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domain_photo_rate.f90
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domain_photo_rate.f90
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module pyramid_photo_rate
use precision, only: dp
use input, only: level_py, partition, number_density, xHI, pi, volume_factor
use array, only: pyramid_grid, &
px_py_pz_dx, px_py_pz_dy, px_py_pz_dz, &
px_py_nz_dx, px_py_nz_dy, px_py_nz_dz, &
px_ny_pz_dx, px_ny_pz_dy, px_ny_pz_dz, &
px_ny_nz_dx, px_ny_nz_dy, px_ny_nz_dz, &
nx_py_pz_dx, nx_py_pz_dy, nx_py_pz_dz, &
nx_py_nz_dx, nx_py_nz_dy, nx_py_nz_dz, &
nx_ny_pz_dx, nx_ny_pz_dy, nx_ny_pz_dz, &
nx_ny_nz_dx, nx_ny_nz_dy, nx_ny_nz_dz
use radiation, only: photoion_solid_angle, photrates
contains
subroutine pyramid_HI_photo_rate_calculation()
call px_py_pz_dx_HI_photo_rate_calculation ()
call px_py_pz_dy_HI_photo_rate_calculation ()
call px_py_pz_dz_HI_photo_rate_calculation ()
call px_py_nz_dx_HI_photo_rate_calculation ()
call px_py_nz_dy_HI_photo_rate_calculation ()
call px_py_nz_dz_HI_photo_rate_calculation ()
call px_ny_pz_dx_HI_photo_rate_calculation ()
call px_ny_pz_dy_HI_photo_rate_calculation ()
call px_ny_pz_dz_HI_photo_rate_calculation ()
call px_ny_nz_dx_HI_photo_rate_calculation ()
call px_ny_nz_dy_HI_photo_rate_calculation ()
call px_ny_nz_dz_HI_photo_rate_calculation ()
call nx_py_pz_dx_HI_photo_rate_calculation ()
call nx_py_pz_dy_HI_photo_rate_calculation ()
call nx_py_pz_dz_HI_photo_rate_calculation ()
call nx_py_nz_dx_HI_photo_rate_calculation ()
call nx_py_nz_dy_HI_photo_rate_calculation ()
call nx_py_nz_dz_HI_photo_rate_calculation ()
call nx_ny_pz_dx_HI_photo_rate_calculation ()
call nx_ny_pz_dy_HI_photo_rate_calculation ()
call nx_ny_pz_dz_HI_photo_rate_calculation ()
call nx_ny_nz_dx_HI_photo_rate_calculation ()
call nx_ny_nz_dy_HI_photo_rate_calculation ()
call nx_ny_nz_dz_HI_photo_rate_calculation ()
end subroutine pyramid_HI_photo_rate_calculation
subroutine px_py_pz_dx_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
!volume錯撚哂 volume計岩之餘仲要用solid angle去tune番個luminosity
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_py_pz_dx(1)%HI_column_density_out(1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_pz_dx(1)%HI_photoionization_rate(1,1) = phi%photo_cell
px_py_pz_dx(1)%HI_heating_rate(1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_py_pz_dx(i_level_py-1)%HI_column_density_out(i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_py_pz_dx(i_level_py-1)%HI_column_density_out(o_primary,o_secondary)
endif
HI_column_density_out = px_py_pz_dx(i_level_py)%HI_column_density_out(i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_pz_dx(i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell
px_py_pz_dx(i_level_py)%HI_heating_rate(i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_py_pz_dx_HI_photo_rate_calculation
subroutine px_py_pz_dy_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_py_pz_dy(1)%HI_column_density_out(1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_pz_dy(1)%HI_photoionization_rate(1,1) = phi%photo_cell
px_py_pz_dy(1)%HI_heating_rate(1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_py_pz_dy(i_level_py-1)%HI_column_density_out(i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_py_pz_dy(i_level_py-1)%HI_column_density_out(o_primary,o_secondary)
endif
HI_column_density_out = px_py_pz_dy(i_level_py)%HI_column_density_out(i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_pz_dy(i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell
px_py_pz_dy(i_level_py)%HI_heating_rate(i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_py_pz_dy_HI_photo_rate_calculation
subroutine px_py_pz_dz_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_py_pz_dz(1)%HI_column_density_out(1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_pz_dz(1)%HI_photoionization_rate(1,1) = phi%photo_cell
px_py_pz_dz(1)%HI_heating_rate(1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_py_pz_dz(i_level_py-1)%HI_column_density_out(i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_py_pz_dz(i_level_py-1)%HI_column_density_out(o_primary,o_secondary)
endif
HI_column_density_out = px_py_pz_dz(i_level_py)%HI_column_density_out(i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_pz_dz(i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell
px_py_pz_dz(i_level_py)%HI_heating_rate(i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_py_pz_dz_HI_photo_rate_calculation
subroutine px_py_nz_dx_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_py_nz_dx(1)%HI_column_density_out(1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_nz_dx(1)%HI_photoionization_rate(1,-1) = phi%photo_cell
px_py_nz_dx(1)%HI_heating_rate(1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_py_nz_dx(i_level_py-1)%HI_column_density_out(i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_py_nz_dx(i_level_py-1)%HI_column_density_out(o_primary,-o_secondary)
endif
HI_column_density_out = px_py_nz_dx(i_level_py)%HI_column_density_out(i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_nz_dx(i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell
px_py_nz_dx(i_level_py)%HI_heating_rate(i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_py_nz_dx_HI_photo_rate_calculation
subroutine px_py_nz_dy_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_py_nz_dy(1)%HI_column_density_out(-1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_nz_dy(1)%HI_photoionization_rate(-1,1) = phi%photo_cell
px_py_nz_dy(1)%HI_heating_rate(-1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_py_nz_dy(i_level_py-1)%HI_column_density_out(-i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_py_nz_dy(i_level_py-1)%HI_column_density_out(-o_primary,o_secondary)
endif
HI_column_density_out = px_py_nz_dy(i_level_py)%HI_column_density_out(-i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_nz_dy(i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell
px_py_nz_dy(i_level_py)%HI_heating_rate(-i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_py_nz_dy_HI_photo_rate_calculation
subroutine px_py_nz_dz_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_py_nz_dz(-1)%HI_column_density_out(1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_nz_dz(-1)%HI_photoionization_rate(1,1) = phi%photo_cell
px_py_nz_dz(-1)%HI_heating_rate(1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_py_nz_dz(-i_level_py+1)%HI_column_density_out(i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_py_nz_dz(-i_level_py+1)%HI_column_density_out(o_primary,o_secondary)
endif
HI_column_density_out = px_py_nz_dz(-i_level_py)%HI_column_density_out(i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_py_nz_dz(-i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell
px_py_nz_dz(-i_level_py)%HI_heating_rate(i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_py_nz_dz_HI_photo_rate_calculation
subroutine px_ny_pz_dx_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_ny_pz_dx(1)%HI_column_density_out(-1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_pz_dx(1)%HI_photoionization_rate(-1,1) = phi%photo_cell
px_ny_pz_dx(1)%HI_heating_rate(-1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_ny_pz_dx(i_level_py-1)%HI_column_density_out(-i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_ny_pz_dx(i_level_py-1)%HI_column_density_out(-o_primary,o_secondary)
endif
HI_column_density_out = px_ny_pz_dx(i_level_py)%HI_column_density_out(-i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_pz_dx(i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell
px_ny_pz_dx(i_level_py)%HI_heating_rate(-i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_ny_pz_dx_HI_photo_rate_calculation
subroutine px_ny_pz_dy_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_ny_pz_dy(-1)%HI_column_density_out(1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_pz_dy(-1)%HI_photoionization_rate(1,1) = phi%photo_cell
px_ny_pz_dy(-1)%HI_heating_rate(1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_ny_pz_dy(-i_level_py+1)%HI_column_density_out(i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_ny_pz_dy(-i_level_py+1)%HI_column_density_out(o_primary,o_secondary)
endif
HI_column_density_out = px_ny_pz_dy(-i_level_py)%HI_column_density_out(i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_pz_dy(-i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell
px_ny_pz_dy(-i_level_py)%HI_heating_rate(i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_ny_pz_dy_HI_photo_rate_calculation
subroutine px_ny_pz_dz_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_ny_pz_dz(1)%HI_column_density_out(1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_pz_dz(1)%HI_photoionization_rate(1,-1) = phi%photo_cell
px_ny_pz_dz(1)%HI_heating_rate(1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_ny_pz_dz(i_level_py-1)%HI_column_density_out(i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_ny_pz_dz(i_level_py-1)%HI_column_density_out(o_primary,-o_secondary)
endif
HI_column_density_out = px_ny_pz_dz(i_level_py)%HI_column_density_out(i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_pz_dz(i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell
px_ny_pz_dz(i_level_py)%HI_heating_rate(i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_ny_pz_dz_HI_photo_rate_calculation
subroutine px_ny_nz_dx_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_ny_nz_dx(1)%HI_column_density_out(-1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_nz_dx(1)%HI_photoionization_rate(-1,-1) = phi%photo_cell
px_ny_nz_dx(1)%HI_heating_rate(-1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_ny_nz_dx(i_level_py-1)%HI_column_density_out(-i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_ny_nz_dx(i_level_py-1)%HI_column_density_out(-o_primary,-o_secondary)
endif
HI_column_density_out = px_ny_nz_dx(i_level_py)%HI_column_density_out(-i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_nz_dx(i_level_py)%HI_photoionization_rate(-i_primary,-i_secondary) = phi%photo_cell
px_ny_nz_dx(i_level_py)%HI_heating_rate(-i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_ny_nz_dx_HI_photo_rate_calculation
subroutine px_ny_nz_dy_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_ny_nz_dy(-1)%HI_column_density_out(-1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_nz_dy(-1)%HI_photoionization_rate(-1,1) = phi%photo_cell
px_ny_nz_dy(-1)%HI_heating_rate(-1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_ny_nz_dy(-i_level_py+1)%HI_column_density_out(-i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_ny_nz_dy(-i_level_py+1)%HI_column_density_out(-o_primary,o_secondary)
endif
HI_column_density_out = px_ny_nz_dy(-i_level_py)%HI_column_density_out(-i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_nz_dy(-i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell
px_ny_nz_dy(-i_level_py)%HI_heating_rate(-i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_ny_nz_dy_HI_photo_rate_calculation
subroutine px_ny_nz_dz_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = px_ny_nz_dz(-1)%HI_column_density_out(1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_nz_dz(-1)%HI_photoionization_rate(1,-1) = phi%photo_cell
px_ny_nz_dz(-1)%HI_heating_rate(1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = px_ny_nz_dz(-i_level_py+1)%HI_column_density_out(i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = px_ny_nz_dz(-i_level_py+1)%HI_column_density_out(o_primary,-o_secondary)
endif
HI_column_density_out = px_ny_nz_dz(-i_level_py)%HI_column_density_out(i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
px_ny_nz_dz(-i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell
px_ny_nz_dz(-i_level_py)%HI_heating_rate(i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine px_ny_nz_dz_HI_photo_rate_calculation
subroutine nx_py_pz_dx_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_py_pz_dx(-1)%HI_column_density_out(1,1)
!write(*,*)HI_column_density_out ! it is zero!!!!
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_pz_dx(-1)%HI_photoionization_rate(1,1) = phi%photo_cell
nx_py_pz_dx(-1)%HI_heating_rate(1,1) = phi%heat_cell
!write(*,*)nx_py_pz_dx(-1)%HI_photoionization_rate(1,1)
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_py_pz_dx(-i_level_py+1)%HI_column_density_out(i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_py_pz_dx(-i_level_py+1)%HI_column_density_out(o_primary,o_secondary)
endif
HI_column_density_out = nx_py_pz_dx(-i_level_py)%HI_column_density_out(i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_pz_dx(-i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell
nx_py_pz_dx(-i_level_py)%HI_heating_rate(i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_py_pz_dx_HI_photo_rate_calculation
subroutine nx_py_pz_dy_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_py_pz_dy(1)%HI_column_density_out(1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_pz_dy(1)%HI_photoionization_rate(1,-1) = phi%photo_cell
nx_py_pz_dy(1)%HI_heating_rate(1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_py_pz_dy(i_level_py-1)%HI_column_density_out(i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_py_pz_dy(i_level_py-1)%HI_column_density_out(o_primary,-o_secondary)
endif
HI_column_density_out = nx_py_pz_dy(i_level_py)%HI_column_density_out(i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_pz_dy(i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell
nx_py_pz_dy(i_level_py)%HI_heating_rate(i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_py_pz_dy_HI_photo_rate_calculation
subroutine nx_py_pz_dz_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_py_pz_dz(1)%HI_column_density_out(-1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_pz_dz(1)%HI_photoionization_rate(-1,1) = phi%photo_cell
nx_py_pz_dz(1)%HI_heating_rate(-1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_py_pz_dz(i_level_py-1)%HI_column_density_out(-i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_py_pz_dz(i_level_py-1)%HI_column_density_out(-o_primary,o_secondary)
endif
HI_column_density_out = nx_py_pz_dz(i_level_py)%HI_column_density_out(-i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_pz_dz(i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell
nx_py_pz_dz(i_level_py)%HI_heating_rate(-i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_py_pz_dz_HI_photo_rate_calculation
subroutine nx_py_nz_dx_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_py_nz_dx(-1)%HI_column_density_out(1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_nz_dx(-1)%HI_photoionization_rate(1,-1) = phi%photo_cell
nx_py_nz_dx(-1)%HI_heating_rate(1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_py_nz_dx(-i_level_py+1)%HI_column_density_out(i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_py_nz_dx(-i_level_py+1)%HI_column_density_out(o_primary,-o_secondary)
endif
HI_column_density_out = nx_py_nz_dx(-i_level_py)%HI_column_density_out(i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_nz_dx(-i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell
nx_py_nz_dx(-i_level_py)%HI_heating_rate(i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_py_nz_dx_HI_photo_rate_calculation
subroutine nx_py_nz_dy_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_py_nz_dy(1)%HI_column_density_out(-1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_nz_dy(1)%HI_photoionization_rate(-1,-1) = phi%photo_cell
nx_py_nz_dy(1)%HI_heating_rate(-1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_py_nz_dy(i_level_py-1)%HI_column_density_out(-i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_py_nz_dy(i_level_py-1)%HI_column_density_out(-o_primary,-o_secondary)
endif
HI_column_density_out = nx_py_nz_dy(i_level_py)%HI_column_density_out(-i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_nz_dy(i_level_py)%HI_photoionization_rate(-i_primary,-i_secondary) = phi%photo_cell
nx_py_nz_dy(i_level_py)%HI_heating_rate(-i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_py_nz_dy_HI_photo_rate_calculation
subroutine nx_py_nz_dz_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_py_nz_dz(-1)%HI_column_density_out(-1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_nz_dz(-1)%HI_photoionization_rate(-1,1) = phi%photo_cell
nx_py_nz_dz(-1)%HI_heating_rate(-1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_py_nz_dz(-i_level_py+1)%HI_column_density_out(-i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_py_nz_dz(-i_level_py+1)%HI_column_density_out(-o_primary,o_secondary)
endif
HI_column_density_out = nx_py_nz_dz(-i_level_py)%HI_column_density_out(-i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_py_nz_dz(-i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell
nx_py_nz_dz(-i_level_py)%HI_heating_rate(-i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_py_nz_dz_HI_photo_rate_calculation
subroutine nx_ny_pz_dx_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_ny_pz_dx(-1)%HI_column_density_out(-1,1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_ny_pz_dx(-1)%HI_photoionization_rate(-1,1) = phi%photo_cell
nx_ny_pz_dx(-1)%HI_heating_rate(-1,1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_ny_pz_dx(-i_level_py+1)%HI_column_density_out(-i_primary,i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_ny_pz_dx(-i_level_py+1)%HI_column_density_out(-o_primary,o_secondary)
endif
HI_column_density_out = nx_ny_pz_dx(-i_level_py)%HI_column_density_out(-i_primary,i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_ny_pz_dx(-i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell
nx_ny_pz_dx(-i_level_py)%HI_heating_rate(-i_primary,i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_ny_pz_dx_HI_photo_rate_calculation
subroutine nx_ny_pz_dy_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_ny_pz_dy(-1)%HI_column_density_out(1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_ny_pz_dy(-1)%HI_photoionization_rate(1,-1) = phi%photo_cell
nx_ny_pz_dy(-1)%HI_heating_rate(1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_ny_pz_dy(-i_level_py+1)%HI_column_density_out(i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_ny_pz_dy(-i_level_py+1)%HI_column_density_out(o_primary,-o_secondary)
endif
HI_column_density_out = nx_ny_pz_dy(-i_level_py)%HI_column_density_out(i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_ny_pz_dy(-i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell
nx_ny_pz_dy(-i_level_py)%HI_heating_rate(i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_ny_pz_dy_HI_photo_rate_calculation
subroutine nx_ny_pz_dz_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_ny_pz_dz(1)%HI_column_density_out(-1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_ny_pz_dz(1)%HI_photoionization_rate(-1,-1) = phi%photo_cell
nx_ny_pz_dz(1)%HI_heating_rate(-1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_ny_pz_dz(i_level_py-1)%HI_column_density_out(-i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_ny_pz_dz(i_level_py-1)%HI_column_density_out(-o_primary,-o_secondary)
endif
HI_column_density_out = nx_ny_pz_dz(i_level_py)%HI_column_density_out(-i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_ny_pz_dz(i_level_py)%HI_photoionization_rate(-i_primary,-i_secondary) = phi%photo_cell
nx_ny_pz_dz(i_level_py)%HI_heating_rate(-i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_ny_pz_dz_HI_photo_rate_calculation
subroutine nx_ny_nz_dx_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
type(photrates) :: phi
! i_level_py = 1
solid_angle = pyramid_grid(1)%solid_angle(1,1)
HI_column_density_in = 0
HI_column_density_out = nx_ny_nz_dx(-1)%HI_column_density_out(-1,-1)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_ny_nz_dx(-1)%HI_photoionization_rate(-1,-1) = phi%photo_cell
nx_ny_nz_dx(-1)%HI_heating_rate(-1,-1) = phi%heat_cell
! i_level_py > 1
do i_level_py = 2,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
if (partition(i_level_py).eq.partition(i_level_py-1)) then
HI_column_density_in = nx_ny_nz_dx(-i_level_py+1)%HI_column_density_out(-i_primary,-i_secondary)
else
o_primary = (i_primary+1)/2
o_secondary = (i_secondary+1)/2
HI_column_density_in = nx_ny_nz_dx(-i_level_py+1)%HI_column_density_out(-o_primary,-o_secondary)
endif
HI_column_density_out = nx_ny_nz_dx(-i_level_py)%HI_column_density_out(-i_primary,-i_secondary)
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,solid_angle)
nx_ny_nz_dx(-i_level_py)%HI_photoionization_rate(-i_primary,-i_secondary) = phi%photo_cell
nx_ny_nz_dx(-i_level_py)%HI_heating_rate(-i_primary,-i_secondary) = phi%heat_cell
enddo
enddo
enddo
end subroutine nx_ny_nz_dx_HI_photo_rate_calculation
subroutine nx_ny_nz_dy_HI_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle