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star-fcv-l - Re: [Star-fcv-l] STAR presentation by Rishabh Sharma for Quark Matter 2023 submitted for review

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Subject: STAR Flow, Chirality and Vorticity PWG

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  • From: rishabh <rishabh AT rcf.rhic.bnl.gov>
  • To: Sooraj Radhakrishnan <skradhakrishnan AT lbl.gov>
  • Cc: "STAR Flow, Chirality and Vorticity PWG" <star-fcv-l AT lists.bnl.gov>, webmaster AT star.bnl.gov
  • Subject: Re: [Star-fcv-l] STAR presentation by Rishabh Sharma for Quark Matter 2023 submitted for review
  • Date: Tue, 29 Aug 2023 20:31:00 +0530

Dear Sooraj,

Thank you so much for your comments. Please find the revised version of slides here: https://drupal.star.bnl.gov/STAR/node/64854

It is somewhat surprising that v3 shows good mass scaling, while v2 doesn't. Is there an explanation for this?

We are reporting that within the statistical uncertainties, we observe that v3 has better mass number scaling.

From BES-I results, we had claimed that mass number scaling holds for v2 within pT/A < 1.5 GeV (PRC 94, 034908 (2016)). With BES-II we see deviations. Do you have a comparison of the BES-I and BES-II results for the different particle species?

Please find the link to the slides comparing light nuclei v2 results between BES-I and BES-II here: https://drupal.star.bnl.gov/STAR/blog/rishabh/Comparison-light-nuclei-v2-between-BES-I-and-BES-II-energies

S4: What is the equation about?

The ALICE Collaboration uses this equation to calculate vn of deuterons from vn of protons. The results are shown as blue bands in the figure.

S4: Why is the fluctuating initial conditions relevant here?

I was hoping to provide motivation for v3 studies of light nuclei.

S5: Please include EPD and ETOF also under BES-II upgrades

Implemented.

S5: track momentum and event plane?

Implemented.

S6: What is track resolution?

Changed it to track momentum resolution.

S9: What is the low pT you refer to here? Please indicate the range

Implemented.

S12: seems to be --> is in

Implemented.

S15: Can you quantify the extend of scaling? May be fit a constant to your lower plots and evaluate the value and uncertainty. This should tell you to within what percentage you can claim v3 scaling

We observe an agreement with mass number scaling within ~10% for v3 of light nuclei.

S16: seems to be --> is in

Implemented.

S17: You could also point to other light nuclei flow results from STAR (Chengdong's talks for eg). In th outlook, you can indicate the remaining energies to be measured and their relevance

Implemented.

Please let me know if you have any further suggestions for me.

Thanks and regards,
Rishabh









On 2023-08-29 02:38, Sooraj Radhakrishnan wrote:
Hi Rishabh,
Thanks for preparing the nice presentation and the interesting
results. Please find a few comments from me below

It is somewhat surprising that v3 shows good mass scaling, while v2
doesn't. Is there an explanation for this?

From BES-I results, we had claimed that mass number scaling holds for
v2 within pT/A < 1.5 GeV (PRC 94, 034908 (2016)). With BES-II we see
deviations. Do you have a comparison of the BES-I and BES-II results
for the different particle species?

S4: What is the equation about?
S4: Why is the fluctuating initial conditions relevant here?
S5: Please include EPD and ETOF also under BES-II upgrades
S5: track momentum and event plane?
S6: What is track resolution?
S9: What is the low pT you refer to here? Please indicate the range
S12: seems to be --> is in
S15: Can you quantify the extend of scaling? May be fit a constant to
your lower plots and evaluate the value and uncertainty. This should
tell you to within what percentage you can claim v3 scaling
S16: seems to be --> is in

S17: You could also point to other light nuclei flow results from STAR
(Chengdong's talks for eg). In th outlook, you can indicate the
remaining energies to be measured and their relevance

Best,
Sooraj

On Mon, Aug 28, 2023 at 7:09 AM rishabh via Star-fcv-l
<star-fcv-l AT lists.bnl.gov> wrote:

Dear Subhash,

Thank you for your comments. Please find the revised version of
slides
here: https://drupal.star.bnl.gov/STAR/node/64854.

s#4: This is for my understanding, how light nuclei v3 of has
better
sensitivity to initial fluctuation, if they are formed at later
stage?

Nucleons will propagate the initial state fluctuations if the light
nuclei are formed by the coalescence mechanism.

s#9: Could you indicate the fraction of reduction in error in
BES-II
relative to BES-I?

The improvement in statistical uncertainty varies from particle to
particle and with the pT bin. On average, we observe a 30–40%
improvement in BES-II energies compared to BES-I energies.
Instead of writing it down on the slide, I was hoping, just like in
my
SQM talk, that I could tell the fraction while delivering the talk.
Please let me know if that is okay.

s#14: At the lowest pT, I see v3 of p and d are consistent. It
might be
better if you specify the pt-range for which mass dependence is
observed.

Implemented.

s#15: You can indicate fit to proton data beside the function in
the
legend. The Y-axis scale of the bottom panels is very large, can
you
try reducing them, so the level of scaling would be clearly
visible.

Implemented.

Please let me know if you have any further suggestions for me.

Thanks and regards,
Rishabh

On 2023-08-28 13:14, subhash via Star-fcv-l wrote:
Dear Rishabh,

Nice slides. I have a few suggestions for your consideration:

s#4: This is for my understanding, how light nuclei v3 of has
better
sensitivity to initial fluctuation, if they are formed at later
stage?

s#9: Could you indicate the fraction of reduction in error in
BES-II
relative to BES-I?

s#14: At the lowest pT, I see v3 of p and d are consistent. It
might
be better if you specify the pt-range for which mass dependence is
observed.

s#15: You can indicate fit to proton data beside the function in
the
legend.
The Y-axis scale of the bottom panels is very large, can you try
reducing them, so the level of scaling would be clearly visible.


Thanks and regsrds,
Subhash


On 2023-08-24 10:01 PM, webmaster--- via Star-fcv-l wrote:
Dear star-fcv-l AT lists.bnl.gov members,

Rishabh Sharma (rishabhsharma AT students.iisertirupati.ac.in) has
submitted a
material for a review, please have a look:
https://drupal.star.bnl.gov/STAR/node/64854

Deadline: 2023-09-03
---
If you have any problems with the review process, please contact
webmaster AT www.star.bnl.gov
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--

Sooraj Radhakrishnan

Research Scientist,
Department of Physics

Kent State University
Kent, OH 44243

Physicist Postdoctoral AffiliateNuclear Science Division
Lawrence Berkeley National Lab
MS70R0319, One Cyclotron Road
Berkeley, CA 94720
Ph: 510-495-2473 [1]

Email: skradhakrishnan AT lbl.gov


Links:
------
[1] tel:%28510%29%20495-2473




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