In fibre laser engineering, few parameters influence cutting, welding, and marking performance as much as beam propagation. And at the centre of that behaviour lies a key concept: Rayleigh length.
Rayleigh length tells us how far a beam stays tightly focused before diffraction causes significant expansion. In practical terms, it defines how stable and forgiving your laser process will be.
“A laser beam with a long attention span gives you fewer headaches.”
Fibre lasers naturally deliver high brightness and low divergence — ideal conditions for a longer Rayleigh length. This brings several advantages:
“A long Rayleigh length is your built-in safety margin.”
Most fibre laser datasheets specify far-field divergence rather than beam waist. Fortunately, we can calculate Rayleigh length directly from divergence.
For a Gaussian beam:
zR=λπθ2z_R = \frac{\lambda}{\pi \theta^2}
zR=4λπΘ2z_R = \frac{4\lambda}{\pi \Theta^2}
This is extremely practical when evaluating cutting heads, fibre delivery systems, and beam quality across different manufacturers.
“Never ignore the divergence figure — it’s the small number that decides the big picture.”
Rayleigh length becomes:zR≈0.61 mz_R \approx 0.61\, \text{m}
This means the beam remains near its minimum size for more than 60 cm, helping explain why single-mode fibre lasers excel in fine cutting, micro-welding and precision processing.
Understanding Rayleigh length is essential when:
“If your Rayleigh length is short, your process window becomes short-tempered.”
Using divergence angle to calculate Rayleigh length gives engineers a fast, reliable way to evaluate beam behaviour without directly measuring the waist. It’s a simple formula with significant impact on real-world fibre laser performance.
In short:Diffraction is unavoidable — but poor understanding of it is not.