Γγ Coincidence and unsuccessful linear gate method results

In summary, the setup for the linear gate method in a γγ coincidence experiment involved using a Na22 source and connecting the SCA output to the logic shaper and then to the MCB gate input. However, changing the angle of one detector did not affect the count rate as expected. Possible troubleshooting steps include checking connections, settings, detector alignment, and source calibration and placement.
  • #1
says
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I had this setup (see attached photo) for the linear gate method in a γγ coincidence experiment. Using a Na22 source.

The pulse from the movable detector enables the gate of the MCB, and any corresponding pulse from the fixed detector that arrives within the gate interval will be considered coincident and will be counted in the spectrum.

Basically, we wanted the signal from the SCA to enable the input of the MCB at the right time. This was done by connecting the SCA output to the logic shaper, and then the logic output to the gate input of the MCB.

However, changing the angle of one detector didn't change the count rate. As the angle between the two detectors was moved either side of 180 degrees we should have seen a reduction in the count rate. However, it generally stayed the same. I'm not really sure why. Everything was connected correctly.

I'm hoping someone has conducted this experiment and method before and this isn't too much of an uncommon error as I want to do it again and would rather not have to troubleshoot for hours!
 

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  • #2
I'd suggest checking the following: 1. Make sure the SCA output is connected properly to the logic shaper, and that the logic shaper is properly connected to the MCB gate input. 2. Make sure the logic shaper is set up correctly to enable the MCB gate input.3. Make sure the MCB gate width is set up correctly.4. Make sure the detectors are properly aligned with each other.5. Make sure the source is properly calibrated.6. Make sure the source is placed in the correct position.
 

1. What is a Γγ coincidence?

A Γγ coincidence is a phenomenon in which a gamma ray and a neutron are detected at the same time, indicating that they were emitted from the same nuclear reaction. This can provide valuable information about the properties of the nucleus that emitted the particles.

2. How is the Γγ coincidence method used in scientific research?

The Γγ coincidence method is commonly used in nuclear and particle physics research to study the properties of atomic nuclei. It allows researchers to measure the energies and angular distributions of gamma rays and neutrons emitted from nuclear reactions, providing insights into the structure and behavior of nuclei.

3. What is the linear gate method and how is it used in conjunction with the Γγ coincidence method?

The linear gate method is a technique used in conjunction with the Γγ coincidence method to select and analyze specific types of nuclear reactions. It involves setting up a linear gate around the expected positions of gamma rays and neutrons in a detector, which allows researchers to filter out unwanted events and focus on the desired reactions.

4. What factors can lead to unsuccessful linear gate method results?

There are several factors that can contribute to unsuccessful linear gate method results, including detector inefficiencies, poor alignment of the detectors, and background noise from other sources. Additionally, if the gate is not set up properly or if the expected reactions do not occur at the expected energies, the results may be unsuccessful.

5. What are some potential solutions to improve the success rate of the linear gate method?

To improve the success rate of the linear gate method, researchers can carefully calibrate and align their detectors, minimize background noise through shielding and other techniques, and conduct multiple experiments to ensure consistent results. Additionally, using advanced statistical methods to analyze the data can help to increase the accuracy and reliability of the results.

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