PHENIX High pt Upgrades

Recent Progress
 (April Core Week)
Yasuo MIAKE
For High pt Upgrade Team
http://utkhii.px.tsukuba.ac.jp/~highpt/

Plan Guestimate
Coverage of 4 TOF panel equivalent as a first stage
150 modules
300 PMT’s ; 12,000,000 yen
400 liter; 20,000,000 yen
Total ; ~40,000,000 yen
Since no space on the East, we install on the West.
Remove 2 lower TOF panels from the East after successful pp measurements
1 spare panel
1 panel to be constructed
TOF 1 panel ; 13,000,000 yen

Extended PID
Measurements of Transmission
Shorter transmittance for shorter wave length.
Shorter transmittance for smaller index.

Wave Length Dependece
Consistent with Rayleigh scattering.
Scatt. dominant
Small absorption
Well known as optical property of Aerogel

Two Design Concepts
KEK-BELLE Type
Collect scattered photons
Non-directional lights
Area of photocathode/cell size
2 PMT per cell
more expensive
Mirror Type
Collect direct photons
Directional lights
Efficient way to get light!?
Sophisticated mirror design?!
Easy to get larger cell size
1 PMT per Cell
Cheaper
Should be easier to stack

KEK Beam Test Setup
Particle Identification
Gas C for electron
TOF for hadron ID
KEK pi-2 channel
1 - 4 GeV/c for momentum scan

Aerogel Signal for protons and pions
Clear separation of protons and pions observed.

Belle Type (1) Reflector
Three types of reflector.
Tyvek
Millipore
Goretex
Offline optical measurements at BNL says “Tyvek is good”
Effect of reflector
Without reflector, < 1/4
Reflector is essential for Belle Type

Belle Type (2) Position Dep.
With Goretex, >25 p.e. obtained everywhere.
In each PMT, exponential behaviour is observed.
 Goretex ; λ= 7.0 cm
Tyvek ; λ= 5.5 cm
Exponential shape may not be trivial.
Attenuation may be due to property of reflector rather than that of aerogel itself.

Belle Type (3) Angular Dep.
Seems to be proportional to the thickness of the aerogel.
Scattered photons have no directionality.

Belle Type (5) Thickness Dep.
Photons proportional to the thickness of the aerogel.
Consistent with;
Angular dependence
No directionality

Mirror Type (1) Shape of Mirror
Flat vs Parabola Mirror
Aluminized mylar sheet with styro foam backing (hand made)
No significant difference at the center as expected from the cone angle of 10 degree.

Mirror Type (2) Position Dep.
Expected Position Dep.
Relation of  Cone angle ~ 10.1 deg. and PMT size
Expected diameter ~ 3” PMT
Broad peak at the center
No significant difference between Flat and Parabola mirrors.

Mirror Type (3) Thickness Dep.
Saturate!
Difficult to get more p.e.
Due to short transmittance

Bell vs Mirror
Even with Mirror type, reflector is important !

Directional vs Scattered Photons
Is the worse results with mirror type due to bad mirrors?
Note that it is hand made with aluminized mylar sheet.
Other way to measure Directional/Scattered photons.
Rotate Belle Box and put the beam straight to aerogel and PMT.
To remove signals from PMT window, subtract (b) from (a).

Measurements with 2” PMT
Assume uniform angular distribution of scattered photons.
Out of 17 p.e. (straight beam geometry), 8 p.e.’s are scattered photons.

Summary of KEK test
Belle Type
It works;  > 20 p.e.
We can estimate performance of Belle Type with any cell size, any thickness.
We understand pretty well.
Mirror Type
~ 10 p.e.
Direct photons at most 10 p.e.
Is there a better way to collect direct and scattered photons? Otherwise, Belle Type seems to be the best.
Needs to be studied
Better mirror? (I’m pessimistic)
UV vs. non-UV PMT
PMT selections
Gain too low?
Russian PMT?
Test of electronics
Use of PMT amp?
First priority of the next test;
Effect of integration sphere behind the aerogel.

Participation of JINR-LHE, Dubna
Two people at KEK last Dec. 01.
Y.M. visited Dubna in March 02.
A.Malakhov
A.G. Litvinenko
S. Afanasev
V, Ladyguine
L. Zolin
A. Kurepin
E. Kravchenko

Participation of JINR-LHE, Dubna
Will have official Agreement between Dubna and Tsukuba for High pt project.
Their participation;
Mechanical design
Mechanical constr.
etc etc
Next KEK Test in May
S. Afanasev
V. Peressedov
L. Zolin