607 research outputs found
Monitoring of nutrient limitation in growing E. coli: a mathematical model of a ppGpp-based biosensor
- Author
- A Battesti
- Alexandra Pokhilko
- CC DiRusso
- DM Raskin
- E Sarubbi
- GL Rosano
- H Cho
- H Trigui
- HD Murray
- HD Murray
- HJ Janssen
- HW Rhee
- J Monod
- J Wang
- JR Houser
- K Ochi
- K Potrykus
- KD Murray
- L Swint-Kruse
- M Jiang
- M Nomura
- M Seyfzadeh
- MA Zundel
- MB Elowitz
- MH Buckstein
- MM Barker
- MP Deutscher
- P Handke
- P Zhang
- R Kaplan
- RJ Heath
- RJ Heath
- RM Lennen
- S Angelini
- SD Colloms
- T Nystrom
- V Ancona
- V Hauryliuk
- X Lu
- X Zhang
- YJ Choi
- Z Rahman
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Rhesus macaque MHC class I molecules show differential subcellular localizations
- Author
- A Neisig
- AJ Blasky
- BR Mothe
- C Hammond
- Cornelia Rosner
- G Voss
- HD Hickman-Miller
- J Robinson
- JA Karl
- JA Urvater
- JE Boyson
- JK Kulski
- JP Scott-Browne
- JT Loffredo
- L Sibilio
- Lutz Walter
- M Bonhomme
- M Bonhomme
- M Garstka
- M Gromme
- M Nei
- MJ Bijlmakers
- MP Vierboom
- N Otting
- N Otting
- N Otting
- NB Myers
- NM Chiu
- Philip H. Kruse
- PJ Goulder
- R Daza-Vamenta
- R Dressel
- R Gruda
- Torben Lübke
- U Sauermann
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2010
- Field of study
The MHC class I gene family of rhesus macaques is characterised by considerable gene duplications. While a HLA-C-orthologous gene is absent, the Mamu-A and in particular the Mamu-B genes have expanded, giving rise to plastic haplotypes with differential gene content. Although some of the rhesus macaque MHC class I genes are known to be associated with susceptibility/resistance to infectious diseases, the functional significance of duplicated Mamu-A and Mamu-B genes and the expression pattern of their encoded proteins are largely unknown. Here, we present data of the subcellular localization of AcGFP-tagged Mamu-A and Mamu-B molecules. We found strong cell surface and low intracellular expression for Mamu-A1, Mamu-A2 and Mamu-A3-encoded molecules as well as for Mamu-B*01704, Mamu-B*02101, Mamu-B*04801, Mamu-B*06002 and Mamu-B*13401. In contrast, weak cell surface and strong intracellular expression was seen for Mamu-A4*1403, Mamu-B*01202, Mamu-B*02804, Mamu-B*03002, Mamu-B*05704, Mamu-I*010201 and Mamu-I*0121. The different expression patterns were assigned to the antigen-binding α1 and α2 domains, suggesting failure of peptide binding is responsible for retaining ‘intracellular’ Mamu class I molecules in the endoplasmic reticulum. These findings indicate a diverse functional role of the duplicated rhesus macaque MHC class I genes
Search for Kaluza-Klein Graviton Emission in ppˉ Collisions at s=1.8 TeV using the Missing Energy Signature
- Author
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Ambrose D
- Amidei D
- Anikeev K
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Badgett W
- Bailey S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Behari S
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berryhill J
- Bhatti A
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bolla G
- Bolshov A
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Brandl A
- Bromberg C
- Brozovic M
- Brubaker E
- Bruner N
- Budagov J
- Budd HS
- Burkett K
- Busetto G
- Byrum KL
- Cabrera S
- Calafiura P
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cecco SD
- Cerri A
- Cerrito L
- Chan AW
- Chang PS
- Chang PT
- Chapman J
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- Chen YC
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
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- Clark AG
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- Connolly A
- Convery M
- Conway J
- Cordelli M
- Cranshaw J
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- de Barbaro P
- de Troconiz JF
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- Flaugher B
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- Yao W
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2004
- Field of study
We report on a search for direct Kaluza-Klein graviton production in a data
sample of 84 pb−1 of \ppb collisions at s = 1.8 TeV, recorded
by the Collider Detector at Fermilab. We investigate the final state of large
missing transverse energy and one or two high energy jets. We compare the data
with the predictions from a 3+1+n-dimensional Kaluza-Klein scenario in which
gravity becomes strong at the TeV scale. At 95% confidence level (C.L.) for
n=2, 4, and 6 we exclude an effective Planck scale below 1.0, 0.77, and 0.71
TeV, respectively.Comment: Submitted to PRL, 7 pages 4 figures/Revision includes 5 figure
Novel insights into the mechanisms mediating the local antihypertrophic effects of cardiac atrial natriuretic peptide: role of cGMP-dependent protein kinase and RGS2
- Author
- A Dietrich
- A Kilic
- A Pfeifer
- Alexander Dietrich
- Andrea Gerling
- CE Grueter
- D Westermann
- DM Bers
- E Saygili
- E Takimoto
- E Takimoto
- EJ Tsai
- FL Martin
- GP Diniz
- GX Xie
- H Fujisaki
- HC Hercule
- HD Kleinert
- Hideo A. Baba
- J Hartmann
- J Sadoshima
- J Surapisitchat
- JA Hill
- Joel Abramowitz
- Josef M. Penninger
- Juan Eduardo Camacho Londoño
- Juliane Schröter
- JW Knowles
- K Katahira
- Katharina Völker
- KM Tang
- L Mazzolai
- LP He
- LR Castro
- LS Maier
- Lutz Birnbaumer
- M Errami
- M Föller
- M Hartmann
- M Kruse
- M Kuhn
- M Kuhn
- M Mongillo
- M Ozaki
- M Seth
- Marc Freichel
- Martin Kruse
- Michael Klaiber
- Michaela Kuhn
- MJ Lopez
- N Frey
- N Onohara
- N Takahahsi
- N Valtcheva
- Olaf Pongs
- P Osei-Owusu
- P Paradis
- R Feil
- R Holtwick
- Robert Feil
- S Kim
- S Weber
- SP Heximer
- Susanne Feil
- T Hofmann
- T Maack
- Y Li
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2010
- Field of study
Cardiac atrial natriuretic peptide (ANP) locally counteracts cardiac hypertrophy via the guanylyl cyclase-A (GC-A) receptor and cGMP production, but the downstream signalling pathways are unknown. Here, we examined the influence of ANP on β-adrenergic versus Angiotensin II (Ang II)-dependent (Gs vs. Gαq mediated) modulation of Ca2+i-handling in cardiomyocytes and of hypertrophy in intact hearts. L-type Ca2+ currents and Ca2+i transients in adult isolated murine ventricular myocytes were studied by voltage-clamp recordings and fluorescence microscopy. ANP suppressed Ang II-stimulated Ca2+ currents and transients, but had no effect on isoproterenol stimulation. Ang II suppression by ANP was abolished in cardiomyocytes of mice deficient in GC-A, in cyclic GMP-dependent protein kinase I (PKG I) or in the regulator of G protein signalling (RGS) 2, a target of PKG I. Cardiac hypertrophy in response to exogenous Ang II was significantly exacerbated in mice with conditional, cardiomyocyte-restricted GC-A deletion (CM GC-A KO). This was concomitant to increased activation of the Ca2+/calmodulin-dependent prohypertrophic signal transducer CaMKII. In contrast, β-adrenoreceptor-induced hypertrophy was not enhanced in CM GC-A KO mice. Lastly, while the stimulatory effects of Ang II on Ca2+-handling were absent in myocytes of mice deficient in TRPC3/TRPC6, the effects of isoproterenol were unchanged. Our data demonstrate a direct myocardial role for ANP/GC-A/cGMP to antagonize the Ca2+i-dependent hypertrophic growth response to Ang II, but not to β-adrenergic stimulation. The selectivity of this interaction is determined by PKG I and RGS2-dependent modulation of Ang II/AT1 signalling. Furthermore, they strengthen published observations in neonatal cardiomyocytes showing that TRPC3/TRPC6 channels are essential for Ang II, but not for β-adrenergic Ca2+i-stimulation in adult myocytes
Measurement of the average time-integrated mixing probability of b-flavored hadrons produced at the Tevatron
- Author
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Ambrose D
- Amidei D
- Anikeev K
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
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- Bhatti A
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
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- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bolla G
- Bolshov A
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Brandl A
- Bromberg C
- Brozovic M
- Brubaker E
- Bruner N
- Budagov J
- Budd HS
- Burkett K
- Busetto G
- Byrum KL
- Cabrera S
- Calafiura P
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cerri A
- Cerrito L
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Chen C
- Chen YC
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung JY
- Chung WH
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- Ciobanu CI
- Clark AG
- Coca M
- Connolly A
- Convery M
- Conway J
- Cordelli M
- Cranshaw J
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 08/09/2003
- Field of study
We have measured the number of like-sign (LS) and opposite-sign (OS) lepton
pairs arising from double semileptonic decays of b and bˉ-hadrons,
pair-produced at the Fermilab Tevatron collider. The data samples were
collected with the Collider Detector at Fermilab (CDF) during the 1992-1995
collider run by triggering on the existence of μμ and eμ candidates
in an event. The observed ratio of LS to OS dileptons leads to a measurement of
the average time-integrated mixing probability of all produced b-flavored
hadrons which decay weakly, χˉ=0.152±0.007 (stat.) ±0.011
(syst.), that is significantly larger than the world average χˉ=0.118±0.005.Comment: 47 pages, 10 figures, 15 tables Submitted to Phys. Rev.
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
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- Joo KK
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- Wyslouch B
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- Yi K
- Yi K
- Yilmaz Y
- Yoh J
- Yoo HD
- Yoon AS
- Yorita K
- Yoshida T
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- 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+→K+μ+μ−, B0→K∗(892)0μ+μ−, and Bs0→ϕ(1020)μ+μ− in a data sample
corresponding to 4.4fb−1 collected in ppˉ collisions at
s=1.96TeV by the CDF II detector at the Fermilab Tevatron
Collider. Using 121±16 B+→K+μ+μ− and 101±12 B0→K∗0μ+μ− 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 K∗0
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 Bs0→ϕμ+μ−decayandmeasureitsbranchingratio{\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
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
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- Cavalli-Sforza M
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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 W′ decaying
to an electron-neutrino pair in ppˉ 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 σ⋅B(W′→eν). Assuming standard
model couplings to fermions and the neutrino from the W′ boson decay to
be light, we exclude a W′ boson with mass less than
1.12\unit{TeV/}c^2 at the 95\unit{%} confidence level.Comment: 7 pages, 2 figures Submitted to PR
Measurements of the properties of Lambda_c(2595), Lambda_c(2625), Sigma_c(2455), and Sigma_c(2520) baryons
- Author
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- 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
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
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- Abolins M
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- Abreu H
- Abulaitia Y
- Acharya BS
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- Adelman J
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- Adye T
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- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
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- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alexandre G
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- Allbrooke BMM
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- Allport PP
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- Ceradini F
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- Chalupkova I
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- Da Cunha Sargedas De Sousa MJ
- Da Via C
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- Esposito B
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- Etienne F
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- Etienvre AI
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- Etzion E
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- Feigl S
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- Feng C
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- Formica A
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- Zaytsev A
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- Zerwas D
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- Zhao Z
- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- 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 direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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- 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
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