Calculate the Compton wavelength λ_C = h/(mc) for any particle. Explore Compton scattering angles, rest energies, and quantum length scales.
The Compton wavelength λ_C = h/(mc) is a fundamental quantum length scale associated with any massive particle. For the electron, it is 2.426 × 10⁻¹² m (2.426 pm) — much smaller than an atom but larger than the classical electron radius. It represents the wavelength of a photon whose energy equals the particle's rest mass energy (E = mc²).
The Compton wavelength appears in Compton scattering, where a photon bouncing off an electron shifts in wavelength by Δλ = λ_C(1 − cos θ). This shift — first measured by Arthur Compton in 1923 — provided direct evidence that photons carry momentum, a key confirmation of quantum mechanics.
This calculator computes the Compton wavelength, reduced Compton wavelength (ƛ = ℏ/mc), rest energy, and Compton scattering shift for any particle from a database of fundamental particles or custom mass input. It includes length scale comparisons and a complete scattering angle table. Check the example with realistic values before reporting.
The Compton wavelength connects rest mass, photon energy, and quantum length scales in a single parameter. Calculating it for different particles requires precise fundamental constants and unit conversions between kg, eV, and atomic mass units.
This calculator provides instant computation for any particle with built-in databases, scattering angle tables, and length scale comparisons. It is useful for physics students, particle physics researchers, and anyone studying quantum mechanics or Compton scattering.
λ_C = h/(mc). Reduced: ƛ_C = ℏ/(mc) = λ_C/(2π). Rest energy: E = mc². Compton scattering: Δλ = λ_C × (1 − cos θ). Compton frequency: f = mc²/h.
Result: 2.4263 × 10⁻¹² m (2.4263 pm)
For the electron (m = 9.109 × 10⁻³¹ kg): λ_C = 6.626×10⁻³⁴ / (9.109×10⁻³¹ × 2.998×10⁸) = 2.4263 × 10⁻¹² m. The rest energy is 0.511 MeV. At 90° scattering, Δλ = λ_C = 2.4263 pm.
Arthur Compton's 1923 experiment scattered X-rays off graphite and measured the wavelength shift of the scattered photons. Classical wave theory predicted no wavelength change — the electron should re-radiate at the same frequency. Instead, Compton found a shift proportional to (1 − cos θ), exactly matching the prediction from treating the photon as a particle with momentum p = h/λ.
This was powerful evidence for the particle nature of light and earned Compton the 1927 Nobel Prize. The shift formula Δλ = (h/mc)(1 − cos θ) contains the electron Compton wavelength as its natural unit of measurement.
Three fundamental electromagnetic length scales characterize the electron: the Bohr radius a₀ = ℏ/(αmc) ≈ 53 pm, the Compton wavelength λ_C = h/(mc) ≈ 2.4 pm, and the classical electron radius r_e = α²a₀ ≈ 2.8 fm. These are related by powers of α ≈ 1/137: r_e = αƛ_C = α²a₀.
The Bohr radius sets the scale of atoms. The Compton wavelength sets the scale where pair creation and relativistic quantum effects become important. The classical electron radius sets the scale of Thomson scattering.
In quantum field theory, the Compton wavelength marks the boundary between quantum mechanics and quantum field theory. Attempting to confine a particle within its Compton wavelength gives it enough energy (by the uncertainty principle) to produce new particle-antiparticle pairs. This is why single-particle quantum mechanics breaks down at this scale.
The concept extends to the gravitational Compton wavelength, where the Schwarzschild radius equals the Compton wavelength at the Planck mass (~22 µg), connecting quantum mechanics and general relativity at the Planck scale.
The Compton wavelength is the wavelength where quantum effects become dominant for a particle. A photon with this wavelength has energy equal to the particle rest mass (E = mc²). It sets the scale at which pair creation becomes possible.
The reduced Compton wavelength ƛ = ℏ/(mc) = λ_C/(2π) appears in the Dirac equation and in the Schwarzschild radius formula. It is the quantum analog of the gravitational radius in general relativity.
λ_C = h/(mc), so heavier particles have shorter Compton wavelengths. The proton is 1836× heavier than the electron, so its Compton wavelength is 1836× shorter.
When a photon collides with an electron, it transfers momentum and the photon wavelength increases by Δλ = λ_C(1 − cos θ). At 90°, the shift equals exactly the Compton wavelength. At 180° (backscatter), the shift is 2λ_C.
Attempting to localize a particle to within its Compton wavelength requires photons energetic enough to create new particles. This connects to the Heisenberg uncertainty principle and is why quantum field theory (not just quantum mechanics) is needed at these scales.
The Compton scattering shift is directly measurable with X-rays. Compton scattering of gamma rays is a major interaction mechanism in medical imaging (CT scanners) and radiation physics.