Calculation and evaluation of narcissus for diffractive surfaces in infrared systems

Tao Liu; Qingfeng Cui; Changxi Xue; Liangliang Yang

doi:10.1364/AO.50.002484

Applied Optics
Vol. 50,
Issue 16,
pp. 2484-2492
(2011)
•https://doi.org/10.1364/AO.50.002484

Calculation and evaluation of narcissus for diffractive surfaces in infrared systems

Tao Liu, Qingfeng Cui, Changxi Xue, and Liangliang Yang

Not Accessible

Your library or personal account may give you access

Get PDF
Email
Share
Get Citation
Copy Citation Text
Tao Liu, Qingfeng Cui, Changxi Xue, and Liangliang Yang, "Calculation and evaluation of narcissus for diffractive surfaces in infrared systems," Appl. Opt. 50, 2484-2492 (2011)

Export Citation
- BibTex
- Endnote (RIS)
- HTML
- Plain Text
Citation alert
Save article

Related Topics
Table of Contents Category
- Optical Design and Fabrication
Optics & Photonics Topics
?

The topics in this list come from the Optics and Photonics Topics applied to this article.

About this Article
History
- Original Manuscript: December 6, 2010
- Revised Manuscript: February 24, 2011
- Manuscript Accepted: February 26, 2011
- Published: May 27, 2011

Abstract

In infrared optical systems, the narcissus effect for diffractive surfaces should be calculated with specific diffraction orders based on the diffraction efficiency. It is shown in this work that the diffraction order of maximum diffraction efficiency varies with the change of the incident angle and wavelength of the backward-traced narcissus flux. Meanwhile, $y n i$ , which is the paraxial evaluation criterion of narcissus intensity for a refractive surface, is modified considering diffraction when a ray passes through diffractive surfaces, and a practical example has been given. The analysis can be used to calculate and control the narcissus intensity in infrared optical systems with diffractive surfaces.

Full Article | PDF Article

More Like This

Evaluation of narcissus for multilayer diffractive optical elements in IR systems

Tao Liu, Qingfeng Cui, Liangliang Yang, Changxi Xue, and Jian Sun
Appl. Opt. 50(33) 6146-6152 (2011)

Simulation and control of narcissus phenomenon using nonsequential ray tracing. I. Staring camera in 3-5 μm waveband

M. Nadeem Akram
Appl. Opt. 49(6) 964-975 (2010)

Accurate and fast narcissus calculation based on sequential ray trace

Yang Liu, Xiaobing Zhong, Ning Zhong, Changsheng Zheng, and Lizhan Wen
Appl. Opt. 52(33) 7899-7903 (2013)

Cited By

You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Figures (7)

You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Tables (8)

You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Equations (44)

You do not have subscription access to this journal. Equations are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

	Diffraction Order for Back Diffractive Surface				Diffraction Order for Front Diffractive Surface
Incident Angles	$- 1$	0	1	2	0	1	2	3
$0 °$	0.685	0.171	0.027	0.011	0.011	0.027	0.171	0.685
$20 °$	0.619	0.219	0.033	0.013	0.016	0.045	0.396	0.415
$40 °$	0.424	0.388	0.044	0.016	0.000	0.002	0.994	0.002
$60 °$	0.172	0.683	0.043	0.014	0.043	0.683	0.172	0.028
$80 °$	0.017	0.957	0.010	0.003	0.467	0.347	0.042	0.016

Entrance pupil diameter	$47 mm$
Cold stop diameter	$7.5 mm$
System focal length	$127 mm$
FPA dimensions	$9.84 mm \times 7.38 mm$
FPA pixel pitch	$30 μm \times 30 μm$
Cold stop $f #$	2.75

No.	Type	Radius	Thickness	Glass
0	Standard	Infinity	Infinity	Air
1	Standard	125.1762	8	ZnSe
2	Binary 2	864.4047	120	Air
3	Standard	$- 22.59946$	6	Germanium
4	Standard	$- 24.61636$	17	Air
5	Standard	37.60503	6	Germanium
6	Standard	50.25131	1	Air
7	Binary 2	19.43353	7	ZnSe
8	Standard	14.76969	9.319	Air
9	Standard	Infinity	2.5	Germanium
10	Standard	Infinity	3	—
Stop	Standard	Infinity	20	—
Image	Standard	Infinity	—	—

No.	Type	$α_{1}$	$α_{2}$
2	Binary 2	$- 3.549789 \times 10^{- 6}$	$8.861466 \times 10^{- 8}$
7	Binary 2	$1.206406 \times 10^{- 3}$	$- 1.610080 \times 10^{- 7}$

No.	Type	$R_{Norm}$	$A_{1}$	$A_{2}$
2	Binary 2	100	$- 1394.3655$	1318.0636
7	Binary 2	100	$- 1898.1135$	$- 46898.928$

No.	Type	$a_{1}$	$a_{2}$	$a_{3}$
2	Diffractive surface	$- 2.2192 \times 10^{- 4}$	$2.0978 \times 10^{- 8}$	$- 1.1933 \times 10^{- 11}$
7	Diffractive surface	$- 3.0209 \times 10^{- 4}$	$- 7.4642 \times 10^{- 7}$	$2.3420 \times 10^{- 9}$

Diffraction Efficiency	Diffraction Order for Back Diffractive Surface of The First Lens				Diffraction Order for Front Diffractive Surface of The Fourth Lens
Diffraction Efficiency	$- 3$	$- 2$	$- 1$	0	2	3	4	5
$η_{m^{'}}$	0.039	0.295	0.525	0.047	0.047	0.525	0.295	0.039

No.	Type	$y n_{F} i_{F}$	y	$y n_{F} i_{F} + N_{D}$	$N_{D}$
1	Refractive	4.435	23.561	—	—
2	Diffractive	$- 4.572$	22.681	$- 4.896$	$- 0.324$
3	Refractive	$- 0.133$	$- 5.892$	—	—
4	Refractive	$- 1.381$	$- 7.423$	—	—
5	Refractive	3.427	$- 9.387$	—	—
6	Refractive	0.319	$- 8.436$	—	—
7	Diffractive	2.470	$- 8.306$	2.496	0.026
8	Refractive	1.379	$- 6.082$	—	—

Abstract

Cited By

Figures (7)

Tables (8)

Equations (44)

Applied Optics