Data Types
type	laser_t

interface	lasers_t

Functions/Subroutines
class(lasers_t) function, pointer	lasers_constructor (namespace)

subroutine, public	lasers_parse_external_fields (this)

subroutine, public	lasers_generate_potentials (this, mesh, space, latt)

subroutine, public	lasers_check_symmetries (this, kpoints)

subroutine	lasers_finalize (this)

subroutine	lasers_deallocate (this)

real(real64) function, public	laser_carrier_frequency (laser)

subroutine	lasers_init_interaction_as_partner (partner, interaction)

subroutine	lasers_update_quantity (this, label)

subroutine	lasers_copy_quantities_to_interaction (partner, interaction)

integer pure elemental function, public	laser_kind (laser)

complex(real64) function, dimension(3), public	laser_polarization (laser)

logical function, public	lasers_with_nondipole_field (lasers)
	Check if a nondipole SFA correction should be computed for the given laser. More...

subroutine, public	lasers_set_nondipole_parameters (this, ndfield, nd_integration_time)
	Set parameters for nondipole SFA calculation. More...

subroutine, public	laser_get_f (laser, ff)

subroutine, public	laser_set_f (laser, ff)

subroutine, public	laser_get_phi (laser, phi)

subroutine, public	laser_set_phi (laser, phi)

subroutine, public	laser_set_empty_phi (laser)

subroutine, public	laser_set_f_value (laser, ii, xx)

subroutine, public	laser_set_frequency (laser, omega)

subroutine, public	laser_set_polarization (laser, pol)

subroutine, public	laser_to_numerical_all (laser, dt, max_iter, omegamax)
	The td functions that describe the laser field are transformed to a "numerical" representation (i.e. time grid, values at this time grid). More...

subroutine, public	laser_to_numerical (laser, dt, max_iter, omegamax)
	The td functions that describe the laser field are transformed to a "numerical" representation (i.e. time grid, values at this time grid). More...

subroutine, public	laser_write_info (lasers, namespace, dt, max_iter, iunit)

subroutine, public	laser_potential (laser, mesh, pot, time)

subroutine, public	laser_vector_potential (laser, mesh, aa, time)

subroutine, public	laser_field (laser, field, time)
	Retrieves the value of either the electric or the magnetic field. If the laser is given by a scalar potential, the field should be a function of space (the gradient of the scalar potential times the temporal dependence), but in that case the subroutine just returns the temporal function. More...

subroutine, public	lasers_nondipole_laser_field_step (this, field, time)
	Retrieves the NDSFA vector_potential correction. The nondipole field is obtained for consecutive timesteps and adds onto field at the previous timestep (for increased speed). The algorithm finds the accumulated A^M from oldtime to time, and add to the input A^M. The Nondipole field is obtained for an electron of q=-abs(e) =-1 a.u. and m = 1 a.u from f$A^{(M)} = \frac{q}{mc} \int dt \sum_i \sum_j A^{(0)}_i \cdot E^{(0)}_j \widehat{r}_j. More...

subroutine, public	laser_electric_field (laser, field, time, dt)
	Returns a vector with the electric field, no matter whether the laser is described directly as an electric field, or with a vector potential in the velocity gauge. More...

subroutine, public	load_lasers (partners, namespace)

Variables
integer, parameter, public	e_field_none = 0

integer, parameter, public	e_field_electric = 1

integer, parameter, public	e_field_magnetic = 2

integer, parameter, public	e_field_vector_potential = 3

integer, parameter, public	e_field_scalar_potential = 4

Function/Subroutine Documentation

◆ lasers_constructor()

class(lasers_t) function, pointer lasers_oct_m::lasers_constructor ( type(namespace_t), intent(in) namespace )

private

Definition at line 225 of file lasers.F90.

◆ lasers_parse_external_fields()

subroutine, public lasers_oct_m::lasers_parse_external_fields ( class(lasers_t), intent(inout) this )

Definition at line 243 of file lasers.F90.

◆ lasers_generate_potentials()

subroutine, public lasers_oct_m::lasers_generate_potentials	(	class(lasers_t), intent(inout)	this,
		class(mesh_t), intent(in)	mesh,
		class(space_t), intent(in)	space,
		type(lattice_vectors_t), intent(in)	latt
	)

Definition at line 443 of file lasers.F90.

◆ lasers_check_symmetries()

subroutine, public lasers_oct_m::lasers_check_symmetries	(	type(lasers_t), intent(in)	this,
		type(kpoints_t), intent(in)	kpoints
	)

Definition at line 555 of file lasers.F90.

◆ lasers_finalize()

subroutine lasers_oct_m::lasers_finalize ( type(lasers_t), intent(inout) this )

private

Definition at line 580 of file lasers.F90.

◆ lasers_deallocate()

subroutine lasers_oct_m::lasers_deallocate ( class(lasers_t), intent(inout) this )

private

Definition at line 591 of file lasers.F90.

◆ laser_carrier_frequency()

real(real64) function, public lasers_oct_m::laser_carrier_frequency ( type(laser_t), intent(in) laser )

Definition at line 621 of file lasers.F90.

◆ lasers_init_interaction_as_partner()

subroutine lasers_oct_m::lasers_init_interaction_as_partner	(	class(lasers_t), intent(in)	partner,
		class(interaction_surrogate_t), intent(inout)	interaction
	)

private

Definition at line 632 of file lasers.F90.

◆ lasers_update_quantity()

subroutine lasers_oct_m::lasers_update_quantity	(	class(lasers_t), intent(inout)	this,
		character(len=*), intent(in)	label
	)

private

Definition at line 650 of file lasers.F90.

◆ lasers_copy_quantities_to_interaction()

subroutine lasers_oct_m::lasers_copy_quantities_to_interaction	(	class(lasers_t), intent(inout)	partner,
		class(interaction_surrogate_t), intent(inout)	interaction
	)

private

Definition at line 692 of file lasers.F90.

◆ laser_kind()

integer pure elemental function, public lasers_oct_m::laser_kind ( type(laser_t), intent(in) laser )

Definition at line 715 of file lasers.F90.

◆ laser_polarization()

complex(real64) function, dimension(3), public lasers_oct_m::laser_polarization ( type(laser_t), intent(in) laser )

Definition at line 726 of file lasers.F90.

◆ lasers_with_nondipole_field()

logical function, public lasers_oct_m::lasers_with_nondipole_field ( type(lasers_t), intent(in) lasers )

Check if a nondipole SFA correction should be computed for the given laser.

Definition at line 739 of file lasers.F90.

◆ lasers_set_nondipole_parameters()

subroutine, public lasers_oct_m::lasers_set_nondipole_parameters	(	type(lasers_t), intent(inout)	this,
		real(real64), dimension(:), intent(in)	ndfield,
		real(real64), intent(in)	nd_integration_time
	)

Set parameters for nondipole SFA calculation.

Definition at line 752 of file lasers.F90.

◆ laser_get_f()

subroutine, public lasers_oct_m::laser_get_f	(	type(laser_t), intent(in)	laser,
		type(tdf_t), intent(inout)	ff
	)

Definition at line 767 of file lasers.F90.

◆ laser_set_f()

subroutine, public lasers_oct_m::laser_set_f	(	type(laser_t), intent(inout)	laser,
		type(tdf_t), intent(inout)	ff
	)

Definition at line 780 of file lasers.F90.

◆ laser_get_phi()

subroutine, public lasers_oct_m::laser_get_phi	(	type(laser_t), intent(in)	laser,
		type(tdf_t), intent(inout)	phi
	)

Definition at line 795 of file lasers.F90.

◆ laser_set_phi()

subroutine, public lasers_oct_m::laser_set_phi	(	type(laser_t), intent(inout)	laser,
		type(tdf_t), intent(inout)	phi
	)

Definition at line 808 of file lasers.F90.

◆ laser_set_empty_phi()

subroutine, public lasers_oct_m::laser_set_empty_phi ( type(laser_t), intent(inout) laser )

Definition at line 823 of file lasers.F90.

◆ laser_set_f_value()

subroutine, public lasers_oct_m::laser_set_f_value	(	type(laser_t), intent(inout)	laser,
		integer, intent(in)	ii,
		real(real64), intent(in)	xx
	)

Definition at line 835 of file lasers.F90.

◆ laser_set_frequency()

subroutine, public lasers_oct_m::laser_set_frequency	(	type(laser_t), intent(inout)	laser,
		real(real64), intent(in)	omega
	)

Definition at line 849 of file lasers.F90.

◆ laser_set_polarization()

subroutine, public lasers_oct_m::laser_set_polarization	(	type(laser_t), intent(inout)	laser,
		complex(real64), dimension(:), intent(in)	pol
	)

Definition at line 862 of file lasers.F90.

◆ laser_to_numerical_all()

subroutine, public lasers_oct_m::laser_to_numerical_all	(	type(laser_t), intent(inout)	laser,
		real(real64), intent(in)	dt,
		integer, intent(in)	max_iter,
		real(real64), intent(in)	omegamax
	)

The td functions that describe the laser field are transformed to a "numerical" representation (i.e. time grid, values at this time grid).

The possible phase and carrier frequency are evaluated and put together with the envelope, so that the envelope describes the full function (zero phase, zero carrier frequency).

Definition at line 883 of file lasers.F90.

◆ laser_to_numerical()

subroutine, public lasers_oct_m::laser_to_numerical	(	type(laser_t), intent(inout)	laser,
		real(real64), intent(in)	dt,
		integer, intent(in)	max_iter,
		real(real64), intent(in)	omegamax
	)

The td functions that describe the laser field are transformed to a "numerical" representation (i.e. time grid, values at this time grid).

Definition at line 914 of file lasers.F90.

◆ laser_write_info()

subroutine, public lasers_oct_m::laser_write_info	(	type(laser_t), dimension(:), intent(in)	lasers,
		type(namespace_t), intent(in)	namespace,
		real(real64), intent(in), optional	dt,
		integer, intent(in), optional	max_iter,
		integer, intent(in), optional	iunit
	)

Definition at line 930 of file lasers.F90.

◆ laser_potential()

subroutine, public lasers_oct_m::laser_potential	(	type(laser_t), intent(in)	laser,
		class(mesh_t), intent(in)	mesh,
		real(real64), dimension(:), intent(inout)	pot,
		real(real64), intent(in), optional	time
	)

Definition at line 1043 of file lasers.F90.

◆ laser_vector_potential()

subroutine, public lasers_oct_m::laser_vector_potential	(	type(laser_t), intent(in)	laser,
		type(mesh_t), intent(in)	mesh,
		real(real64), dimension(:, :), intent(inout)	aa,
		real(real64), intent(in), optional	time
	)

Definition at line 1078 of file lasers.F90.

◆ laser_field()

subroutine, public lasers_oct_m::laser_field	(	type(laser_t), intent(in)	laser,
		real(real64), dimension(:), intent(inout)	field,
		real(real64), intent(in), optional	time
	)

Retrieves the value of either the electric or the magnetic field. If the laser is given by a scalar potential, the field should be a function of space (the gradient of the scalar potential times the temporal dependence), but in that case the subroutine just returns the temporal function.

Definition at line 1115 of file lasers.F90.

◆ lasers_nondipole_laser_field_step()

subroutine, public lasers_oct_m::lasers_nondipole_laser_field_step	(	type(lasers_t), intent(in)	this,
		real(real64), dimension(:), intent(out)	field,
		real(real64), intent(in)	time
	)

Retrieves the NDSFA vector_potential correction. The nondipole field is obtained for consecutive timesteps and adds onto field at the previous timestep (for increased speed). The algorithm finds the accumulated A^M from oldtime to time, and add to the input A^M. The Nondipole field is obtained for an electron of q=-abs(e) =-1 a.u. and m = 1 a.u from f$A^{(M)} = \frac{q}{mc} \int dt \sum_i \sum_j A^{(0)}_i \cdot E^{(0)}_j \widehat{r}_j.

Definition at line 1150 of file lasers.F90.

◆ laser_electric_field()

subroutine, public lasers_oct_m::laser_electric_field	(	type(laser_t), intent(in)	laser,
		real(real64), dimension(:), intent(out)	field,
		real(real64), intent(in)	time,
		real(real64), intent(in)	dt
	)

Returns a vector with the electric field, no matter whether the laser is described directly as an electric field, or with a vector potential in the velocity gauge.

Definition at line 1191 of file lasers.F90.

◆ load_lasers()

subroutine, public lasers_oct_m::load_lasers	(	class(partner_list_t), intent(inout)	partners,
		type(namespace_t), intent(in)	namespace
	)

Definition at line 1228 of file lasers.F90.

Variable Documentation

◆ e_field_none

integer, parameter, public lasers_oct_m::e_field_none = 0

Definition at line 177 of file lasers.F90.

◆ e_field_electric

integer, parameter, public lasers_oct_m::e_field_electric = 1

Definition at line 177 of file lasers.F90.

◆ e_field_magnetic

integer, parameter, public lasers_oct_m::e_field_magnetic = 2

Definition at line 177 of file lasers.F90.

◆ e_field_vector_potential

integer, parameter, public lasers_oct_m::e_field_vector_potential = 3

Definition at line 177 of file lasers.F90.

◆ e_field_scalar_potential

integer, parameter, public lasers_oct_m::e_field_scalar_potential = 4

Definition at line 177 of file lasers.F90.

Data Types

Functions/Subroutines

Variables

Function/Subroutine Documentation

◆ lasers_constructor()

◆ lasers_parse_external_fields()

◆ lasers_generate_potentials()

◆ lasers_check_symmetries()

◆ lasers_finalize()

◆ lasers_deallocate()

◆ laser_carrier_frequency()

◆ lasers_init_interaction_as_partner()

◆ lasers_update_quantity()

◆ lasers_copy_quantities_to_interaction()

◆ laser_kind()

◆ laser_polarization()

◆ lasers_with_nondipole_field()

◆ lasers_set_nondipole_parameters()

◆ laser_get_f()

◆ laser_set_f()

◆ laser_get_phi()

◆ laser_set_phi()

◆ laser_set_empty_phi()

◆ laser_set_f_value()

◆ laser_set_frequency()

◆ laser_set_polarization()

◆ laser_to_numerical_all()

◆ laser_to_numerical()

◆ laser_write_info()

◆ laser_potential()

◆ laser_vector_potential()

◆ laser_field()

◆ lasers_nondipole_laser_field_step()

◆ laser_electric_field()

◆ load_lasers()

Variable Documentation

◆ e_field_none

◆ e_field_electric

◆ e_field_magnetic

◆ e_field_vector_potential

◆ e_field_scalar_potential