1,184 research outputs found
Recommended from our members
Projected WIMP sensitivity of the LUX-ZEPLIN dark matter experiment
- Author
- Akerib DS
- Akerlof CW
- Alsum SK
- Araújo HM
- Arthurs M
- Bai X
- Bailey AJ
- Balajthy J
- Balashov S
- Bauer D
- Belle J
- Beltrame P
- Benson T
- Bernard EP
- Biesiadzinski TP
- Boast KE
- Boxer B
- Brás P
- Buckley JH
- Bugaev VV
- Burdin S
- Busenitz JK
- Carels C
- Carlsmith DL
- Carlson B
- Carmona-Benitez MC
- Chan C
- Cherwinka JJ
- Cole A
- Cottle A
- Craddock WW
- Currie A
- Cutter JE
- Dahl CE
- De Viveiros L
- Dobi A
- Dobson JEY
- Druszkiewicz E
- Edberg TK
- Edwards WR
- Fan A
- Fayer S
- Fiorucci S
- Fruth T
- Gaitskell RJ
- Genovesi J
- Ghag C
- Gilchriese MGD
- Hall CR
- Hans S
- Hanzel K
- Haselschwardt SJ
- Hertel SA
- Hillbrand S
- Hjemfelt C
- Hoff MD
- Hor JYK
- Huang DQ
- Ignarra CM
- Ji W
- Kaboth AC
- Kamdin K
- Keefner J
- Khaitan D
- Khazov A
- Kim YD
- Kocher CD
- Korolkova EV
- Kraus H
- Krebs HJ
- Kreczko L
- Krikler B
- Kudryavtsev VA
- Kyre S
- Lee J
- Lenardo BG
- Leonard DS
- Lesko KT
- Levy C
- Li J
- Liao FT
- Liao J
- Lin J
- Lindote A
- Linehan R
- Lippincott WH
- Liu X
- Lopes MI
- Lorenzon W
- Luitz S
- Lyle JM
- López Paredes B
- Majewski P
- Manalaysay A
- Mannino RL
- Maupin C
- McKinsey DN
- Meng Y
- Miller EH
- Van Der Grinten MGD
- Publication venue
- eScholarship, University of California
- Publication date
- 01/03/2020
- Field of study
LUX-ZEPLIN (LZ) is a next-generation dark matter direct detection experiment that will operate 4850 feet underground at the Sanford Underground Research Facility (SURF) in Lead, South Dakota, USA. Using a two-phase xenon detector with an active mass of 7 tonnes, LZ will search primarily for low-energy interactions with weakly interacting massive particles (WIMPs), which are hypothesized to make up the dark matter in our galactic halo. In this paper, the projected WIMP sensitivity of LZ is presented based on the latest background estimates and simulations of the detector. For a 1000 live day run using a 5.6-tonne fiducial mass, LZ is projected to exclude at 90% confidence level spin-independent WIMP-nucleon cross sections above 1.4×10-48 cm2 for a 40 GeV/c2 mass WIMP. Additionally, a 5σ discovery potential is projected, reaching cross sections below the exclusion limits of recent experiments. For spin-dependent WIMP-neutron(-proton) scattering, a sensitivity of 2.3×10-43 cm2 (7.1×10-42 cm2) for a 40 GeV/c2 mass WIMP is expected. With underground installation well underway, LZ is on track for commissioning at SURF in 2020
Simulations of events for the LUX-ZEPLIN (LZ) dark matter experiment
- Author
- Akerib DS
- Akerlof CW
- Alqahtani A
- Alsum SK
- Anderson TJ
- Angelides N
- Araújo HM
- Armstrong JE
- Arthurs M
- Bai X
- Balajthy J
- Balashov S
- Bang J
- Bauer D
- Baxter A
- Bensinger J
- Bernard EP
- Bernstein A
- Bhatti A
- Biekert A
- Biesiadzinski TP
- Birch HJ
- Boast KE
- Boxer B
- Brás P
- Buckley JH
- Bugaev VV
- Burdin S
- Busenitz JK
- Cabrita R
- Carels C
- Carlsmith DL
- Carmona-Benitez MC
- Cascella M
- Chan C
- Chott NI
- Cole A
- Cottle A
- Cutter JE
- Dahl CE
- de Viveiros L
- Dobson JEY
- Druszkiewicz E
- Edberg TK
- Eriksen SR
- Fan A
- Fayer S
- Fiorucci S
- Flaecher H
- Fraser ED
- Fruth T
- Gaitskell RJ
- Genovesi J
- Ghag C
- Gibson E
- Gilchriese MGD
- Gokhale S
- Hall CR
- Harrison A
- Haselschwardt SJ
- Hertel SA
- Hor JYK
- Horn M
- Huang DQ
- Ignarra CM
- Jahangir O
- Ji W
- Johnson J
- Kaboth AC
- Kamaha AC
- Kamdin K
- Kazkaz K
- Khaitan D
- Khazov A
- Khurana I
- Kocher CD
- Korley L
- Korolkova EV
- Kras J
- Kraus H
- Kravitz S
- Kreczko L
- Krikler B
- Kudryavtsev VA
- Leason EA
- Lee J
- Leonard DS
- Lesko KT
- Levy C
- Li J
- Liao FT
- Liao J
- Lin J
- Lindote A
- Linehan R
- Lippincott WH
- Liu R
- Liu X
- Loniewski C
- van der Grinten MGD
- Publication venue
- eScholarship, University of California
- Publication date
- 01/02/2021
- Field of study
The LUX-ZEPLIN dark matter search aims to achieve a sensitivity to the WIMP-nucleon spin-independent cross-section down to (1–2)×10−12 pb at a WIMP mass of 40 GeV/c2. This paper describes the simulations framework that, along with radioactivity measurements, was used to support this projection, and also to provide mock data for validating reconstruction and analysis software. Of particular note are the event generators, which allow us to model the background radiation, and the detector response physics used in the production of raw signals, which can be converted into digitized waveforms similar to data from the operational detector. Inclusion of the detector response allows us to process simulated data using the same analysis routines as developed to process the experimental data
Recommended from our members
Projected sensitivity of the LUX-ZEPLIN experiment to the 0νββ decay of Xe 136
- Author
- Akerib DS
- Akerlof CW
- Alqahtani A
- Alsum SK
- Anderson TJ
- Angelides N
- Araújo HM
- Armstrong JE
- Arthurs M
- Bai X
- Balajthy J
- Balashov S
- Bang J
- Baxter A
- Bensinger J
- Bernard EP
- Bernstein A
- Bhatti A
- Biekert A
- Biesiadzinski TP
- Birch HJ
- Boast KE
- Boxer B
- Brás P
- Buckley JH
- Bugaev VV
- Burdin S
- Busenitz JK
- Cabrita R
- Carels C
- Carlsmith DL
- Carmona-Benitez MC
- Cascella M
- Chan C
- Chott NI
- Cole A
- Cottle A
- Cutter JE
- Dahl CE
- De Viveiros L
- Dobson JEY
- Druszkiewicz E
- Edberg TK
- Eriksen SR
- Fan A
- Fiorucci S
- Flaecher H
- Fraser ED
- Fruth T
- Gaitskell RJ
- Genovesi J
- Ghag C
- Gibson E
- Gilchriese MGD
- Gokhale S
- Hall CR
- Harrison A
- Haselschwardt SJ
- Hertel SA
- Hor JYK
- Horn M
- Huang DQ
- Ignarra CM
- Jahangir O
- Ji W
- Johnson J
- Kaboth AC
- Kamaha AC
- Kamdin K
- Kazkaz K
- Khaitan D
- Khazov A
- Khurana I
- Kocher CD
- Korley L
- Korolkova EV
- Kras J
- Kraus H
- Kravitz S
- Kreczko L
- Krikler B
- Kudryavtsev VA
- Leason EA
- Lee J
- Leonard DS
- Lesko KT
- Levy C
- Li J
- Liao FT
- Liao J
- Lin J
- Lindote A
- Linehan R
- Lippincott WH
- Liu R
- Liu X
- Loniewski C
- Lopes MI
- López Paredes B
- Van Der Grinten MGD
- Publication venue
- eScholarship, University of California
- Publication date
- 01/07/2020
- Field of study
The LUX-ZEPLIN (LZ) experiment will enable a neutrinoless double β decay search in parallel to the main science goal of discovering dark matter particle interactions. We report the expected LZ sensitivity to Xe136 neutrinoless double β decay, taking advantage of the significant (>600 kg) Xe136 mass contained within the active volume of LZ without isotopic enrichment. After 1000 live-days, the median exclusion sensitivity to the half-life of Xe136 is projected to be 1.06×1026 years (90% confidence level), similar to existing constraints. We also report the expected sensitivity of a possible subsequent dedicated exposure using 90% enrichment with Xe136 at 1.06×1027 years
Use of a non-homologous end-joining-deficient strain (delta-ku70) of the biocontrol fungus Trichoderma virens to investigate the function of the laccase gene lcc1 in sclerotia degradation
- Author
- B Hoff
- B Seiboth
- Bernhard Seiboth
- BL Goméz
- Christian P. Kubicek
- CJ Alexopoulos
- F Gruber
- G Vannacci
- G Vannacci
- GH Goldman
- Giovanni Vannacci
- HC Eisenman
- HJ Willetts
- HJ Willetts
- IS Snoek
- J Sambrook
- Jasmin R. Hauzenberger
- L Hartl
- M Choquer
- M Levy
- Mariarosaria Vergara
- ME da Silva Ferreira
- MJ Butler
- N Benhamou
- P Baldrian
- P Chomczynski
- P Giardina
- P Rey
- PK Chang
- R Lopez-Mondejar
- RL Mach
- S Krappmann
- S Krappmann
- S Le Crom
- S Pöggeler
- S Sarrocco
- Sabrina Sarrocco
- T Benitez
- T Haarmann
- T Nayak
- T Takahashi
- T Yamada
- TK Lundell
- V Meyer
- V Seidl
- V Seidl
- Valentina Catalano
- Verena Seidl-Seiboth
- Y Ninomiya
- Z Guangtao
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2010
- Field of study
The aim of this study was to apply a generated Δtku70 strain with increased homologous recombination efficiency from the mycoparasitic fungus Trichoderma virens for studying the involvement of laccases in the degradation of sclerotia of plant pathogenic fungi. Inactivation of the non-homologous end-joining pathway has become a successful tool in filamentous fungi to overcome poor targeting efficiencies for genetic engineering. Here, we applied this principle to the biocontrol fungus T. virens, strain I10, by deleting its tku70 gene. This strain was subsequently used to delete the laccase gene lcc1, which we found to be expressed after interaction of T. virens with sclerotia of the plant pathogenic fungi Botrytis cinerea and Sclerotinia sclerotiorum. Lcc1 was strongly upregulated at early colonization of B. cinerea sclerotia and steadily induced during colonization of S. sclerotiorum sclerotia. The Δtku70Δlcc1 mutant was altered in its ability to degrade the sclerotia of B. cinerea and S. sclerotiorum. Interestingly, while the decaying ability for B. cinerea sclerotia was significantly decreased, that to degrade S. sclerotiorum sclerotia was even enhanced, suggesting the operation of different mechanisms in the mycoparasitism of these two types of sclerotia by the laccase LCC1
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)
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
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- Yang BZ
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- Zachariadou K
- Zalewska A
- Zalewski P
- Zalite A
- Zalite Y
- Zavrtanik D
- Zeitnitz C
- Zer-Zion D
- Zhang J
- Zhang L
- Zhang ZP
- Zhao J
- Zhao W
- Zhu GY
- Zhu RY
- Zhuang HL
- Zhuravlov V
- Zichichi A
- Ziegler T
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- 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
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
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- Aguilo E
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- Ahmad WH
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- Anastassov A
- Anderson J
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- Andreev Y
- Andrews W
- Anghel IM
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- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
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- Bakken JA
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- Ban Y
- Banerjee S
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- Barbagli G
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- Bauerdick LAT
- Baumgartel D
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- Bayshev I
- Bazterra VE
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- Beaudette F
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- Bedjidian M
- Beernaert K
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- Belotelov I
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- Belyaev A
- Benaglia A
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
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- 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
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- Zoeller MH
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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
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- 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
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
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- Anastopoulos C
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- Anisenkov A
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- ATLAS Collaboration The
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- Bailey DC
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- Zevi Della Porta G
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
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- Zivković L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Widl E
- Wigmans R
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- Williams G
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- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
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- Womersley WJ
- Won S
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- Wood JS
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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
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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
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
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- Albajar C
- Albayrak EA
- Albergo S
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
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