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Usrmed.f for optical photons reflection
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3
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196
|
28 February 2024
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Interpolation scheme in fluscw.f routine
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3
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209
|
12 March 2024
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Event time information
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4
|
307
|
14 February 2024
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Frghns.f direction of reflection
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3
|
177
|
13 February 2024
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Neutron yield from different reaction channel in case of alpha on Sn 116
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9
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361
|
14 February 2024
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Defining magnetic field map from tabulated .txt file
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6
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535
|
9 February 2024
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How to implement .inp file with two fortran file?
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3
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173
|
6 February 2024
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USERDUMP empty output
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5
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348
|
18 January 2024
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Z not conserving in few reaction channels for proton on 7Li reaction
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3
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156
|
6 February 2024
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How to overwrite 50%-50% assumption on isomer production
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3
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167
|
1 February 2024
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How to get readable output in MGDRAW
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7
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353
|
17 January 2024
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Time information
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2
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266
|
25 January 2024
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No of stars and mgdraw output when LAM BIAS card is used
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7
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256
|
25 January 2024
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Circular Proton Beam ( trying to replicate GEANT4 simulation)
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2
|
201
|
22 January 2024
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Modify mgdraw.f routine
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4
|
251
|
8 January 2024
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Flag secondary particles which are the same kind of the one initiating the collision
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6
|
710
|
8 January 2024
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Scoring of equivalent dose for decay of multiple radionuclides
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4
|
289
|
8 January 2024
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WVLNGT variable in multiple user routines
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3
|
174
|
12 December 2023
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What is the exact meanings of weight window?
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3
|
361
|
11 December 2023
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How to debug file include user routine/sub function
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3
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249
|
8 December 2023
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The meaning of dummy arguments
|
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11
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297
|
29 November 2023
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Problems implementing mgdraw
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5
|
249
|
8 December 2023
|
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How to create a mgdraw routine
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4
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662
|
10 November 2023
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Import DICOM images in FLAIR
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2
|
389
|
7 November 2023
|
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CYLI-VOL source and
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3
|
453
|
3 November 2023
|
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Quenching in mgdraw.f
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6
|
416
|
14 October 2023
|
|
Isomer energy level(continue)
|
|
5
|
339
|
14 October 2023
|
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Distinguishing neutrinos from decay-at-rest and decay-in-flight
|
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3
|
235
|
19 October 2023
|
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X-ray tube simulation
|
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9
|
979
|
17 October 2023
|
|
Obtaining particle energy at beginning and end of step
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|
8
|
457
|
12 October 2023
|