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 227 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 245 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 444 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 556 of file lasers.F90.

◆ lasers_finalize()

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

private

Definition at line 581 of file lasers.F90.

◆ lasers_deallocate()

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

private

Definition at line 592 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 622 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 633 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 651 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 695 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 718 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 729 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 742 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 755 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 772 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 785 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 800 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 813 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 828 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 840 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 854 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 867 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 888 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 919 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 935 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 1048 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 1083 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 1120 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 1155 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 1196 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 1233 of file lasers.F90.

Variable Documentation

◆ e_field_none

integer, parameter, public lasers_oct_m::e_field_none = 0

Definition at line 179 of file lasers.F90.

◆ e_field_electric

integer, parameter, public lasers_oct_m::e_field_electric = 1

Definition at line 179 of file lasers.F90.

◆ e_field_magnetic

integer, parameter, public lasers_oct_m::e_field_magnetic = 2

Definition at line 179 of file lasers.F90.

◆ e_field_vector_potential

integer, parameter, public lasers_oct_m::e_field_vector_potential = 3

Definition at line 179 of file lasers.F90.

◆ e_field_scalar_potential

integer, parameter, public lasers_oct_m::e_field_scalar_potential = 4

Definition at line 179 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