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  • From: Nihar Sahoo <nihar AT rcf.rhic.bnl.gov>
  • To: Rosi Reed <rosijreed AT lehigh.edu>
  • Cc: STAR HardProbes PWG <star-hp-l AT lists.bnl.gov>
  • Subject: Re: [Star-hp-l] STAR presentation by Tristan Protzman for Hot Quarks 2022 submitted for review
  • Date: Mon, 10 Oct 2022 11:09:04 +0530

Hello Tristan,

Please find my comments on your v6 and additional comment below.

1) Have you updated your remaining sys uncertainty that we were
waiting
for?
No, my jobs are still processing, they seem to be moving through
rather slowly compared to what I am used to. I took a quick look at
what has been produced so far and it seems consistent with the
existing measurement.
Can you please show some results/plots to support that you mentioned here "seems consistent with the existing measurement"?

Slide19:
_ "Evidence of a non-zero v_2^ch jet in a medium sized system!" -> "Indication of non-zero v_2^ch jet with R=0.2 in Isobar collisions at RHIC"

_ "In general agreement with…ALICE Pb+Pb vch jet 2…Despite the very different system kinematics"
-> "STAR Preliminary results hint the same v2^ch_jet with ALICE"
And make the following two sub bullets
1. Despite different jet pT range and collision system
2. Further systematic study is ongoing

Slide20:
_I think this slide is unnecessary and you can put in backup. But it is up to you if you want to have more discuss on your results at this preliminary stage.

Slide21 conclusion slide:
This slide should conclude your results as I mention in Slide19


Cheers
Nihar



On 2022-10-10 01:13, Rosi Reed wrote:
Hi Tristan,
This is looking quite nice. Probably you should mention Tong's
results somewhere (I believe he's the talk right before you). I
haven't been following - are there any other isobar results coming out
this week? (this question to everyone)

Slide 3: fragmets -> fragments
Slide 5: I'd remove "uncorrelated" from the background, since the
background is indirectly correlated through the EP.

Slide 6: select on jets -> select jets
Slide 8: Indicate this is Au+Au, I know it's written in the legend but
it might be easy for someone to miss.

Slide 9: each jet passed through -> each jet interacted with
collision -> collisions
Slide 13: My mistake - complementary should be complementarity. I
shouldn't make comments before coffee.
Perhaps include the total number of collisions? That could be
interesting.
Slide 14: Include the trigger threshold in GeV.
Slide 20: It's not complete, so medium sized systems will be very
useful. Or something like this.

Cheers,
Rosi

On Sun, Oct 9, 2022 at 1:22 PM Tristan Protzman <tlp220 AT lehigh.edu>
wrote:

Hello Nihar,

An updated draft has been uploaded. I believe I have kept up on the
conversation between you and Rosi while I was working on these
changes, please let me know if I missed something.

1) Have you updated your remaining sys uncertainty that we were
waiting
for?
No, my jobs are still processing, they seem to be moving through
rather slowly compared to what I am used to. I took a quick look at
what has been produced so far and it seems consistent with the
existing measurement.

_2)Comments on Figures:_
_Slide18 fig:_
_1. You don't need to put description of "ALCIE sys bands like
correlated_
_and uncorrelated etc" One green circle is enough to represent
ALICE_
_results._
_2. Please include instead STAR sys box's description in legend_
I have added a label for STARs systematics, but did not remove the
ALICE legend

_Slide17 fig:_
__ Can you include v2 value (with uncertainty) in this figure that
you_
_get from the fitting?_
It was a deliberate choice not to since the v2 of the fit is the
observed v2, not corrected for the event plane resolution. I felt
it would be confusing to quote one value there and then on the next
slide show a different value for the bin.

_3) Additional comment:_
_I think EPD is used for the first time in jet v2 measurement._
_It would be good to include EP resolution plot that you get from
this_
_measurement._
_For that you can combine _slide15-16_ to make a story for EPD and
EP_
_calculation._
I had moved the slide on EPD resolution to the backup for time, what
I think I could do is move the diagram of the EPD on slide 16 to
slide 15, and instead have a resolution plot in its place.

I will remake the resolution plot to better fit the space available,
but this will take a little time soI leave it as is for now.

_4) Slide18(in _vesrion4_):_
_"Suggests that jet modification is path-length dependent, even in
medium_
_sized systems!"_
_Can you please elaborate how we draw the conclusion of " jet_
_modification is path-length dependent" in Isobar ?_
_We don't have any hard-core jet RAA/RCP measurement in isobar. Do
we_
have_?_
Throughout this talk I have been motivating the idea that if we have
a non-zero jet v2, then the jets in plane and out of plane (which
experience a different length through the medium) are modified
different amounts. Hence, path length dependent jet modification.

_We can only say so far (from this preliminary study) what you have_
_mentioned in conclusion slide19 (with slight modification
"hint…")_
_"Hint of non-zero v2^ch jet is observed in a medium sized system "_

_Please bring this statement in slide18_
Changed the last bullet to "Evidence of non-zero v2 in a medium
sized system"

_5) Slide19(v4 version)_
__"A very different system!" -> "A very different kinematic range
and_
_system size"_
Changed.
__"v2ch jet is observed despite the introduced surface bias" ->
"v2ch jet_
_is observed despite the possible surface bias"_
Changed
_ I would be careful on this statement, as I mentioned we have
not done_
_any dijet Aj study in Isobar to _support of the_ surfaced bias jet_
_selection. It could be correct but we have not done any measurement
so_
_we should _abstain mentioning_ this._
_If you want, _then need_ to do Aj measurement for this hard core
jet_
_selection in Isobar._
I have changed the wording as suggested to be less strong, however I
feel it is still important to bring up. Either there is a surface
bias introduced, in which case it is a little surprising we observed
jet v2 at all, or there isn't a surface bias like we see in Au+Au,
in which case our understanding of jet measurements is incomplete.

__"Our picture of jet quenching is not complete - there is still
much to_
_discover"_
_ Sounds a vague statement. Please mention 1) what is not
completed_
_relating to jet quenching? 2) what do you think that needs to be_
_discovered? Please _elaborate this
Elaborated to explain that it seems jet v2 may not be only a path
length effect, as it is in our usual picture of jet quenching. _._

Slide:2
_Second bullet seems out of context here. Coupling is large at low
Q^2
then why is it relevant for the QGP and your jet anisotropy
measurements? This part is not clear here.
It motivates the need for a perturbative object like jets to probe
what we actually want to study, the QGP. Changed text to clarify.

Still it is not clear and confusing for 1st and 3rd bullets.
If you want to motivate jet (which pQCD calculable) and this is used
to
probe QGP (which is asymptotic region of coupling); then what is the
point to mention "alpha_s ~ O(1) at low Q^2."
I would suggest to rephrase;
"Since running coupling is asymptotically small at high Q^2, pQCD
calculable probes are used to study the QGP medium"
Then you don't need 3rd bullet.

The point of mentioning the strong coupling at low Q2 is to explain
why we cannot simply use perturbative calculations to study the QGP,
and instead need a different probe like jets. If there is nothing
factually wrong, I would prefer to keep this.

Slide4 (current v4)
__ "We are interested in understanding the path-length dependence
of_
_these processes" -> "We are interested in understanding the
path-length_
_dependence of jet quenching"_
Changed
__"Both collisional and radiative" -> "Both collisional and
radiative_
_energy loss" or "Parton energy loss via both collisional and
radiative_
_processes"_
Changed

_Slide 5_
__"Soft processes produce a fluctuating background" what is that_
_background? Is it track or _combinatoric_ jet background?_
I'm not quite sure I understand what you are asking, it is the
tracks
from soft processes which produce the combinatorial jet
background, so
I suppose both?
Then it would good to mention, "Soft processes produce a fluctuating
uncorrelated background for jet measurement in heavy-ion collisions"
Here "uncorrelated" is important.
Added uncorrelated.

Slide5 (current v4_), right figure is from STAR data or any model?
No_
_description mentioned there._
Added description

slide8(in v4)
_ we are doing inclusive hard-core jet v2 measurement here. Is not
it?
_I am not convinced to motivate with dijet measurement here. Are we
going to do any dijet measurement in isobar?
_Selecting a hard-core jet may not imply you select surface biased
jet.
For that you need to show the same dijet Aj measurement in isobar
like
in Au+Au. If you have any result to demonstrate that you are
selecting
surfaced bias jet in Isobar, please show those results.
I think we have not done that study.

I believe Rosi's comments address my thoughts on this as well

_Slide 12_
I am stating that although it may be described using the same
framework as flow measurements, jet v2 is a different process.

I would suggest to give a clear idea what could be that different
process, For example...?
Otherwise do not create unnecessary doubt or make statement just for
a
buzz?

Rephrased

Cheers,

Tristan

On Sun, Oct 9, 2022 at 12:03 PM Nihar Sahoo via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hello Rosi,

Thank you for your reply.
My overall suggestion on Tristan's presentation is that due to
limited
time, let's only focus on the observation from this preliminary
results.
for Any physics conclusion we need time to understand and discuss
for
that we don't have time now.

Please find my response inline.

On 2022-10-09 20:09, Rosi Reed wrote:
Hi Nihar,
Just a few comments here:
1. You don't need to put description of "ALCIE sys bands like
correlated
and uncorrelated etc" One green circle is enough to represent
ALICE
results.
I think it's better to keep their descriptions here - otherwise
it is
STAR telling ALICE what their data should look like. The
correlated
vs uncorrelated is important for making a statement about the
comparison, if everything was uncorrelated the significance of
the
apparent agreement is much stronger, so I would be worried that
by
changing their results we would be misleading our audience a
little on
this very interesting result.

That is fine and it is just PAs choice.


Can you please elaborate how we draw the conclusion of " jet
modification is path-length dependent" in Isobar ?
We don't have any hard-core jet RAA/RCP measurement in isobar.
Do we
have?

We don't have RAA/RCP, but I don't see why this is necessary for
the
statement, we know that jet RAA will < 1 in the isobar system
due to
other measurements made by STAR (and PHENIX). You could have a
path-length dependent modification that averages out to
precisely RAA
= 1, though that would be unlikely in a collision with a center
of
mass energy greater than ~40 GeV judging by the RCP measurement
made
by Stephen from the BES data. With a signal at 3.5 sigma, we
can
state that there is evidence for non-zero jet v2 at RHIC. There
must
be some geometrical physics process causing this - if there was
not,
then the v2 would be close to zero. In the paradigm of heavy
ion
collisions we have a choice of initial state effects (so some
MPI),
pressure gradients and path-length dependent suppression (i.e
LPM
effect). We know we can exclude the middle term due to the high
Q^2
and the QGP formation time. There is no evidence for the former
term
as of yet, so within the paradigm of jets in heavy ion
collisions the
latter is the assumption for the interpretation of the data that
remains. I certainly don't think we can overturn a decades long
paradigm on the basis of a single statistics hungry measurement.


Sorry, I still don't understand your argument here.
We don't have very good information about jet RAA/RCP in "isobar"
collision mainly kinematic range in pT etc. I know we have BES RCP
which
is in Au+Au collision.
Here the system size is smaller compared to Au+AU.
Unless we measure Jet RAA/RCP in Isobar we should not make any
conclusion/statement based on what we know from Au+Au measurement.

But it is fine for me with the statement "there is evidence for
non-zero
jet v2 at RHIC in Isobar collision."
We can't say anything more on "jet modification is path-length
dependent" in Isobar collisions; simply because in this
measurement we
have not done any jet modification study.
For that we need to explicitly perform jet suppression study for
this
system.

So I suggest to remove "Suggests that jet modification is
path-length
dependent, even in medium sized systems!" on slide#18.
and replacing this "there is evidence for non-zero jet v2 at RHIC
in
Isobar collision." is very important conclusion here which is
apparent
from the figure.
A further study is warranted to comment on path-length dependent
jet
modification which we can discuss after HQ.

I would be careful on this statement, as I mentioned we have
not
done
any dijet Aj study in Isobar to support of the surfaced bias
jet
selection. It could be correct but we have not done any
measurement
so
we should abstain mentioning this.

I don't believe that we have to measure AJ to state this basic
fact of
nuclear physics. The surface bias of selecting hard
fragmentation has
been discussed since the earliest papers on jet quenching



(https://physics.fjfi.cvut.cz/files/predmety/02RQGP/zs1617/GyulassyPluemer.pdf
[1]
[1] for example), and has been mentioned many times by STAR
itself in
a variety of high pt and jet based measurements. In fact, not
mentioning it after STAR spent so much time discussing jet
geometry
evolution in the earlier AJ measurements would actually be akin
to
walking back our earlier statements since we're using the same
process
in this measurement.

As I mentioned above, we have not done any Aj measurement in this
small
system Isobar collisions.
And we do not have enough time to have this discussion before HQ
which
we can discuss after the conf.
Using same process/cuts may not imply the jets we find are also
surfaced
biased in small system, for this concern we can discuss in details

later.

I have also made some comments on Tristan's talk that he'll
follow up
on, and the official practice of his talk before the council
member
will happen on Monday so there will be a little bit of tweaking,
even
after he submits a draft v5. One quick point on the
uncertainties,
Rongrong was quite correct in the meeting on Thursday that the
uncertainty on the tracking efficiency only plays a role in the
uncertainty if we're unfolding. So there are no further effects
that
will change the systematics for this non-unfolded measurement -
rather
we're waiting on this as a last cross-check.

Looking forward to seeing Tristan's updated version.

Cheers
Nihar

Cheers,
Rosi

On Sun, Oct 9, 2022 at 4:14 AM Nihar Sahoo via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hello Tristan,

Thank you for implementing my comments and your reply.
Please find my further comments and reply to your response.
All my comments on your recent version (v4).
Please don't remove your old version; that can be done after
finishing
our discussion otherwise it is difficult to follow the slide
numbers

with new version.

1) Have you updated your remaining sys uncertainty that we were
waiting
for?

2)Comments on Figures:
Slide18 fig:
1. You don't need to put description of "ALCIE sys bands like
correlated
and uncorrelated etc" One green circle is enough to represent
ALICE
results.
2. Please include instead STAR sys box's description in legend

Slide17 fig:
_ Can you include v2 value (with uncertainty) in this figure
that
you
get from the fitting?

3) Additional comment:
I think EPD is used for the first time in jet v2 measurement.
It would be good to include EP resolution plot that you get
from
this
measurement.
For that you can combine slide15-16 to make a story for EPD and
EP
calculation.

4) Slide18(in vesrion4):
"Suggests that jet modification is path-length dependent, even
in
medium
sized systems!"
Can you please elaborate how we draw the conclusion of " jet
modification is path-length dependent" in Isobar ?
We don't have any hard-core jet RAA/RCP measurement in isobar.
Do we

have?

We can only say so far (from this preliminary study) what you
have
mentioned in conclusion slide19 (with slight modification
"hint…")
"Hint of non-zero v2^ch jet is observed in a medium sized
system "

Please bring this statement in slide18

5) Slide19(v4 version)
_"A very different system!" -> "A very different kinematic
range and

system size"
_"v2ch jet is observed despite the introduced surface bias" ->
"v2ch
jet
is observed despite the possible surface bias"
I would be careful on this statement, as I mentioned we have
not
done
any dijet Aj study in Isobar to support of the surfaced bias
jet
selection. It could be correct but we have not done any
measurement
so
we should abstain mentioning this.
If you want, then need to do Aj measurement for this hard core
jet
selection in Isobar.

_"Our picture of jet quenching is not complete - there is still
much
to
discover"
Sounds a vague statement. Please mention 1) what is not
completed
relating to jet quenching? 2) what do you think that needs to
be
discovered? Please elaborate this.

Remaining reply can be found inline.

On 2022-10-09 07:56, Tristan Protzman via Star-hp-l wrote:
Hello Nihar,

A new draft has been uploaded to Drupal.

Note: it should be written as $p$+$p$ and $p$+Au, etc, which
is
different from the guidance.

Fixed.

Slide:2
_Second bullet seems out of context here. Coupling is large at
low
Q^2
then why is it relevant for the QGP and your jet anisotropy
measurements? This part is not clear here.
It motivates the need for a perturbative object like jets to
probe
what we actually want to study, the QGP. Changed text to
clarify.

Still it is not clear and confusing for 1st and 3rd bullets.
If you want to motivate jet (which pQCD calculable) and this is
used
to
probe QGP (which is asymptotic region of coupling); then what
is the

point to mention "alpha_s ~ O(1) at low Q^2."
I would suggest to rephrase;
"Since running coupling is asymptotically small at high Q^2,
pQCD
calculable probes are used to study the QGP medium"
Then you don't need 3rd bullet.


_ Give reference to the running coupling plot. And you could
replace
with most updated version where LHC measurements (very highQ2
region)
are included if you want to start with it.
Changed.

__GIve a reference or credit for left cartoon._

Figure removed, I felt it did not add to the message.

Slide:4
_3rd bullet: "Leads to path length…" this is not the only
effect;
it
could be various other contributions like color factor, Temp
of
QGP,
initial gluon density, etc. But you need to mention Your
motivation is
to study "path length dependence".
__ same comment for 4th bullet_
I have adjusted this section to clarify that the aspect of jet
modification I am trying to study is the path length dependent
nature
of jet energy loss

Slide4 (current v4)
_ "We are interested in understanding the path-length
dependence of
these processes" -> "We are interested in understanding the
path-length
dependence of jet quenching"

_"Both collisional and radiative" -> "Both collisional and
radiative

energy loss" or "Parton energy loss via both collisional and
radiative
processes"

_ 5th Bullet ("Both collisional and radiative") you need to
provide
reference to the theory calculation for this L/L^2 dependence.
These
are
model calculations.

Slide4 (current v4)
_"Both collisional and radiative" -> "Both collisional and
radiative

energy loss" or "Parton energy loss via both collisional and
radiative
processes"


Removed L/L^2 statements as I am not comparing to any models
in
this
presentation

_ This slide only focus on jet and jet quenching, but it
doesn't
motivate your measurement like why jet anisotropy measurement
is
required? Need to include some text on it.
I suggest you need to motivate jet anisotropy before you go to
any
jet
analysis details like in Slide5 underlying event discussion

The way I have structured my talk is to first motivate that we
have
observed jet quenching. I am using the dijet analysis to this
end. I
then want to contrast that with azimuthal anisotropy, which is
not
a
dissimilar measurement in that it probes jet modification, but
it
does
so in a new way. Therefore, I think it makes sense to talk
about
jet
measurements and then the dijet measurement before introducing
the
idea of anisotropy and motivating how that can get us towards
the
missing path length dependence of a dijet analysis.

SLide:5
_Not clear, what is that right side plot? Is this data or MC
simulation.
What is pT, of track or jet? What is Delta phi?
I agree, this plot was not particularly clear. I have removed
it.
__"Soft processes produce a fluctuating background" what is
that_
_background? Is it track or _combinatoric_ jet background?_
I'm not quite sure I understand what you are asking, it is the
tracks
from soft processes which produce the combinatorial jet
background, so
I suppose both?
Then it would good to mention, "Soft processes produce a
fluctuating

uncorrelated background for jet measurement in heavy-ion
collisions"
Here "uncorrelated" is important.

Slide5 (current v4), right figure is from STAR data or any
model? No

description mentioned there.

__3rd _bulltet_ (Estimated…) it should _be sub-bullet_ of
2nd
bullet
(Soft_
_process…)_
Changed.
__ what is kT?_
The k_T jet finding algorithm, clarified.
__ Jet area -> Jet area(A)_

Changed.

Slide6:
_Not clear, what is that right side plot? Is this data or MC
simulation?
What is pT, eta, and phi?
This is the total track momentum for eta/phi bins for a
collision.
__"A jet finder… had scattering and other processes" ->" had
scattering_
_and combinatorial background in heavy-ion collisions"_
_2nd bullet is not required if you mention above.

_ _I have merged this with slide 5 and changed this wording

SLide:7
I would suggest to use jet pT as $p_{\rm T, jet}$ throughout
your
presentation.
Changed.
__Used in other STAR analysis -> Proved references_
__Provide _referecen_ to ALICE measurement_

Done.

Slide:8
_Move this slide or Isobar jet pT distribution after your
slide14
where
you discuss about Isobar dataset. It seems the left side plot
just
pop-up. This plot should be part of you results discussion
even if
it
is
a STAR performance plot.
Figure removed
__"Statistically unlikely for soft processes…" Please
rephrase
this… not_
_clear._
Changed to clarify that it is unlikely for soft processes to
produce
high pt hadrons which look like jets
__"May bias jet selection towards surface" Not sure the
motivation
of_
_this bullet. _why it is_ important? You are not doing jet
RAA/RCP
study_
_and you do not study trigger jet v2 then why it is important
if
this
jet_
_is trigger biased or not. These jets should be treated as
inclusive
_jet_._

Is it not important to understand the biases we introduce into
our
measurements? By requiring the high pT hadrons the selected
jets
are
biased towards the surface of the QGP. This is the motivation
for
one
of the items we would like to explore next in this analysis,
the
variation of the hard core threshold.

Slide:9
This slide is not relevant. You could put in Backup. (A
distraction)

I disagree, the story I am hoping to tell with this talk is
that
we
saw signs of jet quenching with measurements like dijet
imbalance,
but
that it doesn't tell the complete story. We can continue our
understanding of jet quenching from dijet measurements to jet
v2
measurements.

slide8(in v4)
_ we are doing inclusive hard-core jet v2 measurement here. Is
not
it?
_I am not convinced to motivate with dijet measurement here.
Are we
going to do any dijet measurement in isobar?
_Selecting a hard-core jet may not imply you select surface
biased
jet.
For that you need to show the same dijet Aj measurement in
isobar
like
in Au+Au. If you have any result to demonstrate that you are
selecting
surfaced bias jet in Isobar, please show those results.
I think we have not done that study.


Slide:10
_ 1st bullet: Why it is important for Dijet imbalance
discussion
here?
You are doing inclusive jet v_n measurement. Not clear to me.

See above.

Please see above my concerns.


SLide12
_"A jet in plane interacts with less medium than one out of
plane"
->
"A
jet interacts less with medium in plan than out of plane"
Changed.
__"Since jet production is isotropic, differences in yields
are a
result_
_of medium interactions" Not sure, _what you_ want to say
here?
Please_
reprhase_._
Changed.
__" like flow" Remove this._
I included this to help give context for the measurement to an
audience who may be familiar with flow studies, but not jet
anisotropy
studies. If you feel this is misleading I will remove it.
__ you do not discuss what is v_{2}^{jet} is?_
Changed equation to remove \Delta\phi -> \Psi_2 - \Phi_jet
__"Not a flow effect though!" Can you elaborate this?_

I am stating that although it may be described using the same
framework as flow measurements, jet v2 is a different process.

I would suggest to give a clear idea what could be that
different
process, For example...?
Otherwise do not create unnecessary doubt or make statement
just for
a
buzz?


SLide13
_RHIC produces a different, cooler QGP -> "RHIC produces a
cooler
QGP
medium than the LHC"
Changed.
__"Down to 10 _GeV"_ -> But you are not going to show down to
10
GeV.
So_
_just remove this extra quantifier _subbullet. Main bullet is
fine.

I do show down to 10 Gev though, my first point is 10-12.5
GeV/c
jets.

Slide15:
- Jet trigger -> You don't use any jet trigger and BEMC info
in
your
measurement. If yes, just remove.
I do use the barrel high tower trigger in my analysis, as
detailed
in
the preliminary figure request. I have clarified this as high
tower
trigger rather than jet trigger.
_- Right side STAR detector, please indicate where is TPC,
BEMC,
EPD_
_- Mention kinematic acceptance of these detectors_

See updated slides, Yi mentioned this as well

Slide16:
_you did not discuss what is Delta_phi?
I did not, but I am not sure I need to on this slide. I will
discuss
it on the next slide.
__right side plot, _make title_/_lable_ of x-, y-axis bigger
so
that
it will_
_be visible. And also legends _in side_ the plot._
Changed, made entire plot larger as well

Slide18
Move this slide after Slide15

Changed.

Slide19
_INside fig, mention "red line" is fit fun.
Added.
__ inside fig, p_T^reco -> p_{\rm T, jet}^{reco} ; 12.5 ->
12.5
GeV/c_
Changed.
__ you did not mention anywhere before what is "R"? And what
jet
_R
you
are_ going to _do measurement_?_
It is labeled on the plot, and I will discuss it further on
the
following slide.
__ what is v_{2}^ch? Need to mention _it charged_ jet v2. I
would
suggest_
to use $v_{2}^{\rm ch, jet}$; And the same about v_{2}^ch,abs

Changed.

Slide20:
Before slide20, you need to discuss different jet v2 (all,
hard
core,
matched jet) and their spectra showing side-by-side

I'm not sure I understand why? I think that was a good check
to
make
and certainly worth having in the backup, but the measurement
being
presented is jet v2 using the hard core matching criteria, the
need
for which is motivated earlier in the talk.

Slie21:
_ "Jet v2 is a exciting measurement for determining the
path-length
dependence of jet quenching" -> This statement is fine to
motivate.
But
for your conclusion this may not be relevant. Because we don't
have
jet
v2 measurement for different path length/system size with the
same
kinematic coverage. And you did not discuss what is the
strategy
for
your measurement unless you plan to do the same in AU+AU.

_"Jets which are in plane interact with a different amount of
the
QGP
than those out of plane" Not sure how do you get this
conclusion
from
your measurement.

I have updated my conclusions to better reflect the points I
wish
to
make and where I will go next with this analysis.


Thank you
Nihar
On Thu, Oct 6, 2022 at 1:34 PM Yi Yang <yiyang0429 AT gmail.com>
wrote:

Dear Tristan,

Thanks a lot for the reply and the updated version.
They look very good to me.
Let's wait for your study and the decision on the preliminary
results!

Cheers,
Yi

On Thu, Oct 6, 2022 at 3:26 AM Tristan Protzman
<tlp220 AT lehigh.edu>
wrote:

Hi Yi,

Thank you for the feedback! I have uploaded an updated
version
and
addressed your comments below.

- p4: Are the sub-bullet for the 3rd bullet and the 4th
bullet
the
same?

Yes, I have removed that redundancy.

- p6: toy mode --> toy model

Fixed.

- p9: Just for my own education, could you please tell me why
A_j
can be less than 0 (I am assuming pT^1 and pT^2 are leading
and
subleading jet pT, respectively, is it correct)?

Yes, (pT^1, pT^2) is the (leading, subleading) jet pT. The
red
points are the measurement of A_j using only hard cores.
This is
where leading and subleading are determined, thus no points
below
0.
However, after matching is done, leading and subleading are
not
recalculate, so it is possible for the subleading hard core
to
match
to a jet with more momentum than the leading hard core does,
resulting in negative A_j. There are a few ways this could
happen.
The subleading jet could contain a larger soft component than
the
leading jet, thus when added to the hard core the magnitudes
flip.
Additionally, because of the fluctuating background the
leading
jet
could be over subtracted and the subleading jet under
subtracted,
again flipping the relative magnitude. This would not affect
the
hard core since background subtraction is not done on that
collection.

- p15: It would be good if you can provide more information
for
the
subdetectors, for example eta and phi coverage...

I added more information about each system and labeled the
picture.

- p18: Jet v2 not feasible --> Jet v2 is not feasible

Changed to Jet v2 was not feasible

Cheers,
Tristan

On Wed, Oct 5, 2022 at 1:59 PM Yi Yang <yiyang0429 AT gmail.com>
wrote:

Hi Tristan,

Thanks a lot for the nice slide. I have some
suggestions/comments
for your consideration.
- p4: Are the sub-bullet for the 3rd bullet and the 4th
bullet
the
same?
- p6: toy mode --> toy model
- p8: Title: Hardcore --> Hard core
- p9: Just for my own education, could you please tell me why
A_j
can be less than 0 (I am assuming pT^1 and pT^2 are leading
and
subleading jet pT, respectively, is it correct)?
- p15: It would be good if you can provide more information
for
the
subdetectors, for example eta and phi coverage...
- p18: Jet v2 not feasible --> Jet v2 is not feasible
- Since we are not settled with your preliminary results yet,
I
will comment on p20 and p21 later. :-)

Cheers,
Yi

On Thu, Oct 6, 2022 at 12:36 AM Tristan Protzman via
Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:

Hi All,

I submitted this material for review last week, but it seems
to
have
been lost somehow, so I am resending it.

Cheers,
Tristan

On Wed, Oct 5, 2022 at 12:33 PM webmaster--- via Star-hp-l
<star-hp-l AT lists.bnl.gov> wrote:
Dear Star-hp-l AT lists.bnl.gov members,

Tristan Protzman (tlp220 AT lehigh.edu) has submitted a material
for
a
review,
please have a look:
https://drupal.star.bnl.gov/STAR/node/61264

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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Lehigh University
(610)758-3907
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16 Memorial Drive East Office 406
Bethlehem, PA 18015
she/her/hers

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