4,938 research outputs found
KonenÀön soveltaminen pintaviilun leikkauksessa
- Author
- Publication venue
- Tampereen ammattikorkeakoulu
- Publication date
- 01/01/2005
- Field of study
FPGA-Based Tracklet Approach to Level-1 Track Finding at CMS for the HL-LHC
- Author
- Publication venue
- 'EDP Sciences'
- Publication date
- 01/01/2017
- Field of study
During the High Luminosity LHC, the CMS detector will need charged particle
tracking at the hardware trigger level to maintain a manageable trigger rate
and achieve its physics goals. The tracklet approach is a track-finding
algorithm based on a road-search algorithm that has been implemented on
commercially available FPGA technology. The tracklet algorithm has achieved
high performance in track-finding and completes tracking within 3.4 ÎŒs on a
Xilinx Virtex-7 FPGA. An overview of the algorithm and its implementation on an
FPGA is given, results are shown from a demonstrator test stand and system
performance studies are presented.Comment: Submitted to proceedings of Connecting The Dots/Intelligent Trackers
2017, Orsay, Franc
Vain hintako ratkaisee? : KestÀvÀn kehityksen huomioiminen julkisissa ateriahankinnoissa
- Author
- Publication venue
- Helsingin yliopisto
- Publication date
- 01/01/2010
- Field of study
Julkisilla ateriahankinnoilla on merkittÀvÀ asema suomalaisessa yhteiskunnassa. Julkisessa ruokahuollossa painotetaan erityisesti terveellisyyttÀ ja ravitsemusta. Julkisten ateriahankintojen kautta voidaan edistÀÀ terveellisiÀ ruokatottumuksia ja vÀhentÀÀ terveydenhuollon kustannuksia. Ruokailutottumuksilla voidaan vaikuttaa myös kestÀvÀÀn kehitykseen. Tutkimuksen tavoitteena oli selvittÀÀ kestÀvÀn kehityksen toteutumista julkisissa ateriahankinnoissa. Erityisesti huomiota kiinnitettiin kilpailutuksen toteutumiseen kestÀvÀn kehityksen nÀkökulmasta ja hinnan merkityksen analysointiin julkisissa ateriahankinnoissa. Sen lisÀksi kartoitettiin informaation toimivuutta ruokahuollossa. TÀmÀn tutkimuksessa kÀytetty aineisto perustuu loppukesÀllÀ 2008 tehtyyn kyselyyn, joka osoitettiin kuntien ruokapalveluista vastaaville henkilöille. Kysely lÀhetettiin kaikkiin Suomen kuntiin. Vastauksia saatiin 115 kunnasta, joten vastausprosentiksi muodostui 28. Vastauksista koottiin numeeriset perustiedot ja tuloksia tarkasteltiin prosentuaalisen jakauman perusteella. Kunnat jaoteltiin kÀyttÀmÀllÀ Tilastokeskuksen neljÀn kuntatyypin luokittelua: harvaan asuttu maaseutu, ydinmaaseutu, kaupunkien lÀheinen maaseutu ja kaupunki. Kuntatyyppivertailussa hyödynnettiin ei-parametrista varianssianalyysiÀ. Tutkimustulosten mukaan hinnalla oli keskeinen rooli julkisissa ateriahankinnoissa sekÀ kilpailutuskriteerinÀ ettÀ ateriapalvelujen suunnittelutyössÀ kaikissa kuntatyypeissÀ. Nykyajan palveluyhteiskunnassa tavoitellaan tehokkuutta ja taloudellisuutta, mikÀ on johtanut siihen, ettÀ myös julkisissa ateriahankinnoissa suositaan nopeasti ja helposti saatavia massatuotteita. Elintason nousun myötÀ ruoan saatavuus on lÀhes kaikille suomalaisille itsestÀÀn selvyys, mutta ruoan tuotanto ja sen alkuperÀ ovat jÀÀneet kuluttajille etÀisiksi. Tutkimustulokset osoittivat, ettÀ julkisten aterioiden taustoista kerrotaan kuluttajille varsin vÀhÀn, vaikka tÀmÀ olisi edullinen tapa nostaa julkisen ruokahuollon kestÀvyyttÀ
Measuring the Top Quark Pair Production Cross Section in ATLAS: A Cross Section Analysis on Stream Test Data Using b-Tagging
- Author
- Publication venue
- Faculty of Engineering, Lund University
- Publication date
- 01/01/2008
- Field of study
This thesis presents measurements of the top quark pair production cross section us- ing the ATLAS stream test data. The cross section is determined separately for the semileptonic mode, where events in the electron plus jets channel are isolated, and the dilepton mode, where events in the electron-muon channel are considered. The cross section is determined both with and without using tagging of b-quark jets. For the semileptonic mode, the measured cross section is Ïtt Ì = 740 ± 57 pb without b-tagging and Ïtt Ì = 788 ± 50 pb when using b-tagging. For the dilepton mode, the cross section is Ïtt Ì = 655 ± 73 pb without b-tagging and Ïtt Ì = 704 ± 86 pb when including b-tagging
Improper influence against prosecutors and judges in Finland and Sweden: Findings from two national surveys 2008
- Publication venue
- UniversitĂ€t TĂŒbingen
- Publication date
- 01/01/2016
- Field of study
The web survey was carried out in 2008, targeting all prosecutors and judges in office in Finland and Sweden. The forms of improper influence addressed in the questionnaire were harassment, threats, violence, vandalism and corruption. The reference period applied was the preceding 18 months. The survey was carried out simultaneously in Finland and in Sweden using an identical questionnaire.
Judges and prosecutors have experience of all of the listed forms of improper influences. However, the dominant forms of influence are harassment and threats.
Victimisation occurred primarily at the workplace, and only rarely in the leisure time of the respondents.
Most of the perpetrators were individuals who were not connected with criminal organisations. This is the case in particular when the victim was a judge. Occasionally, however, organised crime representatives were also observed to be involved. This was true for prosecutors in particular.
Swedish prosecutors were harassed and threatened by organised crime representatives significantly more often than Finnish prosecutors.
It was unusual that family members of the civil servants concerned were victimised, but also some such instances were reported, some of them quite serious. Again, such incidents were more likely in Sweden than in Finland.
According to the respondents, the employer organisations of the respondents had not done very much to prevent such incidents or to protect their employees from improper influences. The respondents were also of the opinion that much more should be done about the problem.
The respondents had many suggestions for improvements, some of them quite sophisticated. These included, inter alia, ideas concerning the way their work was organised, the protection of personal data, access control, and the physical design of the offices and courtrooms. Overall, the responses demonstrate that the persons involved should be consulted carefully when planning and implementing new measures to prevent improper influences and to minimize their impact
A high-performance track fitter for use in ultra-fast electronics
- Author
- Publication venue
- 'Elsevier BV'
- Publication date
- 10/07/2018
- Field of study
This article describes a new charged-particle track fitting algorithm
designed for use in high-speed electronics applications such as hardware-based
triggers in high-energy physics experiments. Following a novel technique
designed for fast electronics, the positions of the hits on the detector are
transformed before being passed to a linearized track parameter fit. This
transformation results in fitted track parameters with a very linear dependence
on the hit positions. The approach is demonstrated in a representative detector
geometry based on the CMS detector at the Large Hadron Collider. The fit is
implemented in FPGA chips and optimized for track fitting throughput and
obtains excellent track parameter performance. Such an algorithm is potentially
useful in any high-speed track-fitting application
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
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- Anh TV
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- Antonaki A
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- Antonov A
- Antos J
- Anulli F
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- 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
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- Ask S
- Asman B
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- Asquith L
- Assamagan K
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- Azuelos G
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- Bacci C
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- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
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- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
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- Bardin DY
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- Clark PJ
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- Coccaro A
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- Codina EP
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- Cogan JG
- Coggeshall J
- Cogneras E
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- Collaboration ATLAS
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- Curtis CJ
- Curull XE
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- Czirr H
- Czyczula Z
- D'Auria S
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- D'Orazio A
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- Zhemchugov A
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- Zitoun R
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- Zsenei A
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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 pTâ„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 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{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
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- Acharya BS
- Ackers M
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- Ahlen SP
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- Akesson TPA
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- Alam MA
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- Allwood-Spiers SE
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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
Constraints on the Ï_(c1) versus Ï_(c2) polarizations in proton-proton collisions at âs = 8 TeV
- Author
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- Abbiendi G.
- Abbrescia M.
- Abdullin S.
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- Acharya H.
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- Zientek M.
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- Zorbakir I.âS.
- Zorbilmez C.
- Zotto P.
- Zou D.
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- Zuo X.
- Zuolo D.
- Ălvarez FernĂĄndez A.
- Ăzçelik Ă.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 24/04/2020
- Field of study
The polarizations of promptly produced Ï_(c1) and Ï_(c2) mesons are studied using data collected by the CMS experiment at the LHC, in proton-proton collisions at âs=8ââTeV. The Ï_c states are reconstructed via their radiative decays Ï_c â J/ÏÎł, with the photons being measured through conversions to eâșeâ», which allows the two states to be well resolved. The polarizations are measured in the helicity frame, through the analysis of the Ï_(c2) to Ï_(c1) yield ratio as a function of the polar or azimuthal angle of the positive muon emitted in the J/Ï â ÎŒâșΌ⻠decay, in three bins of J/Ï transverse momentum. While no differences are seen between the two states in terms of azimuthal decay angle distributions, they are observed to have significantly different polar anisotropies. The measurement favors a scenario where at least one of the two states is strongly polarized along the helicity quantization axis, in agreement with nonrelativistic quantum chromodynamics predictions. This is the first measurement of significantly polarized quarkonia produced at high transverse momentum
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
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- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- Volpini G
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorwerk V
- Vos M
- Voss R
- Vossebeld JH
- Vranjes Milosavljevic M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vu Anh T
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlen H
- Wahrmund S
- Wakabayashi J
- Walch S
- Walder J
- Walker R
- Walkowiak W
- Wall R
- Waller P
- Walsh B
- Wang C
- Wang H
- Wang H
- Wang J
- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang X
- Warburton A
- Ward CP
- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
- Watkins PM
- Watson AT
- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh AT
- Waugh BM
- Weber MS
- Webster JS
- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Wells PS
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Wetter J
- Weydert C
- Whalen K
- White A
- White MJ
- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LA
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Williams S
- Willis W
- Willocq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wittig T
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wynne BM
- Xella S
- Xiao M
- Xie S
- Xu C
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviÄ 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 (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) 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<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
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