.claude/skills/3d-lattice-tunneling/SKILL.md
Calculate electron transmission probability through planar barriers in 3D crystals by applying momentum conservation principles. Use when analyzing tunneling in three-dimensional lattices, when perpendicular momentum conservation must be accounted for, or when converting 1D tunneling results to 3D scenarios involving crystal structures.
npx skillsauth add ShaneLogic/SolarLab 3D Lattice TunnelingInstall this skill globally with one command. Works with Claude Code, Cursor, and Windsurf.
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Apply this skill when:
Recognize that in a 3D lattice, momentum components perpendicular to the tunneling direction are conserved. Only the momentum component in the tunneling direction decreases exponentially through the barrier.
Compute the energy associated with momentum perpendicular to tunneling:
E_perp = (ℏ² × k_perp²) / (2m)
where:
Determine the mean energy of the tunneling electron:
E_bar = e × F × a
where:
Calculate the reduction factor η representing the fraction of electrons with favorable momentum distribution:
η = 1 / (1 + (e × F × a) / (4 × E))
This integrated result accounts for the distribution of perpendicular momenta across the electron population.
Combine the reduction factor with the 1D transmission probability:
Te_3D = η × Te_1D
For a flat plate parabolic barrier, the complete expression becomes:
Te_3D = [1 / (1 + (e × F × a) / (4 × E))] × exp(-π × (ΔE)² / (2 × ℏ × e × F))
where ΔE is the energy difference across the barrier.
| Variable | Type | Description | |----------|------|-------------| | η | Factor | Reduction factor due to momentum distribution | | E_perp | Energy | Energy of perpendicular momentum component | | E_bar | Energy | Mean energy of tunneling electron | | k_perp | Wavenumber | Wavevector perpendicular to tunneling direction | | Te_3D | Probability | 3D transmission probability | | Te_1D | Probability | 1D transmission probability |
Returns the reduced transmission probability Te_3D that accounts for 3D momentum distribution effects in crystal lattice tunneling.
Based on calculations by Moll (1964).
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