364 research outputs found
A Study of the Static-Light BB Parameter
- Author
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/08/1996
- Field of study
We calculate the BB parameter, relevant for B0--B0
mixing, from a lattice gauge theory simulation using the static approximation
for the heavy quark and the Wilson action for the light quark and gauge fields.
Improved sources, produced by an optimized variational technique, {\sc most},
reduce statistical errors and minimize excited-state contamination of the
ground-state signal. Renormalization of four-fermion operator coefficients,
using the Lepage-Mackenzie procedure for estimating typical momentum scales, is
linearized to reduce order αs2 uncertainties.Comment: 4 pages (LaTeX), Talk presented at LATTICE96(heavy quarks), Minor
numerically-insignificant changes made and reference adde
Long-distance contribution to ϵK from lattice QCD
- Publication venue
- Publication date
- 03/09/2023
- Field of study
A lattice QCD approach to the calculation of the long-distance contributions
to ϵK is presented. This parameter describes indirect CP violation in
K→ππ decay. While the short-distance contribution to ϵK can
be accurately calculated in terms of standard model parameters and a single
hadronic matrix element, BK, there is a long-distance part which is
estimated to be approximately 5% of the total and is more difficult to
determine. A method for determining this small but phenomenologically important
contribution to ϵK using lattice QCD is proposed and a complete
exploratory calculation of the contribution is presented. This exploratory
calculation uses an unphysical light quark mass corresponding to a 339 MeV pion
mass and an unphysical charm quark mass of 968 MeV, expressed in the
MS scheme at 2 GeV. This calculation demonstrates that
future work should be able to determine this long-distance contribution from
first principles with a controlled error of 10\% or less
A Comparison of Methods for a Priori Bias Correction in Soil Moisture Data Assimilation
- Author
- Publication venue
- Publication date
- 30/09/2011
- Field of study
Data assimilation is being increasingly used to merge remotely sensed land surface variables such as soil moisture, snow and skin temperature with estimates from land models. Its success, however, depends on unbiased model predictions and unbiased observations. Here, a suite of continental-scale, synthetic soil moisture assimilation experiments is used to compare two approaches that address typical biases in soil moisture prior to data assimilation: (i) parameter estimation to calibrate the land model to the climatology of the soil moisture observations, and (ii) scaling of the observations to the model s soil moisture climatology. To enable this research, an optimization infrastructure was added to the NASA Land Information System (LIS) that includes gradient-based optimization methods and global, heuristic search algorithms. The land model calibration eliminates the bias but does not necessarily result in more realistic model parameters. Nevertheless, the experiments confirm that model calibration yields assimilation estimates of surface and root zone soil moisture that are as skillful as those obtained through scaling of the observations to the model s climatology. Analysis of innovation diagnostics underlines the importance of addressing bias in soil moisture assimilation and confirms that both approaches adequately address the issue
Polybenzodiazine Aerogels: All-Nitrogen Analogues of Polybenzoxazines Synthesis, Characterization, and High-Yield Conversion to Nanoporous Carbons
- Author
- Publication venue
- Scholars\u27 Mine
- Publication date
- 01/01/2022
- Field of study
Tetrahydroquinazoline (THQ) was designed as an all-nitrogen analogue of main-stream benzoxazine monomers. THQ solutions in DMF gelled at 100 °C via HCl-catalyzed ring-opening polymerization to polybenzodiazine (PBDAZ) wet gels, which were dried in an autoclave with supercritical fluid CO2 to aerogels. These as-prepared PBDAZ-100 aerogels undergo ring-fusion aromatization at 240 °C under O2. This oxidized form is referred to as PBDAZ-240. Chemical identification of PBDAZ-100 and PBDAZ-240 relied on consideration of all nine possible polymerization pathways, in combination with elemental analysis, infrared and solid-state 13C NMR spectroscopy, and 15N NMR spectroscopy of aerogels from the selectively 15N-enriched THQ monomer. Fully oxidized PBDAZ-240 aerogels were carbonized at 800 °C under Ar to carbon aerogels with 61% w/w yield and with retention of the nanomorphology of the parent PBDAZ-100 aerogels. Direct pyrolysis of PBDAZ-100 at 800 °C, i.e., without prior oxidation, resulted in only 40% w/w yield and complete loss of the fine nanostructure. The evolution of PBDAZ-240 aerogels along pyrolysis toward carbonization was monitored using progressively higher pyrolysis temperatures from 300 to 800 °C under Ar. Aerogels received at 600 and 800 °C (referred to as PBDAZ-600 and PBDAZ-800, respectively) had relatively high surface areas (432 and 346 m2 g-1, respectively), a significant portion of which (79% in both materials) was assigned to micropores. The new polymer aerogels, together with polybenzoxazine aerogels, comprise a suitable basis set for comparing N-rich versus O-rich porous carbons as adsorbers
A calculation of the BB parameter in the static limit
- Author
- A. Abada
- A. Borrelli
- A. Donini
- A. Duncan
- A. J. Buras
- A. J. Buras
- A. J. Buras
- A. K. Ewing
- A. Soni
- C. A. Dominguez
- C. Bernard
- C. Bernard
- C. Morningstar
- C. R. Allton
- C. R. Allton
- C. T. H. Davies
- Craig McNeile
- D. J. Broadhurst
- D. J. Broadhurst
- E. Eichten
- E. Eichten
- E. Eichten
- F. Butler
- F. D. Renzo
- G. Buchalla
- G. Buchalla
- G. Burgio
- G. Martinelli
- G. P. Lepage
- G. P. Lepage
- G. S. Bali
- J. Flynn
- J. M. Flynn
- J. Rosner
- J. Sloan
- Joseph Christensen
- M. Ciuchini
- M. Ciuchini
- M. J. Booth
- M. Neubert
- O. F. Hernández
- R. M. Barnett
- S. Narison
- S. Sharpe
- T. Bhattacharya
- Terrence Draper
- V. Giménez
- V. Giménez
- V. Giménez
- X. Ji
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 06/02/1998
- Field of study
We calculate the BB parameter, relevant for B0 -- B0
mixing, from a lattice gauge theory simulation at β=6.0. The bottom
quarks are simulated in the static theory, the light quarks with Wilson
fermions. Improved smearing functions produced by a variational technique,
MOST, are used to reduce statistical errors and minimize excited-state
contamination of the ground-state signal. We obtain BB(4.33GeV)=0.98−4+4 (statistical) −18+3 (systematic) which corresponds to
BB=1.40−6+6 (statistical) −26+4 (systematic) for
the one-loop renormalization-scheme-independent parameter. The systematic
errors include the uncertainty due to alternative (less favored) treatments of
the perturbatively-calculated mixing coefficients; this uncertainty is at least
as large as residual differences between Wilson-static and clover-static
results. Our result agrees with extrapolations of results from relativistic
(Wilson) heavy quark simulations.Comment: 39 pages (REVTeX) including 10 figures (PostScript); Final version
accepted for publication: Added new section for clarity; Included comparison
to recent results by other groups; slight numerical changes; Essential
conclusions remain the sam
Evaluation of the Parasight Platform for Malaria Diagnosis
- Author
- Publication venue
- eCommons@AKU
- Publication date
- 01/03/2017
- Field of study
The World Health Organization estimates that nearly 500 million malaria tests are performed annually. While microscopy and rapid diagnostic tests (RDTs) are the main diagnostic approaches, no single method is inexpensive, rapid, and highly accurate. Two recent studies from our group have demonstrated a prototype computer vision platform that meets those needs. Here we present the results from two clinical studies on the commercially available version of this technology, the Sight Diagnostics Parasight platform, which provides malaria diagnosis, species identification, and parasite quantification. We conducted a multisite trial in Chennai, India (Apollo Hospital [n = 205]), and Nairobi, Kenya (Aga Khan University Hospital [n = 263]), in which we compared the device to microscopy, RDTs, and PCR. For identification of malaria, the device performed similarly well in both contexts (sensitivity of 99% and specificity of 100% at the Indian site and sensitivity of 99.3% and specificity of 98.9% at the Kenyan site, compared to PCR). For species identification, the device correctly identified 100% of samples with Plasmodium vivax and 100% of samples with Plasmodium falciparum in India and 100% of samples with P. vivax and 96.1% of samples with P. falciparum in Kenya, compared to PCR. Lastly, comparisons of the device parasite counts with those of trained microscopists produced average Pearson correlation coefficients of 0.84 at the Indian site and 0.85 at the Kenyan site
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
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- 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
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
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- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
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- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck GA
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
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- Bellagamba L
- Bellina F
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- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
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- Beretta M
- Berge D
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- Bertin A
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- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek T
- Blocker C
- Blocki J
- Blondel A
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- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeriu OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
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- Boldea V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
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- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
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- Bozovic-Jelisavcic I
- Bracinik J
- Braem A
- Branchini P
- Brandenburg GW
- Brandt A
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- Bratzler U
- Brau B
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- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
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- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
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- Bruni A
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- Bruschi M
- BScher V
- Buanes T
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- Buchanan J
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- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Caballero J
- Caforio D
- Cakir IT
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- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
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- Caloi R
- Calvet D
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- Camarri P
- Cambiaghi M
- Cameron D
- Camilocci ES
- Campana S
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- Canale V
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- Canepaa A
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- Capasso L
- Caprini I
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- Capriotti D
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- Caramarcu C
- Cardarelli R
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- Carlino G
- Carminati L
- Caron B
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- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauz D
- Cavalcanti TP
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciba K
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Cioccaa C
- Ciocio A
- Cirilli M
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
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- Coccaro A
- Cochran J
- Codina EP
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration ATLAS
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- Collins-Tooth C
- Collot J
- Colon G
- Coniavitis E
- Conidi MC
- Consonni M
- Consorti V
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
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- Cowan G
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- Cox BE
- Cranmer K
- Cranshaw J
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Crupi R
- Cuciuc C-M
- Curatolo M
- Curtis CJ
- Curull XE
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
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- D'Orazio A
- Da Costa JBG
- Da Costa JGPF
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Daly CH
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
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- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
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- Davison AR
- Davygora Y
- Dawe E
- Dawson I
- Dawson JW
- Daya-Ishmukhametova RK
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- De Jong P
- De la Hoz SG
- De la Taille C
- De la Torre H
- De Lima JGR
- De Lotto B
- De Mora L
- De Nooij L
- De Pedis D
- De Regie JBDV
- De Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
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- Dean S
- Debbe R
- Dedovich DV
- Degenhardt J
- Dehchar M
- Del Papa C
- Del Peso J
- Del Prete T
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Porta GZ
- della Volpe D
- Delmastro M
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- Delsart PA
- Deluca C
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- Demichev M
- Demirkoz B
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- Denis RDS
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
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- Devetak E
- Deviveiros PO
- Dewhurst A
- DeWilde B
- Dhaliwal S
- Dhullipudi R
- Di Ciaccio A
- Di Ciaccio L
- Di Girolamo A
- Di Girolamo B
- Di Luise S
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Diaz MA
- Diblen F
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- Dietzscha TA
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- Doan TKO
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- Donszelmann TC
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- Dos Anjos A
- Dos Santos DR
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- Dotti A
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- Dowell JD
- Doxiadis AD
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- Duerdoth IP
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- Elmsheuser J
- Elsing M
- Emeliyanov D
- Engelmann R
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- Epp B
- Eppig A
- Erdmann J
- Ereditato A
- Eriksson D
- Ernst J
- Ernst M
- Ernwein J
- Errede D
- Errede S
- Ertel E
- Escalier M
- Eschrich IG
- Escobar C
- Esposito B
- Etienne F
- Etienvre AI
- Etzion E
- Evangelakou D
- Evans H
- Fabbri L
- Fabre C
- Fajardo LSG
- Fakhrutdinov RM
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- Farilla A
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- Farrington SM
- Farthouat P
- Fassnacht P
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- Fatholahzadeh B
- Favareto A
- Fayard L
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- Fedin OL
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- Feligioni L
- Fellmann D
- Felzmann CU
- Feng EJ
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- Fenyuk AB
- Ferencei J
- Ferland J
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- Ferrere D
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- Filipcic A
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- Fiolhais MCN
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- Firan A
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- Fisher SM
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- Fleck I
- Fleckner J
- Fleischmann P
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- Yilmaz M
- Yoosootiniya R
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- Zarzhitsky P
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- Zerwas D
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
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- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
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- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
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- Adelman J
- Aderholz M
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- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
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- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
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- Zema PF
- Zemla A
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- Zenin O
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- Zenonos Z
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- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Single hadron response measurement and calorimeter jet energy scale uncertainty with the ATLAS detector at the LHC
- Author
- A. A. Abdelalim
- A. A. Carter
- A. A. Grillo
- A. A. Komar
- A. A. Minaenko
- A. A. Nepomuceno
- A. A. Snesarev
- A. A. Solodkov
- A. Abdesselam
- A. Ahmad
- A. Akiyama
- A. Aloisio
- A. Alonso
- A. Amorim
- A. Andreazza
- A. Angerami
- A. Anisenkov
- A. Annovi
- A. Antonaki
- A. Antonov
- A. Artamonov
- A. Astbury
- A. Astvatsatourov
- A. B. Fenyuk
- A. B. Lazarev
- A. Bangert
- A. Barashkou
- A. Barbaro Galtieri
- A. Baroncelli
- A. Battaglia
- A. Beddall
- A. Belloni
- A. Bertin
- A. Bingul
- A. Blondel
- A. Bocci
- A. Bogdanchikov
- A. Bogouch
- A. Borisov
- A. Boveia
- A. Braem
- A. Brandt
- A. Bruni
- A. C. König
- A. C. Martyniuk
- A. C. Schaffer
- A. Canepa
- A. Catinaccio
- A. Cattai
- A. Cerri
- A. Chafaq
- A. Cheplakov
- A. Chilingarov
- A. Christov
- A. Ciocio
- A. Clark
- A. Coccaro
- A. Cortes-Gonzalez
- A. D. Doxiadis
- A. D. Hawkins
- A. D. Hershenhorn
- A. D. Pilkington
- A. De Salvo
- A. De Santo
- A. Dell’Acqua
- A. Dewhurst
- A. Di Ciaccio
- A. Di Girolamo
- A. Di Mattia
- A. Di Simone
- A. Do Valle Wemans
- A. Doria
- A. Dos Anjos
- A. Dotti
- A. Dudarev
- A. D’Orazio
- A. E. Barton
- A. E. Kiryunin
- A. Engl
- A. Eppig
- A. Ereditato
- A. F. Saavedra
- A. Farbin
- A. Farilla
- A. Favareto
- A. Ferrari
- A. Ferrer
- A. Ferretto Parodi
- A. Filippas
- A. Filipčič
- A. Firan
- A. Floderus
- A. Formica
- A. Forti
- A. Foussat
- A. G. Buckley
- A. G. Goussiou
- A. G. Kholodenko
- A. G. Myagkov
- A. G. Olchevski
- A. G. Schamov
- A. Gaponenko
- A. Gemmell
- A. Gershon
- A. Gibson
- A. Glazov
- A. Gomes
- A. Gonidec
- A. Gorišek
- A. Guida
- A. Gupta
- A. Haas
- A. Hamilton
- A. Harvey
- A. Henrichs
- A. Hoecker
- A. Hoummada
- A. Huettmann
- A. I. Etienvre
- A. I. Kononov
- A. I. Mincer
- A. Irles Quiles
- A. Ishikawa
- A. J. Armbruster
- A. J. Barr
- A. J. Beddall
- A. J. Fowler
- A. J. Lankford
- A. J. Lowe
- A. J. Martin
- A. J. Tanasijczuk
- A. Jantsch
- A. Jeremie
- A. Juste Rozas
- A. K. Ciftci
- A. K. Morley
- A. Kaczmarska
- A. Kapliy
- A. Kasmi
- A. Kastanas
- A. Khanov
- A. Khodinov
- A. Khomich
- A. Khoroshilov
- A. Kiryunin
- A. Klier
- A. Klimentov
- A. Knue
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- A. Kotwal
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- A. M. Cooper-Sarkar
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- A. Vaniachine
- A. Vartapetian
- A. Ventura
- A. Vest
- A. Vogel
- A. Warburton
- A. White
- A. Wildauer
- A. Wilson
- A. Yamamoto
- A. Yurkewicz
- A. Zaytsev
- A. Zemla
- A. Zhemchugov
- A. Zoccoli
- A. Zsenei
- A.-E. Nuncio-Quiroz
- ATLAS Collaboration
- ATLAS Collaboration
- ATLAS Collaboration
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- ATLAS Collaboration
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- S. Swedish
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- S. Tanaka
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- S. Yacoob
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- S. Yanush
- S. Ye
- S. Youssef
- S. Yu. Sivoklokov
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- S. Zenz
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- S. Zimmermann
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- S.-C. Hsu
- Sw. Banerjee
- T. A. Dietzsch
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- T. Kubota
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- T. Lenz
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- T. M. Hong
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- T. Matsushita
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- T. Meguro
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- V. F. Chepurnov
- V. Ferrara
- V. G. Bondarenko
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- V. Giangiobbe
- V. Gilewsky
- V. Grassi
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- X. Ju
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- X. Li
- X. Lou
- X. Portell Bueso
- X. Prudent
- X. Ruan
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- Y. A. Kurochkin
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- Y. Davygora
- Y. Doi
- Y. F. Ryabov
- Y. Fang
- Y. Gusakov
- Y. Hasegawa
- Y. Hernández Jiménez
- Y. Homma
- Y. Ikegami
- Y. Ilchenko
- Y. Jiang
- Y. Kataoka
- Y. Komori
- Y. Kulchitsky
- Y. Liu
- Y. Mahalalel
- Y. Makida
- Y. Ming
- Y. Munwes
- Y. Nagasaka
- Y. Nakahama
- Y. Ninomiya
- Y. Okumura
- Y. Oren
- Y. Pylypchenko
- Y. Rozen
- Y. S. Gao
- Y. Silver
- Y. Smirnov
- Y. Sugaya
- Y. Suzuki
- Y. Suzuki
- Y. Takahashi
- Y. Takubo
- Y. Tanaka
- Y. Tayalati
- Y. Unno
- Y. V. Grishkevich
- Y. Wu
- Y. Xie
- Y. Yamazaki
- Y. Yang
- Y. Yang
- Y. Yao
- Y. Yasu
- Y. Zhou
- Y. Zhu
- Y. Zolnierowski
- Yu. M. Sviridov
- Z. Czyczula
- Z. D. Greenwood
- Z. Dolezal
- Z. Drasal
- Z. Hajduk
- Z. Hubacek
- Z. Kohout
- Z. L. Ren
- Z. Liang
- Z. Marshall
- Z. Meng
- Z. Qian
- Z. Qin
- Z. Rurikova
- Z. V. Krumshteyn
- Z. van Kesteren
- Z. Weng
- Z. Yan
- Z. Yang
- Z. Zajacova
- Z. Zenonos
- Z. Zhan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 06/03/2012
- Field of study
The uncertainty on the calorimeter energy response to jets of particles is
derived for the ATLAS experiment at the Large Hadron Collider (LHC). First, the
calorimeter response to single isolated charged hadrons is measured and
compared to the Monte Carlo simulation using proton-proton collisions at
centre-of-mass energies of sqrt(s) = 900 GeV and 7 TeV collected during 2009
and 2010. Then, using the decay of K_s and Lambda particles, the calorimeter
response to specific types of particles (positively and negatively charged
pions, protons, and anti-protons) is measured and compared to the Monte Carlo
predictions. Finally, the jet energy scale uncertainty is determined by
propagating the response uncertainty for single charged and neutral particles
to jets. The response uncertainty is 2-5% for central isolated hadrons and 1-3%
for the final calorimeter jet energy scale.Comment: 24 pages plus author list (36 pages total), 23 figures, 1 table,
submitted to European Physical Journal
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