1,489 research outputs found
FimL Regulates cAMP Synthesis in Pseudomonas aeruginosa
- Author
- A Becher
- AJ Leech
- AJ Vallis
- AR Hauser
- AR Hauser
- B Gorke
- BW Holloway
- CB Whitchurch
- CB Whitchurch
- DD Ellefson
- EL Fuchs
- EL Fuchs
- GL Mandell
- HD Kulasekara
- I Ventre
- J Comolli
- J Engel
- J Monod
- J Vieira
- JJ Bertrand
- JL Botsford
- Joanne N. Engel
- JS Mattick
- JS Mattick
- KJ Kanack
- L Friedman
- LP Macfadyen
- LS Siegel
- M Christen
- M Tsuda
- MC Wolfgang
- Medora J. Huseby
- MH Saier Jr
- MW Tan
- N Buddelmeijer
- NB Fulcher
- PJ Kang
- PV Liu
- R Rosqvist
- RE Vance
- RS Smith
- SA Beatson
- SEH West
- Stefan Bereswill
- T Endoh
- TI Nicas
- TT Hoang
- V De Lorenzo
- V Jaumouille
- Yuki F. Inclan
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Pseudomonas aeruginosa, a ubiquitous bacteria found in diverse ecological niches, is an important cause of acute infections in immunocompromised individuals and chronic infections in patients with Cystic Fibrosis. One signaling molecule required for the coordinate regulation of virulence factors associated with acute infections is 3â˛, 5â˛-cyclic adenosine monophosphate, (cAMP), which binds to and activates a catabolite repressor homolog, Vfr. Vfr controls the transcription of many virulence factors, including those associated with Type IV pili (TFP), the Type III secretion system (T3SS), the Type II secretion system, flagellar-mediated motility, and quorum sensing systems. We previously identified FimL, a protein with histidine phosphotransfer-like domains, as a regulator of Vfr-dependent processes, including TFP-dependent motility and T3SS function. In this study, we carried out genetic and physiologic studies to further define the mechanism of action of FimL. Through a genetic screen designed to identify suppressors of FimL, we found a putative cAMP-specific phosphodiesterase (CpdA), suggesting that FimL regulates cAMP levels. Inactivation of CpdA increases cAMP levels and restores TFP-dependent motility and T3SS function to fimL mutants, consistent with in vivo phosphodiesterase activity. By constructing combinations of double and triple mutants in the two adenylate cyclase genes (cyaA and cyaB), fimL, and cpdA, we show that ÎfimL mutants resemble ÎcyaB mutants in TM defects, decreased T3SS transcription, and decreased cAMP levels. Similar to some of the virulence factors that they regulate, we demonstrate that CyaB and FimL are polarly localized. These results reveal new complexities in the regulation of diverse virulence pathways associated with acute P. aeruginosa infections
Genetic Patterns of Domestication in Pigeonpea (Cajanus cajan (L.) Millsp.) and Wild Cajanus Relatives
- Author
- A Bohra
- A Eyre-Walker
- A Liu
- AJ Redd
- B Kilian
- Birinchi K. Sarma
- D Falush
- DA Odeny
- DL Hyten
- DL Swofford
- DN De
- Douglas R. Cook
- Eric J. B. von Wettberg
- ES Buckler
- G Evanno
- G Lewis
- GK Bhatia
- Hari D. Upadhyaya
- HD Tindall
- HD Upadhyaya
- HD Upadhyaya
- J Dubcovsky
- J Guo
- J Souframanien
- JK Pritchard
- JR Harlan
- JR Motta-Aldana
- JW Purseglove
- KB Saxena
- KB Saxena
- KB Saxena
- KB Saxena
- L Excoffier
- L Excoffier
- LA Hauser
- LJ Reddy
- LJG Van der Maesen
- LJG Van der Maesen
- LJG Van der Maesen
- LJG Van der Maesen
- MB Ratnaparkhe
- MD Kajale
- MI Tenaillon
- Mulualem T. Kassa
- MV Bagavathiannan
- N Mallikarjuna
- N Saitou
- Noelia Carrasquilla-Garcia
- PL Morrell
- Q Zhu
- R Peakall
- R. Varma Penmetsa
- Rajeev K. Varshney
- RG Allaby
- RH Fortunato
- S Yang
- SD Tanksley
- Shin-Han Shiu
- Subhojit Datta
- V Macaulay
- WJ Bruno
- X Perrier
- Y Matsuoka
- YH Li
- YL Nene
- Z He
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
Pigeonpea (Cajanus cajan) is an annual or short-lived perennial food legume of acute regional importance, providing significant protein to the human diet in less developed regions of Asia and Africa. Due to its narrow genetic base, pigeonpea improvement is increasingly reliant on introgression of valuable traits from wild forms, a practice that would benefit from knowledge of its domestication history and relationships to wild species. Here we use 752 single nucleotide polymorphisms (SNPs) derived from 670 low copy orthologous genes to clarify the evolutionary history of pigeonpea (79 accessions) and its wild relatives (31 accessions). We identified three well-supported lineages that are geographically clustered and congruent with previous nuclear and plastid sequence-based phylogenies. Among all species analyzed Cajanus cajanifolius is the most probable progenitor of cultivated pigeonpea. Multiple lines of evidence suggest recent gene flow between cultivated and non-cultivated forms, as well as historical gene flow between diverged but sympatric species. Evidence supports that primary domestication occurred in India, with a second and more recent nested population bottleneck focused in tropical regions that is the likely consequence of pigeonpea breeding. We find abundant allelic variation and genetic diversity among the wild relatives, with the exception of wild species from Australia for which we report a third bottleneck unrelated to domestication within India. Domesticated C. cajan possess 75% less allelic diversity than the progenitor clade of wild Indian species, indicating a severe âdomestication bottleneckâ during pigeonpea domestication
Perception of Male Caller Identity in Koalas (Phascolarctos cinereus): Acoustic Analysis and Playback Experiments
- Author
- A Taylor
- AG McElligott
- Allan J. McKinnon
- BD Charlton
- BD Charlton
- BD Charlton
- Benjamin D. Charlton
- BG Tabachnick
- C Shipley
- D Reby
- D Reby
- D Reby
- D Reby
- D Reby
- D Rendall
- D Rendall
- DT Blumstein
- E Vannoni
- E Zimmerman
- EA Tibbetts
- G Fant
- GD Ruxton
- HD Kimmel
- I Charrier
- I Charrier
- IR Titze
- J Fischer
- J Soltis
- JA Bachorowski
- Jacqui Brumm
- JF Hare
- JS Tripovich
- K McComb
- K McComb
- Karen Nilsson
- KH Frommolt
- LS Sayigh
- M Smith
- MD Hauser
- MD Hauser
- MJ Owren
- MJ Owren
- ML East
- MV Torriani
- Nicolas Mathevon
- P Mitchell
- R Martin
- RR Swaisgood
- T Aubin
- T Riede
- W. Tecumseh Fitch
- WAH Ellis
- WAH Ellis
- William A. H. Ellis
- WT Fitch
- WT Fitch
- WT Fitch
- WT Fitch
- WT Fitch
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
The ability to signal individual identity using vocal signals and distinguish between conspecifics based on vocal cues is important in several mammal species. Furthermore, it can be important for receivers to differentiate between callers in reproductive contexts. In this study, we used acoustic analyses to determine whether male koala bellows are individually distinctive and to investigate the relative importance of different acoustic features for coding individuality. We then used a habituation-discrimination paradigm to investigate whether koalas discriminate between the bellow vocalisations of different male callers. Our results show that male koala bellows are highly individualized, and indicate that cues related to vocal tract filtering contribute the most to vocal identity. In addition, we found that male and female koalas habituated to the bellows of a specific male showed a significant dishabituation when they were presented with bellows from a novel male. The significant reduction in behavioural response to a final rehabituation playback shows this was not a chance rebound in response levels. Our findings indicate that male koala bellows are highly individually distinctive and that the identity of male callers is functionally relevant to male and female koalas during the breeding season. We go on to discuss the biological relevance of signalling identity in this species' sexual communication and the potential practical implications of our findings for acoustic monitoring of male population levels
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
- 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
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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 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
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- Worcester M
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- Worm S
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- 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 ΟΟ and eΟ 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, ĎËâ=0.152Âą0.007 (stat.) Âą0.011
(syst.), that is significantly larger than the world average ĎËâ=0.118Âą0.005.Comment: 47 pages, 10 figures, 15 tables Submitted to Phys. Rev.
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
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- Acosta MV
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- Wissing C
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- Wood JS
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- Xiao H
- Xie S
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- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
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- Zielinski M
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
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- Wissing C
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- Woehri HK
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- Womersley WJ
- Won S
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- Wood J
- Wood JS
- Worm SD
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- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
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
- Anastopoulos C
- Ancu LS
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- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
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- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
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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 âs = 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 pTâĽ20 GeV and pseudorapidities {pipe}Ρ{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}Ρ{pipe}<0. 8) for jets with 60â¤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â¤{pipe}Ρ{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. Š 2013 CERN for the benefit of the ATLAS collaboration
X-ray emission from the Sombrero galaxy: discrete sources
- Author
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- Zotto P
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
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- Acosta JG
- Acosta MV
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- Adam W
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- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
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