600 research outputs found
Defining the phenotypes of sickle cell disease.
- Author
- Albers GW
- Ballas SK
- Ballas SK
- Ballas SK
- Ballas SK
- Ballas SK
- Banerjee S
- Bellomo R
- Bookchin RM
- Brazier DJ
- Dana MR
- DeBaun MR
- DeBaun MR
- Dobson SR
- Goldberg MF
- Halabi-Tawil M
- Hatton CS
- Johnson CS
- Karam LB
- Koshy M
- Ohene-Frempong K
- Pearson HA
- Powars D
- Powell RW
- Robertson KD
- Rogers ZR
- Samir K. Ballas
- Shao SH
- Vichinsky EP
- Vichinsky EP
- Vichinsky EP
- West MS
- Williams GC
- Zimmerman SA
- Publication venue
- Jefferson Digital Commons
- Publication date
- 01/01/2011
- Field of study
The sickle cell gene is pleiotropic in nature. Although it is a single gene mutation, it has multiple phenotypic expressions that constitute the complications of sickle cell disease. The frequency and severity of these complications vary considerably both latitudinally in patients and longitudinally in the same patient over time. Thus, complications that occur in childhood may disappear, persist or get worse with age. Dactylitis and stroke, for example, occur mostly in childhood, whereas leg ulcers and renal failure typically occur in adults. It is essential that the phenotypic manifestations of sickle cell disease be defined accurately so that communication among providers and researchers facilitates the implementation of appropriate and cost-effective diagnostic and therapeutic modalities. The aim of this review is to define the complications that are specific to sickle cell disease based on available evidence in the literature and the experience of hematologists in this field
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Projected WIMP sensitivity of the LUX-ZEPLIN dark matter experiment
- Author
- Akerib DS
- Akerlof CW
- Alsum SK
- AraĂşjo 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
- BrĂĄs 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
- LĂłpez 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 1.4Ă10-48 cm2 for a 40 GeV/c2 mass WIMP. Additionally, a 5Ď discovery potential is projected, reaching cross sections below the exclusion limits of recent experiments. For spin-dependent WIMP-neutron(-proton) scattering, a sensitivity of 2.3Ă10-43 cm2 (7.1Ă10-42 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
- AraĂşjo 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
- BrĂĄs 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 (1â2)Ă10â12 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
- AraĂşjo 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
- BrĂĄs 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
- LĂłpez 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 1.06Ă1026 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 1.06Ă1027 years
Climate Change Promotes the Emergence of Serious Disease Outbreaks of Filarioid Nematodes
- Author
- AN Clements
- Antti Oksanen
- AP Dobson
- Ari Venäläinen
- B Ytrehus
- C Rehbinder
- CD Harvell
- DC Calado
- DJ Gubler
- EP Hoberg
- EP Hoberg
- Eric Hoberg
- FM MĂśrchel
- H Delatte
- JA Patz
- JA Patz
- Jouko Kumpula
- JR Anderson
- Jyrki Pusenius
- K Handeland
- KD Lafferty
- LH Taylor
- M Tryland
- P Lemke
- P LĂśwenberg-Neto
- Raine Kortet
- RB Weladj
- RH Pollard
- S Dadaev
- S Laaksonen
- S Laaksonen
- S Laaksonen
- S Nikander
- Sauli Laaksonen
- SJ Kutz
- SJ Kutz
- SJ Kutz
- SJ Kutz
- T Helle
- T Helle
- T Kuiken
- T Nygren
- VV Kadnikov
- WA Barry
- World Health Organization
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2010
- Field of study
Filarioid parasites represent major health hazards with important medical, veterinary, and economic implications, and considerable potential to affect the everyday lives of tens of millions of people globally (World Health Organization, 2007). Scenarios for climate change vary latitudinally and regionally and involve direct and indirect linkages for increasing temperature and the dissemination, amplification, and invasiveness of vector-borne parasites. High latitude regions are especially influenced by global climate change and thus may be prone to altered associations and dynamics for complex host-pathogen assemblages and emergence of disease with cascading effects on ecosystem structure. Although the potential for substantial ecological perturbation has been identified, few empirical observations have emanated from systems across the Holarctic. Coincidental with decades of warming, and anomalies of high temperature and humidity in the sub-Arctic region of Fennoscandia, the mosquito-borne filarioid nematode Setaria tundra is now associated with emerging epidemic disease resulting in substantial morbidity and mortality for reindeer and moose. We describe a host-parasite system that involves reindeer, arthropods, and nematodes, which may contribute as a factor to ongoing declines documented for this ungulate species across northern ecosystems. We demonstrate that mean summer temperatures exceeding 14°C drive the emergence of disease due to S. tundra. An association between climate and emergence of filarioid parasites is a challenge to ecosystem services with direct effects on public health, sustainability of free-ranging and domestic ungulates, and ultimately food security for subsistence cultures at high latitudes
Effect of repeat human blood feeding on Wolbachia density and dengue virus infection in Aedes aegypti
- Author
- AA Hoffmann
- Cameron P Simmons
- CJ McMeniman
- CJ McMeniman
- D Warrilow
- E Rances
- Elizabeth A McGraw
- EP Caragata
- EP Caragata
- FD Frentiu
- FD Frentiu
- G Bian
- Hilaria E Amuzu
- I Iturbe-Ormaetxe
- J Chun
- JC Koella
- K McCall
- K Zouache
- L Mouton
- LA Baton
- LA Moreira
- LR Serbus
- N Kondo
- O Thellin
- P Kittayapong
- P Lu
- PE Cook
- PM Ferree
- R Zug
- S Bhatt
- SJ Thomas
- SL Dobson
- T Ikeda
- T Walker
- TJ Dutton
- TW Scott
- TW Scott
- TW Scott
- WC Black
- X Pan
- YH Ye
- Z Xi
- Z Xi
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 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
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- 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
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boimska B
- Boldizsar L
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondu O
- Bontenackels M
- Boos E
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bortoletto D
- Bose S
- Bose T
- Bostock F
- Botta C
- Boudoul G
- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Broccolo G
- Brochero Cifuentes JA
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmann MA
- Buchmuller O
- Bunkowski K
- Bunn J
- Buontempo S
- Burgmeier A
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
- Campbell A
- Camporesi T
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carrillo Moreno S
- Carroll R
- Cartiglia N
- Carvalho W
- Casal B
- Casimiro Linares E
- Castaldi R
- Castello R
- Castilla-Valdez H
- Castro A
- Castro E
- Caudron J
- Caulfield M
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
- Chen M
- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Cho Y
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cooper W
- Cornelis T
- Correa Martins Junior M
- Cortezon EP
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
- David A
- Davids M
- Davies G
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Troconiz JF
- De Visscher S
- De Wolf EA
- Deisher A
- Deiters K
- Dejardin M
- del Arbol PMR
- Del Re D
- Delaere C
- Delgado Peris A
- Deliomeroglu M
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demortier L
- Denegri D
- Deniz M
- Depasse P
- Dermenev A
- Dero V
- Dhingra N
- Di Giovanni GP
- Di Guida S
- Di Marco E
- Di Matteo L
- Diamond B
- Dias FA
- Diemoz M
- Dierlamm A
- Dietz C
- Dietz-Laursonn E
- Diez Pardos C
- Dimitrov A
- Dinardo ME
- Dirkes G
- Dissertori G
- Dittmar M
- Djordjevic M
- Dobrzynski L
- Dobson M
- Dobur D
- Doesburg R
- Dogangun O
- Dolen J
- Dominguez Vazquez D
- Dominguez A
- Dominik W
- Don CKK
- Dorigo T
- Dorney B
- Doroba K
- Dozen C
- Draeger J
- Dragicevic M
- Dragoiu C
- Drell BR
- Dremin I
- Drouhin F
- Drozdetskiy A
- du Pree T
- Duarte Campderros J
- Duarte J
- Dubinin M
- Dudero PR
- Dudko L
- Duenser M
- Dugad S
- Duggan D
- Dumanoglu I
- Dupont-Sagorin N
- Duric S
- Duris J
- Durkin LS
- Duru F
- Dutta D
- Dutta S
- Dutta V
- Dzelalija M
- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
- Eerola P
- Efron J
- Eggert N
- Ekmedzic M
- El Mamouni H
- Elgammal S
- Elliott-Peisert A
- Ellison J
- Elmer P
- Elvira VD
- Enderle H
- Engh D
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- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Acharya BS
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- Yilmaz M
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- Zitoun R
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- 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 âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâĽ20 GeV and pseudorapidities {pipe}Ρ{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}Ρ{pipe}<0. 8) for jets with 60â¤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â¤{pipe}Ρ{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. Š 2013 CERN for the benefit of the ATLAS collaboration
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
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- Romeo F
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- Sfiligoi I
- Sguazzoni G
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- Sharma A
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- Sharma V
- Sharma V
- Sharp P
- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shipkowski SP
- Shipsey I
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- Soares MS
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- Tsang KV
- Tschudi Y
- Tsirou A
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- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
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- Wolf R
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- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
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- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
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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
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