60 research outputs found
Genetically-Directed, Cell Type-Specific Sparse Labeling for the Analysis of Neuronal Morphology
- Author
- A Burns
- A Duque
- A Sik
- A Tsiola
- AG Leventhal
- AJ Beitz
- AN van den Pol
- BA Szmajda
- BH Wainer
- C Liu
- CG Lobe
- CM Yates
- DL Price
- DM Dacey
- DM Dacey
- DS Auld
- E Hamel
- E Lucas-Meunier
- Eshel Ben-Jacob
- EV Famiglietti Jr
- G Feng
- H Wellmann
- H Zong
- IJ Kim
- J Livet
- JE Bestman
- Jeremy Nathans
- JL Morgan
- John Williams
- K Moriyoshi
- L Peichl
- L Wittner
- LR Fischer
- M D'Apuzzo
- P Davies
- P Young
- Philip M. Smallwood
- PJ Whitehouse
- R Feil
- S Gong
- S Gong
- S Gustincich
- S Hayashi
- S Ramon y Cajal
- SC Fields-Berry
- SM Ngoi
- T Badea
- T Badea
- T Lee
- TC Jakobs
- Thomas Rotolo
- WB Gan
- XG Li
- YW Wong
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
Background: In mammals, genetically-directed cell labeling technologies have not yet been applied to the morphologic analysis of neurons with very large and complex arbors, an application that requires extremely sparse labeling and that is only rendered practical by limiting the labeled population to one or a few predetermined neuronal subtypes. Methods and Findings: In the present study we have addressed this application by using CreER technology to noninvasively label very small numbers of neurons so that their morphologies can be fully visualized. Four lines of IRES-CreER knock-in mice were constructed to permit labeling selectively in cholinergic or catecholaminergic neurons [choline acetyltransferase (ChAT)-IRES-CreER or tyrosine hydroxylase (TH)-IRES-CreER], predominantly in projection neurons [neurofilament light chain (NFL)-IRES-CreER], or broadly in neurons and some glia [vesicle-associated membrane protein2 (VAMP2)-IRES-CreER]. When crossed to the Z/AP reporter and exposed to 4-hydroxytamoxifen in the early postnatal period, the number of neurons expressing the human placental alkaline phosphatase reporter can be reproducibly lowered to fewer than 50 per brain. Sparse Cre-mediated recombination in ChAT-IRES-CreER;Z/AP mice shows the full axonal and dendritic arbors of individual forebrain cholinergic neurons, the first time that the complete morphologies of these very large neurons have been revealed in any species. Conclusions: Sparse genetically-directed, cell type-specific neuronal labeling with IRES-creER lines should prove useful fo
Measurement of the Forward-Backward Asymmetry in the B -> K(*) mu+ mu- Decay and First Observation of the Bs -> phi mu+ mu- Decay
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
- Albrow M
- Alexander J
- Almenar CC
- Alver B
- Alverson G
- Amerio S
- Amidei D
- Anastassov A
- Anastassov A
- Anderson J
- Anghel IM
- Annovi A
- Antonelli L
- Antos J
- Apanasevich L
- Apollinari G
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Atac M
- Auerbach B
- Aurisano A
- Avery P
- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
- Bandurin D
- Banerjee S
- Barbaro-Galtieri A
- Barberis E
- Baringer P
- Barnes VE
- Barnes VE
- Barnett BA
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Bendavid J
- Benelli G
- Benjamin D
- Beretvas A
- Beretvas A
- Berry D
- Berry E
- Berryhill J
- Betchart B
- Betts RR
- Bhat PC
- Bhatti A
- Bhatti A
- Bilki B
- Binkley M
- Biselli A
- Bisello D
- Bizjak I
- Bland KR
- Blekman F
- Bloch I
- Blocker C
- Bloom K
- Blumenfeld B
- Blumenfeld B
- Bocci A
- Bochenek J
- Bodek A
- Bodek A
- Boeriu O
- Bolla G
- Bolton T
- Bonato A
- Borcherding F
- Borrello L
- Bortoletto D
- Bortoletto D
- Bose S
- Boudreau J
- Boulahouache C
- Bourilkov D
- Boutemeur M
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Burkett K
- Busetto G
- Bussey P
- Busza W
- Butler JN
- Butt J
- Butz E
- Buzatu A
- Bylsma B
- Cabrera S
- Calamba A
- Calancha C
- Cali IA
- Callner J
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Cankocak K
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carroll R
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cavanaugh R
- Ceballos GG
- Ceron C
- Cerri A
- Cerrito L
- Chakaberia I
- Chan M
- Chasco M
- Chatterjee A
- Chen J
- Chen M
- Chen YC
- Chertok M
- Chetluru V
- Cheung HWK
- Chiarelli G
- Chlachidze G
- Chlebana F
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung WH
- Chung YS
- Chung YS
- Cihangir S
- Ciobanu CI
- Ciocci MA
- Cirino G
- Claes DR
- Clarida W
- Clark A
- Clark D
- Cole P
- Compostella G
- Convery ME
- Conway J
- Cooper SI
- Corbo M
- Cordelli M
- Cox CA
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- Cremaldi LM
- Crescioli F
- Cuevas J
- Culbertson R
- Cumalat JP
- Cuplov V
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- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dahmes B
- Das S
- Datta M
- de Barbaro P
- de Barbaro P
- De Benedetti A
- De Cecco S
- De Lorenzo G
- Dell'Orso M
- Deluca C
- Demarteau M
- Demina R
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Devoto F
- Di Canto A
- Di Giovanni GP
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- Dinardo ME
- Dittmann JR
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- Farrington S
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- Glenzinski D
- Gleyzer SV
- Godang R
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- Hatakeyama K
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- Husemann U
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- Jayatilaka B
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- Johnson KF
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- Joo KK
- Joshi U
- Jun SY
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- Junk TR
- Kaadze K
- Kalakhety H
- Kamon T
- Karchin PE
- Karmgard DJ
- Kato Y
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- Khotilovich V
- Khukhunaishvili A
- Killewald P
- Kilminster B
- Kilminster B
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- Yao WM
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- Yi K
- Yi K
- Yilmaz Y
- Yoh J
- Yoo HD
- Yoon AS
- Yorita K
- Yoshida T
- Yu GB
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Yun JC
- Zabel J
- Zablocki J
- Zakaria M
- Zanetti A
- Zanetti M
- Zang SL
- Zatserklyaniy A
- Zeng Y
- Zennamo J
- Zhang J
- Zheng Y
- Zhu RY
- Zhukova V
- Ziegler J
- Zielinski M
- Zucchelli SZucchelli Sira D
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We reconstruct the rare decays B+âK+Îź+Îźâ, B0âKâ(892)0Îź+Îźâ, and Bs0ââĎ(1020)Îź+Îźâ in a data sample
corresponding to 4.4fbâ1 collected in ppËâ collisions at
sâ=1.96TeV by the CDF II detector at the Fermilab Tevatron
Collider. Using 121Âą16 B+âK+Îź+Îźâ and 101Âą12 B0âKâ0Îź+Îźâ decays we report the branching ratios. In addition, we report
the measurement of the differential branching ratio and the muon
forward-backward asymmetry in the B+ and B0 decay modes, and the Kâ0
longitudinal polarization in the B0 decay mode with respect to the squared
dimuon mass. These are consistent with the theoretical prediction from the
standard model, and most recent determinations from other experiments and of
comparable accuracy. We also report the first observation of the Bs0ââĎÎź+Îźâdecayandmeasureitsbranchingratio{\mathcal{B}}(B^0_s \to
\phi\mu^+\mu^-) = [1.44 \pm 0.33 \pm 0.46] \times 10^{-6}using27 \pm 6signalevents.ThisiscurrentlythemostrareB^0_s$ decay observed.Comment: 7 pages, 2 figures, 3 tables. Submitted to Phys. Rev. Let
Measurements of the properties of Lambda_c(2595), Lambda_c(2625), Sigma_c(2455), and Sigma_c(2520) baryons
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
- Albrow M
- Alexander J
- Almenar CC
- Alver B
- Alverson G
- Amerio S
- Amidei D
- Anastassov A
- Anastassov A
- Anderson J
- Anghel IM
- Annovi A
- Antonelli L
- Antos J
- Apanasevich L
- Apollinari G
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Atac M
- Auerbach B
- Aurisano A
- Avery P
- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
- Bandurin D
- Banerjee S
- Barbaro-Galtieri A
- Barberis E
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- Zeng Y
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- Zucchelli S Zucchelli Slli Sira D
- Zucchelli SZanetti A
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report measurements of the resonance properties of Lambda_c(2595)+ and
Lambda_c(2625)+ baryons in their decays to Lambda_c+ pi+ pi- as well as
Sigma_c(2455)++,0 and Sigma_c(2520)++,0 baryons in their decays to Lambda_c+
pi+/- final states. These measurements are performed using data corresponding
to 5.2/fb of integrated luminosity from ppbar collisions at sqrt(s) = 1.96 TeV,
collected with the CDF II detector at the Fermilab Tevatron. Exploiting the
largest available charmed baryon sample, we measure masses and decay widths
with uncertainties comparable to the world averages for Sigma_c states, and
significantly smaller uncertainties than the world averages for excited
Lambda_c+ states.Comment: added one reference and one table, changed order of figures, 17
pages, 15 figure
Search for a New Heavy Gauge Boson Wprime with Electron + missing ET Event Signature in ppbar collisions at sqrt(s)=1.96 TeV
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
- Albrow M
- Alexander J
- Almenar CC
- Alver B
- Alverson G
- Amerio S
- Amidei D
- Anastassov A
- Anastassov A
- Anderson J
- Anghel IM
- Annovi A
- Antonelli L
- Antos J
- Apanasevich L
- Apollinari G
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Atac M
- Auerbach B
- Aurisano A
- Avery P
- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
- Bandurin D
- Banerjee S
- Barbaro-Galtieri A
- Barberis E
- Baringer P
- Barnes VE
- Barnes VE
- Barnett BA
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Bendavid J
- Benelli G
- Benjamin D
- Beretvas A
- Beretvas A
- Berry D
- Berry E
- Berryhill J
- Betchart B
- Betts RR
- Bhat PC
- Bhatti A
- Bilki B
- Binkley M
- Biselli A
- Bisello D
- Bizjak I
- Bland KR
- Blekman F
- Bloch I
- Bloom K
- Blumenfeld B
- Blumenfeld B
- Bocci A
- Bochenek J
- Bodek A
- Bodek A
- Boeriu O
- Bolla G
- Bolton T
- Bonato A
- Borcherding F
- Borrello L
- Bortoletto D
- Bortoletto D
- Bose S
- Boudreau J
- Boulahouache C
- Bourilkov D
- Boutemeur M
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Burkett K
- Busetto G
- Bussey P
- Busza W
- Butler JN
- Butt J
- Butz E
- Buzatu A
- Bylsma B
- Calamba A
- Calancha C
- Cali IA
- Callner J
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Cankocak K
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carroll R
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cavanaugh R
- Ceballos GG
- Ceron C
- Cerri A
- Cerrito L
- Chakaberia I
- Chan M
- Chasco M
- Chatterjee A
- Chen J
- Chen M
- Chen YC
- Chertok M
- Chetluru V
- Cheung HWK
- Chiarelli G
- Chlachidze G
- Chlebana F
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung WH
- Chung YS
- Chung YS
- Cihangir S
- Ciobanu CI
- Ciocci MA
- Cirino G
- Claes DR
- Clarida W
- Clark A
- Cole P
- Compostella G
- Convery ME
- Conway J
- Cooper SI
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Cremaldi LM
- Crescioli F
- Cuevas J
- Culbertson R
- Cumalat JP
- Cuplov V
- Cushman P
- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dahmes B
- Das S
- Datta M
- de Barbaro P
- de Barbaro P
- De Benedetti A
- De Cecco S
- De Lorenzo G
- Dell'Orso M
- Deluca C
- Demarteau M
- Demina R
- Demortier L
- Deng J
- Deninno M
- Devoto F
- Di Canto A
- Di Giovanni GP
- Di Ruzza B
- Diamond B
- Dinardo ME
- Dittmann JR
- Dobur D
- Dominguez A
- Donati S
- Dong P
- Dorigo T
- Dorney B
- Dragoiu C
- Drell BR
- Drozdetskiy A
- Dudero PR
- Durkin LS
- Duru F
- Dutta V
- Eads M
- Eartly DP
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- Zucchelli Slli Sira D
- Zucchelli SYun JC
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2010
- Field of study
We present a search for a new heavy charged vector boson WⲠdecaying
to an electron-neutrino pair in ppËâ collisions at a center-of-mass
energy of 1.96\unit{TeV}. The data were collected with the CDF II detector
and correspond to an integrated luminosity of 5.3\unit{fb}^{-1}. No
significant excess above the standard model expectation is observed and we set
upper limits on Ďâ
B(Wâ˛âeν). Assuming standard
model couplings to fermions and the neutrino from the WⲠboson decay to
be light, we exclude a WⲠboson with mass less than
1.12\unit{TeV/}c^2 at the 95\unit{%} confidence level.Comment: 7 pages, 2 figures Submitted to PR
X-ray emission from the Sombrero galaxy: discrete sources
- Author
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- de Barbaro P
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- 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
Search for heavy bottom-like quarks decaying to an electron or muon and jets in ppËâ collisions at sâ=1.96 TeV
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
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- Almenar CC
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- Anastassov A
- Anastassov A
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- Anghel IM
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- Artikov A
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- Askew A
- Atac M
- Auerbach B
- Aurisano A
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- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
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- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
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- Bedeschi F
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- Bodek A
- Bodek A
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- Bonato A
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- Zielinski M
- Zucchelli Si Sira D
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report the most sensitive direct search for pair production of
fourth-generation bottom-like chiral quarks (bâ˛) each decaying promptly to
tW. We search for an excess of events with an electron or muon, at least five
jets (one indentified as due to a b or c quark) and an imbalance of
transverse momentum using data from ppËâ collisions collected by the CDF
II detector at Fermilab with an integrated luminosity of 4.8 fbâ1. We
observe events consistent with background expectation and calculate upper
limits on the bⲠpair production cross section (Ďbbâ˛Ëââ˛30 fb for mbâ˛â>375 GeV/c2) and exclude mbâ˛â<372 \gevcc at 95%
confidence level.Comment: For submission to PR
Search for dijet resonances in 7 TeV pp collisions at CMS
- Author
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- Wrochna G
- Wu JH
- Wu W
- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
- Xie S
- Yagil A
- Yan M
- Yang F
- Yang M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- 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
- Zennamo J
- 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
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
This is the Pre-print version of the Article. The official published version of the paper can be accessed from the link below - Copyright @ 2010 APSA search for narrow resonances in the dijet mass spectrum is performed using data corresponding to an integrated luminosity of 2.9ââpb-1 collected by the CMS experiment at the Large Hadron Collider. Upper limits at the 95% confidence level are presented on the product of the resonance cross section, branching fraction into dijets, and acceptance, separately for decays into quark-quark, quark-gluon, or gluon-gluon pairs. The data exclude new particles predicted in the following models at the 95% confidence level: string resonances, with mass less than 2.50 TeV, excited quarks, with mass less than 1.58 TeV, and axigluons, colorons, and E6 diquarks, in specific mass intervals. This extends previously published limits on these models.This work is supported by FMSR (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); Academy of Sciences and NICPB (Estonia); Academy of Finland, ME, 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); PAEC (Pakistan); SCSR (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MST and MAE (Russia); MSTD (Serbia); MICINN and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); TUBITAK and TAEK (Turkey); STFC (United Kingdom); DOE and NSF (USA)
Transverse-momentum and pseudorapidity distributions of charged hadrons in pp collisions at âs=7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
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- Acosta MV
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- Yetkin T
- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang SL
- Zarubin A
- Zatzerklyaniy A
- Zeidler C
- Zeinali M
- Zeise M
- Zennamo J
- 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
- Zinonos Z
- Zito G
- Zoeller MH
- Zorbilmez C
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Charged-hadron transverse-momentum and pseudorapidity distributions in proton-proton collisions at âs=7ââTeV are measured with the inner tracking system of the CMS detector at the LHC. The charged-hadron yield is obtained by counting the number of reconstructed hits, hit pairs, and fully reconstructed charged-particle tracks. The combination of the three methods gives a charged-particle multiplicity per unit of pseudorapidity dNch/dΡ||Ρ|<0.5=5.78Âą0.01(stat)Âą0.23(syst) for non-single-diffractive events, higher than predicted by commonly used models. The relative increase in charged-particle multiplicity from âs=0.9 to 7 TeV is [66.1Âą1.0(stat)Âą4.2(syst)]%. The mean transverse momentum is measured to be 0.545Âą0.005(stat)Âą0.015(syst)ââGeV/c. The results are compared with similar measurements at lower energies
Dijet azimuthal decorrelations in pp collisions at âs = 7TeV
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- Xiao H
- Xie S
- Xu M
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- 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 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
- American Physical Society
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Measurements of dijet azimuthal decorrelations in pp collisions at âs=7ââTeV using the CMS detector at the CERN LHC are presented. The analysis is based on an inclusive dijet event sample corresponding to an integrated luminosity of 2.9ââpb-1. The results are compared to predictions from perturbative QCD calculations and various Monte Carlo event generators. The dijet azimuthal distributions are found to be sensitive to initial-state gluon radiation
Measurement of the B+ production cross section in pp collisions at âs = 7 TeV
- Author
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Measurements of the total and differential cross sections dĎ/dpTB and dĎ/dyB for B+ mesons produced in pp collisions at âs=7ââTeV are presented. The data correspond to an integrated luminosity of 5.8ââpb-1 collected by the CMS experiment operating at the LHC. The exclusive decay B+âJ/ĎK+, with J/ĎâÎź+Îź-, is used to detect B+ mesons and to measure the production cross section as a function of pTB and yB. The total cross section for pTB>5ââGeV and |yB|<2.4 is measured to be 28.1Âą2.4Âą2.0Âą3.1ââÎźb, where the first uncertainty is statistical, the second is systematic, and the last is from the luminosity measurement
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