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PERCENT REFLECTANCE PER SURFACE<br />

2.0<br />

1.8<br />

1.6<br />

1.4<br />

1.2<br />

1.0<br />

.8<br />

.6<br />

.4<br />

.2<br />

Figure 5.12 Reflectance at surface of substrate with<br />

index n g when coated with a quarter wavelength of<br />

magnesium fluoride (index n=1.38)<br />

air or vacuum index n 1<br />

wavelength l 1<br />

MgF 2 antireflection<br />

coating index n 2<br />

fused silica<br />

glass or silica substrate<br />

index n 3<br />

BK7<br />

optical path difference = 2n 2 b–n 1 a<br />

v 1<br />

a<br />

b v 2<br />

v 3<br />

SF11<br />

LaSFN9<br />

1.4 1.5 1.6 1.7 1.8 1.9<br />

REFRACTIVE INDEX (n g )<br />

Figure 5.13 Reflectance at oblique incidence<br />

Corresponding to the angle of incidence v 1d is an angle of<br />

refraction in the film:<br />

v<br />

As v 1 is reduced from v 1d to zero, the reflectance extremum shifts<br />

in wavelength from l d to l n , where the subscript n denotes normal<br />

incidence.<br />

This wavelength is given by the equation<br />

l<br />

2d<br />

n<br />

⎛ v1d<br />

= arcsin sin ⎞<br />

⎜ .<br />

⎝ n ( l )<br />

⎟<br />

⎠<br />

2 d<br />

⎛ n 2 ( ln)<br />

⎞ ⎛ ld<br />

= ⎜<br />

⎝ n ( l )<br />

⎟ ⎜<br />

⎠ ⎝ cos v<br />

2 d<br />

2d<br />

⎞<br />

⎟ .<br />

⎠<br />

b<br />

h<br />

(5.13)<br />

(5.14)<br />

Corresponding to the arbitrary angle of incidence v 1 and<br />

arbitrary wavelength l 1 are angles of refraction in the coating and<br />

substrate, given by<br />

v<br />

and<br />

v<br />

2<br />

3<br />

⎛<br />

1 l1 v1<br />

= arcsin n ( ) sin ⎞<br />

⎜<br />

⎝ n ( l )<br />

⎟<br />

⎠<br />

2 1<br />

⎛<br />

1 l1 v1<br />

= arcsin n ( ) sin ⎞<br />

⎜<br />

⎝ n ( l )<br />

⎟<br />

⎠ .<br />

3 1<br />

Following are formulas for the single-interface amplitude<br />

reflectances for both the p- and s-polarizations:<br />

r =<br />

12p<br />

r =<br />

23p<br />

r =<br />

12s<br />

r =<br />

23s<br />

n cos v 4n cos v<br />

n cos v + n cos v<br />

2 1 1 2<br />

2 1 1 2<br />

n cos v<br />

n cos v<br />

4n cos v<br />

+ n cos v<br />

3 2 2 3<br />

3 2 2 3<br />

n cos v 4n cos v<br />

n cos v + n cos v<br />

1 1 2 2<br />

1 1 2 2<br />

n cos v<br />

n cos v<br />

4n cos v<br />

2 2 3 3<br />

2 2<br />

+ n cos v<br />

3 3<br />

The subscript “12p,” for example, means that the formula gives the<br />

amplitude reflectance for the p-polarization at the interface between<br />

the first and second media.<br />

The corresponding irradiance reflectances for the coated surface,<br />

accounting for both interferences and the phase differences between<br />

the reflected waves, are given by<br />

and<br />

R =<br />

p<br />

R =<br />

s<br />

2<br />

2<br />

r 12p + r 23p + 2r12pr 23p cos (2 b )<br />

2 2<br />

1 + r r + 2r r cos (2 b )<br />

2<br />

12p 23p<br />

2<br />

12p 23p<br />

r 12s + r 23s + 2r12sr 23s cos (2 b )<br />

2 2<br />

1 + r r + 2r r cos (2 b )<br />

12s 23s<br />

12s 23s<br />

where b is the phase difference (in the external medium) between<br />

waves reflected from the first and second surfaces of the coating.<br />

p<br />

b = 2 n 2 ( l1<br />

) h cos v2<br />

.<br />

l<br />

1<br />

The cosines must be in radians. The average reflectance is given by<br />

R = 1 2 (R p + R s ) .<br />

.<br />

(5.15)<br />

(5.16)<br />

(5.17)<br />

(5.18)<br />

(5.19)<br />

(5.20)<br />

(5.21)<br />

(5.22)<br />

(5.23)<br />

(5.24)<br />

With these formulas, reflectance curves can be calculated as functions<br />

of either wavelength l 1 or angle of incidence v 1 .<br />

Fundamental Optics Gaussian Beam Optics <strong>Optical</strong> Specifications Material Properties <strong>Optical</strong> <strong>Coatings</strong><br />

Visit Us Online! www.mellesgriot.com 1 5.11

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