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1.
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Intro talk / Lamont, Mike (speaker) (CERN) ; Battistin, Michele (speaker) (CERN)
2024 - 1086. ATS Workshop; ATS Workshop 2024 External links: Talk details; Event details In : ATS Workshop 2024
2.
The SHiP experiment at the proposed CERN SPS Beam Dump Facility / SHiP Collaboration
The Search for Hidden Particles (SHiP) Collaboration has proposed a general-purpose experimental facility operating in beam-dump mode at the CERN SPS accelerator to search for light, feebly interacting particles. The SHiP experiment incorporates two complementary detectors. [...]
arXiv:2112.01487.- 2022-05-26 - 23 p. - Published in : Eur. Phys. J. C 82 (2022) 486 Fulltext: document - PDF; 2112.01487 - PDF;
3.
CERN BDF Prototype Target Operation, Removal and Autopsy Steps / Franqueira Ximenes, Rui (CERN) ; Aberle, Oliver (CERN) ; Ahdida, Claudia (CERN) ; Avigni, Pietro (CERN) ; Battistin, Michele (CERN) ; Bianchi, Laura (CERN) ; Buonocore, Luca Rosario (CERN) ; Burger, Stephane (CERN) ; Busom Descarrega, Josep (CERN) ; Calviani, Marco (CERN) et al.
The Beam Dump Facility (BDF), currently in the study phase, is a proposed general-purpose fixed target facility at CERN. Initially will host the Search for Hidden Particles (SHiP) experiment, intended to investigate the origin of dark matter and other weakly interacting particles. [...]
Geneva : JACoW, 2021 - 4 p. - Published in : JACoW IPAC 2021 (2021) 3559-3562 Fulltext: PDF;
In : 12th International Particle Accelerator Conference (IPAC 2021), Online, 24 - 28 May 2021, pp.3559-3562
4.
Track reconstruction and matching between emulsion and silicon pixel detectors for the SHiP-charm experiment / SHiP Collaboration
In July 2018 an optimization run for the proposed charm cross section measurement for SHiP was performed at the CERN SPS. A heavy, moving target instrumented with nuclear emulsion films followed by a silicon pixel tracker was installed in front of the Goliath magnet at the H4 proton beamline. [...]
arXiv:2112.11754.- 2022-03-16 - 14 p. - Published in : JINST Fulltext: 2112.11754 - PDF; document - PDF;
5.
The Forward Physics Facility at the High-Luminosity LHC / Feng, Jonathan L. (UC, Irvine) ; Kling, Felix (DESY) ; Reno, Mary Hall (Iowa U.) ; Rojo, Juan (NIKHEF, Amsterdam ; Vrije U., Amsterdam) ; Soldin, Dennis (Delaware U.) ; Anchordoqui, Luis A. (Lehman Coll.) ; Boyd, Jamie (CERN) ; Ismail, Ahmed (Oklahoma State U.) ; Harland-Lang, Lucian (Oxford U. ; Oxford U., Theor. Phys.) ; Kelly, Kevin J. (CERN) et al.
High energy collisions at the High-Luminosity Large Hadron Collider (LHC) produce a large number of particles along the beam collision axis, outside of the acceptance of existing LHC experiments. The proposed Forward Physics Facility (FPF), to be located several hundred meters from the ATLAS interaction point and shielded by concrete and rock, will host a suite of experiments to probe Standard Model (SM) processes and search for physics beyond the Standard Model (BSM) [...]
arXiv:2203.05090; UCI-TR-2022-01; CERN-PBC-Notes-2022-001; INT-PUB-22-006; BONN-TH-2022-04; FERMILAB-PUB-22-094-ND-SCD-T.- Geneva : CERN, 2023-01-20 - 413 p. - Published in : J. Phys. G 50 (2023) 030501 Fulltext: FERMILAB-PUB-22-094-ND-SCD-T - PDF; 2203.05090 - PDF; blank - PDF; Fulltext from Publisher: PDF; External links: Fermilab Library Server; eConf
In : 2021 Snowmass Summer Study, Seattle, WA, United States, 11 - 20 July 2021, pp.030501
6.
An Ultra-Low Temperature Transcritical R744 Refrigeration System for Future Detectors at CERN LHC / Barroca, Pierre (Norwegian U. Sci. Tech.) ; Hafner, Armin (Norwegian U. Sci. Tech.) ; Verlaat, Bart (CERN) ; Petagna, Paolo (CERN) ; Hulek, Wojciech (CERN) ; Zwalinski, Lukasz (CERN) ; Hanf, Pierre (CERN) ; Battistin, Michele (CERN) ; Davoine, Loic (CERN) ; Teixeira, Daniella (Cape Town U., Dept. Math.)
The cooling systems of the future tracking detectors of the ATLAS and CMS experiments at the Large Hadron Collider (LHC) at CERN will be entirely based on CO$_2$ refrigeration technology. The system is a booster refrigeration system, composed of a two stage primary part with transcritical R744 equipment and a low temperature secondary CO2 pumped loop. [...]
2021 - 15 p. - Published in : Appl. Sciences 11 (2021) 7399 Fulltext: PDF;
7. Best Practice Guide on Pollutant Dispersion Simulations with the Commercial Tool „ ANSYS Fluent“ at CERN
Reference: Poster-2021-1048
Keywords:  Large Eddy Simulation (LES), neutral Atmospheric Boundary Layer (ABL), Synthetic Turbulence Generator (STG), Monin-Obukhov similarity theory, pollutant dispersion, discrete phase model (DPM), Computational Fluid Dynamics (CFD)
Created: 2021. -7 p
Creator(s): Kauflin, Uwe; Battistin, Michele; La Mendola, Saverio; Leitl, Bernd

Large Eddy Simulations (LES) are of raising interest for numerous engineering applications in which an accurate flow prediction is necessary. This paper searches for the optimum mesh resolution in numerical simulations reliably predicting dispersion of pollutants in the lower part of the Atmospheric Boundary Layer (ABL). For the dispersion of pollutants, turbulent quantities have been assessed at several distances from the release point and compared to each other. Areas close to release points located at low altitudes are given a particular importance, because air pollutant concentrations can be too high for people present at such places. To achieve a realistic prediction of the flow and pollutant concentrations close to populated areas, LES are preferred over the Reynolds-Averaged Navier Stokes (RANS) models (Vita et al, 2020). A mesh resolution of 0.5 m is recommended at distances from the release point shorter than 40 m. Near the release point, physical effects like building downwash and horizontal plume enlargement due to the downstream wake region of buildings have a direct impact on pollutant concentrations and particle trajectories. In built-up areas at intermediary distances where the dispersion of the plume is directly influenced by buildings in their given constellation and where the energy production is high, a mesh resolution of 1.5 m is suggested. In areas where the plume is already dispersed and geometrical obstacles are rare, a mesh resolution of 3 m and more is sufficient. In these areas, the dissipation of energy and the transport of particles (mean quantities) that determine the flow are less affected by the mesh size.

Related links:
20th International Conference on Harmonisation within Atmospheric Dispersion Modelling for Regulatory Purposes
© CERN Geneva

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8.
Chapter 17: Technical infrastructure / Tavian, L (CERN) ; Battistin, M (CERN) ; Bertolasi, S (CERN) ; Bertone, C (CERN) ; Di Girolamo, B (CERN) ; Dos Santos, N (CERN) ; Foraz, K (CERN) ; Hakulinen, T (CERN) ; Mattelaer, P (CERN) ; Muffat, P (CERN) et al.
The HL-LHC technical infrastructure includes the civil engineering, the electrical distribution, the cooling & ventilation, the access & alarm system, the technical monitoring, the transport, the logistics, the storage, and the operational safety..
2020 - 28 p. - Published in : 10.23731/CYRM-2020-0010.295 Fulltext: PDF;
In : High-Luminosity Large Hadron Collider (HL-LHC): Technical design report, pp.295-322
9.
CERN Yellow Report Front Cover High-Luminosity Large Hadron Collider (HL-LHC): Technical design report / Aberle, O. ; Béjar Alonso, I (ed.) ; Brüning, O (ed.) ; Fessia, P (ed.) ; Rossi, L (ed.) ; Tavian, L (ed.) ; Zerlauth, M (ed.)
The Large Hadron Collider (LHC) is one of the largest scientific instruments ever built [...]
CERN-2020-010. - Geneva : CERN, 2020. - 390 p. (CERN Yellow Reports: Monographs ; 10/2020)


ebook
10.
Sensitivity of the SHiP experiment to dark photons decaying to a pair of charged particles / SHiP Collaboration
Dark photons are hypothetical massive vector particles that could mix with ordinary photons. The simplest theoretical model is fully characterised by only two parameters: the mass of the dark photon m$_{\gamma^{\mathrm{D}}}$ and its mixing parameter with the photon, $\varepsilon$. [...]
arXiv:2011.05115.- 2021-05-25 - 17 p. - Published in : Eur. Phys. J. C 81 (2021) 451 Article from SCOAP3: PDF; Fulltext: PDF;

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