68 research outputs found
Inclusive V0 Production Cross Sections from 920 GeV Fixed Target Proton-Nucleus Collisions
- Author
- Abt I
- Abyzov A
- Adams M
- Albrecht H
- Amaral V
- Amorim A
- Aplin SJ
- Arefiev A
- Arino I
- Atiya M
- Aushev V
- Bagaturia Y
- Baghshetsyan R
- Balagura V
- Bargiotti M
- Barsuk S
- Barsukova O
- Bassetti V
- Bastos J
- Bauer C
- Bauer TS
- Beck M
- Belkov A
- Belkov A
- Belotelov I
- Belyaev I
- Berkhan K
- Bertin A
- Bobchenko B
- Bocker M
- Bogatyrev A
- Bohm G
- Borgmeier C
- Brauer M
- Broemmelsiek D
- Brunisma M
- Bruschi M
- Buchholz P
- Buchler M
- Buran T
- Capeans M
- Capponi M
- Carvalho J
- Chamanina J
- Chen BX
- Chistov R
- Chmeissani M
- Christensen A
- Conde P
- Cruse C
- Dam M
- Danielsen KM
- Danilov M
- De Castro S
- de Vera MTNP
- Deckers H
- Dehmelt K
- Deppe H
- Dolgoshein B
- Dong X
- Dreis HB
- Dressel M
- Dujmic D
- Eckmann R
- Egorytchev V
- Ehret K
- Eiges V
- Eisele F
- Emeliyanov D
- Erhan S
- Essenov S
- Fabbri L
- Faccioli P
- Fallot-Burghardt W
- Feuerstack-Raible M
- Flammer J
- Fleckenstein H
- Fominykh B
- Fourletov S
- Fuljahn T
- Funcke M
- Galli D
- Garcia A
- Garrido L
- Gascon D
- Gellrich A
- Gerndt KEK
- Giacobbe B
- Glass J
- Glebe T
- Goloubkov D
- Golutvin A
- Golutvin I
- Gorbounov I
- Gorisek A
- Gouchtchine O
- Goulart DC
- Gradl S
- Gradl W
- Guilitsky Y
- Hamacher T
- Hansen JD
- Harr R
- Hast C
- Hausmann S
- Hernandez JM
- Hildebrandt M
- Hofmann W
- Hohlmann M
- Holscher A
- Hopfner K
- Hott T
- Hulsbergen W
- Husemann U
- Igonkina O
- Ispiryan M
- Issever S
- Itterbeck H
- Ivarsson Jenny
- Jagla T
- Jia Y
- Jiang C
- Kaoukher A
- Kapitza H
- Karabekyan S
- Karchin P
- Karpenko N
- Ke Z
- Keller S
- Khasanov F
- Kim H
- Kiryushin Y
- Kisel I
- Klefenz F
- Knopfle KT
- Kochetkov V
- Kolanoski H
- Korpar S
- Krauss C
- Kreuzer P
- Krizan P
- Krucker D
- Kvaratskheliia T
- Lange A
- Lanyov A
- Lau K
- Leffers G
- Legrand I
- Lewendel B
- Liu YQ
- Lohse T
- Loke R
- Lomonosov B
- Ludemann J
- Mankel R
- Manner R
- Marconi U
- Masciocchi S
- Massa I
- Matchikhilian I
- Medin G
- Medinnis M
- Mevius M
- Michetti A
- Mikhailov Y
- Miquel R
- Mizuk R
- Mohapatra A
- Moshkin A
- Moshous B
- Muresan R
- Nam S
- Negodaev M
- Negri I
- Norenberg M
- Nowak S
- Oest T
- Oliveira A
- Ouchrif M
- Ould-Saada F
- Padilla C
- Pakhlov P
- Pavlenko Y
- Peralta D
- Pernack R
- Perschke T
- Pestotnik R
- Petersen BAA
- Piccinini M
- Pleier MA
- Poli M
- Popov V
- Pose A
- Pose D
- Potashnikova I
- Pugatch V
- Pylypchenko Y
- Pyrlik J
- Ramachandran S
- Ratnikov F
- Reeves K
- Ressing D
- Riechmann K
- Rieling J
- Rietz M
- Riu I
- Robmann P
- Rosen J
- Rothe C
- Ruckstuhl W
- Rusinov V
- Rybnikov V
- Ryzhikov D
- Saadi-Ludemann F
- Samtleben D
- Sanchez F
- Sang M
- Saveliev V
- Sbrizzi A
- Schaller S
- Schlein P
- Schmelling M
- Schmidt B
- Schmidt S
- Schmidt-Parzefall W
- Schreiner A
- Schroder H
- Schultz HD
- Schwanke U
- Schwartz AJ
- Schwarz AS
- Schwenninger B
- Schwingenheuer B
- Schwitters R
- Sciacca F
- Semenov S
- Semprini-Cesari N
- Sexauer E
- Seybold L
- Shiu J
- Shuvalov S
- Siccama I
- Skrk D
- Soldatov A
- Solunin S
- Somov A
- Somov S
- Souvorov V
- Sozuer L
- Spahn M
- Spengler J
- Spighi R
- Spiridonov A
- Spratte S
- Stanovnik A
- Staric M
- Stdenis R
- Stegmann C
- Steinbeck S
- Steinkamp O
- Stieler D
- Straumann U
- Sun F
- Sun H
- Symalla M
- Takach S
- Tesch N
- Thurn H
- Tikhomirov I
- Titov M
- Trunk U
- Truol P
- Tsakov I
- Uwer U
- Vagnoni V
- van Eldik C
- van Staa R
- Vassiliev Y
- Villa M
- Vitale A
- Vukotic I
- Wagner G
- Wagner W
- Wahlberg H
- Walenta AH
- Walter M
- Walter T
- Wang JJ
- Wang YM
- Wanke R
- Wegener D
- Werthenbach U
- Weyers PJ
- Wolters H
- Wurth R
- Wurz A
- Xella-Hansen S
- Yang J
- Zaitsev Y
- Zavertyaev M
- Zech G
- Zeuner T
- Zhelezov A
- Zheng Z
- Zhu Z
- Zimmermann R
- Zivko T
- Zoccoli A
- Zweizig J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/12/2002
- Field of study
Inclusive differential cross sections dÏpAâ/dxFâ and
dÏpAâ/dpt2â for the production of \kzeros, \lambdazero, and
\antilambda particles are measured at HERA in proton-induced reactions on C,
Al, Ti, and W targets. The incident beam energy is 920 GeV, corresponding to
sâ=41.6 GeV in the proton-nucleon system. The ratios of differential
cross sections \rklpa and \rllpa are measured to be 6.2±0.5 and 0.66±0.07, respectively, for \xf ââ0.06. No significant dependence upon the
target material is observed. Within errors, the slopes of the transverse
momentum distributions dÏpAâ/dpt2â also show no significant
dependence upon the target material. The dependence of the extrapolated total
cross sections ÏpAâ on the atomic mass A of the target material is
discussed, and the deduced cross sections per nucleon ÏpNâ are
compared with results obtained at other energies.Comment: 17 pages, 7 figures, 5 table
In Vivo Human Apolipoprotein E Isoform Fractional Turnover Rates in the CNS
- Author
- Alison Goate
- AM Fagan
- AS Khachaturian
- Bruce W. Patterson
- C Talbot
- Chengjie Xiong
- David M. Holtzman
- DL Elbert
- DM Hatters
- DM Holtzman
- DM Holtzman
- DR Riddell
- E Fabbrini
- EH Corder
- EH Corder
- ES Krul
- G Ramaswamy
- H Fukumoto
- H Fukumoto
- Hong Jiang
- Hyejin Yoon
- J Kim
- Jacob M. Basak
- JD Fryer
- Jennifer X. Wang
- JM Castellano
- JS Millar
- Jungsu Kim
- K Ikewaki
- K Yamauchi
- KE Yarasheski
- Kevin E. Yarasheski
- KH Weisgraber
- KM Korwek
- KR Bales
- KR Wildsmith
- Kristin R. Wildsmith
- Kwasi G. Mawuenyega
- LA Farrer
- LM Bekris
- M Morikawa
- M Smit
- Maia Parsadanian
- MF Linton
- N Elias
- P Bertrand
- PM Sullivan
- PM Sullivan
- PT Xu
- R Ramakrishnan
- RA Fishman
- Randall J. Bateman
- RE Dinkel
- RE Gregg
- RE Gregg
- RE Gregg
- RJ Bateman
- RJ Bateman
- RR Wolfe
- RW Mahley
- SD Harr
- SE Wahrle
- SE Wahrle
- SJ Wood
- SM Greenberg
- SP Mooijaart
- Steven Estus
- T Lehtimaki
- TD Burt
- Tom Kasten
- U Beffert
- W Zhou
- Wendy C. Sigurdson
- Yuriy Pyatkivskyy
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
Apolipoprotein E (ApoE) is the strongest genetic risk factor for Alzheimerâs disease and has been implicated in the risk for other neurological disorders. The three common ApoE isoforms (ApoE2, E3, and E4) each differ by a single amino acid, with ApoE4 increasing and ApoE2 decreasing the risk of Alzheimerâs disease (AD). Both the isoform and amount of ApoE in the brain modulate AD pathology by altering the extent of amyloid beta (AÎČ) peptide deposition. Therefore, quantifying ApoE isoform production and clearance rates may advance our understanding of the role of ApoE in health and disease. To measure the kinetics of ApoE in the central nervous system (CNS), we applied in vivo stable isotope labeling to quantify the fractional turnover rates of ApoE isoforms in 18 cognitively-normal adults and in ApoE3 and ApoE4 targeted-replacement mice. No isoform-specific differences in CNS ApoE3 and ApoE4 turnover rates were observed when measured in human CSF or mouse brain. However, CNS and peripheral ApoE isoform turnover rates differed substantially, which is consistent with previous reports and suggests that the pathways responsible for ApoE metabolism are different in the CNS and the periphery. We also demonstrate a slower turnover rate for CSF ApoE than that for amyloid beta, another molecule critically important in AD pathogenesis
The QCD transition temperature: results with physical masses in the continuum limit II.
- Author
- Abt I.
- Abyzov A.
- Adams M.
- Albrecht H.
- Amaral V.
- Amorim A.
- Aplin S. J.
- Arefev A.
- Arino I.
- Atiya M.
- Aushev V.
- Bagaturia Y.
- Baghshetsyan R.
- Balagura V.
- Bargiotti M.
- Barsuk S.
- Barsukova O.
- Bassetti V.
- Bastos J.
- Bauer C.
- Bauer T. S.
- Beck M.
- Belkov A.
- Belkov Ar.
- Belotelov I.
- Belyaev I.
- Berkhan K.
- Bertin A.
- Bobchenko B.
- Bocker M.
- Bogatyrev A.
- Bohm G.
- Borgmeier C.
- Brauer M.
- Broemmelsiek D.
- Bruinsma M.
- Bruschi M.
- Buchholz P.
- Buchler M.
- Buran T.
- Capeans M.
- Capponi M.
- Carvalho J.
- Chamanina J.
- Chen B. X.
- Chistov R.
- Chmeissani M.
- Christensen A.
- Conde P.
- Cruse C.
- Dam M.
- Danielsen K. M.
- Danilov M.
- De Castro S.
- Deckers H.
- Dehmelt K.
- Deppe H.
- Dolgoshein B.
- Dong X.
- Dreis H. B.
- Dressel M.
- Dujmic D.
- Eckmann R.
- Egorytchev V.
- Ehret K.
- Eiges V.
- Eisele F.
- Emeliyanov D.
- Erhan S.
- Essenov S.
- Fabbri L.
- Faccioli P.
- Fallot-Burghardt W.
- Feuerstack-Raible M.
- Flammer J.
- Fleckenstein H.
- Fominykh B.
- Fourletov S.
- Fuljahn T.
- Funcke M.
- Galli D.
- Garcia A.
- Garrido L.
- Gascon D.
- Gellrich A.
- Gerndt K. E. K.
- Giacobbe B.
- Glass J.
- Glebe T.
- Goloubkov D.
- Golutvin A.
- Golutvin I.
- Gorbounov I.
- Gorisek A.
- Gouchtchine O.
- Goulart D. C.
- Gradl S.
- Gradl W.
- Guilitsky Yu.
- Hamacher T.
- Hansen J. D.
- Harr R.
- Hast C.
- Hausmann S.
- HERA-B Collaboration
- Hernandez J. M.
- Hildebrandt M.
- Hoepfner Kerstin
- Hofmann W.
- Hohlmann M.
- Holscher A.
- Hott T.
- Hulsbergen W.
- Husemann U.
- Igonkina O.
- Ispiryan M.
- Issever S.
- Itterbeck H.
- Ivarsson J.
- Jagla T.
- Jia Y.
- Jiang C.
- Kaoukher A.
- Kapitza H.
- Karabekyan S.
- Karchin P.
- Karpenko N.
- Ke Z.
- Keller S.
- Khasanov F.
- Kim H.
- Kiryushin Yu.
- Kisel I.
- Klefenz F.
- Knopfle K. T.
- Kochetkov V.
- Kolanoski H.
- Korpar S.
- Krauss C.
- Kreuzer P.
- Krizan P.
- Krucker D.
- Kvaratskheliia T.
- Lange Arnd
- Lanyov A.
- Lau K.
- Leffers G.
- Legrand I.
- Lewendel B.
- Liu Y. Q.
- Lohse T.
- Loke R.
- Lomonosov B.
- Ludemann J.
- Mankel R.
- Manner R.
- Marconi U.
- Masciocchi S.
- Massa I.
- Matchikhilian I.
- Medin G.
- Medinnis M.
- Mevius M.
- Michetti A.
- Mikhailov Yu.
- Miquel R.
- Mizuk R.
- Mohapatra A.
- Moshkin A.
- Moshous B.
- Muresan R.
- Nam S.
- Negodaev M.
- Negri I.
- Norenberg M.
- Nowak S.
- Nunez Pardo de Vera M. T.
- Oest T.
- Oliveira A.
- Ouchrif M.
- Ould-Saada F.
- Padilla C.
- Pakhlov P.
- Pavlenko Yu.
- Peralta D.
- Pernack R.
- Perschke T.
- Pestotnik R.
- Petersen B. A.
- Piccinini M.
- Pleier Marc-Andre
- Poli M.
- Popov V.
- Pose A.
- Pose D.
- Pugatch V. M.
- Pylypchenko Y.
- Pyrlik J.
- Ramachandran S.
- Ratnikov F.
- Reeves K.
- Ressing D.
- Riechmann K.
- Rieling J.
- Rietz M.
- Riu I.
- Robmann P.
- Rosen J.
- Rothe C.
- Ruckstuhl W.
- Rusinov V.
- Rybnikov V.
- Ryzhikov D.
- Saadi-Ludemann F.
- Samtleben D.
- Sanchez F.
- Sang M.
- Saveliev V.
- Sbrizzi A.
- Schaller S.
- Schlein P.
- Schmelling M.
- Schmidt B.
- Schmidt S.
- Schmidt-Parzefall W.
- Schreiner A.
- Schroder H.
- Schultz H. D.
- Schwanke U.
- Schwartz Alan J.
- Schwarz Andreas S.
- Schwenninger B.
- Schwingenheuer B.
- Schwitters R.
- Sciacca F.
- Semenov S.
- Semprini-Cesari N.
- Sexauer E.
- Seybold L.
- Shiu J.
- Shuvalov S.
- Siccama I.
- Skrk D.
- Soldatov A.
- Solunin S.
- Somov A.
- Somov S.
- Souvorov V.
- Sozuer L.
- Spahn M.
- Spengler J.
- Spighi R.
- Spiridonov A.
- Spratte S.
- St. Denis Richard Dante
- Stanovnik A.
- Staric M.
- Stegmann C.
- Steinbeck S.
- Steinkamp O.
- Stieler D.
- Straumann U.
- Sun F.
- Sun H.
- Symalla M.
- Takach S.
- Tesch N.
- Thurn H.
- Tikhomirov I.
- Titov Maxim P.
- Trunk U.
- Truoel Peter
- Tsakov I.
- Uwer U.
- Vagnoni V.
- van Eldik C.
- van Staa R.
- Vassiliev Yu.
- Villa M.
- Vitale A.
- Vukotic I.
- Wagner G.
- Wagner W.
- Wahlberg H.
- Walenta A. H.
- Walter M.
- Walter T.
- Wang J. J.
- Wang Y. M.
- Wanke R.
- Wegener D.
- Werthenbach U.
- Weyers P. J.
- Wolters H.
- Wurth R.
- Wurz A.
- Xella-Hansen S.
- Yang J.
- Zaitsev Yu.
- Zavertyaev M.
- Zech Gunter
- Zeuner T.
- Zhelezov A.
- Zheng Z.
- Zhu Z.
- Zimmermann R.
- Zivko T.
- Zoccoli A.
- Zweizig J.
- Publication venue
- 'IOP Publishing'
- Publication date
- 31/05/2002
- Field of study
We extend our previous study [Phys. Lett. B643 (2006) 46] of the cross-over
temperatures (T_c) of QCD. We improve our zero temperature analysis by using
physical quark masses and finer lattices. In addition to the kaon decay
constant used for scale setting we determine four quantities (masses of the
\Omega baryon, K^*(892) and \phi(1020) mesons and the pion decay constant)
which are found to agree with experiment. This implies that --independently of
which of these quantities is used to set the overall scale-- the same results
are obtained within a few percent. At finite temperature we use finer lattices
down to a <= 0.1 fm (N_t=12 and N_t=16 at one point). Our new results confirm
completely our previous findings. We compare the results with those of the
'hotQCD' collaboration.Comment: 19 pages, 8 figures, 3 table
Measurement of the Top Pair Production Cross Section in the Dilepton Decay Channel in ppbar Collisions at sqrt s = 1.96 TeV
- Author
- Aaltonen T
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Anh TV
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Badgett W
- Barbaro Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Bland KR
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Cabrera S
- Cakir IT
- Calancha C
- Camarda S
- Camillocci ES
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Canto A
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castanheira MTD
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli Sforza M
- Cerri A
- Cerrito L
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung WH
- Chung YS
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Datta M
- De Barbaro P
- De Cecco S
- De Lorenzo G
- DELL'ORSO MAURO
- Deluca C
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Devoto F
- Di Ruzza B
- Dittmann JR
- DONATI SIMONE
- Dong P
- Dorigo T
- Ebina K
- Elagin A
- Eppig A
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eusebi R
- Fang HC
- Farrington S
- Feindt M
- Fernandez JP
- Fernandez PM
- Ferrazza C
- Ferrer JAV
- Field R
- Flanagan G
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Furic I
- Gallego EV
- Gallinaro M
- Galyardt J
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerchtein E
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Ginsburg CM
- Giokaris N
- Giromini P
- Giunta M
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldin D
- Goldschmidt N
- Golossanov A
- Gomez Ceballos G
- Gomez G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Gresele A
- Grinstein S
- Griso SP
- Grosso Pilcher C
- Group RC
- Gunay Unalan Z
- Haber C
- Hahn SR
- Halkiadakis E
- Hamaguchi A
- Han JY
- Happacher F
- Hara K
- Hare D
- Hare M
- Harr RF
- Hatakeyama K
- Hays C
- Heck M
- Heinrich J
- Herndon M
- Hewamanage S
- Hidas D
- Hocker A
- Hopkins W
- Horn D
- Hou S
- Hughes RE
- Hurwitz M
- Husemann U
- Hussain N
- Hussein M
- Huston J
- Introzzi G
- Iori M
- Ivanov A
- James E
- Jang D
- Jayatilaka B
- Jeon EJ
- Jha MK
- Jindariani S
- Johnson W
- Jones M
- Joo KK
- Jun SY
- Junk TR
- Kamon T
- Karchin PE
- Kato Y
- Ketchum W
- Keung J
- Khotilovich V
- Kilminster B
- Kim DH
- Kim HS
- Kim HW
- Kim JE
- Kim MJ
- Kim SB
- Kim SH
- Kim YK
- Kimura N
- Klimenko S
- Kondo K
- Kong DJ
- Konigsberg J
- Korytov A
- Kotwal AV
- Kreps M
- Kroll J
- Krop D
- Krumnack N
- Kruse M
- Krutelyov V
- Kuhr T
- Kurata M
- Kwang S
- Laasanen AT
- Lami S
- Lammel S
- Lancaster M
- Lander RL
- Lannon K
- Lath A
- Latino G
- Lazzizzera I
- LeCompte T
- Lee E
- Lee HS
- Lee JS
- Lee SW
- Leo S
- Leone S
- Lewis JD
- Lin CJ
- Linacre J
- Lindgren M
- Lipeles E
- Lister A
- Litvintsev DO
- Liu C
- Liu Q
- Liu T
- Lockwitz S
- Lockyer NS
- Loginov A
- Lucchesi D
- Lueck J
- Lujan P
- Lukens P
- Lungu G
- Lys J
- Lysak R
- Madrak R
- Maeshima K
- Makhoul K
- Maksimovic P
- Malik S
- Manca G
- Manousakis Katsikakis A
- Margaroli F
- Marino C
- Martinez Ballarin R
- Martinez M
- Mastrandrea P
- Mathis M
- Mattson ME
- Mazzanti P
- McFarland KS
- McIntyre P
- McNulty R
- Mehta A
- Mehtala P
- Menzione A
- Mesropian C
- Miao T
- Mietlicki D
- Milosavljevic MV
- Mitra A
- Mitselmakher G
- Miyake H
- Moed S
- Moggi N
- Mondragon MN
- Moon CS
- Moore R
- Morello MJ
- Morlock J
- Mukherjee A
- Muller T
- Murat P
- Mussini M
- Nachtman J
- Nagai Y
- Naganoma J
- Nakano I
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- Publication venue
- Publication date
- 01/01/2010
- Field of study
Submitted to Phys. Rev. DA measurement of the \ttbar production cross section in \ppbar collisions at sâ = 1.96 TeV using events with two leptons, missing transverse energy, and jets is reported. The data were collected with the CDF II Detector. The result in a data sample corresponding to an integrated luminosity 2.8 fbâ1 is: \sigma_{\ttbar} = 6.27 ± 0.73(stat) ± 0.63(syst) ± 0.39(lum) pb. for an assumed top mass of 175 GeV/c2.A measurement of the ttÌ
production cross section in ppÌ
collisions at âs=1.96ââTeV using events with two leptons, missing transverse energy, and jets is reported. The data were collected with the CDF II detector. The result in a data sample corresponding to an integrated luminosity 2.8ââfb-1 is ÏttÌ
=6.27±0.73(stat)±0.63(syst)±0.39(lum)ââpb. for an assumed top mass of 175ââGeV/c2.Peer reviewe
Measurement of the top-quark mass in ttÂŻ events with dilepton final states in pp collisions at âs = 7 TeV
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- Publication date
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- Field of study
Open Access: This article is distributed under the terms of the Creative Commons Attribution License.-- Chatrchyan, S. et al.The top-quark mass is measured in proton-proton collisions at sâ=7 TeV using a data sample corresponding to an integrated luminosity of 5.0 fbâ1 collected by the CMS experiment at the LHC. The measurement is performed in the dilepton decay channel ttÂŻâ(â+Îœâb)(ââÎœÂŻÂŻâbÂŻ), where â=e,ÎŒ. Candidate top-quark decays are selected by requiring two leptons, at least two jets, and imbalance in transverse momentum. The mass is reconstructed with an analytical matrix weighting technique using distributions derived from simulated samples. Using a maximum-likelihood fit, the top-quark mass is determined to be 172.5±0.4 (stat.)±1.5 (syst.) GeV.Acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France);BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie program and the European Research Council (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt Foundation; the Austrian Science Fund (FWF); the Belgian Federal Science Policy Office; the Fonds pour la Formation Ă la Recherche dans lâIndustrie et dans lâAgriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWTBelgium); the Ministry of Education, Youth and Sports (MEYS) of Czech Republic; the Council of Science and Industrial Research, India; the Compagnia di San Paolo (Torino); and the HOMING PLUS program of Foundation for Polish Science, cofinanced from European Union, Regional Development Fund.Peer Reviewe
A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution
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- Ăzçelik Ă
- Publication venue
- Publication date
- 01/01/2020
- Field of study
We describe a method to obtain point and dispersion estimates for the energies of jets arising from b quarks produced in proton-proton collisions at an energy of s = 13 TeV at the CERN LHC. The algorithm is trained on a large sample of simulated b jets and validated on data recorded by the CMS detector in 2017 corresponding to an integrated luminosity of 41 fb - 1 . A multivariate regression algorithm based on a deep feed-forward neural network employs jet composition and shape information, and the properties of reconstructed secondary vertices associated with the jet. The results of the algorithm are used to improve the sensitivity of analyses that make use of b jets in the final state, such as the observation of Higgs boson decay to b b ÂŻ
Comprehensive molecular characterization of the hippo signaling pathway in cancer
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- Abeshouse A
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- Zmuda E
- Zuna R
- Zwarthoff EC
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2018
- Field of study
Hippo signaling has been recognized as a key tumor suppressor pathway. Here, we perform a comprehensive molecular characterization of 19 Hippo core genes in 9,125 tumor samples across 33 cancer types using multidimensional âomicâ data from The Cancer Genome Atlas. We identify somatic drivers among Hippo genes and the related microRNA (miRNA) regulators, and using functional genomic approaches, we experimentally characterize YAP and TAZ mutation effects and miR-590 and miR-200a regulation for TAZ. Hippo pathway activity is best characterized by a YAP/TAZ transcriptional target signature of 22 genes, which shows robust prognostic power across cancer types. Our elastic-net integrated modeling further reveals cancer-type-specific pathway regulators and associated cancer drivers. Our results highlight the importance of Hippo signaling in squamous cell cancers, characterized by frequent amplification of YAP/TAZ, high expression heterogeneity, and significant prognostic patterns. This study represents a systems-biology approach to characterizing key cancer signaling pathways in the post-genomic era
Measurements of pp â ZZ production cross sections and constraints on anomalous triple gauge couplings at â = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
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- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
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- Akchurin N
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 29/12/2020
- Field of study
© 2021 The CMS Collaboration. The production of Z boson pairs in protonâproton (pp) collisions, pp â (Z/â)(Z/â) â 2â2ââČ, where â,ââČ = e or ÎŒ, is studied at a center-of-mass energy of 13 TeV with the CMS detector at the CERN LHC. The data sample corresponds to an integrated luminosity of 137fbâ1, collected during 2016â2018. The ZZ production cross section, tot(pp â ZZ) = 17.4 ± 0.3 (stat) ± 0.5 (syst) ± 0.4 (Theo) ± 0.3 (lumi) pb, measured for events with two pairs of opposite-sign, same-flavor leptons produced in the mass region 60 < â+ââ < 120 GeV is consistent with standard model predictions. Differential cross sections are also measured and agree with theoretical predictions. The invariant mass distribution of the four-lepton system is used to set limits on anomalous ZZZ and ZZ couplings.SCOAP
Productive performance, egg-related indices, blood profiles, and interferon-Æ gene expression of laying Japanese quails fed on Tenebrio molitor
- Publication venue
- 'Informa UK Limited'
- Publication date
- Field of study
Serum proteins in healthy and diseased Florida manatees (Trichechus manatus latirostris)
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
- âŠ