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PHENIX High pt Upgrades-- Overview --
Yasuo MIAKE for High pt Upgrade Team
http://utkhii.px.tsukuba.ac.jp/~highpt/
2 Yasuo MIAKE, Univ. of Tsukuba
Proposal
• To enhance the PID capability of PHENIX, we like to install Aerogel counters (160 segments) on the West Arm.
• Together with the Aerogel, TOF and RICH, we can extend the PID beyond 5 GeV/c.
3 Yasuo MIAKE, Univ. of Tsukuba
Proposed Extention of PID with Aerogel
Pion-Kaon
separation
Kaon-Protonseparation
TOF ~100 ps 0 - 2.5 - 5
RICH n=1.00044
th~34
5 - 17 17 -
Aerogel n=1.011
th~6.8
1 - 5 5 - 9
0 4 8
0 4 8
0 4 8 0 4 8
0 4 8
0 4 8
Note ; Aerogel together with TOF can extend the PID capability upto 10 GeV/c(Without TOF, no K-proton separation at < 5 GeV/c)
4 Yasuo MIAKE, Univ. of Tsukuba
Physics Motivations
• From basic strategy, it is natural extension for PHENIX to extend its PID in higher pt region.
• Strong motivation given;– Jet Quenching!?
– Large suppression of pions at high pt , while protons show binary scaling!?
• Meson/baryon puzzle?
• Need to extend PID > 5 GeV/c
5 Yasuo MIAKE, Univ. of Tsukuba
Transition Region to Jet Fragmentation
• Hadronic Flow vs Flow at Quark Level?
• Seems to important to measure the transition region to Jet fragmentation.
• PID (pion, kaon, proton) beyond 5 GeV/c is the goal.
6 Yasuo MIAKE, Univ. of Tsukuba
What STAR is doing
• We like to go beyond 6 GeV/c with pion, kaon and proton.
7 Yasuo MIAKE, Univ. of Tsukuba
Aerogel Panel o the West
• 4.5 m from the vertex.
• Coverage ; full z, ** degree in phi.
• Space available for new TOF.
RφZ
160 Cells
Aerogel(11x22x11 cm^3)
Integration Volume
PMT
PMT
8 Yasuo MIAKE, Univ. of Tsukuba
Design of Aerogel Panel
• Direction of every other cell is reversed, so that– Aerogel locates at the same distance from
the vertex,– No dead space in between.
Side View
400 cm (16 Cells)
118 cm(10 cells)
30 cm
Z
Top View
rφ
r
9 Yasuo MIAKE, Univ. of Tsukuba
Cell Design
11cm
11cm
22cm
Aerogelair
n=1.0112+- 0.0002
Prototype in run3-pp
10 Yasuo MIAKE, Univ. of Tsukuba
PMT assembly (prototype)
11 Yasuo MIAKE, Univ. of Tsukuba
Silica Aerogel
• Best index with RICH(CO2) is n< 1.007, too small.
• SP-12M (Matsushita) – Silica aerogel with Lowest
refractive index commercially available.
– Hydrophobic
• Long term stability proved by KEK-Belle.
Refractive Index (Measured) 1.0114 +- 0.0008
Density [g/cm^3] 0.04
Transmission for 10 mm (Measured) 64 % @ 400 nm88% @ 550 nm
Tile Size [mm] 112.5 x 112.5 x 11.0
12 Yasuo MIAKE, Univ. of Tsukuba
1 p.e.
2 p.e.
PMT
• 3” PMT for photon counting
• Gain of > 10^6 at 1500 V w. 1-1-1-1- voltage divider
• One p.e. resolution
13 Yasuo MIAKE, Univ. of Tsukuba
Bleeder
• Hand made bleeder– Thinner material– Less space– Less power (330 mW@1500V) than Hamamatsu standard– Tested upto 3.2 kV for 6 hours
14 Yasuo MIAKE, Univ. of Tsukuba
Magnetic Field on the West
• Magnetic field of the location measured as < 8 G.– Goal set as 16 Gauss !
• Thickness & Size of the mu-metal shield has been optimized using Helmholz Coil.
15 Yasuo MIAKE, Univ. of Tsukuba
Mu-metal Shield
• Magnetic shield of 0.2 mm thick breaks down at around 10 G. – Loss of Gain &
– Loss of Q.E.
• Magnetic shield of 0.5 mm survive till 20 G.
16 Yasuo MIAKE, Univ. of Tsukuba
Final Prototype Test at KEK
• SP-12M
• R6233-01HA w. Bleeder
• Pre-Amp w. cables
• Dubna Box
• Normal ~ 14 p.e.
• Reverse ~ 12 p.e.
17 Yasuo MIAKE, Univ. of Tsukuba
Observed Clean Signal
• Very clean separation– Amount of photons other than Aerogel Chrenkov is small!
+2 GeV/c
1 p.e. peak
~0.4 p.e./PMT
~6.6 p.e./PMT
Final Prototype Test
18 Yasuo MIAKE, Univ. of Tsukuba
Observed Uniform Response
• Uniform response, thanks to Integration Volume– Important to separate in the momentum region of slow rise
• ~10% diff. between normal/reverse, due to diffusive nature of aerogel
Normal Reverse
Oops!
19 Yasuo MIAKE, Univ. of Tsukuba
Uniformity Confirmed at Dubna
• Tested at Dubna with final prototype, but with SP-15.
• Independent setup & calibrations
20 Yasuo MIAKE, Univ. of Tsukuba
Cherenkov Light from PMT window
• Cherenkov from PMT window;– Huge pulse height – Faster Timing (> 5 ns)
Time
Time
P. H.
P. H.Aerogel
(n=1.011)
PMT glass (n=1.5)
21 Yasuo MIAKE, Univ. of Tsukuba
Background Rejection
• Photons from PMT windows can be identified/recognized by itself,– Faster Timing (>5 ns)
• Consistent with optical simulation
– ADC-ADC correlation
• Other sources of photons are carefully surveyed and <1p.e.
• TDC-TDC difference can be used for track association.
22 Yasuo MIAKE, Univ. of Tsukuba
Simulation for PID Performance
• Assumptions;– HIJING Au+Au 200 GeV
– Aerogel;
• n =1.011
• Saturated at 14 p.e. w. poissson distr.
• Occupancy 10%
– RICH ;
• n =1.0044 (CO2)
• Saturated at 10 p.e. w. poissson distr.
• Occupancy 3.4 % (NIM)
23 Yasuo MIAKE, Univ. of Tsukuba
Expected Proton Identification
• Require No-Aerogel & No-RICH
Occupancy
24 Yasuo MIAKE, Univ. of Tsukuba
Expected Kaon Identification
• Require Aerogel & No-RICH (Need TOF for < 5 GeV/c)
25 Yasuo MIAKE, Univ. of Tsukuba
PISA Activity
• All the known material put into PISA.
• Occupancy ~ 8 %
#of fired cell/ central event
~ 8% occupancyback ground sourcesseen in aerogel detector
26 Yasuo MIAKE, Univ. of Tsukuba
Radiation Length by PISA
• <Lrad> ~20 %– Similar to TOF
Radiation Length [%] -->
27 Yasuo MIAKE, Univ. of Tsukuba
Safety Issues
• Known issues; PMT-holder, HV protector
Item Fire Electrical
Status
1) Aerogel 2) Nyron(MC901) 3) Aluminum 4) Mylar5) Gore-tex6) PMT-Bleeder (G10)
-Estimated ?-?--
-----3.2 kV
NewNew---Tested
7) Signal connector PreAMP8) Signal connector Box9) H. V. Connector10) LED connector
UL94V-0UL91V-0/ UL94-0UL94V-0UL94V-0
300 V3 kV3 kV600 V
NewUsed at EMCalUsed at EMCal (but 3-pin)(Small type of )
11) Signal cable to PreAMP12) Signal Cable from PreAMP13) High voltage cable14) LED cable15) L. V. cable for PreAMP
UL ???UL-E108898?
?
?
NewNewLAN cable (Category-5E)?
28 Yasuo MIAKE, Univ. of Tsukuba
Aerogel/PMT Preparation at Tsukuba
29 Yasuo MIAKE, Univ. of Tsukuba
Box Production/Inspection at Dubna
30 Yasuo MIAKE, Univ. of Tsukuba
Dubna Contributions
• Dubna contributions have been very important from R&D’s to productions.
31 Yasuo MIAKE, Univ. of Tsukuba
Backups
32 Yasuo MIAKE, Univ. of Tsukuba
Jet Quench via Flavor Dependences
• Gluons in QCD stronger interaction than quarks
– Gluon density in nucleon larger in small x, & gg > qq
• Larger energy loss of gluons than that of quarks
• dEq/dx < dEg/dx
• At high pt, some particles are fragmented more from gluon than quark jet.
– Gluon jets fragment into same number of particles and anti-particles.
– Gluon jets produce more particles ; softer distr.
• Effect of jet qunching can be seen in particle ratios.
• As an example, anti-proton/proton ratio..
PRC58(98)2321
Nucl.Phys B420(94)583PRD51(95)3436
Good demonstration of importance of PID at high pt
region
33 Yasuo MIAKE, Univ. of Tsukuba
Occupancy Estimation
• TOF– ~ 100 cm2 at 5 m– Sensitive to all > 150 MeV/c– Backgrounds (low energy e/’s
from yoke & EM cal)– Occupancy 10% in Au+Au
• Aerogel of n = 1.01– Sensitive to all > 7.1– Delta rays in Aerogel (~%)– Muon from decayed pion– Backgrounds
• Using RQMD pt distr., occupancy of Aerogel estimated;– 10 % for 300 cm2 @ 4m– 5 % for 150 cm2 @ 4m
Estimation from pt distr. (RQMD)
TOF
Aer
TOF
(pt>0.18)
Aerogel
(pt>0.75)
Multiplicity 158 k 33 k
Segmentation 100 cm2 at 5m 300 cm2 at 4m
Sh
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