Difference between revisions of "QADC spectrum"
Jump to navigation
Jump to search
| Line 6: | Line 6: | ||
=Data Collected= | =Data Collected= | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | GO BACK [https://wiki.iac.isu.edu/index.php/Performance_of_THGEM_as_a_Neutron_Detector#Data_Analysis] | ||
Revision as of 03:04, 17 October 2013
QADC Analysis
The first test for the detector signal after installing U-233 is by using CAEN V792 QDC (Analog charge to digital converter). The aim of this test is to distinguish the emitted particles from U-233 source based on liberated charge from their ionization in gas.
Electronics Description
Data Collected
GO BACK [1]