Transcript TOF Slat

How We Became
Experimentalists
Suzanne Levine
Saba Zuberi
Len Zheleznyak
REU 2002
Define
Problem
Draw Conclusions
New
Questions
Arise
Develop Method(s)
to Investigate the
Problem
Design and Collect
Equipment Needed
for the Experiment(s)
Analyze Data
Collect Data
Develop a
Method to Collect
the Data. (DAQ)
Test,Calibrate, and
Understand the Equipment.
Determine Trends
Expected in Data.
PHOBOS at RHIC
TOF Walls
TZeros
TZeros
Detector Background Information
•The detectors being used provide information about the
energy and time of arrival of incident particles.
- Radiator
- Scintillator
Produces Cherenkov radiation
Atoms are excited when struck
when a charged particle in the
by charged particles producing
medium has a velocity faster
scintillation light when they
than the speed of light in that
decay to their ground state.
medium.
•When coupled with a PMT the light produced is converted to
electrical pulses that can be analyzed electronically.
Radiator
Bare scintillator
with light
guides attached
What’s the problem?
•TZero Counter:
[Cherenkov detector] Investigate the
timing properties of TZero Counters,
varying supply voltage and position of
incident particles. The results of our
investigation will be used to
determine the operating conditions for
the next run at RHIC.
•TOF (Time Of Flight) Slat:
[Scintillation detector] Understand
the position properties of TOF
scintillator with cosmic rays. The
results of the measurements can be
compared with the position studies
with an electron source.
TZero Counter
TOF Wall at RHIC
Develop a Method of Investigation
Example: TOF Slat Setup
TOF Slat setup in PHOBOS lab at Rochester
TOF Slat
PMT
PMT
to define
position
PMT
• Design a setup with three
PMTs to select and define a
position of cosmic rays
• In order for an event to be
recorded, signals must be
received by all three PMTs
• Study the response of the
TOF slat as a function of hit
position
Collect and Assemble Equipment
Scintillator Preparation to Optimize Light Collection:
• 4 steps to wrapping a scintillator
(i) polish scintillator with toothpaste
(ii) wrap in aluminum foil for maximum internal
reflection
(iii) apply optical grease to open end of scintillator and
connect to PMT
(iv) wrap electric tape over foil to stop external light
from penetrating the scintillator
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Electronics
LOGIC
TIME
ANALOG
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•Logic - Select the events
most likely to be cosmic rays
•Time - Measure the time
difference between the arrival of
the cosmic rays and light reaching
the PMTs
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•Energy - Measure the energy
DIGITAL
of the charged particle by
examing the pulse produced by
the PMT
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TIME
LOGIC
DAQ
Why do we need a DAQ?
A Data Acquisition
System (DAQ) will:
(i) Allow the user to read
the information from the
electronics on a PC
(ii) Present and store the
data in a way which is
useful to the user
(iii) Write data to files so
that it can be analyzed
later
ANALOG
DIGITAL
DAQ
Collect Data:
DAQ Graphical User Interface
19cm
QuickTime™ and a
Photo - JPEG decompressor
are needed to see this picture.
Diagram of Setup
Analyze Data
Example: Determine Position from Pulse Height
• L1 = A1e-(x/ )
L2 = A2e-((d-x)/)
•Log(L1/ L2) = -(2/)x + [d/ Log (A1/ A2) ]
•Attenuation factor for this scintillator is
44 + 7 cm.It was calcuated from the
gradient of this graph.
Log(L1/ L2)
•The charge measured is proportional
to the amount of light incident on the
PMT
QuickTime™ and a
GIF decompressor
are needed to see this picture.
Distance (cm)
• Timing resolution improves
with increased voltage up to
-2700V. Beyond this
voltage, no dependence of
resolution on voltage is
apparent
• A requirement was to
achieve a timing resolution
of under 100 picoseconds; at
-2700V the timing peaks
exhibit a 55 picosecond
resolution
Timing Resolution (ps)
Analyze Data:
Results of TZero Experiments
QuickTime™ and a
GIF decompressor
are needed to see this picture.
Voltage (V)
[note: suppressed zero]
Summary of Results
TZERO
• We found that the TZero
response has little
dependence on position
• We have verified that the
most effective operating
voltage is -2700V
TOF Slat
• We studied position
information by both time
and the amount of light
received by the PMTs.
• Both parameters indicate a
linear dependence
• We have determined the
attenuation coefficient to
be 44 + 7 cm and the
effective velocity of
propagation of light in the
scintillator to be
10.3 + 0.8cm/ns.
Lessons Learned
• More of your time is dedicated to isolating and identifying a
problem than correcting the problem itself.
• You learn the most from your mistakes.
• Keep good records. You can never write too much.
• Computers can be a dangerous tool; they will always give you
an answer, whether it makes sense or not.
• You learn a lot by explaining what you did to others.