English

Non-Bessel-Gaussianity and Flow Harmonic Fine-Splitting

Nuclear Theory 2019-03-08 v2 High Energy Physics - Phenomenology Nuclear Experiment

Abstract

Both collision geometry and event-by-event fluctuations are encoded in the experimentally observed flow harmonic distribution p(vn)p(v_n) and 2k2k-particle cumulants cn{2k}c_n\{2k\}. In the present study, we systematically connect these observables to each other by employing Gram-Charlier A series. We quantify the deviation of p(vn)p(v_n) from Bessel-Gaussianity in terms of flow harmonic fine-splitting. Subsequently, we show that the corrected Bessel-Gaussian distribution can fit the simulated data better than the Bessel-Gaussian distribution in the more peripheral collisions. Inspired by Gram-Charlier A series, we introduce a new set of cumulants qn{2k}q_n\{2k\} that are more natural to study distributions near Bessel-Gaussian. These new cumulants are obtained from cn{2k}c_n\{2k\} where the collision geometry effect is extracted from it. By exploiting q2{2k}q_2\{2k\}, we introduce a new set of estimators for averaged ellipticity vˉ2\bar{v}_2 which are more accurate compared to v2{2k}v_2\{2k\} for k>1k>1. As another application of q2{2k}q_2\{2k\}, we show we are able to restrict the phase space of v2{4}v_2\{4\}, v2{6}v_2\{6\} and v2{8}v_2\{8\} by demanding the consistency of vˉ2\bar{v}_2 and v2{2k}v_2\{2k\} with q2{2k}q_2\{2k\} equation. The allowed phase space is a region such that v2{4}v2{6}0v_2\{4\}-v_2\{6\}\gtrsim 0 and 12v2{6}11v2{8}v2{4}012 v_2\{6\}-11v_2\{8\}-v_2\{4\}\gtrsim 0, which is compatible with the experimental observations.

Keywords

Cite

@article{arxiv.1805.04695,
  title  = {Non-Bessel-Gaussianity and Flow Harmonic Fine-Splitting},
  author = {Hadi Mehrabpour and Seyed Farid Taghavi},
  journal= {arXiv preprint arXiv:1805.04695},
  year   = {2019}
}

Comments

24 pages; 9 figures; v2: published version; minor revision of the text

R2 v1 2026-06-23T01:52:48.783Z