1,386 research outputs found
Ratio of the Isolated Photon Cross Sections at \sqrt{s} = 630 and 1800 GeV
- Author
- Abazov VM
- Abbott B
- Abdesselam A
- Abolins M
- Abramov V
- Acharya BS
- Adams DL
- Adams M
- Ahmed SN
- Alexeev GD
- Alton A
- Alves GA
- Amos N
- Anderson EW
- Arnoud Y
- Avila C
- Baarmand MM
- Babintsev VV
- Babukhadia L
- Bacon TC
- Baden A
- Baldin B
- Balm PW
- Banerjee S
- Barberis E
- Baringer P
- Barreto J
- Bartlett JF
- Bassler U
- Bauer D
- Bean A
- Beaudette F
- Begel M
- Belyaev A
- Beri SB
- Bernardi G
- Bertram I
- Besson A
- Beuselinck R
- Bezzubov VA
- Bhat PC
- Bhatnagar V
- Bhattacharjee M
- Blazey G
- Blekman F
- Blessing S
- Boehnlein A
- Bojko NI
- Borcherding F
- Bos K
- Bose T
- Brandt A
- Breedon R
- Briskin G
- Brock R
- Brooijmans G
- Bross A
- Buchholz D
- Buehler M
- Buescher V
- Burtovoi VS
- Butler JM
- Canelli F
- Carvalho W
- Casey D
- Casilum Z
- Castilla-Valdez H
- Chakraborty D
- Chan KM
- Chekulaev SV
- Cho DK
- Choi S
- Chopra S
- Christenson JH
- Chung M
- Claes D
- Clark AR
- Cochran J
- Collaboration D
- Coney L
- Connolly B
- Cooper WE
- Coppage D
- Crepe-Renaudin S
- Cummings MAC
- Cutts D
- da Motta H
- Davis GA
- Davis K
- de Jong SJ
- De K
- Del Signore K
- Demarteau M
- Demina R
- Demine P
- Denisov D
- Denisov SP
- Desai S
- Diehl HT
- Diesburg M
- Doulas S
- Ducros Y
- Dudko LV
- Duensing S
- Duflot L
- Dugad SR
- Duperrin A
- Dyshkant A
- Edmunds D
- Ellison J
- Elvira VD
- Engelmann R
- Eno S
- Eppley G
- Ermolov P
- Eroshin OV
- Estrada J
- Evans H
- Evdokimov VN
- Fahland T
- Feher S
- Fein D
- Ferbel T
- Filthaut F
- Fisk HE
- Fisyak Y
- Flattum E
- Fleuret F
- Fortner M
- Fox H
- Frame KC
- Fu S
- Fuess S
- Gallas E
- Galyaev AN
- Gao M
- Gavrilov V
- Genik RJ
- Genser K
- Gerber CE
- Gershtein Y
- Gilmartin R
- Ginther G
- Gomez B
- Gomez G
- Goncharov PI
- Gordon H
- Goss LT
- Gounder K
- Goussiou A
- Graf N
- Graham G
- Grannis PD
- Green JA
- Greenlee H
- Greenwood ZD
- Grinstein S
- Groer L
- Grunendahl S
- Gupta A
- Gurzhiev SN
- Gutierrez G
- Gutierrez P
- Hadley NJ
- Haggerty H
- Hagopian S
- Hagopian V
- Hall RE
- Hanlet P
- Hansen S
- Hauptman JM
- Hays C
- Hebert C
- Hedin D
- Heinmiller JM
- Heinson AP
- Heintz U
- Heuring T
- Hildreth MD
- Hirosky R
- Hobbs JD
- Hoeneisen B
- Huang Y
- Illingworth R
- Ito AS
- Jaffre M
- Jain S
- Jesik R
- Johns K
- Johnson M
- Jonckheere A
- Jostlein H
- Juste A
- Kahl W
- Kahn S
- Kajfasz E
- Kalinin AM
- Karmanov D
- Karmgard D
- Kehoe R
- Khanov A
- Kharchilava A
- Kim SK
- Klima B
- Knuteson B
- Ko W
- Kohli JM
- Kostritskiy AV
- Kotcher J
- Kothari B
- Kotwal AV
- Kozelov AV
- Kozlovsky EA
- Krane J
- Krishnaswamy MR
- Krivkova P
- Krzywdzinski S
- Kubantsev M
- Kuleshov S
- Kulik Y
- Kunori S
- Kupco A
- Kuznetsov VE
- Landsberg G
- Lee SM
- Leflat A
- Leggett C
- Lehner F
- Li J
- Li QZ
- Li X
- Lima JGR
- Lincoln D
- Linn SL
- Linnemann J
- Lipton R
- Lucotte A
- Lueking L
- Lundstedt C
- Luo C
- Maciel AKA
- Madaras RJ
- Malyshev VL
- Manankov V
- Mao HS
- Marshall T
- Martin MI
- Mauritz KM
- May B
- Mayorov AA
- McCarthy R
- McMahon T
- Melanson HL
- Merkin M
- Merritt KW
- Miao C
- Miettinen H
- Mihalcea D
- Mishra CS
- Mokhov N
- Mondal NK
- Montgomery HE
- Moore RW
- Mostafa M
- Nagy E
- Nang F
- Narain M
- Narasimham VS
- Naumann NA
- Neal HA
- Negret JR
- Negroni S
- Nunnemann T
- O'Neil D
- Oguri V
- Olivier B
- Oshima N
- Padley P
- Pan LJ
- Papageorgiou K
- Para A
- Parashar N
- Partridge R
- Parua N
- Paterno M
- Patwa A
- Pawlik B
- Perkins J
- Peters O
- Petroff P
- Piegaia R
- Pope BG
- Popkov E
- Prosper HB
- Protopopescu S
- Przybycien MB
- Qian J
- Raja R
- Rajagopalan S
- Ramberg E
- Rapidis PA
- Reay NW
- Reucroft S
- Ridel M
- Rijssenbeek M
- Rizatdinova F
- Rockwell T
- Roco M
- Royon C
- Rubinov R
- Ruchti R
- Rutherfoord J
- Sabirov BM
- Sajot G
- Santoro A
- Sawyer L
- Schamberger RD
- Schellman H
- Schwartzman A
- Sen N
- Shabalina E
- Shivpuri RK
- Shpakov D
- Shupe M
- Sidwell RA
- Simak V
- Singh H
- Singh JB
- Sirotenko V
- Slattery P
- Smith E
- Smith RP
- Snihur R
- Snow GR
- Snow J
- Snyder S
- Solis JLG
- Solomon J
- Song Y
- Sorin V
- Sosebee M
- Sotnikova N
- Soustruznik K
- Souza M
- Stanton NR
- Steinbruck G
- Stephens RW
- Stichelbaut F
- Stoker D
- Stolin V
- Stone A
- Stoyanova DA
- Strang MA
- Strauss M
- Strovink M
- Stutte L
- Sznajder A
- Talby M
- Taylor W
- Tentindo-Repond S
- Tripathi SM
- Trippe TG
- Turcot AS
- Tuts PM
- Van Kooten R
- Vaniev V
- Varelas N
- Vertogradov LS
- Villeneuve-Seguier F
- Volkov AA
- Vorobiev AP
- Wahl HD
- Wang H
- Wang ZM
- Warchol J
- Watts G
- Wayne M
- Weerts H
- White A
- White JT
- Whiteson D
- Wightman JA
- Wijngaarden DA
- Willis S
- Wimpenny SJ
- Womersley J
- Wood DR
- Xu Q
- Yamada R
- Yamin R
- Yasuda T
- Yatsunenko YA
- Yip K
- Youssef S
- Yu J
- Yu Z
- Zanabria M
- Zhang X
- Zheng H
- Zhou B
- Zhou Z
- Zielinski M
- Zieminska D
- Zieminski A
- Zutshi V
- Zverev EG
- Zylberstejn A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2001
- Field of study
The inclusive cross section for production of isolated photons has been
measured in \pbarp collisions at s=630 GeV with the \D0 detector at
the Fermilab Tevatron Collider. The photons span a transverse energy (ET)
range from 7-49 GeV and have pseudorapidity ∣η∣<2.5. This measurement is
combined with to previous \D0 result at s=1800 GeV to form a ratio
of the cross sections. Comparison of next-to-leading order QCD with the
measured cross section at 630 GeV and ratio of cross sections show satisfactory
agreement in most of the ET range.Comment: 7 pages. Published in Phys. Rev. Lett. 87, 251805, (2001
Search for Dark Matter Annihilation in the Galactic Center with IceCube-79
- Author
- A Burkert
- A Gazizov
- A. Bernhard
- A. Christov
- A. Fedynitch
- A. Goldschmidt
- A. Groß
- A. H. Cruz Silva
- A. Haj Ismail
- A. Hallgren
- A. Homeier
- A. Ishihara
- A. Kappes
- A. Karle
- A. Keivani
- A. Kheirandish
- A. Koob
- A. M. Brown
- A. Meli
- A. Obertacke
- A. Olivas
- A. Omairat
- A. O’Murchadha
- A. R. Fazely
- A. Sandrock
- A. Schukraft
- A. Schönwald
- A. Stasik
- A. Stößl
- A. Terliuk
- B. Christy
- B. Eberhardt
- B. Eichmann
- B. Hansmann
- B. J. Whelan
- B. Kaminsky
- B. Riedel
- B. Ruzybayev
- C. Arguelles
- C. Bohm
- C. De Clercq
- C. Finley
- C. H. Wiebusch
- C. Ha
- C. Haack
- C. Kopper
- C. Pfendner
- C. Pérez de los Heros
- C. Rott
- C. Spiering
- C. Walck
- C. Wendt
- C. Wichary
- Ch. Weaver
- D Clowe
- D Hooper
- D. Altmann
- D. Berley
- D. Bindig
- D. Bose
- D. Chirkin
- D. F. Cowen
- D. Gier
- D. Grant
- D. Góra
- D. Hebecker
- D. Heereman
- D. Hellwig
- D. J. Boersma
- D. J. Koskinen
- D. L. Xu
- D. Pieloth
- D. R. Nygren
- D. R. Williams
- D. Ryckbosch
- D. Seckel
- D. Soldin
- D. Tosi
- D. Z. Besson
- E. A. Strahler
- E. Beiser
- E. Bernardini
- E. Blaufuss
- E. Cheung
- E. Jacobi
- E. Middell
- E. Middlemas
- E. Pinat
- E. Resconi
- E. Unger
- F Nesti
- F Zwicky
- F. Bos
- F. Halzen
- F. Huang
- F. McNally
- F. Scheriau
- G Bertone
- G Jungman
- G Steigman
- G. Binder
- G. C. Hill
- G. de Wasseige
- G. Golup
- G. Kohnen
- G. Kroll
- G. M. Spiczak
- G. Maggi
- G. Merino
- G. S. Japaridze
- G. T. Przybylski
- G. Tešić
- G. W. Sullivan
- G. Yodh
- GJ Feldman
- H Yuksel
- H Zhao
- H. -G. Sander
- H. -P. Bretz
- H. Dembinski
- H. Kolanoski
- H. Niederhausen
- H. S. Matis
- H. Taavola
- H. Wissing
- I. Taboada
- J Ellis
- J. A. Aguilar
- J. A. Pepper
- J. Adams
- J. Auffenberg
- J. Becker Tjus
- J. Blumenthal
- J. Braun
- J. C. Davis
- J. C. Díaz-Vélez
- J. C. Groh
- J. Casey
- J. Daughhetee
- J. Feintzeig
- J. Felde
- J. G. Gonzalez
- J. Gallagher
- J. Hignight
- J. J. Beatty
- J. Kemp
- J. Kiryluk
- J. Kläs
- J. Kunnen
- J. L. Kelley
- J. L. Lanfranchi
- J. Leuner
- J. Lünemann
- J. Madsen
- J. Miller
- J. P. A. M. de André
- J. P. Dumm
- J. P. Yanez
- J. Posselt
- J. Pütz
- J. Sandroos
- J. Vandenbroucke
- J. van Santen
- J. Veenkamp
- JF Beacom
- JF Navarro
- K Griest
- K Hanson
- K. -H. Becker
- K. Abraham
- K. B. M. Mahn
- K. Clark
- K. D. de Vries
- K. D. Hoffman
- K. Filimonov
- K. Ghorbani
- K. Hanson
- K. Helbing
- K. Holzapfel
- K. Hoshina
- K. Hultqvist
- K. Jero
- K. Krings
- K. Mase
- K. Meagher
- K. Rawlins
- K. Schatto
- K. Wiebe
- K. Woschnagg
- KM Górski
- L Bergström
- L. Brayeur
- L. Classen
- L. Gerhardt
- L. Gladstone
- L. Köpke
- L. Mohrmann
- L. Paul
- L. Rädel
- L. Sabbatini
- L. Schulte
- L. Wille
- M Boylan-Kolchin
- M Ricotti
- M. Ackermann
- M. Ahlers
- M. Ahrens
- M. Archinger
- M. Bissok
- M. Börner
- M. Casier
- M. Day
- M. de With
- M. Dunkman
- M. G. Aartsen
- M. Glagla
- M. Huber
- M. J. Larson
- M. Jurkovic
- M. Kauer
- M. Kowalski
- M. Kroll
- M. Labare
- M. Lesiak-Bzdak
- M. Leuermann
- M. Medici
- M. N. Tobin
- M. Quinnan
- M. Rameez
- M. Relich
- M. Richman
- M. Rongen
- M. Schimp
- M. Schmitz
- M. Stahlberg
- M. Stamatikos
- M. Sutherland
- M. Tselengidou
- M. Usner
- M. Vehring
- M. Voge
- M. Vraeghe
- M. W. E. Smith
- M. Wallraff
- M. Wolf
- M. Zoll
- MS Roberts
- N. A. Stanisha
- N. Buzinsky
- N. Kurahashi
- N. L. Strotjohann
- N. van Eijndhoven
- N. Wandkowsky
- N. Whitehorn
- O. Botner
- O. Fadiran
- P Meade
- P. A. Evenson
- P. A. Toale
- P. B. Price
- P. Berghaus
- P. Desiati
- P. Gretskov
- P. O. Hulth
- P. Redl
- P. Zarzhitsky
- R. Bay
- R. Eagan
- R. G. Stokstad
- R. Gaior
- R. Hellauer
- R. Hoffmann
- R. Konietz
- R. Maruyama
- R. Maunu
- R. Morse
- R. Nahnhauer
- R. Reimann
- R. Shanidze
- R. Ström
- RG Carlberg
- S. BenZvi
- S. Böser
- S. C. Nowicki
- S. Coenders
- S. De Ridder
- S. Euler
- S. Fahey
- S. Flis
- S. Hickford
- S. In
- S. Kopper
- S. M. Saba
- S. Miarecki
- S. R. Klein
- S. Richter
- S. Robertson
- S. Sarkar
- S. Schoenen
- S. Schöneberg
- S. Seunarine
- S. Ter-Antonyan
- S. Tilav
- S. Vallecorsa
- S. Vanheule
- S. W. Barwick
- S. Westerhoff
- S. Yoshida
- T Gaisser
- T Sjöstrand
- T. Anderson
- T. C. Arlen
- T. DeYoung
- T. Ehrhardt
- T. Fischer-Wasels
- T. Fuchs
- T. Glüsenkamp
- T. K. Gaisser
- T. Karg
- T. Kuwabara
- T. Menne
- T. Meures
- T. Montaruli
- T. Palczewski
- T. R. Wood
- T. Ruhe
- T. Schmidt
- T. Stanev
- T. Stezelberger
- U. Naumann
- V Barger
- V Springel
- V. Baum
- W Blok de
- W Tucker
- W. Huelsnitz
- W. Rhode
- WH Press
- X. Bai
- X. W. Xu
- Y. Xu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
The Milky Way is expected to be embedded in a halo of dark matter particles,
with the highest density in the central region, and decreasing density with the
halo-centric radius. Dark matter might be indirectly detectable at Earth
through a flux of stable particles generated in dark matter annihilations and
peaked in the direction of the Galactic Center. We present a search for an
excess flux of muon (anti-) neutrinos from dark matter annihilation in the
Galactic Center using the cubic-kilometer-sized IceCube neutrino detector at
the South Pole. There, the Galactic Center is always seen above the horizon.
Thus, new and dedicated veto techniques against atmospheric muons are required
to make the southern hemisphere accessible for IceCube. We used 319.7 live-days
of data from IceCube operating in its 79-string configuration during 2010 and
2011. No neutrino excess was found and the final result is compatible with the
background. We present upper limits on the self-annihilation cross-section,
\left, for WIMP masses ranging from 30 GeV up to
10 TeV, assuming cuspy (NFW) and flat-cored (Burkert) dark matter halo
profiles, reaching down to ≃4⋅10−24 cm3 s−1, and
≃2.6⋅10−23 cm3 s−1 for the νν
channel, respectively.Comment: 14 pages, 9 figures, Submitted to EPJ-C, added references, extended
limit overvie
Utilisation of an operative difficulty grading scale for laparoscopic cholecystectomy
- Author
- Aawsaj Y
- Abayomi M
- Acharya V
- Aggarwal SK
- Ahmad A
- Ahmed I
- Ahmed J
- Ahmed J
- Ahmed T
- Ainley P
- Akhtar M
- Al Amari K
- Al-Abed YA
- Al-Akash M
- Al-Bahrani AZ
- Al-Khyatt W
- Al-Muhktar A
- Al-Sarireh B
- Al-Taan O
- Alagaratnam S
- Alam I
- Alberts J
- Alderson D
- Aldridge RC
- Aleksandrov D
- Ali H
- Ali S
- Amin K
- Andrew DR
- Appleton S
- Arhi C
- Aroori S
- Aryal K
- Asad M
- Aseem R
- Asprou FM
- Awan A
- Ayaani S
- Aymon
- Babu BI
- Bajwa DS
- Bajwa FM
- Baker AL
- Balfe P
- Ball WR
- Ballance L
- Banwell V
- Barnes J
- Barrie J
- Bartlett F
- Basheer M
- Bashir G
- Basra M
- Basu S
- Basynat P
- Batt J
- Bausbacher H
- Bawa S
- Beasley WD
- Belding R
- Bellini MI
- Bennett SP
- Bhandari CTS
- Bhattacharya V
- Blane C
- Blazeby JM
- Boal M
- Boddy A
- Boland M
- Bond-Smith G
- Booth MI
- Borowski DW
- Bowen L
- Boyce KM
- Boyd AT
- Bradley D
- Bradley N
- Brennan S
- Brett D
- Broadhurst J
- Brooke E
- Brown TH
- Bryant A
- Buchan J
- Bullen N
- Bunnell C
- Bunting DM
- Burke P
- Byrne JP
- Byrnes CK
- Campbell W
- Carney K
- Carney K
- Carroll P
- Carter CR
- Carter NC
- Carty N
- Cassidy JT
- Chambers A
- Chambers A
- Chambers A
- Chan WM
- Chang J
- Charalabopoulos A
- Chauhan N
- Cheung M
- Chishti IA
- Chitre V
- CholeS Study Grp
- CholeS Study Grp
- CholeS Study Grp
- CholeS Study Grp
- Choy A
- Cieplucha K
- Clements JM
- Coats M
- Cockbain AJ
- Coe PO
- Connelly M
- Cooke F
- Courtney MJ
- Cowley JB
- Cross KS
- Cuming T
- Cunha P
- D'Costa C
- Dalgaty F
- Dar F
- Date R
- Dave RV
- Davey P
- Davies J
- Dawson S
- De Marchi JA
- de Siqueira J
- Deguara J
- Delisle TG
- Dennison AR
- Derbyshire L
- Devoto L
- Dhillon A
- Diamond T
- Dickson-Lowe R
- Digney R
- Dindyal S
- Dobbins B
- Doe M
- Dorrian E
- Doulias T
- Downing J
- Downing J
- Drake B
- Driscoll PJ
- Duke D
- Durkin D
- Dwerryhouse SJ
- Ebdewi H
- Ebied H
- Eisawi A
- El-Dhuwaib APY
- El-Hasani SS
- Elkheir N
- Elmasry M
- Elsayed M
- Elshaer M
- Emesih S
- Farag SF
- Farooq A
- Farouk M
- Fasih T
- Fawole AS
- Fenwick S
- Ferguson G
- Ferris P
- Finch D
- Finch JG
- Finch JG
- Finlay I
- Fleming K
- Fletcher T
- Fordham IJ
- Forouzanfar A
- Forrest CR
- Forster L
- Fothergill L
- Frame RJ
- Francombe J
- Frank L
- Fusai G
- Galanopoulos G
- Gallagher PV
- Garcea G
- Gardner-Thorpe J
- Geoghegan JG
- Geogloma I
- Gerakopoulos S
- Ghareeb E
- Ghazanfar MA
- Gibson S
- Giles M
- Giovinazzo F
- Giwa L
- Goh YL
- Gopalswamy S
- Goscimski A
- Gossage JA
- Gough M
- Gould L
- Gould L
- Grant AJ
- Gravante G
- Griffiths EA
- Griffiths EA
- Gull S
- Gunasekera RT
- Gurung K
- Guthrie GJK
- Hafiz S
- Halkias C
- Hall C
- Hamady Z
- Hamdan A
- Hamdan MF
- Hamilton E
- Hancorn K
- Haque M
- Haque SU
- Hardy TJ
- Hargreaves A
- Harilingam ACM
- Harris A
- Harrison E
- Hawkins H
- Heath J
- Hebbar M
- Henderson LT
- Henley N
- Heshaishi M
- Hewes J
- Hewes JC
- Heywood N
- Higgs SM
- Hill ADK
- Hill ADK
- Hindley C
- Hirst NA
- Hisham E
- Ho W-M
- Hoban JR
- Hodgkins KA
- Hodson J
- Holroyd DJ
- Hooks G
- Hopwood B
- Hornby ST
- Hornsby J
- Hosie KB
- Hosie KB
- Hossack MR
- Hossain T
- Hoti E
- Hou D
- Hrycaiczuk A
- Hughes M
- Hunter DI
- Hussain A
- Hussain A
- Hussain AA
- Hussain N
- Iftikhar SY
- Iqbal N
- Iskandar E
- Issa E
- Ivanovski I
- Jackson A
- Jackson C
- Jafferbhoy SF
- Jambulingam P
- Jamdar S
- Jamel S
- Janeczko A
- Jaunoo S
- Jayanthi NVG
- Jelley C
- Jennings NA
- Joel A
- Johnpulle MA
- Johnston D
- Johnstone M
- Johnstone M
- Joji N
- Jones C
- Jones E
- Jones GH
- Jones MA
- Jones MJ
- Jones RP
- Jones SM
- Kadhim A
- Kadirkamanathan S
- Kallaway C
- Kanakala V
- Kanavati O
- Kansal N
- Kaptanis S
- Karavadra B
- Karim L
- Karunakaran P
- Katbeh T
- Kaur P
- Kausar A
- Kelly ME
- Kendal C
- Kennedy D
- Kenny R
- Keogh K
- Khalil AM
- Khan A
- Khan MA
- Khan MAS
- Khan RB
- Khan S
- Khan S
- Khawaja A
- Khawaja Z
- Khogali E
- Kimble A
- Kinghorn A
- Kirkham AJ
- Knight B
- Knight K
- Kourkulos M
- Krysztopik R
- Kumar P
- Kynaston J
- Kyriakidis D
- Lalla K
- Lambert J
- Lammy S
- Lane R
- Larkin D
- Law J
- Lawther R
- Lazim T
- Lee K
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- Zeeshan S
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- Zino S
- Ziprin P
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
Background
A reliable system for grading operative difficulty of laparoscopic cholecystectomy would standardise description of findings and reporting of outcomes. The aim of this study was to validate a difficulty grading system (Nassar scale), testing its applicability and consistency in two large prospective datasets.
Methods
Patient and disease-related variables and 30-day outcomes were identified in two prospective cholecystectomy databases: the multi-centre prospective cohort of 8820 patients from the recent CholeS Study and the single-surgeon series containing 4089 patients. Operative data and patient outcomes were correlated with Nassar operative difficultly scale, using Kendall’s tau for dichotomous variables, or Jonckheere–Terpstra tests for continuous variables. A ROC curve analysis was performed, to quantify the predictive accuracy of the scale for each outcome, with continuous outcomes dichotomised, prior to analysis.
Results
A higher operative difficulty grade was consistently associated with worse outcomes for the patients in both the reference and CholeS cohorts. The median length of stay increased from 0 to 4 days, and the 30-day complication rate from 7.6 to 24.4% as the difficulty grade increased from 1 to 4/5 (both p < 0.001). In the CholeS cohort, a higher difficulty grade was found to be most strongly associated with conversion to open and 30-day mortality (AUROC = 0.903, 0.822, respectively). On multivariable analysis, the Nassar operative difficultly scale was found to be a significant independent predictor of operative duration, conversion to open surgery, 30-day complications and 30-day reintervention (all p < 0.001).
Conclusion
We have shown that an operative difficulty scale can standardise the description of operative findings by multiple grades of surgeons to facilitate audit, training assessment and research. It provides a tool for reporting operative findings, disease severity and technical difficulty and can be utilised in future research to reliably compare outcomes according to case mix and intra-operative difficulty
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Yilmaz M
- Yoosootiniya R
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- Zarzhitsky P
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Zinonos Z
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- Zitoun R
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- 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
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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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
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- 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
- Zhukov V
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- Ziebarth EB
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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
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
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
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- Alonso A
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- Altheimer A
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- Alviggi MG
- Amako K
- Amelung C
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- Anisenkov A
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- ATLAS Collaboration The
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- Backus Mayes J
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- Bailey DC
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- Blair RE
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- Zhemchugov A
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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 inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
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- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
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- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
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
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
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- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
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- Yumiceva F
- Yun JC
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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
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
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- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
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- Addy TN
- Adelman J
- Adomeit S
- Adye T
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- Aguilar-Saavedra JA
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- Ahlen SP
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- Aielli G
- Akesson TP
- Akimoto G
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- Alconada Verzini MJ
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- Aleksandrov IN
- Alexa C
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- Alexandre G
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- Alio L
- Alison J
- Allbrooke BMM
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- Allport PP
- Allwood-Spiers SE
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- Zurzolo G
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Villalba RM
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
- Vishnevskiy D
- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Walker M
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Wan Z
- Wang D
- Wang F
- Wang J
- Wang J
- Wang M
- Wang X
- Wang Z
- Wardle N
- Wasserbaech S
- Wayand S
- Wayne M
- Weber H
- Weber HA
- Weber M
- Weber M
- Weiler T
- Weinberg M
- Wendland L
- Weng Y
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickramage N
- Wilbur S
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winer BL
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Wolfe H
- Wolszczak W
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu L
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yucel M
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zeinali M
- Zeise M
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zheng Y
- Zhokin A
- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- 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
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