343 research outputs found
Flavour Physics and CP Violation in the Standard Model and Beyond
- Author
- Publication venue
- Publication date
- 18/02/2014
- Field of study
We present the invited lectures given at the Third IDPASC School which took
place in Santiago de Compostela in January 2013. The students attending the
school had very different backgrounds, some of them were doing their Ph.D. in
experimental particle physics, others in theory. As a result, and in order to
make the lectures useful for most of the students, we focused on basic topics
of broad interest, avoiding the more technical aspects of Flavour Physics and
CP Violation. We make a brief review of the Standard Model, paying special
attention to the generation of fermion masses and mixing, as well as to CP
violation. We describe some of the simplest extensions of the SM, emphasising
novel flavour aspects which arise in their framework.Comment: Invited talk at the Third IDPASC School 2013, January 21st - February
2nd 2013, Santiago de Compostela, Galiza, Spain; 36 pages, 8 figures, 2
tables; version with few misprints correcte
Leptogenesis in the presence of exact flavor symmetries
- Author
- AD Sakharov
- C Froggatt
- C Hagedorn
- D Aristizabal Sierra
- D Aristizabal Sierra
- D Aristizabal Sierra
- D Aristizabal Sierra
- D Aristizabal Sierra
- D. Aristizabal Sierra
- E Bertuzzo
- E Nardi
- EE Jenkins
- F Bazzocchi
- F-X Josse-Michaux
- Federica Bazzocchi
- G Altarelli
- G Altarelli
- G Giudice
- G Hinshaw
- GC Branco
- I Medeiros Varzielas de
- J Schechter
- J Schechter
- L Covi
- P Minkowski
- R Felipe
- RN Mohapatra
- S Davidson
- SL Glashow
- T Schwetz
- W Buchmüller
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2012
- Field of study
In models with flavor symmetries in the leptonic sector leptogenesis can take
place in a very different way compared to the standard leptogenesis scenario.
We study the generation of a B−L asymmetry in these kind of models in the
flavor symmetric phase pointing out that successful leptogenesis requires (i)
the right-handed neutrinos to lie in different representations of the flavor
group; (ii) the flavons to be lighter at least that one of the right-handed
neutrino representations. When these conditions are satisfied leptogenesis
proceeds due to new contributions to the CP violating asymmetry and -depending
on the specific model- in several stages. We demonstrate the validity of these
arguments by studying in detail the generation of the B−L asymmetry in a
scenario of a concrete A4 flavor model realization.Comment: 25 pages, 7 figures; version 2: A few clarifications added. Version
matches publication in JHE
Implications of Flavor Dynamics for Fermion Triplet Leptogenesis
- Author
- A Abada
- A Abada
- A Arhrib
- A Ibarra
- A Pilaftsis
- A Pilaftsis
- A Strumia
- AD Dolgov
- AD Sakharov
- B Bajc
- B Bajc
- C Wetterich
- Diego Aristizabal Sierra
- E Nardi
- E Nardi
- E Nardi
- F Aguila del
- G Engelhard
- G Hinshaw
- G Lazarides
- GF Giudice
- J Schechter
- J-M Frere
- JA Casas
- JA Harvey
- Jernej F. Kamenik
- JF Kamenik
- L Covi
- M Fukugita
- M Gell-Mann
- Miha Nemevšek
- O Vives
- P Bari Di
- P Minkowski
- R Barbieri
- R Foot
- R Franceschini
- RN Mohapatra
- RN Mohapatra
- S Antusch
- S Antusch
- S Blanchet
- S Blanchet
- S Davidson
- SL Glashow
- T Hambye
- T Hambye
- T Schwetz
- T Yanagida
- VA Kuzmin
- W Fischler
- Y Burnier
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/10/2010
- Field of study
We analyze the importance of flavor effects in models in which leptogenesis
proceeds via the decay of Majorana electroweak triplets. We find that depending
on the relative strengths of gauge and Yukawa reactions the B−L asymmetry can
be sizably enhanced, exceeding in some cases an order of magnitude level. We
also discuss the impact that such effects can have for TeV-scale triplets
showing that as long as the B−L asymmetry is produced by the dynamics of the
lightest such triplet they are negligible, but open the possibility for
scenarios in which the asymmetry is generated above the TeV scale by heavier
states, possibly surviving the TeV triplet related washouts. We investigate
these cases and show how they can be disentangled at the LHC by using Majorana
triplet collider observables and, in the case of minimal type III see-saw
models even through lepton flavor violation observables.Comment: 22 pages, 9 figures, extended discussion on collider phenomenology,
references added. Version matches publication in JHE
Phenomenological discriminations of the Yukawa interactions in two-Higgs doublet models with Z2 Z 2 symmetry
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
The C2HDM revisited
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
The complex two-Higgs doublet model is one of the simplest ways to extend the
scalar sector of the Standard Model to include a new source of CP-violation.
The model has been used as a benchmark model to search for CP-violation at the
LHC and as a possible explanation for the matter-antimatter asymmetry of the
Universe. In this work, we re-analyse in full detail the softly broken
Z2 symmetric complex two-Higgs doublet model (C2HDM). We provide
the code C2HDM_HDECAY implementing the C2HDM in the well-known HDECAY program
which calculates the decay widths including the state-of-the-art higher order
QCD corrections and the relevant off-shell decays. Using C2HDM_HDECAY together
with the most relevant theoretical and experimental constraints, including
electric dipole moments (EDMs), we review the parameter space of the model and
discuss its phenomenology. In particular, we find cases where large CP-odd
couplings to fermions are still allowed and provide benchmark points for these
scenarios. We examine the prospects of discovering CP-violation at the LHC and
show how theoretically motivated measures of CP-violation correlate with
observables.The work of D.F., J.C.R. and J.P.S. is supported in part by the Portuguese Fundacao para a Ciencia e Tecnologia (FCT) under contracts CERN/FIS-NUC/0010/2015 and UID/FIS/00777/2013. MM acknowledges financial support from the DFG project "Precision Calculations in the Higgs Sector - Paving the Way to the New Physics Landscape" (ID: MU 3138/1-1).info:eu-repo/semantics/publishedVersio
Introduction of a new model for time-continuous and non-contact investigations of in-vitro thrombolysis under physiological flow conditions
- Author
- A Blinc
- A Soltani
- AV Alexandrov
- AV Alexandrov
- CA Molina
- CG Lauer
- ChK Holland
- D Harpaz
- D Kwan
- D Paparella
- DV Sakharov
- F Perren
- FC Roessler
- Florian C Roessler
- Florian Stellmacher
- G Tsivgoulis
- Günter Seidel
- I Serša
- J Eggers
- J Eggers
- Jan H Marxsen
- Jürgen Eggers
- K Grabska
- K Mizushige
- LH Edmunds Jr
- M Nedelmann
- Marc Schmieger
- Marcus Ohlrich
- MT Wunderlich
- Peter Trillenberg
- Peter-Karl Weber
- R Aaslid
- RK Greenberg
- S Behrens
- S Behrens
- SB Olsson
- SL Diamond
- St Pfaffenberger
- T Holscher
- U Rosenschein
- V Frenkel
- V Suchkova
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Thrombolysis is a dynamic and time-dependent process influenced by the haemodynamic conditions. Currently there is no model that allows for time-continuous, non-contact measurements under physiological flow conditions. The aim of this work was to introduce such a model.</p> <p>Methods</p> <p>The model is based on a computer-controlled pump providing variable constant or pulsatile flows in a tube system filled with blood substitute. Clots can be fixed in a custom-built clot carrier within the tube system. The pressure decline at the clot carrier is measured as a novel way to measure lysis of the clot. With different experiments the hydrodynamic properties and reliability of the model were analyzed. Finally, the lysis rate of clots generated from human platelet rich plasma (PRP) was measured during a one hour combined application of diagnostic ultrasound (2 MHz, 0.179 W/cm<sup>2</sup>) and a thrombolytic agent (rt-PA) as it is commonly used for clinical sonothrombolysis treatments.</p> <p>Results</p> <p>All hydrodynamic parameters can be adjusted and measured with high accuracy. First experiments with sonothrombolysis demonstrated the feasibility of the model despite low lysis rates.</p> <p>Conclusions</p> <p>The model allows to adjust accurately all hydrodynamic parameters affecting thrombolysis under physiological flow conditions and for non-contact, time-continuous measurements. Low lysis rates of first sonothrombolysis experiments are primarily attributable to the high stability of the used PRP-clots.</p
Search for the standard model Higgs boson at LEP
- Author
- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbiendi G
- Abdallah J
- Abreu P
- Achard P
- Adam W
- Adriani O
- Adzic P
- Affholderbach K
- Aguilar-Benitez M
- Ainsley C
- Akesson PF
- Albrecht T
- Alcaraz J
- Alderweireld T
- Alemanni G
- Alemany-Fernandez R
- Alexander G
- Allaby J
- Allison J
- Allmendinger T
- Allport PP
- Aloisio A
- Alviggi MG
- Amaldi U
- Amapane N
- Amaral P
- Amato S
- Anagnostou G
- Anashkin E
- Anderhub H
- Anderson KJ
- Andreazza A
- Andreev VP
- Andringa S
- Anjos N
- Anselmo F
- Antilogus P
- Antonelli A
- Antonelli M
- Apel WD
- Arcelli S
- Arefiev A
- Armstrong SR
- Arnoud Y
- Asai S
- Ask S
- Asman B
- Augustin JE
- Augustinus A
- Awunor O
- Axen D
- Azemoon T
- Aziz T
- Azuelos G
- Azzurri P
- Baarmand M
- Badaud F
- Bagliesi G
- Bagnaia P
- Bailey I
- Baillon P
- Bajo A
- Baksay G
- Baksay L
- Baldew SV
- Ballestrero A
- Bambade P
- Banerjee S
- Banerjee S
- Barate R
- Barate R
- Barberio E
- Barbier R
- Barczyk A
- Bardin D
- Barillere R
- Barker G
- Barklow T
- Barlow RJ
- Baroncelli A
- Bartalini P
- Basile M
- Batalova N
- Batley RJ
- Battaglia M
- Battiston R
- Baubillier M
- Bay A
- Becattini F
- Bechtle P
- Becker U
- Becks KH
- Begalli M
- Behner F
- Behnke T
- Behrmann A
- Bell KW
- Bell PJ
- Bella G
- Bellerive A
- Bellucci L
- Ben-Haim E
- Bencivenni G
- Benekos N
- Benelli G
- Benvenuti A
- Berat C
- Berbeco R
- Berdugo J
- Berges P
- Berggren M
- Berkelman K
- Berntzon L
- Bertrand D
- Bertucci B
- Besancon M
- Besson N
- Betev BL
- Bethke S
- Beuselinck R
- Biasini M
- Biebell O
- Biglietti M
- Biland A
- Binnie DM
- Blair GA
- Blaising JJ
- Bloch D
- Bloch-Devaux B
- Blom M
- Blondel A
- Bloodworth IJ
- Bluj M
- Blumenschein U
- Blyth SC
- Bobbink GJ
- Boccali T
- Bock P
- Boeriun O
- Bohm A
- Bohrer A
- Boix G
- Boldizsar L
- Bologna G
- Bonacorsi D
- Bonesini M
- Bonissent A
- Boonekamp M
- Booth CN
- Booth PSL
- Borean C
- Borgia B
- Borisov G
- Bossi F
- Botner O
- Boucrot J
- Bouhova-Thacker E
- Boumediene D
- Bouquet B
- Bourilkov D
- Bourquin M
- Boutemeur M
- Bowcock TJV
- Bowdery CK
- Boyko I
- Braccini S
- Bracko M
- Braibant S
- Brandt S
- Branson JG
- Bravo S
- Brenner R
- Brient JC
- Brigliadori L
- Brochu F
- Brodet E
- Brown RM
- Bruckman P
- Bruneliere R
- Brunet JM
- Buchmuller O
- Buesser K
- Bugge L
- Buijs A
- Burckhart HJ
- Burger JD
- Burger WJ
- Buschmann P
- Cai XD
- Callot O
- Calvi M
- Cameron W
- Campana R
- Campana S
- Camporesi T
- Canale V
- Capell M
- Capon G
- Carena F
- Carlino G
- Carnegie RK
- Caron B
- Carr J
- Cartacci A
- Carter AA
- Carter JR
- Cartwright S
- Casado MP
- Casaus J
- Castro N
- Cattaneo A
- Cavallari F
- Cavallo F
- Cavallo N
- Cavanaugh R
- Cecchi C
- Cerrada M
- Cerutti F
- Chamizo M
- Chang CY
- Chang YH
- Chapkin M
- Charlton DG
- Charpentier P
- Checchia P
- Chemarin M
- Chen A
- Chen G
- Chen GM
- Chen HF
- Chen HS
- Chiarella V
- Chiefari G
- Chierici R
- Chiliapnikov P
- Chmeissani M
- Chudoba J
- Chung SU
- Cieslik K
- Cifarelli L
- Cindolo F
- Ciulli V
- Clare I
- Clare R
- Clarke DP
- Clerbaux B
- Clifft RW
- Coignet G
- Colaleo A
- Colas P
- Coles J
- Colino N
- Collins P
- Combley F
- Contri R
- Cosme G
- Cossutti F
- Costa MJ
- Costantini S
- Cowan G
- Coyle P
- Cranmer K
- Crawley B
- Creanza D
- Crennell D
- Crespo JM
- Csilling A
- Cucciarelli S
- Cuevas J
- Cuffiani M
- Curtil C
- D'Hondt J
- da Silva T
- Da Silva W
- Dado S
- Dai TS
- Dallavalle GM
- Dallison S
- Dalmau J
- David A
- Davier M
- Davies G
- De Angelis A
- de Asmundis R
- De Boer W
- De Bonis I
- De Clercq C
- De Filippis N
- de Guevara PL
- de Jong R
- de la Cruz B
- De Lotto B
- De Maria N
- De Min A
- de Palma M
- de Paula L
- De Roeck A
- De Salvo A
- De Vivie de Regie JB
- De Wolf EA
- Debreczeni J
- Decamp D
- Deglon P
- Degre A
- Deiters K
- Della Ricca G
- della Volpe D
- Delmeire E
- Denes P
- DeNotaristefani F
- Desch K
- Dessagne S
- Dhamotharan S
- Di Ciaccio L
- Di Simone A
- Diemoz M
- Dienes B
- Dierckxsens M
- Dietl H
- Dionisi C
- Dissertori G
- Dittmar M
- Donkers M
- Doria A
- Dornan PJ
- Doroba K
- Dova MT
- Drees J
- Drevermann H
- Dris M
- Dubbert J
- Duchesneau D
- Duchovni E
- Duckeck G
- Duerdoth IP
- Duflot L
- Duinker P
- Ealet A
- Echenard B
- Edgecock TR
- Eigen G
- Ekelof T
- El Mamouni H
- Elfgren E
- Eline A
- Ellert M
- Ellis G
- Elsing M
- Engler A
- Eppling FJ
- Etzion E
- Ewers A
- Extermann P
- Fabbri F
- Fabbro B
- Falagan MA
- Falciano S
- Falvard A
- Fanourakis G
- Fassouliotis D
- Favara A
- Fay J
- Fayolle D
- Fedin O
- Feindt M
- Felcini M
- Feld L
- Ferguson DPS
- Ferguson T
- Fernandez E
- Fernandez J
- Fernandez-Bosman M
- Ferrari P
- Ferrer A
- Ferro F
- Fesefeldt H
- Fiandrini E
- Fiedler F
- Field JH
- Filthaut F
- Finch AJ
- Fisher PH
- Fisher W
- Fisk I
- Flagmeyer U
- Fleck I
- Foa L
- Focardi E
- Foeth H
- Fokitis E
- Forconi G
- Ford M
- Forty RW
- Foster F
- Fouchez D
- Frank M
- Freudenreich K
- Frey A
- Fulda-Quenzer F
- Furetta C
- Furtjes A
- Fuster J
- Gagnon P
- Galaktionov Y
- Gandelman M
- Ganguli SN
- Ganis G
- Gao Y
- Garcia C
- Garcia-Abia P
- Garcia-Bellido A
- Garrido L
- Gary JW
- Gataullin M
- Gavillet P
- Gay P
- Gaycken G
- Gazis E
- Geich-Gimbel C
- Gentile S
- Geweniger C
- Ghete VM
- Giacomelli G
- Giacomelli P
- Giagu S
- Giammanco A
- Giannini G
- Gianotti F
- Giassi A
- Girone M
- Girtler P
- Giunta M
- Gokieli R
- Goldberg J
- Golob B
- Gomez-Ceballos G
- Goncalves P
- Gong ZF
- Gonzalez S
- Goy C
- Grauges E
- Graziani E
- Green MG
- Greening TC
- Grenier G
- Grimm O
- Grivaz JF
- Grosdidier G
- Gross E
- Gruenewald MW
- Grunhaus J
- Grupen C
- Gruwe M
- Grzelak K
- Guida M
- Gunther PO
- Gupta A
- Gupta VK
- Gurtu A
- Gutay LJ
- Guy J
- Haag C
- Haas D
- Hajdu C
- Hallgren A
- Hamacher K
- Hamann M
- Hamilton K
- Hanke P
- Hansen J
- Hansen JB
- Hansen JD
- Hansen JR
- Hansen PH
- Hanson GG
- Harder K
- Harel A
- Harin-Dirac M
- Harvey J
- Hatzifotiadou D
- Haug S
- Hauler F
- Hauschild M
- Hauschildt J
- Hawkes CM
- Hawkings R
- Hayes OJ
- He H
- Hebbeker T
- Hedberg V
- Heister A
- Hemingway RJ
- Henneche M
- Hensel C
- Hepp V
- Herr H
- Herten G
- Herve A
- Hess J
- Heuer RD
- Heusse P
- Hill JC
- Hill RD
- Hirschfelder J
- Hodgson PN
- Hofer H
- Hoffman J
- Hoffman K
- Holldorfer F
- Holmgren SO
- Holt PJ
- Holzner G
- Homer RJ
- Horvath D
- Hou SR
- Houlden MA
- Howard R
- Hu H
- Hu Y
- Huang X
- Hughes G
- Hultqvist K
- Huntemeyer P
- Hutchcroft DE
- Huttmann K
- Iaselli G
- Igo-Kemenes P
- Ishii K
- Jacholkowska A
- Jackson JN
- Jakobs K
- Janot P
- Jarlskog G
- Jarry P
- Jeans D
- Jeremie H
- Jezequel S
- Jin BN
- Jin S
- Johansson EK
- Johansson PD
- Jones LT
- Jones LW
- Jones RWL
- Jonsson P
- Joram C
- Josa-Mutuberria I
- Jost B
- Jousset J
- Jovanovic P
- Jungermann L
- Junk TR
- Kachelhoffer T
- Kado M
- Kafer D
- Kanaya N
- Kanzaki J
- Kapusta F
- Karapetian G
- Karlen D
- Kartvelishvili V
- Katsanevas S
- Katsoufis E
- Kaur M
- Kawagoe K
- Kawamoto T
- Kayser F
- Keeler RK
- Kellogg RG
- Kennedy BW
- Kennedy J
- Kernel G
- Kersevan BP
- Kienzle-Focacci MN
- Kiiskinen A
- Kile J
- Kim DH
- Kim JK
- King BT
- Kirkby J
- Kittel W
- Kjaer NJ
- Klein K
- Kleinknecht K
- Klier A
- Klimentov A
- Kluge EE
- Kluit P
- Kluth S
- Kneringer E
- Kobayashi T
- Kobel M
- Kokkinias P
- Komamiya S
- Konig AC
- Konstantinidis N
- Kopal M
- Kormos L
- Kourkoumelis C
- Koutsenko V
- Kouznetsov O
- Kowalewski RV
- Kraber M
- Kraemer RW
- Kramer T
- Krenz W
- Kress T
- Krieger P
- Krop D
- Kruger A
- Kruger K
- Krumstein Z
- Kucharczyk M
- Kuhn D
- Kunin A
- Kupper M
- Kyriakis A
- Lafferty GD
- Laktineh I
- Lamsa J
- Lancon E
- Landi G
- Landsman H
- Lanske D
- Laurelli P
- Layter JG
- Le Coultre P
- Le Goff JM
- Lebeau M
- Lebedev A
- Lebrun P
- Lecomte P
- Lecoq P
- Leder G
- Ledroit F
- Lee HJ
- Lees JP
- Lehto M
- Leibenguth G
- Leinonen L
- Leins A
- Leiste R
- Leitner R
- Lellouch D
- Lemaire MC
- Lemaitre V
- Lemonne J
- Lepeltier V
- Leroy O
- Lesiak T
- Letts J
- Levinson L
- Levtchenko P
- Li C
- Liebig W
- Ligabue F
- Likhoded S
- Liko D
- Lillich J
- Lin CH
- Lin J
- Lin WT
- Linde FL
- Lipniacka A
- Lista L
- Litke AM
- Liu ZA
- Lloyd SL
- Locci E
- Loebinger FK
- Lohmann W
- Longo E
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- Lopes JH
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- Lu YS
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- Luci C
- Luckey D
- Ludwig J
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- Lutz P
- Lynch JG
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- Macpherson A
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- Maggi G
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- Malek A
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- Malgeri L
- Malinin A
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- Marcellini S
- Marchant TE
- Marco J
- Marco R
- Marechal B
- Margoni M
- Marin JC
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- Mariotti C
- Markou A
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- Martin JP
- Martin JP
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- Marzano F
- Masetti G
- Mashimo T
- Masik J
- Mastroyiannopoulos N
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- Matorras F
- Matteuzzi C
- Mattig P
- Mazumdar K
- Mazzucato F
- Mazzucato M
- Mc Nulty R
- McDonald WJ
- McKenna J
- McMahon TJ
- McNamara PA
- McNeil RR
- McPherson RA
- Medcalf T
- Meijers F
- Mele S
- Mendez-Lorenzo P
- Menges W
- Merino G
- Merle E
- Merola L
- Meroni C
- Merritt FS
- Mes H
- Meschini M
- Messineo A
- Metzger WJ
- Meyer WT
- Michel B
- Michelini A
- Migliore E
- Mihara S
- Mihul A
- Mikenberg G
- Milcent H
- Miller DJ
- Minard MN
- Miquel R
- Mir LM
- Mirabelli G
- Misiejuk A
- Mitaroff W
- Mjoernmark U
- Mnich J
- Moa T
- Moch M
- Moed S
- Moenig K
- Mohanty GB
- Mohr W
- Monge R
- Monteil S
- Montenegro J
- Moraes D
- Moreno S
- Morettini P
- Mori T
- Moser HG
- Moutoussi A
- Muanza GS
- Mueller U
- Muenich K
- Muijs AJM
- Mulders M
- Muller AS
- Mundim L
- Murray W
- Murtas F
- Murtas GP
- Muryn B
- Musicar B
- Musy M
- Mutter A
- Myatt G
- Myklebust T
- Nagai K
- Nagy S
- Nakamura I
- Napolitano M
- Nassiakou M
- Navarria F
- Nawrocki K
- Neal HA
- Negus P
- Nessi-Tedaldi F
- Newman H
- Ngac A
- Nicolaidou R
- Nielsen J
- Niessen T
- Nikolenko M
- Nilsson BS
- Nisati A
- Nisius R
- Norton PR
- Nowak H
- Nowell J
- Nuzzo S
- O'Neale SW
- O'Shea V
- Oblakowska-Mucha A
- Obraztsov V
- Ofierzynski R
- Oh A
- Okpara A
- Olshevski A
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- Zivkovic L
- Zobernig G
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- 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
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- Zanetti M
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- 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
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- Abbiendi G
- Abbrescia M
- Abdullin 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
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- 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
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
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
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- Adamek L
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- Alberghi GL
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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
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