US20140340762A1 - Electroactive Optical Device - Google Patents

Electroactive Optical Device Download PDF

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Publication number
US20140340762A1
US20140340762A1 US14/449,070 US201414449070A US2014340762A1 US 20140340762 A1 US20140340762 A1 US 20140340762A1 US 201414449070 A US201414449070 A US 201414449070A US 2014340762 A1 US2014340762 A1 US 2014340762A1
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electroactive
optical element
electrodes
optical device
optical
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US14/449,070
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Mark Blum
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Optotune AG
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Optotune AG
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B3/00Simple or compound lenses
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B3/00Simple or compound lenses
    • G02B3/12Fluid-filled or evacuated lenses
    • G02B3/14Fluid-filled or evacuated lenses of variable focal length
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B26/00Optical devices or arrangements for the control of light using movable or deformable optical elements
    • G02B26/004Optical devices or arrangements for the control of light using movable or deformable optical elements based on a displacement or a deformation of a fluid
    • G02B26/005Optical devices or arrangements for the control of light using movable or deformable optical elements based on a displacement or a deformation of a fluid based on electrowetting
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B7/00Mountings, adjusting means, or light-tight connections, for optical elements
    • G02B7/28Systems for automatic generation of focusing signals
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02NELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
    • H02N2/00Electric machines in general using piezoelectric effect, electrostriction or magnetostriction
    • H02N2/02Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing linear motion, e.g. actuators; Linear positioners ; Linear motors
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N30/00Piezoelectric or electrostrictive devices
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10TTECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
    • Y10T29/00Metal working
    • Y10T29/49Method of mechanical manufacture
    • Y10T29/49002Electrical device making
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10TTECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
    • Y10T29/00Metal working
    • Y10T29/49Method of mechanical manufacture
    • Y10T29/49002Electrical device making
    • Y10T29/49117Conductor or circuit manufacturing

Definitions

  • the invention relates to an electroactive optical device, in particular an electroactive lens, as well as to a method for manufacturing such a device.
  • An electroactive optical device is an optical device whose shape can be changed using the electroactive effect.
  • an electroactive optical lens is a lens whose focal length can be changed using the electroactive effect.
  • electroactive effect describes an electric-field induced deformation of a solid or liquid.
  • the deformation can be due to Coulomb forces between electrodes and/or due to the rearrangement of electrical ions and/or multipoles, in particular dipoles, in an electric field.
  • electroactive materials are: dielectric elastomers, electrostrictive relaxor ferroelectric polymers, piezoelectric polymers (PVDF), liquid crystal elastomers (thermal), ionic polymer-metal composites, mechano-chemical polymers/gels.
  • WO 2008/044937 describes a device where a circularly shaped piezoelectric crystal is bending a thin glass cover, thereby providing a shift of focal length of the lens assembly.
  • Devices based on piezoelectric crystals are, however, comparatively expensive to manufacture.
  • WO 2005/085930 relates to an adaptive optical element that can be configured e.g. as a biconvex lens.
  • the lens consists of a polymer actuator comprising an electroactive polymer layer and layer electrodes. Applying a voltage in the order of 10 kV or more leads to a deformation of the polymer layer, which, in turn, leads to a direct deformation of the lens. Due to the high voltage required to control this device, it is poorly suited for many applications.
  • the device comprises an elastic optical element as well as an electroactive element arranged laterally adjacent to the optical element.
  • the electroactive element comprises at least one electrode pair with an elastic electroactive material, advantageously a dielectric elastomer, arranged between the electrodes of the electrode pair.
  • an elastic electroactive material advantageously a dielectric elastomer
  • the axial distance between the electrodes of the electrode pair changes, i.e. it increases or decreases, thereby elastically varying the volume (i.e. the axial extension) of a first region in the optical element adjacent to the electrode pair.
  • This leads to a radial displacement of material in the optical element between said first region and a second region.
  • One of said regions elastically expands in axial direction, while the other elastically contracts.
  • the optical element In the absence of a voltage over the electrode pair, the optical element is in a mechanically relaxed state.
  • This design uses the advantages of an electroactive actuator, such as its potentially easy manufacturing process, large deformations and low actuation voltage, while providing a solution that has a long lifetime because, in the absence of a voltage, the device is in an elastically relaxed state and therefore is less prone to fatigue than devices where the device is formed by a pre-strained solid and is therefore under continuous strain.
  • the application of the voltage will lead to a decrease of the distance between the electrodes, which in turn will reduce the volume of said first region of the optical element.
  • the compressed electroactive material between the electrodes can exert a lateral pressure onto the optical element. The combination of both effects brings the optical element into a strongly deformed state.
  • the electroactive element comprises a plurality of electrode pairs stacked on top of each other, with gaps between the electrode pairs.
  • the gaps are advantageously filled by the electroactive material. This design allows to obtain a large volume displacement of material in the optical element using low drive voltages.
  • the method comprises the following steps:
  • this process allows to simultaneously form a plurality of the devices with common steps a), b) and c), which reduces manufacturing costs.
  • steps b) and c) are repeated in order to form a plurality of electrode pairs stacked on top of each other in order to manufacture devices that can be controlled with low voltages.
  • FIG. 1 is a sectional view of a lens without applied voltage
  • FIG. 2 is a top view of the lens of FIG. 1 ,
  • FIG. 3 is the lens of FIG. 1 with applied voltage
  • FIG. 4 is a first step in a manufacturing process
  • FIG. 5 is a second step in a manufacturing process
  • FIG. 6 is a third step in a manufacturing process
  • FIG. 7 is a fourth step in a manufacturing process
  • FIG. 8 is a fifth step in a manufacturing process
  • FIG. 9 shows a sectional view of an assembly of two lenses without applied voltage, with small applied voltage and with large applied voltage
  • FIG. 10 shows an assembly of four stacked lenses
  • FIG. 11 is a view of a lens with graded electrodes
  • FIG. 12 shows a top view of a beam deflector
  • FIG. 13 shows a sectional view of the beam deflector along line XIII of FIG. 12 in three different states
  • FIG. 14 shows a further embodiment of an optical device with a buffer layer
  • FIG. 15 shows a further embodiment of an optical device with a lid layer
  • FIG. 16 shows yet a further embodiment of an optical device with a lid layer and a buffer layer.
  • axial is generally used to designate a direction perpendicular to the surface of the center region of the optical element in its relaxed state. If a substrate is present, the substrate will in most cases be aligned perpendicularly to the axial direction.
  • radial is used to designate a direction perpendicular to the axial direction.
  • the present invention can be implemented in a variety of forms, e.g. as an electroactive lens, a beam deflector or an anti-jittering device. In the following, we describe some of these applications.
  • FIGS. 1 and 2 One possible embodiment of the present invention as an electroactive lens is shown in FIGS. 1 and 2 .
  • the lens comprises an elastic optical element 1 and an electroactive element 2 .
  • the optical element 1 is circular and the electroactive element 2 surrounds the optical element.
  • the present invention can also be implemented for non-circular lenses, e.g. cylindrical lenses, as long as electroactive element 2 is laterally adjacent to at least one side of optical element 1 .
  • Electroactive element 2 comprises at least two, advantageously more than two, vertically stacked electrodes 3 a - 3 e forming at least one electrode pair, advantageously several electrode pairs on top of each other.
  • the first, topmost electrode 3 a is, by means of a lead 9 a , electrically connected to a first section 4 a of a side wall, while the second, next electrode 3 b is connected to a second section 4 b of the side wall by means of a lead 9 b , the third electrode 3 c is again connected to first section 4 a by means of a lead 9 c , the fourth electrode 3 d to second section 4 b by means of a lead 9 d , etc, such that adjacent electrodes are connected to different sections of the side wall.
  • the side wall is electrically conducting and it is of a solid material, such as a conductive polymer.
  • An electroactive material 5 is located in the gaps between the electrodes 3 a - 3 e , i.e. all the gaps between the electrodes are filled by the electroactive material 5 .
  • An electroactive material is any material that, when a voltage is applied between neighboring electrodes, yields to the Maxwell stress caused by the Coulomb forces between the electrodes.
  • electroactive material 5 is a solid, such as a dielectric elastomer, or a gel.
  • Optical element 1 of the lens can be of the same material as electroactive material 5 —this simplifies the manufacturing process, as described below.
  • optical element 1 may also be of a material different from electroactive material 5 , which allows to optimize the physical properties of optical element 1 and electroactive element 2 independently.
  • Optical element 1 is a transparent elastic solid or a gel and, in the absence of a voltage applied to the electrodes 3 a - 3 e , it is in a mechanically relaxed state for the reasons mentioned above.
  • Optical element 1 is made from a single piece of material.
  • FIG. 3 The function of the lens of FIGS. 1 and 2 is shown in reference to FIG. 3 .
  • a non-zero voltage V is applied over all neighboring electrode pairs formed by the electrodes 3 a - 3 e .
  • the Coulomb forces between the electrodes and/or a rearrangement of multipoles within the material lead to a decrease or an increase of the axial distance between the electrodes, depending on the electro- active material that is used.
  • liquid crystal elastomers can be engineered to expand in the direction of an applied field, while most other materials will contract.
  • the thickness of the electroactive element 2 is decreased. Since the electroactive element 2 is laterally joined to the optical element 1 , a compressed first region is created in the optical element adjacent to the electrodes. This, in turn, leads to a radial displacement of material of the optical element 1 away from the compressed first region, typically towards the center of the optical element 1 . This, in turn, forms an axially expanding second region in the optical element due to the incompressibility of the material. In FIG. 3 , this axially expanding region is in the center of optical element 2 .
  • the thickness of the electroactive element 2 is increased, and the first region of the optical element 1 expands in axial direction, while the second region contracts.
  • the application of the voltage to the electrodes leads to a redistribution of material within optical element 1 , which in turn affects the curvature of its surface.
  • the optical element 1 becomes thinner in the regions adjacent to those electrodes where the voltage has been applied, while it becomes thicker elsewhere.
  • the deformation causes the surface to bulge outwards, thereby forming a convex lens surface, which affects the focal length of the lens formed by optical part 1 .
  • the present lens is not necessarily a circular lens. It may, as mentioned, e.g. also be cylindrical.
  • optical element 1 is formed by an elongate strip of transparent, elastic material, with at least one elongate electroactive element 2 arranged along at least one side thereof, such that electroactive element 2 can create a compressed or expanded first region in the optical element 1 adjacent to the electrodes, as mentioned above.
  • the lens advantageously comprises a solid, transparent substrate 7 , with the electroactive element 2 and the optical element 1 arranged thereon.
  • a substrate provides mechanical stability to the device and simplifies the manufacturing process as described below.
  • substrate 7 can also be dispensed with.
  • the distance between adjacent electrodes 3 a - 3 e should not be too large in order to obtain strong Coulomb forces even if the applied voltage is small.
  • the distance between two neighboring electrodes should be less than 250 ⁇ m, in particular approximately 10 ⁇ m, and it should be small enough to allow significant deformations at voltages below 1 kV.
  • the electrodes should be compliant, i.e. they should be able to follow the deformations of electroactive element 2 without being damaged.
  • the electrodes are therefore manufactured from one of the following materials:
  • the material for optical element 1 and the electroactive material 5 for electroactive element 2 can e.g. comprise or consist of:
  • FIG. 11 shows an advantageous embodiment where the electrodes 3 a - 3 e have increasingly larger inner diameter towards the surface of the device. In other words, at least the electrode 3 a closest to the top surface has a larger inner diameter than the next lower electrode.
  • top surface designates the surface of the lens that is deformed upon application of a voltage.
  • This design reduces the mechanical strain in the electroactive material 5 as well as in the material of the optical element 1 upon application of a voltage.
  • the inner diameter of at least one of the electrodes 3 a - 3 e can be different from the inner diameter of at least some of the other electrodes. This allows a more refined control of the deformation of optical element 1 .
  • a plurality of electroactive lenses is manufactured at the same time on a common wafer.
  • the common wafer may be pre-shaped e.g. to comprise fixed structures, such as rigid lenses, to be combined with the optical elements 2 .
  • the process starts (step a, FIG. 4 ) from substrate 7 , which originally has a size much larger than an individual lens.
  • the bottommost electrodes 3 e for a plurality of adjacent lenses are deposited on the substrates. Any suitable method can be used for manufacturing these electrodes, as long as it is compatible with the electrode material and the substrate, such as sputtering with subsequent masking and etching.
  • a layer 5 a of the electroactive material 5 is applied over substrate 7 .
  • the layer 5 a may e.g. have a thickness of 10 ⁇ m.
  • a plurality of second electrodes namely the electrodes 3 d , are applied over the layer 5 a of electroactive material.
  • the electrodes 3 d are in register with the electrodes 3 e , with one electrode 3 d attributed to each electrode 3 e.
  • step b is repeated, i.e. a further layer 5 b of the electroactive material is applied as shown in FIG. 6 , whereupon step c is repeated, etc., until a stacked structure of sufficient height with a plurality of stacked electrode pairs on top of each other is manufactured, as shown in FIG. 7 .
  • the walls 4 a , 4 b which have been prefabricated and are e.g. applied to a common carrier (not shown), are pushed from above into the layer structure. Since the layers 5 a , 5 b , . . . are of a soft material, the walls 4 a , 4 b enter the layers as shown in FIG. 8 , whereupon the common carrier (not shown) of the walls can be removed.
  • the walls 4 a , 4 b are positioned such that they contact the electrodes 3 a - 3 e .
  • the electrodes 3 a - 3 e are provided with the leads 9 a - 9 e that laterally extend away from the center of the lens in order to provide a contact with the respective wall section 4 a or 4 b.
  • the product of the above steps is separated into a plurality of electroactive lenses by severing them between the walls of adjacent lenses, e.g. along lines 10 as shown in FIG. 8 .
  • a separation of the lenses can e.g. also be achieved by pushing the walls 4 a , 4 b not only through the electroactive material layers 5 a , 5 b . . . , but also through the substrate 7 .
  • the product shown in FIG. 7 can also be severed first, where-upon the walls 4 a , 4 b, or other means for providing a contact to the electrodes 3 a - 3 e , are applied individually to each lens.
  • step b the following methods can e.g. be used for applying the electroactive material layer 5 a , 5 b . . . :
  • the following materials can e.g. be used for the electroactive material as well as for the optical element:
  • step c the following methods can e.g. be used for applying the compliant electrodes 3 a - 3 d and, optionally, 3 e:
  • optical element 1 can be structured to have a desired shape in its relaxed and/or deformed states. Examples of such lenses are described below in reference to FIGS. 9 and 10 .
  • Suitable lens shapes in the relaxed state can e.g. be:
  • any of the following methods can e.g. be applied for shaping the lens:
  • FIGS. 4-8 e.g. methods c) and d) can take place on the product shown in FIG. 7 .
  • Some other methods will require additional steps.
  • an array of convex lenses on a common carrier can be manufactured by means of methods a), b), or e)-k) and then be applied on top of the product of FIG. 7 .
  • electroactive lenses of the type described above can be combined to form a multi-lens assembly.
  • FIG. 9 An example of such an assembly is shown in FIG. 9 , where two electroactive lenses 11 a , 11 b are mounted to opposite sides of a solid and transparent common substrate 7 .
  • lens 11 a has a flat surface while lens 11 b is concave.
  • lens 11 a can be manufactured e.g. as shown in FIGS. 4-8
  • the optical element of lens 11 b has e.g. subsequently been structured by using above methods c) or d).
  • lens 11 a becomes convex while lens 11 b remains concave, albeit with smaller curvature.
  • both lenses 11 a , 11 b become convex.
  • the present lens can also be combined to even more complex structures.
  • An example of such an assembly is shown in FIG. 10 .
  • the assembly of FIG. 10 comprises four electroactive lenses 11 a , 11 b , 11 c , 11 d as well as four rigid lenses 12 a , 12 b , 12 c , 12 d stacked on top of each other.
  • the walls 4 a , 4 b and additional spacer elements 13 a , 13 b are used to keep the lenses at a correct distance from each other.
  • each electroactive lens 11 a - 11 d is attached to one side of a substrate 7 , with a rigid lens 12 a - 12 d arranged at the opposite side of the same substrate.
  • each rigid lens is attached to a substrate 7 .
  • one or more of the rigid lenses may also be mounted independently of a substrate.
  • the shapes of the electro-active lenses 11 a , 11 b , 11 c , 11 d in the absence of a field can be defined using the structuring methods described above.
  • lenses should be spherical. To create approximately spherical lenses with the designs shown in FIGS. 1-10 , the total thickness of electroactive element 2 and the optical element 1 should be fairly large. Otherwise, in particular if the electroactive layer is bonded to substrate 7 , the deformation under applied voltage will be strong close to the electrodes but weak in the middle of the lens.
  • buffer layer 30 which is arranged between substrate 7 on the one hand and electroactive element 2 and optical element 1 on the other hand, allows the material of optical element 1 to displace more freely, in particular in horizontal direction, i.e. it insulates the optical element 1 from the mechanical constraints of the rigid substrate 7 . Therefore, advantageously, buffer layer 30 is of a comparatively soft material, i.e. it should have a Young's modulus smaller than or equal to the one of the optical element 1 .
  • Buffer layer 30 can be fully attached to substrate 7 as well as to optical element 1 , thereby connecting the two without restricting the motion of optical element 1 when a voltage is applied to the electrodes.
  • FIG. 15 Another measure to improve the surface shape of a spherical lens, i.e. to bring it closer to an ideal spherical lens, is shown in FIG. 15 .
  • a lid layer 31 has been attached to the top side of optical element 1 , i.e. to the side opposite substrate 7 .
  • Lid layer 31 is stiffer than optical element 1 , i.e. it has a Young's modulus larger than the one of optical element 1 .
  • the Young's modulus should be about 60 times larger than the one of optical element 1 . If the layer thickness is thinner, the Young's modulus has to increase to result in a good optical quality.
  • FIGS. 14 and 15 can be combined as shown in FIG. 16 , where the optical device comprises a buffer layer 30 as well as a lid layer 31 .
  • Suitable materials for buffer layer 30 and lid layer 31 are e.g. PDMS, acrylics or polyurethans.
  • the buffer layer has typically a Young's modulus in the range of 200 kPa or less and the lid layer has a Young's modulus of 10 MPa or more. These materials are advantageously combined with elastomer, acrylics and polyurethans for the electroactive material as well as for the lens element.
  • FIGS. 12 and 13 An example of a beam deflector or minor is shown in FIGS. 12 and 13 . It has basically the same set-up as the device of FIGS. 1-3 but the electrodes 3 a and 3 c are each split up into two electrode sections 3 a ′ and 3 a ′′ as well as 3 c ′ and 3 c ′′, each section extending around approximately 180° of optical element 1 . Accordingly, the wall has been split up into three sections 4 a , 4 b , 4 c , with section 4 a being connected to the electrode sections 3 a ′ and 3 c ′, section 4 b being connected to the electrode sections 3 a ′′ and 3 c ′′, and section 4 c being connected to the electrode sections 3 b and 3 d .
  • a voltage V1 can be applied between sections 4 a and 4 c , and a voltage V2 between sections 4 b and 4 c.
  • This type of device can be used as a beam deflector, either in transmission or reflection.
  • a beam extending through optical element 1 can either be deflected to the left or to the right, depending on V1 and V2, as shown by the arrows 21 .
  • At least one of the surfaces of optical element 1 can be provided with a minor element, such as a reflective coating 25 or a rigid reflective minor plate, and a beam can either be deflected to the right or left, respectively, as shown by the dotted arrows 22 .
  • a minor element such as a reflective coating 25 or a rigid reflective minor plate
  • the minor element can, as mentioned, e.g. be a mirror plate affixed to surface 20 , or it may be a coating, such as a liquid metal coating, e.g. of Galinstan.
  • FIG. 12 shows a beam deflector of circular shape.
  • the shape may, however, e.g. be rectangular, with electrodes 3 a ′ and 3 a ′′ arranged at opposite sides of the rectangle.
  • the device can be combined with further optical elements, such as flat or curved mirrors, gratings or holograms.
  • ring sections 4 a , 4 b and 4 c have been used for contacting the electrodes. It must be noted, though, that different means of contact can be used as well. For example, metallic, needle-like structures can be stuck through the leads 9 a , 9 b , 9 c for providing a common contact. Alternatively, conducting vias filled with conducting materials can be integrated into the electroactive material stack during the layer by layer process. This contacting method allows the contacting of the electrodes 3 a - 3 e from one side of the electroactive material stack.
  • the electrodes 3 a , 3 c , 3 e were commonly applied to a first potential, while the electrodes 3 b , 3 d were applied to a second potential. It is also possible to apply individual potentials to some or all of the electrodes in order to control the deformation electroactive element 2 more accurately.
  • one or both surfaces of optical element 1 can be provided with an antireflective layer.
  • the layer can consist of:
  • the shape of the optical element 1 in its deformed state can be influenced by locally hardening or softening parts of the optical element, e.g. by UV curing or chemical treatments.
  • An example of this embodiment is illustrated in FIG. 13 , where a hatched region indicates a rigid element 26 below surface 20 , which has been manufactured by local hardening and provides an improved flatness of surface 20 upon application of a voltage to the device.
  • a rigid element can also be made of a material different from the rest of the optical element and be added to the same e.g. by embedding it or mounting it to a surface thereof. The position of the rigid element is changed when a voltage is applied to the electrodes.
  • the material of optical element 1 can have inhomogeneous hardness, in particular it can comprise an inhomogeneously polymerized polymer.
  • optical element 1 can be an assembly of two or more materials, suitably joined together e.g. in order to correct chromatic aberrations by using two materials having differing optical dispersions.
  • optical element 1 can further be structured, e.g. by means of
  • the electroactive optical device can be used in a large variety of applications, such as:

Abstract

An electroactive optical device, in particular an electroactive lens, comprising an optical element (1) as well as an electroactive element (2) is described. The optical element (1) is an elastic solid, such as a gel or a polymer. The electroactive element (2) comprises a plurality of compliant electrodes (3 a-3 e) stacked on top of each other with an electroactive material (5) between them. The electroactive element (2) is surrounded by a rigid wall (4 a, 4 b), which provides two common contacts for the electrodes (3 a-3 e). In the absence of an applied electric voltage, the optical element (1) is in a mechanically relaxed state, which reduces undesired ageing effects. Upon application of a voltage to the electrodes (3 a-3 e) the optical element (2) is deformed.

Description

    TECHNICAL FIELD
  • The invention relates to an electroactive optical device, in particular an electroactive lens, as well as to a method for manufacturing such a device.
  • BACKGROUND ART
  • An electroactive optical device is an optical device whose shape can be changed using the electroactive effect. In particular, an electroactive optical lens is a lens whose focal length can be changed using the electroactive effect.
  • The term electroactive effect describes an electric-field induced deformation of a solid or liquid. The deformation can be due to Coulomb forces between electrodes and/or due to the rearrangement of electrical ions and/or multipoles, in particular dipoles, in an electric field. Examples of electroactive materials are: dielectric elastomers, electrostrictive relaxor ferroelectric polymers, piezoelectric polymers (PVDF), liquid crystal elastomers (thermal), ionic polymer-metal composites, mechano-chemical polymers/gels.
  • A variety of electroactive lens designs have been known.
  • WO 2008/044937, for example, describes a device where a circularly shaped piezoelectric crystal is bending a thin glass cover, thereby providing a shift of focal length of the lens assembly. Devices based on piezoelectric crystals are, however, comparatively expensive to manufacture.
  • WO 2005/085930 relates to an adaptive optical element that can be configured e.g. as a biconvex lens. The lens consists of a polymer actuator comprising an electroactive polymer layer and layer electrodes. Applying a voltage in the order of 10 kV or more leads to a deformation of the polymer layer, which, in turn, leads to a direct deformation of the lens. Due to the high voltage required to control this device, it is poorly suited for many applications.
  • Also, prior art devices of these types often show ageing effects that degrade their properties over time.
  • Finally, a variety of devices using liquid filled lenses are known. These devices suffer from a plurality of drawbacks. In particular, they are susceptible to distortions due to external forces, such as acceleration, gravitational effects or vibrations.
  • DISCLOSURE OF THE INVENTION
  • Hence, it is a general object of the invention to provide a device of this type that is reliable and that overcomes at least part of the mentioned shortcomings.
  • This object is achieved by the electroactive device of claim 1. Accordingly, the device comprises an elastic optical element as well as an electroactive element arranged laterally adjacent to the optical element. The electroactive element comprises at least one electrode pair with an elastic electroactive material, advantageously a dielectric elastomer, arranged between the electrodes of the electrode pair. When a voltage is applied over the electrode pair, the axial distance between the electrodes of the electrode pair changes, i.e. it increases or decreases, thereby elastically varying the volume (i.e. the axial extension) of a first region in the optical element adjacent to the electrode pair. This, in turn, leads to a radial displacement of material in the optical element between said first region and a second region. One of said regions elastically expands in axial direction, while the other elastically contracts. In the absence of a voltage over the electrode pair, the optical element is in a mechanically relaxed state.
  • By varying the axial extension of the two regions and thereby radially displacing material of the optical element, a strong change of the curvature of the surface of the optical element can be achieved.
  • This design uses the advantages of an electroactive actuator, such as its potentially easy manufacturing process, large deformations and low actuation voltage, while providing a solution that has a long lifetime because, in the absence of a voltage, the device is in an elastically relaxed state and therefore is less prone to fatigue than devices where the device is formed by a pre-strained solid and is therefore under continuous strain.
  • Advantageously, the application of the voltage will lead to a decrease of the distance between the electrodes, which in turn will reduce the volume of said first region of the optical element. Additionally, the compressed electroactive material between the electrodes can exert a lateral pressure onto the optical element. The combination of both effects brings the optical element into a strongly deformed state.
  • In most cases, the above effects will lead to an increase of the thickness of the optical element upon application of a voltage to the electrode pairs.
  • Advantageously, the electroactive element comprises a plurality of electrode pairs stacked on top of each other, with gaps between the electrode pairs. The gaps are advantageously filled by the electroactive material. This design allows to obtain a large volume displacement of material in the optical element using low drive voltages.
  • In a further aspect of the invention, it is an object to provide an efficient manufacturing method for such a device. This object is achieved by the second independent claim. Accordingly, the method comprises the following steps:
      • a) providing a plurality of first electrodes,
      • b) applying, over said first electrodes, a layer of electroactive material,
      • c) applying a plurality of second electrodes over said first electrodes, with each second electrode attributed to a first electrode, and
      • d) separating a resulting assembly of said steps a), b) and c) into a plurality of said electroactive devices.
  • As can be seen, this process allows to simultaneously form a plurality of the devices with common steps a), b) and c), which reduces manufacturing costs.
  • Advantageously, steps b) and c) are repeated in order to form a plurality of electrode pairs stacked on top of each other in order to manufacture devices that can be controlled with low voltages.
  • BRIEF DESCRIPTION OF THE DRAWINGS
  • The invention will be better understood and objects other than those set forth above will become apparent when consideration is given to the following detailed description thereof. Such description makes reference to the annexed drawings, wherein:
  • FIG. 1 is a sectional view of a lens without applied voltage,
  • FIG. 2 is a top view of the lens of FIG. 1,
  • FIG. 3 is the lens of FIG. 1 with applied voltage,
  • FIG. 4 is a first step in a manufacturing process,
  • FIG. 5 is a second step in a manufacturing process,
  • FIG. 6 is a third step in a manufacturing process,
  • FIG. 7 is a fourth step in a manufacturing process,
  • FIG. 8 is a fifth step in a manufacturing process,
  • FIG. 9 shows a sectional view of an assembly of two lenses without applied voltage, with small applied voltage and with large applied voltage,
  • FIG. 10 shows an assembly of four stacked lenses,
  • FIG. 11 is a view of a lens with graded electrodes,
  • FIG. 12 shows a top view of a beam deflector,
  • FIG. 13 shows a sectional view of the beam deflector along line XIII of FIG. 12 in three different states,
  • FIG. 14 shows a further embodiment of an optical device with a buffer layer,
  • FIG. 15 shows a further embodiment of an optical device with a lid layer, and
  • FIG. 16 shows yet a further embodiment of an optical device with a lid layer and a buffer layer.
  • MODES FOR CARRYING OUT THE INVENTION
  • Definitions
  • The term “axial” is generally used to designate a direction perpendicular to the surface of the center region of the optical element in its relaxed state. If a substrate is present, the substrate will in most cases be aligned perpendicularly to the axial direction.
  • The term “radial” is used to designate a direction perpendicular to the axial direction.
  • Introduction
  • The present invention can be implemented in a variety of forms, e.g. as an electroactive lens, a beam deflector or an anti-jittering device. In the following, we describe some of these applications.
  • Electroactive Lenses
  • One possible embodiment of the present invention as an electroactive lens is shown in FIGS. 1 and 2. The lens comprises an elastic optical element 1 and an electroactive element 2. In the present embodiment, the optical element 1 is circular and the electroactive element 2 surrounds the optical element. However, as mentioned below, the present invention can also be implemented for non-circular lenses, e.g. cylindrical lenses, as long as electroactive element 2 is laterally adjacent to at least one side of optical element 1.
  • Electroactive element 2 comprises at least two, advantageously more than two, vertically stacked electrodes 3 a-3 e forming at least one electrode pair, advantageously several electrode pairs on top of each other.
  • The first, topmost electrode 3 a is, by means of a lead 9 a, electrically connected to a first section 4 a of a side wall, while the second, next electrode 3 b is connected to a second section 4 b of the side wall by means of a lead 9 b, the third electrode 3 c is again connected to first section 4 a by means of a lead 9 c, the fourth electrode 3 d to second section 4 b by means of a lead 9 d, etc, such that adjacent electrodes are connected to different sections of the side wall. The side wall is electrically conducting and it is of a solid material, such as a conductive polymer. When a voltage difference is applied over the two sections 4 a, 4 b of the side wall, the same voltage difference is applied over each neighboring pair of the electrodes 3 a-3 e.
  • An electroactive material 5 is located in the gaps between the electrodes 3 a-3 e, i.e. all the gaps between the electrodes are filled by the electroactive material 5. An electroactive material is any material that, when a voltage is applied between neighboring electrodes, yields to the Maxwell stress caused by the Coulomb forces between the electrodes. Advantageously, electroactive material 5 is a solid, such as a dielectric elastomer, or a gel.
  • Optical element 1 of the lens can be of the same material as electroactive material 5—this simplifies the manufacturing process, as described below. However, optical element 1 may also be of a material different from electroactive material 5, which allows to optimize the physical properties of optical element 1 and electroactive element 2 independently.
  • Optical element 1 is a transparent elastic solid or a gel and, in the absence of a voltage applied to the electrodes 3 a-3 e, it is in a mechanically relaxed state for the reasons mentioned above. Advantageously, it is made from a single piece of material.
  • The function of the lens of FIGS. 1 and 2 is shown in reference to FIG. 3. As can be seen, when a non-zero voltage V is applied over all neighboring electrode pairs formed by the electrodes 3 a-3 e, the Coulomb forces between the electrodes and/or a rearrangement of multipoles within the material lead to a decrease or an increase of the axial distance between the electrodes, depending on the electro- active material that is used. In particular, liquid crystal elastomers can be engineered to expand in the direction of an applied field, while most other materials will contract.
  • If the electroactive material contracts upon application of the field, the thickness of the electroactive element 2 is decreased. Since the electroactive element 2 is laterally joined to the optical element 1, a compressed first region is created in the optical element adjacent to the electrodes. This, in turn, leads to a radial displacement of material of the optical element 1 away from the compressed first region, typically towards the center of the optical element 1. This, in turn, forms an axially expanding second region in the optical element due to the incompressibility of the material. In FIG. 3, this axially expanding region is in the center of optical element 2.
  • If the electroactive material expands along the applied field, the thickness of the electroactive element 2 is increased, and the first region of the optical element 1 expands in axial direction, while the second region contracts.
  • Hence, the application of the voltage to the electrodes leads to a redistribution of material within optical element 1, which in turn affects the curvature of its surface. In particular, due to the boundary conditions imposed by the contracting electroactive element, the optical element 1 becomes thinner in the regions adjacent to those electrodes where the voltage has been applied, while it becomes thicker elsewhere.
  • Depending on the thickness and volume of the optical element 1 as well as the electroactive element 2, one contribution to the deformation of the optical element 1, if the distance between the electrodes decreases, is provided by the fact that, upon application of the voltage, the electroactive material 5 between them is compressed. This compression is translated into a lateral expansion of the material (constant volume approximation), which leads to a flow of material from the electroactive element 2 into the optical element 1, thereby making the optical element 1 thicker and, advantageously, more voluminous. In particular if wall 4 a, 4 b is a solid, advantageously rigid, ring, the lateral expansion is directed inwards and exerts a pressure on the elastic material of optical element 1, which results in a deformation of its surface. As shown in FIG. 3, if the relaxed surface (FIG. 1) is originally flat, the deformation causes the surface to bulge outwards, thereby forming a convex lens surface, which affects the focal length of the lens formed by optical part 1.
  • As mentioned, the present lens is not necessarily a circular lens. It may, as mentioned, e.g. also be cylindrical. In this case, optical element 1 is formed by an elongate strip of transparent, elastic material, with at least one elongate electroactive element 2 arranged along at least one side thereof, such that electroactive element 2 can create a compressed or expanded first region in the optical element 1 adjacent to the electrodes, as mentioned above. Also in this case it is advantageous to locate a solid wall at the second (opposite) side of the electroactive element 2 in order to prevent the electroactive material 5 from yielding in that direction, thereby directing the whole voltage-induced displacement of material towards optical element 1.
  • As can be seen from FIGS. 1-3, the lens advantageously comprises a solid, transparent substrate 7, with the electroactive element 2 and the optical element 1 arranged thereon. Such a substrate provides mechanical stability to the device and simplifies the manufacturing process as described below. However, if optical element 1 has sufficient mechanical stability, substrate 7 can also be dispensed with.
  • The distance between adjacent electrodes 3 a-3 e should not be too large in order to obtain strong Coulomb forces even if the applied voltage is small. Advantageously, the distance between two neighboring electrodes should be less than 250 μm, in particular approximately 10 μm, and it should be small enough to allow significant deformations at voltages below 1 kV.
  • The electrodes should be compliant, i.e. they should be able to follow the deformations of electroactive element 2 without being damaged. Advantageously, the electrodes are therefore manufactured from one of the following materials:
      • Carbon nanotubes (see “Self-clearable carbon nanotube electrodes for improved performance of dielectric elastomer actuators”, Proc. SPIE, Vol. 6927, 69270P (2008);)
      • Carbon black (see “Low voltage, highly tunable diffraction grating based on dielectric elastomer actuators”, Proc. SPIE, Vol. 6524, 65241N (2007);)
      • Carbon grease
      • Ions (Au, Cu, Cr, . . . ) (see “Mechanical properties of electroactive polymer microactuators with ion-implanted electrodes”, Proc. SPIE, Vol. 6524, 652410 (2007);)
      • Fluid metals (e.g. Galinstan)
      • Metallic powders, in particular metallic nanoparticles (Gold, silver, copper)
      • Conductive polymers
      • Rigid electrodes connected to deformable leads
  • The material for optical element 1 and the electroactive material 5 for electroactive element 2 can e.g. comprise or consist of:
      • Gels (Optical Gel OG-1001 by Liteway),
      • Elastomers (TPE, LCE, Silicones e.g. PDMS Sylgard 186, Acrylics, Urethanes)
      • Thermoplaste (ABS, PA, PC, PMMA, PET, PE, PP, PS, PVC, . . . )
      • Duroplast
  • The geometries of the electrodes 3 a-3 e do not necessarily have to be identical. FIG. 11 shows an advantageous embodiment where the electrodes 3 a-3 e have increasingly larger inner diameter towards the surface of the device. In other words, at least the electrode 3 a closest to the top surface has a larger inner diameter than the next lower electrode. (In this context, “top surface” designates the surface of the lens that is deformed upon application of a voltage.)
  • This design reduces the mechanical strain in the electroactive material 5 as well as in the material of the optical element 1 upon application of a voltage.
  • In more general terms, the inner diameter of at least one of the electrodes 3 a-3 e can be different from the inner diameter of at least some of the other electrodes. This allows a more refined control of the deformation of optical element 1.
  • In the following, an advantageous manufacturing process is described by reference to FIGS. 4 to 8. In this process, a plurality of electroactive lenses is manufactured at the same time on a common wafer. The common wafer may be pre-shaped e.g. to comprise fixed structures, such as rigid lenses, to be combined with the optical elements 2.
  • The process starts (step a, FIG. 4) from substrate 7, which originally has a size much larger than an individual lens. The bottommost electrodes 3 e for a plurality of adjacent lenses are deposited on the substrates. Any suitable method can be used for manufacturing these electrodes, as long as it is compatible with the electrode material and the substrate, such as sputtering with subsequent masking and etching.
  • Now (step b, FIG. 5), a layer 5 a of the electroactive material 5 is applied over substrate 7. The layer 5 a may e.g. have a thickness of 10 μm.
  • In a next step (step c, FIG. 6), a plurality of second electrodes, namely the electrodes 3 d, are applied over the layer 5 a of electroactive material. The electrodes 3 d are in register with the electrodes 3 e, with one electrode 3 d attributed to each electrode 3 e.
  • Then, step b is repeated, i.e. a further layer 5 b of the electroactive material is applied as shown in FIG. 6, whereupon step c is repeated, etc., until a stacked structure of sufficient height with a plurality of stacked electrode pairs on top of each other is manufactured, as shown in FIG. 7.
  • After completing the layer structure of FIG. 7, the walls 4 a, 4 b, which have been prefabricated and are e.g. applied to a common carrier (not shown), are pushed from above into the layer structure. Since the layers 5 a, 5 b, . . . are of a soft material, the walls 4 a, 4 b enter the layers as shown in FIG. 8, whereupon the common carrier (not shown) of the walls can be removed. The walls 4 a, 4 b are positioned such that they contact the electrodes 3 a-3 e. For this purpose, as it can best be seen in FIG. 7 as well as FIGS. 1 and 2, the electrodes 3 a-3 e are provided with the leads 9 a-9 e that laterally extend away from the center of the lens in order to provide a contact with the respective wall section 4 a or 4 b.
  • Finally, the product of the above steps is separated into a plurality of electroactive lenses by severing them between the walls of adjacent lenses, e.g. along lines 10 as shown in FIG. 8. Alternatively, if substrate 7 is sufficiently soft, a separation of the lenses can e.g. also be achieved by pushing the walls 4 a, 4 b not only through the electroactive material layers 5 a, 5 b . . . , but also through the substrate 7. In yet a further alternative, the product shown in FIG. 7 can also be severed first, where-upon the walls 4 a, 4 b, or other means for providing a contact to the electrodes 3 a-3 e, are applied individually to each lens.
  • In above step b, the following methods can e.g. be used for applying the electroactive material layer 5 a, 5 b . . . :
      • Spin-coating with subsequent hardening
      • Spraying with subsequent hardening
      • Printing (e.g. screen printing)
      • Chemical vapor deposition, in particular PECVD (Plasma enhanced chemical vapor deposition)
      • prefabricating the material layers and applying them on the substrate, advantageously by bonding them thereto—in this case, the layers may optionally be non-elastically stretched prior to their application in order to decrease their thickness.
  • The following materials can e.g. be used for the electroactive material as well as for the optical element:
      • Gels (Optical Gel OG-1001 by Litway)
      • Polymers (e.g. PDMS Sylgard 186 by Dow Corning, Neukasil RTV 25
      • Acrylic materials (e.g. VHB 4910 by the company 3M)
      • Elastomers
  • In above step c, the following methods can e.g. be used for applying the compliant electrodes 3 a-3 d and, optionally, 3 e:
      • Ion-implantation (see “Mechanical properties of electroactive polymer microactuators with ion-implanted electrodes”, Proc. SPIE, Vol. 6524, 652410 (2007);)
      • PVD, CVD
      • Evaporation
      • Sputtering
      • Printing, in particular contact printing, inkjet printing, laser printing, and screen printing.
      • Field-guided self-assembly (see e.g. “Local surface charges direct the deposition of carbon nanotubes and fullerenes into nanoscale patterns”, L. Seemann, A. Stemmer, and N. Naujoks, Nano Letters 7, 10, 3007-3012, 2007)
      • Brushing
      • Electrode plating
  • Optionally, optical element 1 can be structured to have a desired shape in its relaxed and/or deformed states. Examples of such lenses are described below in reference to FIGS. 9 and 10. Suitable lens shapes (in the relaxed state) can e.g. be:
      • Spherical lenses (convex and concave)
      • Aspherical lenses (convex and concave)
      • Flat
      • Squares, triangles, lines or pyramids
      • Any micro (e.g. micro lens array, diffraction grating, hologram) or nano (e.g. antireflection coating) structure can be integrated into the clear aperture of optical element 1 and the compliant electrode containing polymer layer.
  • Any of the following methods can e.g. be applied for shaping the lens:
      • a) Casting, in particular injection molding
      • b) Nano-imprinting, e.g. by hot embossing nanometer-sized structures
      • c) Etching (e.g. chemical or plasma)
      • d) Sputtering
      • e) Hot embossing
      • f) Soft lithography (i.e. casting a polymer onto a pre-shaped substrate)
      • g) Chemical self-assembly (see e.g. “Surface tension-powered self-assembly of microstructures—the state-of-the-art”, R. R. A. Syms, E. M. Yeatman, V. M. Bright, G. M. Whitesides, Journal of Microelectromechanical Systems 12(4), 2003, pp. 387-417)
      • h) Electro-magnetic field guided pattern forming (see e.g. “Electro-magnetic field guided pattern forming”, L. Seemann, A. Stemmer, and N. Naujoks, Nano Lett., 7 (10), 3007-3012, 2007. 10.1021/n10713373.
  • As will be apparent to the skilled person, some of the above methods are directly compatible with the manufacturing process described in reference to
  • FIGS. 4-8, e.g. methods c) and d) can take place on the product shown in FIG. 7. Some other methods will require additional steps. For example, an array of convex lenses on a common carrier can be manufactured by means of methods a), b), or e)-k) and then be applied on top of the product of FIG. 7.
  • Several electroactive lenses of the type described above can be combined to form a multi-lens assembly.
  • An example of such an assembly is shown in FIG. 9, where two electroactive lenses 11 a, 11 b are mounted to opposite sides of a solid and transparent common substrate 7. As can be seen from the left part of the figure, in the absence of an applied voltage, lens 11 a has a flat surface while lens 11 b is concave. While lens 11 a can be manufactured e.g. as shown in FIGS. 4-8, the optical element of lens 11 b has e.g. subsequently been structured by using above methods c) or d).
  • When a small voltage is applied, as shown in the central part of the figure, lens 11 a becomes convex while lens 11 b remains concave, albeit with smaller curvature. Finally, and as shown in the right part of FIG. 9, when the voltage is sufficiently large, both lenses 11 a, 11 b become convex.
  • The present lens can also be combined to even more complex structures. An example of such an assembly is shown in FIG. 10.
  • The assembly of FIG. 10 comprises four electroactive lenses 11 a, 11 b, 11 c, 11 d as well as four rigid lenses 12 a, 12 b, 12 c, 12 d stacked on top of each other. The walls 4 a, 4 b and additional spacer elements 13 a, 13 b are used to keep the lenses at a correct distance from each other. In the example of FIG. 10, each electroactive lens 11 a-11 d is attached to one side of a substrate 7, with a rigid lens 12 a-12 d arranged at the opposite side of the same substrate.
  • In the embodiment of FIG. 10, each rigid lens is attached to a substrate 7. However, one or more of the rigid lenses may also be mounted independently of a substrate.
  • The shapes of the electro- active lenses 11 a, 11 b, 11 c, 11 d in the absence of a field can be defined using the structuring methods described above.
  • Spherical Lenses
  • For many applications, lenses should be spherical. To create approximately spherical lenses with the designs shown in FIGS. 1-10, the total thickness of electroactive element 2 and the optical element 1 should be fairly large. Otherwise, in particular if the electroactive layer is bonded to substrate 7, the deformation under applied voltage will be strong close to the electrodes but weak in the middle of the lens.
  • On the other hand, using the manufacturing process of FIGS. 4-8 requires a comparatively large number of individual layers 5 a, 5 b, . . . if the total thickness of optical element 1 and electroactive layer 2 is to be large, which renders the process expensive.
  • For this reason, it is advantageous to use a design as shown in FIG. 14, where the electrodes 3 a-3 e are separated from substrate 7 by an elastic buffer layer 30. Buffer layer 30, which is arranged between substrate 7 on the one hand and electroactive element 2 and optical element 1 on the other hand, allows the material of optical element 1 to displace more freely, in particular in horizontal direction, i.e. it insulates the optical element 1 from the mechanical constraints of the rigid substrate 7. Therefore, advantageously, buffer layer 30 is of a comparatively soft material, i.e. it should have a Young's modulus smaller than or equal to the one of the optical element 1.
  • Buffer layer 30 can be fully attached to substrate 7 as well as to optical element 1, thereby connecting the two without restricting the motion of optical element 1 when a voltage is applied to the electrodes.
  • Another measure to improve the surface shape of a spherical lens, i.e. to bring it closer to an ideal spherical lens, is shown in FIG. 15. In the embodiment of FIG. 15, a lid layer 31 has been attached to the top side of optical element 1, i.e. to the side opposite substrate 7. Lid layer 31 is stiffer than optical element 1, i.e. it has a Young's modulus larger than the one of optical element 1. For a high-quality lens, particular, the Young's modulus should be about 60 times larger than the one of optical element 1. If the layer thickness is thinner, the Young's modulus has to increase to result in a good optical quality.
  • The measures of FIGS. 14 and 15 can be combined as shown in FIG. 16, where the optical device comprises a buffer layer 30 as well as a lid layer 31.
  • Suitable materials for buffer layer 30 and lid layer 31 are e.g. PDMS, acrylics or polyurethans. The buffer layer has typically a Young's modulus in the range of 200 kPa or less and the lid layer has a Young's modulus of 10 MPa or more. These materials are advantageously combined with elastomer, acrylics and polyurethans for the electroactive material as well as for the lens element.
  • Beam Deflectors
  • The technologies described above can not only be applied to lenses, but to a variety of other electroactive optical devices, such as beam deflectors or anti-jittering devices.
  • An example of a beam deflector or minor is shown in FIGS. 12 and 13. It has basically the same set-up as the device of FIGS. 1-3 but the electrodes 3 a and 3 c are each split up into two electrode sections 3 a′ and 3 a″ as well as 3 c′ and 3 c″, each section extending around approximately 180° of optical element 1. Accordingly, the wall has been split up into three sections 4 a, 4 b, 4 c, with section 4 a being connected to the electrode sections 3 a′ and 3 c′, section 4 b being connected to the electrode sections 3 a″ and 3 c″, and section 4 c being connected to the electrode sections 3 b and 3 d. A voltage V1 can be applied between sections 4 a and 4 c, and a voltage V2 between sections 4 b and 4 c.
  • If V1=V2=0, the surface of optical element 1 is flat and horizontal as shown in the left hand part of FIG. 13. If V1≠0 and V2=0, the surface of optical element is substantially tilted to one side, while, if V1=0 and V2 ≠0, the surface of optical element is substantially tilted to the opposite side.
  • This type of device can be used as a beam deflector, either in transmission or reflection.
  • If the device is operated in transmission, a beam extending through optical element 1 can either be deflected to the left or to the right, depending on V1 and V2, as shown by the arrows 21.
  • If the device is operated in reflection, at least one of the surfaces of optical element 1 can be provided with a minor element, such as a reflective coating 25 or a rigid reflective minor plate, and a beam can either be deflected to the right or left, respectively, as shown by the dotted arrows 22.
  • The minor element can, as mentioned, e.g. be a mirror plate affixed to surface 20, or it may be a coating, such as a liquid metal coating, e.g. of Galinstan.
  • FIG. 12 shows a beam deflector of circular shape. The shape may, however, e.g. be rectangular, with electrodes 3 a′ and 3 a″ arranged at opposite sides of the rectangle.
  • Other Types of Devices: The technologies described above can be applied in yet other types of devices, such as optical phase retarders (using technologies as e.g. described in WO 2007/090843).
  • Also, the device can be combined with further optical elements, such as flat or curved mirrors, gratings or holograms.
  • Further Notes:
  • In the embodiments above, ring sections 4 a, 4 b and 4 c have been used for contacting the electrodes. It must be noted, though, that different means of contact can be used as well. For example, metallic, needle-like structures can be stuck through the leads 9 a, 9 b, 9 c for providing a common contact. Alternatively, conducting vias filled with conducting materials can be integrated into the electroactive material stack during the layer by layer process. This contacting method allows the contacting of the electrodes 3 a-3 e from one side of the electroactive material stack.
  • Furthermore, in the example of FIGS. 1-3, the electrodes 3 a, 3 c, 3 e were commonly applied to a first potential, while the electrodes 3 b, 3 d were applied to a second potential. It is also possible to apply individual potentials to some or all of the electrodes in order to control the deformation electroactive element 2 more accurately.
  • In a particularly advantageous embodiment, one or both surfaces of optical element 1 can be provided with an antireflective layer. The layer can consist of:
      • “nanometer-structures”, either formed in the material of optical element 1 itself or in a separate coating material. The structures have a size well below the wavelength of the light, e.g. of a size <400 nm. They can e.g. be applied by means of etching, molding, casting or embossing.
      • An antireflective thin layer coating.
  • In yet a further advantageous embodiment, the shape of the optical element 1 in its deformed state can be influenced by locally hardening or softening parts of the optical element, e.g. by UV curing or chemical treatments. An example of this embodiment is illustrated in FIG. 13, where a hatched region indicates a rigid element 26 below surface 20, which has been manufactured by local hardening and provides an improved flatness of surface 20 upon application of a voltage to the device. A rigid element can also be made of a material different from the rest of the optical element and be added to the same e.g. by embedding it or mounting it to a surface thereof. The position of the rigid element is changed when a voltage is applied to the electrodes.
  • In more general terms, the material of optical element 1 can have inhomogeneous hardness, in particular it can comprise an inhomogeneously polymerized polymer.
  • Also, optical element 1 can be an assembly of two or more materials, suitably joined together e.g. in order to correct chromatic aberrations by using two materials having differing optical dispersions.
  • Furthermore, optical element 1 can further be structured, e.g. by means of
      • microstructures, such as diffractive structures or holographic structures,
      • deformable coatings, such as reflective or anti-reflective coatings (as mentioned above) or absorptive coatings.
  • Some Applications:
  • The electroactive optical device can be used in a large variety of applications, such as:
      • Cameras (zoom and auto focus), such as in mobile phones, digital SLR cameras, cameras in vehicles, surveillance systems
      • Optical part of projectors for macro- and nano-projectors in beamers and mobile phone projectors.
      • Industrial applications including laser cutting or welding
      • Microscopes, magnifying glasses
      • Vision correction (implanted lens in a human eye).
      • Endoscopes
      • Magnification glasses
      • Vision systems, such as any kind of camera
      • Research applications for quantum computing
      • Telecommunication applications (amplitude modulation)
      • Laser applications, such as for deflecting laser beams
      • Telescopes
      • Displays
  • While there are shown and described presently preferred embodiments of the invention, it is to be distinctly understood that the invention is not limited thereto but may be otherwise variously embodied and practiced within the scope of the following claims.

Claims (29)

1. An electroactive optical device, in particular an electroactive lens, comprising
an elastic optical element (1),
an electroactive element (2) arranged laterally adjacent to said optical element (1) and comprising at least one electrode pair of two electrodes (3 a-3 e) with an elastic electroactive material (5) arranged between said electrode pair,
wherein upon application of a voltage over said at least one electrode pair an axial distance between said electrodes changes, thereby varying a volume of a first region in said optical element adjacent to said electrode pair, thereby radially displacing material in said optical element (1) between said first region and a second region of said optical element (1), wherein one of said regions elastically expands and the other elastically contracts in an axial direction, thereby bringing said optical element (1) into a deformed state, while, in the absence of a voltage over said at least one electrode pair, said optical element (1) is in an elastically relaxed state.
2. The electroactive optical device of claim 1 wherein said electroactive element (2) comprises a plurality of electrode pairs stacked on top of each other with a plurality of gaps between said electrode pairs, and in particular wherein said gaps are filled by said electroactive material.
3. The electroactive optical device of any of the preceding claims wherein the optical element (1) is a solid or a gel.
4. The electroactive optical device of any of the preceding claims wherein the electroactive element (2) comprises or consists of a material selected from the group comprising gels, polymers, acrylic materials and elastomers.
5. The electroactive optical device of any of the preceding claims wherein the optical element (1) is the same material as the electroactive material (5).
6. The electroactive optical device of any of the claims 1 to 4 wherein the optical element (1) is of a material different from the electroactive material (5).
7. The electroactive optical device of any of the preceding claims wherein said electro active element (2) surrounds said optical element (1).
8. The electroactive optical device of any of the preceding claims wherein said optical material is arranged at a first side of said electroactive element (2) and wherein said electroactive optical device further comprises a solid wall (4 a, 4 b) at a second side of said electroactive element (2), wherein said second side is opposite to said first side.
9. The electroactive optical device of claim 8 wherein each of said electrodes (3 a-3 e) is electrically connected to one of at least two different sections (4 a, 4 b) of said wall.
10. The electroactive optical device of any of the preceding claims wherein said electroactive element (2) comprises at least one electrode made from at least one material selected from the group comprising carbon nanotubes, carbon black, carbon grease, metal ions, fluid metals, metallic powders, conductive polymers, and rigid electrodes connected to deformable leads.
11. The electroactive optical device of any of the preceding claims further comprising a solid substrate (7), and in particular wherein said electroactive element (2) and said optical element (1) are arranged on said substrate (7).
12. The electroactive optical device of claim 11 further comprising a buffer layer (30) arranged between said substrate (7) and said electroactive element (2) and said optical element (1), wherein said buffer layer (30) has a Young's modulus smaller than or equal to the Young's modulus of said optical element (1), and in particular wherein said buffer layer (30) is attached to said substrate (7).
13. The electroactive optical device of any of the preceding claims further comprising a lid layer (30) attached to said optical element (1), wherein said lid layer (30) has a Young's modulus larger than a Young's modulus of said optical element (1).
14. The electroactive optical device of any of the preceding claims wherein a distance between neighboring electrodes (3 a-3 e) is less than 250 μm, in particular approximately 10 μm.
15. The electroactive optical device of any of the preceding claims wherein an inner diameter of at least one of the electrodes (3 a-3 e) is different from the inner diameter of at least some of the other electrodes,
and in particular wherein an electrode (3 a) closest to a top surface of said optical device has a larger inner diameter than a next lower electrode (3 b), wherein the top surface is the surface that is deformed upon application of a voltage.
16. The electroactive optical device of any of the preceding claims further comprising a mirror element (25) on at least one surface of said optical element (1).
17. The electroactive optical device of any of the preceding claims further comprising a rigid element (26) in the optical element.
18. The electroactive optical device of any of the preceding claims further comprising an antireflective layer on at least one surface of said optical element, and in particular wherein said antireflective layer comprises structures having a size smaller than 400 nm.
19. The electroactive optical device of any of the preceding claims wherein said optical element (1) is of an inhomogeneous hardness, in particular wherein said optical element comprises an inhomogeneously polymerized polymer.
20. The electroactive optical device of any of the preceding claims wherein, upon application of a voltage over said at least one electrode pair, said electroactive material (5) is compressed and exerts a lateral pressure onto said optical element (1), thereby bringing said optical element (1) into said deformed state.
21. The electroactive optical device of any of the preceding claims wherein said electroactive material is such that upon application of the voltage over said at least one electrode pair the axial distance between said electrodes decreases, thereby compressing said first region, thereby radially displacing material in said optical element (1) away from said first region into said second region.
22. An assembly of at least two electroactive devices (11 a, 11 b . . . ) of any of the preceding claims on top of each other.
23. The assembly of claim 22 wherein said electroactive devices (11 a, 11 b . . . ) are mounted to opposite sides of a common solid substrate (7).
24. A method for manufacturing the electroactive optical device of any of the preceding claims comprising the steps of
a) providing a plurality of first electrodes (3 e),
b) applying, over said first electrodes (3 e), a layer (5 a) of electroactive material,
c) applying a plurality of second electrodes (3 d) over said layer (5 a) of electroactive material, with each second electrode (3 d) attributed to a first electrode (3 e), and
d) separating a resulting product of said steps a), b) and c) into a plurality of said electroactive devices.
25. The method of claim 24 wherein said steps b) and c) are repeated for forming a plurality of electrode pairs on top of each other.
26. The method of any of the claim 24 or 25 wherein said plurality of first electrodes (3 e) is arranged on a solid substrate (7).
27. The method of any of the claims 24 to 26 wherein said step b) comprises the application of said electroactive material (5) by a method selected from the group comprising spin coating, spraying, printing, applying a prefabricated material layer, and chemical vapor deposition, in particular plasma-enhanced chemical vapor deposition.
28. The method of any of the claims 24 to 27 wherein solid walls (4 a, 4 b) are inserted into said layers (5 a, 5 b, . . . ) of electroactive material (5) for contacting the electrodes (3 a-3 e).
29. The method of any of the claims 24 to 28 wherein said optical element (1) made from a single piece of material.
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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20160351785A1 (en) * 2015-05-28 2016-12-01 Honda Motor Co., Ltd. Electrostrictive element
DE102015226173A1 (en) * 2015-12-21 2017-06-22 Robert Bosch Gmbh Optical imaging system with a deformable due to electrical and / or magnetic forces lens
US20190049750A1 (en) * 2017-08-08 2019-02-14 International Business Machines Corporation Dielectric electro-active polymer contact lenses
RU2750110C2 (en) * 2016-11-21 2021-06-22 Конинклейке Филипс Н.В. Optical beam processing device

Families Citing this family (51)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7948683B2 (en) 2006-05-14 2011-05-24 Holochip Corporation Fluidic lens with manually-adjustable focus
US8064142B2 (en) 2005-05-14 2011-11-22 Holochip Corporation Fluidic lens with reduced optical aberration
US7697214B2 (en) 2005-05-14 2010-04-13 Holochip Corporation Fluidic lens with manually-adjustable focus
WO2010015093A1 (en) 2008-08-08 2010-02-11 Optotune Ag Electroactive optical device
EP2382502B1 (en) * 2008-12-30 2019-04-17 Datalogic IP TECH S.r.l. Liquid lens image capture device
US8699141B2 (en) 2009-03-13 2014-04-15 Knowles Electronics, Llc Lens assembly apparatus and method
US8659835B2 (en) 2009-03-13 2014-02-25 Optotune Ag Lens systems and method
US9164202B2 (en) 2010-02-16 2015-10-20 Holochip Corporation Adaptive optical devices with controllable focal power and aspheric shape
GB201006913D0 (en) 2010-04-26 2010-06-09 Taylor Richard Refractive eyewear
US8944647B2 (en) 2010-09-02 2015-02-03 Optotune Ag Illumination source with variable divergence
DE102010044404A1 (en) 2010-09-04 2012-03-08 Leica Microsystems (Schweiz) Ag Image sensor, video camera and microscope
BR112013005408A8 (en) * 2010-09-09 2018-04-03 Koninklijke Philips Nv ACTUATOR AND ACTUATOR MANUFACTURING METHOD
JP2014500522A (en) 2010-10-26 2014-01-09 オプトチューン アクチエンゲゼルシャフト Variable focus lens with two liquid chambers
DE102011053566B4 (en) 2011-09-13 2022-06-23 HELLA GmbH & Co. KGaA lens device
KR101951319B1 (en) * 2012-02-07 2019-02-22 삼성전자주식회사 Varifocal lens
US9081190B2 (en) * 2012-04-26 2015-07-14 Qualcomm Mems Technologies, Inc. Voltage controlled microlens sheet
JP6275129B2 (en) * 2012-07-20 2018-02-07 フィリップス ライティング ホールディング ビー ヴィ Illumination device for obtaining a predetermined light distribution in a target area
DE102013103059B4 (en) * 2013-03-26 2021-06-24 Conti Temic Microelectronic Gmbh Optical lens assembly with a deformable lens body
BR102013010396A2 (en) * 2013-04-29 2015-11-17 Roberto Massaru Amemiya continuous multifocal flexible lenses, their control mechanisms and processes for obtaining the products
KR102064872B1 (en) 2013-08-28 2020-01-10 한국전자통신연구원 Shape-variable optical element
EP2860556A1 (en) 2013-10-08 2015-04-15 Optotune AG Tunable Lens Device
CN103616738B (en) * 2013-12-16 2015-02-18 厦门大学 Method for manufacturing curved-surface fly-eye micro lens with different focal lengths
US9310560B2 (en) 2014-02-26 2016-04-12 TeraDiode, Inc. Systems and methods for multiple-beam laser arrangements with variable beam parameter product
CN104049340A (en) * 2014-06-03 2014-09-17 联想(北京)有限公司 Camera lens, electronic device and zooming method
DE102014116120A1 (en) * 2014-11-05 2016-05-12 Bürkert Werke GmbH Membrane actuator and method for producing a membrane actuator
EP3256887A1 (en) * 2014-11-07 2017-12-20 CooperVision International Holding Company, LP Method and apparatus for an adaptive focus lens
EP3032597B1 (en) * 2014-12-09 2019-02-27 LG Display Co., Ltd. Transformable device and method of manufacturing the same
CN104613303B (en) * 2015-01-16 2017-03-22 西北工业大学 Controllable out-of-plane deformation unit based on electric active soft matter
CN104698631B (en) * 2015-03-30 2018-07-20 京东方科技集团股份有限公司 A kind of ultra-thin glass bonding structure and its stripping means, display device
US10007034B2 (en) * 2015-09-09 2018-06-26 Electronics And Telecommunications Research Institute Auto focusing device
CN106547172B (en) * 2015-09-17 2018-11-13 上海微电子装备(集团)股份有限公司 A kind of exposure device
TWI781085B (en) 2015-11-24 2022-10-21 日商索尼半導體解決方案公司 Fly-eye lens module and fly-eye camera module
US10838116B2 (en) 2016-01-06 2020-11-17 University Of Utah Research Foundation Low-power large aperture adaptive lenses for smart eyeglasses
KR101924613B1 (en) * 2016-03-30 2019-02-27 전북대학교산학협력단 Tunable-focus lenticular microlens array using gel and method for fabricating the same
WO2017191542A1 (en) * 2016-05-02 2017-11-09 Gilad Barzilay Intraocular lens and methods and/or components associated therewith
CN105824063B (en) * 2016-05-17 2018-03-16 西安交通大学 A kind of zoom microlens array structure and preparation technology based on electric actuation
JP6878018B2 (en) 2017-01-26 2021-05-26 ソニーセミコンダクタソリューションズ株式会社 AF module, camera module, and electronic devices
KR101922098B1 (en) 2017-04-10 2018-11-26 한국기술교육대학교 산학협력단 Variable focus double convex lens
JP6957271B2 (en) 2017-08-31 2021-11-02 ソニーセミコンダクタソリューションズ株式会社 Laminated lens structure, solid-state image sensor, and electronic equipment
JP7246068B2 (en) * 2017-12-28 2023-03-27 国立大学法人信州大学 Optical element and method for producing optical element
JP7233082B2 (en) * 2017-12-28 2023-03-06 国立大学法人信州大学 Optical element, microlens array, and method for fabricating optical element
WO2019131925A1 (en) * 2017-12-28 2019-07-04 日東電工株式会社 Optical element, microlens array, and method for producing optical element
WO2019131933A1 (en) * 2017-12-28 2019-07-04 日東電工株式会社 Optical element, and method for producing optical element
US11245065B1 (en) 2018-03-22 2022-02-08 Facebook Technologies, Llc Electroactive polymer devices, systems, and methods
US10962791B1 (en) 2018-03-22 2021-03-30 Facebook Technologies, Llc Apparatuses, systems, and methods for fabricating ultra-thin adjustable lenses
US10914871B2 (en) 2018-03-29 2021-02-09 Facebook Technologies, Llc Optical lens assemblies and related methods
US11107972B2 (en) 2018-12-11 2021-08-31 Facebook Technologies, Llc Nanovoided tunable optics
WO2020203313A1 (en) * 2019-03-29 2020-10-08 株式会社ジャパンディスプレイ Display device and lens array
US11175521B2 (en) 2019-06-04 2021-11-16 Facebook Technologies, Llc Drive schemes for transparent tunable optical elements
CN112731651A (en) * 2021-01-05 2021-04-30 南京邮电大学 Electrically-controlled thickness-adjustable optical phase modulator
KR20230116561A (en) * 2022-01-28 2023-08-04 삼성전자주식회사 Temperature sensor and device

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20020102102A1 (en) * 2001-01-30 2002-08-01 Yoji Watanabe Focal-length adjusting unit for photographing apparatuses
US20060256429A1 (en) * 2003-10-23 2006-11-16 Andreas Obrebski Imaging optics with adjustable optical power and method of adjusting an optical power of an optics
US20070087564A1 (en) * 1998-10-14 2007-04-19 Stuart Speakman Method of forming an electronic device
US20080144185A1 (en) * 2006-12-15 2008-06-19 Hand Held Products, Inc. Apparatus and method comprising deformable lens element

Family Cites Families (66)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2062468A (en) 1934-07-26 1936-12-01 Edwin H Land Optical device
FR2271586B1 (en) 1973-11-29 1978-03-24 Instruments Sa
US4494826A (en) 1979-12-31 1985-01-22 Smith James L Surface deformation image device
US4572616A (en) 1982-08-10 1986-02-25 Syracuse University Adaptive liquid crystal lens
US4783155A (en) 1983-10-17 1988-11-08 Canon Kabushiki Kaisha Optical device with variably shaped optical surface and a method for varying the focal length
JPS61160714A (en) 1985-01-09 1986-07-21 Canon Inc Vari-focal lens
US4802746A (en) * 1985-02-26 1989-02-07 Canon Kabushiki Kaisha Variable-focus optical element and focus detecting device utilizing the same
JPS62148903A (en) 1985-12-24 1987-07-02 Canon Inc Variable focus optical element
JPH01166004A (en) * 1987-12-22 1989-06-29 Fuji Photo Film Co Ltd Optical element
JPH01166003A (en) * 1987-12-22 1989-06-29 Fuji Photo Film Co Ltd Optical element
US5138494A (en) 1990-05-07 1992-08-11 Stephen Kurtin Variable focal length lens
US5212583A (en) 1992-01-08 1993-05-18 Hughes Aircraft Company Adaptive optics using the electrooptic effect
US5446591A (en) 1993-02-08 1995-08-29 Lockheed Missiles & Space Co., Inc. Lens mounting for use with liquid lens elements
US5999328A (en) 1994-11-08 1999-12-07 Kurtin; Stephen Liquid-filled variable focus lens with band actuator
WO1997036365A1 (en) * 1996-03-26 1997-10-02 Stefan Johansson An actuator motor and a method for fabrication of such an actuator
JP3400270B2 (en) 1996-11-08 2003-04-28 株式会社デンソー Laminated piezoelectric actuator and variable focus lens device
US6812624B1 (en) 1999-07-20 2004-11-02 Sri International Electroactive polymers
JPH11133210A (en) * 1997-10-30 1999-05-21 Denso Corp Variable focus lens
JP4144079B2 (en) * 1998-09-04 2008-09-03 株式会社デンソー Variable focus lens
US7027683B2 (en) 2000-08-15 2006-04-11 Nanostream, Inc. Optical devices with fluidic systems
US7672059B2 (en) * 2000-10-20 2010-03-02 Holochip Corporation Fluidic lens with electrostatic actuation
US7646544B2 (en) 2005-05-14 2010-01-12 Batchko Robert G Fluidic optical devices
US7405884B2 (en) 2000-12-21 2008-07-29 Olympus Corporation Optical apparatus
GB0100031D0 (en) 2001-01-02 2001-02-14 Silver Joshua D Variable focus optical apparatus
JP2002357774A (en) 2001-03-28 2002-12-13 Olympus Optical Co Ltd Varifocal optical element
US6747806B2 (en) 2001-04-19 2004-06-08 Creo Srl Method for controlling light beam using adaptive micro-lens
US6538823B2 (en) 2001-06-19 2003-03-25 Lucent Technologies Inc. Tunable liquid microlens
US6715876B2 (en) 2001-11-19 2004-04-06 Johnnie E. Floyd Lens arrangement with fluid cell and prescriptive element
US6860601B2 (en) 2002-02-06 2005-03-01 John H. Shadduck Adaptive optic lens system and method of use
US6935743B2 (en) 2002-02-06 2005-08-30 John H. Shadduck Adaptive optic lens and method of making
JP2005522162A (en) 2002-03-18 2005-07-21 エスアールアイ インターナショナル Electroactive polymer devices that move fluids
US6864951B1 (en) 2002-05-08 2005-03-08 University Of Central Florida Tunable electronic lens and prisms using inhomogeneous nano scale liquid crystal droplets
US20040001180A1 (en) 2002-07-01 2004-01-01 Saul Epstein Variable focus lens with internal refractive surface
US6966649B2 (en) 2002-08-12 2005-11-22 John H Shadduck Adaptive optic lens system and method of use
EP1581832A1 (en) 2002-12-30 2005-10-05 Koninklijke Philips Electronics N.V. Optical device comprising a polymer actuator
US6891682B2 (en) 2003-03-03 2005-05-10 Lucent Technologies Inc. Lenses with tunable liquid optical elements
US6930817B2 (en) 2003-04-25 2005-08-16 Palo Alto Research Center Incorporated Configurable grating based on surface relief pattern for use as a variable optical attenuator
US7079203B1 (en) 2003-06-23 2006-07-18 Research Foundation Of The University Of Central Florida, Inc. Electrically tunable polarization-independent micro lens using polymer network twisted nematic liquid crystal
JP2005092175A (en) 2003-08-08 2005-04-07 Olympus Corp Variable optical-property optical element
WO2005040909A1 (en) 2003-10-09 2005-05-06 E-Vision, Llc Improved hybrid electro-active lens
US6859333B1 (en) 2004-01-27 2005-02-22 Research Foundation Of The University Of Central Florida Adaptive liquid crystal lenses
DE102004011026A1 (en) 2004-03-04 2005-09-29 Siemens Ag Adaptive optical element with a polymer actuator
CN101069106A (en) 2004-03-31 2007-11-07 加利福尼亚大学校务委员会 Fluidic adaptive lens
GB0407414D0 (en) 2004-04-01 2004-05-05 1 Ltd Variable focal length lens
JP2006090189A (en) * 2004-09-22 2006-04-06 Omron Healthcare Co Ltd Air pump, pump system, electronic sphygmomanometer and massaging machine
WO2006088514A2 (en) 2004-11-05 2006-08-24 The Regents Of The University Of California Fluidic adaptive lens systems with pumping systems
US8885139B2 (en) 2005-01-21 2014-11-11 Johnson & Johnson Vision Care Adaptive electro-active lens with variable focal length
US7142369B2 (en) 2005-01-21 2006-11-28 Research Foundation Of The University Of Central Florida, Inc. Variable focus liquid lens
US7697214B2 (en) 2005-05-14 2010-04-13 Holochip Corporation Fluidic lens with manually-adjustable focus
JP4697786B2 (en) 2005-08-23 2011-06-08 セイコープレシジョン株式会社 Variable focus lens, and focus adjustment device and imaging device using the same
US7768712B2 (en) 2005-10-28 2010-08-03 J & J Technologies Limited Variable focus lens
CN101341606A (en) 2005-12-20 2009-01-07 皇家飞利浦电子股份有限公司 Camera diaphragm and lens positioning system employing a dielectrical polymer actuator
EP1816493A1 (en) 2006-02-07 2007-08-08 ETH Zürich Tunable diffraction grating
CN101427160A (en) * 2006-08-10 2009-05-06 松下电器产业株式会社 Varifocal lens device
CN101501534A (en) 2006-08-15 2009-08-05 皇家飞利浦电子股份有限公司 Variable focus lens
JP2008058841A (en) 2006-09-02 2008-03-13 Wakayama Univ Variable shape liquid type varifocal lens
CN101600976B (en) 2006-10-11 2011-11-09 珀莱特公司 Design of compact adjustable lens
KR20080043106A (en) 2006-11-13 2008-05-16 삼성전자주식회사 Optical lens and manufacturing method thereof
CN101197402B (en) * 2006-12-08 2010-09-29 鸿富锦精密工业(深圳)有限公司 Led
US7729068B2 (en) 2007-02-27 2010-06-01 Konica Minolta Holdings, Inc. Polymer actuator and optical unit
EP2034338A1 (en) 2007-08-11 2009-03-11 ETH Zurich Liquid Lens System
US7906891B2 (en) * 2008-02-05 2011-03-15 Sony Ericsson Mobile Communications Ab Light control of an electronic device
FR2930352B1 (en) 2008-04-21 2010-09-17 Commissariat Energie Atomique IMPROVED MEMBRANE, IN PARTICULAR FOR A DEFORMABLE MEMBRANE OPTICAL DEVICE
WO2010015093A1 (en) 2008-08-08 2010-02-11 Optotune Ag Electroactive optical device
FR2938349B1 (en) 2008-11-07 2011-04-15 Commissariat Energie Atomique OPTICAL DEVICE WITH DEFORMABLE MEMBRANE WITH IMPROVED ACTUATION
WO2010078662A1 (en) 2009-01-09 2010-07-15 Optotune Ag Electroactive optical device

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20070087564A1 (en) * 1998-10-14 2007-04-19 Stuart Speakman Method of forming an electronic device
US20020102102A1 (en) * 2001-01-30 2002-08-01 Yoji Watanabe Focal-length adjusting unit for photographing apparatuses
US20060256429A1 (en) * 2003-10-23 2006-11-16 Andreas Obrebski Imaging optics with adjustable optical power and method of adjusting an optical power of an optics
US20080144185A1 (en) * 2006-12-15 2008-06-19 Hand Held Products, Inc. Apparatus and method comprising deformable lens element

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20160351785A1 (en) * 2015-05-28 2016-12-01 Honda Motor Co., Ltd. Electrostrictive element
US10020439B2 (en) * 2015-05-28 2018-07-10 Honda Motor Co., Ltd. Electrostrictive element
DE102015226173A1 (en) * 2015-12-21 2017-06-22 Robert Bosch Gmbh Optical imaging system with a deformable due to electrical and / or magnetic forces lens
RU2750110C2 (en) * 2016-11-21 2021-06-22 Конинклейке Филипс Н.В. Optical beam processing device
RU2769092C2 (en) * 2016-11-21 2022-03-28 Конинклейке Филипс Н.В. Optical beam processing device
US20190049750A1 (en) * 2017-08-08 2019-02-14 International Business Machines Corporation Dielectric electro-active polymer contact lenses
US10663762B2 (en) * 2017-08-08 2020-05-26 International Business Machines Corporation Dielectric electro-active polymer contact lenses

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JP5456040B2 (en) 2014-03-26
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US20110149410A1 (en) 2011-06-23
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US8797654B2 (en) 2014-08-05

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