Estimate plasma wavelength precisely using density, units, and optional relativistic correction controls. View frequency, period, and wake scale, then export results as files fast.
c, e, ε₀, mₑ.
Relativistic correction applied as ωₚ → ωₚ / √γ.
The electron plasma angular frequency is:
ωₚ = √( nₑ e² / (ε₀ mₑ) )
With an optional relativistic factor γ, the effective frequency is:
ωₚ,eff = ωₚ / √γ
The plasma wavelength follows from the phase relation:
λₚ = 2π c / ωₚ,eff (equivalently, λₚ = c / fₚ where fₚ = ωₚ,eff / 2π).
| nₑ (cm⁻³) | λₚ (µm) | fₚ (THz) | Notes |
|---|---|---|---|
| 1×10¹⁶ | 333.894 | 0.8979 | Low-density plasma, longer wake scale. |
| 1×10¹⁷ | 105.587 | 2.839 | Intermediate density, common beam-plasma studies. |
| 1×10¹⁸ | 33.389 | 8.979 | Laser-wakefield scale in many setups. |
| 1×10¹⁹ | 10.559 | 28.39 | High-density regime, short wavelength. |
| 1×10²⁰ | 3.339 | 89.79 | Very high density, extremely short scale. |
The plasma wavelength λₚ sets the natural longitudinal scale of collective electron oscillations. In beam-driven and laser-driven wakefields, it approximates the distance between successive accelerating and decelerating buckets.
Because ωₚ ∝ √nₑ, the wavelength scales as λₚ ∝ 1/√nₑ. Increasing density by 100× reduces λₚ by 10×. This square-root law is central when matching driver duration to the plasma response.
The plasma frequency fₚ sets characteristic timescales for oscillations and phase slippage. The plasma period Tₚ can be used to estimate synchronization tolerances for injection, modulation, or diagnostics that resolve femtosecond dynamics.
In strongly relativistic electron motion, the effective inertia increases, reducing the oscillation rate. A simple model applies ωₚ,eff = ωₚ/√γ, increasing λₚ by √γ. Use γ = 1 when unsure.
Laboratory literature often states density in cm⁻³, while simulations typically use SI m⁻³. This calculator converts internally to SI before computing ωₚ and λₚ, then reports practical units like µm and THz.
For wakefield accelerators, driver duration and spot size are commonly chosen relative to λₚ. A driver too long can wash out the wake, while a properly matched driver enhances the accelerating gradient and reduces energy spread.
Interferometry, Thomson scattering, and coherent transition radiation often tie directly to density and hence λₚ. Knowing λₚ helps interpret modulation wavelengths and choose detector bandwidths for plasma waves.
Start with a target λₚ for your application, back-calculate a density range, then iterate with γ if relativistic effects are expected. Exporting CSV/PDF makes it easy to document runs and share assumptions.
Use the free electron density nₑ. In a quasi-neutral plasma, nₑ is close to ion density, but the electron density controls ωₚ and λₚ.
It sets the spacing of accelerating buckets and guides matching of driver pulse length. A driver tuned to λₚ can excite stronger wakes with better phase stability.
Adjust γ if electron motion is highly relativistic and you want a first-order correction. If you are not modeling relativistic plasma oscillations, keep γ = 1.
ωₚ is angular frequency in rad/s, while fₚ is cycles per second in Hz. They relate by fₚ = ωₚ / (2π).
In this cold-plasma model, temperature is neglected. Temperature influences damping and Debye length, but λₚ is primarily set by density in many regimes.
Yes. The conversion uses 1 cm⁻³ = 10⁶ m⁻³. The calculator converts to SI internally, then reports results in m, mm, µm, and nm.
This tool targets electron plasma oscillations. For ion plasma frequency, replace mₑ with ion mass and use the relevant charge state; results will differ significantly.
Accurate plasma scales help design experiments and diagnostics safely.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.