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CERN Document Server 28 notices trouvées  1 - 10suivantfin  aller vers la notice: La recherche a duré 0.69 secondes. 
1.
The Study of a European Neutrino Factory Complex / Gruber, P ; Aleksa, M ; Aman, JF ; Autin, B ; Baldy, JL ; Benedikt, M ; Benett, R ; Bemardon, A ; Blondel, A ; Bongardt, K et al.
CERN-PS-2002-080-PP.- Geneva : CERN, 2002 - 73 p. Fulltext: PDF;
Notice détaillée - Notices similaires
2.
Phase Rotation, Cooling And Acceleration Of Muon Beams: A Comparison Of Different Approaches / Franchetti, G. (CERN) ; Gilardoni, Simone S. (CERN) ; Gruber, P. (CERN) ; Hanke, K. (CERN) ; Haseroth, H. (CERN) ; Holzer, E.B. (CERN) ; Kuchler, D. (CERN) ; Lombardi, A.M. (CERN) ; Scrivens, R. (CERN)
Experimental and theoretical activities are underway at CERN [1] with the aim of examining the feasibility of a very-high-flux neutrino source (»1021 neutrinos/year). In the present scheme, a high-power proton beam (some 4 MW) bombards a target where pions are produced. [...]
physics/0008065; LINAC2000-THC17; CERN-NUFACT-Note-41; CERN-PS-2000-054.- Geneva : CERN, 2000 - 3 p. - Published in : eConf C: 000821 (2000) , pp. THC17
- Published in : , pp. 893-895 Fulltext: arXiv:physics_0008065 - PDF; CERN-PS-2000-054 - PDF;
In : 20th International Linear Accelerator Conference, Monterey, CA, USA, 21 - 25 Aug 2000, pp.THC17
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3.
LLAMA: The Low Level Abstraction For Memory Access / Gruber, Bernhard Manfred (CERN ; Dresden, Tech. U. ; CASUS) ; Amadio, Guilherme (CERN) ; Blomer, Jakob (CERN) ; Matthes, Alexander (HZDR, Dresden) ; Widera, René (HZDR, Dresden) ; Bussmann, Michael (CASUS)
The performance gap between CPU and memory widens continuously. Choosing the best memory layout for each hardware architecture is increasingly important as more and more programs become memory bound. [...]
arXiv:2106.04284.- 2023-01-01 - 39 p. - Published in : Softw Pract Exper. 2022 (2022) 1- 27 Fulltext: PDF; External links: 00011 Throughput comparison of several copy implementations between different mappings. The particle record dimension consists of 7 \lstinline{float}s. The event record dimension consists of the first 100 \lstinline{int32}s, \lstinline{int64}s, \lstinline{float}s, \lstinline{byte}s and \lstinline{bool}s as they occur in an internal event dataset from the CMS detector at CERN (cf. the example on LLAMA's GitHub repository for the full definition). The (p) versions are parallel. The (r) versions read contiguously, whereas the (w) versions write contiguously. For the field-wise naive and \lstinline{std::copy}, the throughput depends a lot on the field types of the record dimension. The \lstinline{aosoa_copy} outperforms both of them in most cases, single- and multithreaded.; 00009 Throughput comparison of several copy implementations between different mappings. The particle record dimension consists of 7 \lstinline{float}s. The event record dimension consists of the first 100 \lstinline{int32}s, \lstinline{int64}s, \lstinline{float}s, \lstinline{byte}s and \lstinline{bool}s as they occur in an internal event dataset from the CMS detector at CERN (cf. the example on LLAMA's GitHub repository for the full definition). The (p) versions are parallel. The (r) versions read contiguously, whereas the (w) versions write contiguously. For the field-wise naive and \lstinline{std::copy}, the throughput depends a lot on the field types of the record dimension. The \lstinline{aosoa_copy} outperforms both of them in most cases, single- and multithreaded.; 00010 Throughput comparison of several copy implementations between different mappings. The particle record dimension consists of 7 \lstinline{float}s. The event record dimension consists of the first 100 \lstinline{int32}s, \lstinline{int64}s, \lstinline{float}s, \lstinline{byte}s and \lstinline{bool}s as they occur in an internal event dataset from the CMS detector at CERN (cf. the example on LLAMA's GitHub repository for the full definition). The (p) versions are parallel. The (r) versions read contiguously, whereas the (w) versions write contiguously. For the field-wise naive and \lstinline{std::copy}, the throughput depends a lot on the field types of the record dimension. The \lstinline{aosoa_copy} outperforms both of them in most cases, single- and multithreaded.; 00008 Throughput comparison of several copy implementations between different mappings. The particle record dimension consists of 7 \lstinline{float}s. The event record dimension consists of the first 100 \lstinline{int32}s, \lstinline{int64}s, \lstinline{float}s, \lstinline{byte}s and \lstinline{bool}s as they occur in an internal event dataset from the CMS detector at CERN (cf. the example on LLAMA's GitHub repository for the full definition). The (p) versions are parallel. The (r) versions read contiguously, whereas the (w) versions write contiguously. For the field-wise naive and \lstinline{std::copy}, the throughput depends a lot on the field types of the record dimension. The \lstinline{aosoa_copy} outperforms both of them in most cases, single- and multithreaded.; 00000 Conceptual overview of LLAMA.; 00001 Overview of the C++ library components of LLAMA.; 00007 : Caption not extracted; 00004 : Move with 256Mi particles; 00005 : Caption not extracted; 00002 Concept of LLAMA mappings. A mapping defines how a record and array dimension index tuple is translated into a blob number and offset.; 00006 : Move with 256Mi particles; 00003 : Caption not extracted
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4.
The MICE Muon Beam on ISIS and the beam-line instrumentation of the Muon Ionization Cooling Experiment / MICE Collaboration
The international Muon Ionization Cooling Experiment (MICE), which is under construction at the Rutherford Appleton Laboratory (RAL), will demonstrate the principle of ionization cooling as a technique for the reduction of the phase-space volume occupied by a muon beam. Ionization cooling channels are required for the Neutrino Factory and the Muon Collider. [...]
arXiv:1203.4089; FERMILAB-PUB-12-886-APC.- 2012 - 41 p. - Published in : JINST 7 (2012) P05009 Fermilab Library Server: PDF; Fulltext: PDF; IOP Open Access article: PDF; External link: Fermilab Library Server (fulltext available)
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5.
Measurement of the production cross-sections of $\pi^\pm$ in p-C and $\pi^\pm$-C interactions at 12 GeV/c / HARP Collaboration
The results of the measurements of the double-differential production cross-sections of pions in p-C and $\pi^\pm$-C interactions using the forward spectrometer of the HARP experiment are presented. The incident particles are 12 GeV/c protons and charged pions directed onto a carbon target with a thickness of 5% of a nuclear interaction length. [...]
arXiv:0802.0657; CERN-PH-EP-2008-006; CERN-PH-EP-2008-006.- Geneva : CERN, 2008 - 25 p. - Published in : Astropart. Phys. 29 (2008) 257-281 Fulltext: arXiv:0802.0657 - PDF; phep-2008-006 - PDF; External link: Fulltext
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6.
Particle identification algorithms for the HARP forward spectrometer / Catanesi, M G (Bari U. ; INFN, Bari) ; Catanesi, M G ; Radicioni, E ; Edgecock, R ; Ellis, M ; Robbins, S ; Soler, F J P ; Go Xling, C ; Bunyatov, S ; Chelkov, G et al.
The particle identification (PID) methods used for the calculation of secondary pion yields with the HARP forward spectrometer are presented. Information from time of flight and Cherenkov detectors is combined using likelihood techniques. [...]
2007 - Published in : Nucl. Instrum. Methods Phys. Res., A 572 (2007) 899-921
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7.
The HARP detector at the CERN PS / Catanesi, M G ; Muciaccia, M T ; Radicioni, E ; Simone, S ; Edgecock, R ; Ellis, M ; Robbins, S ; Soler, F J P ; Gößling, C ; Mass, M et al.
HARP is a high-statistics, large solid angle experiment to measure hadron production using proton and pion beams with momenta between 1.5 and 15 GeV/c impinging on many different solid and liquid targets from low to high Z. The experiment, located in the T9 beam of the CERN PS, took data in 2001 and 2002. [...]
2007 - Published in : Nucl. Instrum. Methods Phys. Res., A 571 (2007) 527-561
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8.
Large-angle production of charged pions by 3 GeV/c - 12 GeV/c protons on carbon, copper and tin targets / HARP Collaboration
A measurement of the double-differential $\pi^{\pm}$ production cross-section in proton--carbon, proton--copper and proton--tin collisions in the range of pion momentum $100 \MeVc \leq p < 800 \MeVc$ and angle $0.35 \rad \le \theta <2.15 \rad$ is presented. The data were taken with the HARP detector in the T9 beam line of the CERN PS. [...]
arXiv:0709.3464.- 2008 - 36 p. - Published in : Eur. Phys. J. C 53 (2008) 177-204 Fulltext: PDF; Springer Open Access article: PDF; External link: DURHAM
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9.
Measurement of the production of charged pions by protons on a tantalum target / HARP Collaboration
A measurement of the double-differential cross-section for the production of charged pions in proton--tantalum collisions emitted at large angles from the incoming beam direction is presented. The data were taken in 2002 with the HARP detector in the T9 beam line of the CERN PS. [...]
arXiv:0706.1600.- 2007 - 49 p. - Published in : Eur. Phys. J. C 51 (2007) 787-824 Fulltext: PDF; External link: DURHAM
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10.
Measurement of the production cross-section of positive pions in the collision of 8.9 GeV/c protons on beryllium / HARP Collaboration
The double-differential production cross-section of positive pions, $d^2\sigma^{\pi^{+}}/dpd\Omega$, measured in the HARP experiment is presented. The incident particles are 8.9 \GeVc protons directed onto a beryllium target with a nominal thickness of 5% of a nuclear interaction length. [...]
hep-ex/0702024.- 2007 - 35 p. - Published in : Eur. Phys. J. C 52 (2007) 29-53 Access to fulltext document: PDF; Fulltext: PDF; External link: DURHAM
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CERN Document Server : 28 notices trouvées   1 - 10suivantfin  aller vers la notice:
Voir aussi: noms d'auteurs similaires
2 Gruber, P M
9 Gruber, P.
3 Gruber, Peter
2 Gruber, Peter M
2 Gruber, Petra
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