1,103 research outputs found
Myc inhibition is effective against glioma and reveals a role for Myc in proficient mitosis.
- Author
- Publication venue
- Nat Commun
- Publication date
- 01/01/2014
- Field of study
Gliomas are the most common primary tumours affecting the adult central nervous system and respond poorly to standard therapy. Myc is causally implicated in most human tumours and the majority of glioblastomas have elevated Myc levels. Using the Myc dominant negative Omomyc, we previously showed that Myc inhibition is a promising strategy for cancer therapy. Here, we preclinically validate Myc inhibition as a therapeutic strategy in mouse and human glioma, using a mouse model of spontaneous multifocal invasive astrocytoma and its derived neuroprogenitors, human glioblastoma cell lines, and patient-derived tumours both in vitro and in orthotopic xenografts. Across all these experimental models we find that Myc inhibition reduces proliferation, increases apoptosis and remarkably, elicits the formation of multinucleated cells that then arrest or die by mitotic catastrophe, revealing a new role for Myc in the proficient division of glioma cells
High levels of the adhesion molecule CD44 on leukemic cells generate acute myeloid leukemia relapse after withdrawal of the initial transforming event
- Author
- B Yin
- C Buske
- C Roumier
- C Schessl
- DS Krause
- E Kroon
- E Kroon
- F Schneider
- H Kawagoe
- HJ Lawrence
- IP Touw
- J Borrow
- J Faber
- J Redondo-Munoz
- JL Grisolano
- JM Bjornsson
- KL Rhoades
- L Jin
- L Palmqvist
- LJ Bendall
- M Andreeff
- M Magnusson
- M Stefanidakis
- MC Magli
- MC Magli
- ML Nielsen
- N Pineault
- PB Staber
- PJ Valk
- PM Ayton
- RP Somerville
- S Goverdhana
- S Koschmieder
- S Legras
- SJ Erkeland
- SJ Horton
- T Lapidot
- T Nakamura
- TR Golub
- U Thorsteinsdottir
- U Thorsteinsdottir
- U Thorsteinsdottir
- W Yuan
- WF Shen
- WF Shen
- Y Yuan
- YY Wang
- Publication venue
- Nature Publishing Group
- Publication date
- 01/01/2010
- Field of study
Multiple genetic hits are detected in patients with acute myeloid leukemia (AML). To investigate this further, we developed a tetracycline-inducible mouse model of AML, in which the initial transforming event, overexpression of HOXA10, can be eliminated. Continuous overexpression of HOXA10 is required to generate AML in primary recipient mice, but is not essential for maintenance of the leukemia. Transplantation of AML to secondary recipients showed that in established leukemias, ∼80% of the leukemia-initiating cells (LICs) in bone marrow stopped proliferating upon withdrawal of HOXA10 overexpression. However, the population of LICs in primary recipients is heterogeneous, as ∼20% of the LICs induce leukemia in secondary recipients despite elimination of HOXA10-induced overexpression. Intrinsic genetic activation of several proto-oncogenes was observed in leukemic cells resistant to inactivation of the initial transformation event. Interestingly, high levels of the adhesion molecule CD44 on leukemic cells are essential to generate leukemia after removal of the primary event. This suggests that extrinsic niche-dependent factors are also involved in the host-dependent outgrowth of leukemias after withdrawal of HOXA10 overexpression event that initiates the leukemia
Angular and Current-Target Correlations in Deep Inelastic Scattering at HERA
- Author
- Abbiendi G
- Abe T
- Abramowicz H
- Acosta D
- Adamczyk L
- Adamus M
- Ahn Sh
- Amelung C
- An Sh
- Anselmo F
- Antonioli P
- Arneodo M
- Bacon Tc
- Badgett Wf
- Bailey Dc
- Bailey Ds
- Bamberger A
- Barbagli G
- Bari G
- Barreiro F
- Barret O
- Bashindzhagyan Gl
- Bashkirov V
- Basile M
- Bauerdick Lat
- Bednarek B
- Behrens U
- Bellagamba L
- Bertolin A
- Bhadra S
- Bienlein Jk
- Blaikley He
- Bohnet I
- Bokel C
- Boogert S
- Bornheim A
- Borzemski P
- Boscherini D
- Botje M
- Breitweg J
- Brock I
- Brook Nh
- Brugnera Riccardo
- Brummer N
- Bruni A
- Bruni G
- Burgard C
- Burow Bd
- Bussey Pj
- Butterworth Jm
- Bylsma B
- CA ZEUS Collaboration
- Caldwell A
- Capua M
- Carlin Roberto
- Cartiglia N
- Cashmore Rj
- Castellini G
- Catterall Cd
- Chapin D
- Chekanov S
- Chwastowski J
- Ciborowski J
- Cifarelli L
- Cindolo F
- Cirio R
- Cloth P
- Coboken K
- Coldewey C
- Cole Je
- Contin A
- COOPER SARKAR Am
- Coppola N
- Cormack C
- Corradi M
- Corriveau F
- Costa M
- Cottingham Wn
- Crittenden J
- Cross R
- D'Agostini G
- Dagan S
- DAL CORSO F
- Dardo M
- DE PASQUALE S
- DE WOLF E
- Deffner R
- DEL PESO J
- Deppe O
- Derrick M
- Deshpande A
- Desler K
- Devenish Rce
- Dhawan S
- Dolgoshein Ba
- Dondana S
- Dosselli U
- Doyle At
- Drews G
- Dulinski Z
- Durkin Ls
- Dusini S
- Eckert M
- Edmonds Jk
- Eisenberg Y
- Eisenhardt S
- Engelen J
- Epperson D
- Ermolov Pf
- Eskreys A
- Fagerstroem Cp
- Fernandez Jp
- Ferrero Mi
- Figiel J
- Filges D
- Foster B
- Foudas C
- FOX MURPHY A
- Fricke U
- Frisken Wr
- Fusayasu T
- Gadaj T
- Galea R
- Gallo E
- Garcia G
- Garcia Yz
- Garfagnini Alberto
- Gendner N
- Gialas I
- Gilmore J
- Ginsburg Cm
- Giusti P
- Gladilin Lk
- Glasman C
- Goebel F
- Golubkov Ya
- Gottlicher P
- Grabosch Hj
- Graciani R
- GROSSE KNETTER J
- Grzelak G
- Haas T
- Hain W
- HALL WILTON R
- Hamatsu R
- Hanna Ds
- Harnew N
- Hart Jc
- Hartmann H
- Hartmann J
- Hartner Gf
- Hasell D
- Hayes Me
- Heapby Ea
- Heath Gp
- Heath Hf
- Hebbel K
- Heinloth K
- Heinz L
- Hernandez Jm
- Heusch C
- Hilger E
- Hirose T
- Hochman D
- Holm U
- Homma K
- Hong Sj
- Howell G
- Hughes Vw
- Iacobucci G
- Iannotti L
- Iga Y
- Inuzuka M
- Ishii T
- Jakob Hp
- Jelen K
- Jeoung Hy
- Jing Z
- Johnson Kf
- Jones Tw
- Kananov S
- Kappes A
- Karshon U
- Kasemann M
- Katz Uf
- Kcira D
- Kerger R
- Khakzad M
- Khein La
- Kim Cl
- Kim Jy
- Kisielewska D
- Kitamura S
- Klanner R
- Klimek K
- Koch W
- Koffeman E
- Kooijman P
- Koop T
- Korotkova Na
- Korzhavina Ia
- Kotanski A
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- Kowal Am
- Kowalski H
- Kowalski T
- Krakauer D
- Kreisel A
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- Labarga L
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- Ling Ty
- Liu W
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- Lukina Oy
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- Okrasinski Jr
- Olkiewicz K
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- Palmonari F
- Park Ih
- Park Sk
- Parsons Ja
- Paul E
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- Pawlak Jm
- Pawlak R
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- Poelz G
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- Przybycien Mb
- Puga J
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- Raach H
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- Redondo I
- Reeder Dd
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- Ritz S
- Riveline M
- Rohde M
- Romeo Gc
- RULIKOWSKA ZAREBSKA E
- Ruske O
- Ruspa M
- Sabetfakhri A
- Sacchi R
- Sadrozinski Hfw
- Salehi H
- Sampson S
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- Saull Prb
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- Schlenstedt S
- Schmidke Wb
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- Schnurbusch H
- Schwarzer O
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- Shah Tp
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- Sideris D
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- Skillicorn Io
- Smalska B
- Smith Wh
- Solano A
- Solomin An
- Son D
- ST LAURENT M
- Staiano A
- Stairs Dg
- Stanco L
- Stanek R
- Stifutkin A
- Stonjek S
- Straub Pb
- Strickland E
- Stroili Roberto
- Susinno G
- Suszycki L
- Sutton Mr
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- Tandler J
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- Tapper Rj
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- Voci C
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- Walczak R
- Walker R
- Wang Sm
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- Waugh R
- Weber A
- Whitmore Jj
- Wichmann R
- Wick K
- Wieber H
- Wiggers L
- Wildschek T
- Williams Dc
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- Wodarczyk M
- Wolf G
- Wolfle S
- Wollmer U
- Wroblewski Ak
- Yamada S
- Yamashita T
- Yamauchi K
- Yamazaki Y
- Yoshida R
- Youngman C
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- Zakrzewski Ja
- Zarnecki Af
- Zawiejski L
- Zetsche F
- Zeuner W
- Zhu Q
- Zichichi A
- Zotkin Sa
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1999
- Field of study
Correlations between charged particles in deep inelastic ep scattering have
been studied in the Breit frame with the ZEUS detector at HERA using an
integrated luminosity of 6.4 pb-1. Short-range correlations are analysed in
terms of the angular separation between current-region particles within a cone
centred around the virtual photon axis. Long-range correlations between the
current and target regions have also been measured. The data support
predictions for the scaling behaviour of the angular correlations at high Q2
and for anti-correlations between the current and target regions over a large
range in Q2 and in the Bjorken scaling variable x. Analytic QCD calculations
and Monte Carlo models correctly describe the trends of the data at high Q2,
but show quantitative discrepancies. The data show differences between the
correlations in deep inelastic scattering and e+e- annihilation.Comment: 26 pages including 10 figures (submitted to Eur. J. Phys. C
Precise measurement of the W-boson mass with the CDF II detector
- Author
- Aaltonen T.
- Abbaneo D
- Adzic P
- Aguilar-Benitez M
- Ahmad M
- Ahmed I
- Albajar C
- Allfrey P
- Almeida N
- Alvarez Gonzalez B.
- Amerio S.
- Amidei D.
- Anastassov A.
- Andreev V
- Andreev Y
- Annovi A.
- Antos J.
- Apollinari G.
- Appel J. A.
- Arce P
- Arisawa T.
- Artikov A.
- Asaadi J.
- Asghar MI
- Ashmanskas W.
- Auerbach B.
- Auffray E
- Aurisano A.
- Auzinger G
- Azarkin M
- Azfar F.
- Azhgirey I
- Badgett W.
- Bae T.
- Baillon P
- Ball AH
- Barbaro-Galtieri A.
- Barnes V. E.
- Barnett B. A.
- Barney D
- Barria P.
- Bartos P.
- Battilana C
- Bauce M.
- Bedeschi F.
- Bedoya CF
- Beecher D.
- Behari S.
- Bell AJ
- Bellettini G.
- Bellinger J.
- Belotelov I
- Benedetti D
- Benjamin D.
- Beretvas A.
- Bernet C
- Bhatti A.
- Bialas W
- Bilinskas MJ
- Binkley M.
- Bisello D.
- Bitioukov S
- Bizjak I.
- Bland K. R.
- Bloch P
- Blumenfeld B.
- Bocci A
- Bocci A.
- Bodek A.
- Bolognesi S
- Bondar N
- Boos E
- Bortoletto D.
- Boudreau J.
- Boveia A.
- Breuker H
- Brigliadori L.
- Bromberg C.
- Brona G
- Brucken E.
- Budagov J.
- Budd H. S.
- Bunin P
- Bunkowski K
- Burelo ED
- Burkett K.
- Busetto G.
- Bussey P.
- Butler PH
- Buzatu A.
- Caballero IG
- Cabrillo IJ
- Calamba A.
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- Campderros JD
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- Warburton A.
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- Weinberger M.
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- Winer B. L.
- Wittich P.
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- Wohri HK
- Wolbers S.
- Wolbers S.
- Wolfe H.
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- Wright T.
- Wrochna G
- Wu X.
- Wu X.
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- Yamamoto K.
- Yamamoto K.
- Yamaoka J.
- Yamato D.
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- Yang T.
- Yang U. K.
- Yang U. K.
- Yang Y. C.
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- Yao W. -M.
- Yao W. -M.
- Yeh G. P.
- Yeh G. P.
- Yi K.
- Yi K.
- Yoh J.
- Yoh J.
- Yorita K.
- Yorita K.
- Yoshida T.
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- Yu G. B.
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- Yun J. C.
- Yun J. C.
- Zalewski R
- Zanetti A.
- Zanetti A.
- Zarubin A
- Zeng Y.
- Zeng Y.
- Zhokin A
- Zhou C.
- Zucchelli S..
- Zucchelli S..ng S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We have measured the W-boson mass MW using data corresponding to 2.2/fb of
integrated luminosity collected in proton-antiproton collisions at 1.96 TeV
with the CDF II detector at the Fermilab Tevatron collider. Samples consisting
of 470126 W->enu candidates and 624708 W->munu candidates yield the measurement
MW = 80387 +- 12 (stat) +- 15 (syst) = 80387 +- 19 MeV. This is the most
precise measurement of the W-boson mass to date and significantly exceeds the
precision of all previous measurements combined
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Bellettini
- Bellinger
- Benjamin
- Beretvas
- Bhatti
- Bisello
- Bizjak
- Bland
- Blumenfeld
- Bocci
- Bodek
- Bortoletto
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- Ginsburg
- Giokaris
- Giromini
- Giurgiu
- Glagolev
- Glenzinski
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- Goldschmidt
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- Goncharov
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- Yang
- Yang
- Yao
- Yeh
- Yi
- Yoh
- Yorita
- Yoshida
- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta MV
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
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- Zoeller MH
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Czellar S
- D'Agnolo RT
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- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
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- Aliev T
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- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
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- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
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- Wissing C
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- Won S
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- Wood JS
- Worm SD
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- Wyslouch B
- Xiao H
- Xie S
- Xu M
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- Yang F
- Yang M
- Yang Y
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram JL
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Measurement of the Z/gamma* + b-jet cross section in pp collisions at 7 TeV
- Author
- Abbaneo D.
- Abbiendi G.
- Abbrescia M.
- Abdullin S.
- Acosta D.
- Acosta J. G.
- Acosta M. Vazquez
- Adair A.
- Adam N.
- Adam W.
- Adams M. R.
- Adams T.
- Adiguzel A.
- Adler V.
- Adzic P.
- Afanasiev S.
- Agostino L.
- Agram J-L
- Aguilar-Benitez M.
- Aguilo E.
- Ahmad M.
- Ahmad W. Haj
- Ahuja S.
- Akchurin N.
- Akgun B.
- Akgun U.
- Akin I. V.
- Alagoz E.
- Albajar C.
- Albayrak E. A.
- Albergo S.
- Albrow M.
- Alcaraz Maestre J.
- Alda Junior W. L.
- Alexander J.
- Aliev T.
- Almeida N.
- Alver B.
- Alverson G.
- Alves G. A.
- Amapane N.
- Amsler C.
- Anagnostou G.
- Anastassov A.
- Anderson J.
- Anderson M.
- Andrea J.
- Andreev V.
- Andreev V.
- Andreev Yu.
- Andrews W.
- Anghel I. M.
- Anjos T. S.
- Antonelli L.
- Antunes J. Rodrigues
- Antunovic Z.
- Apanasevich L.
- Apollinari G.
- Appelt E.
- Apresyan A.
- Aranyi A.
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- Arcidiacono R.
- Arenton M. W.
- Arfaei H.
- Argiro S.
- Arisaka K.
- Arneodo M.
- Arora S.
- Asawatangtrakuldee C.
- Asghar M. I.
- Askew A.
- Assran Y.
- Ata M.
- Atac M.
- Atramentov O.
- Attikis A.
- Auffray E.
- Autermann C.
- Auzinger G.
- Avdeeva E.
- Avery P.
- Avetisyan A.
- Azarkin M.
- Azhgirey I.
- Aziz T.
- Azzi P.
- Azzolini V.
- Azzurri P.
- Baarmand M. M.
- Babb J.
- Bacchetta N.
- Bachtis M.
- Baden A.
- Baeni L.
- Baesso P.
- Baffioni S.
- Bagliesi G.
- Bai Y.
- Baillon P.
- Bainbridge R.
- Bakhshiansohi H.
- Bakirci M. N.
- Bakken J. A.
- Balazs M.
- Ball A. H.
- Ball G.
- Ban Y.
- Banerjee S.
- Banerjee S.
- Bansal S.
- Banzuzi K.
- Barbagli G.
- Barberis E.
- Barbone L.
- Bardak C.
- Barfuss A. F.
- Bargassa P.
- Barge D.
- Baringer P.
- Barker A.
- Barnes V. E.
- Barnett B. A.
- Barney D.
- Barone L.
- Barrett M.
- Bartalini P.
- Barth C.
- Basegmez S.
- Basso L.
- Battilana C.
- Baty C.
- Bauer G.
- Bauerdick L. A. T.
- Baumgartel D.
- Baur U.
- Bayshev I.
- Bazterra V. E.
- Bean A.
- Beauceron S.
- Beaudette F.
- Beaupere N.
- Bedjidian M.
- Beernaert K.
- Behrenhoff W.
- Behrens U.
- Belforte S.
- Beliy N.
- Belknap D.
- Bell A. J.
- Bell K. W.
- Bellan P.
- Bellan R.
- Bellinger J. N.
- Belotelov I.
- Belyaev A.
- Belyaev A.
- Benaglia A.
- Bencze G.
- Bendavid J.
- Benedetti D.
- Benelli G.
- Benhabib L.
- Beni N.
- Benucci L.
- Benussi L.
- Benvenuti A. C.
- Beranek S.
- Beretvas A.
- Bergauer T.
- Berger J.
- Bergholz M.
- Beri S. B.
- Bernardes C. A.
- Bernardini J.
- Bernet C.
- Berry D.
- Berry E.
- Berryhill J.
- Bertl W.
- Berzano U.
- Besancon M.
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- Weinberg M.
- Wendland L.
- Weng J.
- Weng Y.
- Wenger E. A.
- Werner J. S.
- West C.
- Wetzel J.
- Whitbeck A.
- Whitmore J.
- Whyntie T.
- Wickens J.
- Wickramage N.
- Widl E.
- Wigmans R.
- Wilken R.
- Wilkinson R.
- Williams G.
- Williams T.
- Willmott C.
- Wimpenny S.
- Winn D.
- Winstrom L.
- Wissing C.
- Wittich P.
- Wittmer B.
- Woehri H. K.
- Wolf M.
- Wolf R.
- Womersley W. J.
- Won S.
- Wood D.
- Wood J.
- Wood J. S.
- Worm S. D.
- Wright D.
- Wrochna G.
- Wu W.
- Wuerthwein F.
- Wulz C-E
- Wyslouch B.
- Xiao H.
- Xie S.
- Xu M.
- Yagil A.
- Yalvac M.
- Yang F.
- Yang M.
- Yang Y.
- Yang Z. C.
- Yazgan E.
- Yelton J.
- Yetkin T.
- Yi K.
- Yildirim E.
- Yilmaz Y.
- Yohay R.
- Yoo H. D.
- Yoo J.
- Yoon A. S.
- York A.
- Yu I.
- Yu S. S.
- Yumiceva F.
- Yun J. C.
- Zabel J.
- Zabi A.
- Zablocki J.
- Zaganidis N.
- Zakaria M.
- Zalewski P.
- Zanetti M.
- Zang J.
- Zang S. L.
- Zarubin A.
- Zatserklyaniy A.
- Zeinali M.
- Zeise M.
- Zeuner W. D.
- Zeyrek M.
- Zhang J.
- Zhang Z.
- Zheng Y.
- Zhokin A.
- Zhu B.
- Zhu R. Y.
- Zhukov V.
- Zhukova V.
- Ziebarth E. B.
- Ziegler J.
- Zielinski M.
- Zito G.
- Zoeller M. H.
- Zotto P.
- Zou W.
- Zumerle G.
- Zuranski A.
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
The production of b jets in association with a Z/gamma* boson is studied
using proton-proton collisions delivered by the LHC at a centre-of-mass energy
of 7 TeV and recorded by the CMS detector. The inclusive cross section for
Z/gamma* + b-jet production is measured in a sample corresponding to an
integrated luminosity of 2.2 inverse femtobarns. The Z/gamma* + b-jet cross
section with Z/gamma* to ll (where ll = ee or mu mu) for events with the
invariant mass 60 < M(ll) < 120 GeV, at least one b jet at the hadron level
with pT > 25 GeV and abs(eta) < 2.1, and a separation between the leptons and
the jets of Delta R > 0.5 is found to be 5.84 +/- 0.08 (stat.) +/- 0.72 (syst.)
+(0.25)/-(0.55) (theory) pb. The kinematic properties of the events are also
studied and found to be in agreement with the predictions made by the MadGraph
event generator with the parton shower and the hadronisation performed by
PYTHIA.Comment: Submitted to the Journal of High Energy Physic
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