Tunable liquid crystal optical device

• US 9,904,086 B2
• Filed: 12/17/2014
• Issued: 02/27/2018
• Est. Priority Date: 05/05/2014
• Status: Active Grant

• Current Assignee: LensVector, Inc.
• Original Assignee: LensVector, Inc.
• Inventors: Galstian, Tigran, Viens, Jean-Franois, Tork, Amir
• Primary Examiner(s): Glick, Edward
• Assistant Examiner(s): Liu, Shan
• Application Number:
  US15/128,894
• Publication Number:
  US 20170160600A1
• Time in Patent Office: 1,168 Days
• Field of Search: 349138, 349 43, 349 52, 349123, 349 33, 349 34, 349200, 349 57, 349 15, 349 95, 349201, 349202
• CPC Class Codes: G02B 3/14 of variable focal length
• CPC Class Codes: G02F 1/13306 Circuit arrangements or driving methods for the control of single liquid crystal cells G02F1/132, G02F1/133382 take precedence
• CPC Class Codes: G02F 1/133345 Insulating layers G02F1/1335, G02F1/1337, G02F1/135, G02F1/136 take precedence
• CPC Class Codes: G02F 1/1337 Surface-induced orientation of the liquid crystal molecules, e.g. by alignment layers
• CPC Class Codes: G02F 1/1341 Filling or closing of cells
• CPC Class Codes: G02F 1/134309 characterised by their geometrical arrangement
• CPC Class Codes: G02F 1/137 characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering

Abstract

A variable liquid crystal optical device for controlling the propagation of light has one or more transparent thin-film highly-resistive layer (HRL) coupled to a substrate and an electrode structure. The HRL has core layer and a cover or proximity layer, wherein the core layer material has a higher electrical conductivity and higher refractive index than the cover layer material; and wherein the core and cover layer materials have substantially the same free energies of formation of oxide. In this way, the electrode structure will be environmentally stable and responsive to an applied electrical current to generate a spatially non-uniform magnetic field.

Claims

1. A gradient-index liquid crystal optical device comprising:

transparent substrates defining a gap between inner sides of the substrates;

a liquid crystal material filling the gap;

an alignment layer covering said substrates for orienting the liquid crystal material;

electrodes supported by the inner sides of the substrates and structured to create a spatially non-uniform electric field in the gap;

a highly resistive layer having a core weakly conductive material with an index of refraction higher than an index of refraction of the substrates and encapsulated by layers of a proximity material having insulating properties and an index of refraction between the index of refraction of the core weakly conductive material and the index of refraction of the substrates, the proximity material having substantially a same free energy of formation of oxide as the core weakly conductive material;

wherein said core weakly conductive material comprises titanium oxide, and said proximity material comprises a layer of Ta₂O₅ on each side of the core weakly conductive material and a layer of Al₂O₃ on a side of the layer of Ta₂O₅ opposite to the core weakly conductive material.

2. The device as defined in claim 1, wherein said device comprises two said gaps filled with said liquid crystal material, said alignment layer covering said substrates so as to provide orthogonal orientations of said liquid crystal materials in said two gaps, said device being configured to act on both linear polarizations of light.

3. The device as defined in claim 1, further comprising drive circuitry connected to said electrodes and configured to provide a variable electrical signal to said electrodes to control an optical state of said device.

4. The device as defined in claim 3, wherein said drive circuitry is configured to define said variable electrical signal as a function of a desired optical state value, and to use one of:

an initial and factory setting characterizing a resistance value of said highly resistive layer as a function of ambient temperature only without variation due to oxidation changes of the core weakly conductive material when determining said variable electrical signal as a function of said desired optical state value.

5. The device as defined in claim 1, wherein said device is a variable optical power lens.

6. The device as defined in claim 1, wherein said device is a variable optical axis position lens.

7. A method of manufacturing a gradient-index liquid crystal optical device, the method comprising:

providing transparent substrates;

depositing on a first one of said substrates;

at least one electrode structured to create a spatially non-uniform electric field between the substrates; and

a plurality of layers forming a highly resistive layer having a core weakly conductive material with an index of refraction higher than an index of refraction of the substrates and encapsulated by layers of a proximity material having insulating properties and an index of refraction between the index of refraction of the core weakly conductive material and the index of refraction of the substrates, the proximity material having substantially a same free energy of formation of oxide as the core weakly conductive material,

wherein said plurality of layers are deposited first onto said first one of said substrates, or at least one of said at least one electrode is deposited first onto said first one of said substrate;

depositing at least one electrode on a second one of said substrates;

providing an alignment layer covering said substrates for orienting the liquid crystal material;

providing at least one cell wall on said substrates;

depositing a liquid crystal material on one of said substrates in said cell wall;

covering said one of said substrates with said second one of said substrates to enclose said liquid crystal material within said cell wall; and

bonding said substrates together;

wherein said core weakly conductive material comprises titanium oxide, and said proximity material comprises a layer of Ta₂O₅ on each side of the core weakly conductive material and a layer of Al₂O₃ on a side of the layer of Ta₂O₅ opposite to the core weakly conductive material.

8. The method of manufacturing a gradient-index liquid crystal optical device as defined in claim 7, wherein said transparent substrates are prepared for an array of devices to be manufactured by wafer-scale fabrication, wherein an array of said cell walls are provided on said substrates, said depositing of said liquid crystal material is performed for each one of bottom barriers, and further comprising singulating individual devices from a resulting wafer comprising said substrates.

9. The method of manufacturing a gradient-index liquid crystal optical device as claimed in claim 7, wherein said devices each comprise two liquid crystal cells, wherein a first one of said cells has liquid crystal oriented in a first linear direction, and a second one of said cells has liquid crystal oriented in a second linear direction orthogonal to said first linear direction, said device acting on both linear polarizations of light.