Raparia Deepak
MOPC06
Luminosity maximization in a small vertex region at RHIC
44
For the 2024 100 GeV proton run at RHIC, the new sPHENIX detector will require a maximum amount of collisions within ±10 cm of its central Interaction Point (IP), and preferably few or no collisions outside this range. To maximize the collisions within the vertex, a large crossing angle of up to 2 mrad will be used, operating the Large Piwinski Angle (LPA) scheme. To compensate for the reduction in luminosity from the large Piwinski angle, a β=50 cm lattice has been designed and supported with dynamic aperture simulations. To further compensate the luminosity reduction, injector studies have been performed to support up to a 45% increase in the injected intensity relative to the previous 100 GeV run in 2015.1
  • K. Hock, B. Lepore, C. Liu, D. Raparia, G. Atoian, G. Robert-Demolaize, H. Huang, J. Beebe-Wang, K. Zeno, K. Drees, M. Minty, R. Michnoff, T. Shrey, V. Schoefer, W. Fischer, X. Gu, Y. Luo
    Brookhaven National Laboratory
Paper: MOPC06
DOI: reference for this paper: 10.18429/JACoW-IPAC2024-MOPC06
About:  Received: 15 May 2024 — Revised: 20 May 2024 — Accepted: 20 May 2024 — Issue date: 01 Jul 2024
Cite: reference for this paper using: BibTeX, LaTeX, Text/Word, RIS, EndNote
MOPC07
RHIC Au-Au operation at 100 GeV in Run 23
48
The Relativistic Heavy Ion Collider (RHIC) Run 23 program consisted of collisions of 100 GeV gold beams at two collision points for the first time since 2016; the sPHENIX collaboration used the beam to commission their new detector systems while STAR took physics data. Completion of sPHENIX construction pushed the start of the run to May, forcing the collider complex to operate over the summer months and incurring lower than normal availability due to heat and power dip related problems. Issues with dynamic pressure rise during acceleration through transition resulted in a slower ramp up of intensity compared to prior years. Finally, a failure of a warm-to-cold current lead interface in the valve box for the Main Magnet power supply forced the run to end. This paper will discuss the progress made by each experiment and the failure mode, repair and mitigation efforts in preparation for Run 24.
  • T. Shrey, A. Zaltsman, C. Mi, C. Liu, D. Raparia, F. Severino, G. Marr, G. Robert-Demolaize, H. Huang, I. Blackler, J. Escallier, J. Morris, J. Sandberg, K. Zeno, K. Hughes, K. Mernick, K. Hock, K. Yip, K. Drees, M. Valette, M. Minty, R. Hulsart, R. Michnoff, R. Feder, V. Schoefer, W. Fischer
    Brookhaven National Laboratory
Paper: MOPC07
DOI: reference for this paper: 10.18429/JACoW-IPAC2024-MOPC07
About:  Received: 15 May 2024 — Revised: 23 May 2024 — Accepted: 23 May 2024 — Issue date: 01 Jul 2024
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WEPS01
High-intensity polarized and unpolarized H⁻ sources development and operation at BNL
2691
The AGS-RHIC injector complex includes H- ion sources at 35 keV, 750 keV RFQ and 200 MeV Linac. This report will focus on the recent upgrade of the 35 KeV Low Energy Beam Transport (LEBT) with three sources: two high-intensity magnetron H- sources and an Optically Pumped Polarized Ion Source (OPPIS) polarized H- source. There were still significant beam intensity losses in the 8 m long OPPIS transport line due to H- stripping, therefore, to meet the demand for the higher beam intensity in the 2024 polarized run, the OPPIS LEBT length was reduced by about two meters. Another possibility for increasing beam intensity is to increase the beam pulse width. The sources performance and operation in Run-2024 will be presented.
  • A. Cannavó, A. Zelenski, B. Snyder, D. Raparia, G. Atoian, J. Ritter, T. Lehn
    Brookhaven National Laboratory
Paper: WEPS01
DOI: reference for this paper: 10.18429/JACoW-IPAC2024-WEPS01
About:  Received: 15 May 2024 — Revised: 22 May 2024 — Accepted: 22 May 2024 — Issue date: 01 Jul 2024
Cite: reference for this paper using: BibTeX, LaTeX, Text/Word, RIS, EndNote