1,169 research outputs found
ЧАСТОТНЫЕ ХАРАКТЕРИСТИКИ ИНТЕГРАЛЬНЫХ ДАТЧИКОВ ХОЛЛА
- Publication venue
- БГУИР
- Publication date
- 03/06/2019
- Field of study
The results of device-technological and schematic simulation of the silicon Hall sensor with the purpose of determine its dynamic characteristics are presented. The influence of the dimensions of the active region is investigated, the theoretical and actual values of the upper limit of the bandwidth of the Hall sensor are determined, taking into account the internal parasitic capacitance, and the presence and absence of a capacitive load. The characteristics of the Hall sensor combined on a single crystal with a differential amplifier are simulated.Представлены результаты приборно-технологического и схемотехнического моделирования кремниевого датчика Холла с целью определения его динамических характеристик. Исследовано влияние размеров активной области, определены теоретическое и фактическое значения верхнего предела полосы пропускания датчика Холла с учетом внутренней паразитной емкости, а также при наличии и отсутствии емкостной нагрузки. Промоделированы характеристики датчика Холла, совмещенного на одном кристалле с дифференциальным усилителем
Assessing decentralised policy implementation in Vietnam : The case of land recovery and resettlement in the Vung Ang Economic Zone
- Author
- Publication venue
- Wit, J.W. (Joop) de
- Publication date
- 16/07/2012
- Field of study
From 2006 plans were implemented to create a deep-sea water port linked to an Economic Zone in the coastal Province of Ha Tinh, located in north central Vietnam. The multi-purpose Zone entitled ‘Vung Ang’, was to attract foreign investors, while the port would provide a link to nearby Laos and Thailand. The project obviously had large implications for the administrations at various levels of governance from Hanoi to the coastal communes and villages, but even more serious impacts on the people living in the affected areas. A large area of about 23,000 hectares was to be cleared, affecting the people of 9 communes, in some of which all inhabitants had to leave their houses and homesteads, to be relocated to completely new settlements about 10 miles inland. These tightly knit communities were not too happy with the prospect to leave their homes and land, the burial places of their ancestors, and the long term comforts of community support networks. While initial decision making process started at the highest levels of Vietnam Governance, the implementation of port and industrial park construction and the related relocation policy was delegated to Ha Tinh province, which is consistent with current decentralisation policies in Vietnam. Actual implementation was carried out by the affected District and Commune level officials – with support from the Communist Party led Mass Organisations – who were in charge of the planning and implementation of the relocation process. This entailed a complex and sensitive series of steps to inform affected households, prepare relocation areas and allocate compensation and alternative housing. This paper describes the implementation dynamics of relocation by depicting and assessing the roles of all stakeholders involved, including the impacts - for better or for worse – of the relocated households. It brings out the way local authorities dealt with affected people, including efforts linked to the ideal of grass-roots democracy. Key areas of contestation are uncovered, such as inadequate infrastructure and low compensation rates. The paper has a second objective to assess the degree to which decentralisation in Vietnam has been actually implemented, and how this affects policy making processes such as the Vung Ang port/industrial zone project. The paper concludes that the relocation policy was implemented in a fairly efficient and harmonious way – with a very intensive engagement of the entire provincial administrative machinery, but that it is too early to assess the livelihood opportunities of the relocated households
Sources of Multidrug Resistance in Patients With Previous Isoniazid-Resistant Tuberculosis Identified Using Whole Genome Sequencing: A Longitudinal Cohort Study
- Author
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/01/2020
- Field of study
Background
Meta-analysis of patients with isoniazid-resistant tuberculosis given standard first-line anti-tuberculosis treatment indicated an increased risk of multi-drug resistant tuberculosis (MDR-TB) emerging (8%), compared to drug-sensitive tuberculosis (0.3%). Here we use whole genome sequencing (WGS) to investigate whether treatment of patients with pre-existing isoniazid resistant disease with first-line anti-tuberculosis therapy risks selecting for rifampicin resistance, and hence MDR-TB.
Methods
Patients with isoniazid-resistant pulmonary TB were recruited and followed up for 24 months. Drug-susceptibility testing was performed by Microscopic observation drug-susceptibility assay (MODS), Mycobacterial Growth Indicator Tube (MGIT) and by WGS on isolates at first presentation and in the case of re-presentation. Where MDR-TB was diagnosed, WGS was used to determine the genomic relatedness between initial and subsequent isolates. De novo emergence of MDR-TB was assumed where the genomic distance was five or fewer single nucleotide polymorphisms (SNPs) whereas reinfection with a different MDR-TB strain was assumed where the distance was 10 or more SNPs.
Results
239 patients with isoniazid-resistant pulmonary tuberculosis were recruited. Fourteen (14/239, 5.9%) patients were diagnosed with a second episode of tuberculosis that was multi-drug resistant. Six (6/239, 2.5%) were identified as having evolved MDR-TB de novo and six as having been re-infected with a different strain. In two cases the genomic distance was between 5-10 SNPs and therefore indeterminate.
Conclusions
In isoniazid-resistant TB, de novo emergence and reinfection of MDR-TB strains equally contributed to MDR development. Early diagnosis and optimal treatment of isoniazid resistant TB are urgently needed to avert the de novo emergence of MDR-TB during treatment
КОНСТРУКТИВНО-ТЕХНОЛОГИЧЕСКИЕ ОСОБЕННОСТИ СЕНСОРНЫХ УСТРОЙСТВ НА ОСНОВЕ ШИРОКОЗОННЫХ ПОЛУПРОВОДНИКОВ
- Author
- Publication venue
- БГУИР
- Publication date
- 03/06/2019
- Field of study
The development and research of new constructive solutions, materials and technologies for sensor systems production is an actual problem. The transistor with high electron mobility (HEMT) is increasingly being used in such systems. The device-technological simulation of the characteristics of HEMT, based on AlGaN / GaN using different substrate materials has implemented. The influence of the percentage of Al and Ga in combination Alх Gaх-1N on the characteristics of considered unit has studied.Разработка сенсорных систем и исследование новых конструкционых решений, материалов и технологий для их получения является актуальной задачей. Транзистор с высокой подвижностью электронов находит все большее применение в таких системах. Выполнено приборно-технологическое моделирование характеристик транзисторов с высокой подвижностью электронов, изготовленных на основе AlGaN/GaN с использованием различных материалов подложки. Исследовано влияние процентного содержания Al и Ga в соединении Alх Gaх-1N на характеристики рассматриваемого прибора
ИНТЕГРАЛЬНЫЙ ТРЕХМЕРНЫЙ МАГНИТОМЕТР НА ОСНОВЕ ДАТЧИКОВ ХОЛЛА, ИЗГОТОВЛЕННЫЙ ПО СТАНДАРТНОЙ КМОП-ТЕХНОЛОГИИ
- Author
- Publication venue
- БГУИР
- Publication date
- 03/06/2019
- Field of study
The results of the device simulation of a three-dimensional magnetometer based on Hall sensors integrated in a standard CMOS technology are presented. The Hall voltage vs magnetic field, Hall voltage vs magnetic field deviation angle, and sensitivity vs temperature curves were measured. The first-principles simulation of chalcogenide spinel CuCr2Se4 used in creation of a magnetic field concentrator was performed.Представлены результаты приборно-технологического моделирования горизонтальных и вертикальных структур датчика Холла, используемых в качестве элемента интегрального трехмерного магнитометра. Исследованы зависимости напряжения Холла от величины и угла отклонения вектора индукции магнитного поля, а также зависимости чувствительности от температуры. Проведено моделирование из первых принципов соединения халькогенидной шпинели CuCr2Se4, применяемого в качестве материала концентратора магнитного поля
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
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- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
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- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
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- Ahmad A
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- Aielli G
- Akesson TP
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- Albert J
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- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
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- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- Zeniš T
- Zerwas D
- Zevi Della Porta G
- Zhang D
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- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhu CG
- Zhu H
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- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- 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
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
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- 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 cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
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- Feng H
- Fenyuk AB
- Fenyuk AB
- Fernando W
- Fernando W
- Ferrag S
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
- Ferrari P
- Ferrari R
- Ferrari R
- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
- Ferretti C
- Fiascaris M
- Fiascaris M
- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
- Finelli KD
- Fiolhais MCN
- Fiolhais MCN
- Fiorini L
- Fiorini L
- Firan A
- Firan A
- Fischer J
- Fischer J
- Fisher MJ
- Fisher MJ
- Fitzgerald EA
- Fitzgerald EA
- Flechl M
- Flechl M
- Fleck I
- Fleck I
- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
- Fletcher GT
- Flick T
- Flick T
- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
- Fox H
- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
- Franchino S
- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
- Friedrich F
- Froidevaux D
- Froidevaux D
- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
- Galster G
- Gan KK
- Gan KK
- Gandrajula RP
- Gandrajula RP
- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
- Gaur B
- Gauthier L
- Gauthier L
- Gauzzi P
- Gauzzi P
- Gavrilenko IL
- Gavrilenko IL
- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
- Gellerstedt K
- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
- Giagu S
- Giangiobbe V
- Giangiobbe V
- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
- Gibbard B
- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
- Gillam TPS
- Gillberg D
- Gillberg D
- Gillman AR
- Gillman AR
- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
- Giordano R
- Giorgi FM
- Giorgi FM
- Giraud PF
- Giraud PF
- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
- Gjelsten BK
- Gkialas I
- Gkialas I
- Gladilin LK
- Gladilin LK
- Glasman C
- Glasman C
- Glatzer J
- Glatzer J
- Glazov A
- Glazov A
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- Godfrey J
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- Goeringer C
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- Goessling C
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- Goldfarb S
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- Golubkov D
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- Gonalo R
- Goncalo R
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- Gonzalez de la Hoz S
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- Gonzalez Parra G
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- Gonzalez BA
- Gonzalez-Sevilla S
- Gonzalez-Sevilla S
- Goossens L
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- Gorbounov PA
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- Gordon HA
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- Gorelov I
- Gorelov I
- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
- Goshaw AT
- Gostkin MI
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- Gouighri M
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- Goujdami D
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- Goulette MP
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- Goussiou AG
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- Goy C
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- Gozpinar S
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- Grabas HMX
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- Graber L
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- Grafstroem P
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- Gramstad E
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- Grancagnolo S
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- Grancagnoloa F
- Grassi V
- Grassi V
- Gratchev V
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- Gray HM
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- Graziani E
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- Grebenyuk OG
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- Greenwood ZD
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- Gregersen K
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- Gregor IM
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- Grenier P
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- Griffiths J
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- Grillo AA
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- Grimm K
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- Grinstein S
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- Gris P
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- Griso SP
- Grivaz J-F
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- Grohs JP
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- Grohsjean A
- Gross AGE
- Gross E
- Grosse-Knetter J
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- Grossi GC
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- Groth-Jensen J
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- Guan L
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- Guescini F
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- Guest D
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- Gueta O
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- Guicheney C
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- Guido E
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- Guindon S
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- Gul U
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- Gutierrez P
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- Gutschow C
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- Guttman N
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- Guyot C
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- Haddad N
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- Haefner P
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- Hajduk Z
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- Hanninger GN
- Hansen JB
- Hansen JD
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- Harenberg T
- Harkusha S
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- Harrington RD
- Harris OM
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- Hartjes F
- Harvey A
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- Hasegawa Y
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- Hawkings RJ
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- Haywood SJ
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- Henderson RCW
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- Hernandez Jimenez Y
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- Ideal E
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- Igonkina O
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- Zhemchugov A
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- Zibell A
- Zieminska D
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- Zimmermann C
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- Zurzolo G
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
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
- 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
- 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
- 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
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
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- 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
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