Optimizing performance parameters for switchable polymer dispersed liquid crystal optical elements

• US 7,570,405 B1
• Filed: 04/07/2006
• Issued: 08/04/2009
• Est. Priority Date: 04/08/2003
• Status: Active Grant

• Current Assignee: Leidos, Inc. (Leidos Holdings, Inc.)
• Original Assignee: Science Applications International Corporation
• Inventors: Siwecki, Stephen A., Tondiglia, Vince P., Sutherland, Richard L.
• Primary Examiner(s): AMARI, ALESSANDRO V
• Application Number:
  US11/399,519
• Time in Patent Office: 1,215 Days
• Field of Search: 359/15, 359/246, 359/484, 359/573, 349/201
• US Class Current: 359/15
• CPC Class Codes: G02B 5/32 Holograms used as optical elements
• CPC Class Codes: G02F 1/13342 Holographic polymer dispersed liquid crystals
• CPC Class Codes: G03H 1/22 Processes or apparatus for obtaining an optical image from holograms G03H1/26 - G03H1/34 take precedence
• CPC Class Codes: G03H 2250/38 Liquid crystal

Abstract

Described herein are the materials, mechanisms and procedures for optimizing various performance parameters of HPDLC optical devices in order to meet differing performance requirements. These optimization tailoring techniques include control and independent optimization of switchable HPDLC optical devices to meet the demanding requirements of anticipated applications for, inter alia, the telecommunications and display industries. These techniques include optimization of diffraction efficiency, i.e., index modulation, polarization dependence control, haze, cosmetic quality, control of response and relaxation time, voltage driving for on and off switching, and material uniformity. This control and independent optimization tailors properties of switchable HPDLC optical devices according to the specific requirements of the application of the switchable HPDLC optical device. The invention disclosed herein retains the desirable attributes of the multi-functional acrylate system for forming HPDLC optical devices, but adds new materials to the acrylate system and/or new process control to the recording to optimize performance parameters as may be needed for specific applications. This results in high optical quality switchable holograms with good diffraction efficiency and low, stable switching voltage.

Claims

1. A method for switching a holographic diffraction grating via a switching field between a first diffraction efficiency and a second diffraction efficiency comprising:

orienting the holographic diffraction grating such that an internal angle of p-polarized light incident thereon satisfies the following condition for a switching field of zero,

$\tan <br><br><br><br>{\mathrm{\theta <br><br>}}_{\mathrm{\rho <br><br>}}={\left(\frac{{\mathrm{\varepsilon <br><br>}}_{x<br><br><br><br>x}^{\left(1\right)}}{{\mathrm{\varepsilon <br><br>}}_{z<br><br><br><br>z}^{\left(1\right)}}\right)}^{1/2}$

wherein θ

_ρ

is the angle of incidence of a reference wave of the incident light and ε

_xx⁽¹⁾ and ε

_zz⁽¹⁾ are the x and z components of the modulation of the dielectric tensor for a material comprising the holographic diffraction grating and the holographic diffraction grating has a first diffraction efficiency; and

applying a switching field greater than zero in order to switch the holographic diffraction grating to a second diffraction efficiency.

2. The method according to claim 1, wherein the first diffraction efficiency is approximately zero and the second diffraction efficiency is greater than zero.

3. The method according to claim 1, wherein when a field is applied, ε

_xx⁽¹⁾ increases while δ

_zz⁽¹⁾ decreases.

4. The method according to claim 1, wherein the grating is turned on for p-polarized light when the applied field strength is approximately equal to the critical field strength for switching.

5. The method according to claim 1, wherein the grating is turned off for s-polarized light when the applied field strength is approximately equal to the critical field strength for switching.

6. The method according to claim 1, wherein the grating is an inverse mode grating.

7. The method according to claim 6, wherein the inverse mode grating comprises:

at least a first and a second electrode for applying a switching field to the switchable grating in order to vary a diffraction efficiency thereof, wherein the application of the switching field increases the diffraction efficiency of the grating and removal of the switching field decreases the diffraction efficiency of the grating.

8. The method according to claim 7, further comprising a light signal having a p-polarization component and an s-polarization component, wherein the light signal is incident upon the grating at an incident angle greater than zero.

9. The method according to claim 8, wherein the application of the switching field to the grating decreases the diffraction efficiency of the p-polarization component of the incident light signal.

10. A method for switching an inverse mode holographic polymer dispersed liquid crystal grating, the method comprising the steps of:

orienting a holographic diffraction grating so that an internal incident angle of p-polarized light at zero field satisfies

$\tan <br><br><br><br>{\mathrm{\theta <br><br>}}_{\mathrm{\rho <br><br>}}={\left(\frac{{\mathrm{\varepsilon <br><br>}}_{x<br><br><br><br>x}^{\left(1\right)}}{{\mathrm{\varepsilon <br><br>}}_{z<br><br><br><br>z}^{\left(1\right)}}\right)}^{1/2}$

wherein θ

_ρ

is the angle of incidence of a reference wave of the incident light and ε

_xx⁽¹⁾ and ε

_zz⁽¹⁾ are the x and z components of the modulation of the dielectric tensor for a material comprising the holographic diffraction grating.

11. The method according to claim 10, further comprising the step of applying a switching field greater than zero in order to switch the holographic diffraction grating from a first diffraction efficiency to a second diffraction efficiency.

12. The method according to claim 11, wherein the second diffraction efficiency is greater than zero.

13. The method according to claim 10, wherein a diffraction efficiency of the holographic diffraction grating is approximately zero.

14. The method according to claim 10, wherein the grating is turned on for p-polarized light when a strength of the field that is applied is approximately equal to the critical field strength for switching.

15. The method according to claim 10, wherein the grating is turned off for s-polarized light when a strength of the field that is applied is approximately equal to the critical field strength for switching.

16. The method according to claim 10, wherein the inverse mode grating comprises:

at least a first and a second electrode for applying a switching field to the grating in order to vary a diffraction efficiency thereof, wherein the application of the switching field increases the diffraction efficiency of the grating and removal of the switching field decreases the diffraction efficiency of the grating.

17. The method according to claim 16, further comprising a light signal having a p-polarization component and an s-polarization component, wherein the light signal is incident upon the grating at an incident angle greater than zero.

18. The method according to claim 17, wherein the application of the switching field to the grating increases the diffraction efficiency of the p-polarization component of the incident light signal.

19. The method according to claim 16, wherein the grating is a reflection grating.

20. A method for switching an inverse mode holographic polymer dispersed liquid crystal grating, the method comprising the steps of:

orienting a holographic diffraction grating so that an internal incident angle of p-polarized light at zero field satisfies

$\tan <br><br><br><br>{\mathrm{\theta <br><br>}}_{\mathrm{\rho <br><br>}}={\left(\frac{{\mathrm{\varepsilon <br><br>}}_{x<br><br><br><br>x}^{\left(1\right)}}{{\mathrm{\varepsilon <br><br>}}_{z<br><br><br><br>z}^{\left(1\right)}}\right)}^{1/2}$

wherein θ

_ρ

is the angle of incidence of a reference wave of the incident light and δ

_xx⁽¹⁾ land ε

_zz⁽¹⁾ are the x and z components of the modulation of the dielectric tensor for a material comprising the holographic diffraction grating, wherein when a field is applied, ∈

_xx⁽¹⁾ increases while ∈

_zz⁽¹⁾ decreases.