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  • From: tc88qy <tc88qy AT rcf.rhic.bnl.gov>
  • To: Yu-Ming Liu <a0978279515 AT gmail.com>
  • Cc: Yi Yang <yiyang0429 AT gmail.com>, STAR HardProbes PWG <star-hp-l AT lists.bnl.gov>
  • Subject: Re: [Star-hp-l] [Star-hf-l] STAR presentation by Qian Yang for SQM 2022 submitted for review
  • Date: Mon, 13 Jun 2022 09:20:58 +0800

Hi All
Please find the updated version in the same link

Qian Yang
On 2022-06-13 08:57, Yu-Ming Liu wrote:
Hi Qian,

Attached is the mass plot which Yi mentioned.

Yu-Ming

Yu-Ming Liu <a0978279515 AT gmail.com> 於 2022年6月12日 週日
上午12:00寫道:

Hi Qian,

Attached is the systematic you need in p15. As for the mass plot, I
will give you tomorrow.

Best,
Yu-Ming

tc88qy via Star-hp-l <star-hp-l AT lists.bnl.gov> 於 2022年6月11日
週六 下午10:00寫道:

Hi Sooraj
Thanks for sign-off.

P15, I will wait Yu-ming until Sunday. If no, I will only keep
low-pT
range data point.

Qian Yang

On 2022-06-11 21:43, Sooraj Radhakrishnan wrote:
Hi Qian,
Thanks for addressing the comments. I believe Yu-Ming will
provide
you with the details. But its standard EP method, but the
phi-Psi_2
bin counting being effectively continuous now.

On S.13, you still need to add the STAR Preliminary label for
the
figure.
done
On S.15, as I had suggested during last week's meeting, you
could
remove the high pT data point from the plot and focus on just
the
value in the pT integrated bin from 0.3 - 4 GeV/c. I am not
against
keeping the high pT point (with systematic uncertainties), but I
dont
think its essential for the purpose/message here.

With these comments addressed I sign off as well.

thanks
Sooraj

On Sat, Jun 11, 2022 at 6:23 PM tc88qy <tc88qy AT rcf.rhic.bnl.gov>
wrote:

Hi Sooraj

New version (v7) is updated.

Qian Yang

On 2022-06-11 00:28, Sooraj Radhakrishnan wrote:
Hi Qian,
Thanks for preparing these very nice slides. Sorry for the
late
comments. Please find some from me on your latest version (v6)

S3: Not sure, for J/Psi we should say experience evolution of
QGP
as
its color neutral. May be could indicate that its a valuable
tool
to
study the color screening in QGP?

S3: and J/Psi regeneration
done
S4: Does it is --> Is it
done
S5:Do you want to put the second bullet as a second sub-bullet
to
first?
S5: What do you refer to as the small systems here? Isobar?
But
there
has been no discussion if it yet. Also, small system is used
for
pA or
pp collisions, so might be better ti change as 'Does it have a
system
size dependence?'
done
S5: control non-flow --> reduce non-flow?
dine
S6: precisely --> with good precision
done
S6: second bullet, do you want to indicate the MB number of
events
and
HT sampled luminosity?
done for MB
S6: pin down non-flow --> reduce non-flow
done
S6: you say 'moderate sized system' here, so could avoid the
small
system discussion in the previous slide
S8: Highest precision measurement --> High precision
measurement?
done
S9: Do you want to add references for the published results?
Also
on
the following slides
done

S11: What do you mean by initial system size here? I think no
geometry
dependence and collision system dependence, as you conclude on
S9,
are
also suited here.
done
S11: Collision energy dependence was never discussed so far in
the
talk. Could be confusing here, better to remove
done
S12: You could add the formula for SP method here, similar to
the
next
slide for the EP method
It will be very busy if I put the formula here. Maybe I can put
it
in
backup if people want to discuss it .

S13: Psi_r --> Psi_n in the top formular, it should be the EP,
not
the
RP
S13: The v2_obs formula, second term sum should be only on
Background
S13: Remember during last weeks PWG meeting it was mentioned
that
there is a normalization factor for the background, is it
already
applied in the plots?
S13: You are showing the 3-4 GeV bin here, which we dont show
in
the
results. I think its better to change, there will be question
why
its
not shown
S13: I think you need STAR Preliminary label on these plots as
it
directly gives the v2
For Page13, as may you already know from the email. Barbara and
I
both
suggested Yu-ming
provide some material for this page. But I did not get a
response.
Current page is what I understand for this analysis.
Actually,I am
not
willing to show something that I am not familiar with. Because
it
will
cause confusion if people ask, but I do not know how to give an
answer.

In page 15, we do not have the sys. uncert. from HT dataset.
Results

rushed for conference always make me very nervous. We don't
have any

time to discuss about analysis details but just release result.

S16: Do you want to switch the order of the bullets here?
done
S16: is the dominant
done

thanks
Sooraj

On Fri, Jun 10, 2022 at 8:55 PM tc88qy via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hi Yi
It will be good that Yu-ming can also send me the sys.
uncert. at
the
high-pT range at P15.
I am ok with a mass from HT data at P13
Please ignore P18, I did not put sys. uncert. on this plot.
P18
will
be delete.

Qian Yang

On 2022-06-10 22:33, Yi Yang wrote:
Hi Qian,

Thanks a lot for the new version.
I have one last minor comment/suggestion for your
consideration.
- p13: It would be good to put a mass from the high tower
trigger
to
show the statistics (Yu-Ming can send 4-5 GeV at 0-80% to
you).

Question: what are the differences between p16(right) and
p18?
The
systematic uncertainties in Au+Au seem to be different.

Cheers,
Yi

On Fri, Jun 10, 2022 at 10:19 PM tc88qy
<tc88qy AT rcf.rhic.bnl.gov>
wrote:

Hi Barbara
Thanks for your sign-off

Hi All
Do you have any other comments?

Qian Yang

On 2022-06-10 19:50, Barbara Trzeciak wrote:
Hi Qian,
thanks. I sign off.

Cheers,
Barbara

On Fri, Jun 10, 2022 at 8:04 AM tc88qy
<tc88qy AT rcf.rhic.bnl.gov>
wrote:

Hi Barbar

I put the Au+Au results on slide 16 for comparison, also
the
sys.
unc.
have been added.
The same version v6 can be found in the same link.

Qian Yang

On 2022-06-10 12:48, Barbara Trzeciak wrote:
Hi Qian,
I think we should have the isobar and Au+Au comparison.
These
are
results that we have. And the isobar results at hight pT
have
worse
precision than hight pT Au+Au, right ? It's even visible
on
the
plot
where you integrate into two bins. And when you write
about
the
precision, you should be then clear the improvement is
at
low
pT,
below 4 GeV.
Also, we discussed that it would be good to have sys.
unc.
for
Au+Au
plotted.

Cheers,
Barbara

On Fri, 10 Jun 2022, 04:32 Yu-Ming Liu,
<a0978279515 AT gmail.com>
wrote:

Hi Qian,

Attached are the plots in pdf version.
I noticed that there are something wrong in formula v2
observed
in
p13. cos(2(phi-psi2)) is the correct one not
cos(2(phi)-psi2)
.
I think cosine distribution can show the particles
relate
to
the
plane angle. Particles have a trend lying in-plane and
shoot
up
from
plane.

Best,
Yu-Ming

tc88qy via Star-hp-l <star-hp-l AT lists.bnl.gov> 於
2022年6月10日
週五 上午9:48寫道:

Hi Barbara
Thanks for your comments. Please find my rely inline.
New version (v6)

Qian Yang

On 2022-06-09 22:07, Barbara Trzeciak wrote:
Hi Qian,

thanks for the updates, the slides look good to me.
Just last comments.
- There were suggestions to have a comparison of
isobar
results
in
fine binning (not the pT integrated one) in 0-80%
centrality
to
the
Au+Au results at the same centrality. You can add
the
Au+Au
on
slide
14 or 16.

I tried it in the backup slides. In the plot, high-pT
range
are
very
distracting.
It will give an impression of Au+Au have the better
precision.
That why I do not put the Au+Au results. If conveners
think
better
to
also put Au+Au results, I am fine with it.

- s15: improvement of precision is not so clear to me
for
high
pT. The
blue point seems to have actually larger uncertainty
than
the
Au+Au
point, and the blue result is in a wider pT range.
Also,
there
is no
legend for the blue point.
And that's also another reason I think it's better to
have
a
comparison of Au+Au and isobar with the original
isobar
binning.
You
say on this slide we have better precision now, but
the
shown
isobar
points are in wide bins, which of course reduces the
uncertainties.

We have different binning comparing to Au+Au. we have
three
bins
between
0.3 to 4 GeV/c. While Au+Au results have only 2 bins
below
4
GeV/c. For
each data point the error bars is comparable between
Isobar
data
and
Au+Au data.
By looking at the data, your instant feeling is that
the
measurement
precision is not improved. Just like in slide 18

- s16: that affecting -> that affects
done
- s17: no obvious system size and energy dependence
->
no
significant
collision system and energy dependence at the same
<N_part>
done
- s17: effect dominated -> effect dominates
done

And regarding your question. What we agreed during
meetings
before,
when we discussed the non-flow estimation, is that at
high
pT
the
uncertainties are anyway large and the non-flow will
not
change
the
conclusions of zero v2. So we prioritized finalizing
other
parts
of
the analysis.
For the publication, the non-flow effect will be
estimated.
ok

Cheers,
Barbara

On Thu, Jun 9, 2022 at 2:37 PM tc88qy via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hi all
Please find the new version in the same link(v5).
As Barbara suggested it would be good that Yu-ming
can
prepare
some
materials for TPC event-plane method in slide 13.
Please provide me the systematic uncertainties in
slide
14
(20-60%)and 15 (pT-integral) ASAP.

I have a concern about the TPC method. We currently
do
not
estimate
the non-flow contribution, which could be a main
source
for
high-pT
J/psi especially for a small system.
Comparing to Au+Au with similar N_part, the non-flow
is
about
0.2
for
J/psi. If I was asked about the non-flow
contribution
during
the
meeting. How do we reply? we should have a strategy
now.

For other comments please find inline.
Also to remind you, my talk is June 14, which is 5
days
to
go.
So
please send out your comments ASAP.

Yi please find my reply inline below.
Qian Yang

On 2022-06-09 14:55, Yi Yang wrote:
Hi Qian,

Thanks a lot for the updated version.

I have some comments/suggestions for your
consideration:
- p3: (top part) you should mention that "early
creation"
and
"long
lifetime" can lead you to understand the QGP
evolution,
otherwise
these two pullets seem to have no connection.
(bottom part) Make them larger? And highlight v2
with
different colors?
done
- p5: In the previous page (p4), you compare LHC
and
RHIC,
I
would
think that it would be better if you could compare
the
v2
from
LHC
here again and mention what we can learn more than
LHC.
(I understand that you want to emphasize the
systema
size on
this page, but it seems more natural compared to
the
LHC's
results.)

- p6: minimum bias + high tower
But the EPD has worse event plane resolution,
right?
Should
we mention it? Probably you can mention it orally.
done
- p7: identification --> Identification (two
places)
You should add a description on "EPD ', like the
other
three
subdetecctors.
done
- p8: More differential measurements
done
- p9 and p10: I would put "central" and
"peripheral"
in
the
title to
make it clear.
done
- p10: you have the cartoons for collisions, can
you
add
them
in
here
as well?
done
- p13: Yu-Ming also has a very nice J/psi mass
plot,
can
you
add
one
of them in this page?
- p14: I remember what we discussed on the
right-handed
plot
is
using
20 - 60% for both SP and EP from isobar (like the
left-handed
one),
right?
(Yu-Ming is working on this plot now.)
Second bullet: I am not sure I can get "Significant
non-flow
suppression by using scalar-product method" from
the
plot
(I
assume
you are talking about the right-handed one). Since
you
might
change
the right-handed plot, you might consider restating
this
bullet.
(By the way, I thought it is "known" that using the
non-flow
contribution will be smaller using scalar-product
method,
right?)

- p15: I would suggest using the pT dependent plot
for
isobar
(the
right-handed plot on p14), and please add the HT
result
here.
- Most precise v2 measurement
- It would be good to make the v2 = 0.003 +/- 0.017
+/-
0.010 in one line
We are comparing a result with zero. Then what we
want
to
answer is
a
question of yes or no. I think it would be more
suitable
to
give
audience an idea of our final conclusion.

- p16: Adding J/psi v2 from LHC in the right-handed
plot?
The reason I did not put LHC v2 result is that this
is a
short
talk.
It
will be good to more focus on our physics picture.
RAA
and
v2
at
RHIC
alone is already fruitful for this talk.
- p17: Should mention RAA first (this is the order
of
your
presentation).
Any remarks from comparing the RHIC and LHC
results?

Cheers,
Yi

On Wed, Jun 8, 2022 at 7:07 PM tc88qy via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hi Barbara and all

After a local STAR group rehearsal, I updated the
new
version
in
the
same link (v4)
Please send out your comments. Thanks

Qian Yang

On 2022-06-05 09:50, tc88qy via Star-hp-l wrote:
Hi Barbara

Thanks for your suggestion, Please find my rely
inline.
and
new
version of slides are in the same link


Qian Yang

On 2022-06-04 16:37, Barbara Trzeciak wrote:
Hi Qian,

thanks for the update. The slides are very nice,
please
find my
comments below.

Cheers,
Barbara

s3 - I would also mention CNM effects
Here I want to more focus on the hot medium
effect.
so
I
did
not
mention CNM.

s4 - How it affect -> How is it affected
done
s5 - w be established -> evolves (?)
done
s6 - v2 -> v_2
done
s8 - make the left plot larger
done
s9- dependence were shown -> dependence is
observed
done
s11 - you can emphasise here precision of the
isobar
measurement
done
s13 - it would be good to have better quality
plots
here.
Maybe
Yu-Ming can prepare example procedure figures
with
better
graphics.
Also, are these efficiency weighed, is there
some
physics
one
can
extract ?
Sure, It will be good that Yu-Ming can prepare
one
page
of
slides
for
the procedure.
The graphic is from Yu-Ming's preliminary request
slides,
I
think
it
is efficiency weighted.

s14 - I think it makes more sense to compare
0-80%
isobar
to
0-80%
Au+Au - so to have the Au+Au results on the left
plot.
But
let's
also
see what others think and we can then decide on
the
final
version
of
these plots.
Also, for the 20-60% range please keep in mind
that
Yu-Ming
might
have
his HT results early next week - in this case
please
update
the
plot.
s15 - since we have higher pT results it would
be
nice
to
have
here
also the integrated v2 for higher pT > 4 GeV/c
from
the
HT.

ok

s15 - it's not so obvious to me how much better
precision
we
have
in
isobar compared to Au+Au. Is it possible to
combine
Au+Au
for
pT
< 4
GeV/c ? Also, I think it would be better not to
combine
stat.
and
sys.
uncertainties for Au+Au results (also for the
other
comparison),
it
might show better statistical differences
between
the
two
results.

The combination is not just combine the final
physics
data
point,
But
do the extraction from the beginning.
and the stat. and sys. are all needs
re-calculation.
I did not put sys. uncertainties for the Au+Au
results,
the
error
bars
are just stat. uncertainties.
But the sys. uncertainties is small for Au+Au.

s15 - for low pT, i.e. ~< 1 GeV/c, we expect 0
v2
because
of
the
mass
effect. If it's fast, can you calculate
integrated
v2
for
pT >
1
GeV/c
?
I need to do some change to have this results.
Let's
us
see,
If
I
can
have the final results next week.

On Fri, Jun 3, 2022 at 8:54 AM tc88qy via
Star-hf-l
<star-hf-l AT lists.bnl.gov> wrote:

Hello All

As we discussed in yesterday's HP meeting. I
have
updated
the
slides to
a new version.
Please find in the same link. Your comments and
suggestion
are
welcome.

Qian Yang

On 2022-05-31 19:27, webmaster--- via Star-hf-l
wrote:
Dear star-hf-l AT lists.bnl.gov members,

Qian Yang (qianyangstar AT gmail.com) has
submitted a
material
for
a
review,
please have a look:
https://drupal.star.bnl.gov/STAR/node/59787

---
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

--

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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