INGENIA

QNT-06

Rectangular-barrier tunneling

T ≈ exp(−2 κ L), κ = √(2m(V−E))/ħ.

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TunnelingGamow / WKB

Governing equation

T≈exp⁡(−2κL),κ=2m(V−E)ℏT\approx\exp(-2\kappa L),\quad \kappa=\dfrac{\sqrt{2m(V-E)}}{\hbar}

L∈[0.05,5]L \in \left[0.05, 5\right]

where

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

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QNT-06 · quantum
00:0 / 00:08
①

Governing law — red

T≈exp⁡(−2κL),κ=2m(V−E)ℏT\approx\exp(-2\kappa L),\quad \kappa=\dfrac{\sqrt{2m(V-E)}}{\hbar}

L∈[0.05,5]L \in \left[0.05, 5\right]

L=0.05L = 0.05κ=0.412\kappa = 0.412

②

Domain of the variable — blue

Lmin⁡=0.05,Lmax⁡=5L_{\min} = 0.05,\quad L_{\max} = 5

L∈[0.05,5]L \in \left[0.05, 5\right]

L=0.05L = 0.05L=0.05L = 0.05

③

Response curve — green

T≈exp⁡(−2κL),κ=2m(V−E)ℏT\approx\exp(-2\kappa L),\quad \kappa=\dfrac{\sqrt{2m(V-E)}}{\hbar}

L∈[0.05,5]L \in \left[0.05, 5\right]

L=0.05L = 0.05κ=0.412\kappa = 0.412

④

Rate of change — amber

dκdL\frac{\mathrm{d}\kappa}{\mathrm{d}L}

L∈[0.05,5]L \in \left[0.05, 5\right]

L=0.081L = 0.081κ′=−4.423\kappa^{\prime} = -4.423

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

Calculator

Inputs

Outputs

  • Decay constant \kappa8.874 1/nm
  • Transmission T0.000140 —
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QNT-06 · quantum
00:0 / 00:08

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