576 research outputs found
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Alderweireldt S
- Alexander J
- Aliev T
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- Auzinger G
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- Avetisyan A
- Avila C
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- Azhgirey I
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- Azzurri P
- Baarmand MM
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- Bacchetta N
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- Baden A
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- Baffioni S
- Bagliesi G
- Bahtiyar H
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
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- Banerjee S
- Banerjee S
- Bansal M
- Bansal S
- Barbagli G
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- Basegmez S
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- Chan KM
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- Chanon N
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- Charaf O
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- Chertok M
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- Chinellato J
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- Choudhury S
- Christiansen T
- Christopher G
- Chuang SH
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
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- Clarida W
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
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- Yildirim E
- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- Zeinali M
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- Zeyrek M
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- 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
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yildirim E
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
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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
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
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- Brinkerhoff A
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- Brochero Cifuentes JA
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- Choudhary BC
- Choudhury RK
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- Christiansen T
- Chuang SH
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- Chung YS
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
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- Cockerill DJA
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- Colafranceschi S
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- Contardo D
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- Conway J
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- Cooper SI
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- Correa Martins Junior M
- Cortezon EP
- Cossutti F
- Costa M
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- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Das S
- Daskalakis G
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- Daubie E
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- David A
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- de Barbaro P
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- de Cassagnac RG
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- de Troconiz JF
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- Yilmaz Y
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- Yun JC
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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
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Cumalat JP
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- Yilmaz Y
- Yohay R
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- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
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- Zarubin A
- Zatserklyaniy A
- Zeinali M
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- Zeyrek M
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- Zheng Y
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- Zhu B
- Zhu RY
- Zhukov V
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- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Search for anomalous t t-bar production in the highly-boosted all-hadronic final state
- Author
- A. A. Ocampo Rios
- A. Abdulsalam
- A. Adair
- A. Adiguzel
- A. Anastassov
- A. Apresyan
- A. Askew
- A. Attikis
- A. Avetisyan
- A. B. Meyer
- A. Baden
- A. Barker
- A. Bean
- A. Belyaev
- A. Belyaev
- A. Benaglia
- A. Beretvas
- A. Bethani
- A. Bhatti
- A. Bocci
- A. Bodek
- A. Bonato
- A. Bornheim
- A. Branca
- A. Brinkerhoff
- A. Burgmeier
- A. C. Benvenuti
- A. C. Marini
- A. C. Mignerey
- A. Cakir
- A. Calderon
- A. Campbell
- A. Castro
- A. Chatterjee
- A. Cimmino
- A. Colaleo
- A. Custódio
- A. David
- A. De Benedetti
- A. De Cosa
- A. De Roeck
- A. Deisher
- A. Delgado Peris
- A. Dermenev
- A. Dierlamm
- A. Dimitrov
- A. Dominguez
- A. Drozdetskiy
- A. Elliott-Peisert
- A. Ellithi Kamel
- A. Ershov
- A. Everett
- A. F. Barfuss
- A. F. Osorio Oliveros
- A. Fahim
- A. Falkiewicz
- A. Fanfani
- A. Ferapontov
- A. Ferrando
- A. Garcia-Bellido
- A. Gaz
- A. Geiser
- A. Ghezzi
- A. Giammanco
- A. Giassi
- A. Gilbert
- A. Givernaud
- A. Go
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- A. Gozzelino
- A. Graziano
- A. Gribushin
- A. Gude
- A. Guneratne Bryer
- A. Gurrola
- A. Gurtu
- A. Güth
- A. H. Ball
- A. Hahn
- A. Harel
- A. Heikkinen
- A. Heister
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- A. Ivanov
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- W. Wu
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- W.-S. Hou
- X. Janssen
- X. Meng
- X. Quan
- X. Shi
- X. T. Huang
- X. Wang
- Y Bai
- Y. Assran
- Y. Bai
- Y. Ban
- Y. Chao
- Y. Chen
- Y. Cho
- Y. Choi
- Y. Eshaq
- Y. F. Liu
- Y. Fu
- Y. Gao
- Y. Gershtein
- Y. Gotra
- Y. Guo
- Y. H. Chang
- Y. H. Chang
- Y. Hsiung
- Y. Iiyama
- Y. Ivanov
- Y. J. Lei
- Y. J. Lu
- Y. K. Choi
- Y. Kim
- Y. Kubota
- Y. Kuessel
- Y. Lu
- Y. M. Tzeng
- Y. Ma
- Y. Mao
- Y. Maravin
- Y. Musienko
- Y. Onel
- Y. Pakhotin
- Y. Roh
- Y. S. Chung
- Y. Sirois
- Y. Tschudi
- Y. Tu
- Y. W. Chang
- Y. Weng
- Y. Yang
- Y. Yilmaz
- Y. Zheng
- Y.-J. Lee
- YL Dokshitzer
- Yu. Andreev
- Z. Antunovic
- Z. C. Yang
- Z. Chen
- Z. Hatherell
- Z. Hu
- Z. J. Guo
- Z. K. Liu
- Z. L. Trocsanyi
- Z. Szillasi
- Z. Tsamalaidze
- Z. Wang
- Z. Zhang
- Zero J. Kim
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
A search is presented for a massive particle, generically referred to as a
Z', decaying into a t t-bar pair. The search focuses on Z' resonances that are
sufficiently massive to produce highly Lorentz-boosted top quarks, which yield
collimated decay products that are partially or fully merged into single jets.
The analysis uses new methods to analyze jet substructure, providing
suppression of the non-top multijet backgrounds. The analysis is based on a
data sample of proton-proton collisions at a center-of-mass energy of 7 TeV,
corresponding to an integrated luminosity of 5 inverse femtobarns. Upper limits
in the range of 1 pb are set on the product of the production cross section and
branching fraction for a topcolor Z' modeled for several widths, as well as for
a Randall--Sundrum Kaluza--Klein gluon. In addition, the results constrain any
enhancement in t t-bar production beyond expectations of the standard model for
t t-bar invariant masses larger than 1 TeV.Comment: Submitted to the Journal of High Energy Physics; this version
includes a minor typo correction that will be submitted as an erratu
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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- Yun JC
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- Zachariadou A
- Zalewski P
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- Zanetti M
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- Zatzerklyany A
- Zeidler C
- Zeinali M
- Zeise M
- Zelepoukine S
- Zeuner WD
- Zeyrek M
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- Zheng Y
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- Zhokin A
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- Zhu RY
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- Zhukova V
- Ziebarth EB
- Zielinski M
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
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- Zumerle G
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
Serelaxin as a potential treatment for renal dysfunction in cirrhosis: Preclinical evaluation and results of a randomized phase 2 trial
- Author
- A Escorsell
- A Krag
- A O’Brien
- Adrian Thomson
- Anna M. Hoy
- Antonella Pellicoro
- B Vairappan
- C Alessandria
- C Fagundes
- CA McIntyre
- Carmel M. Moran
- CD Tsien
- CH Leo
- D Barthelmes
- David J. Webb
- DE Newby
- Denise Yates
- Dilip Patel
- DO Debrah
- F Faul
- H Ring-Larsen
- Isaac Shaw
- J Besso
- J Fernandez
- J Novak
- J Trebicka
- JA Fallowfield
- Jeremy S. Duffield
- JM Salmeron
- JM Trawale
- John P. Iredale
- Jonathan A. Fallowfield
- JR Teerlink
- JT McGuane
- Judy Pak
- KP Conrad
- L Bax
- L Ruiz-del-Arbol
- M Jelinic
- M Martin-Llahi
- M Metra
- Maarten W. Taal
- Maurits A. Jansen
- MC Kew
- MC Smith
- N Shah
- NC McAvoy
- Neelesh Dongre
- Neil J. Lachlan
- NM Selby
- P Angeli
- Patrick W. F. Hadoke
- Peter C. Hayes
- Prakash Ramachandran
- R Garcia-Martinez
- R Moreau
- Rajnish Saini
- Rebecca L. Aucott
- RM Edwards
- RM Pereira
- Ross J. Lennen
- S Robertson
- Scott I. Semple
- SW Kim
- T Dschietzig
- TD Boyer
- Thomas Severin
- Timothy J. Kendall
- V Stadlbauer
- Victoria K. Snowdon
- Will Mungall
- XL Moore
- Z Kobalava
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2017
- Field of study
<div><p>Background</p><p>Chronic liver scarring from any cause leads to cirrhosis, portal hypertension, and a progressive decline in renal blood flow and renal function. Extreme renal vasoconstriction characterizes hepatorenal syndrome, a functional and potentially reversible form of acute kidney injury in patients with advanced cirrhosis, but current therapy with systemic vasoconstrictors is ineffective in a substantial proportion of patients and is limited by ischemic adverse events. Serelaxin (recombinant human relaxin-2) is a peptide molecule with anti-fibrotic and vasoprotective properties that binds to relaxin family peptide receptor-1 (RXFP1) and has been shown to increase renal perfusion in healthy human volunteers. We hypothesized that serelaxin could ameliorate renal vasoconstriction and renal dysfunction in patients with cirrhosis and portal hypertension.</p><p>Methods and findings</p><p>To establish preclinical proof of concept, we developed two independent rat models of cirrhosis that were characterized by progressive reduction in renal blood flow and glomerular filtration rate and showed evidence of renal endothelial dysfunction. We then set out to further explore and validate our hypothesis in a phase 2 randomized open-label parallel-group study in male and female patients with alcohol-related cirrhosis and portal hypertension. Forty patients were randomized 1:1 to treatment with serelaxin intravenous (i.v.) infusion (for 60 min at 80 μg/kg/d and then 60 min at 30 μg/kg/d) or terlipressin (single 2-mg i.v. bolus), and the regional hemodynamic effects were quantified by phase contrast magnetic resonance angiography at baseline and after 120 min. The primary endpoint was the change from baseline in total renal artery blood flow.</p><p>Therapeutic targeting of renal vasoconstriction with serelaxin in the rat models increased kidney perfusion, oxygenation, and function through reduction in renal vascular resistance, reversal of endothelial dysfunction, and increased activation of the AKT/eNOS/NO signaling pathway in the kidney. In the randomized clinical study, infusion of serelaxin for 120 min increased total renal arterial blood flow by 65% (95% CI 40%, 95%; <i>p <</i> 0.001) from baseline. Administration of serelaxin was safe and well tolerated, with no detrimental effect on systemic blood pressure or hepatic perfusion. The clinical study’s main limitations were the relatively small sample size and stable, well-compensated population.</p><p>Conclusions</p><p>Our mechanistic findings in rat models and exploratory study in human cirrhosis suggest the therapeutic potential of selective renal vasodilation using serelaxin as a new treatment for renal dysfunction in cirrhosis, although further validation in patients with more advanced cirrhosis and renal dysfunction is required.</p><p>Trial registration</p><p>ClinicalTrials.gov <a href="https://clinicaltrials.gov/ct2/show/NCT01640964" target="_blank">NCT01640964</a></p></div
Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams JR
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agapitos A
- Agram JL
- Ahmad A
- Ahmad M
- Ahuja S
- Akchurin N
- Akgun B
- Akin IV
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- Aleksandrov A
- Alexander J
- Alimena J
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anderson I
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- Pol ME
- Polatoz A
- Polese G
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- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popov A
- Popov V
- Potenza A
- Potenza R
- Poyraz D
- Pozdnyakov A
- Pozdnyakov I
- Pozzobon N
- Prado Da Silva WL
- Preuten M
- Primavera F
- Prokofyev O
- Prosper H
- Psallidas A
- Ptochos F
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- Pugliese G
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- Python Q
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- Razis PA
- Re V
- Rebane L
- Rebassoo F
- Redaelli N
- Redjimi R
- Redondo I
- Regnard S
- Reid ID
- Reis T
- Reithler H
- Rekovic V
- Renker D
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- Rezaei Hosseinabadi F
- Ribeiro Cipriano PM
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- Ricci-Tam F
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- Richman J
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- Rizzi A
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- Rodozov M
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- Rodrigues Antunes J
- Rodriguez JL
- Rodríguez-Marrero AY
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- Roland B
- Roland C
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- Rosowsky A
- Ross I
- Rossi AM
- Rossini M
- Rougny R
- Rovelli C
- Rovelli T
- Rovere M
- Roy D
- Ruchti R
- Ruiz Alvarez JD
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Rusakov SV
- Ruspa M
- Russ J
- Ryckbosch D
- Ryd A
- Rykaczewski H
- Ryu G
- Ryu MS
- Ryutin R
- Röcker S
- Sabes D
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- Safonov A
- Safronov G
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- Sakuma T
- Salazar Ibarguen HA
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- Salfeld-Nebgen J
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- Sanabria JC
- Sanchez-Hernandez A
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- Sandoval Gonzalez ID
- Sani M
- Santanastasio F
- Santaolalla J
- Santocchia A
- Santoro A
- Saoulidou N
- Sarangi T
- Sarkar S
- Sauvan JB
- Savin A
- Savoy-Navarro A
- Savrin V
- Saxena P
- Scarborough T
- Schael S
- Schettler H
- Schizzi A
- Schleper P
- Schlieckau E
- Schmidt A
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoerner-Sadenius T
- Schröder M
- Schulte JF
- Schwick C
- Schäfer C
- Schöfbeck R
- Scodellaro L
- Seez C
- Seidel M
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- Seitz C
- Seixas J
- Sekaric J
- Sekmen S
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- Senkin S
- Serban AT
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- Sexton-Kennedy E
- Sgandurra L
- Sguazzoni G
- Shalhout S
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- Shchutska L
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- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shipsey I
- Shmatov S
- Shoaib M
- Shrinivas A
- Shukla P
- Shumeiko N
- Siegrist P
- Sigamani M
- Sikler F
- Silkworth C
- Silva P
- Silvers D
- Silvestris L
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh G
- Singh JB
- Singovsky A
- Sinthuprasith T
- Sirois Y
- Siroli GP
- Sirunyan AM
- Skatchkov N
- Skhirtladze N
- Skinnari L
- Skovpen K
- Skuja A
- Smirnov I
- Smirnov V
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- Spiegel L
- Spiezia A
- Spiga D
- Spiridonov A
- Spiropulu M
- Squillacioti P
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- St John J
- Stadie H
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- Staiano A
- Starodumov A
- Steggemann J
- Steinbrück G
- Stenson K
- Stephans GS
- Stickland D
- Stieger B
- Stiliaris E
- Stober FM
- Stolin V
- Stolp D
- Stone R
- Stoye M
- Stoykova S
- Stoynev S
- Strauss J
- Stringer R
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- Strologas J
- Strom D
- Stuart D
- Stupak J
- Sturdy J
- Suarez Gonzalez J
- Suarez I
- Sudhakar K
- Sudic L
- Sulak L
- Sulimov V
- Sultanov G
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- Sumowidagdo S
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- Tabarelli de Fatis T
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- Teo WD
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- Thea A
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- Trocino D
- Trocsanyi ZL
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- Tsai JF
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- Tsirou A
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- Tuominen E
- Tuominiemi J
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- Ujvari B
- Ulmer KA
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- Veeraraghavan V
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- Velkovska J
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- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili M
- Vernieri C
- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal Marono M
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Vilela Pereira A
- Villella I
- Vinogradov A
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- Vorobiev I
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- Vorobyev A
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- Wickramage N
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- Wissing C
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- Wolf R
- Wolfe E
- Wolfe H
- Wollny H
- Womersley WJ
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- Wood JS
- Woodard A
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- Worm SD
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- Wulsin HW
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- Wyslouch B
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- Xiao H
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- Xie S
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- Zabel J
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- Zaganidis N
- Zakaria M
- Zalewski P
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- Zarubin A
- Zeinali M
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- Zeyrek M
- Zhang F
- Zhang J
- Zhang L
- Zhokin A
- Zhu RY
- Zhukov V
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- Zotto P
- Zou W
- Zsigmond AJ
- Zucchetta A
- Zumerle G
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- Zvada M
- Publication venue
- Publication date
- 01/01/2014
- Field of study
Peer reviewe
- …