564 research outputs found
Development of International Learning Outcomes for Shelter Medicine in Veterinary Education: A Delphi Approach
- Publication venue
- 'University of Toronto Press Inc. (UTPress)'
- Publication date
- 30/09/2020
- Field of study
Shelter medicine is a veterinary discipline of growing importance. Formally accepted as a clinical specialty in the USA in 2014, the practice of shelter medicine worldwide is expanding. As a topic in veterinary pre-registration (undergraduate) education, it is frequently used as an opportunity to teach primary care skills, but increasingly recognized as a subject worthy of teaching in its own right. The aim of this study was to use a Delphi consensus methodology to identify learning outcomes relevant to shelter medicine education.
Shelter medicine educators worldwide in a variety of settings, including universities, non-governmental organisations and shelters were invited to participate. Participants were initially invited to share shelter medicine teaching materials. These were synthesised and formatted into Learning Outcomes (LOs) based on Bloom’s taxonomy and organised into five subject-specific domains.
Participants were then asked to develop and evaluate the identified LOs in two rounds of online surveys. Consensus was determined at >80% of panellists selecting “agree” or “strongly agree” in response to the statement “please indicate whether you would advise that it should be included in a shelter medicine education program” for each LO. In the second survey, where re-wording of accepted LOs was suggested, preference was determined at >50% agreement.
Through this method, 102 agreed LOs have been identified and refined. These LOs, as well as those which did not reach consensus, are presented here. These are intended for use by shelter medicine educators worldwide, to enable and encourage the further development of this important veterinary discipline
Determination of masses of the central black holes in NGC524 and NGC2549 using Laser Guide Star Adaptive Optics
- Author
- Aller
- Bacon
- Bender
- Binney
- Boccas
- Bolton
- Bower
- Cappellari
- Cappellari
- Cappellari
- Cappellari
- Cappellari
- Cappellari
- Cappellari
- Cappellari
- Copin
- Croton
- Davies
- Davies
- Davor Krajnovi��
- de Lorenzi
- de Vaucouleurs
- Di Matteo
- Doeleman
- Dolphin
- Emsellem
- Emsellem
- Emsellem
- Faber
- Falcke
- Ferrarese
- Ferrarese
- Ferrarese
- Ferrarese
- Ferrarese
- Franx
- Freedman
- Gebhardt
- Gebhardt
- Gerhard
- Gerhard
- Ghez
- Ghez
- Gillessen
- Graham
- Graham
- G��ltekin
- G��ltekin
- Hopkins
- Hopkins
- Houghton
- H��ring
- H��ring-Neumayer
- Koopmans
- Kormendy
- Kormendy
- Kormendy
- Krajnovi��
- Krajnovi��
- Krist
- Kuntschner
- Kurucz
- Lauer
- Lawson
- Le Louarn
- Livingston
- Magorrian
- Maiolino
- Makino
- Marconi
- McDermid
- Merritt
- Michele Cappellari
- Mihos
- Milosavljevi��
- Milosavljevi��
- Milosavljevi��
- Monnet
- Neumayer
- Nowak
- Nowak
- Onken
- Press
- Quinlan
- Rest
- Richard M. McDermid
- Richstone
- Rix
- Roger L. Davies
- Rusin
- Rybicki
- Schlegel
- Schwarzschild
- Sch��del
- Shapiro
- Shen
- Silk
- Silva
- Siopis
- Statler
- S��nchez-Bl��zquez
- Thomas
- Tonry
- Vacca
- Valluri
- van de Ven
- van den Bosch
- van den Bosch
- van der Marel
- van der Marel
- Verolme
- Wallace
- Winge
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2009
- Field of study
[abridged] We present observations of NGC524 and NGC2549 with LGS AO obtained
at GEMINI North telescope using the NIFS IFU in the K band. The purpose of
these observations, together with previously obtained observations with the
SAURON IFU, is to determine the masses (Mbh) of the supermassive black holes
(SMBH). The targeted galaxies were chosen to have central light profiles
showing a core (NGC524) and a cusp (NGC2549), to probe the feasibility of using
the galaxy centre as the NGS required for LGS AO. We employ an innovative `open
loop' technique. The data have spatial resolution of 0.23" and 0.17" FWHM,
showing that high quality LGS AO observations of these objects are possible. We
construct axisymmetric three-integral dynamical models which are constrained
with both the NIFS and SAURON data. The best fitting models yield Mbh=(8.3 +2.7
-1.3) x 10^8 Msun for NGC524 and Mbh=(1.4 +0.2 -1.3) x 10^7 Msun for NGC2549
(all errors are at the 3 sigma CL). We demonstrate that the wide-field SAURON
data play a crucial role in the M/L determination increasing the accuracy of
M/L by a factor of at least 5, and constraining the upper limits on Mbh. The
NIFS data are crucial in constraining the lower limits of Mbh and in
combination with the large scale data reducing the uncertainty by a factor of 2
or more. We find that the orbital structure of NGC524 shows significant
tangential anisotropy, while at larger radii both galaxies are consistent with
having almost perfectly oblate velocity ellipsoids. Tangential anisotropy in
NGC524 coincides with the size of SMBH sphere of influence and the core region
in the light profile. We test the accuracy to which Mbh can be measured using
seeings obtained from typical LGS AO observations, and conclude that for a
typical conditions and Mbh the expected uncertainty is of the order of 50%.Comment: 19 pages, 14 figure
Spatial and Temporal Variability of Macroinvertebrates in Spawning and Non-Spawning Habitats during a Salmon Run in Southeast Alaska
- Author
- AA Berryman
- AC Benke
- B McCune
- Björn Brembs
- BL Kerans
- C Gjerløv
- CG Jones
- DP Peterson
- DT Chaloner
- Emily Y. Campbell
- EY Campbell
- FR Hauer
- HBN Hynes
- J Lancaster
- J Rüegg
- JH Winterbottom
- JL Lessard
- JL Lessard
- JN Negishi
- JR Sedell
- JW Moore
- JW Moore
- JW Moore
- KA Monaghan
- Kenneth W. Cummins
- M. Eric Benbow
- MA Palmer
- MJ Oliver
- MS Field-Dodgson
- N Minakawa
- PS Levi
- PS White
- RBD Rosario
- Richard W. Merritt
- RW Merritt
- SD Tiegs
- SD Tiegs
- SG Hildebrand
- SM Gende
- TP Quinn
- VH Resh
- Publication venue
- Public Library of Science
- Publication date
- 20/06/2012
- Field of study
Spawning salmon create patches of disturbance through redd digging which can reduce macroinvertebrate abundance and biomass in spawning habitat. We asked whether displaced invertebrates use non-spawning habitats as refugia in streams. Our study explored how the spatial and temporal distribution of macroinvertebrates changed during a pink salmon (Oncorhynchus gorbuscha) spawning run and compared macroinvertebrates in spawning (riffle) and non-spawning (refugia) habitats in an Alaskan stream. Potential refugia included: pools, stream margins and the hyporheic zone, and we also sampled invertebrate drift. We predicted that macroinvertebrates would decline in riffles and increase in drift and refugia habitats during salmon spawning. We observed a reduction in the density, biomass and taxonomic richness of macroinvertebrates in riffles during spawning. There was no change in pool and margin invertebrate communities, except insect biomass declined in pools during the spawning period. Macroinvertebrate density was greater in the hyporheic zone and macroinvertebrate density and richness increased in the drift during spawning. We observed significant invertebrate declines within spawning habitat; however in non-spawning habitat, there were less pronounced changes in invertebrate density and richness. The results observed may be due to spawning-related disturbances, insect phenology, or other variables. We propose that certain in-stream habitats could be important for the persistence of macroinvertebrates during salmon spawning in a Southeast Alaskan stream
Search for Kaluza-Klein Graviton Emission in ppˉ Collisions at s=1.8 TeV using the Missing Energy Signature
- Author
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Ambrose D
- Amidei D
- Anikeev K
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Badgett W
- Bailey S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Behari S
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berryhill J
- Bhatti A
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bolla G
- Bolshov A
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Brandl A
- Bromberg C
- Brozovic M
- Brubaker E
- Bruner N
- Budagov J
- Budd HS
- Burkett K
- Busetto G
- Byrum KL
- Cabrera S
- Calafiura P
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cecco SD
- Cerri A
- Cerrito L
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Chen C
- Chen YC
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung JY
- Chung WH
- Chung YS
- Ciobanu CI
- Clark AG
- Coca M
- Connolly A
- Convery M
- Conway J
- Cordelli M
- Cranshaw J
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- de Barbaro P
- de Troconiz JF
- de Troconiz JF
- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Demers S
- Demortier L
- Deninno M
- Denis RS
- Derwent PF
- Devlin T
- Dionisi C
- Dittmann JR
- Dominguez A
- Donati S
- Dorigo T
- Eddy N
- Einsweiler K
- Engels E
- Erbacher R
- Errede D
- Errede S
- Eusebi R
- Fan Q
- Farrington S
- Feild RG
- Fernandez JP
- Ferretti C
- Field RD
- Fiori I
- Flaugher B
- Flores-Castillo LR
- Foster GW
- Franklin M
- Freeman J
- Friedman J
- Fukui Y
- Furic I
- Galeotti S
- Gallas A
- Gallinaro M
- Gao T
- Garcia-Sciveres M
- Garfinkel AF
- Gatti P
- Gay C
- Gerdes DW
- Gerstein E
- Giagu S
- Giannetti P
- Giolo K
- Giordani M
- Giromini P
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Goldstein J
- Gomez G
- Goncharov M
- Gorelov I
- Goshaw AT
- Gotra Y
- Goulianos K
- Green C
- Greene MG
- Gresele A
- Grim G
- Grosso-Pilcher C
- Guenther M
- Guillian G
- Haas RM
- Haber C
- Hahn SR
- Halkiadakis E
- Hall C
- Handa T
- Handler R
- Happacher F
- Hara K
- Hardman AD
- Harris RM
- Hartmann F
- Hatakeyama K
- Hauser J
- Heinrich J
- Heiss A
- Hennecke M
- Herndon M
- Hill C
- Hocker A
- Hoffman KD
- Hollebeek R
- Holloway L
- Hou S
- Huffman BT
- Hughes R
- Huston J
- Huth J
- Ikeda H
- Incandela J
- Introzzi G
- Iori M
- Issever C
- Ivanov A
- Iwai J
- Iwata Y
- Iyutin B
- James E
- Jones M
- Joshi U
- Kambara H
- Kamon T
- Kaneko T
- Kang J
- Karr K
- Kartal S
- Kasha H
- Kato Y
- Keaffaber TA
- Kelley K
- Kelly M
- Kennedy RD
- Kephart R
- Khazins D
- Kikuchi T
- Kilminster B
- Kim BJ
- Kim DH
- Kim HS
- Kim MJ
- Kim SB
- Kim SH
- Kim TH
- Kim YK
- Kirby M
- Kirk M
- Kirsch L
- Klimenko S
- Koehn P
- Kondo K
- Konigsberg J
- Korn A
- Korytov A
- Kostritskiy AV
- Kotcher J
- Kotelnikov K
- Kothari B
- Kotwal AV
- Kovacs E
- Kovacs E
- Kozelov AV
- Kozlovsky EA
- Krane J
- Krishnaswamy MR
- Krivkova P
- Kroll J
- Kroll J
- Kruse M
- Kruse M
- Krutelyov V
- Krutelyov V
- Krzywdzinski S
- Kubantsev M
- Kuhlmann SE
- Kuhlmann SE
- Kuleshov S
- Kulik Y
- Kunori S
- Kupco A
- Kurino K
- Kurino K
- Kuwabara T
- Kuwabara T
- Kuznetsov VE
- Kuznetsova N
- Kuznetsova N
- Laasanen AT
- Laasanen AT
- Lai N
- Lai N
- Lami S
- Lami S
- Lammel S
- Lammel S
- Lamoureux JI
- Lancaster J
- Lancaster J
- Lancaster M
- Lancaster M
- Lander R
- Lander R
- Landsberg G
- Lannon K
- Lannon K
- Lath A
- Lath A
- Latino G
- Latino G
- Le Y
- Le Y
- LeCompte T
- LeCompte T
- Lee AM
- Lee J
- Lee J
- Lee K
- Lee SW
- Lee SW
- Lee WM
- Leflat A
- Lehner F
- Leonardo N
- Leonardo N
- Leone S
- Leone S
- Leonidopoulos C
- Lewis JD
- Lewis JD
- Li J
- Li K
- Li K
- Li QZ
- Lima JGR
- Lin CS
- Lin CS
- Lincoln D
- Lindgren M
- Lindgren M
- Linn SL
- Linnemann J
- Lipton R
- Liss TM
- Liss TM
- Litvintsev DO
- Litvintsev DO
- Liu JB
- Liu JB
- Liu T
- Liu T
- Liu YC
- Liu YC
- Lobban O
- Lockyer NS
- Lockyer NS
- Loginov A
- Loginov A
- Loken J
- Loken J
- Loreti M
- Loreti M
- Lucchesi D
- Lucchesi D
- Lueking L
- Lukens P
- Lukens P
- Lundstedt C
- Luo C
- Lusin S
- Lusin S
- Lyons L
- Lyons L
- Lys J
- Lys J
- Maciel AKA
- Madaras RJ
- Madrak R
- Madrak R
- Maeshima K
- Maeshima K
- Maksimovic P
- Maksimovic P
- Malferrari L
- Malferrari L
- Malyshev VL
- Manankov V
- Manca G
- Manca G
- Mangano M
- Mangano M
- Mao HS
- Mariotti M
- Mariotti M
- Marshall T
- Martignon G
- Martignon G
- Martin A
- Martin A
- Martin M
- Martin M
- Martin MI
- Martin V
- Martin V
- Martinez M
- Martinez M
- Matthews JAJ
- Matthews JAJ
- Mattingly SEK
- Mayer J
- Mayorov AA
- Mazzanti P
- Mazzanti P
- McCarthy R
- McFarland KS
- McFarland KS
- McIntyre P
- McIntyre P
- McKigney E
- McMahon T
- Melanson HL
- Melnitchouk A
- Menguzzato M
- Menguzzato M
- Menzione A
- Menzione A
- Merkel P
- Merkel P
- Merkin M
- Merritt KW
- Mesropian C
- Mesropian C
- Meyer A
- Meyer A
- Miao C
- Miao T
- Miao T
- Miettinen H
- Mihalcea D
- Miller JS
- Miller JS
- Miller R
- Miller R
- Minato H
- Minato H
- Miscetti S
- Miscetti S
- Mishina M
- Mishina M
- Mitselmakher G
- Mitselmakher G
- Miyazaki Y
- Moggi N
- Moggi N
- Mokhov N
- Mondal NK
- Montgomery HE
- Moore E
- Moore E
- Moore R
- Moore R
- Moore RW
- Morita Y
- Morita Y
- Moulik T
- Moulik T
- Mukherjee A
- Mukherjee A
- Mulhearn M
- Mulhearn M
- Muller T
- Muller T
- Munar A
- Munar A
- Murat P
- Murat P
- Murgia S
- Murgia S
- Musy M
- Mutaf YD
- Nachtman J
- Nachtman J
- Nagaslaev V
- Nagy E
- Nahn S
- Nahn S
- Nakada H
- Nakada H
- Nakano I
- Nakano I
- Nakaya T
- Napora R
- Napora R
- Narain M
- Narasimham VS
- Naumann NA
- Neal HA
- Neal HKorytov A
- Negret JP
- Nelson C
- Nelson C
- Nelson S
- Nelson T
- Nelson T
- Neu C
- Neu C
- Neubauer MS
- Neubauer MS
- Neuberger D
- Neuberger D
- Newman-Holmes C
- Newman-Holmes C
- Ngan CYP
- Ngan CYP
- Nicolaidi P
- Niell F
- Niell F
- Nigmanov T
- Nigmanov T
- Niu H
- Niu H
- Nodulman L
- Nodulman L
- Nomerotski A
- Nomerotski A
- Nunnemann T
- O'Neil D
- Oguri V
- Oh SH
- Oh SH
- Oh YD
- Oh YD
- Ohmoto T
- Ohmoto T
- Ohsugi T
- Ohsugi T
- Oishi R
- Oishi R
- Okusawa T
- Okusawa T
- Olsen J
- Olsen J
- Orejudos W
- Orejudos W
- Oshima N
- Padley P
- Pagliarone C
- Pagliarone C
- Palmonari F
- Palmonari F
- Pan Y
- Paoletti R
- Paoletti R
- Papadimitriou V
- Papadimitriou V
- Pappas SP
- Parashar N
- Partos D
- Partos D
- Partridge R
- Parua N
- Patrick J
- Patrick J
- Patwa A
- Pauletta G
- Pauletta G
- Paulini M
- Paulini M
- Pauly T
- Pauly T
- Paus C
- Paus C
- Pedis DD
- Pellett D
- Pellett D
- Penzo A
- Penzo A
- Pescara L
- Pescara L
- Peters O
- Petroff P
- Phillips TJ
- Phillips TJ
- Piacentino G
- Piacentino G
- Piedra J
- Piedra J
- Piegaia R
- Pitts KT
- Pitts KT
- Plunkett R
- Pompos A
- Pompos A
- Pondrom L
- Pondrom L
- Pope BG
- Pope G
- Pope G
- Popovic M
- Poukhov O
- Pratt T
- Pratt T
- Prepost R
- Prokoshin F
- Prokoshin F
- Prosper HB
- Protopopescu S
- Proudfoot J
- Proudfoot J
- Przybycien MB
- Ptohos F
- Ptohos F
- Pukhov O
- Pukhov O
- Punzi G
- Punzi G
- Qian J
- Rademacker J
- Rademacker J
- Ragan K
- Rajagopalan S
- Rakitine A
- Rakitine A
- Rapidis PA
- Ratnikov F
- Ratnikov F
- Ray H
- Ray H
- Reay NW
- Reher D
- Reher D
- Reichold A
- Reichold A
- Renton P
- Renton P
- Rescigno M
- Rescigno M
- Reucroft S
- Ribon A
- Ribon A
- Ridel M
- Riegler W
- Riegler W
- Rijssenbeek M
- Rimondi F
- Rimondi F
- Ristori L
- Ristori L
- Riveline M
- Riveline M
- Rizatdinova F
- Robertson WJ
- Robertson WJ
- Robinson A
- Rockwell T
- Rodrigo T
- Rodrigo T
- Rolli S
- Rolli S
- Rosenson L
- Rosenson L
- Roser R
- Roser R
- Rossin R
- Rossin R
- Rott C
- Rott C
- Roy A
- Roy A
- Royon C
- Rubinov P
- Ruchti R
- Ruiz A
- Ruiz A
- Ryan D
- Ryan D
- Sabirov BM
- Safonov A
- Safonov A
- Sajot G
- Sakumoto WK
- Sakumoto WK
- Saltzberg D
- Saltzberg D
- Sanchez C
- Sanchez C
- Sansoni A
- Sansoni A
- Santi L
- Santi L
- Santoro A
- Sarkar S
- Sarkar S
- Sato H
- Sato H
- Savard P
- Savard P
- Savoy-Navarro A
- Savoy-Navarro A
- Sawyer L
- Schamberger RD
- Schellman H
- Schlabach P
- Schlabach P
- Schmidt EE
- Schmidt EE
- Schmidt MP
- Schmidt MP
- Schmitt M
- Schmitt M
- Schwartzman A
- Scodellaro L
- Scodellaro L
- Scott A
- Scott A
- Scribano A
- Scribano A
- Sedov A
- Sedov A
- Segler S
- Seidel S
- Seidel S
- Seiya Y
- Seiya Y
- Semenov A
- Semenov A
- Semeria F
- Semeria F
- Shabalina E
- Shah T
- Shah T
- Shapiro MD
- Shapiro MD
- Shepard PF
- Shepard PF
- Shibayama T
- Shibayama T
- Shimojima M
- Shimojima M
- Shivpuri RK
- Shochet M
- Shochet M
- Shpakov D
- Shupe M
- Sidoti A
- Sidoti A
- Sidwell RA
- Siegrist J
- Siegrist J
- Signorelli G
- Sill A
- Sill A
- Simak V
- Sinervo P
- Sinervo P
- Singh P
- Singh P
- Sirotenko V
- Slattery P
- Slaughter AJ
- Slaughter AJ
- Sliwa K
- Sliwa K
- Smith C
- Smith RP
- Snider FD
- Snider FD
- Snihur R
- Snihur R
- Snow GR
- Snow J
- Snyder S
- Solodsky A
- Solodsky A
- Solomon J
- Song Y
- Sorin V
- Sosebee M
- Sotnikova N
- Soustruznik K
- Souza M
- Spalding J
- Speer T
- Speer T
- Spezziga M
- Spezziga M
- Sphicas P
- Sphicas P
- Spiegel L
- Spiegel L
- Spinella F
- Spinella F
- Spiropulu M
- Spiropulu M
- St Denis R
- Stanton NR
- Steele J
- Stefanini A
- Stefanini A
- Steinbruck G
- Stoker D
- Stolin V
- Stone A
- Stoyanova DA
- Strang MA
- Strauss M
- Strologas J
- Strologas J
- Strovink M
- Strumia F
- Strumia F
- Stuart D
- Stuart D
- Stutte L
- Sukhanov A
- Sukhanov A
- Sumorok K
- Sumorok K
- Suzuki T
- Suzuki T
- Sznajder A
- Takano T
- Takano T
- Takashima R
- Takashima R
- Takikawa K
- Takikawa K
- Talby M
- Tamburello P
- Tamburello P
- Tan P
- Tanaka M
- Tanaka M
- Tannenbaum B
- Tannenbaum B
- Taylor W
- Tecchio M
- Tecchio M
- Teng PK
- Teng PK
- Tentindo-Repond S
- Terashi K
- Terashi K
- Tesarek RJ
- Tesarek RJ
- Tether S
- Tether S
- Theriot D
- Thom J
- Thom J
- Thompson AS
- Thompson AS
- Thomson E
- Thomson E
- Thurman-Keup R
- Thurman-Keup R
- Tipton P
- Tipton P
- Tkaczyk S
- Tkaczyk S
- Toback D
- Toback D
- Tollefson K
- Tollefson K
- Tollestrup A
- Tonelli D
- Tonelli D
- Tonnesmann M
- Tonnesmann M
- Toyoda H
- Toyoda H
- Trippe TG
- Trischuk W
- Trischuk W
- Tseng J
- Tseng J
- Tsybychev D
- Tsybychev D
- Turcot AS
- Turini N
- Turini N
- Turini N
- Turner M
- Tuts PM
- Ukegawa F
- Ukegawa F
- Ukegawa F
- Unel MK
- Unverhau T
- Unverhau T
- Unverhau T
- Uozumi S
- Usynin D
- Vacavant L
- Vaiciulis T
- Vaiciulis T
- Vaiciulis T
- Valls J
- Van Kooten R
- Vaniev V
- Varelas N
- Varganov A
- Varganov A
- Varganov A
- Vataga E
- Vataga E
- Vataga E
- Vejcik S
- Vejcik S
- Vejcik S
- Velev G
- Velev G
- Velev G
- Veramendi G
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- Yao W
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- Yao W
- Yasuda T
- Yatsunenko YA
- Yeh GP
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- Zhou J
- Zsenei A
- Zucchelli Spatra AK
- Zucchelli Sychev D
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2004
- Field of study
We report on a search for direct Kaluza-Klein graviton production in a data
sample of 84 pb−1 of \ppb collisions at s = 1.8 TeV, recorded
by the Collider Detector at Fermilab. We investigate the final state of large
missing transverse energy and one or two high energy jets. We compare the data
with the predictions from a 3+1+n-dimensional Kaluza-Klein scenario in which
gravity becomes strong at the TeV scale. At 95% confidence level (C.L.) for
n=2, 4, and 6 we exclude an effective Planck scale below 1.0, 0.77, and 0.71
TeV, respectively.Comment: Submitted to PRL, 7 pages 4 figures/Revision includes 5 figure
Measurement of the average time-integrated mixing probability of b-flavored hadrons produced at the Tevatron
- Author
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- Wicklund E
- Wijngaarden DA
- Wilkes T
- Williams HH
- Williams HH
- Williams HH
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- Winer BL
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- Womersley J
- Wood DR
- Worcester M
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- Worm S
- Wright T
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- Wu X
- Wu X
- Wurthwein F
- Wurthwein F
- Wurthwein F
- Wyatt A
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- Yagil A
- Yagil A
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- Yamashita T
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- Yu S
- Yu S
- Yu Z
- Yu Z
- Yu Z
- Yun JC
- Yun JC
- Zanello L
- Zanello L
- Zanetti A
- Zanetti A
- Zaw I
- Zetti F
- Zetti F
- Zhou J
- Zsenei A
- Zucchelli Spatra AK
- Zucchelli Sychev D
- Zucchelli SZetti F
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 08/09/2003
- Field of study
We have measured the number of like-sign (LS) and opposite-sign (OS) lepton
pairs arising from double semileptonic decays of b and bˉ-hadrons,
pair-produced at the Fermilab Tevatron collider. The data samples were
collected with the Collider Detector at Fermilab (CDF) during the 1992-1995
collider run by triggering on the existence of μμ and eμ candidates
in an event. The observed ratio of LS to OS dileptons leads to a measurement of
the average time-integrated mixing probability of all produced b-flavored
hadrons which decay weakly, χˉ=0.152±0.007 (stat.) ±0.011
(syst.), that is significantly larger than the world average χˉ=0.118±0.005.Comment: 47 pages, 10 figures, 15 tables Submitted to Phys. Rev.
Search for the standard model Higgs boson at LEP
- Author
- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbiendi G
- Abdallah J
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- Achard P
- Adam W
- Adriani O
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- Affholderbach K
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- Vallage B
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- Wu SL
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- Wyatt TR
- Wynhoff S
- Xia L
- Xie Y
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- Xue S
- Yamamoto J
- Yamashita S
- Yang BZ
- Yang CG
- Yang HJ
- Yang M
- Yeh SC
- Yuan C
- Yushchenko O
- Zachariadou K
- Zalewska A
- Zalewski P
- Zalite A
- Zalite Y
- Zavrtanik D
- Zeitnitz C
- Zer-Zion D
- Zhang J
- Zhang L
- Zhang ZP
- Zhao J
- Zhao W
- Zhu GY
- Zhu RY
- Zhuang HL
- Zhuravlov V
- Zichichi A
- Ziegler T
- Zilizi G
- Zimin NI
- Zimmermann B
- Zintchenko A
- Zito G
- Zivkovic L
- Zobernig G
- Zoller M
- Zupan M
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
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
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
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- Amundsen G
- Anastopoulos C
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- Argyropoulos S
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- Carrillo-Montoya GD
- Carter JR
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- Casadei D
- Casado MP
- Castaneda-Miranda E
- Castanheira MTD
- Castelli A
- Castillo Gimenez V
- Castillo IS
- Castillo LRF
- Castillo LRF
- Castro NF
- Catastini P
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavaliere V
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerio B
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cerv M
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chan K
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
- Chen L
- Chen S
- Chen X
- Chen Y
- Cheng HC
- Cheng Y
- Cheplakov A
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiefari G
- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Chouridou S
- Chow BKB
- Christidi IA
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciocio A
- Cirkovic P
- Citron ZH
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- Clark A
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- Coccaro A
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- Cogan JG
- Coggeshall J
- Cole B
- Cole S
- Colijn AP
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- Collins-Tooth C
- Collot J
- Colombo T
- Colon G
- Compostella G
- Conde Muino P
- Coniavitis E
- Conidi MC
- Connelly IA
- Consonni SM
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- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
- Cottin G
- Coutinho YA
- Cowan G
- Cox BE
- Cranmer K
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Cuciuc C-M
- Cummings J
- Curatolo M
- Cuthbert C
- Czirr H
- Czodrowski P
- Czyczula Z
- D'Auria S
- D'Onofrio M
- Da Costa JBG
- Da Costa JGPF
- Da Costa JGPF
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dafinca A
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Daniells AC
- Dao V
- Darbo G
- Darlea GL
- Darmora S
- Dassoulas JA
- Davey W
- David C
- Davidek T
- Davies E
- Davies M
- Davignon O
- Davison AR
- Davison P
- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Asmundis R
- De Bruin PHS
- De Castro S
- De Cecco S
- de Graat J
- De Groot N
- de Jong P
- De la Taille C
- De la Torre H
- de Lima DEF
- de Lima DEF
- De Lorenzi F
- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De Zorzi G
- De K
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Degenhardt J
- Deigaard I
- Del Peso J
- Del Prete T
- Delemontex T
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- Deliyergiyev M
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- Dell'Asta L
- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demilly A
- Demirkoz B
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
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- Deviveiros PO
- Dewhurst A
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- Di Ciaccio A
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
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- Diehl EB
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- Evans H
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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
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
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- Zobernig G
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- zur Nedden M
- Zutshi V
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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- Abdallah J
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
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- Youssef S
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- Zaidan R
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- Zanzi D
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- Zemla A
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- Zenin O
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
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