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| class(lasers_t) function, pointer | lasers_oct_m::lasers_constructor (namespace) |
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| subroutine, public | lasers_oct_m::lasers_parse_external_fields (this) |
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| subroutine, public | lasers_oct_m::lasers_generate_potentials (this, mesh, space, latt) |
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| subroutine, public | lasers_oct_m::lasers_check_symmetries (this, kpoints) |
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| subroutine | lasers_oct_m::lasers_finalize (this) |
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| subroutine | lasers_oct_m::lasers_deallocate (this) |
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| real(real64) function, public | lasers_oct_m::laser_carrier_frequency (laser) |
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| subroutine | lasers_oct_m::lasers_init_interaction_as_partner (partner, interaction) |
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| subroutine | lasers_oct_m::lasers_update_quantity (this, iq) |
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| subroutine | lasers_oct_m::lasers_copy_quantities_to_interaction (partner, interaction) |
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| integer pure elemental function, public | lasers_oct_m::laser_kind (laser) |
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| complex(real64) function, dimension(3), public | lasers_oct_m::laser_polarization (laser) |
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| logical function, public | lasers_oct_m::lasers_with_nondipole_field (lasers) |
| | Check if a nondipole SFA correction should be computed for the given laser. More...
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| subroutine, public | lasers_oct_m::lasers_set_nondipole_parameters (this, ndfield, nd_integration_time) |
| | Set parameters for nondipole SFA calculation. More...
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| subroutine, public | lasers_oct_m::laser_get_f (laser, ff) |
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| subroutine, public | lasers_oct_m::laser_set_f (laser, ff) |
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| subroutine, public | lasers_oct_m::laser_get_phi (laser, phi) |
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| subroutine, public | lasers_oct_m::laser_set_phi (laser, phi) |
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| subroutine, public | lasers_oct_m::laser_set_empty_phi (laser) |
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| subroutine, public | lasers_oct_m::laser_set_f_value (laser, ii, xx) |
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| subroutine, public | lasers_oct_m::laser_set_frequency (laser, omega) |
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| subroutine, public | lasers_oct_m::laser_set_polarization (laser, pol) |
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| subroutine, public | lasers_oct_m::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...
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| subroutine, public | lasers_oct_m::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...
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| subroutine, public | lasers_oct_m::laser_write_info (lasers, namespace, dt, max_iter, iunit) |
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| subroutine, public | lasers_oct_m::laser_potential (laser, mesh, pot, time) |
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| subroutine, public | lasers_oct_m::laser_vector_potential (laser, mesh, aa, time) |
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| subroutine, public | lasers_oct_m::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...
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| subroutine, public | lasers_oct_m::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...
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| subroutine, public | lasers_oct_m::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...
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| subroutine, public | lasers_oct_m::load_lasers (partners, namespace) |
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1.9.4