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PreprintCC BY 4.0arXiv

Λ(1520) as a probe of resonance-driven deuteron formation at the LHC

Abstract

Light nuclei such as deuterons are produced abundantly in high-energy proton-proton and nuclear collisions despite their tiny binding energies. Their production mechanism remains unresolved, as both nucleon coalescence and statistical thermal models reproduce inclusive LHC yields. We propose a direct invariant-mass observable that discriminates between these scenarios using the long-lived Λ(1520) → pK resonance. If decay protons coalesce into deuterons, the produced nuclei remain correlated with the kaon, allowing the resonance peak to be reconstructed experimentally through proxy masses, M(d/2)K, formed from kaons and half the deuteron four-momentum. Using Thermal-FIST and PYTHIA with a deuteron coalescence afterburner, we show that a M(d/2)K peak emerges only in the coalescence scenario. This observable provides a direct experimental probe of resonance-fed deuteron production and of late-stage coalescence dynamics in high-energy collisions.

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BibTeX
@misc{tripathy2026λ1520,
  title = {{$Λ$(1520) as a probe of resonance-driven deuteron formation at the LHC}},
  author = {Sushanta Tripathy and Peter Christiansen},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2606.10668},
  eprint = {2606.10668},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2606.10668},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Λ(1520) as a probe of resonance-driven deuteron formation at the LHC
AU  - Sushanta Tripathy
AU  - Peter Christiansen
PY  - 2026
DA  - 2026/10/29
PB  - arXiv
DO  - 10.48550/arxiv.2606.10668
UR  - https://arxiv.org/abs/2606.10668
AB  - Light nuclei such as deuterons are produced abundantly in high-energy proton-proton and nuclear collisions despite their tiny binding energies. Their production mechanism remains unresolved, as both nucleon coalescence and statistical thermal models reproduce inclusive LHC yields. We propose a direct invariant-mass observable that discriminates between these scenarios using the long-lived Λ(1520) → pK resonance. If decay protons coalesce into deuterons, the produced nuclei remain correlated with the kaon, allowing the resonance peak to be reconstructed experimentally through proxy masses, M_(d/2)K, formed from kaons and half the deuteron four-momentum. Using Thermal-FIST and PYTHIA with a deuteron coalescence afterburner, we show that a M_(d/2)K peak emerges only in the coalescence scenario. This observable provides a direct experimental probe of resonance-fed deuteron production and of late-stage coalescence dynamics in high-energy collisions.
ER  -