The bug of MPI parallel calculations with tetrahedral-geometry stopped abruptly in ver. 3.10 has been fixed.
The bug that the magnetic field maps given in r-z grid (type=-2 or -4) cannot be properly considered has been fixed.
Annihilation photons are double counted in the RI source generation function when the production of both positron and photon are considered. To avoid the problem, a new parameter iannih has been introduced to exclude the annihilation photons in the case of proj=photon.
The new parameters cnt(1), cnt(2), and cnt(3) have been introduced in [source] section to specify the initial counter values for each multi-source subsection
[ phits310 ] 2019/04/09 Important improvements
A new function to generate source particles from tetrahedron geometry was implemented.
mesh=xyz became available in [weight window] and [t-wwg] sections.
Coefficients depending on particle type can be defined in [multiplier] section, using part parameter. Owing to this improvement, several types of radiation doses can be directly calculated using pre-defined [multiplier] sections.
[t-deposit] with output=deposit can be used in the case that source weight is not 1.
A bug in [t-deposit] in the cases of output=deposit, dresol≠0 and part≠all was fixed.
A bug in the range calculation of charged nuclei in some tallies when iMeVperu=1 was fixed.
The probability density of the number of interactions by individual history can be outputted from [t-star]. The number of interactions occurred in the track-structure mode can be also counted in the tally. In addition, the tally name was changed to [t-interact] in order to explicitly state that it is the tally for counting the number of interactions, though the former name [t-star] can still be accepted.
The function to calculate the deposition energy using kerma approximation, which used to be implemented only in [t-heat], became available in [t-deposit]. Necessity of the use of kerma approximation in the energy deposition calculation is automatically judged based on the status of e-mode and negs specified in [parameters] section. Owing to this improvement, we recommend to use [t-deposit] instead of [t-heat] in all situations of deposition energy calculations.
[t-deposit] with output=deposit can be used in the case that weight is not always 1 unless weights of energy depositing particles change within one history. Then, this mode works in the cases that you set s-type=9 and dir=-all in [source] section, or you use [forced collisions] for neutral particles.
The graph style for [t-cross] with axis=z is changed from histogram to dot & line.
Specification of z-type=1 and nz=0 is allowed for [t-cross] to calculate fluences of particles passing through a certain surface.
Numbers of delta-rays produced by ions (including protons) and knock-on electrons produced by electron scattering can be separately calculated in [t-interact] section. In addition, they can be distinguished in [counter] section too.
RI source function was improved to produce Auger electrons even when the Auger electron spectrum data are not included in RIsource.ack.
A bug in [t-product] in the case of iMeVperu=1 was fixed.
By defining igamma as negative, Doppler effect owing to the motion of the emitter nuclei is disregarded. Specific gamma-rays are observed as mono-energetic peak in the energy spectrum.
GEM Ver.2 including nucleon-gamma emission competition was developed. This version is available by setting ngem=2 in [parameters] section.
New format of [transform] was implemented to deﬁne rotation around z,y,x axes simply.
The distributed-memory parallel computing using a MPI protocol became available on Windows.
mesh=xyz became available in [weight window] for EGS5.
Conversion coefficients for soft error rates on semiconductor devices were added to default data of [multiplier].
The user-defined activation cross section data can be used in the [t-yield] and [t-dchain] sections.
For RI sources, characteristics x-ray and internal conversion electron are now considered.
Tetrahedral geometries that are converted from CAD can now be used, even when the surface of tetrahedron does not perfectly match the boundary surfaces.
The parameters (c1-c99) specified in the input file can be used in the user-defined source file ("usrsors.f").
The high-speed mode of ANGEL, which does not check numerical data while plotting the results, has become the default.
For cylindrical sources (s-type=1), a few bugs, such as the bug occurring when a source particle is sampled between 0 and r1 with the setting of r0=r1, have been fixed.
Procedure for coupling PHITS with thermal analysis software such as ANSYS Fluent is established. For this purpose, a function to read tetrahedral-mesh geometry written in bulk-data format of NASTRAN is implemented. A new mesh option, mesh=tet, is introduced in [t-track], [t-deposit], [t-yield], [t-product], and [t-dpa] to output the tallied quantities in each tetrahedral mesh. Field-data format used in OpenFoam, which can be directly read by thermal analysis software, has become selected as an output format.
As a part of the improvements for coupling with thermal analysis software, a new option, unit=5, is introduced in [t-deposit] to output the deposition energy in J/m3/source.
Sample ﬁles for using high-energy nuclear data library JENDL-4.0/HE are provided in the PHITS package.
A function to read magnetic ﬁeld maps written in xyz or r-z grid is implemented.
[t-dchain] has become applicable to mesh=xyz. In reply to this improvement, DCHAIN-SP is also updated. Note that the function to visualize the induced activities in xyz mesh has not been developed yet.
Error and warning ID numbers are introduced for some messages.
A nuclear reaction model to handle the reactions by electron-, mu-, tau-neutrino and their antiparticles up to 150 MeV of incident energy is incorporated. Neutrinos can interact with orbital electrons, 1H, and 2H whereas the nuclei heavier than 2H are currently out of the range of this model.
INC-ELF, an intra-nuclear cascade model developed by Kyushu University, is updated to consider collective excitation of the target nucleus and to precisely calculate charged particle emission barriers.
Electron track-structure mode is improved to consider the production of Auger electrons.
User-defined energy resolution function has been implemented to [T-deposit] in order to reproduce energy resolution which cannot be realized by dresol and dfano. Users can deﬁne the functional forms of energy resolution in "usresol.f," which is activated by defining negative dresol. As a sample, the default "usresol.f" contains a numerical model proposed by Meleshenkovskii et al. to reproduce asymmetric peaks of a CdZnTe detector.
A new option, gshow=5 and [t-gshow] with output=10, is introduced to visualize the geometry in the pixel format. This option is useful for properly visualize the geometries with ﬁne structure such as voxel and tetrahedral phantoms.
Time for reading lattice structure is reduced by introducing compressed format.
Some parameters in the muonic atom cascade program have become adjustable.
The third user-defined function, "usrdfn3.f," is introduced for weighting the results of [t-deposit]. The default program of usrdfn3.f can convert the absorbed dose to the water equivalent dose, which is frequently used in medical physics.
Remaining batch number has become adjustable using "batch.out."
In [t-cross] with mesh=xyz or r-z, a new option, enclose=1, is introduced for calculating incoming and outgoing particle fluxes (or currents) from each mesh.
Deposition energies in the cells with the same ID but placed in different lattice coordinates can be separately analyzed in the case of [t-deposit] with output=deposit.
Nuclear data libraries containing more than 1000 γ-ray spectra such as the latest version of ENDF and JEFF have become acceptable in PHITS.
The fixed charge mode, ifixchg=1, is introduced for calculating the stopping power of particles with a certain charge state. Note the charge exchange reaction has not been implemented yet, so the fixed charge mode is appropriate only when target material is extremely thin at this moment.
Several bugs are fixed, including the problem in positron transport when emin(12) is specified without specifying emin(13), and that in electron and positron transports in the magnetic ﬁeld defined at a lattice structure.
[ phits302 ] 2017/12/05 Important improvements
New parameters nudtvar and udtvar(i) were introduced for [t-userdefined]
New options were implemented for the unit of [t-let] and [t-sed]
The bug in the calculation of angular straggling using nspred = 2 was fixed.
This bug was introduced in PHITS2.96, and calculation results for charged
particle beam using the versions between 2.96 and 3.01 might be strange.
A special ANGEL parameter sangel was introduced to insert all ANGEL parameters
into tally output files.
Reading algorithm for tetrahedral geometry was revised to reduce the computational
ANGEL was revised to reduce the computational time for making eps files of 2-dimensional plots
[ phits300 ] 2017/10/17 Important improvements
In the default setting, "c" became unusable as comment marks in [material] section in order to avoid an error that the elemental symbol for carbon, C, is read as comment marks.
When you use "c" as comment marks in the section, set icommat=1 in [parameters] section.
A new option of [t-deposit] was developed to sum up the deposit energies weighted by user defined conditions.
This option can be applied to simulation, for example soft errors in semiconductor devices.
A new function to use results of tallies as an energy distribution of source particles was added in [source].
This function can be used by specifying e-type=20.
User defined function 2 (usrdfn2.f) in [t-deposit] was changed to the new option to estimate biological dose on the basis of Microdosimetric Kinetic Model.
See the paper in more detail.
A new function to analyze the motion of electrons and positrons in the electro-magnetic fields was implemented.
The default value of the ascat2 parameter introduced in version 2.77 was revised from 0.088 to 0.038, in accordance with the original paper.
The PHITS results obtained by setting nspred=2 without specifying ascat2 will be changed.
A new function to generate xyz-mesh distribution source was implemented.
Using this function, you can reproduce sources having a complex spatial distribution.
A new tally named [t-volume] was developed in order to automatically calculate the volume of each cell.
A new parameter timeout was introduced in the [parameters] section.
When CPU time exceeds this value, the PHITS simulation is automatically stopped.
A new parameter stdcut was introduced in each tally.
When the all statistical uncertainties of the tally results become less than this value, the PHITS simulation is automatically stopped.
Nuclear and atomic interactions are explicitly distinguished in [t-product], [t-star], and [counter].
Information on further detailed channels such as the production of bremsstrahlung can be also deduced.
A new function to display error bars of statistical uncertainties in eps files of tally results was implemented.
This function is available by setting epsout=2 in each tally section.
Some bugs in the combination of EGS5 and [t-cross] or [t-track] were fixed.
The default setting of output in [t-dchain] tally changed to cutoff in order to score particles stopped in specified regions.
Note that in the previous setting output=product heavy ions produced in a thin target were scored even though the ions don't stop in the target.
A new parameter file(1) was introduced to specify the PHITS installation folder name.
When you properly set this parameter, you do not have to specify the name of other input files i.e. file(7, 20, 21, 24, and 25) unless you have changed the folder structure of PHITS.
A new parameter nucdata was introduced to automatically adjust emin(2) and dmax(2) parameters suitable for JENDL-4.0.
The default value of this parameter is set to 1, i.e. neutrons below 20 MeV are automatically transported using nuclear data library.
A new option for negs parameter, -1, was introduced.
When you set negs=-1, PHITS treats photon transport using the original algorithm (i.e. not EGS5), and ignores the electron and positron transport.
This option is selected as the default setting.
The default value of ides parameter was changed to 1, i.e. photon does not produce electrons in the PHITS original algorithm.
If you would like to transport electrons and positrons, you have to use EGS5.
The default value of igamma parameter was changed to 2, i.e.
γ-rays are produced in the de-excitation process based on EBITEM model in the default setting.
RI source function was improved to be applicable to α and β decays including Auger electron production.
Track-structure mode was developed in PHITS.
Using this mode, PHITS can analyze ionization, excitation, and oscillation induced by electrons and positrons event-by-event.
A new method for calculating the energy loss of charged particles with explicitly generating δ-rays was developed, based on their restricted stopping power.
This method is selected as the default setting, i.e. irlet=1.
JAMQMD, which is used for simulating nucleus-nucleus interactions above 3 GeV/u, was improved to consider the relativistic effect.
[t-dpa] was improved to be capable of calculating DPA by electrons, positrons, pions etc.
Bug in the normalization process of the self-fission source (ispfs option) was fixed.
The procedure for s-type depending on the setting of the energy of source particles was changed.
The mono-energetic and energy-distributed sources can be defined by setting e0 and e-type, respectively, irrespective of the value of s-type.
If both e0 and e-type are defined, the energy is decided according to the previous procedure of s-type.
A new section [ww bias] and a new tally [t-wwbg] were implemented to bias [weight window] to obtain better statistics for a certain direction.
The numerical data of tally results are outputted after each batch is finished even for itall=0 (default).
Thus, the difference between itall=1 and 0 is whether the image (*.eps) files are generated or not.
Only related tallies to the setting of the icntl parameter work.
For example, all tallies except for [t-volume] are disabled when icntl=14, while [t-volume] is disabled when icntl≠14.
Warning is outputted when infl or set command is written in the disabled section.
Some ANGEL parameters were introduced to change the length or time axis of figures.
For example, you can draw a figure of spatial dose distribution with the axis in nm scale by setting angel=cmnm in the tally.
PHITS execution is terminated when two or more [parameters] sections exist in one input file.
A new parameter iMeVperu was introduced to convert the unit of nucleus energy [MeV] to [MeV/u] in outputs of all tallies.
By setting of iMeVperu=1 in [parameters], all tally results are output with the unit of MeV/u for the nucleus energy.
New parameters r-from and r-to in [t-cross] with mesh=reg were added, because conventional parameters r-in and r-out were confusing.
r-from and r-to can be used instead of r-in and r-out, respectively.
The option of the stopping power ndedx=3 became applicable for target nuclei with the mass number of 93≤ Z≤ 97 (from Np to Bk).
By adding "$OMP=N" (N is the number of CPU cores to be used) before the first section in a PHITS input file, the shared-memory parallel computing using OpenMP is executed.
Even when infl: is set, a line of "file=input file name" is not required.
In Mac OS, a terminal window is opened when PHITS is executed by drag and drop on the Dock.
Note that these function are not available when to run PHITS on the command line on Linux and so on.
The default value of the switching energy from JQMD to JAMQMD, ejamqmd, was changed to 3GeV.
The Kurotama model was used as the default model to give nucleus-nucleus reaction cross sections.
The natural isotope expansion was effective in input files of DCHAIN-SP generated by [t-dchain].
[ phits288 ] 2016/09/30 Important improvements
Neutron decay can be considered. Mean life time of neutron is approximately 886.7 sec.
Bug in the treatment of the Doppler effect using the EGS5 mode was fixed.
Bug in the high-energy photon transport (approximately above 10 MeV) using
EGS5 mode was fixed. You do not have to set "deltm = large value"
Bug in the capture reaction of negative muon when 1H is included in the
material was fixed.
The unit of esmin and esmax parameters is changed from MeV to MeV/u. These parameters define the minimum and maximum energy of charged particles treated in the simulation, respectively.
Algorithm of stopping power calculation ATIMA in PHITS was improved to
reduce the computational time. Then, the default model for calculating
stopping power was changed from SPAR to ATIMA.
High-energy heavy ion reaction model, JAMQMD, which works above 3 GeV/u,
was improved to JAMQMD2, in the same manner as JQMD. The accuracy as well
as the stability of the calculation are improved, particularly for cosmic-ray
The pion total reaction cross section model was improved, and employed
as the default model.
A new model for deuteron-nucleus total reaction cross sections was introduced.
This model can be used by setting icrdm=1 in [parameters] section. See
this paper in more detail.
Muon nuclear reaction model was improved. See this paper in more detail.
A new section [Data Max] was introduced to specify the dmax parameter for
each nucleus and material.
A new parameter natural was introduced. When you define an element without
specifying its mass number in [material] section, and set natural = 1 or
2, PHITS assumes that it has natural isotope composition.
The RI-source function was implemented. Using this function, PHITS can generate photon sources with energy spectra of radioisotope (RI) decay by simply specifying the activity and name of the RIs. Nuclear decay database DECDC was used in this function. This database is equivalent to ICRP107.
The name of file to output the current batch information was changed from
batch.now to batch.out. You can specify this file name by setting file(22)
in [parameters] section.
A function to output the tally results in xyz-mesh in the input format
A new tally [t-wwg] was introduced. Using this tally, you can automatically
determine an appropriate setting for the [Weight Window] section.
The arrows to indicate the xyz coordinates are depicted in [t-3dshow] tally.
Two options of the function about user defined cross sections were developed.
One is an extrapolation function to extrapolate given data for incident
energies, emission angles, and emission energies. The other is effective
in the case that there are no data of differential cross section. You can
use nuclear reaction models to simulate nuclear reaction events only with
data of total reaction cross section.
[ phits282 ] 2015/12/25 Important improvements
The following improvements related to EGS5 mode were implemented, and some bugs of the mode were revised.
A new parameter ipegs was introduced to control PEGS5 execution before PHITS simulation.
A new parameter imsegs was introduced to precisely simulate the multiple scattering of electron every time when electron goes into a new material.
The limitation of the number of material when you use EGS5 was eliminated.
However, PHITS calculation may crash due to insufficient memory when you
define more than a few hundred materials. In addition, the maximum number
of elements per one material is still limited to 20.
Mass data from carbon to aluminum (6 =< Z =< 13) were revised.
Algorithm to consider energy straggling of charged particles was revised to reproduce the doses around Bragg peak more precisely.
A new parameter idelt was introduced to reduce the computational time for particle transport simulation in very large gas area. When idelt=1, deltm and deltc are divided by the density of each material.
Muon-nuclear interaction model was implemented. Characteristic X-ray production from muonic atoms as well as associating muon capture reaction can be also considered.
The function for simulating nuclear resonance florescence (NRF) was implemented. In this function, the polarization of photon can be also considered.
A new parameter pnimul was introduced to bias the photo-nuclear reaction cross section against photo-atomic interaction cross section.
A new parameter NONU was added in [parameters] section to control the neutron multiplicity.
We changed the default setting of the nuclear reaction model in the case that light ions are targets. When such a reaction occurs, PHITS calculates it with regarding the light ions as projectile on the basis of the inverse kinematics. For example, in the default setting, INCL is used even for heavy ion induced reactions when deuteron is set to be its target nucleus.
Some bugs in the muon- and photon-induced nuclear reaction models as well as JQMD-2.0 were fixed.
Three new functions were implemented in [source] section.
Generation of neutron sources from spontaneous fission by ispfs parameter.
Generation of source particles from a triangle prism.
Generation of source particles with arbitrary time information.
The function to properly calculate the uncertainty of tally results was implemented in the case of using dump source.
The function to read tetrahedral geometry (a kind of polygonal geometry)
was implemented. This implementaion was carried out under support of HUREL, Hanyang University, Korea.
The function to read user defined cross sections was implemented.
A new option fiss was added in [counter] section to output the information on secondary particles generated through fission reaction, particularly in each generation of sequential fissions.
Point estimator tally [t-point] was implemented to calculate the particle fluence at a certain point or ring.
A new function to calculate the particle fluence in sector prisms was implemented in [t-track] tally by introducing θ mesh in the case of mesh = r-z.
Contribution of each particle can be properly calculated using [t-deposit] with output = deposit option.
A new parameter elastic was added in [t-yield] tally to output recoil nucleus from elastic scattering.
Restart calculation using [t-dpa] tally became feasible.
A new output option was added in [t-star] tally to output star density for a reaction which induces transmutation of target nucleus.
The maximum number of regions that can be specified in [t-dchain] was extended up to 500. We fixed a bug in [t-dchain] to properly consider the successive lines.
Sum tally function became applicable to all tallies except for [t-dchain].
We fixed a bug in [t-heat] with mesh=r-z.
We fixed a bug in [t-deposit], mesh=reg, output=deposit when you use [delta-ray] section.
Bug in the calculation of the uncertainty of [t-yield] was fixed.
We revised makefile to consider the dependence of each source file. Owning to this improvement, you can use "make -j" option to speed up the compilation of PHITS.
Instructions how to use tetrahedral geometry (TetraGEOM), point estimator tally (tpoint), and user-defined tally (usrtally) were added in the utility folder.
[ phits276 ] 2015/03/20 Important improvements
Transport algorithm for photons, electrons and positions in EGS5 (Electron
Gamma Shower Version 5) was incorporated..
Muon-nuclear interaction model based on the virtual photon production theory
was implemented. Characteristic X-ray production from muonic atoms as well
as associating muon capture reaction can be also considered in the new
Adjustment parameters for determing the magnitude of angular straggling
for nspred = 2 were introduced.
Version of DCHAIN-SP included in the PHITS package was changed from DCHAIN-SP2001
A new function to combine two (or more) tally results, named “sum tally”,
was implemented. At this moment, this function works only for the results
obtained from [t-track] and [t-deposit]. (From ver. 2.82, this function became applicable to all tallies except for [t-dchain].)
The Kurotama model was revised to be capable of calculating the cross sections over 5 GeV/n.
The gamma de-excitation data contained in trxcrd.dat was incorporated in
the source files of PHITS. Consequently, file(14) parameter is not necessary
to be specified in PHITS input file even setting e-mode?1 or igamma?1.
High-energy photo-nuclear reaction can be treated up to 100 GeV by implementing
pion-production and non-resonant photonuclear reaction mechanism in JQMD
The event generator mode ver.2 was improved to precisely determine the
charged particle spectra on the basis of their cross section data such
as (n, p) and (n, α) contained in evaluated nuclear data library.
JQMD was improved to consider the relativistic effect. The algorithm for
stabilizing the initial state of nucleus was also implemented.
Detector resolution can be considered in the event-by-event deposition
energy calculation using [t-deposit] with output = deposit.
A geometry check function was implemented. This function works when you specify a tally for generating the two-dimensional view of your geometry. When double defined or undefined regions are detected, their regions are painted on the two-dimensional view.
New parameter infout was added to control output information in file(6) (D=phits.out).
Cone shape can be used for specifying the source locations by setting s-type=18,
Dumpall and dump function for [t-cross], [t-time], [t-product] tallies
can be used in the restart calculation.
We increased the total memory usage of PHITS (mdas) given in the param.inc
file, and the maximum number of lattice (latmax) in a cell.
Algorithm for including discrete spectra calculated by DWBA (Distorted
Wave Born Approximation) was implemented. In several nuclear reactions
induced by protons or deuterons, discrete peaks are added to neutron and
proton spectra obtained by nuclear reaction models.
Results in the unit of Gy can be also obtained in [t-heat] tally. We corrected a bug that NaN was detected
in the case of void regions.
OpenMP version of executable file for Windows was compiled in 64-bit compatible
mode in order to increase the allocatable memory size. Consequently, only
single version of PHITS can be executed on Windows 32-bit machine.
[ phits264 ] 2013/11/20 Minor revisions and bug fix
Bug in the connecting calculation between DCHAIN-SP and PHITS2.63 was fixed
Bugs in photo-nuclear reaction model and EBITEM were fixed
[ phits263 ] 2013/10/28 Important improvements
Algorithm for de-excitation of nucleus after the evaporation process was
improved by implementing EBITEM (ENSDF-Based Isomeric Transition and isomEr
production Model). Prompt gamma spectrum can be precisely estimated, including
discrete peaks. The isomer production rates can be properly estimated.
Quasi-deuteron disintegration, which is the dominant photo-nuclear mechanism
between 25 to 140 MeV, was implemented in JQMD. Thus, PHITS2.60 can treat
the photo-nuclear reaction up to 140 MeV. The evaporation process after
the giant resonance of 6Li, 12C, 14N, and 16O was improved by considering
the isospin of excited nucleus. Thus the alpha emission is suppressed and
neutron and proton emission is enhanced from the giant resonance of these
Particle transport simulation in the combination field of electro-magnetic
fields became available. See [Electro Magnetic Field] section in detail.
Number of cells acceptable in [t-dchain] was increased
Several algorithms were optimized to reduce the computational time, especially
for xyz mesh tally with istdev = 2.
The references of PHITS and INCL were changed
7-digit cell ID became acceptable
Maximum dmax for electron and positron was changed from 1 GeV to 10 GeV
Restart calculation became available even when PHITS did not stop properly
Lattice cell became acceptable in [t-dchain]
Avoid the termination of PHITS when some strange error occurs in JAM
New multiplier function k=-120 was added to weight the density
Minor bug fix in SMM, user defined tally, range calculation, transform, electron lost particle, random number generation for MPI, delta-ray production.
Nuclear data for some nuclei was revised by following the revision of JENDL-4.0.
Bug in reading proton data library was fixed.
[ phits252 ] 2013/03/05 Updates related to the PHITS package
Windows and Mac installers as well as instruction files for the installation
and execution of PHITS are prepared.
Two executable files of PHITS for Windows and Mac, respectively, are included in "bin" folder; one is for single computing, and the other is for memory-shared parallel computing.
Shell script and batch file for executing PHITS were developed. They are included in "bin" folder. In Windows PC, user can execute PHITS from Windows Explore using "sendto" command.
Neutron nuclear data library based on JENDL-4.0 was revised. Photo- and Electro-atomic data libraries were developed. They are included in "XS" folder.
Materials for PHITS tutorial are included in "lecture" folder.
Sample input files for various situations are included in "recommendation" folder.
The PHITS manual was revised. It is included in "manual" folder.
Instructions for using tools related PHITS were prepared. They are included in "utility" folder.
A test version of PHITS in combination with EGS5 was developed. Its executable files are included in "bin" folder.
An activation calculation program DCHAIN-SP is included in "dchain-sp" folder.
Updates related to the PHITS source code
A function to generate knocked-out electrons so-called delta-rays was implemented.
The functions "dumpall" and "dump" for [t-cross], [t-time], and [t-product] tallies became available in the MPI parallel computing.
The radiation damage model for calculating DPA (Displacement Per Atom) was improved using the screened Coulomb scattering.
A new section named [multiplier] was developed for multiplying user-defined function with the results obtained from [t-track]. Using this function, user can directly calculate the ambient dose equivalent, H*(10), using PHITS.
The procedure for calculating statistical uncertainties was revised. The function to restart the PHITS calculation based the tally results obtained by past PHITS simulations was implemented in order to increase the history number when the number is not enough.
The shared memory parallel computing using OpenMP architecture became available. For this purpose, the source code of PHITS was dramatically revised, and old Fortran compilers such as f77 and g77 cannot be used for compiling PHITS anymore.
The cross section data for photo-nuclear reaction was revised based on JENDL Photonuclear Data File 2004 (JENDL/PD-2004).
The Statistical Multi-fragmentation Model (SMM) was implemented in the statistical decay of highly-excited residual nuclei.
Intra-Nuclear Cascade of Li`ege (INCL) was implemented, and employed as the default model for simulating nuclear reactions induced by neutrons, protons, pions, deuterons, tritons, He-3 and alpha particles at intermediate energies.
KUROTAMA model, which gives reaction cross sections of nucleon-nucleus and nucleus-nucleus, was implemented.
Intra-Nuclear Cascade with Emission of Light Fragment (INC-ELF) was implemented.
A user-defined tally named [t-userdefined] was introduced in order to deduce user specific quantities from the PHITS simulation.
Electron, positron and photon transport algorithms were revised. In the new version, effective stopping powers of electrons and positions vary with their cut-off energies. The energies are conserved in an event induced by photon-atomic interactions such as the photo-electric effect.
A new tally [t-dchain] was implemented to generate input files of DCHAIN-SP, which can calculate the time dependence of activation during and after irradiations.
Macro bodies of Right Elliptical Cylinder (REC), Truncated Right-angle Cone (TRC), Ellipsoid (ELL), and Wedge (WED) are implemented.
[ phits230 ] 2011/08/11
We have added mdp-uni90.f, unix90.f for gfortran and fortran90.
We have introduced the contribution of Coulomb scattering of charged particles and heavy ions in [t-dpa].
We have introduced [Multiplier] section.
In this section we can define any functions numerically
which is used in [t-track] tally multiplied with the track length.
[ phits228 ] 2011/06/21
We have improved the dump functions used in 'dumpall',
[t-cross], [t-time], and [t-product] in order to use them in the MPI parallel calculations.
We have added an information of the angle of the crossing surface in dumpall.
We have fixed many bugs in read00.f, update.f, ....,
which are not serious.
(Thanks to Furuta of RIKEN.)
We added the contributions of cut-off energy of electron and positron in [t-deposit], which are neglected before.
By this, the heats counted in [t-heat] and [t-deposit] became the same.
The number of PE for MPI calculation is increased from 200 to 20000.
We have fixed a bug in the input echo for [source].
(Thanks to Numba of Japan Radioisotope Association.)
[ phits226 ] 2011/05/18
We have implemented the [Delta Ray] section, which controls the delta ray production from charged particle in materials.
[ phits224L ] 2010/12/28
The nuclear data library for neutron based on JENNDL-4.0 (FSXKIB-J40) has been included in the PHITS package.
[ phits224 ] 2010/01/12
We have fixed a bug which causes a infinite loop when we use the nuclear data for proton induced reaction.
(Thanks to Kosako of Shimizu Corporation.)
[ phits223 ] 2010/01/04
We have revised the photonuclear reaction in the GDR region and the angular distribution of photon production by electrons.
[ phits218 ] 2009/10/07
We have re-written the program for the parts of GG geometry and the processing the nuclear data in an original way.
This does not affect the calculation results at all.
We have fixed a bug in the output of [t-star] with r-z mesh.
(Thanks to Yosuke Iwamot of JAEA)
[ phits217 ] 2009/09/03
We have introduced the process of photonuclear reactions in the GDR region.
This function is not complete, but in test stage.
[ phits216 ] 2009/06/02
We have fixed a bug in the e-mode calculation, which causes wrong deposit energy distribution.
However, the affects of it is not serious.
The related source files are ggm05.f, read00.f and talls01.f.
(Thanks to Tatsuhiko Sato and Yosuke Iwamot of JAEA)
[ phits215 ] 2009/03/02
We have extended the function of e-mode for thermal region of low energy neutron transport with/without S(a,b).
By the previous version, the neutron spectrum was not described correctly in thermal region by e-mode.
correctly in thermal region by e-mode.
We have fixed a bug in the counter function, which leads wrong number of the counter
when we specify the partilce 'part' for collision event 'coll'.
The particle specification for 'coll' means the incident particle, not the produced particles in the collision.
So all particles produced by a collision have the same counter value.
(Thanks to Matsuzaki of Hokkaido Univ.)
[ phits214 ] 2008/02/15
We have fixed a bug which stops the program in e-mode.
(Thanks to Marlies Luszik-Bhadra of Physikalisch-Technische Bundesanstalt.)
[ phits213 ] 2006/08/16
A bug came into the code when we fixed the problem;
ATIMA was stopped when the nucleus above Z=120 comes in, at phits210.
Please recalculate if you use the code after phits210 with ATIMA.
(Thanks to Iwase of GSI.)
[ phits212 ] 2006/04/21
Negative kf-code could not be read in the input file for particle specification.
This bug is fixed.
(Thanks to Watanabe of Kyusyu Univ.)
In the event generator mode, we introduced the branching ratio between the first excited state S(1)
and the ground state S(0) in the excitation function of 7Li for 10B(n,alpha)7Li reaction as S(1)/S(0)=14.9
according to the experimental data.
(Thanks to Arita of Renesas Technology Corp.)
We have fixed a bug by which nothing is scored in [t-track] with 'multiplier' and 'part=all'.
[ phits211 ] 2006/03/29
The LET values were wrong in the LET tally with ATIMA option.
This bug did not affect the transport calculation with the ATIMA option.
We have changed and put only 'main.f, range.f' for the new source.
(Thanks to Davide Mancusi of Chalmers Univ.)
[ phits210 ] 2006/03/27
We have changed the critical distance by which two different surfaces can be distinguished in GG of MCNP-based geometry
from the default value (1.e-04cm=1um) to 1.e-08cm in order to treat small regions.
(Thanks to Arita of Renesas Technology Corp.)
We have fixed the following problems;
1) ATIMA was stopped when the nucleus above Z=120 comes in.
2) GEM was stopped when unexpected nucleus comes in.
(Thanks to Inseok Baek of MSU.)
We have fixed some bugs in talls07.f.
(Thanks to Davide Mancusi of Chalmers Univ.)