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Subject: STAR Flow, Chirality and Vorticity PWG

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  • From: subhash <subhash AT rcf.rhic.bnl.gov>
  • To: star-fcv-l AT lists.bnl.gov
  • Cc: Sooraj Radhakrishnan <skradhakrishnan AT lbl.gov>, mfarhan_taseer AT impcas.ac.cn, Diyu Shen <dyshen AT fudan.edu.cn>, Richard Seto <seto AT ucr.edu>, Subhash Singha <subhash AT impcas.ac.cn>, Prithwish Tribedy <prithwish2005 AT gmail.com>
  • Subject: Re: [[Star-fcv-l] ] v1 v2 talk at the workshop
  • Date: Mon, 02 Dec 2024 21:27:25 +0800

Dear Shinichi, All,

If you check slide#21, you will see that the parameter C_B is controlling the baryon diffusion. C_B=0 and 1 is roughly the extreme cases with and without baryon diffusion.

Thanks and regards,
Subhash

On 2024-12-02 09:19 PM, EsumiShinIchi wrote:
Dear Sooraj and Muhammad
Thank you very much for the information.
Could you please tell me what is the difference between CB=0
and CB=1 at the page 36-39 of Muhammad’s paper proposal
slide on 13/Nov/2024?
Best regards, ShinIchi

2024/12/02 16:06、Sooraj Radhakrishnan
<skradhakrishnan AT lbl.gov>のメール:

Hi Shinichi, Prithwish,
Thanks for the slides and comments

Regarding the v1 difference and hadro comparisons, there are a
couple of points to note

1) The difference in v1 between protons and anti-protons is
explained using different initial tilted distributions for the bulk
and for transported protons. There is no independent constraint on
this and the tilts are tuned to data. In other words, the difference
in the final state v1 is carried over to the difference in initial
distributions - but without an independent constraint. So doesnt
have much predictive power or helps explaining the v1 difference we
see. Please find some more details here
https://arxiv.org/pdf/2211.15659 [2]

2) What is interesting though is that the centrality dependence is
explained through baryon diffusion. As you can see on S.37 here

https://drupal.star.bnl.gov/STAR/system/files/FCV_Comments_Measurement%20of%20system%20size%20dependence%20of%20directed%20flow%20of%20protons%20%28anti-protons%29%20at%20RHIC_2.pdf,
its the baryon diffusion that makes the difference go negative in
peripheral collisions. The initial tilt difference is such that the
proton v1 gets a positive contribution compared to anti-proton v1.
Without the diffusion the difference doesnt go negative. Not sure,
but I think its possible, constraints on the baryon diffusion can be
checked with other measurements, for example on spectra or v2

In short its the baryon inhomogeneity coupled with baryon diffusion
that produced negative delta v1 in hydro calculations. Thought that
is useful to point out

Best,
Sooraj

On Sun, Dec 1, 2024 at 6:41 PM EsumiShinIchi
<esumi.shinichi.gn AT u.tsukuba.ac.jp> wrote:

Dear Prithwish and Diyu
Thank you very much for the suggestions, ALICE D0-D0bar are
already included.
Let’s discuss whether we want to move this to Friday or not.
I’ll try to include
the Lambda results.
Best regards, ShinIchi

2024/12/02 10:48、Diyu Shen <dyshen AT fudan.edu.cn>のメール:

Hi Prithwish and ShinIchi,

I think for this topic it is necessary to include all the
results in heavy-ion experiment, not only from STAR but also from
ALICE.
So I would suggest to discuss D meson splitting observed by
ALICE after point 5.

Say D-Dbar results show 2.8 sigma splitting, despite D’s have
no electrical charge — challenges naive EM-field explanation.

Best,
Diyu


On Dec 2, 2024, at 05:05, Prithwish Tribedy
<ptribedy AT rcf.rhic.bnl.gov> wrote:

Hi ShinIchi and all,
Thank you for the excellent compilation! Should we consider
moving your v1​ talk to Friday? This would allow you to include
both public and STAR internal results, providing more flexibility
to address key issues that support or challenge EM-field
explanations. I list a few points for you to consider on both
support and apparent challenge to EM-field explanations:

1. Proton results change sign with centrality across all
energies -- supports naive EM-field expectations
2. Kaon results follow proton trends but are weaker --
supports EM-field if we assume strange quark behave differently
3. Pion results align with protons/kaons at low energies,
pion-proton-kaon all showing same trend -- challenging
transport-only explanations.
4. Above (#3) may not be the case for 200 GeV, it's unclear
if pion results change sign like protons at 200 GeV -- points to
something is missing in our understanding
5. Net-ΛΛ results are almost on top of protons, despite
Λ's have no electric charge -- challenges naive EM-field
explanation
6. Splitting increases with ΔqΔq, ΔBΔB, and ΔSΔS, if
you assume NCQ scaling holds for produced particles -- supports
both EM-field & has been explained by hydro models with baryon
inhomogeneity
8. NCQ scaling -- crucial but is hard to verify, attempt made
for produced quarks only with limited significance, but there are
proof that it does not hold for mixture of produced & transported
quarks
7. Hydro models explain proton data without EM fields --
challenging EM explanations
8. Hydro models has not demonstrated that they can explain
all PID data -- incompleteness to hydro models that challenge
EM-field explanations
9. Other models such as mean field -- I am not an expert but
it's worth touching.

Overall, this is a fascinating topic that deserves lengthy
discussion, so having it as the last talk of the day may not be
ideal.

Let me know your thoughts!

Best,
Prithwish


On 2024-12-01 12:40, EsumiShinIchi wrote:
Dear Rich, Subhash, Prithwish and all
I send you the draft of my talk on v1 splitting with materials
that
are already in public,
if you have any suggestions, please let me know. Thank you
very much
in advance.
Best regards, ShinIchi



https://drupal.star.bnl.gov/STAR/system/files/v1split_bes2star_Esumi_2024Dec04.pdf
[1]
Hi Everyone
I like Subash’s suggestion
To be clear it is now
Sooraj - v1, v2 (and v3?) of light and strange hadrons and
implications
Chengdong Han - light and hyper nuclei flow
Xingrui Gou - Global and local polarization in BES-II COL
(note that
we intend to make FXT-polarization a separate talk)
Zhiwan Xu - Chiral effects (CME related) in BES-II and 200GeV
Shinichi - v1 splitting and possible interpretations
Pretty good. Hope we can fit it all in. I think at least
Sooraj and
Shinichi’s talks should be in the open session with the
theorists
-Rich
Dear Sooraj, ShinIchi, Richard and Prithwish,
My understanding is that we were looking for candidates
whose
talks could present an unbiased perspective on topics such
as the
onset of partonic collectivity (bringing together all
viewpoints)
and the electromagnetic field (covering both electromagnetic
and
non-electromagnetic scenarios). However, we did not reach a
consensus on the EM-talk.
Therefore, may I suggest having ShinIchi give a summary talk
on
the experimental results of v1-splitting from STAR (if
possible
and if you agree), followed by a theorist? I would recommend
Sandeep Chatterjee to discuss v1 with hydrodynamics. He is
an
expert on v1 splitting due to EM (predicted D-meson v1
splitting)
and non-electromagnetic scenario with baryon. This talk
could be
part of an open session, as most of our v1 results are
public.
Although I don't see much space in agenda to accommodate
v1-splitting theory speaker, I’m cc’ing ShinIchi here
to get
his opinion on this.
The followings are rest of the talks from FCV:
Sooraj - Summarizing v1, v2 of light and strange hadrons
Chengdong Han - light and hyper nuclei flow
Xingrui Gou - Global and local polarization in BES-II COL
(note
that we intend to make FXT-polarization a separate talk)
Zhiwan Xu - Chiral effects (CME related) in BES-II and
200GeV
Thanks and regards,
Subhash


--

Sooraj Radhakrishnan

Research Scientist,
Department of Physics

Kent State University
Kent, OH 44242

Physicist Postdoctoral Affiliate Nuclear Science Division
Lawrence Berkeley National Lab
MS70R0319, One Cyclotron Road
Berkeley, CA 94720
Ph: 510-495-2473 [3]

Email: skradhakrishnan AT lbl.gov



Links:
------
[1] https://drupal.star.bnl.gov/STAR/system/files/v1split_bes2star_Esumi_2024Dec04.pdf
[2] https://urldefense.com/v3/__https://arxiv.org/pdf/2211.15659__;!!P4SdNyxKAPE!DeQFNclXH4GbLXJ1rhi2DLiNsmhQGY7esZCvfplVqI46p7yGVkd5Gs24ya0Zo28C6fHVy2tmKIvGxXqM6NGBrlu2fk9bTTc5xWNCy4iaRLk$
[3] tel:%28510%29%20495-2473



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