434 research outputs found
Visualizing Rank Deficient Models: A Row Equation Geometry of Rank Deficient Matrices and Constrained-Regression
- Author
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Situations often arise in which the matrix of independent variables is not of full column rank. That is, there are one or more linear dependencies among the independent variables. This paper covers in detail the situation in which the rank is one less than full column rank and extends this coverage to include cases of even greater rank deficiency. The emphasis is on the row geometry of the solutions based on the normal equations. The author shows geometrically how constrained-regression/generalized-inverses work in this situation to provide a solution in the face of rank deficiency
Energy- and flux-budget (EFB) turbulence closure model for the stably stratified flows. Part I: Steady-state, homogeneous regimes
- Author
- AF Kurbatsky
- AN Kolmogorov
- AS Monin
- AS Monin
- CR Rehmann
- CR Rehmann
- EB Kraus
- EJ Strang
- F Bertin
- F Dalaudier
- FG Jacobitz
- GL Mellor
- GS Poulos
- H Hanazaki
- H Hanazaki
- I. Rogachevskii
- IN Esau
- J Kondo
- JC Kaimal
- JC Rotta
- JCR Hunt
- JJ Rohr
- JR Holton
- K Keller
- L Mahrt
- L Umlauf
- L Umlauf
- LF Richardson
- LH Jin
- LH Shih
- N. Kleeorin
- PJ Luyten
- RG Moser
- RM Banta
- RV Ozmidov
- S Zilitinkevich
- S. S. Zilitinkevich
- SS Zilitinkevich
- SS Zilitinkevich
- SW Churchill
- T Elperin
- T Elperin
- T Foken
- T Mauritsen
- T. Elperin
- U Schumann
- VM Canuto
- VM Canuto
- W Weng
- Y Cheng
- Y Ohya
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 19/10/2006
- Field of study
We propose a new turbulence closure model based on the budget equations for
the key second moments: turbulent kinetic and potential energies: TKE and TPE
(comprising the turbulent total energy: TTE = TKE + TPE) and vertical turbulent
fluxes of momentum and buoyancy (proportional to potential temperature).
Besides the concept of TTE, we take into account the non-gradient correction to
the traditional buoyancy flux formulation. The proposed model grants the
existence of turbulence at any gradient Richardson number, Ri. Instead of its
critical value separating - as usually assumed - the turbulent and the laminar
regimes, it reveals a transition interval, 0.1< Ri <1, which separates two
regimes of essentially different nature but both turbulent: strong turbulence
at Ri<<1; and weak turbulence, capable of transporting momentum but much less
efficient in transporting heat, at Ri>1. Predictions from this model are
consistent with available data from atmospheric and lab experiments, direct
numerical simulation (DNS) and large-eddy simulation (LES).Comment: 40 pages, 6 figures, Boundary-layer Meteorology, resubmitted, revised
versio
Nonrandom Mixing Models of HIV Transmission
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1989
- Field of study
Models of HIV transmission and the AIDS epidemic generally assume random mixing among those infected with HIV and those who
are not. For sexually transmitted HIV, this implies that individuals select sex partners without regard to attributes such as familiarity,
attractiveness, or risk of infection. This paper formulates a model for examining the impact of nonrandom mixing on HIV transmission. We
present threshold conditions that determine when HIV epidemics can occur within the framework of this model. Nonrandom mixing is
introduced by assuming that sexually active individuals select sex partners to minimize the risk of infection. In addition to variability in risky
sex rates, some versions of our model allow for error (or noise) in information exchanged between prospective partners. We investigate
several models including random partner selection (or proportionate mixing), segregation of the population by risky sex rates, a probabilistic
combination of segregation and random selection induced by imperfect information (or preferred mixing), and a model of costly search with
perfect information. We develop examples which show that nonrandom mixing can lead to epidemics that are more severe or less severe than
random mixing. For reasonable parameter choices describing the AIDS epidemic, however, the results suggest that random mixing models
overstate the number of HIV infections that will occur
Frequent burning promotes invasions of alien plants into a mesic African savanna
- Author
- Andrew K. Skidmore
- AS MacDougall
- B Holle Von
- BW Wilgen Van
- BW Wilgen Van
- BW Wilgen Van
- BW Wilgen Van
- DJ Gibson
- DL Barnes
- E Edward
- F Langevelde Van
- F Oudtshoorn Van
- GE Gibbs Russell
- Herbert H. T. Prins
- HF Glen
- IM Grundy
- JE Keeley
- JL Lockwood
- JN Barney
- JP Grime
- K Roques
- K Shea
- L Henderson
- L Valery
- M Coates-Palgrave
- M Rouget
- M Sankaran
- Mhosisi Masocha
- MJ Crawley
- N Govender
- P Alpert
- P Frost
- P Savadogo
- PA Furley
- PJ Watson
- RJ Hobbs
- RM Strang
- S Lavorel
- SI Higgins
- SI Higgins
- WJ Bond
- WJ Bond
- WJ Bond
- WJ Bond
- WP Sousa
- Xavier Poshiwa
- Publication venue
- Publication date
- 01/01/2010
- Field of study
Fire is both inevitable and necessary for maintaining the structure and functioning of mesic savannas. Without disturbances such as fire and herbivory, tree cover can increase at the expense of grass cover and over time dominate mesic savannas. Consequently, repeated burning is widely used to suppress tree recruitment and control bush encroachment. However, the effect of regular burning on invasion by alien plant species is little understood. Here, vegetation data from a long-term fire experiment, which began in 1953 in a mesic Zimbabwean savanna, were used to test whether the frequency of burning promoted alien plant invasion. The fire treatments consisted of late season fires, lit at 1-, 2-, 3-, and 4-year intervals, and these regularly burnt plots were compared with unburnt plots. Results show that over half a century of frequent burning promoted the invasion by alien plants relative to areas where fire was excluded. More alien plant species became established in plots that had a higher frequency of burning. The proportion of alien species in the species assemblage was highest in the annually burnt plots followed by plots burnt biennially. Alien plant invasion was lowest in plots protected from fire but did not differ significantly between plots burnt triennially and quadrennially. Further, the abundance of five alien forbs increased significantly as the interval (in years) between fires became shorter. On average, the density of these alien forbs in annually burnt plots was at least ten times as high as the density of unburnt plots. Plant diversity was also altered by long-term burning. Total plant species richness was significantly lower in the unburnt plots compared to regularly burnt plots. These findings suggest that frequent burning of mesic savannas enhances invasion by alien plants, with short intervals between fires favouring alien forbs. Therefore, reducing the frequency of burning may be a key to minimising the risk of alien plant spread into mesic savannas, which is important because invasive plants pose a threat to native biodiversity and may alter savanna functioning
Search for Kaluza-Klein Graviton Emission in ppËâ Collisions at sâ=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
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- Le Y
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- Lee K
- Lee SW
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- Lee WM
- Leflat A
- Lehner F
- Leonardo N
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- Leone S
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- 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
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- Lyons L
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- Lys J
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- 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
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- Martin MI
- Martin V
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- Martinez M
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- 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
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- 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
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- Narain M
- Narasimham VS
- Naumann NA
- Neal HA
- Neal HKorytov A
- Negret JP
- Nelson C
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- Neu C
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- Neubauer MS
- Neubauer MS
- Neuberger D
- Neuberger D
- Newman-Holmes C
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- Ngan CYP
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- Nicolaidi P
- Niell F
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- Nigmanov T
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- Niu H
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- Nodulman L
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- 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
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- Pauly T
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- Paus C
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- Pedis DD
- Pellett D
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- Penzo A
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- Pescara L
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- Peters O
- Petroff P
- Phillips TJ
- Phillips TJ
- Piacentino G
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- Piedra J
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- Piegaia R
- Pitts KT
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- Plunkett R
- Pompos A
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- Pope BG
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- Popovic M
- Poukhov O
- Pratt T
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- Prepost R
- Prokoshin F
- Prokoshin F
- Prosper HB
- Protopopescu S
- Proudfoot J
- Proudfoot J
- Przybycien MB
- Ptohos F
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- Pukhov O
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- Punzi G
- Punzi G
- Qian J
- Rademacker J
- Rademacker J
- Ragan K
- Rajagopalan S
- Rakitine A
- Rakitine A
- Rapidis PA
- Ratnikov F
- Ratnikov F
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- Reay NW
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- Reichold A
- Reichold A
- Renton P
- Renton P
- Rescigno M
- Rescigno M
- Reucroft S
- Ribon A
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- Ridel M
- Riegler W
- Riegler W
- Rijssenbeek M
- Rimondi F
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- Ristori L
- Ristori L
- Riveline M
- Riveline M
- Rizatdinova F
- Robertson WJ
- Robertson WJ
- Robinson A
- Rockwell T
- Rodrigo T
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- Rolli S
- Rosenson L
- Rosenson L
- Roser R
- Roser R
- Rossin R
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- Ruchti R
- Ruiz A
- Ruiz A
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- Ryan D
- Sabirov BM
- Safonov A
- Safonov A
- Sajot G
- Sakumoto WK
- Sakumoto WK
- Saltzberg D
- Saltzberg D
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- Sansoni A
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- 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
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- Schmidt EE
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- Schmitt M
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- Schwartzman A
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- Scodellaro L
- Scott A
- Scott A
- Scribano A
- Scribano A
- Sedov A
- Sedov A
- Segler S
- Seidel S
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- Seiya Y
- Seiya Y
- Semenov A
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- Semeria F
- Semeria F
- Shabalina E
- Shah T
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- Shapiro MD
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- Shepard PF
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- Shibayama T
- Shibayama T
- Shimojima M
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- Shivpuri RK
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- Spinella F
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- 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
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- Strumia F
- Strumia F
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- Sukhanov A
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- Suzuki T
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- Takashima R
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- Talby M
- Tamburello P
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- Tanaka M
- Tanaka M
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- Tannenbaum B
- Taylor W
- Tecchio M
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- Tentindo-Repond S
- Terashi K
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- Tesarek RJ
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- Tipton P
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- Tkaczyk S
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- Toback D
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- Tollefson K
- Tollefson K
- Tollestrup A
- Tonelli D
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- Tonnesmann M
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- Toyoda H
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- Trippe TG
- Trischuk W
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- Tseng J
- Tseng J
- Tsybychev D
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- Turcot AS
- Turini N
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- Ukegawa F
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- Ukegawa F
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- Unverhau T
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- Uozumi S
- Usynin D
- Vacavant L
- Vaiciulis T
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- Van Kooten R
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- Vejcik S
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- von der Mey M
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- von Wimmersperg-Toeller JH
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- Waschke S
- Waschke S
- Watanabe T
- Watanabe T
- Waters D
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- Waters D
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- Wayne M
- Webb R
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- Weber M
- Weerts H
- Wenzel H
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- Whiteson D
- Wicklund AB
- Wicklund AB
- Wicklund AB
- Wicklund E
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- Wijngaarden DA
- Wilkes T
- Williams HH
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- Wimpenny SJ
- Winer BL
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- Xu Q
- Yagil A
- Yagil A
- Yamada R
- Yamamoto K
- Yamashita T
- Yang UK
- Yang UK
- Yang UK
- Yao W
- Yao W
- Yao W
- Yasuda T
- Yatsunenko YA
- Yeh GP
- Yeh GP
- Yeh GP
- Yeh P
- Yi K
- Yi K
- Yoh J
- Yoh J
- Yoon P
- Yorita K
- Yosef C
- Yoshida T
- Yoshida T
- Yu I
- Yu I
- 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
- 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 pbâ1 of \ppb collisions at sâ = 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
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Ambrose D
- Amidei D
- Anikeev K
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
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- Bachacou H
- Badgett W
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- Bisello D
- Bishai M
- Blair RE
- Blocker C
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- Blusk SR
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- Bodek A
- Bolla G
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- Boudreau J
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- Brubaker E
- Bruner N
- Budagov J
- Budd HS
- Burkett K
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- Byrum KL
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- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
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- Cauz D
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- Chang PT
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- Cheng MT
- Chertok M
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- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
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- Clark AG
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- Cordelli M
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- Culbertson R
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- da Costa JG
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- de Troconiz JF
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- Dell'Orso M
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- Dittmann JR
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- Worm S
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- Wu X
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- Wurthwein F
- Wurthwein F
- Wurthwein F
- Wyatt A
- Wyss J
- Wyss J
- Xu Q
- Yagil A
- Yagil A
- Yamada R
- Yamamoto K
- Yamashita T
- Yang UK
- Yang UK
- Yang UK
- Yao W
- Yao W
- Yao W
- Yeh GP
- Yeh GP
- Yeh P
- Yi K
- Yi K
- Yoh J
- Yoh J
- Yoon P
- Yorita K
- Yosef C
- Yoshida T
- Yoshida T
- Yu I
- Yu I
- 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 bË-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 ΌΌ and eΌ 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, ÏËâ=0.152±0.007 (stat.) ±0.011
(syst.), that is significantly larger than the world average ÏËâ=0.118±0.005.Comment: 47 pages, 10 figures, 15 tables Submitted to Phys. Rev.
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
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- Zaidan R
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- Zanzi D
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- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
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- Zhao Z
- Zhemchugov A
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) 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<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
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
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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 Ï 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, Ï, 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 ÎČ in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- 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
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MS
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
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- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
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- Altheimer A
- Gonzalez BA
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
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- Anastopoulos C
- Ancu LS
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- Andrieux M-L
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- Anghinolfi F
- Anisenkov A
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- Antonaki A
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- Apolle R
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- Mayes JB
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- Bailey DC
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- Baker OK
- Baker MD
- Baker S
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- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
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- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
- Ye S
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
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- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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- Zhemchugov A
- Zhong J
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fbâ1 of sâ=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan ÎČ < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
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- Abajyan T
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- Abdallah J
- Abdelalim AA
- Abdinov O
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- Yilmaz M
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- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zerwas D
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- Zhemchugov A
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal ZâČ Models
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