1,399 research outputs found
Cancer management during COVID-19 pandemic: is immune checkpoint inhibitors-based immunotherapy harmful or beneficial?
- Publication venue
- 'MDPI AG'
- Publication date
- 01/08/2020
- Field of study
The coronavirus disease 2019 (COVID-19) is currently representing a global health threat especially for fragile individuals, such as cancer patients. It was demonstrated that cancer patients have an increased risk of developing a worse symptomatology upon severe acute respiratory syndrome associated coronavirus-2 (SARS-CoV-2) infection, often leading to hospitalization and intensive care. The consequences of this pandemic for oncology are really heavy, as the entire healthcare system got reorganized. Both oncologists and cancer patients are experiencing rescheduling of treatments and disruptions of appointments with a concurrent surge of fear and stress. In this review all the up-to-date findings, concerning the association between COVID-19 and cancer, are reported. A remaining very debated question regards the use of an innovative class of anti-cancer molecules, the immune checkpoint inhibitors (ICIs), given their modulating effects on the immune system. For that reason, administration of ICIs to cancer patients represents a question mark during this pandemic, as its correlation with COVID-19-associated risks is still under investigation. Based on the mechanisms of action of ICIs and the current evidence, we suggest that ICIs not only can be safely administered to cancer patients, but they might even be beneficial in COVID-19-positive cancer patients, by exerting an immune-stimulating action
Axis II comorbidity of borderline personality disorder: description of 6-year course and prediction to time-to-remission
- Publication venue
- 'Wiley'
- Publication date
- 01/12/2004
- Field of study
Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/65824/1/j.1600-0447.2004.00362.x.pd
Pathologic characteristics of resected squamous cell carcinoma of the trachea: prognostic factors based on an analysis of 59 cases
- Author
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2009
- Field of study
While squamous cell carcinoma (SCC) is the most common tracheal malignancy, few reports describe the pathologic considerations that may guide intraoperative decisions and prognostic assessment. We reviewed 59 tracheal SCC treated between 1985 and 2008 by segmental resection of the trachea, including resection of the carina in 24% and inferior larynx in 14%. We classified these tumors by grading histologic differentiation and microscopic features used in SCC of other sites. Of 59 tumors, 24% (14 of 59) were well differentiated, 49% (29 of 59) were moderately differentiated, and 27% (16 of 59) were poorly differentiated. Unfavorable prognostic factors were tumor extension into the thyroid gland (all of five so-afflicted patients died of tumor progression within 3 years) and lymphatic invasion (mean survival 4.6 versus 7.6 years). Keratinization, dyskeratosis, acantholysis, necrosis, and tumor thickness did not predict prognosis. As surgical resection is the only curative treatment; the surgeon should establish clean lines of resection using, as appropriate, intraoperative frozen section. The pathologist can provide additional important prognostic information, including tumor differentiation and extent, invasion of surgical margins, and extension into the thyroid
The stellar and sub-stellar IMF of simple and composite populations
- Author
- A Duquennoy
- A Maeder
- A Parravano
- A Sollima
- A Sollima
- A Stolte
- A Vazdekis
- A Vazdekis
- AA Muench
- AE Piskunov
- AJ Cenarro
- AN Belikov
- AP Whitworth
- AR Boss
- AS Eddington
- AT Myers
- B Binggeli
- B García
- B Reipurth
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- C Briceño
- C Esteban
- C Flynn
- C Grillo
- C Hayashi
- C Koen
- C Low
- C Reylé
- C Soubiran
- C Weidner
- C Weidner
- C Weidner
- C Weidner
- C Weidner
- C Weidner
- C Weidner
- C Yasui
- CA Tout
- CJ Clarke
- CJ Grillmair
- CJ Lada
- CJ Lonsdale
- CL Slesnick
- CM Baugh
- CM Boily
- D Calzetti
- D Gouliermis
- D Gouliermis
- D Stamatellos
- D Stamatellos
- D Stamatellos
- D Stamatellos
- D Vanbeveren
- DA Fischer
- DA Forbes
- DA Tilley
- DA Tilley
- DC Heggie
- DF Figer
- DJ Pinfield
- DJ Price
- DR Weisz
- E Brocato
- E Casuso
- E Corbelli
- E Moraux
- E Schilbach
- E Vesperini
- E Vesperini
- EA Evstigneeva
- EA Hoversten
- EE Salpeter
- F D’Antona
- F Egusa
- F Motte
- F Najarro
- F Palla
- F Paresce
- F Selman
- FC Adams
- FC Adams
- FD Kahn
- G Basri
- G Bosch
- G Chabrier
- G Chabrier
- G Chabrier
- G Chabrier
- G Chabrier
- G Chabrier
- G Duchêne
- G Garcia-Segura
- G Garcia-Segura
- G Marchi de
- G Marchi de
- G Marchi De
- G Piotto
- G Weigelt
- G Wuchterl
- G Wuchterl
- GE Miller
- GR Blumenthal
- GR Meurer
- H Bartko
- H Baumgardt
- H Baumgardt
- H Bouy
- H Jahreiss
- H Kirk
- H Sana
- H Zinnecker
- H Zinnecker
- HT Janka
- I Baraffe
- I Misgeld
- I Thies
- I Thies
- I Thies
- I Thies
- IA Bonnell
- IA Bonnell
- IA Bonnell
- IA Bonnell
- IA Bonnell
- IA Bonnell
- IN Reid
- IN Reid
- IN Reid
- IN Reid
- J Binney
- J Bouvier
- J Dabringhausen
- J Dabringhausen
- J Dabringhausen
- J Jijina
- J Köppen
- J Maíz Apellániz
- J Maíz Apellániz
- J Maíz Apellániz
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Pflamm-Altenburg
- J Strader
- JB Lamb
- JC Tan
- JD Neill
- JE Dale
- JE Gizis
- JH Jeans
- JJ Bochanski
- JL Beuzit
- JL Halbwachs
- JM Kirk
- JM Oliveira
- JM Scalo
- JN Bahcall
- JP Anderson
- JS Kalirai
- JS Ulvestad
- K Fuhrmann
- K Kuijken
- KD Finkelstein
- KL Luhman
- KL Luhman
- KS Boer de
- L Siess
- L Testi
- LA Hillenbrand
- LA Hillenbrand
- LJ Smith
- LM Close
- LR Penny
- M Andersen
- M Andersen
- M Beech
- M Dominik
- M Fellhauer
- M Fellhauer
- M Fellhauer
- M Fellhauer
- M Fumagalli
- M Haywood
- M Mac Low
- M Marks
- M Marks
- M Marks
- M Marks
- M Marks
- M Marks
- M Nagashima
- M Ramspeck
- M Schmalzl
- M Schwarzschild
- M Sirianni
- MA Pérez-Torres
- MG Wolfire
- MJ Disney
- MN Machida
- MN Machida
- MR Bate
- MR Bate
- MR Bate
- MR Krumholz
- MR Krumholz
- MR Krumholz
- MS Oey
- MS Oey
- N Bastian
- N Ivanova
- N Kevlahan
- N Lodieu
- N McCrady
- N Moeckel
- N Murray
- N Phan-Bao
- N Reid
- N Rio Da
- NC Hambly
- NC Hambly
- O Malkov
- OY Malkov
- P Girichidis
- P Hennebelle
- P Hennebelle
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Kroupa
- P Massey
- P Massey
- P Padoan
- P Padoan
- P Wang
- PA Crowther
- PC Clark
- PC Myers
- PFL Maxted
- PG Dokkum van
- PG Dokkum van
- PJE Peebles
- PP Papadopoulos
- PP Papadopoulos
- PR Allen
- R Chini
- R Fuente Marcos de La
- R Kudritzki
- R Parra
- R Wojtak
- R Wünsch
- RB Larson
- RB Larson
- RB Stothers
- RC Kennicutt Jr
- RJ Parker
- RJ Parker
- RJ Parker
- RJ Smith
- RJ White
- RS Klessen
- RS Klessen
- RS Stobie
- S Banerjee
- S Basu
- S Basu
- S Bontemps
- S Dib
- S Dib
- S Djorgovski
- S Feltzing
- S Hocuk
- S Mieske
- S Mieske
- S Nayakshin
- S Recchi
- S Roychowdhury
- S Röser
- S Shen
- S Zucker
- SD Murray
- SF Portegies Zwart
- SJ Aarseth
- SLW McMillan
- SM Wilkins
- SP Goodwin
- SP Goodwin
- SP Goodwin
- SP Goodwin
- SP Goodwin
- SS Kim
- SS Vogt
- ST Megeath
- T Chlebowski
- T Hippel von
- T Maschberger
- T Maschberger
- T Maschberger
- T Onishi
- T Peters
- T Peters
- T Preibisch
- T Tsujimoto
- TE Lutz
- TJ Henry
- TV Veltchev
- U Löckmann
- V Bromm
- V Joergens
- V Weidemann
- VV Gvaramadze
- VV Gvaramadze
- W Jao
- W-H Hsu
- WJ Wit de
- WJ Wit de
- X Delfosse
- X Delfosse
- Y Li
- Z-Y Li
- Å Nordlund
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 04/11/2012
- Field of study
The current knowledge on the stellar IMF is documented. It appears to become
top-heavy when the star-formation rate density surpasses about 0.1Msun/(yr
pc^3) on a pc scale and it may become increasingly bottom-heavy with increasing
metallicity and in increasingly massive early-type galaxies. It declines quite
steeply below about 0.07Msun with brown dwarfs (BDs) and very low mass stars
having their own IMF. The most massive star of mass mmax formed in an embedded
cluster with stellar mass Mecl correlates strongly with Mecl being a result of
gravitation-driven but resource-limited growth and fragmentation induced
starvation. There is no convincing evidence whatsoever that massive stars do
form in isolation. Various methods of discretising a stellar population are
introduced: optimal sampling leads to a mass distribution that perfectly
represents the exact form of the desired IMF and the mmax-to-Mecl relation,
while random sampling results in statistical variations of the shape of the
IMF. The observed mmax-to-Mecl correlation and the small spread of IMF
power-law indices together suggest that optimally sampling the IMF may be the
more realistic description of star formation than random sampling from a
universal IMF with a constant upper mass limit. Composite populations on galaxy
scales, which are formed from many pc scale star formation events, need to be
described by the integrated galactic IMF. This IGIMF varies systematically from
top-light to top-heavy in dependence of galaxy type and star formation rate,
with dramatic implications for theories of galaxy formation and evolution.Comment: 167 pages, 37 figures, 3 tables, published in Stellar Systems and
Galactic Structure, Vol.5, Springer. This revised version is consistent with
the published version and includes additional references and minor additions
to the text as well as a recomputed Table 1. ISBN 978-90-481-8817-
Measurement of D-s(+) and D-s(*+) production in B meson decays and from continuum e(+)e(-) annihilation at √s=10.6 GeV
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Andress JC
- Angelini C
- Anjomshoaa A
- Anthony PL
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- Azzopardi DE
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baird K
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Benayoun M
- Berger N
- Beringer J
- Bernard D
- Bernet R
- Best D
- Bettarini S
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom E
- Bloom P
- Blouw J
- Bona M
- Bondioli M
- Bonneaud GR
- Borean C
- Borgland AW
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandt T
- Brau B
- Brau J
- Breon AB
- Briand H
- Bright-Thomas PG
- Brigljevic V
- Brochard F
- Brose J
- Brown CM
- Brown D
- Brown DN
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Bulos F
- Burchat PR
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Cahn RN
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Carroll M
- Cartaro C
- Cavallo N
- Cavoto G
- Chao M
- Charles E
- Chauveau J
- Chen E
- Chen GP
- Chen JC
- Cheng CH
- Chevalier N
- Christ S
- Chun S
- Clark AR
- Clark PJ
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colberg T
- Colecchia F
- Contri R
- Convery MR
- Copty N
- Cottingham WN
- Coupal DP
- Cowan G
- Cowan R
- Coward DH
- Crawley HB
- Cremaldi L
- Crosetti G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dasu S
- Dauncey PD
- David P
- Davis CL
- De Groot N
- de la Vaissiere C
- de Lesquen A
- de Monchenault GH
- De Nardo G
- de Sangro R
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- Devmal S
- Di Lodovico F
- Dickopp M
- Dima MO
- Dittongo S
- Dixon P
- Dorfan DE
- Dorfan J
- Dorigo A
- Dubitzky RS
- Dubois-Felsmann GP
- Dunwoodie W
- Dvoretskii A
- Dyce N
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Eschenburg V
- Eschrich I
- Fabozzi F
- Faccini R
- Fahey S
- Falbo M
- Falciai D
- Farbin A
- Ferrag S
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fischer PA
- Flood K
- Ford WT
- Forti AC
- Forti F
- Foster B
- Franek B
- Frank ED
- Frey R
- Fry JR
- Fullwood J
- Gabathuler E
- Gabriel TA
- Gaidot A
- Gaillard JM
- Galeazzi F
- Gamba D
- Gamet R
- Ganzhur SF
- Gatto C
- Geddes NI
- Geld TL
- George M
- George S
- Gill MS
- Giorgi MA
- Giraud PF
- Gladney L
- Glanzman T
- Godfrey GL
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy S
- Green MG
- Grillo AA
- Gritsan AV
- Grosdidier G
- Grosso P
- Grothe M
- Groysman Y
- Gunawardane NJW
- Guo QH
- Haas T
- Haire M
- Hamilton R
- Hamon O
- Handler T
- Harrison PF
- Harrison TJ
- Hart PA
- Harton JL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Henderson R
- Hertzbach SS
- Heusch CA
- Hicheur A
- Himel T
- Hitlin DG
- Hocker A
- Hryn'ova T
- Hu H
- Huffer ME
- Innes WR
- Ivanchenko VN
- Iwasaki M
- Izen JM
- Jackson F
- Jackson PD
- Jacobsen RG
- Jawahery A
- Jayatilleke S
- Jessop C
- Johnson DR
- Johnson JR
- Johnson RP
- Jolly S
- Judd D
- Kadel RW
- Kadyk J
- Karyotakis Y
- Kay M
- Kelsey MH
- Kerth LT
- Khan A
- Kim P
- Kirkby D
- Kitayama I
- Knowles DJ
- Koch H
- Kocian ML
- Kofler R
- Kolomensky YG
- Koptchev VG
- Kordich TMB
- Korol AA
- Kowalewski R
- Kozanecki W
- Kral JF
- Kravchenko EA
- Krishnamurthy M
- Kroeger R
- Kunze M
- Kurup A
- Kuznetsova N
- Lacker HM
- Lafferty GD
- Lamanna E
- Lamsa J
- Lanceri L
- Lange D
- Langenegger U
- Langer M
- Lankford AJ
- Laplace S
- Lavin D
- Le Diberder F
- LeClerc C
- Lees JP
- Leith DWGS
- Leonardi E
- Lepeltier V
- Leruste P
- Levi ME
- Levy SL
- Lewandowski B
- Lillard V
- Lista L
- Liu R
- Lo Vetere M
- Lockman WS
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu A
- Lu C
- Luitz S
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Mackay C
- Macri M
- Mallik U
- Maly E
- Mancinelli G
- Mandelkern M
- Manfredi PF
- Margoni M
- Marker CE
- Marsiske H
- Martin JP
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazzoni MA
- McDonald KT
- McGrath P
- McKemey AK
- McKenna JA
- McMahon S
- McMahon TR
- Meadows BT
- Menke S
- Messner R
- Metzler S
- Meyer TI
- Meyer WT
- Michelon G
- Miftakov V
- Milek M
- Moffeit KC
- Monge MR
- Moore TB
- Morandin M
- Morganti M
- Morganti S
- Morii M
- Mount R
- Mugge M
- Muheim F
- Muller DR
- Muller-Pfefferkorn R
- Nash JA
- Nauenberg U
- Neal H
- Neri N
- Nicholson H
- Nief JY
- O'Grady CP
- O'Neale SW
- Ocariz J
- Oddone PJ
- Olivas A
- Olsen J
- Onuchin AP
- Otto S
- Oyang J
- Ozcan VE
- Paick K
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Passaggio S
- Pastore FC
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Penny RC
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petrak S
- Pia MG
- Piccolo D
- Piccolo M
- Piemontese L
- Piredda G
- Plaszczynski S
- Playfer S
- Pompili A
- Poropat P
- Porter FC
- Posocco M
- Potter RJL
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Quinn H
- Rahatlou S
- Rama M
- Rankin P
- Ratcliff BN
- Raven G
- Re V
- Reidy J
- Ricciardi S
- Richman JD
- Rizzo G
- Roat C
- Robbe P
- Roberts DA
- Robertson SH
- Robutti E
- Rochester LS
- Roe NA
- Romosan A
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roussot E
- Roy J
- Ryd A
- Sadrozinski H
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Sanders P
- Sandrelli F
- Santroni A
- Savvas N
- Schaffner SF
- Schalk T
- Schieck JR
- Schietinger T
- Schindler RH
- Schmitz RE
- Schmuecker H
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Sciacca C
- Sciolla G
- Scott I
- Scott IJ
- Seiden A
- Seitz R
- Sekula SJ
- Sen S
- Serbo VV
- Serednyakov SI
- Serfass B
- Serra M
- Sharma V
- Shelkov VG
- Shorthouse HW
- Simi G
- Simonetto F
- Simopoulos ET
- Sinev NB
- Singh H
- Skovpen YI
- Sloane RJ
- Smith AJS
- Smith D
- Smith JG
- Smol A
- Snyder A
- Soffer A
- Soha A
- Sokoloff MD
- Spaan B
- Spanier SM
- Speziali V
- Staengle H
- Stark J
- Steinke M
- Stelzer J
- Stoker DP
- Stroili R
- Strom D
- Strother P
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sutton CS
- Swain JE
- T'Jampens S
- Tanaka HA
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Telnov VI
- Thiebaux C
- Thiessen D
- Tinslay J
- Tisserand V
- Toki WH
- Torassa E
- Tosi S
- Touramanis C
- Treadwell E
- Triggiani G
- Trincaz-Duvoid S
- Tumanov A
- Turnbull L
- Turri M
- Va'vra J
- Vaitsas G
- van Bibber K
- van Hoek WC
- Varnes EW
- Vasileiadis G
- Vasseur G
- Verderi M
- Verkerke W
- Versille S
- Vidal PB
- Voci C
- Voena C
- von Wimmersperg-Toeller JH
- Vuagnin G
- Wagner DL
- Wagner SR
- Wagoner DE
- Waldi R
- Walkowiak W
- Wallom D
- Walsh J
- Wang P
- Watson AT
- Watson NK
- Weatherall JH
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams MI
- Willocq S
- Wilson FF
- Wilson MG
- Wilson RJ
- Wisniewski WJ
- Witherell M
- Wormser G
- Wright DH
- Wright DM
- Wu SL
- Xella SM
- Xie Y
- Yamamoto RK
- Yang S
- Yeche C
- Yellin S
- Young CC
- Yu Z
- Yumiceva FX
- Yushkov AN
- Zacek V
- Zallo A
- Zhang J
- Zhu RY
- Zhu YS
- Zito M
- Publication venue
- American Physical Society
- Publication date
- 01/01/2002
- Field of study
This is the pre-print version of the Article. The official published version can be accessed from the links below. Copyright @ 2002 APSNew measurements of Ds+ and Ds*+ meson production rates from B decays and from qq̅ continuum events near the Υ(4S) resonance are presented. Using 20.8 fb-1 of data on the Υ(4S) resonance and 2.6 fb-1 off-resonance, we find the inclusive branching fractions B(B⃗Ds+X)=(10.93±0.19±0.58±2.73)% and B(B⃗Ds*+X)=(7.9±0.8±0.7±2.0)%, where the first error is statistical, the second is systematic, and the third is due to the Ds+→φπ+ branching fraction uncertainty. The production cross sections σ(e+e-→Ds+X)×B(Ds+→φπ+)=7.55±0.20±0.34pb and σ(e+e-→Ds*±X)×B(Ds+→φπ+)=5.8±0.7±0.5pb are measured at center-of-mass energies about 40 MeV below the Υ(4S) mass. The branching fractions ΣB(B⃗Ds(*)+D(*))=(5.07±0.14±0.30±1.27)% and ΣB(B⃗Ds*+D(*))=(4.1±0.2±0.4±1.0)% are determined from the Ds(*)+ momentum spectra. The mass difference m(Ds+)-m(D+)=98.4±0.1±0.3MeV/c2 is also measured.This work was supported by DOE and NSF (USA), NSERC (Canada), IHEP (China), CEA and CNRS-IN2P3 (France), BMBF (Germany), INFN (Italy), NFR (Norway), MIST (Russia), and PPARC (United Kingdom). Individuals have received support from the Swiss NSF, A. P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
Study of Bc+ decays to the K+K−π+ final state and evidence for the decay Bc+→χc0π+
- Author
- Aaij R
- Adeva B
- Adinolfi M
- Ajaltouni Z
- Akar S
- Albrecht J
- Alessio F
- Alexander M
- Ali S
- Alkhazov G
- Altarelli M Pepe
- Amato S
- Amerio S
- Amhis Y
- An L
- Anderlini L
- Andreassi G
- Andreotti M
- Andrews JE
- Appleby RB
- Archilli F
- Artamonov A
- Artuso M
- Aslanides E
- Auriemma G
- Baalouch M
- Babuschkin I
- Bachmann S
- Back JJ
- Badalov A
- Baesso C
- Baldini W
- Barlow RJ
- Barschel C
- Barsuk S
- Barter W
- Baszczyk M
- Batozskaya V
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- Wark HM
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- Websdale D
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- Wimberley J
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- Wislicki W
- Witek M
- Wormser G
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- Wyllie K
- Xie Y
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- Yin H
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- Yushchenko O
- Zangoli M
- Zarebski KA
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- Zhokhov A
- Zhu X
- Zhukov V
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2016
- Field of study
A study of Bc+→K+K−π+ decays is performed for the first time
using data corresponding to an integrated luminosity of 3.0 fb−1
collected by the LHCb experiment in pp collisions at centre-of-mass energies
of 7 and 8 TeV. Evidence for the decay Bc+→χc0(→K+K−)π+
is reported with a significance of 4.0 standard deviations, resulting in the
measurement of
σ(B+)σ(Bc+)×B(Bc+→χc0π+) to
be (9.8−3.0+3.4(stat)±0.8(syst))×10−6.
Here B denotes a branching fraction while σ(Bc+) and
σ(B+) are the production cross-sections for Bc+ and B+ mesons.
An indication of bˉc weak annihilation is found for the region
m(K−π+)<1.834GeV/c2, with a significance of
2.4 standard deviations.Comment: All figures and tables, along with any supplementary material and
additional information, are available at
https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2016-022.html,
link to supplemental material inserted in the reference
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
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- Abhayasinghe DK
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- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
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- Abdallah J
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- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- 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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Abolins M
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- Wells PS
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- Wendler S
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- Wenglers T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Weydert C
- Whalen K
- Wheeler-Ellis SJ
- Whitaker SP
- White A
- White MJ
- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicek F
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielersis M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
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- Wildt MA
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- Wilkens HG
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- Wingerter-Seez I
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- Wolter MW
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- Wooden G
- Wosiek BK
- Wotschack J
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- Wu SL
- Wu X
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- Wulf E
- Wunstorf R
- Wynne BM
- Xaplanteris L
- Xella S
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- Xu C
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- Xu G
- Yabsley B
- Yacoobb S
- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
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- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
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