INGENIA

QNT-06

Rectangular-barrier tunneling

T ≈ exp(−2 κ L), κ = √(2m(V−E))/ħ.

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TunnelingGamow / WKB

Governing equation

Texp(2κL),κ=2m(VE)T\approx\exp(-2\kappa L),\quad \kappa=\dfrac{\sqrt{2m(V-E)}}{\hbar}

where

V
Barrier height (eV)
E
Energy (eV)
L
Width (nm)
m
Mass (m_e)
\kappa
Decay constant (1/nm)
T
Transmission ()

Lecture brief

Historical brief

Planck (1900), Einstein’s photoelectric law, Bohr, de Broglie, Heisenberg and Schrödinger’s 1926 equation rebuilt matter as amplitude. These sheets are the first solvable models: wells, spin, tunneling, uncertainty. This sheet (QNT-06 — Rectangular-barrier tunneling) is the form associated with Gamow / WKB. Working symbols: VV, EE, LL, mm \rightarrow κ\kappa, TT. The WKB (and exact thick-barrier) transmission is exponentially small in the product of decay constant and width, the origin of α-decay lifetimes.

Purpose

Purpose: compute κ\kappa, TT from VV, EE, LL, mm in Quantum mechanics via Texp(2κL),κ=2m(VE)T\approx\exp(-2\kappa L),\quad \kappa=\dfrac{\sqrt{2m(V-E)}}{\hbar} T ≈ exp(−2 κ L), κ = √(2m(V−E))/ħ. Use it when a real quantum mechanics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given V=5.000eVV = 5.000\,\mathrm{eV}, E=2.000eVE = 2.000\,\mathrm{eV}, L=0.500nmL = 0.500\,\mathrm{nm}, m=1.000mem = 1.000\,\mathrm{m_e}, the governing relation Texp(2κL),κ=2m(VE)T\approx\exp(-2\kappa L),\quad \kappa=\dfrac{\sqrt{2m(V-E)}}{\hbar} yields κ=8.8741/nm\kappa = 8.874\,\mathrm{1/nm}, T=1.400e4T = 1.400e-4\,\mathrm{—}. E < V, thick barrier, electron mass. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Decay constant \kappa8.874 1/nm
  • Transmission T0.000140
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QNT-06 · quantum
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Narration of this film

E < V, thick barrier, electron mass.

The WKB (and exact thick-barrier) transmission is exponentially small in the product of decay constant and width, the origin of α-decay lifetimes.

Reading speed

Watch on YouTube