butterworth JM
- Bylsma B
- Caldwell A
- Campbell-Robson S
- Capua M
- Cara Romeo G
- Carlin R
- Cartiglia N
- Cases G
- Cashmore RJ
- Castellini G
- Catterall CD
- Chapin D
- Chlebana F
- Chwastowski J
- Ciborowski J
- Cifarelli L
- Cindolo F
- Cirio R
- Cloth P
- Coböken K
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- Cole JE
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- Cross R
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- Devenish RCE
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- Fusayasu T
- Galea R
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- Gialas I
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- Grzelak G
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- Hong SJ
- Horstmann D
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- Hughes VW
- Hung BHY
- Hung LW
- Iacobucci G
- Iannotti L
- Iga Y
- Inuzuka M
- Ishii T
- Jakob H-P
- Jeleń K
- Jing Z
- Johnson KF
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- Katz UF
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- Koch W
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- Korotkova NA
- Korzhavina IA
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- Lukina OY
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- Matsushita T
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- Pelucchi F
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- Roff DG
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- Rulikowska-Zarebska E
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- Suzuki I
- Talaga RL
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- Teuscher RJ
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- Wedemeyer R
- Westphal D
- Whitmore JJ
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- Zamora Garcia Y
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- Zeuner W
- Zhang H
- Zhu Q
- Zichichi A
- Zotkin SA
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1997
- Field of study
By making decomposition of the Wigner function simultaneously in both the
spinor and the isospin spaces we derive a set of kinetic equations for the
quark distribution functions and the spin densities. A detailed analysis of the
consequences imposed by the chiral invariance on the form of the transport
equations is presented.Comment: Revtex, 25 pages, no figure
Evidence of causal effect of major depression on alcohol dependence: findings from the psychiatric genomics consortium
- Author
- Abdellaoui A
- Adams MJ
- Adkins AE
- Adkins DE
- Agee M
- Agerbo E
- Agrawal A
- Air TM
- Alanne-Kinnunen M
- Aliev F
- Alipanahi B
- Andlauer TMF
- Arolt V
- Auton A
- Bacanu S-A
- Baekvad-Hansen M
- Batzler A
- Baune BT
- Beekman AFT
- Bell RK
- Berger K
- Bertelsen S
- Biernacka JM
- Bierut LJ
- Bigdeli TB
- Binder EB
- Blackwood DRH
- Boardman JD
- Boden JM
- Boomsma D
- Borglum AD
- Breen G
- Brown SA
- Bryc K
- Bryois J
- Bucholz KK
- Buttenschon HN
- Bybjerg-Grauholm J
- Byrne EM
- Cai N
- Castelao E
- Chen D
- Chen L-S
- Choi D-S
- Chou Y-L
- Christensen JH
- Cichon S
- Clarke T-K
- Coleman JIR
- Colodro-Conde L
- Copeland WE
- Costello EJ
- Couvy-Duchesne B
- Craddock N
- Crawford GE
- Crowley CA
- Culverhouse RC
- Dahmen N
- Dannlowski U
- Dashti HS
- Davies G
- de Geus ECJ
- de Wit H
- Deary IJ
- Degenhardt F
- Degenhardt L
- DePaulo JR
- Derks EM
- Diazgranados N
- Dick DM
- Direk N
- Docherty AR
- Dolan C
- Domenici E
- Domingue BW
- Domschke K
- Dunn EC
- Edenberg HJ
- Edwards AC
- Eley TC
- Elson SL
- Eriksson JG
- Eriksson N
- Escott-Price V
- Esko T
- Farrer LA
- Finucane HK
- Fontanillas P
- Foo JC
- Foroud TM
- Forstner AJ
- Fox L
- Frank J
- Frye MA
- Furlotte NA
- Gabel W
- Gaspar HA
- Gelernter J
- Gerring Z
- Giegling I
- Gill M
- Gillespie NA
- Giusti-Rodriguez P
- Goate AM
- Goes FS
- Goldman D
- Gordon S
- Gordon SD
- Grabe HJ
- Grove J
- Grucza RA
- Hack LM
- Hall LS
- Hamilton SP
- Hancock DB
- Hannon E
- Hansen CS
- Hansen TF
- Harris KM
- Hartmann AM
- Hartz SM
- Hayward C
- Heath AC
- Heilmann-Heimbach S
- Herms S
- Hesselbrock V
- Hewitt JK
- Hickie IB
- Hinds DA
- Hodgkinson C
- Hoffmann P
- Homuth G
- Hopfer CJ
- Horn C
- Horwood J
- Hottenga J-J
- Hottenga JJ
- Hougaard DM
- Hu M
- Huber KE
- Hyde CL
- Iacono W
- Ising M
- Jansen R
- Jin F
- Johnson EC
- Johnson EO
- Jorgenson E
- Kaprio JA
- Karpyak VM
- Kendler KS
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- Kiadeh FHF
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- Lai D
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- MacKinnon DF
- Madden PAF
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- Maes HH
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- Meyers JL
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- Sinnamon GBC
- Smit JH
- Smith DJ
- Smoller JW
- Soyka M
- Stallings MC
- Stefansson H
- Stefansson K
- Steinberg S
- Stockmeier CA
- Streit F
- Strohmaier J
- Sullivan PF
- Tansey KE
- Tarter RE
- Teismann H
- Teumer A
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- Thomson PA
- Thorgeirsson TE
- Tian C
- Tiemeier H
- Traylor M
- Treutlein J
- Trubetskoy V
- Trzaskowski M
- Tung JY
- Uher R
- Uitterlinden AG
- Umbricht D
- Vacic V
- Van der Auwera S
- van Hemert AM
- Vanyukov MM
- Viktorin A
- Visscher PM
- Volzke H
- Vrieze S
- Wall TL
- Walters RK
- Wang J-C
- Wang Y
- Webb BT
- Wedow R
- Weinsheimer SM
- Weissman MM
- Wellmann J
- Werge T
- Wetherill L
- Whitfield JB
- Willemsen G
- Wills AG
- Wilson CH
- Winslow AR
- Witt S
- Witt SH
- Wodarz N
- Wray NR
- Wu Y
- Xi HS
- Yang J
- Zhang F
- Zhao H
- Zill P
- Publication venue
- CAMBRIDGE UNIV PRESS
- Publication date
- 01/05/2019
- Field of study
BACKGROUND
Despite established clinical associations among major depression (MD), alcohol dependence (AD), and alcohol consumption (AC), the nature of the causal relationship between them is not completely understood. We leveraged genome-wide data from the Psychiatric Genomics Consortium (PGC) and UK Biobank to test for the presence of shared genetic mechanisms and causal relationships among MD, AD, and AC.
METHODS
Linkage disequilibrium score regression and Mendelian randomization (MR) were performed using genome-wide data from the PGC (MD: 135 458 cases and 344 901 controls; AD: 10 206 cases and 28 480 controls) and UK Biobank (AC-frequency: 438 308 individuals; AC-quantity: 307 098 individuals).
RESULTS
Positive genetic correlation was observed between MD and AD (rgMD−AD = + 0.47, P = 6.6 × 10−10). AC-quantity showed positive genetic correlation with both AD (rgAD−AC quantity = + 0.75, P = 1.8 × 10−14) and MD (rgMD−AC quantity = + 0.14, P = 2.9 × 10−7), while there was negative correlation of AC-frequency with MD (rgMD−AC frequency = −0.17, P = 1.5 × 10−10) and a non-significant result with AD. MR analyses confirmed the presence of pleiotropy among these four traits. However, the MD-AD results reflect a mediated-pleiotropy mechanism (i.e. causal relationship) with an effect of MD on AD (beta = 0.28, P = 1.29 × 10−6). There was no evidence for reverse causation.
CONCLUSION
This study supports a causal role for genetic liability of MD on AD based on genetic datasets including thousands of individuals. Understanding mechanisms underlying MD-AD comorbidity addresses important public health concerns and has the potential to facilitate prevention and intervention efforts
Genetic variants in novel pathways influence blood pressure and cardiovascular disease risk.
- Author
- Abecasis GR
- Abecasis Gonçalo R.
- Absher D
- Adair Linda S.
- Adeyemo Adebowale
- Aherrahrou Z
- Ahmadi KR
- Ala-Korpela Mika
- Alexander Myriam
- Altshuler D
- Altshuler David
- Amin Najaf
- Andersen K
- Aragam J
- Arfan Ikram M.
- Arking DE
- Arking Dan E.
- Arnett D
- Arora Pankaj
- Artigas Maria Soler
- Aspelund T
- Aspelund Thor
- Assimes TL
- Atkinson EJ
- Aulchenko YS
- Aulchenko YS
- Aulchenko YS
- Aulchenko Yurii
- Badola S
- Bakker SJ
- Bakker Stephan J. L.
- Ball SG
- Balmforth AJ
- Bandinelli Stefania
- Barbalic M
- Barroso Inês
- Beckmann J
- Beckmann Jacques S.
- Beilby John P.
- Benjamin E
- Benjamin EJ
- Bergman Richard N.
- Bergmann Sven
- Bickel C
- Bilo HJ
- Bis J
- Bis JC
- Bis JC
- Bis Joshua C.
- Blankenberg S
- Blankenberg S
- Blankenberg S
- Blettner M
- Boban M
- Bochud M
- Bochud Murielle
- Boehnke Michael
- Boerwinkle E
- Boerwinkle E
- Boerwinkle E
- Boerwinkle Eric
- Bolton Judith A Hoffman
- Bonnycastle Lori L.
- Borecki I
- Bornstein Stefan R.
- Bots Michiel L.
- Bragg-Gresham Jennifer L.
- Brand Eva
- Brand Stefan-Martin
- Brandstätter A
- Braund PS
- Braund Peter S.
- Brown MJ
- Brown Morris J.
- Bruse P
- Burnett MS
- Burton Paul R.
- Burtt N
- Böger CA
- Böhm BO
- Cambien F
- Campbell H
- Campbell S
- Campbell Harry
- Casas Juan P.
- Caulfield MJ
- Caulfield Mark J.
- Cavalieri M
- Chakravarti Aravinda
- Chambers JC
- Chambers John C.
- Chandak Giriraj R.
- Chang PP
- Chang Yen-Pei C.
- Charchar Fadi J.
- Charlotte Onland-Moret N.
- Chasman DI
- Chasman Daniel I.
- Chaturvedi Nish
- Chen IY
- Chen L
- Chen Ming-Huei
- Cho Yoon Shin
- Clarke Robert
- Collins Francis S.
- Connell JM
- Connell John M.
- Cook HT
- Cook HT
- Cooper Jackie A.
- Cooper Matthew N.
- Cooper Richard S.
- Coresh J
- Coresh Josef
- Cornelis MC
- Corsi Anna Maria
- Cotlarciuc I
- Cotlarciuc I
- Couper D
- Cupples LA
- Cupples LA
- Curhan GC
- Dahgam Santosh
- Dandona S
- Danesh John
- Davey Smith G
- Davey Smith G
- Day Ian N. M.
- de Andrade M
- de Boer J
- de Jong PE
- de Silva R
- de Silva R
- Deckers JW
- Dehghan A
- Dehghan A
- Dehghan A
- Dehghan A
- Dehghan Abbas
- Deloukas Panos
- Demirkan Ayse
- Demissie S
- Demissie-Banjaw S
- Deng G
- Deng G
- Denniff Matthew
- Devaney J
- Devuyst O
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- Dikkeschei LD
- Dikkeschei LD
- Dimkovic T
- Dobnig H
- Dockrell M
- Doering A
- Dominiczak A
- Dominiczak Anna F.
- Dong Yanbin
- Doumatey Ayo
- Dreisbach Albert W.
- Dörr M
- Dörr Marcus
- Ebrahim S
- Eggermann T
- Ehret Georg B.
- Eiriksdottir G
- Ellinghaus D
- Elliot P
- Elliott Paul
- Elosua R
- Elosua Roberto
- Emilsson Valur
- Endlich K
- Epstein S
- Erdmann J
- Erdmann J
- Erdmann Jeanette
- Eyheramendy Susana
- Farrall M
- Farrall Martin
- Fava Cristiano
- Feitosa M
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- Zhu Haidong
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- Zukowska-Szczechowska Ewa
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- Publication venue
- Nature
- Publication date
- 01/01/2011
- Field of study
Blood pressure is a heritable trait influenced by several biological pathways and responsive to environmental stimuli. Over one billion people worldwide have hypertension (≥140 mm Hg systolic blood pressure or ≥90 mm Hg diastolic blood pressure). Even small increments in blood pressure are associated with an increased risk of cardiovascular events. This genome-wide association study of systolic and diastolic blood pressure, which used a multi-stage design in 200,000 individuals of European descent, identified sixteen novel loci: six of these loci contain genes previously known or suspected to regulate blood pressure (GUCY1A3-GUCY1B3, NPR3-C5orf23, ADM, FURIN-FES, GOSR2, GNAS-EDN3); the other ten provide new clues to blood pressure physiology. A genetic risk score based on 29 genome-wide significant variants was associated with hypertension, left ventricular wall thickness, stroke and coronary artery disease, but not kidney disease or kidney function. We also observed associations with blood pressure in East Asian, South Asian and African ancestry individuals. Our findings provide new insights into the genetics and biology of blood pressure, and suggest potential novel therapeutic pathways for cardiovascular disease prevention
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
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- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Performance of missing transverse momentum reconstruction with the ATLAS detector using proton–proton collisions at √s = 13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying τ -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fb−1
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
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- Yildiz H Duran
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- Yusuff I
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- Zemaityte G
- Zeng JC
- Zeng Q
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- Zgubic M
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- Zhemchugov A
- Zhou B
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- Zhou M
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- Zhou N
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- Zhu CG
- Zhu H
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Alberich LC
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
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- Zhemchugov A
- Zheng Z
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- Zieminska D
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- Zimmermann S
- Zinonos Z
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
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- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
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- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
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