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Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter
- From: Mickey Chiu <chiu AT bnl.gov>
- To: "Sickles, Anne M" <sickles AT illinois.edu>
- Cc: "sphenix-emcal-l AT lists.bnl.gov" <sphenix-emcal-l AT lists.bnl.gov>, sphenix-hcal-l AT lists.bnl.gov
- Subject: Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter
- Date: Thu, 02 Jun 2016 13:17:55 -0400
Hi Anne, et al,
I think
> trading the EMCal performance for a barrel time of flight detector.
is not how I would characterize John's proposal. First, it's not at all clear you're losing much, if any, performance. Secondly, the trade is for a tracking detector we actually want, rather than one that is forced upon us by financial circumstances. I'm assuming we could save enough to make this statement though I haven't seen the numbers. If this is true, then a more accurate statement would be "replace building a new EMCAL with building an entirely new tracking system." The question is really between whether a new EMCAL with a whacked up tracking system is a better realization of the sPHENIX physics goals of jets and upsilons, or would an old EMCAL and new tracking system be better. Of course if you don't save enough then what I say above isn't true... The TOF stuff I mention only of course because I'm working on it, but I do think that it is only possible with outside funding or if there is enough contingency left over. It's like a cherry you can put on the top if we can afford it, but it's not the main course.
The PbSc Moliere radius of 3 cm is listed in table 1 here:
http://arxiv.org/pdf/nucl-ex/0202009.pdf
In the olden days when I was looking for the PbSc Moliere radius and noticed that it was much smaller than the segmentation, I was surprised and checked it with Edward and he confirmed it. It might be a good idea to re-confirm it with simulation and test-beam if we decide to go this route.
I agree we'd need a full simulation to be sure, but I think what John had proposed really wouldn't be much of a negative for the Upsilons or jets. The reduced measurement capabilities for the Upsilons in the triangles between sectors would be much less than the 40% loss we've already deemed acceptable for the Upsilon, and for a jet measurement where you just integrate in a cone I think the weird geometry there isn't going to be too bad. As for projectivity in phi, we had zero problems in PHENIX with the 20 degree angle of incidence using the GAMS-derived clustering, and the PHENIX EMCAL had zero projectivity, so I see no major issues there. The projectivity in eta was already a major issue in the baseline sPHENIX EMCAL, so that might be a wash. I do think that someone would need to look into the clustering/reconstruction at polar angles higher than 20 degrees, since I think there the GAMS-derived clustering we used in PHENIX may have some issues. There would be additional information if we decided to go with longitudinal segmentation, however.
Cheers,
Mickey
On 06/02/2016 12:09 PM, Sickles, Anne M wrote:
Hi everyone,
Thanks John for kicking off an interesting discussion.
I think if people would like to seriously consider this route, we need a
real model of the geometry for a reused PbSc and simulations. The
segmentation that John quotes is significantly worse than even the
ganged 2x2 towers that we are considering and while the improved
resolution would help with the e/h separation the lack of projectivity
in both eta and phi will be a drawback. In addition, the gaps between
the sectors would result in a decreased acceptance for upsilons and
photon and non-uniformities in the jets. It’s a quantitative question as
to what the performance actually would be and since we have real
simulations for the SPACAL, we would need real simulations for a reused
PbSc as well. There seems to be a factual disagreement between John and
Mickey as to what the Moliere radius of the PbSc actually is and I
couldn’t find documentation of that in either the web page John linked
to or the NIM paper:
http://www.phenix.bnl.gov/phenix/WWW/pub/phenixnim/d_emcal/nim_4d_emcal.pdf
It is really not clear to me what the impact to the schedule is of a
reused EMCal. It does exist, but it would take a few months to
implement in simulations and convince ourselves that it could meet our
physics requirements. Given the physics aims of sPHENIX (jets and
upsilons), I don’t see the logic in trading the EMCal performance for a
barrel time of flight detector.
The 2D projective shashlik that Craig mentions obviously deals with some
of these issues (it could be designed to be 2D projective for example)
and I think we had a MC model for it at some point (?). However given
that it is orthogonal to the last few years of R&D we have done, I agree
with Craig’s assessment of a very long delay to the project.
This is something we could certainly discuss at the EMCal meeting next week.
Best,
Anne
On Jun 2, 2016, at 9:41 AM, Mickey Chiu <chiu AT bnl.gov
<mailto:chiu AT bnl.gov>> wrote:
Hi John, et al,
I think this idea isn't as crazy as it sounds. The energy resolution
would be much better, 8% vs 12%, which buys back some of the e/pi
separation (through E/p and residually through shower shape cuts). The
caveat in the E-resolution argument is that we'd need to understand
whether the constant term can be reduced to the version we had in the
test beam, or the one we had in PHENIX.
I think if you go this route you would want to optically split the PbSc
longitudinally, which then would provide equal or superior e/p
separation to the dual EMC/iHCal that is the default now. Just reading
out the front and back wouldn't help very much, though in the
longitudinal split you certainly would want to collect the light from
the front and back. I think you could start working on the
"construction" almost right away, with just a short R&D period to figure
out how to best split it longitudinally. Longitudinal segmentation also
gives you a crude sort of projectivity along eta.
One down-side that I see is the segmentation is much coarser, but this
can also be solved rather easily. The PbSc Moliere radius is actually
3.0 cm, a fact that is not very well known. The fibers could be
rearranged to buy back some of that segmentation.
The only other down-side I can think of are the the triangular gaps
between sectors. (Well, there's also the mental down-side that this
won't have that new car smell...) I'm not sure what you want to do with
those gaps, but I'm betting you will need to fill them somehow. However,
I don't agree with Craig that re-using the PbSc is going to be as
expensive as building brand new... I'd expect it to be _significantly_
cheaper, and with a better schedule. As I mentioned above, you could
probably start working on the "construction" of this as soon as we get
the PbSc off the East Carriage around late August/September. My guess
right now is that it would be some simple mods to the existing
calorimeter. We have a prototype in the basement which we can get Sean
cranking on today if desired.
With the money I'd expect we could save, we could consider more optimal
configurations of the tracking. In addition, based on the EIC R&D I
have been working on, I'm currently 90% confident that I can build a
mRPC TOF system capable of 20 ps, which would give PID capabilities
similar to what we have in PHENIX, but over the whole 2pi acceptance.
This would cost just $4M (not counting contingency but otherwise is the
whole project cost). This estimate is based on 4 times larger STAR TOF
cost, which was $7M, so it might be considered a conservative estimate.
The remaining 10% uncertainty in my confidency level above is due to
whether we could create electronics capable of handling the 4 us trigger
latency. I had thought I could retire that risk by this coming winter,
but current labor changes at BNL make that time-scale more uncertain.
In any case, we have a plan in place for how to make the electronics for
this. Over the next year I'm hoping we can demonstrate 10 ps resolution
(and incidentally reduce the cost further). If we can do that, we
should be able to surpass the PHENIX (and RHIC-wide) momentum reach for
PID by \sqrt{2}. Of course it should be obvious that full acceptance
PID would significantly enhance the sPHENIX physics program...
Cheers,
Mickey
On 06/02/2016 09:23 AM, Gabor David wrote:
On Thu, 2 Jun 2016, Craig Woody wrote:
Hi, Craig and All,
Hi John,
I have to say that I was thinking the same thing. When we talk about
eliminating the Inner HCAL (which is clearly like having a vital
appendage removed in my opinion...), one does have to ask, why is there
this large gap between the EMCAL and the wall of the magnet ? I agree
the main justification for going to a tungsten absorber was to keep the
EMCAL compact, thus allowing the HCAL to be kept smaller in order to
reduce the cost. However, if the entire radial space from ~ 90-140 cm is
available for the EMCAL, keeping the Outer HCAL the same, then it would
make sense to reconsider lead as an absorber again. If I recall Tom
Cormier's design, it essentially just fit into this space with ~ 18 Xo.
One could then consider a projective (even 2D projective) shashlik
design with SiPM readout. However, I don't think it makes sense to
In fact, ideally dual readout (front and back), this would
buy back some of the lost e/p separation
actually consider using the existing PHENIX shashlik, since it's
completely the wrong geometry and I would be the cost to rework it would
Fully agree
be more than building a new one. Nevertheless, if we have the radial
space, it would be worth considering a lead absorber again in terms of
cost and performance. The only problem with doing that is that it would
set us back about two years in terms of schedule.
Aye, there's the rub... (more later, I got an appointment)
Gabor
Craig
On 6/2/2016 12:10 AM, John Haggerty wrote:
Hello,
This is not for Friday's descoping document, but I think that given
some
of the ideas going around now, we might have to go back to ideas that
were dismissed many workfests ago, since they might not be as bad as
some of the descoping options we're now talking about.
The one in particular that's been bothering me the last few days is
going to a single calorimeter inside the solenoid with lead absorber.
If we multiplex the EMCAL to 2x2, one could ask why you need expensive
tungsten to make a short radiation length. Maybe lead would be good
enough. (I should note that Edward often asks this question, but when
we had 1 Moliere radius towers, it was easy to say that only tungsten
could achieve the short radiation length without going to hugely
expensive crystals, and only tungsten would allow us to cram ~1.5
interaction lengths inside the solenoid.)
Once you think lead, you may as well think the PHENIX EMCAL, it's as
good as any lead-scintillator calorimeter. It's about 17.5 radiation
lengths, about 0.85 interaction lengths in depth, which is about
375 mm,
so it would fill up about the same volume as the EMCAL and Inner HCAL
(1000 to 1400 mm in radius), and one could read it out at the inner
radius with SiPM's.
My facts com from Edward's web page
http://www.phenix.bnl.gov/phenix/WWW/emcal/computing/online/EmcDoc112602/Introduction.htmland the NIM paper, by the way.
A tower is 55.35 mm square, I think, so there are something like 100
towers in phi and 60 in eta and natural numerology would make it 0.058
(phi) x 0.037 (eta). I think the Moliere radius of the EMCAL is about
55 mm, so it is matched, as is common, to the segmentation, and the
108*60=6480 towers takes 3 PHENIX sectors.
The natural segmentation leaving the (12x12) supermodules alone would
lead to a nine-sided calorimeter (9*12=108), odd, but not impossible.
(If one can take apart the supermodules, one could contemplate a seven
sided structure with 16x16 supermodules, I don't know if that's
feasible
or not).
There are many bad features of this idea, which is why we dismissed it
in the first place. It's not naturally projective; there are likely to
be sizable gaps for support; you can afford less photodetector coverage
than you could with PMT's; the segmentation is just barely adequate.
Some of these problems could conceivably be overcome with ingenuity and
labor, but the segmentation and the radiation length are what they are.
You can say the rework still costs a lot, but the difference in cost is
more in design, mechanics, and modifying the existing modules, and some
of that is common, and much of it is labor, which is not the immediate
problem. You lose the Inner HCAL, but the total interaction lengths is
less than one less, from nearly 6 at zero rapidity to 5. Part of this
package would be to leave the Outer HCAL alone, or perhaps even augment
it by splitting the tiles in half and reading both inner and outer
radius. We may lose in e-pi, but if the calorimeter's resolution
survives intact (to be show with reduced photodetector coverage), maybe
E/p is enough better to make up for that loss.
Bad idea? Many of us thought so, but depending on the results of the
budget exercise, it may be worth kicking around again.
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Anne Sickles
Assistant Professor, Department of Physics
University of Illinois at Urbana-Champaign
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-
[Sphenix-hcal-l] Inner calorimeter,
John Haggerty, 06/02/2016
- Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter, Edward Kistenev, 06/02/2016
-
Re: [Sphenix-hcal-l] Inner calorimeter,
Craig Woody, 06/02/2016
-
Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter,
Gabor David, 06/02/2016
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Message not available
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Message not available
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Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter,
Mickey Chiu, 06/02/2016
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Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter,
Rosi Reed, 06/02/2016
- Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter, Xiaochun He, 06/02/2016
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Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter,
Rosi Reed, 06/02/2016
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Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter,
Mickey Chiu, 06/02/2016
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Message not available
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Message not available
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Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter,
Gabor David, 06/02/2016
- Re: [Sphenix-hcal-l] [Sphenix-emcal-l] Inner calorimeter, EdwardOBrien, 06/02/2016
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