To demonstrate a new feature in TFCalc 3.2, we design sunglasses using two dielectric materials. For these sunglasses, we have the following requirements at normal incidence:
1 f- [0 [+ c9 \A. Transmittance Do continuous targets lead to better designs? In general, the answer is Yes. The graph below shows the performance of a coating designed using discrete targets every 10 nm (shown as circles). There are clearly two "leaks" (where the performance is not controlled between discrete targets) near 450 nm and another small leak at 515 nm.
6 V* l$ v' k: v
- n1 A2 C" I( }; d3 ] Here is the design, with the first layer closest to the substrate and thickness given in nm.
7 F6 P: \; a) g- e1 ?/ w, r TiO2 69.95
2 J4 O" p. |' ~4 q5 m SiO2 32.82& M8 ~( `* x6 v) O+ [, B$ `- @
TiO2 32.68$ o6 D* N" B1 ~9 u
SiO2 111.15
1 K2 V, q4 b1 ]( H( u TiO2 106.07! W. X" X/ V' F% h
SiO2 93.12
+ K( `- x% e7 {8 c) \4 C9 ~! c' N3 A TiO2 28.137 g* t) T5 G5 r
SiO2 69.00; B* U! p6 G+ R6 ~ e! \
TiO2 57.755 v. v! m I2 {5 t2 m; A' L/ L
SiO2 172.278 \% A2 m, L, }7 R
TiO2 60.40
6 b4 c$ f! F( `5 | SiO2 94.82
- l+ y3 k$ I: H8 ~ TiO2 50.146 q' n( y1 [' F
SiO2 73.58
) e1 o3 k& o: S TiO2 44.78# H. U; M; E R2 p
SiO2 90.29 {# z, j5 h4 s5 z5 Q
TiO2 27.178 I1 x' _# W& \
SiO2 59.580 _$ y+ D0 F. \8 z i+ a
TiO2 62.56
1 g* P8 |' H# A3 W6 Z SiO2 113.669 `" X. B9 Y& V: {
TiO2 68.53
; ] P; X* P2 w! R# Y8 A! M SiO2 189.07, s a) G5 e. s3 b. e# A
TiO2 63.17$ d5 o5 t; s s- o+ y
SiO2 129.47' q: w/ t; M3 e$ a% i: a& S
TiO2 110.55
* p7 Y/ c$ {& @3 O( m" t" k SiO2 123.90
k" B. z, }4 C( `; P TiO2 73.899 j$ w) W. F3 A1 c
SiO2 32.414 T+ C9 m8 [- P! i: ?) i G
TiO2 21.12 |