Beamage-M² User Manual
Mathematically, it is given by the following equation:
Far from the beam waist, the beam expansion becomes linear and the theoretical divergence half-angle
(half of the angle shown in Figure 4-1) can be obtained by evaluating the limit of the beam radius's
ℎ
first derivative as the position tends towards infinity:
=
ℎ
For a laser beam that passes through a focusing lens of focal length f, the theoretical radius of the beam
at the focal spot of the lens can be obtained by multiplying the beam divergence half-angle with the
ℎ
focal length f:
As mentioned, all of the equations above describe theoretical ideal Gaussian beams. However, they can
describe the propagation of real laser beams if we modify them slightly using the M
mathematically defined by the following equations:
2
=
With mathematics, it is easy to understand why small M
divergences and small experimental beam waist radiuses.
The experimental beam waist radius
experimental beam radius at the focal spot of the lens
equations:
ℎ
( )
ℎ
=
→∞
→∞
ℎ
0
0
=
> 1
ℎ
0
ℎ
(), the experimental half-angle divergence
( ) =
0
ℎ
=
Revision 6
2
(
)
0
ℎ
=
√ 1 + (
0
ℎ
(
0
=
=
ℎ
0
ℎ
2
values correspond to low experimental
are therefore given by the following
2
2
√
+
(
(
0
ℎ
2
=
0
2
=
0
2
)
=
2
)
0
ℎ
ℎ
2
factor, which can be
>
=
0
ℎ
0
ℎ
2
)
2
)
14
, and the