| Output-densitiesThe output of electron, hole and other charge densities is controlled by this 
keyword. !-------------------------------------------------------------------!for electrolyte$output-densities                                          
optional !
 destination-directory                   
character        
required !
 electrons                               
character        
optional !
 holes                                   
character        
optional !
 charge-density                          
character        
optional !
 intrinsic-density                       
character        
optional !
 ionized-dopant-density                  
character        
optional !
 dopant-energy-levels                    
character        
optional !
 piezo-electricity                       
character        
optional !
 pyro-electricity                        
character        
optional !
 interface-density                       
character        
optional !
 integrated-density                      
character        
optional !
 subband-density                         
character        
optional !
 spin-up-spin-down-kp-densities          character        
optional !
 ion-density                             
character         
optional !
effective-density-of-states-Nc-Nv       character        
optional !
 detailed-output                         character        
optional !
 $end_output-densities                                      
optional !
 !-------------------------------------------------------------------!
 
 
 Syntax:destination-directory = my-directory/e.g. = densities/
 
  Name of directory to which the files should be written. Must exist 
  and directory name has to include the slash (\ for DOS and / for UNIX).   electrons              = yes / 
no
 
  Flag whether to output electron density. More details, see below.     holes                  = yes / no
 
  Flag whether to output hole density. More details, see below.   charge-density         = yes / 
no 
 
  Flag whether to output overall charge density. More details, see below.   intrinsic-density      = yes / 
no 
 
  Flag whether to output the intrinsic density. More details, see below.   ionized-dopant-density = yes / 
no 
 
  Flag whether to output the ionized acceptor and donor densities.They are written to these files:
 acceptors (negative) + donors 
	(positive)density1Ddopants_ionized.dat   -
acceptors only, for each impurity 
	number and total density. Here, the density is plotted with a positive sign.density1Dacceptors_ionized.dat -
donors     
	only, for each impurity number and total densitydensity1Ddonors_ionized.dat    -
   dopant-energy-levels = yes / 
no 
 
  Flag whether to output the energy levels (energy-levels-relative, 
	see $impurity-parameters) 
	of the donors and acceptors relative to the lowest conduction band edge and 
	highest valence band edge.They are written to this file:
 It makes sense to plot this file together with the conduction and 
	valence band edges.dopant_level_profile.dat
 
 position[nm]  donor_001[eV]  acceptor_001[eV]
 ...           
	...            ...
 
   piezo-electricity      = yes / 
no
 
  Flag whether to output the piezoelectric polarization charge density. This 
  file contains the piezoelectric interface and background charge densities. The 
  latter occur in graded materials, e.g. a ternary with a linear variation of 
  the x content. More details, see below.   pyro-electricity      = yes / 
no
 
  Flag whether to output the pyroelectric polarization charge density. This 
  file contains the pyroelectric interface and background charge densities. The 
  latter occur in graded materials, e.g. a ternary with a linear variation of 
  the x content. More details, see below.   interface-density     = yes / 
no
 
  Flag whether to output information about the interface charge 
  densities, e.g. piezo- and pyroelectric interface charges as well as 
  interfaces states. More details, see below.   integrated-density    = yes / 
no
 
  Flag whether to output the integrated electron or hole charge density 
	(applies also to space charge density, dopant density, ion densities). 1D: Units [e/cm2]2D: Units
 [e/cm]3D: Units
 [e]   subband-density    = yes / 
no
 
  Flag whether to output the subband density.The electron (hole) subband density of eigenstates that are far above (below) 
  the Fermi level should be zero.
 The sum of all subband densities of the eigenstates must be equal to the 
  integrated quantum mechanical density.
 
    Similar for the holes.In a 1D quantum well one has several confined eigenstates forming 
    subbands.The file '
 subband1D_el_qc001_sg001_deg001_integrated.dat' contains the 
    electron density for each eigenstate in units of [e/cm²].If four eigenvalues have been calculated, this file contains four values.
 
 The file '
 subband1D_el_qc001_sg001_deg001.dat' contains the 
    electron density for each eigenstate in units of [1 * 1018 e/cm³].If four eigenvalues have been calculated, this file contains 1 + 4 = 5 
    columns where the first column is the grid coordinate.
 
In a 2D quantum wire one has several confined eigenstates forming 
    subbands.The file '
 subband2D_el_qc001_sg001_deg001_integrated.dat' contains the 
    electron density for each eigenstate in units of [e/cm].If four eigenvalues have been calculated, this file contains four values.
 
 The files '
 subband2D_el_qc001_sg001_deg001_ev_001.fld', 
    '*.coord', '*.dat'  contains the 
    electron density for the first eigenstate in units of [1 
    * 1018 e/cm³], similar for the second, third, ... 
    eigenstates.
In a 3D quantum dot one has several confined eigenstates.The file '
 subband3D_el_qc001_sg001_deg001_integrated.dat' contains the 
    electron density for each eigenstate in units of [e].If four eigenvalues have been calculated, this file contains four values.
 
 The files '
 subband3D_el_qc001_sg001_deg001_ev_001.fld', 
    '*.coord', '*.dat'  contains the 
    electron density for the first eigenstate in units of [1 
    * 1018 e/cm³], similar for the second, third, ... 
    eigenstates.
 Similar for k.p.
 1D example: The relevant files are: 
    densities/subband1D_el_qc001_sg001_deg001_integrated.dat
    (for Gamma conduction band)densities/subband1D_hl_qc001_sg001_deg001_integrated.dat
    (for heavy holes)densities/subband1D_hl_qc001_sg002_deg001_integrated.dat
    (for light holes)densities/subband1D_hl_qc001_sg003_deg001_integrated.dat
    (for split-off holes) qc001 means "quantum cluster no. 1".
 Note: If the electron bands at the L and X valleys are split due to 
  strain, the relevant output files should be interpreted carefully.Note: The single-band eigenstates are two-fold spin-degenerate. Thus the 
	subband density is twice as high as in the case of k.p.
   spin-up-spin-down-kp-densities = yes / 
no
 
  Flag whether to output the k.p densities 
  sorted into spin up and spin down contributions of the relevant
  k.p spinors to the densities.(Currently only 1D).
 
 Relevant output files:
 
 - densities/density1Del_kpSpinUpSpinDown.dat (electrons)(holes)- densities/density1Dhl_kpSpinUpSpinDown.dat
Contains the following four colums for the quantum mechanical 
  densities:
 
grid points        k.p density (spin 
  up)           k.p 
  density (spin down)        total 
  k.p density (spin up + spin down)
 The last column (total density) is identical to the 
  quantum mechanical k.p density output in the files:
 - densities/density1Del.dat (electrons)- densities/
density1Dhl.dat
  (holes) ion-density           = yes / 
no
 
  Flag whether to output the ion charge density of the 
  electrolyte. Note that the units are [1*1018 cm-3].The electrolyte contains i different ion species plus H3O+, 
  OH
 -, anion-and cation+ 
  ions ($electrolyte-ion-content).The density of electrolyte was calculated by the Poisson-Boltzmann 
equation in
  FUNCTION 
   
densities.
 density1Dion001.dat - first ion species
 density1Dion002.dat - second ion species
 ...
 density1Dion00i+1.dat - H3O+ ions
 density1Dion00i+2.dat - OH-ions
 density1Dion00i+3.dat - anion-ions 
  related to concentration of H3O+
 density1Dion00i+4.dat - cation+ ions related to 
  concentration of OH-
 density1DIonConcentrationCorrection.dat - Correction due to H+ 
  adsorbed or dissociated from the oxide/electrolyte interface.
 density1Dion_total.dat - sum over all ion charge densities   effective-density-of-states-Nc-Nv = yes / 
no   !
default = no
 
  Flag whether to output the effective density of states for the conduction 
	and valence bands.
 Nc = valley_degeneracy * 2
	(2 pi me 
    kBT / h² )3/2 = ... [1 * 1018 cm-3]
 Nv =                              2
	(2 pi mh 
    kBT / h² )3/2 = ... [1 * 1018 cm-3]
 
 
 ==> 2 = spin degeneracy
 The effective DOS depends on the temperature and on the effective mass.
 (Note that for the derivation of this formula an isotropic and parabolic 
	energy dispersion E(k) is assumed).
 
 The columns in the output files have the following meaning:
 
 Nc_cb1D_ind001.dat:  grid point [nm]    Nc(Gamma)        
	Nc(L)            
	Nc(X)The units ofNv_cb1D_ind001.dat:  grid point [nm]    Nv(heavy 
	hole)   Nv(light hole)   Nv(split-off 
	hole)
 
 Nc, Nv
	are [1 * 1018 cm-3].   detailed-output = yes / 
no   !
default = yes (1D)
  
                             !
default = no  (2D/3D)
 
  Flag whether to output additional densities with respect to- Gamma band
 - L band
 - X band
 - heavy hole (hh) band
 - light hole (lh) band
 - split-off hole (so) band
 
 - classical density (cl)
 - quantum mechanical density (qm)
 
 
 electrons = yes  ! contains 
	the sum of Gamma, L and X bands
 holes     = yes  ! contains the sum of heavy hole, light hole and split-off hole band
 By default, the sum of classical and quantum mechanical 
	densities is contained in the density output for the electrons and holes.
 
 This flag is useful if one is interested in the contribution of each band to 
	the total density.
 
 The relevant 1D output is
 
 - density1Del.dat - contains total electron density, quantum 
	mechanical part of the density and classical part of the density:
   The columns are labeled with el[1e18/cm3] 
	el_qm[1e18/cm3] el_cl[1e18/cm3].The electron density in is the sum over all 
conduction band edges, i.e. Gamma band, L band and X band.
 
 - density1Dhl.dat - contains total hole       
	density, quantum mechanical part of the density and classical part of the 
	density:
   The columns are labeled with hl[1e18/cm3] 
	hl_qm[1e18/cm3] hl_cl[1e18/cm3].The hole density in is the sum over all valence 
band edges, i.e. heavy hole, light hole and split-off hole band.
 - density1DGamma_L_X.dat - densities of Gamma, L and X bandsThe output file only has three columns (Gamma density, 
L density, X density) if there is no strain applied.
   In case of strain, the L and X bands can be split 
and thus additional columns arise for those grid points.
 - density1Dhh_lh_so.dat  - densities of heavy hole, light 
	hole and split-off hole band
   The output file always has three columns: hh density, 
lh density, split-off hole density
   If one does k.p for holes, one cannot 
distinguish between hh, lh, and so densities. Therefore this output is omitted.
   (The only disadvantage is if there are regions in the 
device where the classical hole density dominates,
   or if there are several quantum regions with different 
hole quantum models,
   then there will be no way to see if the density 
originates from hh, lh or so classical or single-band densities.)
   (Of course, if needed, one could split this output into classical and quantum 
mechanical contributions to the density.)   Output:1D filenames and structure:  
   Electron density [1018
cm-3]
 filename: 
  
    | density1Del_ind000.dat |  
    |  | _ind000 | number of voltage step corresponding to 
    this output file (only if voltage sweep is turned on) |  structure: For a quantum mechanical calculation: 
  
    | position | el | el_qm (quantum 
    mechanical  
    part only) | el_cl (classical 
	part only) |  
    | 0.000000E+00 | 0.000000E+00 | 0.000000E+00 | 0.000000E+00 |  
    | position in space [nm] | Electron density [1018 e/cm3] | Electron density [1018 e/cm3] | Electron density [1018 e/cm3] |  For a classical calculation: 
  
    | position | el |  
    | 0.000000E+00 | 0.000000E+00 |  
    | position in space [nm] | Electron density [1018 e/cm3] |    
   Hole density [1018
cm-3]
 filename: 
  
    | density1Dhl_ind000.dat |  
    |  | _ind000 | number of voltage step corresponding to 
    this output file (only if voltage sweep is turned on) |  structure: For a quantum mechanical calculation: 
  
    | position | hl | hl_qm (quantum 
    mechanical  part only) | hl_cl (classical 
    part only) |  
    | 0.000000E+00 | 0.000000E+00 | 0.000000E+00 | 0.000000E+00 |  
    | position in space [nm] | Hole density [1018 e/cm3] | Hole density [1018 e/cm3] | Hole density [1018 e/cm3] |  For a classical calculation: 
  
    | position | hl |  
    | 0.000000E+00 | 0.000000E+00 |  
    | position in space [nm] | Hole density [1018 e/cm3] |    
   Space charge density = -n + p -NA + ND 
+ rhopiezo + rhopyro     
[1018 cm-3]
 Note: Here, the electron density 
n and the acceptor density NA have a negative sign.Piezo and pyro charges are included as well.
 So this file contains the total density present in the device.
 filename: 
  
    | density1Dspace_charge_ind001.dat |  
    |  | _ind000 | number of voltage step corresponding to 
    this output file (only if voltage sweep is turned on) |  structure:                           
  
    | position | dens_space |  
    | 0.000000E+00 | 0.000000E+00 |  
    | position in space [nm] | Space charge density [1018 e/cm3] |    
   Intrinsic density n_i = SQRT(n * p) 
[cm-3]
 filename: structure:                           
  
    | position | dens_space |  
    | 0.000000E+00 | 0.000000E+00 |  
    | position in space [nm] | intrinsic density [e/cm3] |  Note: For the intrinsic density it is more transparent to output it in units 
of [cm-3] rather than [1018 cm-3] 
as is the case for the other densities. Note: The output in 1D contains 3 columns.- The 1st  column is position in space in [nm].
 - The 2nd column is the intrinsic density ni = SQRT(ni 
* pi) for the bulk material at the relevant grid points.
 (Note: Doping, the Poisson equation and heterostructure effects are not 
considered!)
 This is the value of the intrinsic density that enters the recombination 
rates.
 - The 3rd column is the quantity ni' = SQRT(n * p) 
for the the relevant grid points.
 Here, the densities n(x) and p(x) are the classical 
electron and hole densities at the grid point x for the calculated 
electrostatic built-in potential in equilibrium.
 This quantity is just for information. It does not enter anywhere into 
the actual calculation.
 
 
   Piezoelectric 
polarization charge density filename: structure:                           
  
    | position | dens_piezo |  
    | 0.000000E+00 | 0.000000E+00 |  
    | position in space [nm] | Piezo-charge density  
    [1018 e/cm3] |    
   Pyroelectric 
polarization charge density filename: structure:                           
  
    | position | dens_pyro |  
    | 0.000000E+00 | 0.000000E+00 |  
    | position in space [nm] | Pyro-charge density  [1018 e/cm3] |    
    Integrated density filenames: 
  
    | int_el_dens.dat(Electron density)
 int_hl_dens.dat      (Hole density)(Space charge density)int_sp_dens.dat
 |  structure:                           
  
    | Pois_001 | Cl_001 | Total |  
    | 0.000000E+00 | 0.000000E+00 | 0.000000E+00 |  
    | Voltage at poisson cluster 
	[001]  [V] | Integrated density for 
	material cluster [001] Units: 1D: [carriers/cm2]
 2D: [carriers/cm]
 3D: [carriers]
 | Sum of all clusters |    
 Surface and interface 
charge density Filename: Structure: Information about interface/surface charge densities:
 Scaling: n2d0= 1.000000000000000E+016
 e.g.:    n2d0=1d4 --> particles/cm^2
 [C/m^2] => / |e| / n2d0 => 
|e| 
10^16 m^-2
 
 ---------------------
 PIEZOELECTRIC CHARGES
 ---------------------
 Left boundary:        0.000000000000000E+000
 Left boundary:        0.000000000000000E+000
 Right boundary:       0.000000000000000E+000
 Right boundary:       0.000000000000000E+000
 
 Interface number 1 at position 100.000000000000 nm
 piezoelectric charge:  2.762229388428833E-003   C/m^2
 piezoelectric charge:  1.72403413480667         
1E12 |e| / cm^2
 
 Interface number 2 at position 117.000000000000 nm
 piezoelectric charge: -2.762229388428833E-003   C/m^2
 piezoelectric charge: -1.72403413480667         
1E12 |e| / cm^2
 
 
 --------------------
 PYROELECTRIC CHARGES
 --------------------
 Left boundary:       0.000000000000000E+000     
C/m^2
 Left boundary:       0.000000000000000E+000     
1E12 |e| / cm^2
 Right boundary:      0.000000000000000E+000     
C/m^2
 Right boundary:      0.000000000000000E+000     
1E12 |e| / cm^2
 
 Interface number 1 at position 100.000000000000 nm
 pyroelectric charge:  2.934399999999997E-003    C/m^2
 pyroelectric charge:  1.83149371531894          
1E12 |e| / cm^2
 
 Interface number 2 at position 117.000000000000 nm
 pyroelectric charge: -2.934399999999997E-003    C/m^2
 pyroelectric charge: -1.83149371531894          
1E12 |e| / cm^2
     Full-band density approach 
(k.p) The following file contains the background charge density when using the 
full-band envelope-function approach (broken-gap = 
full-band-density).
 density1DFullBandBackground.dat If using $quantum-model-electrons, 
this number contains the positive background charge density.If using
  $quantum-model-holes   
, this number contains the negative background charge density. For the same structure, using 
$quantum-model-electrons, the positive background charge density is 
three times larger than the negative background charge density (when using
$quantum-model-holes). |