Bubble Chamber Beam Test September 2015

Bubble Chamber Turn On

• Fill with natural N₂O – test bubble chamber systems operation

• With beam on bubble chamber radiator:

1. How does CCD camera perform under beam-on conditions?
2. Count rates on bubble chamber. Do we get single or multiple bubbles from Bremsstrahlung beam exposure?
3. Measure gamma ray beam spatial profile as reflected by bubble distribution. Is collimator effective in defining the gamma-ray beam?
4. Test the bubble chamber laser shutter (gumby shutter)

• Background measurements:

1. Measure beam off environmental background in chamber-injector area
2. Measure beam on background by looking outside fiducial volume
3. Measure background with beam to Faraday Cup in CEBAF beamline (about two meters from chamber)
4. Measure neutron events in chamber. Neutron radiation detectors in injector region will indicate if any neutrons are generated (especially at beam kinetic energies higher than 8.5 MeV).

Bubble Chamber Beam Test

• Chamber is filled with natural N₂O

• Cross sections:

The cross sections are shown in the following figure:

• Expected rates:

The expected rates are calculated with 3 cm cell thickness and Bremsstrahlung beam from copper radiator.

• The expected rates are shown in the following figure:

• The expected rates from oxygen isotopes are shown in the following figure:

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Run Plan:

• Check if Bubble Chamber is working properly:

1. Start with K.E. of 7.7 MeV
2. Determine the initial operational pressure and temperature
3. Measure bubble rate. The expected rate is 1 bubble per sec at 10 µA
4. Measure rate vs beam current (0.01, 0.1 and 1.0 µA)
5. Measure the number of bubbles for 30 minutes per beam current

• Suppression of ¹⁴N(γ,p)¹³C events:

1. Start with beam at K.E. 7.0 MeV
2. Increase beam K.E. by 0.2 MeV steps all the way to 8.6 MeV
3. Adjust beam current to maintain a bubble rate of few per minute
4. Measure the number of bubbles for 30 minutes per energy
5. Reproduce the overall rate shown above
6. At K.E. of 8.6 MeV, increase the chamber threshold by increasing the pressure. Suppress the ¹⁴N(γ,p)¹³C events.
7. Once ¹⁴N(γ,p)¹³C is suppressed, the rate should drop by three orders of magnitude

• Measuring rates from ¹⁸O(γ,α)¹⁴C:

1. Now the chamber is at the new pressure
2. Start with beam at K.E. 7.2 MeV
3. Increase beam K.E. by 0.2 MeV steps all the way to 9.2 MeV
4. Adjust beam current to maintain a bubble rate of few per minute
5. Measure the number of bubbles for 30 minutes per energy
6. Reproduce the overall rate from oxygen isotopes shown above
7. Note the change in slope of rates vs. beam K.E. and the sharp kink around 7.6 MeV

• Measuring ¹⁸O(γ,α)¹⁴C cross section:

1. Start with beam at K.E. 7.4 MeV
2. Increase beam K.E. by 0.1 MeV steps all the way to 8.4 MeV
3. Adjust beam current to maintain a bubble rate of few per minute
4. Perform Penfold-Leiss unfolding

Beam Kinetic Energy (MeV)	Beam Current (µA)	Time (hour)
7.4	10	10
7.5	10	10
7.6	10	5
7.7	2	5
7.8	2	5
7.9	1	5
8.0	1	5
8.1	0.8	5
8.2	0.4	5
8.3	0.2	5
8.4	0.2	5

The expected yield (counts) is shown in the following figure:

The Penfold-Leiss unfolded cross section is shown in the following figure:

• Root macro files used to generate the figures above (change txt to tar): media:BubbleTest_Sept.txt

Analysis Files

• Presentations=

• MCC 8 am presentation: media:FirstTests.pptx

• Events in fiducial volume: media:comp.png

• Beam Current:

The following command dumps the archived current readback from Keithley Picoammeter K6485 to a file:

mySampler -b "2015-09-10 18:00:00" -s 1s -n 14400 IFY5D04K6485dataRead > BubbleCur_Sept10.txt

• Data file of beam current on Bubble Chamber Faraday Cup or Radiator/Dump (September 10, 18:00 - 22:00): media:BubbleCur_Sept10.txt

• Data file of beam current on Bubble Chamber Faraday Cup or Radiator/Dump (September 11, 17:00 - 24:00): media:BubbleCur_Sept11.txt