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Subject: sPHENIX EMCal discussion

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Chronological Thread  
  • From: Gabor David <david AT bnl.gov>
  • To: Craig Woody <woody AT bnl.gov>
  • Cc: sphenix-emcal-l AT lists.bnl.gov, sphenix-hcal-l AT lists.bnl.gov
  • Subject: Re: [Sphenix-emcal-l] [Sphenix-hcal-l] Inner calorimeter
  • Date: Thu, 2 Jun 2016 09:23:53 -0400 (EDT)

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.html
and 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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--
Gabor David (david AT bnl.gov)
Brookhaven National Laboratory
Physics Department, Bldg 510/c
UPTON NY 11973
Tel: (631)344-3016
FAX: (631)344-3253




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