21
Table 3-1: Table summarising the various properties of the scintillators under study.
Scintillator
EJ200
EJ208
EJ260
BC408
UPS923A
Protvino
Manufactured by:
Eljen
Technology
Eljen
Technology
Eljen
Technolog
y
Saint Gobain
Crystals
Institute of
Scintillating
Materials,
Kharkiv.
(Used
in
MBTS)
Institute of High
Energy
Physics
(IHEP),
Protvino
in
association with
SIA
luch,
Podolsk.
(Used in Tile
Barrel)
Base
PVT
PVT
PVT
PVT
PS
PS
Primary Fluor
0.3%
organic
fluors
0.3%
organic
fluors
0.3%
organic
fluors
Not available
(However,
listed
as
a
performance
equivalent of
EJ200)
2% PTP
1.5% PTP
Secondary Fluor
0.03%
POPOP
0.044%
POPOP
Light Output, %
Anthracene
64
60
60
64
60
Not available
Wavelength
of
Max.
Emission,
nm
425
435
490
425
425
Rise Time, ns
0,9
1
~
0,9
0,9
Decay Time, ns
2,1
3,3
9,2
2,1
3,3
Density, g/cc:
1,023
1,023
1,023
1,032
1,06
Refractive Index
1,58
1,58
1,58
1,58
1,6
Light
attenuation
length (cm)
~400*
~400*
~400*
380**
400
Source
[21]
[22]
[23]
[24]
*In a cast sheet of dimensions 2 cm x 20 cm x 300 cm
**In a cast sheet of dimensions 1 cm x 20 cm x 200 cm
22
The Protvino type plastic scintillators were manufactured specifically for the Tile
Calorimeter using an injection molding technique. The design
of the scintillator
was specifically geared towards cutting cost of manufacture since these
scintillators were to be used in the barrels and would require a large quantity of
material. In comparison to a similar Bicron RH4 cast scintillator, the Protvino
scintillator yielded ~2.5 times less light in response to ~3 MeV minimum ionizing
beta particles from a Ru
106
source [25].
Studies were also conducted by the Institute of High Energy Physics (IHEP) team,
into the effect of changing concentration of the fluors.
For an increase in PTP
concentration from 0.1% to 0.2%, the light output increased by 10% , whilst an
increase in concentration of POPOP from 0.02% to 0.1% had little effect on light
yield [24]. Since UPS923A scintillators are very similar in composition to the
Protvino type, with the exception of different
concentrations of fluors, we can
assume that they are the better performing of the two in terms of light response.
UPS923A is marketed by the manufacturer as being a good general purpose
scintillator with good transparency.
EJ200 and BC408 are recommended by their respective manufacturers, for use in
time of flight systems which require large area coverage
due to their short rise
and decay times. They also have the highest light output from the 6 scintillators
investigated.
EJ208 has a longer emission wavelength than EJ200, and is ideal for systems in
which uniformity of light collection is of utmost importance, whilst timing takes
a secondary priority. In addition, EJ208 is predicted to offer greater tolerance
against radiation damage since damage results in the increased optical attenuation
of light at shorter wavelengths.
EJ260 has the longest emission wavelength and shifts light to the green spectrum.
It is therefore proposed to offer greater radiation tolerance than conventional blue
emitting plastic scintillators and can still be coupled
to common blue sensitive
phototubes.