Procedure | Location | Procedure Type | Description |
---|---|---|---|
alps_error | alps_io | Subroutine | Error catching subroutine. |
alps_error_init | alps_io | Subroutine | Open a file for the error log. |
besselI | alps_nhds | Function | Calculates the modified Bessel function of argument x and order n. |
BESSI | alps_nhds | Function | Function to calculate the first kind modified Bessel function of integer order N for any real X. |
BESSI0 | ../../generate_distribution.f90 | Function | This function calculates the modified Bessel function of the first kind of order zero for any positive real argument x. |
BESSI0 | alps_nhds | Function | Auxiliary Bessel functions for N=0, N=1 |
BESSI1 | ../../generate_distribution.f90 | Function | This function calculates the modified Bessel function of the first kind of order one for any positive real argument x. |
BESSI1 | alps_nhds | Function | Modified Bessel function of order 1. |
BESSJ | alps_fns_rel | Function | This function calculates the first kind Bessel function of integer order N, for any REAL X. We use here the classical recursion formula, when X > N. For X < N, Miller's algorithm is used to avoid overflows. Reference: C.W.Clenshaw, Chebyshev Series for Mathematical Functions, Mathematical Tables, Vol. 5, 1962. |
BESSJ0 | alps_fns_rel | Function | This function calculates the first kind Bessel function of order 0, for any REAL X. The polynomial approximation by series of Chebyshev polynomials is used for 0<X<8 and 0<8/X<1. References: M.Abramowitz, I.A.Stegun, Handbook of Mathematical Functions, 1965. C.W.Clenshaw, Chebyshev Series for Mathematical Functions, Mathematical Tables, Vol. 5, 1962. |
BESSJ1 | alps_fns_rel | Function | This subroutine calculates the First Kind Bessel Function of order 1, for any real number X. The polynomial approximation by series of Chebyshev polynomials is used for 0<X<8 and 0<8/X<1. References: M.Abramowitz, I.A.Stegun, Handbook of Mathematical Functions, 1965. C.W.Clenshaw, Chebyshev Series for Mathematical Functions, Mathematical Tables, Vol. 5, 1962. |
BESSK | ../../generate_distribution.f90 | Function | This function calculates the modified Bessel function of the third kind of integer order N, for any REAL X. The classical recursion formula is used. Reference: C.W.Clenshaw, Chebyshev Series for Mathematical Functions, Mathematical Tables, Vol. 5, 1962. |
BESSK0 | ../../generate_distribution.f90 | Function | This function calculates the modified Bessel function of the third kind of order zero for any positive real argument x. |
BESSK1 | ../../generate_distribution.f90 | Function | This function calculates the modified Bessel function of the third kind of order zero for any positive real argument x. |
bM_read | alps_io | Subroutine | Reads in bi-Maxwellian/cold-plasma parameters. |
calc_chi | alps_nhds | Subroutine | Subroutine that calculates the susceptibility of species j based on NHDS. |
calc_chi_cold | alps_nhds | Subroutine | Subroutine that calculates the susceptibility of species j based on the cold-plasma dispersion relation based on the paper Verscharen & Chandran, ApJ 764, 88, 2013. |
calc_eigen | alps_fns | Subroutine | This subroutine calculates the relative electric and magnetic field amplitudes, the relative fluctuations in the density and velocity of all species, and the heating rates of the given solution. It is based on the calc_eigen routine by Greg Howes and Kris Klein. |
calc_ypsilon | alps_nhds | Subroutine | Calculates the Y-tensor according to Stix for a bi-Maxwelling, using the NHDS calculation. |
CBESSJ | alps_fns_rel | Subroutine | This subroutine calculates the complex Bessel function. It is based on the CBESSJ function release 1.1 by J-P Moreau, Paris (www.jpmoreau.fr). |
derivative_f0 | alps_fns | Subroutine | This subroutine calculates the perpendicular and parallel derivatives of the background velocity distribution function f0. |
derivative_f0_rel | alps_fns_rel | Subroutine | This subroutine calculates the derivatives of the background velocity distribution function f0 for the relativistic calculation. |
determine_bessel_array | alps_fns | Subroutine | This subroutine determines the array of Bessel functions that is used in the T-tensor of Eq. (2.10) of the code paper. |
determine_GLLS | alps_analyt | Subroutine | This subroutine evaluates the General Linear Least Squares fit to the distribution function for component 'is' using the selected polynomial basis functions. |
determine_JT | alps_analyt | Subroutine | This subroutine calculates the transposed Jacobian matrix of the fit function with respect to the fit parameter array. |
determine_nmax | alps_fns | Subroutine | This subroutine determines the maximum required order of the Bessel functions in Eq. (2.9) of the code paper. |
determine_param_fit | alps_analyt | Subroutine | This is the fitting routine for the hybrid analytic continuation. It determines the full field param_fit. |
determine_resonances | alps_fns | Subroutine | This subroutine determines whether any kinetic resonances are located in the integration domain. |
determine_sproc_rel | alps_fns_rel | Subroutine | This subroutine determines sproc_rel for the given process. |
disp | alps_fns | Function | This function returns the determinant of the dispersion tensor for a given frequency om. |
dispfunct | alps_nhds | Function | Calculates the dispersion function based on the complex error function. |
display_credits | alps_io | Subroutine | Writes the opening credits. |
distribution_analyt | alps_distribution_analyt | Function | This function returns the pre-defined function as f0. |
eval_fit | alps_analyt | Function | This function evaluates the fit to f0 at and the complex parallel momentum ppar_valC. It requires the fit parameters that will be determined by the subroutine determine_param_fit. |
Fact | alps_fns_rel | Function | This function returns the factorial k! of its argument k. |
factorial | alps_analyt | Function | |
find_minima | alps_fns | Subroutine | This subroutine identifies the minima of the coarse map grid. It is called by map_search. The code is based on a routine by Greg Howes, 2006. |
fit_function | alps_analyt | Function | This function evaluates the fit to f0 at real pperp_val and complex ppar_val, provided that the one-dimensional fit-parameter array params is fed into the function. This is only used during the fitting. For the evaluation in ALPS, use eval_fit. |
fit_function_poly | alps_analyt | Function | This function evaluates the orthogonal polynomical fit to f0 at real pperp_val and complex ppar_val, with the one-dimensional polynomical coefficient array fit_coeffs is fed into the function. For the evaluation in ALPS, use eval_fit. kgk: should this be .gt. or .ge. ? |
fit_read | alps_io | Subroutine | Reads in fit parameters for component is. |
full_integrate | alps_fns | Function | This function returns the full integral expression according to Eq. (2.9) in the code paper. |
funct_g | alps_fns | Function | This function returns the function from Eq. (3.2) of the code paper. |
funct_g_rel | alps_fns_rel | Function | This function returns the function from Eq. (3.2) of the code paper for a relativistic calculation. |
Gamma | alps_fns_rel | Function | This function returns the Gamma-function. |
get_indexed_double_namelist_unit | alps_io | Subroutine | A version of get_indexed_namelist_unit, extended to allow for double indexing in order to read in multiple fits for a single species. |
get_indexed_namelist_unit | generate_distribution | Subroutine | Determines unused I/O unit. |
get_indexed_namelist_unit | alps_io | Subroutine | Determines unused I/O unit. |
get_runname | generate_distribution | Subroutine | Get runname for output files from input argument. |
get_runname | alps_io | Subroutine | Get runname for output files from input argument. |
get_runname | interpolate | Subroutine | Get runname for output files from input argument. |
get_unused_unit | generate_distribution | Subroutine | Determine unused number for I/O index. |
get_unused_unit | alps_io | Subroutine | Determine unused number for I/O index. |
get_unused_unit | interpolate | Subroutine | This subroutine returns an available unit number. It is taken from the AstroGK code. |
init_param | alps_io | Subroutine | Read in system parameters from *.in file. Only processor 0 calls this routine: |
input_unit | generate_distribution | Function | Assigns input unit for namelist opening. |
input_unit | alps_io | Function | Assigns input unit for namelist opening. |
input_unit | interpolate | Function | This function returns a unit number for a namelist. It is taken from the AstroGK code. |
input_unit_exist | generate_distribution | Function | Determine if a particular namelist already opened. |
input_unit_exist | alps_io | Function | Determine if a particular namelist already opened. |
input_unit_exist | interpolate | Function | This function checks whether a unit number exists. It is taken from the AstroGK code. |
int_ee | alps_fns | Function | This function returns the ee term in Eq. (2.9). |
int_ee_rel | alps_fns_rel | Function | This function returns the ee term in Eq. (2.9) for the relativistic calculation. |
int_T | alps_fns | Function | This function returns the T-tensor according to Eq. (2.10) of the code paper. |
int_T_rel | alps_fns_rel | Function | This function returns the T-tensor according to Eq. (2.10) of the code paper for the relativistic calculation. |
int_T_res | alps_fns | Function | This function returns the T-tensor according to Eq. (2.10) of the code paper for the case in which it is evaluated at the complex resonance momentum. |
int_T_res_rel | alps_fns_rel | Function | This function returns the T-tensor according to Eq. (2.10) of the code paper for the case in which it is evaluated at the complex resonance momentum for the relativistic calculation. |
integrate | alps_fns | Function | This function performs the integral in Eq. (2.9) of the code paper, but without accounting for the Landau contour integral. It is called by full_integrate. |
integrate_res | alps_fns | Function | This function performs the integration near resonances as described in Section 3.1 of the code paper. It is only called if resonances are present in or near the integration domain. |
integrate_res_rel | alps_fns_rel | Function | This function performs the integration near resonances as described in Section 3.1 of the code paper for a relativistic calculation. It is only called if resonances are present in or near the integration domain. |
integrate_resU_rel | alps_fns_rel | Function | This function evaluates the integral with the integrand proportional to in Eq. (2.9) of the code paper for a relativistic calculation. |
isnancheck | alps_io | Function | Checks if double precision number input is NaN. |
landau_integrate | alps_fns | Function | This function evaluates the Landau contour according to Eqs. (3.8) and (3.9) of the code paper. |
landau_integrate_rel | alps_fns_rel | Function | This function evaluates the Landau contour according to Eqs. (3.8) and (3.9) of the code paper for a relativistic calculation. |
least_squares_fit | alps_analyt | Subroutine | Solves General Linear Least Squares Normal Equation |
LM_nonlinear_fit | alps_analyt | Subroutine | This subroutine processes the nonlinear Levenberg-Marquart algorithm and returns the one-dimensional array params at a given iperp. The variable quality is the sum of the squares of all residuals. |
map_read | alps_io | Subroutine | Reads in complex frequency map parameters. |
map_search | alps_fns | Subroutine | This subroutine calculates the map of the determinant of the dispersion tensor in complex frequency space. check |
normalize | ../../interpolation.f90 | Subroutine | This subroutine normalises the fine interpolation grid. |
om_double_scan | alps_fns | Subroutine | This subroutine scans along a prescribed plane in wavevector space to map out in this space. It is required that n_scan=2. KGK: This line causes the solution to (occasionally) smoothly transition to unphysical values. Suppressing until we understand the error. |
om_scan | alps_fns | Subroutine | This subroutine scans solutions along a single prescribed path in wavevector space. KGK: This line causes the solution to (occasionally) smoothly transition to unphysical values. Suppressing until we understand the error. |
output_fit | alps_analyt | Subroutine | This subroutine outputs the fit parameters for iperp=0 to stdout to monitor the fit. |
output_time | alps_io | Subroutine | Outputs the date and time in a given format using intrinsic FORTRAN function. |
pass_distribution | alps_com | Subroutine | Passes distribution functions and associated parameters. |
pass_instructions | alps_com | Subroutine | Passes information between processes. |
poly_read | alps_io | Subroutine | Reads in Polynomial Basis Function Parameters |
polyharmonic_spline | ../../interpolation.f90 | Subroutine | This soubroutine interpolates the grid with a polyharmonic thin-plate spline. This subroutine needs the LUPACK and BLAS libraries to evoke the dgesv subroutine. The method uses the Thin Plate Spline. We use these resources: http://cseweb.ucsd.edu/~sjb/eccv_tps.pdf http://www.univie.ac.at/nuhag-php/bibtex/open_files/po94_M%20J%20D%20Powell%2003%2093.pdf http://vision.ucsd.edu/sites/default/files/fulltext(4).pdf |
polyharmonic_spline | alps_fns_rel | Subroutine | This soubroutine interpolates the grid with a polyharmonic thin-plate spline. This subroutine needs the LUPACK and BLAS libraries to evoke the dgesv subroutine. The method uses the Thin Plate Spline. We use these resources: http://cseweb.ucsd.edu/~sjb/eccv_tps.pdf http://www.univie.ac.at/nuhag-php/bibtex/open_files/po94_M%20J%20D%20Powell%2003%2093.pdf http://vision.ucsd.edu/sites/default/files/fulltext(4).pdf |
principal_integral_rel | alps_fns_rel | Function | This function performs the integration near resonances as described in Section 3.1 of the code paper for a relativistic calculation. It is only called if resonances are present in or near the integration domain. |
read_f0 | alps_io | Subroutine | Subroutine for reading in background distribution function |
read_in_params | generate_distribution | Subroutine | This subroutine reads in the parameters for the generation of distribution functions for ALPS. |
read_in_params | interpolate | Subroutine | This subroutine reads in system parameters input file (namelist) as argument after executable:
|
refine_guess | alps_fns | Subroutine | This subroutine refines the guess at the starting point of the search for solutions to the dispersion relation when scanning. It is also used by map_search to identify the roots on the map. |
resU | alps_fns | Function | This function evaluates the term proportional to in Eq. (2.9) of the code paper. |
resU_rel | alps_fns_rel | Function | This function evaluates the term proportional to in Eq. (2.9) of the code paper for the relativistic calculation. |
scan_read | alps_io | Subroutine | The most important subroutine. Reads in wavevector scan parameters. Defines scanner, which controls the behavior of the wavevector scan. |
secant | alps_fns | Subroutine | This subroutine applies the secant method to find the roots of the dispersion tensor. |
set_polynomial_basis | alps_analyt | Subroutine | This subroutine evaluates the General Linear Least Squares fit to the distribution function for component 'is' using the selected polynomial basis functions. |
solution_read | alps_io | Subroutine | Reads in initial guesses for dispersion solutions. |
spec_read | generate_distribution | Subroutine | Subroutine for reading in species parameters. |
spec_read | alps_io | Subroutine | Subroutine for reading in species parameters |
split_processes | alps_fns | Subroutine | This subroutine defines the tasks for the individual processes. It uses the number of species and the required orders of the Bessel functions to define the splitting across the MPI processes. |
WOFZ | alps_nhds | Subroutine | Given a complex number Z = (XI,YI), this subroutine computes the value of the Faddeeva function W(Z) = exp(-Z2)erfc(-IZ), where erfc is the complex complementary error function and I is the imaginary unit. |