Photon- and muon-induced reaction models
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.. list-table:: **ipnint**
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   * - Value
     - Explanation
   * -  | (D=0)
     -  | Options for photo-nuclear reaction. [#]_
   * -  | =0
     -  | This reaction mechanism is not considered.
   * -  | =1
     -  | This reaction mechanism is considered, except for nuclear  resonance fluorescence.
   * -  | =2
     -  | This reaction mechanism is considered, including nuclear  resonance fluorescence.
        | (See notes below this table for polarization of incident photons.)
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.. list-table:: **pnimul**
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   * - Value
     - Explanation
   * -  | (D=1.0)
     -  | Multiplying factor to increase sampling probability of  photo-nuclear  reaction.
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.. list-table:: **imucap**
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   * - Value
     - Explanation
   * -  | (D=1)
     -  | Options for capture reactions of negative-muons considering  characteristic X-ray production from muonic atoms and nuclear absorption.
   * -  | =0
     -  | This reaction mechanism is not considered.
   * -  | =1
     -  | This reaction mechanism is considered with default parameters used  for calculation of characteristic X-ray production.
   * -  | =2
     -  | This reaction mechanism is considered with user defined parameters  written in file(28) used for calculation of characteristic  X-ray production.
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.. list-table:: **iqmdscm**
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   * - Value
     - Explanation
   * -  | (D=0)
     -  | Option for Surface Coalescence Model [#]_ (SCM) in the  calculation of capture reactions of negative-muons.
   * -  | =0
     -  | Turn off SCM.
   * -  | =1
     -  | Activate the SCM.
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.. list-table:: **scm_h0**
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   * - Value
     - Explanation
   * -  | (D=0.25)
     -  | Adjustable parameter of SCM,  :math:`h0` . [GeV fm/c]
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.. list-table:: **scm_d**
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   * - Value
     - Explanation
   * -  | (D=1.75)
     -  | Adjustable parameter of SCM,  :math:`D` . [fm]
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.. list-table:: **scm_rcls**
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   * - Value
     - Explanation
   * -  | (D=-1.124)
     -  | Adjustable parameter of SCM,  :math:`Rcls` [fm].  The adjustable parameter of SCM,  :math:`R0`  [fm], is calculated as follows:
   * -  | > 0
     -  | :math:`R0 = Rcls`
   * -  | < 0
     -  | :math:`R0 = \left|Rcls\right| * A^{-1/3}`

For the nuclear resonance fluorescence considered in ipnint=2,  polarization of incident photons can be specified using sx,sy,sz  in the [source] section.  The angular distribution of the scattered photons is determined with  regard to the polarization. 

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.. list-table:: **imuint**
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   * - Value
     - Explanation
   * -  | (D=1)
     -  | Options for muon-induced nuclear reaction based on the virtual photon  theory.
   * -  | =0
     -  | This reaction mechanism is not considered.
   * -  | =1
     -  | This reaction mechanism is considered.
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.. list-table:: **imubrm**
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   * - Value
     - Explanation
   * -  | (D=1)
     -  | Options for muon-induced bremsstrahlung.
   * -  | =0
     -  | This reaction mechanism is not considered.
   * -  | =1
     -  | This reaction mechanism is considered.
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.. list-table:: **imuppd**
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   * - Value
     - Explanation
   * -  | (D=1)
     -  | Options for muon-induced electron-positron pair production.
   * -  | =0
     -  | This reaction mechanism is not considered.
   * -  | =1
     -  | This reaction mechanism is considered.
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.. list-table:: **emumin**
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   * - Value
     - Explanation
   * -  | (D=200.0)
     -  | Minimum energy of muon-induced nuclear reaction [MeV].  The change of emumin also changes the reaction cross sections over the entire energy range.
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.. list-table:: **emumax**
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   * - Value
     - Explanation
   * -  | (D=1.0e+6)
     -  | Maximum energy of muon-induced nuclear reaction [MeV].

.. [#]  Until ver. 2.30, this parameter was named ipngdr. 
.. [#] \Y. Watanabe and D. N. Kadrev, Proc. Int. Conf. Nucl. Data Sci. Technol. 2007 (ND2007) (2007) 1121-1124.