260 research outputs found
Impact of Forest Seral Stage on use of Ant Communities for Rapid Assessment of Terrestrial Ecosystem Health
- Author
- Publication venue
- University of Wisconsin Library
- Publication date
- Field of study
Bioassessment evaluates ecosystem health by using the responses of a community of organisms that integrate all aspects of the ecosystem. A variety of bioassessment methods have been applied to aquatic ecosystems; however, terrestrial methods are less advanced. The objective of this study was to examine baseline differences in ant communities at different seral stages from clear cut to mature pine plantation as a precursor to developing a broader terrestrial bioassessment protocol. Comparative sampling was conducted at nine sites having four seral stages: clearcut, 5 year recovery, 15 year recovery, and mature stands. Soil and vegetation data were also collected at each site. Ants were identified to genus. Analysis of the ant data indicated that ants respond strongly to habitat changes that accompany ecological succession in managed pine forests, and both individual genera and ant community structure can be used as indicators of successional change. Ants exhibited relatively high diversity in both early and mature seral stages. High ant diversity in mature seral stages was likely related to conditions on the forest floor favoring litter dwelling and cold climate specialists. While ants may be very useful in identifying environmental stress in managed pine forests, adjustments must be made for seral stage when comparing impacted and unimpacted forests
Effect of environmental quality and mesohabitat structure on a Biotic Integrity Index based on fish assemblages of cerrado streams from Rio Cuiabá basin, Brazil
- Author
- ALLAN JD
- ALLAN JD.
- ALLAN JD.
- ANGERMEIER PL.
- ANGERMEIER PL.
- ARAÚJO FG.
- BOZZETTI M
- BRITSKI H.A.
- CHURCH M.
- EM. Venticinque
- FAUSCH KD.
- FERREIRA MT.
- GALUCH AV.
- GANASAN V.
- HILL BH.
- J. Penha
- JAMESON SC.
- JEPSON W.
- JOY MK.
- KARR JR
- KARR JR.
- KARR JR.
- KENNARD MJ.
- KERANS BL
- KIMBERLING DN
- KLINK CA
- LIBOS M.
- LYONS J.
- MAGNUSSON WE
- MEADOR MR.
- MICACCHION M
- NG Machado
- NIEMI GJ
- OBERDORFF T.
- OBERDORFF T.
- OLIVEIRA RS.
- OVIDIO M
- PAULY D.
- PICHON C
- PRINGLE C
- RATTER JA.
- REIS R.E.
- ROBINSON CT.
- RODRÍGUEZ-OLARTE D.
- SCHLOSSER IJ
- STAUFFER JC
- STRIBLING JB
- TOHAM AK
- VUGTEVEEN P
- WANTZEN KM
- WEISBERG SB
- WIENS JA
- ZAR JH.
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Secure and scalable deduplication of horizontally partitioned health data for privacy-preserving distributed statistical computation
- Author
- A Beimel
- A Geissbuhler
- AF Karr
- AF Karr
- AL Potosky
- Antonis Michalas
- AS Lunde
- B Pinkas
- BA Malin
- BA Stewart
- BH Bloom
- C Clifton
- C Friedman
- C Quantin
- D Vatsalan
- EA Durham
- G Cormode
- G Hripcsak
- GM Weber
- GM Weber
- GM Weber
- IS Kohane
- J Gichoya
- J Vaidya
- JF Ludvigsson
- JH Holmes
- JL Warren
- Johan Gustav Bellika
- JT Finnell
- K Emam El
- K Emam El
- K Emam El
- K Emam El
- Kassaye Yitbarek Yigzaw
- L Fan
- L Lenert
- LH Curtis
- M Kantarcioglu
- MA Hailemichael
- MA Hernández
- MK Ross
- O Goldreich
- P Christen
- P Paillier
- P Saint-Andre
- R Cramer
- R Lazarus
- R Lazarus
- R Schnell
- RL Richesson
- S Tarkoma
- SC Pohlig
- SM Randall
- T Dimitriou
- W Du
- W Du
- WB Lober
- Y Lindell
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Background
Techniques have been developed to compute statistics on distributed datasets without revealing private information except the statistical results. However, duplicate records in a distributed dataset may lead to incorrect statistical results. Therefore, to increase the accuracy of the statistical analysis of a distributed dataset, secure deduplication is an important preprocessing step.
Methods
We designed a secure protocol for the deduplication of horizontally partitioned datasets with deterministic record linkage algorithms. We provided a formal security analysis of the protocol in the presence of semi-honest adversaries. The protocol was implemented and deployed across three microbiology laboratories located in Norway, and we ran experiments on the datasets in which the number of records for each laboratory varied. Experiments were also performed on simulated microbiology datasets and data custodians connected through a local area network.
Results
The security analysis demonstrated that the protocol protects the privacy of individuals and data custodians under a semi-honest adversarial model. More precisely, the protocol remains secure with the collusion of up to N − 2 corrupt data custodians. The total runtime for the protocol scales linearly with the addition of data custodians and records. One million simulated records distributed across 20 data custodians were deduplicated within 45 s. The experimental results showed that the protocol is more efficient and scalable than previous protocols for the same problem.
Conclusions
The proposed deduplication protocol is efficient and scalable for practical uses while protecting the privacy of patients and data custodians
On a smoothed penalty-based algorithm for global optimization
- Author
- A Auslender
- AE Xavier
- AF Karr
- AMAC Rocha
- AMAC Rocha
- Ana Maria A. C. Rocha
- CAC Coello
- CC Gonzaga
- DP Bertsekas
- E Mezura-Montes
- ED Dolan
- Edite M. G. P. Fernandes
- EG Birgin
- EK Silva
- G Pillo Di
- HJC Barbosa
- I Boussaïd
- J Brest
- J Derrac
- J-L Liu
- JD Griffin
- JH Holland
- K Deb
- K Socha
- K Sörensen
- M Neshat
- M. Fernanda P. Costa
- MFP Costa
- MM Ali
- MM Ali
- N Hansen
- N Hansen
- R Hooke
- S Kirkpatrick
- YG Petalas
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
This paper presents a coercive smoothed penalty framework for nonsmooth and nonconvex constrained global optimization problems. The properties of the smoothed penalty function are derived. Convergence to an ε -global minimizer is proved. At each iteration k, the framework requires the ε(k) -global minimizer of a subproblem, where ε(k)→ε . We show that the subproblem may be solved by well-known stochastic metaheuristics, as well as by the artificial fish swarm (AFS) algorithm. In the limit, the AFS algorithm convergence to an ε(k) -global minimum of the real-valued smoothed penalty function is guaranteed with probability one, using the limiting behavior of Markov chains. In this context, we show that the transition probability of the Markov chain produced by the AFS algorithm, when generating a population where the best fitness is in the ε(k)-neighborhood of the global minimum, is one when this property holds in the current population, and is strictly bounded from zero when the property does not hold. Preliminary numerical experiments show that the presented penalty algorithm based on the coercive smoothed penalty gives very competitive results when compared with other penalty-based methods.The authors would like to thank two anonymous referees for their valuable comments and
suggestions to improve the paper.
This work has been supported by COMPETE: POCI-01-0145-FEDER-007043 and FCT
- Fundac¸ao para a Ci ˜ encia e Tecnologia within the projects UID/CEC/00319/2013 and ˆ
UID/MAT/00013/2013.info:eu-repo/semantics/publishedVersio
Diffractive Dijet Production at sqrt(s)=630 and 1800 GeV at the Fermilab Tevatron
- Author
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Amaral P
- 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
- Bailey S
- Band HR
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berge JP
- Berryhill J
- Bhatti A
- Bianchi F
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bolla G
- Bona M
- Bonushkin Y
- Borras K
- Bortoletto D
- Bosisio L
- Boudreau J
- Brandl A
- Bromberg C
- Brown CM
- Brozovic M
- Brubaker E
- Bruner N
- Buckley-Geer E
- Budagov J
- Budd HS
- Bugg W
- Burchat PR
- Burkett K
- Busetto G
- Byon-Wagner A
- Byrum KL
- Cabrera S
- Calafiura P
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cerri A
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Charles E
- Chen C
- Chen YC
- Cheng CH
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung JY
- Chung YS
- Ciobanu CI
- Clark AG
- Cohn H
- Colijn AP
- Connolly A
- Convery ME
- Conway J
- Cordelli M
- Coward DH
- Cranshaw J
- Cropp R
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dasu S
- de Barbaro P
- de Troconiz JF
- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Della Ricca G
- Demers S
- Demortier L
- Deninno M
- Derwent PF
- Devlin T
- Di Lodovico F
- Dittmann JR
- Dominguez A
- Donati S
- Done J
- Dong D
- Dorfan J
- Dorigo T
- Dunwoodie W
- Eddy N
- Eichenbaum AM
- Einsweiler K
- Elias JE
- Engels E
- Erbacher R
- Errede D
- Errede S
- Fan Q
- Fang HC
- Feild RG
- Fernandez JP
- Ferretti C
- Field RC
- Field RD
- Fiori I
- Flaugher B
- Foster GW
- Franklin M
- Freeman J
- Friedman J
- Fukui Y
- Furic I
- Galeotti S
- Gallas A
- Gallinaro M
- Gamba D
- Gao T
- Garcia-Sciveres M
- Garfinkel AF
- Gatti P
- Gay C
- Gerdes DW
- Giannetti P
- Glagolev V
- Glanzman T
- Glenzinski D
- Godfrey GL
- Gold M
- Goldstein J
- Gorelov I
- Goshaw AT
- Gotra Y
- Goulianos K
- Gowdy SJ
- Green C
- Grim G
- Gris P
- Grosso P
- Grosso-Pilcher C
- Guenther M
- Guillian G
- Haas RM
- Haas T
- Haber C
- Hahn SR
- Hall C
- Handa T
- Handler R
- Hao W
- Happacher F
- Hara K
- Hardman AD
- Harris RM
- Hartmann F
- Hatakeyama K
- Hauser J
- Heinrich J
- Heiss A
- Henderson R
- Herndon M
- Hill C
- Himel T
- Hocker A
- Hoffman KD
- Hollebeek R
- Holloway L
- Hryn'ova T
- Hu H
- Huffer ME
- Huffman BT
- Hughes R
- Huston J
- Huth J
- Ikeda H
- Incandela J
- Innes WR
- Introzzi G
- Ivanov A
- Iwai J
- Iwata Y
- Izen JM
- Jackson PD
- James E
- Jessop CP
- Johnson JR
- Jones M
- Joshi U
- Kambara H
- Kamon T
- Kaneko T
- Karr K
- Kartal S
- Kasha H
- Kato Y
- Keaffaber TA
- Kelley K
- Kelly M
- Kelsey MH
- Khazins D
- Kikuchi T
- Kilminster B
- Kim BJ
- Kim DH
- Kim HS
- Kim MJ
- Kim P
- Kim SB
- Kim SH
- Kim YK
- Kirby M
- Kirk M
- Kirsch L
- Kitayama I
- Klimenko S
- Kocian ML
- Koehn P
- Kondo K
- Konigsberg J
- Kordich TMB
- Korn A
- Korytov A
- Kovacs E
- Kowalewski R
- Kroll J
- Kruse M
- Kuhlmann SE
- Kurino K
- Kuwabara T
- Laasanen AT
- Lai N
- Lami S
- Lammel S
- Lancaster J
- Lancaster M
- Lanceri L
- Lander R
- Langenegger U
- Lath A
- Latino G
- LeCompte T
- Lee AM
- Lee K
- Leith DWGS
- Leone S
- Lewis JD
- Lindgren M
- Liss TM
- Litvintsev DO
- Liu JB
- Liu R
- Liu YC
- Lobban O
- Lockyer NS
- Loken J
- Loreti M
- Lou XC
- Lucchesi D
- Luitz S
- Lukens P
- Lusin S
- Luth V
- Lynch HL
- Lyons L
- Lys J
- Madrak R
- Maeshima K
- Maksimovic P
- Malferrari L
- Mangano M
- Mariotti M
- Marsiske H
- Martignon G
- Martin A
- Matthews JAJ
- Mayer J
- Mazzanti P
- McFarland KS
- McIntyre P
- Menguzzato M
- Menke S
- Menzione A
- Merkel P
- Mesropian C
- Messner R
- Meyer A
- Meyer TI
- Miao T
- Miller JS
- Miller R
- Minato H
- Miscetti S
- Mishina M
- Mitselmakher G
- Miyazaki Y
- Moffeit KC
- Moggi N
- Moore C
- Moore E
- Moore R
- Morita Y
- Moulik T
- Mount R
- Mukherjee A
- Mulhearn M
- Muller DR
- Muller T
- Munar A
- Murat P
- Murgia S
- Nachtman J
- Nagaslaev V
- Nahn S
- Nakada H
- Nakano I
- Neal H
- Nelson C
- Nelson T
- Neu C
- Neuberger D
- Newman-Holmes C
- Ngan CYP
- Niu H
- Nodulman L
- Nomerotski A
- O'Grady CP
- Oh SH
- Oh YD
- Ohmoto T
- Ohsugi T
- Oishi R
- Okusawa T
- Olsen J
- Orejudos W
- Ozcan VE
- Pagliarone C
- Palmonari F
- Pan Y
- Panvini RS
- Paoletti R
- Papadimitriou V
- Partos D
- Patrick J
- Pauletta G
- Paulini M
- Paus C
- Pellett D
- Perl M
- Pescara L
- Petrak S
- Phillips TJ
- Piacentino G
- Pitts KT
- Pompos A
- Pondrom L
- Pope G
- Popovic M
- Poropat P
- Prepost R
- Prokoshin F
- Proudfoot J
- Ptohos F
- Pukhov O
- Punzi G
- Quinn H
- Rakitine A
- Ratcliff BN
- Ratnikov F
- Reher D
- Reichold A
- Renton P
- Ribon A
- Riegler W
- Rimondi F
- Ristori L
- Riveline M
- Roat C
- Robertson SH
- Robertson WJ
- Robinson A
- Rochester LS
- Rodrigo T
- Rolli S
- Roney JM
- Roodman A
- Rosenson L
- Roser R
- Rossin R
- Rott C
- Roy A
- Ruiz A
- Safonov A
- Sakumoto WK
- Salnikov AA
- Saltzberg D
- Sanchez C
- Sansoni A
- Santi L
- Sato H
- Savard P
- Savoy-Navarro A
- Schietinger T
- Schindler RH
- Schlabach P
- Schmidt EE
- Schmidt MP
- Schmitt M
- Schwiening J
- Scodellaro L
- Scott A
- Scott IJ
- Scribano A
- Sedov A
- Segler S
- Seidel S
- Seiya Y
- Sekula SJ
- Semenov A
- Semeria F
- Serbo VV
- Shah T
- Shapiro MD
- Shepard PF
- Shibayama T
- Shimojima M
- Shochet M
- Sidoti A
- Siegrist J
- Sill A
- Sinervo P
- Singh P
- Slaughter AJ
- Sliwa K
- Smith C
- Smol A
- Snider FD
- Snyder A
- Soha A
- Solodsky A
- Spalding J
- Spanier SM
- Speer T
- Sphicas P
- Spiegel L
- Spinella F
- Spiropulu M
- St Denis R
- Steele J
- Stefanini A
- Stelzer J
- Strologas J
- Strumia F
- Stuart D
- Su D
- Sullivan MK
- Sumorok K
- Suzuki T
- Takano T
- Takashima R
- Takikawa K
- Tamburello P
- Tanaka HA
- Tanaka M
- Tannenbaum B
- Tecchio M
- Teng PK
- Terashi K
- Tesarek RJ
- Tether S
- Thompson AS
- Thomson E
- Thurman-Keup R
- Tipton P
- Tkaczyk S
- Toback D
- Tollefson K
- Tollestrup A
- Tonelli D
- Toyoda H
- Trischuk W
- Tseng J
- Tsybychev D
- Turini N
- Ukegawa F
- Va'vra J
- Vaiciulis T
- Valls J
- van den Brink S
- Vejcik S
- Velev G
- Veramendi G
- Vidal R
- Vila I
- Vilar R
- Volobouev I
- von der Mey M
- von Wimmersperg-Toeller JH
- Vuagnin G
- Vucinic D
- Wagner RG
- Wagner RL
- Wagner SR
- Wallace NB
- Wan Z
- Wang C
- Wang MJ
- Wang SM
- Ward B
- Waschke S
- Watanabe T
- Waters D
- Watts T
- Webb R
- Weinstein AJR
- Wenzel H
- Wester WC
- Wicklund AB
- Wicklund E
- Wilkes T
- Williams HH
- Wilson P
- Winer BL
- Winn D
- Wisniewski WJ
- Wolbers S
- Wolinski D
- Wolinski J
- Wolinski S
- Worm S
- Wright DH
- Wu SL
- Wu X
- Wyss J
- Yao W
- Yeh GP
- Yeh P
- Yoh J
- Yosef C
- Yoshida T
- Young CC
- Yu I
- Yu S
- Yu Z
- Yu Z
- Zanetti A
- Zetti F
- Zucchelli S DP
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 17/09/2001
- Field of study
We report a measurement of the diffractive structure function FjjD of
the antiproton obtained from a study of dijet events produced in association
with a leading antiproton in pˉp collisions at s=630 GeV at the
Fermilab Tevatron. The ratio of FjjD at s=630 GeV to FjjD
obtained from a similar measurement at s=1800 GeV is compared with
expectations from QCD factorization and with theoretical predictions. We also
report a measurement of the ξ (x-Pomeron) and β (x of parton in
Pomeron) dependence of FjjD at s=1800 GeV. In the region
0.035<ξ<0.095, ∣t∣<1 GeV2 and β<0.5, FjjD(β,ξ) is
found to be of the form β−1.0±0.1ξ−0.9±0.1, which obeys
β-ξ factorization.Comment: LaTeX, 9 pages, Submitted to Phys. Rev. Letter
A Study of B0 -> J/psi K(*)0 pi+ pi- Decays with the Collider Detector at Fermilab
- Author
- Affolder T
- Akimoto H
- Akopian A
- Albrow MG
- Amaral P
- Amidei D
- Anikeev K
- Anthony PL
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Aston D
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Bailey S
- Baird K
- Band HR
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berge JP
- Berryhill J
- Bhatti A
- Bianchi F
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom E
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bokhari W
- Bolla G
- Bona M
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Boyarski AM
- Brandl A
- Bromberg C
- Brown CM
- Brozovic M
- Brubaker E
- Bruner N
- Buckley-Geer E
- Budagov J
- Budd HS
- Bugg W
- Bulos F
- Burchat PR
- Burkett K
- Busetto G
- Byon-Wagner A
- Byrum KL
- Cabrera S
- Calafiura P
- Calderini G
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cerri A
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Charles E
- Chen C
- Chen YC
- Cheng CH
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung YS
- Ciobanu CI
- Clark AG
- Claus R
- Cohn H
- Colijn AP
- Connolly A
- Convery MR
- Conway J
- Cordelli M
- Coupal DP
- Coward DH
- Cranshaw J
- Cropp R
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dasu S
- de Barbaro P
- De Silva A
- de Troconiz JF
- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Demortier L
- Deninno M
- Derwent PF
- Devlin T
- Di Girolamo B
- Di Lodovico F
- Dittmann JR
- Dominguez A
- Donati S
- Done J
- Dorfan J
- Dorigo T
- Doser M
- Dunwoodie W
- Eddy N
- Eichenbaum AM
- Einsweiler K
- Elias JE
- Engels E
- Erbacher R
- Errede D
- Errede S
- Fan Q
- Fang HC
- Feild RG
- Fernandez JP
- Ferretti C
- Field RC
- Field RD
- Fiori I
- Flaugher B
- Foster GW
- Franklin M
- Freeman J
- Friedman J
- Fukui Y
- Furic I
- Galeotti S
- Gallas A
- Gallinaro M
- Gamba D
- Gao T
- Garcia-Sciveres M
- Garfinkel AF
- Gatti P
- Gay C
- Gerdes DW
- Giannetti P
- Giromini P
- Glagolev V
- Glanzman T
- Glenzinski D
- Godfrey L
- Gold M
- Goldstein J
- Gorelov I
- Goshaw AT
- Gotra Y
- Goulianos K
- Gowdy SJ
- Green C
- Grim G
- Gris P
- Groer L
- Grosso P
- Grosso-Pilcher C
- Guenther M
- Guillian G
- Haas RM
- Haber C
- Hahn SR
- Hall C
- Handa T
- Handler R
- Hao W
- Happacher F
- Hara K
- Hardman AD
- Harris RM
- Hartmann F
- Hatakeyama K
- Hauser J
- Heinrich J
- Heiss A
- Henderson R
- Herndon M
- Hill C
- Himel T
- Hoffman KD
- Holck C
- Hollebeek R
- Holloway L
- Hu H
- Huffer ME
- Huffman BT
- Hughes R
- Huston J
- Huth J
- Ikeda H
- Incandela J
- Innes WR
- Introzzi G
- Iwai J
- Iwata Y
- Izen JM
- James E
- Jessop CP
- Johnson JR
- Jones M
- Joshi U
- Kambara H
- Kamon T
- Kaneko T
- Karr K
- Kasha H
- Kato Y
- Keaffaber TA
- Kelley K
- Kelly M
- Kelsey MH
- Kennedy RD
- Kephart R
- Khazins D
- Kikuchi T
- Kilminster B
- Kim BJ
- Kim DH
- Kim HS
- Kim MJ
- Kim P
- Kim SB
- Kim SH
- Kim YK
- Kirby M
- Kirk M
- Kirkby D
- Kirsch L
- Kitayama I
- Klimenko S
- Kocian ML
- Koehn P
- Kondo K
- Konigsberg J
- Kordich TMB
- Korn A
- Korytov A
- Kovacs E
- Kowalewski R
- Kroll J
- Kruse M
- Kuhlmann SE
- Kurino K
- Kuwabara T
- Laasanen AT
- Lai N
- Lami S
- Lammel S
- Lancaster J
- Lancaster M
- Lanceri L
- Lander R
- Langenegger U
- Lath A
- Latino G
- LeCompte T
- Lee AM
- Lee K
- Leith DWGS
- Leone S
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 09/08/2001
- Field of study
We report a study of the decays B0 -> J/psi K(*)0 pi+ pi-, which involve the
creation of a u u-bar or d d-bar quark pair in addition to a b-bar -> c-bar(c
s-bar) decay. The data sample consists of 110 1/pb of p p-bar collisions at
sqrt{s} = 1.8 TeV collected by the CDF detector at the Fermilab Tevatron
collider during 1992-1995. We measure the branching ratios to be BR(B0 -> J/psi
K*0 pi+ pi-) = (8.0 +- 2.2 +- 1.5) * 10^{-4} and BR(B0 -> J/psi K0 pi+ pi-) =
(1.1 +- 0.4 +- 0.2) * 10^{-3}. Contributions to these decays are seen from
psi(2S) K(*)0, J/psi K0 rho0, J/psi K*+ pi-, and J/psi K1(1270)
Search for Kaluza-Klein Graviton Emission in ppˉ Collisions at s=1.8 TeV using the Missing Energy Signature
- Author
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- 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
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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 AB
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- Wicklund AB
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- Wicklund E
- Wijngaarden DA
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- Williams HH
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- Winer BL
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- Winn D
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- Worcester M
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- 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 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.
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
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- Alison J
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- Allwood-Spiers SE
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- Amelung C
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- Zhemchugov A
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- 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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- 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
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
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- Bracinik J
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- Castanheira MTD
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- Zarzhitsky P
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- Zenonos Z
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- Zhemchugov A
- Zheng S
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
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