1,199 research outputs found
Foxp3 and IL-10 Expression Correlates with Parasite Burden in Lesional Tissues of Post Kala Azar Dermal Leishmaniasis (PKDL) Patients
- Author
- A Ismail
- A Mukherjee
- AP Campanelli
- C Baecher-Allan
- Christian R. Engwerda
- E Bourreau
- EE Zijlstra
- Gajendra Kumar Katara
- GD Miralles
- HW Murray
- M Murai
- M Walther
- ML Alegre
- ML Murphy
- NA Ansari
- Nasim Akhtar Ansari
- PJ Guerin
- Poonam Salotra
- PS Linsley
- R Kumar
- S Ganguly
- S Gasim
- S Nylén
- S Saha
- S Verma
- Sandeep Verma
- SK Rathi
- T Lindsten
- V. Ramesh
- Y Belkaid
- Publication venue
- Public Library of Science
- Publication date
- 31/05/2011
- Field of study
Post kala azar dermal leishamniasis (PKDL), an unusual dermatosis develops in 5–15% of apparently cured visceral leishmaniasis cases in India and in about 60% of cases in Sudan. PKDL cases assume importance since they constitute a major human reservoir for the parasite. Inadequate treatment of VL, genetics, nutrition and immunological mechanisms that allow renewed multiplication of latent parasites or reinfection predispose to PKDL. Immunopathogenesis of PKDL is poorly understood. IL-10 is widely accepted as an immuno-suppressive cytokine and produced by diverse cell populations including, B cells, macrophages and CD4+ T cells. Natural T regulatory (nTreg) cells are subpopulation of CD4+ T cells that inhibit the response of other T cells. In this study we reported the accumulation of nTreg cells in lesion tissues of PKDL patients. Further correlation of Treg markers and IL-10 with parasite load in lesion tissues suggested a role of IL-10 and Treg in parasite establishment or persistence. Further studies are warranted to explore antigen specific IL-10 source in lesion tissues and unravel the concerted induction or accumulation of Treg in PKDL
Cell-Free Antigens from Paracoccidioides brasiliensis Drive IL-4 Production and Increase the Severity of Paracoccidioidomycosis
- Author
- A Pina
- A Restrepo
- A Restrepo
- A Restrepo-Moreno
- AF Popi
- Ana Paula Campanelli
- Ana Paula Moreira
- AP Campanelli
- AP Moreira
- AS Karhawi
- BE Jimenez-Finkel
- C Arruda
- CP Taborda
- Cristiane M. Milanezi
- E Brummer
- E Cenci
- EC Saraiva
- EG Rodrigues
- EM do Nascimento Martins
- EM do Nascimento Martins
- Fabrine S. M. Tristao
- Fernanda A. Rocha
- G Benard
- G Benard
- Jaqueline O. Vancim
- JG McEwen
- JI Figueroa
- Joao S. Silva
- JT Souto
- Karen A. Cavassani
- KC Coltri
- KS Ferreira
- KS Ferreira
- LE Cano
- Leandro L. Oliveira
- Luciano A. Panagio
- M Casotto
- M Franco
- M Kopf
- M Moscardi-Bacchi
- Marcos A. Rossi
- MC Livonesi
- MC Livonesi
- MI Borges-Walmsley
- MT Peracoli
- Niels Olsen Saraiva Câmara
- R de Bastos Ascenco Soares
- R Puccia
- Roberto Martinez
- S Bertini
- S Commins
- SR Almeida
- TA Costa
- VL Calich
- VL Calich
- W Noel
- WX Wang
- Z Zhu
- ZF Coutinho
- ZP Camargo
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
The thermally dimorphic fungus Paracoccidioides brasiliensis (Pb) is the causative agent of paracoccidioidomycosis (PCM), one of the most frequent systemic mycosis that affects the rural population in Latin America. PCM is characterized by a chronic inflammatory granulomatous reaction, which is consequence of a Th1-mediated adaptive immune response. In the present study we investigated the mechanisms involved in the immunoregulation triggered after a prior contact with cell-free antigens (CFA) during a murine model of PCM. The results showed that the inoculation of CFA prior to the infection resulted in disorganized granulomatous lesions and increased fungal replication in the lungs, liver and spleen, that paralleled with the higher levels of IL-4 when compared with the control group. The role of IL-4 in facilitating the fungal growth was demonstrated in IL-4-deficient- and neutralizing anti-IL-4 mAb-treated mice. The injection of CFA did not affect the fungal growth in these mice, which, in fact, exhibited a significant diminished amount of fungus in the tissues and smaller granulomas. Considering that in vivo anti-IL-4-application started one week after the CFA-inoculum, it implicates that IL-4-CFA-induced is responsible by the mediation of the observed unresponsiveness. Further, the characterization of CFA indicated that a proteic fraction is required for triggering the immunosuppressive mechanisms, while glycosylation or glycosphingolipids moieties are not. Taken together, our data suggest that the prior contact with soluble Pb antigens leads to severe PCM in an IL-4 dependent manner
Lorentz-violating inflationary magnetogenesis
- Author
- A Akhtari-Zavareh
- A Ashoorioon
- A Berera
- A Berera
- A Brandenburg
- A Brandenburg
- A Brandenburg
- A Dolgov
- A Kandus
- A Mazumdar
- A Neronov
- AC Davis
- AL Maroto
- AP Kouretsis
- B Cheng
- B Ratra
- BA Bassett
- C Caprini
- C Fronsdal
- C Zunckel
- CG Tsagas
- CG Tsagas
- CG Tsagas
- CT Byrnes
- D Biskamp
- D Colladay
- D Lemoine
- DH Lyth
- DT Son
- E Fermi
- EW Kolb
- F Tavecchio
- F Tavecchio
- FA Membiela
- FD Mazzitelli
- G Betschart
- G Tasinato
- I Agullo
- J Gamboa
- J Martin
- JD Barrow
- JD Barrow
- JD Barrow
- JD Barrow
- JP Vallée
- K Bamba
- K Bamba
- K Bamba
- K Bamba
- K Bamba
- K Bamba
- K Bamba
- K Bamba
- K Dimopoulos
- K Dimopoulos
- K Dolag
- KE Kunze
- KE Kunze
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Campanelli
- L Parker
- LD Landau
- Leonardo Campanelli
- LM Widrow
- M Christensson
- M Gasperini
- M Giovannini
- M Giovannini
- M Giovannini
- M Giovannini
- M Giovannini
- M Giovannini
- M Giovannini
- M Giovannini
- M Marklund
- M Shiraishi
- MM Anber
- MR Garousi
- MS Turner
- N Barnaby
- ND Birrell
- O Bertolami
- P Olesen
- PP Kronberg
- PP Kronberg
- R Banerjee
- R Banerjee
- R Banerjee
- R Durrer
- R Durrer
- R Gambini
- R Pakmor
- RJZ Ferreira
- RJZ Ferreira
- SW Hawking
- T Fujita
- T Kahniashvili
- T Kahniashvili
- T Kahniashvili
- T Kahniashvili
- T Kahniashvili
- T Prokopec
- T Suyama
- V Demozzi
- VA Kostelecky
- VA Kostelecky
- VA Kostelecky
- WE Boyce
- Y Shtanov
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for Charged Higgs Bosons in e+e- Collisions at \sqrt{s} = 189 GeV
- Author
- Acciarri M
- Achard P
- Adriani O
- Aguilar-Benitez M
- Alcaraz J
- Alemanni G
- Allaby J
- Aloisio A
- Alviggi MG
- Ambrosi G
- Anderhub H
- Andreev VP
- Angelescu T
- Anselmo F
- Arefiev A
- Azemoon T
- Aziz T
- Bagnaia P
- Baksay L
- Balandras A
- Ball RC
- Banerjee S
- Banerjee S
- Barczyk A
- Barillere R
- Barone L
- Bartalini P
- Basile M
- Battiston R
- Bay A
- Becattini F
- Becker U
- Behner F
- Bellucci L
- Berdugo J
- Berges P
- Bertucci B
- Betev BL
- Bhattacharya S
- Biasini M
- Biland A
- Blaising JJ
- Blyth SC
- Bobbink GJ
- Bohm A
- Boldizsar L
- Borgia B
- Bourilkov D
- Bourquin M
- Bourquin M
- Braccini S
- Braccini S
- Branson JG
- Branson JG
- Brigljevic V
- Brigljevic V
- Brochu F
- Brochu F
- Buffini A
- Buijs A
- Burger JD
- Burger WJ
- Busenitz J
- Button A
- Cai XD
- Campanelli M
- Capell M
- Carlino G
- Cartacci AM
- Casaus J
- Castellini G
- Cavallari F
- Cavallo N
- Cecchi C
- Cerrada M
- Cesaroni F
- Chamizo M
- Chang YH
- Chaturvedi UK
- Chemarin M
- Chen A
- Chen G
- Chen GM
- Chen HF
- Chen HS
- Chereau X
- Chiefari G
- Cifarelli L
- Cindolo F
- Civinini C
- Clare I
- Clare R
- Coignet G
- Colijn AP
- Colino N
- Costantini S
- Cotorobai F
- Cozzoni B
- Csilling A
- Cucciarelli S
- D'Alessandro R
- Dai TS
- de Asmundis R
- de Guevara PL
- de Jong P
- de la Cruz B
- De Notaristefani F
- De Salvo A
- Deglon P
- Degre A
- Deiters K
- della Volpe D
- Denes P
- Di Lodovico F
- Diemoz M
- Dionisi C
- Dittmar M
- Dominguez A
- Doria A
- Dova MT
- Duchesneau D
- Dufournaud D
- Duinker P
- Duran I
- El Mamouni H
- Engler A
- Eppling FJ
- Erne FC
- Extermann P
- Fabre M
- Faccini R
- Falagan MA
- Falciano S
- Favara A
- Fay J
- Fedin O
- Felcini M
- Ferguson T
- Ferroni F
- Fesefeldt H
- Fiandrini E
- Field JH
- Filthaut F
- Fisher PH
- Fisk I
- Forconi G
- Fredj L
- Freudenreich K
- Furetta C
- Galaktionov Y
- Ganguli SN
- Garcia-Abia P
- Gataullin M
- Gau SS
- Gentile S
- Gheordanescu N
- Giagu S
- Gong ZF
- Grenier G
- Grimm O
- Gruenewald MW
- Guida M
- Gupta VK
- Gurtu A
- Gutay LJ
- Haas D
- Hasan A
- Hatzifotiadou D
- Hebbeker T
- Herve A
- Hidas P
- Hirschfelder J
- Hofer H
- Holzner G
- Hoorani H
- Hou SR
- Iashvili I
- Jin BN
- Jones LW
- Josa-Mutuberria I
- Kamrad D
- Kaur M
- Khan RA
- Kienzle-Focacci MN
- Kim D
- Kim DH
- Kim JK
- Kim SC
- Kirkby J
- Kiss D
- Kittel W
- Klimentov A
- Konig AC
- Kopp A
- Korolko I
- Koutsenko V
- Kraber M
- Kraemer RW
- Krenz W
- Kunin A
- Laktineh I
- Landi G
- Lassila-Perini K
- Laurikainen P
- Lavorato A
- Le Coultre P
- Le Goff JM
- Lebeau M
- Lebedev A
- Lebrun P
- Lecomte P
- Lecoq P
- Lee HJ
- Leiste R
- Leonardi E
- Levtchenko P
- Li C
- Lin CH
- Lin WT
- Linde FL
- Lista L
- Liu ZA
- Lohmann W
- Longo E
- Lu YS
- Lubelsmeyer K
- Luci C
- Luckey D
- Lugnier L
- Luminari L
- Lustermann W
- Ma WG
- Maity M
- Malgeri L
- Malinin A
- Mana C
- Mangeol D
- Marchesini P
- Marian G
- Martin JP
- Marzano F
- Massaro GGG
- Mazumdar K
- McNeil RR
- Mele S
- Merola L
- Meschini M
- Metzger WJ
- Mihul A
- Milcent H
- Mirabelli G
- Mnich J
- Mohanty GB
- Molnar P
- Monteleoni B
- Moulik T
- Muanza GS
- Muheim F
- Muijs AJM
- Musy M
- Napolitano M
- Nessi-Tedaldi F
- Newman H
- Niessen T
- Nisati A
- Nowak H
- Oh YD
- Organtini G
- Ostonen R
- Palomares C
- Pandoulas D
- Paoletti S
- Paolucci P
- Paramatti R
- Park HK
- Park IH
- Pascale G
- Passaleva G
- Patricelli S
- Paul T
- Pauluzzi M
- Paus C
- Pauss F
- Peach D
- Pedace M
- Pensotti S
- Perret-Gallix D
- Petersen B
- Piccolo D
- Pierella F
- Pieri M
- Piroue PA
- Pistolesi E
- Plyaskin V
- Pohl M
- Pojidaev V
- Postema H
- Pothier J
- Produit N
- Prokofiev D
- Prokofiev DO
- Quartieri J
- Rahal-Callot G
- Rahaman MA
- Raics P
- Raja N
- Ramelli R
- Rancoita PG
- Raven G
- Razis P
- Ren D
- Rescigno M
- Reucroft S
- Riemann S
- Riles K
- Robohm A
- Rodin J
- Roe BP
- Romeo GC
- Romero L
- Rosca A
- Rosier-Lees S
- Rubio JA
- Ruschmeier D
- Rykaczewski H
- Salicio J
- Sanchez E
- Sanders MP
- Sarakinos ME
- Sarkar S
- Schafer C
- Schegelsky V
- Schmidt-Kaerst S
- Schmitz D
- Schopper H
- Schotanus DJ
- Schwering G
- Sciacca C
- Scianrino D
- Seganti A
- Servoli L
- Shevchenko S
- Shivarov N
- Shoutko V
- Shumilov E
- Shvorob A
- Siedenburg T
- Smith B
- Son D
- Spillantini P
- Steuer M
- Stickland DP
- Stone A
- Stone H
- Stoyanov B
- Straessner A
- Sudhakar K
- Sultanov G
- Sun LZ
- Suter H
- Swain JD
- Szillasi Z
- Sztaricskai T
- Tang XW
- Tauscher L
- Taylor L
- Timmermans C
- Ting SCC
- Ting SM
- Tonwar SC
- Toth J
- Tully C
- Tung KL
- Uchida Y
- Ulbricht J
- Valente E
- van Dalen JA
- van Dierendonck D
- van Gulik R
- van Rhee T
- Vesztergombi G
- Vetlitsky I
- Vicinanza D
- Viertel G
- Villa S
- Vivargent M
- Vlachos S
- Vodopianov I
- Vogel H
- Vogt H
- von der Mey M
- Vorobiev I
- Vorobyov AA
- Vorvolakos A
- Wadhwa M
- Wallraff W
- Wang M
- Wang XL
- Wang ZM
- Weber A
- Weber M
- Wienemann P
- Wilkens H
- Wu SX
- Wynhoff S
- Xia L
- Xu ZZ
- Yang BZ
- Yang CG
- Yang HJ
- Yang M
- Ye JB
- Yeh SC
- Zalite A
- Zalite Y
- Zhang ZP
- Zhu GY
- Zhu RY
- Zichichi A
- Ziegler F
- Zilizi G
- Zoller M
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1999
- Field of study
A search for pair-produced charged Higgs bosons is performed with the L3
detector at LEP using data collected at a centre-of-mass energy of 188.6 GeV,
corresponding to an integrated luminosity of 176.4 pb^-1. Higgs decays into a
charm and a strange quark or into a tau lepton and its associated neutrino are
considered. The observed events are consistent with the expectations from
Standard Model background processes. A lower limit of 65.5 GeV on the charged
Higgs mass is derived at 95 % confidence level, independent of the decay
branching ratio Br(H^{+/-} -> tau nu)
Measurement of CP-violation asymmetries in D0 to Ks pi+ pi-
- Author
- Aaltonen T
- Ahmed S
- Alam MS
- Albert J
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Azzolini V
- Badgett W
- Bae T
- Band HR
- Banerjee S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bedeschi F
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Bhuyan B
- Bianchi F
- Bisello D
- Bizjak I
- Bland KR
- Blumenfeld B
- Bocci A
- Bodek A
- Bomben M
- Bortoletto D
- Bosisio L
- Boudreau J
- Boveia A
- Brigliadori L
- Bromberg C
- Brucken E
- Budagov J
- Budd HS
- Bula R
- Burchat PR
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Calamba A
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Cartaro C
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chen X
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chung WH
- Chung YS
- Ciocci MA
- Clark A
- Clarke C
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cossutti F
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dasu S
- Datta M
- de Barbaro P
- Dell'Orso M
- Della Ricca G
- Demortier L
- Deninno M
- Devoto F
- Di Canto A
- Di Ruzza B
- Dittmann JR
- Donati S
- Dong P
- Dorigo M
- Dorigo T
- Ebina K
- Eckmann R
- Edwards AJ
- Elagin A
- Eppig A
- Erbacher R
- Ernst JA
- Errede S
- Ershaidat N
- Eusebi R
- Farrington S
- Feindt M
- Fernandez JP
- Fernandez PM
- Field R
- Flanagan G
- Flood KT
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Funakoshi Y
- Furic I
- Gallinaro M
- Gallo F
- Gamba D
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerchtein E
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Ginsburg CM
- Giokaris N
- Giromini P
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldin D
- Goldschmidt N
- Golossanov A
- Gomez G
- Gomez-Ceballos G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Grinstein S
- Griso SP
- Grosso-Pilcher C
- Group RC
- Hahn SR
- Halkiadakis E
- Hamaguchi A
- Hamano K
- Han JY
- Happacher F
- Hara K
- Hare D
- Hare M
- Harr RF
- Harrison PF
- Hatakeyama K
- Hays C
- Heck M
- Heinrich J
- Herndon M
- Hewamanage S
- Hocker A
- Hollar JJ
- Hopkins W
- Horn D
- Hou S
- Hughes RE
- Hurwitz M
- Husemann U
- Hussain N
- Hussein M
- Huston J
- Ilic J
- Introzzi G
- Iori M
- Ivanov A
- Izen JM
- Jain V
- James E
- Jang D
- Jayatilaka B
- Jeon EJ
- Jindariani S
- Jones M
- Joo KK
- Jun SY
- Junk TR
- Kamon T
- Karchin PE
- Kasmi A
- Kato Y
- Ketchum W
- Keung J
- Khotilovich V
- Kilminster B
- Kim DH
- Kim HS
- Kim JE
- Kim MJ
- Kim P
- Kim SB
- Kim SH
- Kim YJ
- Kim YK
- Kimura N
- Kirby M
- Klimenko S
- Knoepfel K
- Kocian ML
- Kondo K
- Kong DJ
- Konigsberg J
- Kotwal AV
- Kowalewski R
- Kreps M
- Krishnamurthy M
- Kroll J
- Krop D
- Kruse M
- Krutelyov V
- Kuhr T
- Kurata M
- Kutter PE
- Kwang S
- Laasanen AT
- Lami S
- Lammel S
- Lancaster M
- Lanceri L
- Lander RL
- Lannon K
- Lath A
- Latham TE
- Latino G
- LeCompte T
- Lee E
- Lee HS
- Lee JS
- Lee SW
- Leith DWGS
- Leo S
- Leone S
- Lewis JD
- Li S
- Limosani A
- Lin CJ
- Lindgren M
- Lipeles E
- Lister A
- Litvintsev DO
- Liu C
- Liu H
- Liu Q
- Liu T
- Lockwitz S
- Loginov A
- Lopez-March N
- Lou XC
- Lucchesi D
- Lueck J
- Luitz S
- Lujan P
- Lukens P
- Lungu G
- Luth V
- Lynch HL
- Lys J
- Lysak R
- MacFarlane DB
- Madrak R
- Maeshima K
- Maestro P
- Majewski SA
- Malik S
- Manca G
- Manousakis-Katsikakis A
- Margaroli F
- Marino C
- Marsiske H
- Martinez M
- Martinez-Vidal F
- Mastrandrea P
- Matera K
- Mattson ME
- Mazzacane A
- Mazzanti P
- McFarland KS
- McIntyre P
- McNulty R
- Mehta A
- Mehtala P
- Mesropian C
- Messner R
- Miao T
- Mietlicki D
- Milanes DA
- Mitra A
- Miyake H
- Miyashita TS
- Moed S
- Moggi N
- Mohanty GB
- Mondragon MN
- Moon CS
- Moore R
- Morello MJ
- Morlock J
- Mukherjee A
- Muller DR
- Muller T
- Murat P
- Mussini M
- Nachtman J
- Nagai Y
- Naganoma J
- Nakano I
- Napier A
- Neal H
- Nett J
- Neu C
- Neubauer MS
- Nielsen J
- Nodulman L
- Noh SY
- Norniella O
- Nugent IM
- O'Grady CP
- Oakes L
- Ofte I
- Oh SH
- Oh YD
- Oksuzian I
- Okusawa T
- Orava R
- Ortolan L
- Oyanguren A
- Pagliarone C
- Palencia E
- Pan B
- Pan Y
- Papadimitriou V
- Paramonov AA
- Patrick J
- Pauletta G
- Paulini M
- Paus C
- Pellett DE
- Pelliccioni M
- Penzo A
- Perazzo A
- Perl M
- Petersen BA
- Phillips TJ
- Piacentino G
- Pianori E
- Pierini M
- Pilot J
- Pitts K
- Plager C
- Pondrom L
- Poprocki S
- Potamianos K
- Pranko A
- Prepost R
- Prokoshin F
- Ptohos F
- Pulliam T
- Punzi G
- Rahaman A
- Ramakrishnan V
- Ranjan N
- Ratcliff BN
- Redondo I
- Renton P
- Rescigno M
- Riddick T
- Rimondi F
- Ristori L
- Ritchie JL
- Robson A
- Rodrigo T
- Rodriguez T
- Rogers E
- Rolli S
- Roney JM
- Roodman A
- Roser R
- Ruffini F
- Ruiz A
- Ruland AM
- Russ J
- Rusu V
- Saeed MA
- Safonov A
- Sakumoto WK
- Sakurai Y
- Salnikov AA
- Santi L
- Sato K
- Saveliev V
- Savoy-Navarro A
- Schilling CJ
- Schindler RH
- Schlabach P
- Schmidt A
- Schmidt EE
- Schwarz T
- Schwiening J
- Schwitters RF
- Scodellaro L
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- Wisniewski WJ
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- Yang YC
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- Yarritu AK
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- Yeh GP
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- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Zain SB
- Zanetti A
- Zeng Y
- Zhou C
- Ziegler V
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of time-integrated CP-violation asymmetries in the
resonant substructure of the three-body decay D0 to Ks pi+ pi- using CDF II
data corresponding to 6.0 invfb of integrated luminosity from Tevatron ppbar
collisions at sqrt(s) = 1.96 TeV. The charm mesons used in this analysis come
from D*+(2010) to D0 pi+ and D*-(2010) to D0bar pi-, where the production
flavor of the charm meson is determined by the charge of the accompanying pion.
We apply a Dalitz-amplitude analysis for the description of the dynamic decay
structure and use two complementary approaches, namely a full Dalitz-plot fit
employing the isobar model for the contributing resonances and a
model-independent bin-by-bin comparison of the D0 and D0bar Dalitz plots. We
find no CP-violation effects and measure an asymmetry of ACP = (-0.05 +- 0.57
(stat) +- 0.54 (syst))% for the overall integrated CP-violation asymmetry,
consistent with the standard model prediction.Comment: 15 page
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
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- Abbott B
- Abbott DC
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- Abhayasinghe DK
- Abidi SH
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- Zhemchugov A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Zaidan R
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- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Abdallah J
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- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Can Research Assessments Themselves Cause Bias in Behaviour Change Trials? A Systematic Review of Evidence from Solomon 4-Group Studies
- Author
- AD Lopez
- Antje Timmer
- AP Braeken
- B Traeen
- CJ Cherpitel
- Diana Elbourne
- DJ del Junco
- DM Lawson
- DM Mungas
- DP French
- DT Campbell
- E Nuesch
- EJ Duryea
- EM van Sluijs
- G Godin
- GD Freeman
- I Kirsch
- I Kirsch
- IL Kvalem
- J McCambridge
- J McCambridge
- J McCambridge
- J McCambridge
- JB Daeppen
- JC Coyne
- JC Spence
- Jim McCambridge
- John Witton
- JT Shope
- K Kypri
- K Kypri
- Kaanan Butor-Bhavsar
- KB Carey
- M Dignan
- MB Dignan
- MC Fox
- MCW Braver
- PC Campanelli
- PR Clifford
- PR Clifford
- R McCarney
- RE Kraut
- RL Solomon
- SA Clemes
- SL Lusk
- ST Walters
- T Sandberg
- TJ Kaptchuk
- VL Willson
- Publication venue
- Public Library of Science
- Publication date
- 19/10/2011
- Field of study
BACKGROUND: The possible effects of research assessments on participant behaviour have attracted research interest, especially in studies with behavioural interventions and/or outcomes. Assessments may introduce bias in randomised controlled trials by altering receptivity to intervention in experimental groups and differentially impacting on the behaviour of control groups. In a Solomon 4-group design, participants are randomly allocated to one of four arms: (1) assessed experimental group; (2) unassessed experimental group (3) assessed control group; or (4) unassessed control group. This design provides a test of the internal validity of effect sizes obtained in conventional two-group trials by controlling for the effects of baseline assessment, and assessing interactions between the intervention and baseline assessment. The aim of this systematic review is to evaluate evidence from Solomon 4-group studies with behavioural outcomes that baseline research assessments themselves can introduce bias into trials. METHODOLOGY/PRINCIPAL FINDINGS: Electronic databases were searched, supplemented by citation searching. Studies were eligible if they reported appropriately analysed results in peer-reviewed journals and used Solomon 4-group designs in non-laboratory settings with behavioural outcome measures and sample sizes of 20 per group or greater. Ten studies from a range of applied areas were included. There was inconsistent evidence of main effects of assessment, sparse evidence of interactions with behavioural interventions, and a lack of convincing data in relation to the research question for this review. CONCLUSIONS/SIGNIFICANCE: There were too few high quality completed studies to infer conclusively that biases stemming from baseline research assessments do or do not exist. There is, therefore a need for new rigorous Solomon 4-group studies that are purposively designed to evaluate the potential for research assessments to cause bias in behaviour change trials
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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- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
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