428 research outputs found
Measurement of the top quark mass using the matrix element technique in dilepton final states
- Author
- Abazov VM
- Abbott B
- Acharya BS
- Adams M
- Adams T
- Agnew JP
- Alexeev GD
- Alkhazov G
- Alton A
- Askew A
- Atkins S
- Augsten K
- Aushev V
- Aushev Y
- Avila C
- Badaud F
- Bagby L
- Baldin B
- Bandurin DV
- Banerjee S
- Barberis E
- Baringer P
- Bartlett JF
- Bassler U
- Bazterra V
- Bean A
- Begalli M
- Bellantoni L
- Beri SB
- Bernardi G
- Bernhard R
- Bertram I
- Besancon M
- Beuselinck R
- Bhat PC
- Bhatia S
- Bhatnagar V
- Blazey G
- Blessing S
- Bloom K
- Boehnlein A
- Boline D
- Boos EE
- Borissov G
- Borysova M
- Brandt A
- Brandt O
- Brochmann M
- Brock R
- Bross A
- Brown D
- Bu XB
- Buehler M
- Buescher V
- Bunichev V
- Burdin S
- Buszello CP
- Camacho-Perez E
- Casey BCK
- Castilla-Valdez H
- Caughron S
- Chakrabarti S
- Chan KM
- Chandra A
- Chapon E
- Chen G
- Cho SW
- Choi S
- Choudhary B
- Cihangir S
- Claes D
- Clutter J
- Collaboration D0
- Cooke M
- Cooper WE
- Corcoran M
- Couderc F
- Cousinou M-C
- Cuth J
- Cutts D
- Das A
- Davies G
- de Jong SJ
- De La Cruz-Burelo E
- de Sa R Lopes
- Deliot F
- Demina R
- Denisov D
- Denisov SP
- Desai S
- Deterre C
- DeVaughan K
- Diehl HT
- Diesburg M
- Ding PF
- Dominguez A
- Dubey A
- Dudko LV
- Duperrin A
- Dutt S
- Eads M
- Edmunds D
- Ellison J
- Elvira VD
- Enari Y
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- Evdokimov VN
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- Fiedler F
- Filthaut F
- Fisher W
- Fisk HE
- Fortner M
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- Franc J
- Fuess S
- Garbincius PH
- Garcia-Bellido A
- Garcia-Gonzalez JA
- Gavrilov V
- Geng W
- Gerber CE
- Gershtein Y
- Ginther G
- Gogota O
- Golovanov G
- Grannis PD
- Greder S
- Greenlee H
- Grenier G
- Gris Ph
- Grivaz J-F
- Grohsjean A
- Grunendahl S
- Grunewald MW
- Guillemin T
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- Gutierrez P
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- Illingworth R
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- Tokmenin VV
- Tsai Y-T
- Tsybychev D
- Tuchming B
- Tully C
- Uvarov L
- Uvarov S
- Uzunyan S
- Van Kooten R
- van Leeuwen WM
- Varelas N
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- Vertogradov LS
- Verzocchi M
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- Vilanova D
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- Wood DR
- Wyatt TR
- Xie Y
- Yamada R
- Yang S
- Yasuda T
- Yatsunenko YA
- Ye W
- Ye Z
- Yin H
- Yip K
- Youn SW
- Yu JM
- Zennamo J
- Zhao TG
- Zhou B
- Zhu J
- Zielinski M
- Zieminska D
- Zivkovic L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 10/06/2016
- Field of study
We present a measurement of the top quark mass in pp¯ collisions at a center-of-mass energy of 1.96 TeV at the Fermilab Tevatron collider. The data were collected by the D0 experiment corresponding to an integrated luminosity of 9.7 fb−1. The matrix element technique is applied to tt¯ events in the final state containing leptons (electrons or muons) with high transverse momenta and at least two jets. The calibration of the jet energy scale determined in the lepton+jets final state of tt¯ decays is applied to jet energies. This correction provides a substantial reduction in systematic uncertainties. We obtain a top quark mass of mt=173.93±1.84 GeV
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
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
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- Anh TV
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- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
- Feng H
- Fenyuk AB
- Fenyuk AB
- Fernando W
- Fernando W
- Ferrag S
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
- Ferrari P
- Ferrari R
- Ferrari R
- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
- Ferretti C
- Fiascaris M
- Fiascaris M
- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
- Finelli KD
- Fiolhais MCN
- Fiolhais MCN
- Fiorini L
- Fiorini L
- Firan A
- Firan A
- Fischer J
- Fischer J
- Fisher MJ
- Fisher MJ
- Fitzgerald EA
- Fitzgerald EA
- Flechl M
- Flechl M
- Fleck I
- Fleck I
- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
- Fletcher GT
- Flick T
- Flick T
- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
- Fox H
- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
- Franchino S
- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
- Friedrich F
- Froidevaux D
- Froidevaux D
- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
- Galster G
- Gan KK
- Gan KK
- Gandrajula RP
- Gandrajula RP
- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
- Gaur B
- Gauthier L
- Gauthier L
- Gauzzi P
- Gauzzi P
- Gavrilenko IL
- Gavrilenko IL
- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
- Gellerstedt K
- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
- Giagu S
- Giangiobbe V
- Giangiobbe V
- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
- Gibbard B
- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
- Gillam TPS
- Gillberg D
- Gillberg D
- Gillman AR
- Gillman AR
- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
- Giordano R
- Giorgi FM
- Giorgi FM
- Giraud PF
- Giraud PF
- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
- Gjelsten BK
- Gkialas I
- Gkialas I
- Gladilin LK
- Gladilin LK
- Glasman C
- Glasman C
- Glatzer J
- Glatzer J
- Glazov A
- Glazov A
- Glonti GL
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- Goblirsch-Kolb M
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- Goddard JR
- Godfrey J
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- Godlewski J
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- Goeringer C
- Goeringer C
- Goessling C
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- Goldfarb S
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- Golling T
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- Golubkov D
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- Gomes A
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- Gonalo R
- Goncalo R
- Gonella L
- Gonella L
- Gonzalez de la Hoz S
- Gonzalez de la Hoz S
- Gonzalez Parra G
- Gonzalez Parra G
- Gonzalez BA
- Gonzalez-Sevilla S
- Gonzalez-Sevilla S
- Goossens L
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- Gorbounov PA
- Gorbounov PA
- Gordon HA
- Gordon HA
- Gorelov I
- Gorelov I
- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
- Goshaw AT
- Gostkin MI
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- Gouighri M
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- Goujdami D
- Goujdami D
- Goulette MP
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- Goussiou AG
- Goussiou AG
- Goy C
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- Gozpinar S
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- Grabas HMX
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- Graber L
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- Grabowska-Bold I
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- Grafstroem P
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- Gramling J
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- Gramstad E
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- Grancagnolo F
- Grancagnolo S
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- Grancagnoloa F
- Grassi V
- Grassi V
- Gratchev V
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- Gray HM
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- Graziani E
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- Grebenyuk OG
- Grebenyuk OG
- Greenwood ZD
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- Gregersen K
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- Gregor IM
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- Grenier P
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- Griffiths J
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- Grillo AA
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- Grimm K
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- Grinstein S
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- Gris P
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- Grishkevich YV
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- Griso SP
- Grivaz J-F
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- Grohs JP
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- Grohsjean A
- Gross AGE
- Gross E
- Grosse-Knetter J
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- Grossi GC
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- Groth-Jensen J
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- Guan L
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- Guescini F
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- Guest D
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- Gueta O
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- Guicheney C
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- Guido E
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- Guindon S
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- Gul U
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- Guo J
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- Gutierrez P
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- Gutschow C
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- Guttman N
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- Guyot C
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- Haefner P
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- Hansen JD
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- Harenberg T
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- Hartjes F
- Harvey A
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- Hasegawa Y
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- Hawkings RJ
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- Hernandez Jimenez Y
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- Ideal E
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- Igonkina O
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- Zhemchugov A
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- Zibell A
- Zieminska D
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- Zimmermann C
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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 pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TP
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
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- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
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
- Author
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- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
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- Thong WM
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- Tibbetts MJ
- Tikhomirov VO
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- Tskhadadze EG
- Tsukerman II
- Tsulaia V
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- Tsybychev D
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- Tykhonov A
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- Valls Ferrer JA
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- van der Geer R
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- van der Ster D
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- van Huysduynen LH
- Van Nieuwkoop J
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- Whiteson D
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- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilkens HG
- Will JZ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson A
- 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
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- Wright M
- Wu M
- 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
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- 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
Quality of antimalarial drugs and antibiotics in Papua New Guinea: A survey of the health facility supply chain
- Author
- A Attaran
- A Nair
- AA Amin
- AC Kogawa
- AM Dondorp
- AP Cruz
- BR Moore
- CJ Chaccour
- CP Davy
- Evelyn K. Lavu
- FM Fernandez
- GM Nayyar
- GN Galappaththy
- H Kaur
- Inoni Betuela
- J Achan
- J Carmona-Fonseca
- J Pulford
- J Pulford
- Joshua Yukich
- Justin Pulford
- JW Kazura
- L Evans 3rd
- LO Gostin
- M Ahmed
- M Page-Sharp
- Madhu Page-Sharp
- Manuel W. Hetzel
- MC Gaudiano
- MS Arayne
- Nancy Bala
- NJ White
- NJ White
- NT Hehonah
- O Onwujekwe
- PM Graves
- PN Newton
- PN Newton
- PN Newton
- PN Newton
- PN Newton
- R Arun
- R Bate
- R Bate
- RE Howes
- S Phanouvong
- S Phanouvong
- S Salman
- S Shekalaghe
- SS Ranher
- T Almuzaini
- Timothy M. E. Davis
- V Pribluda
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2014
- Field of study
Background: Poor-quality life-saving medicines are a major public health threat, particularly in settings with a weak regulatory environment. Insufficient amounts of active pharmaceutical ingredients (API) endanger patient safety and may contribute to the development of drug resistance. In the case of malaria, concerns relate to implications for the efficacy of artemisinin-based combination therapies (ACT). In Papua New Guinea (PNG), Plasmodium falciparum and P. vivax are both endemic and health facilities are the main source of treatment. ACT has been introduced as first-line treatment but other drugs, such as primaquine for the treatment of P. vivax hypnozoites, are widely available. This study investigated the quality of antimalarial drugs and selected antibiotics at all levels of the health facility supply chain in PNG.Methods and Findings: Medicines were obtained from randomly sampled health facilities and selected warehouses and hospitals across PNG and analysed for API content using validated high performance liquid chromatography (HPLC). Of 360 tablet/capsule samples from 60 providers, 9.7% (95% CI 6.9, 13.3) contained less, and 0.6% more, API than pharmacopoeial reference ranges, including 29/37 (78.4%) primaquine, 3/70 (4.3%) amodiaquine, and one sample each of quinine, artemether, sulphadoxine-pyrimethamine and amoxicillin. According to the package label, 86.5% of poor-quality samples originated from India. Poor-quality medicines were found in 48.3% of providers at all levels of the supply chain. Drug quality was unrelated to storage conditions.Conclusions: This study documents the presence of poor-quality medicines, particularly primaquine, throughout PNG. Primaquine is the only available transmission-blocking antimalarial, likely to become important to prevent the spread of artemisinin-resistant P. falciparum and eliminating P. vivax hypnozoites. The availability of poor-quality medicines reflects the lack of adequate quality control and regulatory mechanisms. Measures to stop the availability of poor-quality medicines should include limiting procurement to WHO prequalified products and implementing routine quality testing
Deciphering Diseases and Biological Targets for Environmental Chemicals using Toxicogenomics Networks
- Author
- AF Heder
- Agnieszka Sierakowska Juncker
- AL Hopkins
- AP Davis
- BH Moon
- C Eil
- C von Mering
- CA Lipinski
- CE Bonferroni
- CF Kuper
- CR Williams-Devane
- CT Keith
- D Bauer
- DA Geier
- DC Volz
- DE Amacher
- DF Veber
- DH Phillips
- DR Boverhof
- DS Wishart
- E Birney
- F Salehi
- Francisco J. S. S. A. Roque
- G Block
- G Latini
- G Martinasso
- GA Westphal
- GD Bader
- GV Paolini
- HA Sani
- HS Kim
- J Lamb
- J Mestres
- J Vlasblom
- JF Rual
- K Lage
- Karine Audouze
- Konrad Krysiak-Baltyn
- L Yang
- LD Stein
- M Ashburner
- M Campillos
- M Kakeyama
- M Rebhan
- MA Yildirim
- ME Legare
- MJ Keiser
- MJ Keiser
- N Fletcher
- N Turan
- ND Lalwani
- NI Krinsky
- Nils Weinhold
- Olaf G. Wiest
- Olivier Taboureau
- P Toniolo
- R Morphy
- S Brohée
- S van Dongen
- SY Kim
- Søren Brunak
- T Nayyar
- T Suga
- Thomas Skøt Jensen
- TI Oprea
- TM Edwards
- U Peters
- Y Horiuchi
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Exposure to environmental chemicals and drugs may have a negative effect on human health. A better understanding of the molecular mechanism of such compounds is needed to determine the risk. We present a high confidence human protein-protein association network built upon the integration of chemical toxicology and systems biology. This computational systems chemical biology model reveals uncharacterized connections between compounds and diseases, thus predicting which compounds may be risk factors for human health. Additionally, the network can be used to identify unexpected potential associations between chemicals and proteins. Examples are shown for chemicals associated with breast cancer, lung cancer and necrosis, and potential protein targets for di-ethylhexyl-phthalate, 2,3,7,8-tetrachlorodibenzo-p-dioxin, pirinixic acid and permethrine. The chemical-protein associations are supported through recent published studies, which illustrate the power of our approach that integrates toxicogenomics data with other data types
Inclusive Production of the X(4140) State in pp¯ Collisions at D0
- Author
- Abazov VM
- Abbott B
- Acharya BS
- Adams M
- Adams T
- Agnew JP
- Alexeev GD
- Alkhazov G
- Alton A
- Askew A
- Atkins S
- Augsten K
- Avila C
- Badaud F
- Bagby L
- Baldin B
- Bandurin DV
- Banerjee S
- Barberis E
- Baringer P
- Bartlett JF
- Bassler U
- Bazterra V
- Bean A
- Begalli M
- Bellantoni L
- Beri SB
- Bernardi G
- Bernhard R
- Bertram I
- Besancon M
- Beuselinck R
- Bhat PC
- Bhatia S
- Bhatnagar V
- Blazey G
- Blessing S
- Bloom K
- Boehnlein A
- Boline D
- Boos EE
- Borissov G
- Borysova M
- Brandt A
- Brandt O
- Brock R
- Bross A
- Brown D
- Bu XB
- Buehler M
- Buescher V
- Bunichev V
- Burdin S
- Buszello CP
- Camacho-Perez E
- Casey BCK
- Castilla-Valdez H
- Caughron S
- Chakrabarti S
- Chan KM
- Chandra A
- Chapon E
- Chen G
- Cho SW
- Choi S
- Choudhary B
- Cihangir S
- Claes D
- Clutter J
- Cooke M
- Cooper WE
- Corcoran M
- Couderc F
- Cousinou M-C
- Cuth J
- Cutts D
- Das A
- Davies G
- De Jong SJ
- De La Cruz-Burelo E
- De Sa RL
- Deliot F
- Demina R
- Denisov D
- Denisov SP
- Desai S
- Deterre C
- DeVaughan K
- Diehl HT
- Diesburg M
- Ding PF
- Dominguez A
- Dubey A
- Dudko LV
- Duperrin A
- Dutt S
- Eads M
- Edmunds D
- Ellison J
- Elvira VD
- Enari Y
- Evans H
- Evdokimov A
- Evdokimov VN
- Faure A
- Feng L
- Ferbel T
- Fiedler F
- Filthaut F
- Fisher W
- Fisk HE
- Fortner M
- Fox H
- Fuess S
- Garbincius PH
- Garcia-Bellido A
- Garcia-Gonzalez JA
- Gavrilov V
- Geng W
- Gerber CE
- Gershtein Y
- Ginther G
- Gogota O
- Golovanov G
- Grannis PD
- Greder S
- Greenlee H
- Grenier G
- Gris P
- Grivaz J-F
- Grohsjean A
- Gruenendahl S
- Gruenewald MW
- Guillemin T
- Gutierrez G
- Gutierrez P
- Haley J
- Han L
- Harder K
- Harel A
- Hauptman JM
- Hays J
- Head T
- Hebbeker T
- Hedin D
- Hegab H
- Heinson AP
- Heintz U
- Hensel C
- Heredia-De La Cruz I
- Herner K
- Hesketh G
- Hildreth MD
- Hirosky R
- Hoang T
- Hobbs JD
- Hoeneisen B
- Hogan J
- Hohlfeld M
- Holzbauer JL
- Howley I
- Hubacek Z
- Hynek V
- Iashvili I
- Ilchenko Y
- Illingworth R
- Ito AS
- Jabeen S
- Jaffre M
- Jayasinghe A
- Jeong MS
- Jesik R
- Jiang P
- Johns K
- Johnson E
- Johnson M
- Jonckheere A
- Jonsson P
- Joshi J
- Jung AW
- Juste A
- Kajfasz E
- Karmanov D
- Katsanos I
- Kaur M
- Kehoe R
- Kermiche S
- Khalatyan N
- Khanov A
- Kharchilava A
- Kharzheev YN
- Kiselevich I
- Kohli JM
- Kozelov AV
- Kraus J
- Kumar A
- Kupco A
- Kurca T
- Kuzmin VA
- Lammers S
- Lebrun P
- Lee HS
- Lee SW
- Lee WM
- Lei X
- Lellouch J
- Li D
- Li H
- Li L
- Li QZ
- Lim JK
- Lincoln D
- Linnemann J
- Lipaev VV
- Lipton R
- Liu H
- Liu Y
- Lobodenko A
- Lokajicek M
- Luna-Garcia R
- Lyon AL
- Maciel AKA
- Madar R
- Magana-Villalba R
- Malik S
- Malyshev VL
- Mansour J
- Martinez-Ortega J
- McCarthy R
- McGivern CL
- Meijer MM
- Melnitchouk A
- Menezes D
- Mercadante PG
- Merkin M
- Meyer A
- Meyer J
- Miconi F
- Mondal NK
- Mulhearn M
- Nagy E
- Narain M
- Nayyar R
- Neal HA
- Negret JP
- Neustroev P
- Nguyen HT
- Nunnemann T
- Orduna J
- Osman N
- Osta J
- Pal A
- Parashar N
- Parihar V
- Park SK
- Partridge R
- Parua N
- Patwa A
- Penning B
- Perfilov M
- Peters Y
- Petridis K
- Petrillo G
- Petroff P
- Pleier M-A
- Podstavkov VM
- Popov AV
- Prewitt M
- Price D
- Prokopenko N
- Qian J
- Quadt A
- Quinn B
- Ratoff PN
- Razumov I
- Ripp-Baudot I
- Rizatdinova F
- Rominsky M
- Ross A
- Royon C
- Rubinov P
- Ruchti R
- Sajot G
- Sanchez-Hernandez A
- Sanders MP
- Santos AS
- Savage G
- Savitskyi M
- Sawyer L
- Scanlon T
- Schamberger RD
- Scheglov Y
- Schellman H
- Schott M
- Schwanenberger C
- Schwienhorst R
- Sekaric J
- Severini H
- Shabalina E
- Shary V
- Shaw S
- Shchukin AA
- Simak V
- Skubic P
- Slattery P
- Smirnov D
- Snow GR
- Snow J
- Snyder S
- Soeldner-Rembold S
- Sonnenschein L
- Soustruznik K
- Stark J
- Stoyanova DA
- Strauss M
- Suter L
- Svoisky P
- Titov M
- Tokmenin VV
- Tsai Y-T
- Tsybychev D
- Tuchming B
- Tully C
- Uvarov L
- Uvarov S
- Uzunyan S
- Van Kooten R
- Van Leeuwen WM
- Varelas N
- Varnes EW
- Vasilyev IA
- Verkheev AY
- Vertogradov LS
- Verzocchi M
- Vesterinen M
- Vilanova D
- Vokac P
- Wahl HD
- Wang MHLS
- Warchol J
- Watts G
- Wayne M
- Weichert J
- Welty-Rieger L
- Williams MRJ
- Wilson GW
- Wobisch M
- Wood DR
- Wyatt TR
- Xie Y
- Yamada R
- Yang S
- Yasuda T
- Yatsunenko YA
- Ye W
- Ye Z
- Yin H
- Yip K
- Youn SW
- Yu JM
- Zennamo J
- Zhao TG
- Zhou B
- Zhu J
- Zielinski M
- Zieminska D
- Zivkovic L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 02/12/2015
- Field of study
Studies of X(3872) and ψ(2S) production in p\bar{p}over-bar collisions at 1.96 TeV
- Author
- Abazov VM
- Abbott B
- Acharya BS
- Adams M
- Adams T
- Agnew JP
- Alexeev GD
- Alkhazov G
- Alton A
- Askew A
- Atkins S
- Augsten K
- Aushev V
- Aushev Y
- Avila C
- Badaud F
- Bagby L
- Baldin B
- Bandurin D
- Banerjee S
- Barberis E
- Baringer P
- Bartlett JF
- Bassler U
- Bazterra V
- Bean A
- Begalli M
- Bellantoni L
- Beri SB
- Bernardi G
- Bernhard R
- Bertram I
- Besancon M
- Beuselinck R
- Bhat PC
- Bhatia S
- Bhatnagar V
- Blazey G
- Blessing S
- Bloom K
- Boehnlein A
- Boline D
- Boos EE
- Borissov G
- Borysova M
- Brandt A
- Brandt O
- Brochmann M
- Brock R
- Bross A
- Brown D
- Bu XB
- Buehler M
- Buescher V
- Bunichev V
- Burdin S
- Buszello CP
- Camacho-Perez E
- Casey BCK
- Castilla-Valdez H
- Caughron S
- Chakrabarti S
- Chan KM
- Chandra A
- Chapon E
- Chen G
- Cho SW
- Choi S
- Choudhary B
- Cihangir S
- Claes D
- Clutter J
- Cooke M
- Cooper WE
- Corcoran M
- Couderc F
- Cousinou M-C
- Cuth J
- Cutts D
- Das A
- Davies G
- de Jong SJ
- De La Cruz-Burelo E
- de Sa RL
- Deliot F
- Demina R
- Denisov D
- Denisov SP
- Desai S
- Deterre C
- DeVaughan K
- Diehl HT
- Diesburg M
- Ding PF
- Dominguez A
- Drutskoy A
- Dubey A
- Dudko L
- Duperrin A
- Dutt S
- Eads M
- Edmunds D
- Ellison J
- Elvira VD
- Enari Y
- Evans H
- Evdokimov A
- Evdokimov VN
- Faure A
- Feng L
- Ferbel T
- Fiedler F
- Filthaut F
- Fisher W
- Fisk HE
- Fortner M
- Fox H
- Franc J
- Fuess S
- Garbincius PH
- Garcia-Bellido A
- Garcia-Gonzalez JA
- Gavrilov V
- Geng W
- Gerber CE
- Gershtein Y
- Ginther G
- Gogota O
- Golovanov G
- Grannis PD
- Greder S
- Greenlee H
- Grenier G
- Gris P
- Grivaz J-F
- Grohsjean A
- Grunendahl S
- Grunewald MW
- Guillemin T
- Gutierrez G
- Gutierrez P
- Haley J
- Han L
- Harder K
- Harel A
- Hauptman JM
- Hays J
- Head T
- Hebbeker T
- Hedin D
- Hegab H
- Heinson AP
- Heintz U
- Hensel C
- Heredia-De La Cruz I
- Herner K
- Hesketh G
- Hildreth MD
- Hirosky R
- Hoang T
- Hobbs JD
- Hoeneisen B
- Hogan J
- Hohlfeld M
- Holzbauer JL
- Howley I
- Hubacek Z
- Hynek V
- Iashvili I
- Ilchenko Y
- Illingworth R
- Ito AS
- Jabeen S
- Jaffre M
- Jayasinghe A
- Jeong MS
- Jesik R
- Jiang P
- Johns K
- Johnson E
- Johnson M
- Jonckheere A
- Jonsson P
- Joshi J
- Jung AW
- Juste A
- Kajfasz E
- Karmanov D
- Katsanos I
- Kaur M
- Kehoe R
- Kermiche S
- Khalatyan N
- Khanov A
- Kharchilava A
- Kharzheev YN
- Kiselevich I
- Kohli JM
- Kozelov A
- Kraus J
- Kumar A
- Kupco A
- Kuzmin VA
- Lammers S
- Lebrun P
- Lee HS
- Lee SW
- Lee WM
- Lei X
- Lellouch J
- Li D
- Li H
- Li L
- Li QZ
- Lim JK
- Lincoln D
- Linnemann J
- Lipaev VV
- Lipton R
- Liu H
- Liu Y
- Lobodenko A
- Lokajicek M
- Luna-Garcia R
- Lyon AL
- Maciel AKA
- Madar R
- Magana-Villalba R
- Malik S
- Malyshev VL
- Mansour J
- Martinez-Ortega J
- McCarthy R
- McGivern CL
- Meijer MM
- Melnitchouk A
- Menezes D
- Mercadante PG
- Merkin M
- Meyer A
- Meyer J
- Miconi F
- Mondal NK
- Mulhearn M
- Nagy E
- Narain M
- Nayyar R
- Neal HA
- Negret JP
- Neustroev P
- Nguyen HT
- Nunnemann T
- Orduna J
- Osman N
- Pal A
- Parashar N
- Parihar V
- Park SK
- Partridge R
- Parua N
- Patwa A
- Penning B
- Perfilov M
- Peters Y
- Petridis K
- Petrillo G
- Petroff P
- Pleier M-A
- Podstavkov VM
- Popov A
- Prewitt M
- Price D
- Prokopenko N
- Qian J
- Quadt A
- Quinn B
- Ratoff PN
- Razumov I
- Ripp-Baudot I
- Rizatdinova F
- Rominsky M
- Ross A
- Royon C
- Rubinov P
- Ruchti R
- Sajot G
- Sanchez-Hernandez A
- Sanders MP
- Santos AS
- Savage G
- Savitskyi M
- Sawyer L
- Scanlon T
- Schamberger RD
- Scheglov Y
- Schellman H
- Schott M
- Schwanenberger C
- Schwienhorst R
- Sekaric J
- Severini H
- Shabalina E
- Shary V
- Shaw S
- Shchukin AA
- Shkola O
- Simak V
- Skubic P
- Slattery P
- Snow GR
- Snow J
- Snyder S
- Soldner-Rembold S
- Sonnenschein L
- Soustruznik K
- Stark J
- Stefaniuk N
- Stoyanova DA
- Strauss M
- Suter L
- Svoisky P
- Titov M
- Tokmenin VV
- Tsai Y-T
- Tsybychev D
- Tuchming B
- Tully C
- Uvarov L
- Uvarov S
- Uzunyan S
- Van Kooten R
- van Leeuwen WM
- Varelas N
- Varnes EW
- Vasilyev IA
- Verkheev AY
- Vertogradov LS
- Verzocchi M
- Vesterinen M
- Vilanova D
- Vokac P
- Wahl HD
- Wang C
- Wang MHLS
- Warchol J
- Watts G
- Wayne M
- Weichert J
- Welty-Rieger L
- Williams MRJ
- Wilson GW
- Wobisch M
- Wood DR
- Wyatt TR
- Xie Y
- Yamada R
- Yang S
- Yasuda T
- Yatsunenko YA
- Ye W
- Ye Z
- Yin H
- Yip K
- Youn SW
- Yu JM
- Zennamo J
- Zhao TG
- Zhou B
- Zhu J
- Zielinski M
- Zieminska D
- Zivkovic L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/10/2020
- Field of study
We present various properties of the production of the X (3872) and ψ(2S) states based on 10.4fb‾¹ collected by the D0 experiment in Tevatron p\bar{p} collisions at \sqrt{s} = 1.96 TeV. For both states, we measure the nonprompt fraction fNP of the inclusive production rate due to decays of b-flavored hadrons. We find the fNP values systematically below those obtained at the LHC. The fNP fraction for ψ(2S) increases with transverse momentum, whereas for the X(3872) it is constant within large uncertainties, in agreement with the LHC results. The ratio of prompt to nonprompt ψ(2S) production, (1 - fNP)/fNP, decreases only slightly going from the Tevatron to the LHC, but for the X(3872), this ratio decreases by a factor of about 3. We test the soft-pion signature of the X(3872) modeled as a weakly bound charm-meson pair by studying the production of the X(3872) as a function of the kinetic energy of the X(3872) and the pion in the X(3872) π center-of-mass frame. For a subsample consistent with prompt production, the results are incompatible with a strong enhancement in the production of the X(3872) at the small kinetic energy of the X(3872) and the π in the X(3872)π center-of-mass frame expected for the X + soft-pion production mechanism. For events consistent with being due to decays of hadrons, there is no significant evidence for the soft-pion effect, but its presence at the level expected for the binding energy of 0.17 MeV and the momentum scale Λ = M(π) is not ruled out
Properties of Z±c(3900) produced in pp¯ collisions
- Author
- Abazov VM
- Abbott B
- Acharya BS
- Adams M
- Adams T
- Agnew JP
- Alexeev GD
- Alkhazov G
- Alton A
- Askew A
- Atkins S
- Augsten K
- Aushev V
- Aushev Y
- Avila C
- Badaud F
- Bagby L
- Baldin B
- Bandurin DV
- Banerjee S
- Barberis E
- Baringer P
- Bartlett JF
- Bassler U
- Bazterra V
- Bean A
- Begalli M
- Bellantoni L
- Beri SB
- Bernardi G
- Bernhard R
- Bertram I
- Besancon M
- Beuselinck R
- Bhat PC
- Bhatia S
- Bhatnagar V
- Blazey G
- Blessing S
- Bloom K
- Boehnlein A
- Boline D
- Boos EE
- Borissov G
- Borysova M
- Brandt A
- Brandt O
- Brochmann M
- Brock R
- Bross A
- Brown D
- Bu XB
- Buehler M
- Buescher V
- Bunichev V
- Burdin S
- Buszello CP
- Camacho-Perez E
- Casey BCK
- Castilla-Valdez H
- Caughron S
- Chakrabarti S
- Chan KM
- Chandra A
- Chapon E
- Chen G
- Cho SW
- Choi S
- Choudhary B
- Cihangir S
- Claes D
- Clutter J
- Cooke M
- Cooper WE
- Corcoran M
- Couderc F
- Cousinou M-C
- Cuth J
- Cutts D
- Das A
- Davies G
- de Jong SJ
- De La Cruz-Burelo E
- de Sa RL
- Deliot F
- Demina R
- Denisov D
- Denisov SP
- Desai S
- Deterre C
- DeVaughan K
- Diehl HT
- Diesburg M
- Ding PF
- Dominguez A
- Drutskoy A
- Dubey A
- Dudko LV
- Duperrin A
- Dutt S
- Eads M
- Edmunds D
- Ellison J
- Elvira VD
- Enari Y
- Evans H
- Evdokimov A
- Evdokimov VN
- Faure A
- Feng L
- Ferbel T
- Fiedler F
- Filthaut F
- Fisher W
- Fisk HE
- Fortner M
- Fox H
- Franc J
- Fuess S
- Garbincius PH
- Garcia-Bellido A
- Garcia-Gonzalez JA
- Gavrilov V
- Geng W
- Gerber CE
- Gershtein Y
- Ginther G
- Gogota O
- Golovanov G
- Grannis PD
- Greder S
- Greenlee H
- Grenier G
- Gris P
- Grivaz J-F
- Grohsjean A
- Grunendahl S
- Grunewald MW
- Guillemin T
- Gutierrez G
- Gutierrez P
- Haley J
- Han L
- Harder K
- Harel A
- Hauptman JM
- Hays J
- Head T
- Hebbeker T
- Hedin D
- Hegab H
- Heinson AP
- Heintz U
- Hensel C
- Heredia-De La Cruz I
- Herner K
- Hesketh G
- Hildreth MD
- Hirosky R
- Hoang T
- Hobbs JD
- Hoeneisen B
- Hogan J
- Hohlfeld M
- Holzbauer JL
- Howley I
- Hubacek Z
- Hynek V
- Iashvili I
- Ilchenko Y
- Illingworth R
- Ito AS
- Jabeen S
- Jaffre M
- Jayasinghe A
- Jeong MS
- Jesik R
- Jiang P
- Johns K
- Johnson E
- Johnson M
- Jonckheere A
- Jonsson P
- Joshi J
- Jung AW
- Juste A
- Kajfasz E
- Karmanov D
- Katsanos I
- Kaur M
- Kehoe R
- Kermiche S
- Khalatyan N
- Khanov A
- Kharchilava A
- Kharzheev YN
- Kiselevich I
- Kohli JM
- Kozelov AV
- Kraus J
- Kumar A
- Kupco A
- Kurca T
- Kuzmin VA
- Lammers S
- Lebrun P
- Lee HS
- Lee SW
- Lee WM
- Lei X
- Lellouch J
- Li D
- Li H
- Li L
- Li QZ
- Lim JK
- Lincoln D
- Linnemann J
- Lipaev VV
- Lipton R
- Liu H
- Liu Y
- Lobodenko A
- Lokajicek M
- Luna-Garcia R
- Lyon AL
- Maciel AKA
- Madar R
- Magana-Villalba R
- Malik S
- Malyshev VL
- Mansour J
- Martinez-Ortega J
- McCarthy R
- McGivern CL
- Meijer MM
- Melnitchouk A
- Menezes D
- Mercadante PG
- Merkin M
- Meyer A
- Meyer J
- Miconi F
- Mondal NK
- Mulhearn M
- Nagy E
- Narain M
- Nayyar R
- Neal HA
- Negret JP
- Neustroev P
- Nguyen HT
- Nunnemann T
- Orduna J
- Osman N
- Pal A
- Parashar N
- Parihar V
- Park SK
- Partridge R
- Parua N
- Patwa A
- Penning B
- Perfilov M
- Peters Y
- Petridis K
- Petrillo G
- Petroff PP
- Pleier M-A
- Podstavkov VM
- Popov AV
- Prewitt M
- Price D
- Prokopenko N
- Qian J
- Quadt A
- Quinn B
- Ratoff PN
- Razumov I
- Ripp-Baudot I
- Rizatdinova F
- Rominsky M
- Ross A
- Royon C
- Rubinov P
- Ruchti R
- Sajot G
- Sanchez-Hernandez A
- Sanders MP
- Santos AS
- Savage G
- Savitskyi M
- Sawyer L
- Scanlon T
- Schamberger RD
- Scheglov Y
- Schellman H
- Schott M
- Schwanenberger C
- Schwienhorst R
- Sekaric J
- Severini H
- Shabalina E
- Shary V
- Shaw S
- Shchukin AA
- Shkola O
- Simak V
- Skubic P
- Slattery P
- Snow GR
- Snow J
- Snyder S
- Soldner-Rembold S
- Sonnenschein L
- Soustruznik K
- Stark J
- Stefaniuk N
- Stoyanova DA
- Strauss M
- Suter L
- Svoisky P
- Titov M
- Tokmenin VV
- Tsai Y-T
- Tsybychev D
- Tuchming B
- Tully C
- Uvarov L
- Uvarov S
- Uzunyan S
- Van Kooten R
- van Leeuwen WM
- Varelas N
- Varnes EW
- Vasilyev IA
- Verkheev AY
- Vertogradov LS
- Verzocchi M
- Vesterinen M
- Vilanova D
- Vokac P
- Wahl HD
- Wang MHLS
- Warchol J
- Watts G
- Wayne M
- Weichert J
- Welty-Rieger L
- Williams MRJ
- Wilson GW
- Wobisch M
- Wood DR
- Wyatt TR
- Xie Y
- Yamada R
- Yang S
- Yasuda T
- Yatsunenko YA
- Ye W
- Ye Z
- Yin H
- Yip K
- Youn SW
- Yu JM
- Zennamo J
- Zhao TG
- Zhou B
- Zhu J
- Zielinski M
- Zieminska D
- Zivkovic L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2019
- Field of study
We study the production of the exotic charged charmoniumlike state
Z
±
c
(
3900
)
in
p
¯
p
collisions through the sequential process
ψ
(
4260
)
→
Z
±
c
(
3900
)
π
∓
,
Z
±
c
(
3900
)
→
J
/
ψ
π
±
. Using the subsample of candidates originating from semi-inclusive weak decays of
b
-flavored hadrons, we measure the invariant mass and natural width to be
M
=
3902.6
+
5.2
−
5.0
(
stat
)
+
3.3
−
1.4
(
syst
)
MeV
and
Γ
=
3
2
+
28
−
21
(
stat
)
+
26
−
7
(
syst
)
MeV
, respectively. We search for prompt production of the
Z
±
c
(
3900
)
through the same sequential process. No significant signal is observed, and we set an upper limit of 0.70 at the 95% credibility level on the ratio of prompt production to the production via
b
-hadron decays. The study is based on
10.4
f
b
−
1
of
p
¯
p
collision data collected by the D0 experiment at the Fermilab Tevatron collider
Combined Tevatron upper limit on gg->H->W+W- and constraints on the Higgs boson mass in fourth-generation fermion models
- Author
- Aaltonen T
- Abazov VM
- Abbott B
- Abolins M
- Acharya BS
- Adams M
- Adams T
- Adelman J
- Aguilo E
- Alexeev GD
- Alkhazov G
- Almenar CC
- Alton A
- Alverson G
- Alves GA
- Amerio S
- Amidei D
- Anastassov A
- Ancu LS
- Annovi A
- Antos J
- Aoki M
- Apollinari G
- Appel J
- Apresyan A
- Arisawa T
- Arnoud Y
- Arov M
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Asman B
- Atramentov O
- Attal A
- Aurisano A
- Avila C
- Azfar F
- BackusMayes J
- Badaud F
- Badgett W
- Bagby L
- Baldin B
- Bandurin DV
- Banerjee S
- Barbaro Galtieri A
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- Zucchelli SSevior M. E.
- Publication venue
- Publication date
- 01/01/2010
- Field of study
Report number: FERMILAB-PUB-10-125-EWe combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg->H->W+W- in p=pbar collisions at the Fermilab Tevatron Collider at sqrt{s}=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% Confidence Level upper limit on \sigma(gg->H) x B(H->W+W-) is 1.75 pb at m_H=120 GeV, 0.38 pb at m_H=165 GeV, and 0.83 pb at m_H=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% Confidence Level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.We combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg→H→W+W- in pp̅ collisions at the Fermilab Tevatron Collider at √s=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% confidence level upper limit on σ(gg→H)×B(H→W+W-) is 1.75 pb at mH=120 GeV, 0.38 pb at mH=165 GeV, and 0.83 pb at mH=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% confidence level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.Peer reviewe
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