Classes
struct	parameters_8band_nostrain
class	cartesian_8band
struct	effective_mass_properties
class	cartesian_effective_mass
class	hamiltonian
Typedefs
typedef libmodelxx::grid::cartesian_grid < libmodelxx::structure::material *, 1, 1 >	matgrid
typedef libmodelxx::grid::cartesian_grid < double, 1, 1 >	potgrid
typedef libmodelxx::grid::cartesian_grid < libmodelxx::structure::material *, 1, 1 >	matgrid_t
typedef libmodelxx::grid::cartesian_grid < double, 1, 1 >	potgrid_t
Enumerations
enum	cartesian_8terms { CS_P = 0, CS_M, VH_P, VL_P, VL_M, VH_M, VO_P, VO_M }
enum	effective_mass_parameter { OOMSTAR, MSTAR, POTENTIAL, TOTAL_POTENTIAL, EC, EPSILON }
enum	gerror_domains { HAMILTONIAN_CARTESIAN_EFFECTIVE_MASS_GERROR_DOMAIN, HAMILTONIAN_CARTESIAN_8BAND_GERROR_DOMAIN }
enum	model { KDOTP_EFFECTIVE_MASS, KDOTP_8BAND }
enum	boundary_condition { HARDWALL, PERIODIC }
Functions
static short	get_consts_index (short unsigned row, short unsigned col)
static int	check_constants_hermiticity (unsigned short *eye)
static GError *	store_reduced_material_parameters (struct parameters_8band_nostrain params, matgrid mg, potgrid *pg)
Variables
static const struct llw_complex_double	consts_8band []

Typedef Documentation

typedef libmodelxx::grid::cartesian_grid<libmodelxx::structure::material*,1,1> kdotp::libkdotp::hamiltonian::matgrid

Definition at line 41 of file hamiltonian_cartesian_8band.c++.

typedef libmodelxx::grid::cartesian_grid<libmodelxx::structure::material*,1,1> kdotp::libkdotp::hamiltonian::matgrid_t

Definition at line 42 of file hamiltonian_cartesian_effective_mass.c++.

typedef libmodelxx::grid::cartesian_grid<double,1,1> kdotp::libkdotp::hamiltonian::potgrid

Definition at line 42 of file hamiltonian_cartesian_8band.c++.

typedef libmodelxx::grid::cartesian_grid<double,1,1> kdotp::libkdotp::hamiltonian::potgrid_t

Definition at line 43 of file hamiltonian_cartesian_effective_mass.c++.

Enumeration Type Documentation

enum kdotp::libkdotp::hamiltonian::boundary_condition

Enumerator:

HARDWALL
PERIODIC

Definition at line 44 of file hamiltonians.h++.

                              {
  HARDWALL,
  PERIODIC
      };

enum kdotp::libkdotp::hamiltonian::cartesian_8terms

Note:: CS = conduction band S-state VH is valence heavy hole VL is valence light hole VO is valence split-off _P is plus (+ 1/2 or 3/2 depending on state) _M is minus (- 1/2 or 3/2 depending on state)

Enumerator:

CS_P
CS_M
VH_P
VL_P
VL_M
VH_M
VO_P
VO_M

Definition at line 41 of file hamiltonian_cartesian_8band.h++.

                            {
  CS_P = 0,
  CS_M,
  VH_P,
  VL_P,
  VL_M,
  VH_M,
  VO_P,
  VO_M
      };

enum kdotp::libkdotp::hamiltonian::effective_mass_parameter

Enumerator:

OOMSTAR
MSTAR
POTENTIAL
TOTAL_POTENTIAL
EC
EPSILON

Definition at line 50 of file hamiltonian_cartesian_effective_mass.h++.

                                    {
  OOMSTAR,
  MSTAR,
  POTENTIAL,
  TOTAL_POTENTIAL,
  EC,
  EPSILON
      };

enum kdotp::libkdotp::hamiltonian::gerror_domains

Enumerator:

HAMILTONIAN_CARTESIAN_EFFECTIVE_MASS_GERROR_DOMAIN
HAMILTONIAN_CARTESIAN_8BAND_GERROR_DOMAIN

Definition at line 31 of file hamiltonians.h++.

                          {
  HAMILTONIAN_CARTESIAN_EFFECTIVE_MASS_GERROR_DOMAIN,
  HAMILTONIAN_CARTESIAN_8BAND_GERROR_DOMAIN
      };

enum kdotp::libkdotp::hamiltonian::model

Enumerator:

KDOTP_EFFECTIVE_MASS
KDOTP_8BAND

Definition at line 39 of file hamiltonians.h++.

                 {
  KDOTP_EFFECTIVE_MASS,
  KDOTP_8BAND
      };

Function Documentation

static int kdotp::libkdotp::hamiltonian::check_constants_hermiticity ( unsigned short * eye ) [static]

does a quick check to make sure the constants matrix is truly Hermitean

Parameters:

eye	pointer to a short unsigned int to store the row index of the invalid constant.

Returns:: -j if a real portion was not identical across a transpose +j if a complex portion was not negated across a transpose 0 if identical

Note:: this is a debugging/safety aid, but costs basically no time.

Definition at line 139 of file hamiltonian_cartesian_8band.c++.

Referenced by kdotp::libkdotp::hamiltonian::cartesian_8band::cartesian_8band().

                                                                  {
  for(unsigned short i=0; i<8; i++) {
    for(unsigned short j=0; j<8; j++) {
      /*
       *This is buggy and this file currently unused, so it's been commented out so that things will build.
      if(consts_8band[get_consts_index(i, j)].re 
         != consts_8band[get_consts_index(i, j)].re) {
        *eye = i;
        return -j;
      }
      if(consts_8band[get_consts_index(i, j)].im 
         != -consts_8band[get_consts_index(i, j)].im) {
        *eye = i;
        return j;
      }
      */
    }
  }
  return 0;
      }

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static short kdotp::libkdotp::hamiltonian::get_consts_index	(	short unsigned	row,
		short unsigned	col
	)		`[inline, static]`

Simple helper function to get the appropriate constant out of consts_8band[]

Note:: entries are stored in column-major order.; rows, cols are in the order of page 215 in Winkler's spin-orbit book

Definition at line 128 of file hamiltonian_cartesian_8band.c++.

                                                                                   {
  return row*8 + col;
      }

static GError* kdotp::libkdotp::hamiltonian::store_reduced_material_parameters	(	struct parameters_8band_nostrain *	params,
		matgrid *	mg,
		potgrid *	pg
	)		`[static]`

Definition at line 160 of file hamiltonian_cartesian_8band.c++.

Referenced by kdotp::libkdotp::hamiltonian::cartesian_8band::cartesian_8band().

                                                                                                                           {
  int e;
  char *s;
  const char* paramstring[] = {"E_g_Gamma", "E_v", "Delta", "m_e_Gamma", "gamma1", "gamma2", "gamma3", "Ep"};
  double temp_params[8];
  for(long unsigned i=0; i<mg->L[0]; i++) {
    for(short unsigned p=0; p<8; p++) {
      temp_params[i] = mg->data[i]->get_property(paramstring[p], &e);
      if(e != 0) {
        return g_error_new(HAMILTONIAN_CARTESIAN_8BAND_GERROR_DOMAIN, 10+e, "Got error %d getting property (%s) at site %lu (material %s).\n", e, paramstring[p], i, s=mg->data[i]->get_name());
      }
    }
    params[i].Ec = temp_params[0]+temp_params[1];
    params[i].Ev = temp_params[1];
    params[i].Eso = temp_params[1]-temp_params[2];
    params[i].P = sqrt(hbar*hbar/(2*m0)*temp_params[7]);
    /*For the reduced param terms, see Winkler's Spin-orbit book page 216*/
    params[i].oo_mstar = 1.0/temp_params[4] - temp_params[7]/(3*m0)*(2/(temp_params[0]+temp_params[1]) + 1/(temp_params[0]+temp_params[1]+temp_params[2]));
    params[i].gamma1 = temp_params[4] - temp_params[7]/(3*(temp_params[0] + temp_params[1]));
    params[i].gamma2 = temp_params[5] - temp_params[7]/(6*(temp_params[0] + temp_params[1]));
    params[i].gamma3 = temp_params[6] - temp_params[7]/(6*(temp_params[0] + temp_params[1]));
  }
  return NULL;
      }

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Variable Documentation

const struct llw_complex_double kdotp::libkdotp::hamiltonian::consts_8band[] [static]

Note:: This matrix contains all of the *constants* of the 8-band k-dot-p matrix. Any non-constants across the nanostructure (e.g. the coupling constants P, gamma_i, m', etc.) are dependent upon position and, therefore, not included (they're not constant across the entire structure (nor can they be determined at compile time)

Definition at line 50 of file hamiltonian_cartesian_8band.c++.

kdotp::libkdotp::hamiltonian Namespace Reference

Classes

Typedefs

Enumerations

Functions

Variables

Typedef Documentation

Enumeration Type Documentation

Function Documentation

Variable Documentation