Bubble Chamber Beam Test September 2015

Run Plan

• 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 thin 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:

• Suppression of ¹⁴N(γ,p)¹³C events:

1. Determine an initial pressure and temperature with no beam
2. Start with beam at K.E. 6.5 MeV
3. Increase beam K.E. by 0.2 MeV steps all the way to 8.5 MeV
4. Adjust beam current to maintain a bubble rate of few per minute
5. Reproduce the overall rate shown above
6. At K.E. of 8.5 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. Reproduce the overall rate from oxygen isotopes shown above
6. 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

The expected yield is shown in the following figure:

The measured cross section using Penfold-Leiss unfolding is shown in the following figure: