5.2.25. Others

Table 5.2.211 inucr

Value

Explanation


Option for selecting the output quantities in the cross-section and kerma-factor output mode (icntl=1). Please see “phits/sample/icntl1” in more detail.
=2
Output total, inelastic, and elastic reaction cross sections of a target nucleus.
=12
Output neutron kerma factors of a target material.
=14
Output photon kerma factors of a target material.
=16
Output stopping power of charged particle in a target material.
=100
Output various data contained in cross section libraries of a target material.
Table 5.2.212 idam(i)

Value

Explanation

integer
User-defined integer variable.
Table 5.2.213 rdam(i)

Value

Explanation

real*8
User-defined real variable.
i=1-100
These values can be used in the PHITS code by
common /userp/ idam(100), rdam(100)
Table 5.2.214 icommat

Value

Explanation

(D=0)
Option for comment marks in [material] section.
=0
c \(\sqcup\) ( \(\sqcup\) is a space) cannot be used as comment marks.
=1
c \(\sqcup\) ( \(\sqcup\) is a space) can be used as comment marks.
Table 5.2.215 idvkmat

Value

Explanation

(D=0)
Number of materials to be used in DVK mode. DVK mode is intended for use in combination with RT-PHITS; for details, please refer to 0utility/RT-PHITS/DVKmode . Furthermore, if a negative value is specified, the calculation mode remains unchanged (normal particle transport is performed), but the simulation is accelerated by performing source sampling in ascending order of xyz for settings with s-type = 22 (xyz-mesh source) and isbias = 2 .

From version 2.89, in the default setting, c \(\sqcup\) ( \(\sqcup\) is a space), cannot be used as comment marks in [material] section. To use c \(\sqcup\) as comment marks in the section, set icommat=1.