Presentation is loading. Please wait.

Presentation is loading. Please wait.

FP420 TOF- Past and Future TOF in ATLAS and CMS proposals The problem

Similar presentations


Presentation on theme: "FP420 TOF- Past and Future TOF in ATLAS and CMS proposals The problem"— Presentation transcript:

1 FP420 TOF- Past and Future TOF in ATLAS and CMS proposals The problem
The solution How to build and regain credibility Sebastian White,BNL Dec.7, Manchester

2 Cerenkov approach Amazing paper by Nagoya with Quartz radiator and MCPPMT in test beam But FP420 is a very high rate experiment-ie 200Mhz(pe)/cm^2 and MCPPMT is definitely not a high rate device Even for Nagoya, rate is a huge issue at Super-Belle and it’s at least an order of magnitude worse in FP420 Sebastian White,BNL Dec.7, Manchester

3 Cerenkov approach(II)
The issues: Rate limit-ie gain distortion from space charge Lifetime=deterioration of photocathode Easy to calculate with elementary knowledge of PMT’s and access to data-sometimes hard to corroborate Some dreams of improvements with complicated surface physics,etc- doesn’t belong in a proposal Should never have touched them in the first place Sebastian White,BNL Dec.7, Manchester

4 The radiator FP420 has two solutions- gas and Quartz- not clear whether any point to using both Both have issues For Gas it’s segmentation and maybe edge and geometry For quartz I know at least uniformity but certainly no final design. Sebastian White,BNL Dec.7, Manchester

5 Segmentation We have to deal with segmentation at 1034
Assume you are only willing to waste~1/4 of the luminosity Then at 420 you don’t need segmentation At 220 you have to associate Cerenkov hit with track for 2 tracks Probably have same segmentation for both and clone detectors Sebastian White,BNL Dec.7, Manchester

6 Timing solution Very hard to find one. Most said impossible,particularly if insist on Cerenkov. Interesting non-Cerenkov solution-see below Recently Japanese tried to find high rate alternative to MCP Hybrid photodetectors interesting. Speed limitation in the target. Developed new low capacitance high speed APD target. About to become a Hamamatsu product. I am buying the first one. Pretty expensive. Sebastian White,BNL Dec.7, Manchester

7 Sebastian White,BNL Dec.7, Manchester

8 Sebastian White,BNL Dec.7, Manchester

9 Sebastian White,BNL Dec.7, Manchester

10 The new tube Physics of TTS not in APD or focusing. It is Photocathode thickness. Only 1psec for 10nm! But 30psec FWHM for a thick one. So probably could have pretty big photocathode. But available 3mm,6mm,8mm probably ok. Discussing. Rate tested to >100Mhz. Electronics limited. We will build something better at BNL. Sebastian White,BNL Dec.7, Manchester

11 The new tube Packaging ok but not optimal. But Hamamatsu says can break out tube. Probably build better electronics anyway. Lifetime: don’t know but Rehak(who was pretty skeptical) says it should be ok CMS very interested in APD rad damage. Tested their thin APDs to 100Grad! So pretty good chance that it works. Sebastian White,BNL Dec.7, Manchester

12 The radiator Start from the ground up. Choice of material and geometry should be optimized. Maybe Quartz. Problem of getting all those photons onto that little photocathode. First clarify segmentation. Simple statistics. Probably 4. Then develop several concepts- lenses and mirrors, parabolic mirror, light pipe- have a few solutions Sebastian White,BNL Dec.7, Manchester

13 How to build and test something credible
Radiator: my preference is to have it done by professionals who know something about optical properties of materials and optics-maybe Labsphere Work with them on our application, acceptable dispersion,etc. They would know how to choose the right quartz, for example. With state of the art optical simulation and good expertise build it right the first time instead of trial and error approach Sebastian White,BNL Dec.7, Manchester

14 Building it The PMT: obviously with so much riding on it this has to be understood very quickly. There are details like whether we can get the right photocathode material, what are the possible parameters wrt area, how quickly we can get at least one so we can say we’ve seen one and things about cost and delivery and.of course, radiation Sebastian White,BNL Dec.7, Manchester

15 Electronics Probably new preamp but maybe Hamamatsu ok.
All the rest- Krzysztof and Jim’s CFD, HPTDC, ref timing system, should be just fine Sounds like pretty many channels (at least 32) but that is due to segmentation anyway Sebastian White,BNL Dec.7, Manchester

16 Resources Electronics beyond the preamp: Assume there are open issues.
Cabling, clock distribution and other infrastructure important Possibly further studies of these tubes.BNL Instrumentation would be an asset. Sebastian White,BNL Dec.7, Manchester

17 The alternative Why not try to do better than Nagoya? Their application is not the same as ours anyway. If APD is so fast why go through the trouble of making photons, worrying about optics, then converting them to electrons and detecting them. Just measure the protons directly. It’s better and cheaper. And don’t have to deal with Hamamatsu any more. Sebastian White,BNL Dec.7, Manchester

18 APD’s Advanced Photonics and RMD interesting
Hamamatsu not interresting Very fast in a variety of geometries Prefer RMD 8x8mm. Just perfect for our segmentation. Huge signals! Ie 25V for a particle. Sebastian White,BNL Dec.7, Manchester

19 Ru106(e-~3.546MeV) RMD-8x8, HV=1670V, e- Sebastian White,BNL
Dec.7, Manchester

20 Ru106(e-~3.546MeV) APhI-5, HV=1850V, e- Sebastian White,BNL
Dec.7, Manchester

21 Conclusion So maybe things aren’t all that bad-2 solutions
Sorry I couldn’t be there Sebastian White,BNL Dec.7, Manchester


Download ppt "FP420 TOF- Past and Future TOF in ATLAS and CMS proposals The problem"

Similar presentations


Ads by Google