576 research outputs found
Effects of using coding potential, sequence conservation and mRNA structure conservation for predicting pyrroly-sine containing genes
- Author
- B Chaudhuri
- B Knudsen
- C Notredame
- Christian Theil Have
- DG Longstaff
- E Torarinsson
- E Torarinsson
- EP Nawrocki
- GV Kryukov
- Henning Christiansen
- I Hofacker
- IL Hofacker
- IL Hofacker
- IU Heinemann
- J Atkins
- J Reeder
- JA Krzycki
- JD Thompson
- JD Thompson
- K Katoh
- M Bauer
- M Fujita
- M Höchsmann
- MA Gaston
- MA Gaston
- N Wirth
- S Bernhart
- S Lindgreen
- S Mørk
- S Will
- SE Seemann
- SF Altschul
- Sine Zambach
- T Abe
- TM Martin Simonsen
- X Xu
- Y Zhang
- Z Yao
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
BACKGROUND: Pyrrolysine (the 22nd amino acid) is in certain organisms and under certain circumstances encoded by the amber stop codon, UAG. The circumstances driving pyrrolysine translation are not well understood. The involvement of a predicted mRNA structure in the region downstream UAG has been suggested, but the structure does not seem to be present in all pyrrolysine incorporating genes. RESULTS: We propose a strategy to predict pyrrolysine encoding genes in genomes of archaea and bacteria. We cluster open reading frames interrupted by the amber codon based on sequence similarity. We rank these clusters according to several features that may influence pyrrolysine translation. The ranking effects of different features are assessed and we propose a weighted combination of these features which best explains the currently known pyrrolysine incorporating genes. We devote special attention to the effect of structural conservation and provide further substantiation to support that structural conservation may be influential – but is not a necessary factor. Finally, from the weighted ranking, we identify a number of potentially pyrrolysine incorporating genes. CONCLUSIONS: We propose a method for prediction of pyrrolysine incorporating genes in genomes of bacteria and archaea leading to insights about the factors driving pyrrolysine translation and identification of new gene candidates. The method predicts known conserved genes with high recall and predicts several other promising candidates for experimental verification. The method is implemented as a computational pipeline which is available on request
Bortezomib/docetaxel combination therapy in patients with anthracycline-pretreated advanced/metastatic breast cancer: a phase I/II dose-escalation study
- Author
- A Awada
- A Meluch
- AL Hamilton
- AP MacLaren
- BA Teicher
- C Aghajanian
- CL Vogel
- CN Papandreou
- D Kandioler-Eckersberger
- EA Eisenhauer
- EM Berns
- ES Lightcap
- F Cardoso
- F Cardoso
- GK Dy
- H Rosing
- HJ Lenz
- J Adams
- J Adams
- J Albanell
- J Baselga
- J Codony-Servat
- J O'Shaughnessy
- J Overgaard
- J Sjostrom
- JB Sunwoo
- JC Cusack
- JD Hainsworth
- JM Nabholtz
- K Colson
- L Y Dirix
- M Boccadoro
- M J Piccart
- M Tapia
- MC Bissery
- MH Shah
- MP Fanucchi
- NC Farneth
- P A Canney
- P Gascon
- P Lara Jr
- P Therasse
- PC Mack
- PD Pharoah
- PH Gumerlock
- PH Gumerlock
- PP Osin
- R Dreicer
- RC Kane
- RG Maki
- RZ Orlowski
- RZ Orlowski
- S Chan
- S Lonial
- S Williams
- SA Shah
- SE Jones
- SM Blaney
- ST Nawrocki
- ST Nawrocki
- T Gil
- T Hideshima
- T Ikezoe
- WA Messersmith
- YC Lin
- Publication venue
- Nature Publishing Group
- Publication date
- 01/05/2008
- Field of study
The aim of this study was to determine the dose-limiting toxicities (DLTs) and maximum tolerated dose (MTD) of bortezomib plus docetaxel in patients with anthracycline-pretreated advanced/metastatic breast cancer. Forty-eight patients received up to eight 21-day cycles of docetaxel (60–100 mg m−2 on day 1) plus bortezomib (1.0–1.5 mg m−2 on days 1, 4, 8, and 11). Pharmacodynamic and pharmacokinetic analyses were performed in a subset of patients. Five patients experienced DLTs: grade 3 bone pain (n=1) and febrile neutropenia (n=4). The MTD was bortezomib 1.5 mg m−2 plus docetaxel 75 mg m−2. All 48 patients were assessable for safety and efficacy. The most common adverse events were diarrhoea, nausea, alopecia, asthenia, and vomiting. The most common grade 3/4 toxicities were neutropenia (44%), and febrile neutropenia and diarrhoea (each 19%). Overall patient response rate was 29%. Median time to progression was 5.4 months. In patients with confirmed response, median time to response was 1.3 months and median duration of response was 3.2 months. At the MTD, response rate was 38%. Pharmacokinetic characteristics of bortezomib/docetaxel were comparable with single-agent data. Addition of docetaxel appeared not to affect bortezomib inhibition of 20S proteasome activity. Mean alpha-1 acid glycoprotein concentrations increased from baseline at nearly all time points across different bortezomib dose levels. Bortezomib plus docetaxel is an active combination for anthracycline-pretreated advanced/metastatic breast cancer. The safety profile is manageable and consistent with the side effects of the individual agents
Search for the standard model Higgs boson at LEP
- Author
- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbiendi G
- Abdallah J
- Abreu P
- Achard P
- Adam W
- Adriani O
- Adzic P
- Affholderbach K
- Aguilar-Benitez M
- Ainsley C
- Akesson PF
- Albrecht T
- Alcaraz J
- Alderweireld T
- Alemanni G
- Alemany-Fernandez R
- Alexander G
- Allaby J
- Allison J
- Allmendinger T
- Allport PP
- Aloisio A
- Alviggi MG
- Amaldi U
- Amapane N
- Amaral P
- Amato S
- Anagnostou G
- Anashkin E
- Anderhub H
- Anderson KJ
- Andreazza A
- Andreev VP
- Andringa S
- Anjos N
- Anselmo F
- Antilogus P
- Antonelli A
- Antonelli M
- Apel WD
- Arcelli S
- Arefiev A
- Armstrong SR
- Arnoud Y
- Asai S
- Ask S
- Asman B
- Augustin JE
- Augustinus A
- Awunor O
- Axen D
- Azemoon T
- Aziz T
- Azuelos G
- Azzurri P
- Baarmand M
- Badaud F
- Bagliesi G
- Bagnaia P
- Bailey I
- Baillon P
- Bajo A
- Baksay G
- Baksay L
- Baldew SV
- Ballestrero A
- Bambade P
- Banerjee S
- Banerjee S
- Barate R
- Barate R
- Barberio E
- Barbier R
- Barczyk A
- Bardin D
- Barillere R
- Barker G
- Barklow T
- Barlow RJ
- Baroncelli A
- Bartalini P
- Basile M
- Batalova N
- Batley RJ
- Battaglia M
- Battiston R
- Baubillier M
- Bay A
- Becattini F
- Bechtle P
- Becker U
- Becks KH
- Begalli M
- Behner F
- Behnke T
- Behrmann A
- Bell KW
- Bell PJ
- Bella G
- Bellerive A
- Bellucci L
- Ben-Haim E
- Bencivenni G
- Benekos N
- Benelli G
- Benvenuti A
- Berat C
- Berbeco R
- Berdugo J
- Berges P
- Berggren M
- Berkelman K
- Berntzon L
- Bertrand D
- Bertucci B
- Besancon M
- Besson N
- Betev BL
- Bethke S
- Beuselinck R
- Biasini M
- Biebell O
- Biglietti M
- Biland A
- Binnie DM
- Blair GA
- Blaising JJ
- Bloch D
- Bloch-Devaux B
- Blom M
- Blondel A
- Bloodworth IJ
- Bluj M
- Blumenschein U
- Blyth SC
- Bobbink GJ
- Boccali T
- Bock P
- Boeriun O
- Bohm A
- Bohrer A
- Boix G
- Boldizsar L
- Bologna G
- Bonacorsi D
- Bonesini M
- Bonissent A
- Boonekamp M
- Booth CN
- Booth PSL
- Borean C
- Borgia B
- Borisov G
- Bossi F
- Botner O
- Boucrot J
- Bouhova-Thacker E
- Boumediene D
- Bouquet B
- Bourilkov D
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- Bowcock TJV
- Bowdery CK
- Boyko I
- Braccini S
- Bracko M
- Braibant S
- Brandt S
- Branson JG
- Bravo S
- Brenner R
- Brient JC
- Brigliadori L
- Brochu F
- Brodet E
- Brown RM
- Bruckman P
- Bruneliere R
- Brunet JM
- Buchmuller O
- Buesser K
- Bugge L
- Buijs A
- Burckhart HJ
- Burger JD
- Burger WJ
- Buschmann P
- Cai XD
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- Cameron W
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- Camporesi T
- Canale V
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- Carnegie RK
- Caron B
- Carr J
- Cartacci A
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- Carter JR
- Cartwright S
- Casado MP
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- Castro N
- Cattaneo A
- Cavallari F
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- Cavanaugh R
- Cecchi C
- Cerrada M
- Cerutti F
- Chamizo M
- Chang CY
- Chang YH
- Chapkin M
- Charlton DG
- Charpentier P
- Checchia P
- Chemarin M
- Chen A
- Chen G
- Chen GM
- Chen HF
- Chen HS
- Chiarella V
- Chiefari G
- Chierici R
- Chiliapnikov P
- Chmeissani M
- Chudoba J
- Chung SU
- Cieslik K
- Cifarelli L
- Cindolo F
- Ciulli V
- Clare I
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- Clarke DP
- Clerbaux B
- Clifft RW
- Coignet G
- Colaleo A
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- Combley F
- Contri R
- Cosme G
- Cossutti F
- Costa MJ
- Costantini S
- Cowan G
- Coyle P
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- Crawley B
- Creanza D
- Crennell D
- Crespo JM
- Csilling A
- Cucciarelli S
- Cuevas J
- Cuffiani M
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- D'Hondt J
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- Dallavalle GM
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- De Bonis I
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- de Guevara PL
- de Jong R
- de la Cruz B
- De Lotto B
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- Di Simone A
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- Flagmeyer U
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- Frey A
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- Ganguli SN
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- Giacomelli G
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- Giammanco A
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- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Aaltonen
- Alvarez González
- Amerio
- Amidei
- Anastassov
- Annovi
- Antos
- Apollinari
- Appel
- Arisawa
- Artikov
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- Bauce
- Bedeschi
- Behari
- Bellettini
- Bellinger
- Benjamin
- Beretvas
- Bhatti
- Bisello
- Bizjak
- Bland
- Blumenfeld
- Bocci
- Bodek
- Bortoletto
- Boudreau
- Boveia
- Brigliadori
- Bromberg
- Brucken
- Budagov
- Budd
- Burkett
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- Chertok
- Chiarelli
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- Dittmann
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- Ginsburg
- Giokaris
- Giromini
- Giurgiu
- Glagolev
- Glenzinski
- Gold
- Goldin
- Goldschmidt
- Golossanov
- Gomez
- Gomez-Ceballos
- Goncharov
- González
- Gorelov
- Goshaw
- Goulianos
- Grillo
- Grinstein
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- Guimaraes Da Costa
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- Konigsberg
- Korolchuk VI
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- Rahaman
- Rahman I
- Ramakrishnan
- Rami A
- Ramm G
- Randall G
- Randow F
- Ranjan
- Rao VA
- Rathmell JC
- Ravikumar B
- Ray SK
- Redondo
- Reed BH
- Reed JC
- Reggiori F
- Reichert AS
- Reiners JJ Jr
- Reiter RJ
- Ren J
- Renton
- Rescigno
- Revuelta JL
- Rhodes CJ
- Riddick
- Rimondi
- Ristori
- Ritis K
- Rizzo E
- Robbins J
- Roberge M
- Robson
- Roca H
- Roccheri MC
- Rocchi S
- Rodemann HP
- Rodrigo
- Rodriguez
- Rodríguez de Córdoba S
- Rogers
- Rohrer B
- Rolli
- Roninson IB
- Rosen K
- Roser
- Rost-Roszkowska MM
- Rouis M
- Rouschop KM
- Rovetta F
- Rubin BP
- Rubinsztein DC
- Ruckdeschel K
- Rucker EB 3rd
- Rudich A
- Rudolf E
- Ruffini
- Ruiz
- Ruiz-Opazo N
- Russ
- Russo R
- Rusten TE
- Rusu
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- Ryter SW
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- S.R.
- S.S.
- S.W.
- S.Y.
- S.Y.
- S.Z.
- Sabatini DM
- Sadoshima J
- Safonov
- Saha T
- Saitoh T
- Sakagami H
- Sakai Y
- Sakumoto
- Sakurai
- Salekdeh GH
- Salomoni P
- Salvaterra PM
- Salvesen G
- Salvioli R
- Sanchez AM
- Sandri M
- Sankar U
- Sansanwal P
- Santambrogio L
- Santi
- Saran S
- Sarkar S
- Sarwal M
- Sasakawa C
- Sasnauskiene A
- Sass M
- Sato
- Sato K
- Sato M
- Saveliev
- Savoy-Navarro
- Schapira AH
- Scharl M
- Scheper W
- Schiaffino S
- Schlabach
- Schmidt
- Schmidt
- Schneider C
- Schneider ME
- Schneider-Stock R
- Schoenlein PV
- Schorderet DF
- Schwartz GK
- Schwarz
- Schätzl HM
- Schüller C
- Scodellaro
- Scorrano L
- Scribano
- Scuri
- Sealy L
- Seglen PO
- Segura-Aguilar J
- Seidel
- Seiliez I
- Seiya
- Seleverstov O
- Sell C
- Semenov
- Seo JB
- Separovic D
- Setaluri V
- Setoguchi T
- Settembre C
- Sforza
- Shacka JJ
- Shalhout
- Shanmugam M
- Shapiro IM
- Shaulian E
- Shaw RJ
- Shears
- Shelhamer JH
- Shen HM
- Shen WC
- Sheng ZH
- Shepard
- Shi Y
- Shibuya K
- Shidoji Y
- Shieh JJ
- Shih CM
- Shimada Y
- Shimizu S
- Shimojima
- Shintani T
- Shirihai OS
- Shochet
- Shore GC
- Shreyber-Tecker
- Sibirny AA
- Sidhu SB
- Sikorska B
- Silva-Zacarin EC
- Simmons A
- Simon AK
- Simon HU
- Simone C
- Simonenko
- Simonsen A
- Sinclair DA
- Sinervo
- Singh R
- Sinha D
- Sinicrope FA
- Sirko A
- Siu PM
- Sivridis E
- Skop V
- Skulachev VP
- Slack RS
- Sliwa
- Smaili SS
- Smith
- Smith DR
- Snider
- Soengas MS
- Soha
- Soldati T
- Song
- Song X
- Sood AK
- Soong TW
- Sorin
- Sotgia F
- Spector SA
- Spies CD
- Springer W
- Squillacioti
- Srinivasula SM
- St. Denis
- Stancari
- Stefanis L
- Steffan JS
- Stelzer
- Stelzer-Chilton
- Stendel R
- Stenmark H
- Stentz
- Stephanou A
- Stern ST
- Sternberg C
- Stork B
- Strologas
- Strycker
- Strålfors P
- Subauste CS
- Sudo
- Sui X
- Sukhanov
- Sulzer D
- Sun SY
- Sun J
- Sun ZJ
- Sung JJ
- Suslov
- Suzuki K
- Suzuki T
- Swanson MS
- Swanton C
- Sweeney ST
- Sy LK
- Szabadkai G
- Sánchez-Alcázar JA
- Sánchez-Prieto R
- T.
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- T.J.
- T.R.
- Tabas I
- Taegtmeyer H
- Tafani M
- Takano Y
- Takegawa K
- Takemasa
- Takemura G
- Takeshita F
- Takeuchi
- Takács-Vellai K
- Talbot NJ
- Tan KS
- Tanaka K
- Tanaka K
- Tang
- Tang D
- Tang D
- Tanida I
- Tannous BA
- Tavernarakis N
- Taylor GA
- Taylor GS
- Taylor JP
- Tecchio
- Teng
- Terada LS
- Terman A
- Tettamanti G
- Thevissen K
- Thom
- Thome
- Thompson
- Thompson CB
- Thomson
- Thorburn A
- Thumm M
- Tian F
- Tian Y
- Toback
- Tocchini-Valentini G
- Tokar
- Tolkovsky AM
- Tollefson
- Tomino Y
- Tomura
- Tonelli
- Tooze SA
- Torre
- Torretta
- Totaro
- Tournier C
- Tower J
- Towns R
- Trajkovic V
- Travassos LH
- Trovato
- Tsai TF
- Tschan MP
- Tsubata T
- Tsung A
- Turk B
- Turner LS
- Tyagi SC
- Tönges L
- U.
- U.K.
- Uchiyama Y
- Ueno T
- Ukegawa
- Umekawa M
- Umemiya-Shira
- Uozumi
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.E.
- Varganov
- Velev
- Vellidis
- Vidal
- Vila
- Vilar
- Vizán
- Vogel
- Volpi
- Vázquez
- W.
- W.
- W.
- W.
- W.-M.
- W.C.
- W.H.
- W.K.
- Wagner
- Wagner
- Wakisaka
- Wallny
- Wang
- Warburton
- Waters
- Wester
- Whiteson
- Wick
- Wicklund
- Wicklund
- Wilbur
- Williams
- Wilson
- Wilson
- Winer
- Wittich
- Wolbers
- Wolfe
- Wright
- Wu
- Wu
- X.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.C.
- Y.C.
- Y.D.
- Y.J.
- Y.K.
- Y.S.
- Yamamoto
- Yamato
- Yang
- 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
Search for supersymmetric particles in scenarios with a gravitino LSP and stau NLSP
- Author
- Abreu P
- Adam W
- Adye T
- Adzic P
- Albrecht Z
- Alderweireld T
- Alekseev GD
- Alemany R
- Allmendinger T
- Allport PP
- Almehed S
- Amaldi U
- Amapane N
- Amato S
- Anassontzis EG
- Andersson P
- Andreazza A
- Andringa S
- Antilogus P
- Apel WD
- Arnoud Y
- Asman B
- Augustin JE
- Augustinus A
- Baillon P
- Ballestrero A
- Bambade P
- Barao F
- Barbiellini G
- Barbier R
- Bardin DY
- Barker G
- Baroncelli A
- Battaglia M
- Baubillier M
- Becks KH
- Begalli M
- Behrmann A
- Beilliere P
- Belokopytov Y
- Belous K
- Benekos NC
- Benvenuti AC
- Berat C
- Berggren M
- Bertrand D
- Besancon M
- Bilenky MS
- Bizouard MA
- Bloch D
- Blom HM
- Bonesini M
- Boonekamp M
- Booth PSL
- Borisov G
- Bosio C
- Botner O
- Boudinov E
- Bouquet B
- Bourdarios C
- Bowcock TJV
- Boyko I
- Bozovic I
- Bozzo M
- Bracko M
- Branchini P
- Brenner RA
- Bruckman P
- Brunet JM
- Bugge L
- Buran T
- Buschbeck B
- Buschmann P
- Caballero IG
- Cabrera S
- Caccia M
- Calvi M
- Camporesi T
- Canale V
- Carena F
- Carroll L
- Caso C
- Cattai A
- Cavallo FR
- Chabaud V
- Chapkin M
- Charpentier P
- Checchia P
- Chelkov GA
- Chierici R
- Chliapnikov P
- Chochula P
- Chorowicz V
- Chudoba J
- Cieslik K
- Collaboration DELPHI
- Collins P
- Contri R
- Cortina E
- Cosme G
- Cossutti F
- Costa M
- Crawley HB
- Crennell D
- Crepe S
- Crosetti G
- Czellar S
- Da Silva W
- Davenport M
- De Angelis A
- De Boer W
- De Clercq C
- De Lotto B
- De Min A
- De Paula L
- Della Ricca G
- Delpierre P
- Demaria N
- Di Ciaccio L
- Dijkstra H
- Dolbeau J
- Doroba K
- Dracos M
- Drees J
- Dris M
- Duperrin A
- Durand JD
- Eigen G
- Ekelof T
- Ekspong G
- Ellert M
- Elsing M
- Engel JP
- Fanourakis G
- Fassouliotis D
- Fayot J
- Feindt M
- Ferrer A
- Ferrer-Ribas E
- Ferro F
- Fichet S
- Firestone A
- Flagmeyer U
- Foeth H
- Fokitis E
- Fontanelli F
- Franek B
- Frodesen AG
- Fruhwirth R
- Fulda-Quenzer F
- Fuster J
- Galloni A
- Gamba D
- Gamblin S
- Gandelman M
- Garcia C
- Garcia SMI
- Gaspar C
- Gaspar M
- Gasparini U
- Gavillet P
- Gazis EN
- Gele D
- Geralis T
- Ghodbane N
- Gil I
- Gimenez MVC
- Glege F
- Gokieli R
- Golob B
- Gomez-Ceballos G
- Goncalves P
- Gopal G
- Gorn L
- Gouz Y
- Gracco V
- Grahl J
- Graziani E
- Gris P
- Grosdidier G
- Grzelak K
- Guy J
- Haag C
- Hahn F
- Hahn S
- Haider S
- Hallgren A
- Hamacher K
- Hansen J
- Harris FJ
- Hauler F
- Hedberg V
- Heising S
- Hernandez JJ
- Herquet P
- Herr H
- Hessing TL
- Heuser JM
- Higon E
- Holmgren SO
- Holt PJ
- Hoorelbeke S
- Houlden M
- Hrubec J
- Huber M
- Huet K
- Hughes GJ
- Hultqvist K
- Jackson JN
- Jacobsson R
- Jalocha P
- Janik R
- Jarlskog C
- Jarlskog G
- Jarry P
- Jean-Marie B
- Jeans D
- Johansson EK
- Jonsson P
- Joram C
- Juillot P
- Jungermann L
- Kapusta F
- Karafasoulis K
- Katsanevas S
- Katsoufis EC
- Keranen R
- Kernel G
- Kersevan BP
- Khokhlov Y
- Khomenko BA
- Khovanski NN
- Kiiskinen A
- King B
- Kinvig A
- Kjaer NJ
- Klapp O
- Klein H
- Kluit P
- Kokkinias P
- Kostioukhine V
- Kourkoumelis C
- Kouznetsov O
- Krammer M
- Kriznic E
- Krumstein Z
- Kubinec P
- Kurowska J
- Kurvinen K
- Lamsa JW
- Lane DW
- Lapin V
- Laugier JP
- Lauhakangas R
- Leder G
- Ledroit F
- Lefebure V
- Leinonen L
- Leisos A
- Leitner R
- Lenzen G
- Lepeltier V
- Lesiak T
- Lethuillier M
- Libby J
- Liebig W
- Liko D
- Lipniacka A
- Lippi I
- Loerstad B
- Loken JG
- Lopes JH
- Lopez JM
- Lopez-Fernandez R
- Loukas D
- Lutz P
- Lyons L
- MacNaughton J
- Maestro JC
- Mahon JR
- Maio A
- Malek A
- Malmgren TGM
- Maltezos S
- Malychev V
- Mandl F
- Marco J
- Marco R
- Marechal B
- Margoni M
- Marin JC
- Mariotti C
- Markou A
- Martinez-Rivero C
- Masik J
- Mastroyiannopoulos N
- Matorras F
- Matteuzzi C
- Matthiae G
- Mazzucato F
- Mazzucato M
- McCubbin M
- McKay R
- McNulty R
- McPherson G
- Meroni C
- Meyer WT
- Miagkov A
- Migliore E
- Mirabito L
- Mitaroff WA
- Mjoernmark U
- Moa T
- Moch M
- Moeller R
- Moenig K
- Monge MR
- Moraes D
- Moreau X
- Morettini P
- Morton G
- Mueller U
- Muenich K
- Mulders M
- Mulet-Marquis C
- Muresan R
- Murray WJ
- Muryn B
- Myatt G
- Myklebust T
- Naraghi F
- Nassiakou M
- Navarria FL
- Nawrocki K
- Negri P
- Neufeld N
- Nicolaidou R
- Nielsen BS
- Niezurawski P
- Nikolenko M
- Nomokonov V
- Nygren A
- Obraztsov V
- Olshevski AG
- Onofre A
- Orava R
- Orazi G
- Osterberg K
- Ouraou A
- Oyanguren A
- Paganoni M
- Paiano S
- Pain R
- Paiva R
- Palacios J
- Palka H
- Papadopoulou TD
- Pape L
- Parkes C
- Parodi F
- Parzefall U
- Passeri A
- Passon O
- Pavel T
- Pegoraro M
- Peralta L
- Pernicka M
- Perrotta A
- Petridou C
- Petrolini A
- Phillips HT
- Pierre F
- Pimenta M
- Piotto E
- Podobnik T
- Pol ME
- Polok G
- Poropat P
- Pozdniakov V
- Privitera P
- Pukhaeva N
- Pullia A
- Radojicic D
- Ragazzi S
- Rahmani H
- Rames J
- Ratoff PN
- Read AL
- Rebecchi P
- Redaelli NG
- Regler M
- Rehn J
- Reid D
- Reinertsen P
- Reinhardt R
- Renton PB
- Resvanis LK
- Richard F
- Ridky J
- Rinaudo G
- Ripp-Baudot I
- Rohne O
- Romero A
- Ronchese P
- Rosenberg EI
- Rosinsky P
- Roudeau P
- Rovelli T
- Royon C
- Ruhlmann-Kleider V
- Ruiz A
- Saarikko H
- Sacquin Y
- Sadovsky A
- Sajot G
- Salt J
- Sampsonidis D
- Sannino M
- Santo ME
- Schwemling P
- Schwering B
- Schwickerath U
- Scuri F
- Seager P
- Sedykh Y
- Segar AM
- Seibert N
- Sekulin R
- Shellard RC
- Siebel M
- Simard L
- Simonetto F
- Sisakian AN
- Smadja G
- Smirnova O
- Smith GR
- Solovianov O
- Sopczak A
- Sosnowski R
- Spassov T
- Spiriti E
- Squarcia S
- Stanescu C
- Stanic S
- Stanitzki M
- Stevenson K
- Stocchi A
- Strauss J
- Strub R
- Stugu B
- Szczekowski M
- Szeptycka M
- Tabarelli T
- Taffard A
- Tegenfeldt F
- Terranova F
- Thomas J
- Timmermans J
- Tinti N
- Tkatchev LG
- Tobin M
- Todorova S
- Tomaradze A
- Tome B
- Tonazzo A
- Tortora L
- Tortosa P
- Transtromer G
- Treille D
- Tristram G
- Trochimczuk M
- Troncon C
- Turluer ML
- Tyapkin IA
- Tyapkin P
- Tzamarias S
- Ullaland O
- Uvarov V
- Valenti G
- Vallazza E
- Van Dam P
- Van den Boeck W
- Van Eldik J
- Van Lysebetten A
- van Remortel N
- Van Vulpen I
- Vegni G
- Ventura L
- Venus W
- Verbeure F
- Verdier P
- Verlato M
- Vertogradov LS
- Verzi V
- Vilanova D
- Vitale L
- Vlasov E
- Vodopyanov AS
- Voulgaris G
- Vrba V
- Wahlen H
- Walck C
- Washbrook AJ
- Weiser C
- Wicke D
- Wickens JH
- Wilkinson GR
- Winter M
- Witek M
- Wolf G
- Yi J
- Yushchenko O
- Zalewska A
- Zalewski P
- Zavrtanik D
- Zevgolatakos E
- Zimin NI
- Zintchenko A
- Zoller P
- Zucchelli GC
- Zumerle G
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2000
- Field of study
Sleptons, neutralinos and charginos were searched for in the context of
scenarios where the lightest supersymmetric particle is the gravitino. It was
assumed that the stau is the next-to-lightest supersymmetric particle. Data
collected with the DELPHI detector at a centre-of-mass energy near 189 GeV were
analysed combining the methods developed in previous searches at lower
energies. No evidence for the production of these supersymmetric particles was
found. Hence, limits were derived at 95% confidence level.Comment: 31 pages, 14 figure
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.
- Calancha C.
- Calderon A
- Calvo E
- Camarda S.
- Campanelli M.
- Campbell M.
- Campderros JD
- Camporesi T
- Canelli F.
- Cano E
- Carls B.
- Carlsmith D.
- Carosi R.
- Carrillo S.
- Carron S.
- Casal B.
- Casarsa M.
- Castro A.
- Catastini P.
- Cauz D.
- Cavaliere V.
- Cavalli-Sforza M.
- Cepeda M
- Cerminara G
- Cerrada M
- Cerri A.
- Cerrito L.
- Chen Y. C.
- Chertok M.
- Chiarelli G.
- Chlachidze G.
- Chlebana F.
- Cho K.
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chokheli D.
- Christiansen T
- Chuang SH
- Chung W. H.
- Chung Y. S.
- Cifuentes JAB
- Ciocci M. A.
- Clark A.
- Clarke C.
- Codispoti G
- Colino N
- Compostella G.
- Convery M. E.
- Conway J.
- Corbo M.
- Cordelli M.
- Cortabitarte RV
- Cox C. A.
- Cox D. J.
- Crescioli F.
- Cuevas J
- Cuevas J.
- Culbertson R.
- Cure B
- Cwiok M
- d'Ascenzo N.
- D'Enterria D
- d'Errico M.
- D'Onofrio M.
- da Costa J. Guimaraes
- Dagenhart D.
- Datta M.
- David A
- de Barbaro P.
- De La Cruz B
- De Roeck A
- de Troconiz JF
- Dell'Orso M
- Demortier L.
- Deninno M.
- Devoto F.
- Di Canto A.
- Di Ruzza B.
- Dittmann J. R.
- Djordjevic M
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- Yao W. -M.
- Yao W. -M.
- Yeh G. P.
- Yeh G. P.
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- Yoh J.
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- Zalewski R
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- 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
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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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
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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
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- Zeuner WD
- Zeyrek M
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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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- Civinini C
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- CMS Collaboration
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- Coughlan JA
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- Cremaldi LM
- Cripps N
- Cuevas J
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- Cumalat JP
- Cuplov V
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- Cushman P
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- 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
- Da Silva WLP
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
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- Das S
- Daskalakis G
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- Daubie E
- David A
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- de Barbaro P
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- de Cassagnac RG
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- de Monchenault GH
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- Eugster J
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- Zumerle G
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- 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
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- 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
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- Ziebarth EB
- Ziegler J
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- Zito G
- 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
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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- Abbaneo D
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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
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