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  • From: Nihar Sahoo <nihar AT rcf.rhic.bnl.gov>
  • To: Tong Liu <tong.liu AT yale.edu>
  • Cc: Yi Yang <yiyang0429 AT gmail.com>, STAR HardProbes PWG <star-hp-l AT lists.bnl.gov>
  • Subject: Re: [Star-hp-l] STAR presentation by Tong Liu for Hot Quarks 2022 submitted for review
  • Date: Thu, 06 Oct 2022 10:51:26 +0530

Hello Tong,

I don't have any further comments. I sign off.

Cheers
Nihar

On 2022-10-06 09:28, Tong Liu wrote:
Hi all,

I just posted my latest draft version to drupal. Please take a look.

Tong Liu
Ph.D. Student '2023
Physics Dept., Yale University

Tel: 203-435-2130

On Wed, Oct 5, 2022 at 5:49 PM Tong Liu <tong.liu AT yale.edu> wrote:

Hi all,

Thanks for the comments; please find my responses to some of the
points below.
I just did a rehearsal at Yale a few hours ago, and I have got some
comments there as well. I'll update my slides ASAP once I addressed
those comments.

Cheers,

Tong Liu
Ph.D. Student '2023
Physics Dept., Yale University

Tel: 203-435-2130

Nihar:

Slide13:

I think it would be good if you could put some texts mentioning the

reason for the shrinking of the uncertainty band compared to QM2022
and

also results up to smaller <Npart>. What do you think?
I don’t think it’s a good idea, since the updated version is
clearly a more correct and accurate one, and that’s the message we
want to leave people with. The QM version is what it is out of the
box, but physically speaking we clearly should use the current 42 mb
simulation, and now that we have the right version I don’t think
we should mention the earlier one. That being said, I’d be happy
to put something in backup, so that if somebody asks we can have
something prepared.
Slide14:

_ "More input needed in the next week" do you want to update
anything?

I was planning to, but I don’t think I will be able to. I was
planning on another simulation, which was cutting it very close
already, then the Yale cluster was down the whole day yesterday;
I’m going to leave it till afterwards. This physics message should
already suffice.

Barbara:

- s15: the blue text is not so well visible on the green background.

Yeah I’m not very happy about that either… but now that I just
did a rehearsal at Yale and I’m over time, I kinda want to lose
this slide altogether since it was supposed to be a transition slide
between my talk and the other low-pt spectrum talk back at QM.

Yi:

p5: Could you please tell me why there are many repeated lines for
Ru+Ru and Zr+Zr collisions on the right plot? What does that mean,
just for my own education?

That’s to stress the point that we are alternating between Ru and
Zr collision on a run-by-run bases, instead of running Ru for half
the time and then switch to Zr for the remaining half. I’ll make
it more clear in the text.

p6: Could you please remind me why there is a drop at 7 GeV on both
collisions?

That’s because the p+p collision was larger than it’s supposed
to be at the range. Statistical fluctuations.

p8, p9: What is this blue box for?

That one is just to guide the eye where I want to temporarily block
the low pt region and let people focus on the high pt. It was a
solid block until Nihar asked me to make it transparent, but now it
looks like I’m trying to highlight it instead of blocking it…

p13: Could you please remind me what Y^ch_pT is?

Here I treat the synthetic PYTHIA events as real events and
calculate its Raa. In the Yale rehearsal people have suggested to
take the pT>5GeV part off since it’s in the text anyway

On Wed, Oct 5, 2022 at 1:14 PM Yi Yang via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hi Tong,

Thanks a lot for the very nice slides. I have some minor
comments/suggestions for your consideration.
p3: the RAA formula, is it possible to let "RAA" to be in the same
line with the rest?
p5: Could you please tell me why there are many repeated lines for
Ru+Ru and Zr+Zr collisions on the right plot? What does that mean,
just for my own education?
p6: Could you please remind me why there is a drop at 7 GeV on both
collisions?
p8, p9: What is this blue box for?
p13: Could you please remind me what Y^ch_pT is?
p15: The last bullet in blue is a bit difficult to read, is it
possible to change to another color?

Cheers,
Yi

On Wed, Oct 5, 2022 at 10:32 PM Barbara Trzeciak via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hi Tong,

very nice slides, please find my additional comments below. WIth
these addressed I sign off.

Cheers,
Barbara

- s6: if p+p uncertainties are not preliminary, please add
references (we often do this on the plot itself e.g."pp
uncertainty, PRL 91, 172302 (2003)")
- s11-13: somewhere there you should explain what is "HF-PYTHIA
N_hard" and "HF-PYTHIA Y_pT^ch > 5 GeV/c" (what's the difference
between them).
- s14: same question as Nihar, are you still planning on adding
something here ? I would suggest not to add too much of the last
moment studies.
- s15: the blue text is not so well visible on the green background.

On Wed, Oct 5, 2022 at 2:31 PM Nihar Sahoo via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:
Hi Tong,

As discussed yesterday, probably we need to be careful not to change

again these Model calculations in our preliminary plots. So I would
suggest crosschecking and confirming again from your side on this
model
calculation to show at HQ2022.

Besides, I have the following comments on your last updated
presentation
slides (_1003.pdf).

Slide11:
NN -> Nucleon-Nucleon (NN)
What is b_NN? You need to describe it.

Slide13:
I think it would be good if you could put some texts mentioning the
reason for the shrinking of the uncertainty band compared to QM2022
and
also results up to smaller <Npart>. What do you think?

Slide14:
_ what is "nMPI"? Do you need to mention it somewhere?
_ "More input needed in the next week" do you want to update
anything?

Thank you
Nihar

On 2022-10-04 06:11, Tong Liu wrote:
HI Nihar,

I uploaded a new version of the slides, please take a look. As for
the
pt range in previous results, I decided to do some "subtraction"
instead of "addition" by removing the word "isobar" from the text
on
figure, so that it looks more like I'm referring to everyone.
Please
let me know what you think about it. Also I'll try to push on the
pythia MPI side, but I'm not very sure I'll be able to get
anywhere
significant beyond where I am now. Let's assume this is the
message we
are going to give, and I'll let you know if I dig up something.

Tong Liu
Ph.D. Student '2023
Physics Dept., Yale University

Tel: 203-435-2130

On Mon, Oct 3, 2022 at 9:07 AM Nihar Sahoo
<nihar AT rcf.rhic.bnl.gov>
wrote:

Hi Tong,

Please find my reply inline.
And looking forward to seeing your updated presentation slides.

On 2022-10-02 07:43, Tong Liu wrote:
Hi Nihar,

Thanks for your comments. Please find my responses below-- those
not
mentioned are applied to my slides already. However I'd like to
take
until Sunday night and hopefully make some more changes to them
before
uploading again, since we already have a lot to discuss here.

Title: good catch; I meant “high-pt”. One of the worst
places
to
have a typo :p
Slide#3:

_Do you want to say something about right side plots? Any link
to
your

analysis…please point out that.
Here it’s just an introduction to high pt hadron as a proxy to
jet
quenching effect. The plot I used is the Au+Au high-pt hadron
Raa,
which is going to be used later as well; in the text I was
really
trying to be general and not talk about any specific
measurement,
but
I might talk about it orally. If you think it’s too much
though
I
can take it off; but I’d say let’s wait till a first
rehearsal.

OK. that's fine.

Also it might be a good idea to put this slide right after the
title
slide?
Slide#4:

STAR TPC eta acceptance is |eta| < 1.4 (without iTPC)

What acceptance you are quoting here?
I'm pretty sure it's |eta|<1… Please see slide 4 in




https://indico.cern.ch/event/689846/contributions/2947105/attachments/1635225/2608617/Yichang-ChiYang.pdf
[1]
Slide#6

_Can you please remind me where do you get this "p+p
uncertainty"?

That comes from this paper:STAR Phys. Rev. Lett. 91, 172302
(2003)
Slide#10:

It is important to mention for Au+Au, d+Au, and Cu+Cu, what pT
ranges

were used?

It’s also using 5.1-10 GeV, same as isobar. The statement at
the
bottom of the graph was meant for all measurements, but
apparently
it
was not clear enough. Any suggestions?

I would add one bullet mentioning this.

Slide#12:

_ you have now two models: I) HG-PYTHIA QM2022 preliminary and
II)
new

results that you labeled as "X+X N_hard"

AFAIK, the difference between I) and II) is due to choice of
N_hard
and

N_part . Is not that?

But from your labels it seems for I) you used pT>5 GeV, and for
II)

N_hard is used but all pT range.

Is that true?
_ Why your uncertainty band for I) QM2022 preliminary results
has
been

changed? It looks wider band in your preliminary results.
OK let me explain further here… what the HG-PYTHIA model does
is, it
generates a Glauber-level collision, throw a Poisson dice and
determine how many hard collisions each NN collision has
(Nhard).
Then
it goes to PYTHIA and ask for a p+p collision with nMPI=Nhard
(yeah
that part I don’t understand yet either); then all the tracks
from
all the PYTHIA collisions are stacked together to be the
synthetic
event. Here in the plot, both options categorized events into
centralities with the “refmult” of this synthetic event, but
the
“benchmark values” are calculated in different ways: in the
“Nhard” option, the average Nhard in each centrality class
is
compared to <Nhard> of pp collisions, while in the “Y_ch”
option,
the invariant yield of 5 GeV+ tracks is used (<Ncoll> scaling is
applied in both cases, of course). I didn’t use any <N_part>
in
this
baseline beyond the x axis.
As for the change to QM prelim, that one was easy: I squeezed
much
larger statistics out of the simulation. In fact this one is
still
statistical error only, and I’ll try to get a crude
systematics
in
the next week.

Ok, I got it some extent now.

Thank you
Nihar

Slide#14:

Do you have associated systematic uncertainty for <Ncoll> and
<Npart>

scaled?

The systematic uncertainty assigned to <Ncoll> and <Npart> by
the
centrality group is VERY small, and I suspect they are
correlated
between species, so they also largely cancel out.

Tong Liu
Ph.D. Student '2023
Physics Dept., Yale University

Tel: 203-435-2130

On Sat, Oct 1, 2022 at 3:03 AM Nihar Sahoo via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hello Tong,

Please find my comments below on your nice presentation
slides.

Slide#1:
Title: System size dependence of pT hadron yield
modification…"
->
"System size dependence of hadron yield suppression…" or
something
like
that
Here, "pT hadron yield modification" sounds awkward.

Slide#3:
_Title: "…QGP probe" -> "…QGP Probe"
_"..lose energy to QGP" -> "… lose energy in QGP"
_"…RAA: comparison to p+p collisions" -> not quite right?
Define
RAA
using Au+Au and nuclear thickness function..
It is important for your previous bullet for Npart and Ncoll
_Do you want to say something about right side plots? Any link
to
your
analysis…please point out that.

Slide#4:
STAR TPC eta acceptance is |eta| < 1.4 (without iTPC)
What acceptance you are quoting here?

Slide#6
_Can you please remind me where do you get this "p+p
uncertainty"?

Slide#8-9
I would make that blue box transparent such that the data
points
can
be
visible behind.

Slide#10:
It is important to mention for Au+Au, d+Au, and Cu+Cu, what pT
ranges
were used?

Slide#12:

_ you have now two models: I) HG-PYTHIA QM2022 preliminary and
II)
new
results that you labeled as "X+X N_hard"
AFAIK, the difference between I) and II) is due to choice of
N_hard
and
N_part . Is not that?
But from your labels it seems for I) you used pT>5 GeV, and for
II)
N_hard is used but all pT range.
Is that true?

_ Why your uncertainty band for I) QM2022 preliminary results
has
been
changed? It looks wider band in your preliminary results.

Slide#14:
Do you have associated systematic uncertainty for <Ncoll> and
<Npart>
scaled?

Cheers
Nihar

On 2022-09-29 09:54, webmaster--- via Star-hp-l wrote:
Dear Star-hp-l AT lists.bnl.gov members,

Tong Liu (tong.liu AT yale.edu) has submitted a material for a
review,
please
have a look:
https://drupal.star.bnl.gov/STAR/node/61208

Deadline: 2022-10-11
---
If you have any problems with the review process, please
contact
webmaster AT www.star.bnl.gov
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https://indico.cern.ch/event/689846/contributions/2947105/attachments/1635225/2608617/Yichang-ChiYang.pdf
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