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PreprintarXiv licencearXiv

Liquid xenon positron target flow optimizations

Abstract

In a previous work, we explored liquid xenon (LXe)-based positron targets as an alternative to conventional high-Z metallic targets for high energy physics applications. In this paper, we apply computational fluid dynamics simulations to the LXe target and containment vessel, including entrance and exit windows. We design a flow geometry that is able to quickly move heated LXe from previous beam pulses out of the target volume without significant boil-off. While our simulations indicate that the temperature of the exit window can be kept stable, the peak energy deposition density exceeds the widely accepted damage threshold of 35 Jg−1 for ILC-like conditions.

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BibTeX
@misc{varverakis2026liquid,
  title = {{Liquid xenon positron target flow optimizations}},
  author = {Max Varverakis and Spencer Gessner and Silviu Covrig Dusa and Joseph Grames and Nathan Majernik and Sanjeev Chauhan},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2609.38614},
  eprint = {2609.38614},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.38614},
}
RIS
TY  - UNPB
TI  - Liquid xenon positron target flow optimizations
AU  - Max Varverakis
AU  - Spencer Gessner
AU  - Silviu Covrig Dusa
AU  - Joseph Grames
AU  - Nathan Majernik
AU  - Sanjeev Chauhan
PY  - 2026
DA  - 2026/10/05
PB  - arXiv
DO  - 10.48550/arxiv.2609.38614
UR  - https://arxiv.org/abs/2609.38614
AB  - In a previous work, we explored liquid xenon (LXe)-based positron targets as an alternative to conventional high-Z metallic targets for high energy physics applications. In this paper, we apply computational fluid dynamics simulations to the LXe target and containment vessel, including entrance and exit windows. We design a flow geometry that is able to quickly move heated LXe from previous beam pulses out of the target volume without significant boil-off. While our simulations indicate that the temperature of the exit window can be kept stable, the peak energy deposition density exceeds the widely accepted damage threshold of 35 Jg^−1 for ILC-like conditions.
ER  -