sph-cqcd-2017-001-l AT lists.bnl.gov
Subject: Discussion of sPHENIX note sPH-cQCD-2017-001
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Re: [Sph-cqcd-2017-001-l] Comments on the Letter of Intent for Forward Instrumentation at sPHENIX
- From: John Lajoie <lajoie AT iastate.edu>
- To: sph-cqcd-2017-001-l AT lists.bnl.gov
- Subject: Re: [Sph-cqcd-2017-001-l] Comments on the Letter of Intent for Forward Instrumentation at sPHENIX
- Date: Thu, 25 May 2017 17:57:28 -0500
Hi Jamie, Thanks for the thorough and thoughtful comments. As for the
"money plot" for DY I am working on this with Hannu Paukkunen.
He's agreed to see if we can do a reweighing to estimate the
effect on EPPS16 if we can provide him with some pseudodata - I'm
working on getting him the pseudodata. Figure 1.7 assume a Q^2 range from 25-64 GeV^2, consistent
with the invariant mass region 5-8 GeV, as described in Section
4.2. We have not done a serious study of forward photons with the
FEMC as merged pi0 showers will be an issue at the highest
rapidities, which access the lowest x in the nucleus. In PHENIX
we had to build the MPC-EX to do this from 3 < eta < 4, and
the FEMC tower size is larger - 5.5 cm vs. 2.2 cm for the MPC. I
would suspect you could do something at the lower rapidities, but
the details would need to be studied. However, DY is far superior to prompt photons because in DY
you get full reconstruction of the event kinematics at LO. The
ability to reconstruct the kinematics at LO should have a much
stronger constraint on the nuclear PDF's as you don't just
constrain the integral, but the shape as well. Prompt photons +
jet could do this, but again you wouldn't be able to get the high
rapidity prompt photons that reach the lowest x in the nucleus. The kinematic coverage is the "big deal" - not only do you
reach low x where there is a dearth of data to constrain the
nPDF's but in a limited Q^2 region you reach lower x than the EIC
will reach. This makes the measurement complementary to the EIC,
not directly competing with it. Hope this helps. John On 5/25/2017 5:14 PM, Jamie Nagle
wrote:
(2) how antiquarks move around in
nuclei? antiquarks only come from quantum fluctuations in the
proton and in nuclei and can tell us a lot about QCD.
Antiquark distributions in protons have already shown some big
surprises. Measure antiquarks via DY in p+A.
Where is the money plot?
Apologies here, but I do not find any such plot. Something
with the x-distribution of anti-up or anti-down
in nuclei at a given Q^2 with experimental uncertainties ...
overlay with EPPS16 fit results.
Figure 1.7 is okay, but not a
delivery/money plot.
A couple other questions on
DY. For Figure 1.7, what is the DY mass range assumed to be
accessible?
I am also interested in how
one compared the deliverable from forward direct, real photons
to these DY virtual
photons. I think that
needs a crisp answer/discussion.
Anti-quarks are unique (?) to
hadron-hadron, in other experiments by running to separate
proton+neutron and
proton+proton one can get at
anti-up versus anti-down. That is not the case here... One
gets at the sea via
DIS, so the real argument is
in the kinematic coverage?
--
Contact me: john.lajoie |
-
[Sph-cqcd-2017-001-l] Comments on the Letter of Intent for Forward Instrumentation at sPHENIX,
Jamie Nagle, 05/25/2017
- Re: [Sph-cqcd-2017-001-l] Comments on the Letter of Intent for Forward Instrumentation at sPHENIX, John Lajoie, 05/25/2017
- <Possible follow-up(s)>
- [Sph-cqcd-2017-001-l] Comments on the Letter of Intent for Forward Instrumentation at sPHENIX, Jamie Nagle, 05/26/2017
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