Study emission and absorption signatures with confidence. Model Balmer, Lyman, Paschen, and custom transitions instantly. Visualize line behavior, compare results, and export polished reports.
Sample transitions for quick validation and educational reference.
| Label | Z | n₂ | n₁ | Series | Approx. Vacuum Wavelength (nm) | Region |
|---|---|---|---|---|---|---|
| Lyman-α | 1 | 2 | 1 | Lyman | 121.567 | Ultraviolet |
| Balmer-α (Hα) | 1 | 3 | 2 | Balmer | 656.280 | Visible Red |
| Balmer-β (Hβ) | 1 | 4 | 2 | Balmer | 486.133 | Visible Blue-Green |
| Paschen-α | 1 | 4 | 3 | Paschen | 1875.626 | Infrared |
| He⁺ 4→3 | 2 | 4 | 3 | Paschen-like | 468.906 | Visible Blue |
1) Rydberg relation for hydrogen-like ions:
1 / λ = R × Z² × (1 / n₁² − 1 / n₂²)
2) Frequency:
ν = c / λ
3) Photon energy:
E = hν = hc / λ
4) Wavenumber:
ṽ = 1 / λ
5) Redshift:
z = (λobs − λrest) / λrest
6) Non-relativistic radial velocity estimate:
v ≈ zc
7) Instrument resolution element:
Δλ = λ / R
8) Effective broadening:
FWHMeff = √(FWHMintrinsic² + Δλ²)
This calculator uses an ideal hydrogen-like one-electron approximation. It is excellent for teaching, quick checks, and many astrophysical estimates, but not a full multi-electron quantum treatment.
It calculates vacuum wavelength, observed wavelength, frequency, wavenumber, photon energy, transition energy gap, redshift, estimated radial velocity, and line broadening metrics for hydrogen-like transitions.
It is best for hydrogen and hydrogen-like ions with one electron, such as He⁺ or Li²⁺. Multi-electron atoms need more advanced structure models.
A spectral transition between bound states uses a higher initial level and a lower final level for emission. The Rydberg term becomes invalid if n₂ is not greater.
Rest wavelength comes from the ideal transition formula. Observed wavelength includes motion, redshift, and any calibration offset or directly measured line position you enter.
Use it when you already identified a line in experimental or telescope data. The calculator then derives redshift and velocity from that measured line position.
Resolving power determines the instrument’s wavelength discrimination. Higher values mean smaller resolution elements, sharper lines, and better ability to separate nearby transitions.
No. This version uses the common non-relativistic approximation v ≈ zc. It works well for modest speeds but becomes less accurate for very large redshifts.
The dry-air conversion is only applied in a practical wavelength range. Outside that range, vacuum values remain the safer and more standard reference.
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.