ITO material model
1. Introduction
This page contains the OghmaNano material model for ITO (In2O3:Sn).
Indium tin oxide (In2O3:Sn), degenerate transparent conducting oxide
The model is written in Lua and provides simulation-ready material parameterisations for use within OghmaNano. For documentation, licensing, references, and information about the scope and accuracy of these models, see the material scripting documentation.
2. Lua material model
Supporting definitions
-- See end of file for copyright, licensing and documentation links.
local material = {}
Material name (material.name)
function material.name()
local enabled = true
return "ITO", enabled
end
Material description (material.description)
function material.description()
local enabled = true
return "Indium tin oxide (In2O3:Sn), degenerate transparent conducting oxide", enabled
end
Chemical formula (material.formula)
function material.formula()
local enabled = true
return "In2O3:Sn", enabled
end
Band gap energy (material.Eg)
function material.Eg(state)
-- Units: eV
--
-- Reference:
-- A. Walsh et al., "Nature of the band gap of In2O3 revealed by
-- first-principles calculations and X-ray spectroscopy",
-- Phys. Rev. Lett. 100, 167402, 2008.
--
-- Subtlety: the true fundamental (direct) gap of In2O3 is ~2.9 eV,
-- but the onset transition is weak/dipole-forbidden, so the strong
-- optical absorption edge sits higher (~3.75 eV), and in degenerate
-- ITO the Burstein-Moss shift widens the apparent optical gap
-- further to ~3.75-4.3 eV.
--
-- A device-relevant value of 3.6 eV is used. Constant.
local enabled = true
local value = 3.6
return value, enabled
end
Deformation potential Xi (material.Xi)
function material.Xi(state)
-- Electron affinity
-- Units: eV
--
-- Reference:
-- ITO electrode work-function literature.
--
-- ITO work function is treatment-dependent (~4.4-4.8 eV; ~4.7 eV
-- after oxygen-plasma / UV-ozone). Because ITO is DEGENERATE, the
-- Fermi level sits in the conduction band and the effective work
-- function nearly coincides with the electron affinity. The work
-- function is the number that sets contact alignment. Approximate.
local enabled = true
local value = 4.7
return value, enabled
end
Effective conduction-band density of states (material.Nc)
function material.Nc(state)
-- Effective conduction-band density of states
-- Units: m^-3
--
-- Reference:
-- From In2O3 CB effective mass m_e* ~ 0.3 m0:
-- Nc(300 K) ~ 4e18 cm^-3 = 4e24 m^-3.
--
-- Note: ITO is degenerate (free-electron density ~1e21 cm^-3), so
-- this parabolic Nc is a formal quantity only; carrier density is
-- set by doping. Approximate.
local enabled = true
local T = state.T
local value = 4.0e24*(T/300.0)^1.5
return value, enabled
end
Effective valence-band density of states (material.Nv)
function material.Nv(state)
-- Effective valence-band density of states
-- Units: m^-3
--
-- Reference:
-- From a heavy valence-band mass (m_h* ~ 1 m0):
-- Nv(300 K) ~ 2.5e19 cm^-3 = 2.5e25 m^-3.
--
-- Note: the In2O3 hole mass is poorly constrained; approximate.
-- Rarely relevant for an n-type TCO.
local enabled = true
local T = state.T
local value = 2.5e25*(T/300.0)^1.5
return value, enabled
end
Electron mobility (material.mu_e)
function material.mu_e(state)
-- Low-field electron mobility
-- Units: m^2 V^-1 s^-1
--
-- Reference:
-- Representative ITO thin-film Hall mobility ~15-50 cm^2/V/s; a
-- mid value of 35 cm^2/V/s = 0.0035 m^2/V/s is used.
--
-- Note: transport is ionised-impurity limited in this degenerate
-- material (not phonon limited), so no (300/T)^n law is applied.
-- Approximate.
local enabled = true
local value = 0.0035
return value, enabled
end
Electron mobility in the x direction (material.mue_x)
function material.mue_x(state)
return material.mu_e(state)
end
Electron mobility in the y direction (material.mue_y)
function material.mue_y(state)
return material.mu_e(state)
end
Electron mobility in the z direction (material.mue_z)
function material.mue_z(state)
return material.mu_e(state)
end
Hole mobility (material.mu_h)
function material.mu_h(state)
-- Low-field hole mobility
-- Units: m^2 V^-1 s^-1
--
-- Note: ITO is an n-type electrode; hole transport is essentially
-- irrelevant to device operation and not experimentally
-- constrained. Small placeholder; do not rely on it.
local enabled = true
local value = 1.0e-4
return value, enabled
end
Hole mobility in the x direction (material.muh_x)
function material.muh_x(state)
return material.mu_h(state)
end
Hole mobility in the y direction (material.muh_y)
function material.muh_y(state)
return material.mu_h(state)
end
Hole mobility in the z direction (material.muh_z)
function material.muh_z(state)
return material.mu_h(state)
end
Relative dielectric permittivity (material.epsilonr)
function material.epsilonr(state)
-- Relative static permittivity
-- Dimensionless
--
-- Reference:
-- In2O3 / ITO static permittivity ~8.9-9.5 (In2O3 optical and
-- dielectric literature).
--
-- A representative value of 9.0 is used.
local enabled = true
local value = 9.0
return value, enabled
end
Free-carrier radiative recombination (material.free_to_free_recombination)
function material.free_to_free_recombination(state)
-- Radiative (band-to-band) recombination coefficient
-- Units: m^3 s^-1
--
-- Note: as a degenerate electrode, bulk radiative recombination is
-- not the operative physics (contact recombination dominates).
-- Poorly constrained placeholder.
local enabled = true
local value = 1.0e-21
return value, enabled
end
Electron Auger recombination coefficient (material.auger_Cn)
function material.auger_Cn(state)
-- Electron Auger recombination coefficient
-- Units: m^6 s^-1
--
-- Note: not characterised for ITO. Order-of-magnitude placeholder.
local enabled = true
local value = 1.0e-43
return value, enabled
end
Hole Auger recombination coefficient (material.auger_Cp)
function material.auger_Cp(state)
-- Hole Auger recombination coefficient
-- Units: m^6 s^-1
--
-- Note: not characterised for ITO. Order-of-magnitude placeholder.
local enabled = true
local value = 1.0e-43
return value, enabled
end
Interface trap energy (material.ss_srh_trap_energy)
function material.ss_srh_trap_energy(state)
-- SRH trap energy relative to the middle of the band gap.
-- Units: eV
--
-- Positive values are above mid-gap (towards the conduction band).
-- Negative values are below mid-gap (towards the valence band).
local enabled = true
local value = 0.0
return value, enabled
end
Interface trap density (material.ss_srh_Nt)
function material.ss_srh_Nt(state)
-- SRH trap density
-- Units: m^-3
--
-- Material-quality dependent placeholder.
local enabled = true
local value = 1.0e21
return value, enabled
end
Interface electron capture cross-section (material.ss_srh_sigma_n)
function material.ss_srh_sigma_n(state)
-- Electron capture cross section
-- Units: m^2
local enabled = true
local value = 1.0e-19
return value, enabled
end
Interface hole capture cross-section (material.ss_srh_sigma_p)
function material.ss_srh_sigma_p(state)
-- Hole capture cross section
-- Units: m^2
local enabled = true
local value = 1.0e-19
return value, enabled
end
Lattice thermal conductivity (material.thermal_kl)
function material.thermal_kl(state)
-- Thermal conductivity
-- Units: W m^-1 K^-1
--
-- Reference:
-- ITO thin-film thermal conductivity ~3-11 W/m/K (thin-film
-- thermal-transport literature).
--
-- A representative 8 W/m/K is used. Poorly constrained /
-- thickness-dependent.
local enabled = true
local value = 8.0
return value, enabled
end
Specific heat capacity (material.heat_capacity)
function material.heat_capacity(state)
-- Specific heat capacity
-- Units: J kg^-1 K^-1
--
-- Reference:
-- In2O3, c_p(300 K) ~ 360 J/kg/K (CRC Handbook of Chemistry and
-- Physics). Approximate.
local enabled = true
local value = 360.0
return value, enabled
end
Mass density (material.density)
function material.density(state)
-- Mass density
-- Units: kg m^-3
--
-- Reference:
-- In2O3 / ITO rho ~ 7.15 g/cm^3 (CRC Handbook of Chemistry and
-- Physics).
local enabled = true
local value = 7150.0
return value, enabled
end
Crystal lattice constant (material.lattice_constant)
function material.lattice_constant(state)
-- Cubic lattice constant
-- Units: m
--
-- ENABLED: unlike the other TCOs here, the parent oxide In2O3
-- crystallises in the CUBIC bixbyite structure, so a single cubic
-- lattice constant IS meaningful.
--
-- Reference (crystallography):
-- R. W. G. Wyckoff, "Crystal Structures".
-- Bixbyite In2O3: a = 10.117 A at 300 K (large 80-atom cell); Sn
-- substitutes on In sites in ITO. Linear thermal expansion
-- ~6.7e-6 /K near 300 K is applied (approximate).
local enabled = true
local T = state.T
local a300 = 10.117e-10
local expansion = 6.7e-6
local value = a300*(1.0 + expansion*(T - 300.0))
return value, enabled
end
Electron thermal relaxation time (material.thermal_tau_e)
function material.thermal_tau_e(state)
-- Electron energy relaxation time towards the lattice temperature
-- Units: s
--
-- Value basis: Numerical fallback
-- Confidence: Low
--
-- Reference:
-- No specific reference supplied.
--
-- Comments:
-- Normally used as a degenerate conductor/electrode, not as a bipolar
-- non-degenerate DD layer. Fast fallback only.
local enabled = false
local value = 1.000000e-14
return value, enabled
end
Hole thermal relaxation time (material.thermal_tau_h)
function material.thermal_tau_h(state)
-- Hole energy relaxation time towards the lattice temperature
-- Units: s
--
-- Value basis: Numerical fallback
-- Confidence: Low
--
-- Reference:
-- No specific reference supplied.
--
-- Comments:
-- Normally used as a degenerate conductor/electrode, not as a bipolar
-- non-degenerate DD layer. Fast fallback only.
local enabled = false
local value = 1.000000e-14
return value, enabled
end
Material parameter summary (material.print)
function material.print()
local state = {
T = 300.0,
x = 0.0,
y = 0.0,
z = 0.0,
photon_density = 0.0,
}
print(string.format("Material: %s", material.name()))
print(string.format("Description: %s", material.description()))
print(string.format("Formula: %s", material.formula()))
print(string.format("Temperature: %.2f K", state.T))
print(string.format("Position: %.6e, %.6e, %.6e m", state.x, state.y, state.z))
print(string.format("Photon density: %.6e m^-3", state.photon_density))
print(string.format("Band gap: %.6f eV", material.Eg(state)))
print(string.format("Electron affinity: %.6f eV", material.Xi(state)))
print(string.format("Electron mobility: %.6e m^2/V/s", material.mu_e(state)))
print(string.format("Hole mobility: %.6e m^2/V/s", material.mu_h(state)))
print(string.format("Nc: %.6e m^-3", material.Nc(state)))
print(string.format("Nv: %.6e m^-3", material.Nv(state)))
print(string.format("Relative permittivity: %.6f", material.epsilonr(state)))
print(string.format("Radiative coeff.: %.6e m^3/s", material.free_to_free_recombination(state)))
print(string.format("Electron Auger coeff.: %.6e m^6/s", material.auger_Cn(state)))
print(string.format("Hole Auger coeff.: %.6e m^6/s", material.auger_Cp(state)))
print(string.format("SRH trap energy: %.6f eV", material.ss_srh_trap_energy(state)))
print(string.format("SRH trap density: %.6e m^-3", material.ss_srh_Nt(state)))
print(string.format("SRH sigma n: %.6e m^2", material.ss_srh_sigma_n(state)))
print(string.format("SRH sigma p: %.6e m^2", material.ss_srh_sigma_p(state)))
print(string.format("Electron energy relax.: %.6e s", material.thermal_tau_e(state)))
print(string.format("Hole energy relax.: %.6e s", material.thermal_tau_h(state)))
print(string.format("Thermal conductivity: %.6e W/m/K", material.thermal_kl(state)))
print(string.format("Heat capacity: %.6e J/kg/K", material.heat_capacity(state)))
print(string.format("Mass density: %.6e kg/m^3", material.density(state)))
end
return material
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