Transmission Coefficient Calculator
Calculate quantum transmission probability through a square potential barrier for particle energy and barrier height.
What Is a Transmission Coefficient Calculator?
The transmission coefficient T gives the probability that a quantum particle passes through a potential barrier instead of reflecting off it. Our Transmission Coefficient Calculator models a rectangular barrier of height V0 and width L, covering both the tunneling case (E below V0) and the oscillatory case (E above V0).
How the Calculation Works
When the particle energy E is below the barrier height, the wavefunction decays inside the barrier and T is:
$$T = \left[1 + \frac{V_0^2 \sinh^2(\kappa L)}{4E(V_0 - E)}\right]^{-1}, \qquad \kappa = \frac{\sqrt{2m(V_0 - E)}}{\hbar}$$
When E is above the barrier, the interior wave propagates and the expression becomes oscillatory:
$$T = \left[1 + \frac{V_0^2 \sin^2(k L)}{4E(E - V_0)}\right]^{-1}, \qquad k = \frac{\sqrt{2m(E - V_0)}}{\hbar}$$
Where:
- m is the particle mass
- V₀ is the barrier height and E is the particle energy
- L is the barrier width
- κ is the decay constant below the barrier and k the wavenumber above it
- ħ is the reduced Planck constant
Worked Example
An electron with E = 0.5 eV meets a 1 eV barrier that is 0.5 nm wide. The decay constant is κ = 3.62 × 10⁹ m⁻¹, so κL = 1.81 and sinh²(1.81) = 8.83. Substituting gives T = (1 + 8.83)⁻¹ ≈ 0.102, meaning roughly a 10% chance of tunneling through.
Related tools include the Wavenumber Calculator and the Work and Power Calculator.
Frequently Asked Questions
What is quantum tunneling?
Quantum tunneling is the ability of a particle to cross an energy barrier that it could not overcome classically. The wavefunction decays exponentially inside the barrier rather than dropping to zero, giving a non-zero transmission probability.
Why does a wider barrier lower T?
Below the barrier, the wavefunction decays as exp(-κL). Increasing the width L multiplies the exponent, so the amplitude reaching the far side drops sharply and the transmission coefficient falls.
What happens when E is greater than V0?
Classically the particle should always pass, but the wave nature of matter causes partial reflection at each interface. T then oscillates with energy and barrier width, reaching 1 at certain resonance points.
Does the particle mass matter?
Yes. The decay constant κ depends on the square root of mass, so heavier particles tunnel far less readily than light ones. This is why tunneling is prominent for electrons but negligible for macroscopic objects.