Tune transition strength and medium index instantly here. See I_sat, power, and saturation parameter quickly. Export results to files for lab notes and reports.
Representative values (illustrative). Results depend on convention and line strength.
| lambda0 (nm) | Gamma/2pi (MHz) | n | C | Factor | Isat (mW/cm^2) | w0 (um) | Psat (W) |
|---|---|---|---|---|---|---|---|
| 780.241 | 6.065 | 1.0000 | 1.00 | 1.0 | ~ 1.67 | 1000 | ~ 0.026 |
| 589.159 | 9.794 | 1.0000 | 1.00 | 1.0 | ~ 6.3 | 500 | ~ 0.025 |
Baseline saturation intensity for a two-level electric-dipole transition:
Isat = (pi * h * c * Gamma) / (3 * lambda^3)
Practical scaling used here:
Isat = Ibase * (convention factor) / (line strength C)
Saturation parameter and scattering rate (single beam):
s = I/Isat, Rsc = (Gamma/2) * s / (1 + s + (2*Delta/Gamma)^2)
Saturation intensity, Isat, marks the optical power density where a driven transition begins to respond nonlinearly. Below Isat, excitation scales almost linearly with intensity; above it, the excited-state population approaches a limit set by the natural decay rate. In laser cooling, fluorescence, and absorption spectroscopy, choosing I near Isat balances signal and power broadening.
The baseline model uses Isat = (π h c Γ) / (3 λ3), where Γ is the natural linewidth in rad/s and λ is the wavelength inside the medium. The tool supports entry as Γ/2π in MHz, then converts to angular units automatically.
Isat scales as Γ/λ3. Shorter wavelengths therefore raise Isat strongly. With a refractive index n, the calculator applies λ = λ0/n and c = c0/n, so Isat changes roughly with n2 for fixed λ0.
Real atoms have multiple Zeeman and hyperfine channels. A relative line strength C (< 1) increases the required intensity because the effective dipole coupling is weaker. A separate convention factor helps match common definitions in literature, for example cycling versus polarization-averaged cases.
For the Rb D2 line near 780.241 nm with Γ/2π ≈ 6.065 MHz, the two-level cycling convention gives Isat ≈ 1.67 mW/cm2. For Na D2 near 589.159 nm with Γ/2π ≈ 9.794 MHz, a typical value is around 6.3 mW/cm2. These numbers are included in the example table for quick checks.
Many labs control power rather than intensity. For a Gaussian beam, the peak intensity is I0 = 2P/(πw02), so Psat = Isatπw02/2. For a top-hat beam of radius r, Psat = Isatπr2.
The saturation parameter s = I/Isat feeds the standard scattering rate Rsc = (Γ/2) s /(1 + s + (2Δ/Γ)2). Increasing detuning reduces scattering while keeping intensity fixed, which is important for low-heating probing and optical pumping strategies.
This calculator is ideal for first-pass design and cross-checks. For dense vapors, strong fields, or near-resonant multi-level dynamics, additional effects may matter, including optical depth, radiation trapping, and coherent dark states. Use the convention factor and C to align with your specific transition model and measurement geometry.
It is the intensity where a transition begins to saturate: the excited-state population no longer rises linearly, and power broadening becomes significant. It provides a convenient normalization for laser-atom interaction strength.
Multi-level atoms rarely behave like a perfect two-level system. A smaller C represents weaker effective coupling, increasing the intensity required to reach the same saturation parameter under your polarization and selection rules.
Use the natural linewidth when you want a standard Isat reference. If your transition is broadened by collisions or power, a larger effective linewidth can be used for a rough operating-point estimate.
The formula depends on wavelength and light speed in the medium. Using λ = λ0/n and c = c0/n alters the scaling, which can matter in liquids, solids, or waveguide environments.
A common starting point is s between 0.5 and 2 on resonance, adjusted for detuning and heating constraints. The calculator reports s and Rsc so you can tune for signal versus broadening.
It is the laser power needed to reach Isat under the chosen beam model. For Gaussian beams it uses peak intensity at the waist; for top-hat beams it assumes uniform intensity across the radius.
It provides the basic single-beam scattering force estimate ℏkRsc. Accurate forces in experiments may require multi-beam geometry, polarization gradients, magnetic fields, and multi-level optical pumping effects.
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.