PC-2015-07-09a » History » Version 2
Pidcott, Celeste, 10 July 2015 13:28
1 | 1 | Rogers, Chris | h1. PC-2015-07-09 |
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3 | Chris Rogers |
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4 | Celeste Pidcott |
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5 | 2 | Pidcott, Celeste | |
6 | * Basic principle of measurement determined to be to prove consistency between |
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7 | - individual PID variables and MC |
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8 | - between the US variables |
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9 | - between the DS variables |
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10 | - between US and DS pid |
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12 | * Need to determine a way to represent the consistency (or lack thereof) between the probability of a pid given by the variables - some sort of plot that shows where variables are in agreement/disagreement/cases where one variable assigns a probability and the other doesn't. |
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14 | * The probrabilities assigned to each pid should be the probability of the particle having that pid at the tracker reference plane. |
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16 | * Currently, PDFs are created from simulations of non-decaying particles. Ideally, they would actually be made from particle samples taken from a simulation of a realistic beam, however this brings up the issue of how to simulate a realistic beam. |
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18 | * One possible alternative would be to begin with the PDFs that exist currently, and then determine the appropriate simulated beam by running the PID, improving the make-up of the beam based on iterations of the PID routines. |
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20 | * Chris suggested looking at how other experiments have validated their PID routines. Celeste had looked into this previously and only ever seen this done by experiments pre-supposing to know the particle types used in their validation samples. Chris suggested asking Steve B how they did their validation for T2K. |
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21 | - Turns out they used test beams so again the particle types were already known, and determining the consistency of the PID still looks like the only way forward. |