1,557 research outputs found
Viral Agents Causing Brown Cap Mushroom Disease of Agaricus bisporus
- Author
- Publication venue
- 'American Society for Microbiology'
- Publication date
- 07/08/2015
- Field of study
SMARTPOP: Inferring the impact of social dynamics on genetic diversity through high speed simulations
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
Background: Social behavior has long been known to influence patterns of genetic diversity, but the effect of social processes on population genetics remains poorly quantified - partly due to limited community-level genetic sampling (which is increasingly being remedied), and partly to a lack of fast simulation software to jointly model genetic evolution and complex social behavior, such as marriage rules.Results: To fill this gap, we have developed SMARTPOP - a fast, forward-in-time genetic simulator - to facilitate large-scale statistical inference on interactions between social factors, such as mating systems, and population genetic diversity. By simultaneously modeling genetic inheritance and dynamic social processes at the level of the individual, SMARTPOP can simulate a wide range of genetic systems (autosomal, X-linked, Y chromosomal and mitochondrial DNA) under a range of mating systems and demographic models. Specifically designed to enable resource-intensive statistical inference tasks, such as Approximate Bayesian Computation, SMARTPOP has been coded in C++ and is heavily optimized for speed and reduced memory usage.Conclusion: SMARTPOP rapidly simulates population genetic data under a wide range of demographic scenarios and social behaviors, thus allowing quantitative analyses to address complex socio-ecological questions. Š 2014 Guillot and Cox; licensee BioMed Central Ltd
Measurement of the top quark mass using the matrix element technique in dilepton final states
- Author
- Abazov VM
- Abbott B
- Acharya BS
- Adams M
- Adams T
- Agnew JP
- Alexeev GD
- Alkhazov G
- Alton A
- Askew A
- Atkins S
- Augsten K
- Aushev V
- Aushev Y
- Avila C
- Badaud F
- Bagby L
- Baldin B
- Bandurin DV
- Banerjee S
- Barberis E
- Baringer P
- Bartlett JF
- Bassler U
- Bazterra V
- Bean A
- Begalli M
- Bellantoni L
- Beri SB
- Bernardi G
- Bernhard R
- Bertram I
- Besancon M
- Beuselinck R
- Bhat PC
- Bhatia S
- Bhatnagar V
- Blazey G
- Blessing S
- Bloom K
- Boehnlein A
- Boline D
- Boos EE
- Borissov G
- Borysova M
- Brandt A
- Brandt O
- Brochmann M
- Brock R
- Bross A
- Brown D
- Bu XB
- Buehler M
- Buescher V
- Bunichev V
- Burdin S
- Buszello CP
- Camacho-Perez E
- Casey BCK
- Castilla-Valdez H
- Caughron S
- Chakrabarti S
- Chan KM
- Chandra A
- Chapon E
- Chen G
- Cho SW
- Choi S
- Choudhary B
- Cihangir S
- Claes D
- Clutter J
- Collaboration D0
- Cooke M
- Cooper WE
- Corcoran M
- Couderc F
- Cousinou M-C
- Cuth J
- Cutts D
- Das A
- Davies G
- de Jong SJ
- De La Cruz-Burelo E
- de Sa R Lopes
- Deliot F
- Demina R
- Denisov D
- Denisov SP
- Desai S
- Deterre C
- DeVaughan K
- Diehl HT
- Diesburg M
- Ding PF
- Dominguez A
- Dubey A
- Dudko LV
- Duperrin A
- Dutt S
- Eads M
- Edmunds D
- Ellison J
- Elvira VD
- Enari Y
- Evans H
- Evdokimov A
- Evdokimov VN
- Faure A
- Feng L
- Ferbel T
- Fiedler F
- Filthaut F
- Fisher W
- Fisk HE
- Fortner M
- Fox H
- Franc J
- Fuess S
- Garbincius PH
- Garcia-Bellido A
- Garcia-Gonzalez JA
- Gavrilov V
- Geng W
- Gerber CE
- Gershtein Y
- Ginther G
- Gogota O
- Golovanov G
- Grannis PD
- Greder S
- Greenlee H
- Grenier G
- Gris Ph
- Grivaz J-F
- Grohsjean A
- Grunendahl S
- Grunewald MW
- Guillemin T
- Gutierrez G
- Gutierrez P
- Haley J
- Han L
- Harder K
- Harel A
- Hauptman JM
- Hays J
- Head T
- Hebbeker T
- Hedin D
- Hegab H
- Heinson AP
- Heintz U
- Hensel C
- Heredia-De La Cruz I
- Herner K
- Hesketh G
- Hildreth MD
- Hirosky R
- Hoang T
- Hobbs JD
- Hoeneisen B
- Hogan J
- Hohlfeld M
- Holzbauer JL
- Howley I
- Hubacek Z
- Hynek V
- Iashvili I
- Ilchenko Y
- Illingworth R
- Ito AS
- Jabeen S
- Jaffre M
- Jayasinghe A
- Jeong MS
- Jesik R
- Jiang P
- Johns K
- Johnson E
- Johnson M
- Jonckheere A
- Jonsson P
- Joshi J
- Jung AW
- Juste A
- Kajfasz E
- Karmanov D
- Katsanos I
- Kaur M
- Kehoe R
- Kermiche S
- Khalatyan N
- Khanov A
- Kharchilava A
- Kharzheev YN
- Kiselevich I
- Kohli JM
- Kozelov AV
- Kraus J
- Kumar A
- Kupco A
- Kurca T
- Kuzmin VA
- Lammers S
- Lebrun P
- Lee HS
- Lee SW
- Lee WM
- Lei X
- Lellouch J
- Li D
- Li H
- Li L
- Li QZ
- Lim JK
- Lincoln D
- Linnemann J
- Lipaev VV
- Lipton R
- Liu H
- Liu Y
- Lobodenko A
- Lokajicek M
- Luna-Garcia R
- Lyon AL
- Maciel AKA
- Madar R
- Magana-Villalba R
- Malik S
- Malyshev VL
- Mansour J
- Martinez-Ortega J
- McCarthy R
- McGivern CL
- Meijer MM
- Melnitchouk A
- Menezes D
- Mercadante PG
- Merkin M
- Meyer A
- Meyer J
- Miconi F
- Mondal NK
- Mulhearn M
- Nagy E
- Narain M
- Nayyar R
- Neal HA
- Negret JP
- Neustroev P
- Nguyen HT
- Nunnemann T
- Orduna J
- Osman N
- Pal A
- Parashar N
- Parihar V
- Park SK
- Partridge R
- Parua N
- Patwa A
- Penning B
- Perfilov M
- Peters Y
- Petridis K
- Petrillo G
- Petroff P
- Pleier M-A
- Podstavkov VM
- Popov AV
- Prewitt M
- Price D
- Prokopenko N
- Qian J
- Quadt A
- Quinn B
- Ratoff PN
- Razumov I
- Ripp-Baudot I
- Rizatdinova F
- Rominsky M
- Ross A
- Royon C
- Rubinov P
- Ruchti R
- Sajot G
- Sanchez-Hernandez A
- Sanders MP
- Santos AS
- Savage G
- Savitskyi M
- Sawyer L
- Scanlon T
- Schamberger RD
- Scheglov Y
- Schellman H
- Schott M
- Schwanenberger C
- Schwienhorst R
- Sekaric J
- Severini H
- Shabalina E
- Shary V
- Shaw S
- Shchukin AA
- Simak V
- Skubic P
- Slattery P
- Snow GR
- Snow J
- Snyder S
- Soldner-Rembold S
- Sonnenschein L
- Soustruznik K
- Stark J
- Stefaniuk N
- Stoyanova DA
- Strauss M
- Suter L
- Svoisky P
- Titov M
- Tokmenin VV
- Tsai Y-T
- Tsybychev D
- Tuchming B
- Tully C
- Uvarov L
- Uvarov S
- Uzunyan S
- Van Kooten R
- van Leeuwen WM
- Varelas N
- Varnes EW
- Vasilyev IA
- Verkheev AY
- Vertogradov LS
- Verzocchi M
- Vesterinen M
- Vilanova D
- Vokac P
- Wahl HD
- Wang MHLS
- Warchol J
- Watts G
- Wayne M
- Weichert J
- Welty-Rieger L
- Williams MRJ
- Wilson GW
- Wobisch M
- Wood DR
- Wyatt TR
- Xie Y
- Yamada R
- Yang S
- Yasuda T
- Yatsunenko YA
- Ye W
- Ye Z
- Yin H
- Yip K
- Youn SW
- Yu JM
- Zennamo J
- Zhao TG
- Zhou B
- Zhu J
- Zielinski M
- Zieminska D
- Zivkovic L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 10/06/2016
- Field of study
We present a measurement of the top quark mass in ppÂŻ collisions at a center-of-mass energy of 1.96 TeV at the Fermilab Tevatron collider. The data were collected by the D0 experiment corresponding to an integrated luminosity of 9.7ââfbâ1. The matrix element technique is applied to ttÂŻ events in the final state containing leptons (electrons or muons) with high transverse momenta and at least two jets. The calibration of the jet energy scale determined in the lepton+jets final state of ttÂŻ decays is applied to jet energies. This correction provides a substantial reduction in systematic uncertainties. We obtain a top quark mass of mt=173.93Âą1.84ââGeV
Anomalias craniofaciais: descrição e avaliação das caracterĂsticas gerais da atenção no Sistema Ănico de SaĂşde
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Standard values and relationship-specific validity of the Bielefeld Relationship Expectations Questionnaire (BFPE)
- Author
- A Hinz
- B Strauss
- C Hazan
- C Hinnen
- D HĂśger
- D HĂśger
- D HĂśger
- E Pollack
- EE Noftle
- Elmar Brähler
- EM Merz
- G Sommer
- G Sommer
- Gesine Grande
- Hendrik Berth
- J Bowlby
- J Fahrenberg
- J Schumacher
- JA Simpson
- JA Simpson
- JM Moreira
- K Hahlweg
- K Hahlweg
- KA Brennan
- KA Brennan
- Katja Petrowski
- L Campbell
- L Goldbeck
- L Grau
- L Marcus
- MCG Booher
- MDS Ainsworth
- NL Collins
- NL Collins
- RA Stackert
- RL Weiss
- SĂśren Paul
- T Fydrich
- T Fydrich
- T Fydrich
- Yve StĂśbel-Richter
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>The Bielefeld Partnership Expectations Questionnaire (BFPE) is a tool to assess attachment in the romantic relationships of adults. The attachment styles are operationalized as configuration patterns of scale scores. While convergent validity has already been investigated, discriminant validity is still lacking confirmation.</p> <p>Methods</p> <p>The present sample (n = 1509) is representative for the German population aged 18 to 50. The mean age was 34.6 years. Most of the participants lived in a relationship (77.3 %). Discriminant validity was analyzed using a marital quality questionnaire (PFB), a social support questionnaire (F-Soz-U K-14), and a life satisfaction questionnaire (FLZ).</p> <p>Results</p> <p>All the BFPE scales have a satisfying internal consistency between r = .79 and .86. Those individuals who showed a secure pattern, i.e. increased "Readiness for Self-Disclosure" and "Conscious Need for Care" as well as reduced "Fear of Rejection" experienced their partner as socially supportive, reported higher marital quality in all of its facets, and were more satisfied within the life-domains "family/children" and "relationship/sexuality". Standard values for each scale are presented.</p> <p>Conclusions</p> <p>The BFPE has repeatedly been verified as a short, reliable, and valid instrument applicable to research practice with healthy individuals as well as within clinical contexts.</p
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
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- LeCompte T
- LeCompte T
- Lee AM
- Lee J
- Lee J
- Lee K
- Lee SW
- Lee SW
- Lee WM
- Leflat A
- Lehner F
- Leonardo N
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- Leone S
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- Leonidopoulos C
- Lewis JD
- Lewis JD
- Li J
- Li K
- Li K
- Li QZ
- Lima JGR
- Lin CS
- Lin CS
- Lincoln D
- Lindgren M
- Lindgren M
- Linn SL
- Linnemann J
- Lipton R
- Liss TM
- Liss TM
- Litvintsev DO
- Litvintsev DO
- Liu JB
- Liu JB
- Liu T
- Liu T
- Liu YC
- Liu YC
- Lobban O
- Lockyer NS
- Lockyer NS
- Loginov A
- Loginov A
- Loken J
- Loken J
- Loreti M
- Loreti M
- Lucchesi D
- Lucchesi D
- Lueking L
- Lukens P
- Lukens P
- Lundstedt C
- Luo C
- Lusin S
- 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
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- 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
Observation of the Baryonic Flavor-Changing Neutral Current Decay Lambda_b -> Lambda mu+ mu-
- Author
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- Zucchelli Sones M.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report the first observation of the baryonic flavor-changing neutral
current decay Lambda_b -> Lambda mu+ mu- with 24 signal events and a
statistical significance of 5.8 Gaussian standard deviations. This measurement
uses ppbar collisions data sample corresponding to 6.8fb-1 at sqrt{s}=1.96TeV
collected by the CDF II detector at the Tevatron collider. The total and
differential branching ratios for Lambda_b -> Lambda mu+ mu- are measured. We
find B(Lambda_b -> Lambda mu+ mu-) = [1.73+-0.42(stat)+-0.55(syst)] x 10^{-6}.
We also report the first measurement of the differential branching ratio of B_s
-> phi mu+ mu- using 49 signal events. In addition, we report branching ratios
for B+ -> K+ mu+ mu-, B0 -> K0 mu+ mu-, and B -> K*(892) mu+ mu- decays.Comment: 8 pages, 2 figures, 4 tables. Submitted to Phys. Rev. Let
Measurement of the average time-integrated mixing probability of b-flavored hadrons produced at the Tevatron
- Author
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- Yagil A
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- Yang UK
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- Yao W
- Yao W
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- Yeh GP
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- Yi K
- Yoh J
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- Yoon P
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- Yosef C
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- Yun JC
- Yun JC
- Zanello L
- Zanello L
- Zanetti A
- Zanetti A
- Zaw I
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- 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.
Search for the standard model Higgs boson at LEP
- Author
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- Abbaneo D
- Abbiendi G
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- Abdallah J
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- Wyatt TR
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- Yamamoto J
- Yamashita S
- Yang BZ
- Yang CG
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- Zachariadou K
- Zalewska A
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- Zavrtanik D
- Zeitnitz C
- Zer-Zion D
- Zhang J
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- Zhu GY
- Zhu RY
- Zhuang HL
- Zhuravlov V
- Zichichi A
- Ziegler T
- Zilizi G
- Zimin NI
- Zimmermann B
- Zintchenko A
- Zito G
- Zivkovic L
- Zobernig G
- Zoller M
- Zupan M
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
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
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- 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
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