Introduction to Adaptive Lenses E-Book

Hongwen Ren

• Herausgeber: John Wiley & Sons
• Kategorie: Wissenschaft und neue Technologien
• Serie: Wiley Series in Pure and Applied Optics
• Sprache: Englisch

Seitenzahl: 464

Veröffentlichungsjahr: 2012

Beschreibung

Presents readers with the basic science, technology, and applications for every type of adaptive lens

An adaptive lens is a lens whose shape has been changed to a different focal length by an external stimulus such as pressure, electric field, magnetic field, or temperature. Introduction to Adaptive Lenses is the first book ever to address all of the fundamental operation principles, device characteristics, and potential applications of various types of adaptive lenses.

This comprehensive book covers basic material properties, device structures and performance, image processing and zooming, optical communications, and biomedical imaging. Readers will find homework problems and solutions included at the end of each chapter—and based on the described device structures, they will have the knowledge to fabricate adaptive lenses for practical applications or develop new adaptive devices or concepts for advanced investigation.

Introduction to Adaptive Lenses includes chapters on:

• Optical lenses

• Elastomeric membrane lenses

• Electro-wetting lenses

• Dielectrophoretic lenses

• Mechanical-wetting lenses

• Liquid crystal lenses

This is an important reference for optical engineers, research scientists, graduate students, and undergraduate seniors.

Leseprobe

Table of Contents

Series Page

Title Page

Copyright

Preface

Chapter 1: Optical Lens

1.1 Introduction

1.2 Conventional Lens

1.3 Aberration and Resolution

1.4 Merits and Demerits of Solid Lens

1.5 Adaptive Optical Lenses

1.6 Homework Problems

References

Chapter 2: Elastomeric Membrane Lens

2.1 Polydimethylsiloxane (PDMS) Membrane

2.2 Device Structure

2.3 Actuators

2.4 PDMS Microlens Array

2.5 Solid PDMS Lenses

2.6 Hybrid Lens System

2.7 Summary and Technical Challenges

2.8 Homework Problems

References

Chapter 3: Electrowetting Lens

3.1 Introduction

3.2 Surface Tension

3.3 Contact Angle and Wetting

3.4 Basic Theory of Electrowetting

3.5 Droplet Deformation

3.6 Electrowetting Lens

3.7 Tunable electrowetting lens

3.8 Desired Properties of the Liquids

3.9 Singlet Lens with Two Liquids

3.10 Microlens Array

3.11 Remaining Challenges

3.12 Summary

3.13 Homework Problems

References

Chapter 4: Dielectrophoretic Lens

4.1 Introduction

4.2 Dielectrophoretic Force

4.3 Dielectric Liquid Materials

4.4 Singlet Lens

4.5 Microlens Array

4.6 Switchable Lens

4.7 Gravity Effect

4.8 Applications

4.9 Summary

4.10 Homework Problems

References

Chapter 5: Other Adaptive Liquid Lenses

5.1 Introduction

5.2 Mechanical-Wetting Lens

5.3 Ferrofluidic Transducer Lens

5.4 Electromagnetic Actuator Lens

5.5 Stimuli Response Hydrogel Lens

5.6 Acoustic Liquid Lens

5.7 Electrochemical Actuation Lens

5.8 Electrostatic Force Actuation

5.9 Summary

5.10 Homework Problems

References

Chapter 6: Liquid Crystal Lens

6.1 Introduction

6.2 Physical Properties

6.3 LC Device

6.4 Focal Length Equation

6.5 Curved Electrode

6.6 Strip-Patterned Electrode

6.7 Hole-Patterned Electrode

6.8 Modal Addressing

6.9 Cylindrical LC Lens

6.10 Polymer–LC composite lens

6.11 Diffractive LC Lens

6.12 LC Microlens Array

6.13 Summary

6.14 Homework Problems

References

Index

Wiley Series

For further information visit: the book web page http://www.openmodelica.org, the Modelica Association web page http://www.modelica.org, the authors research page http://www.ida.liu.se/labs/pelab/modelica, or home page http://www.ida.liu.se/~petfr/, or email the author at [email protected]. Certain material from the Modelica Tutorial and the Modelica Language Specification available at http://www.modelica.org has been reproduced in this book with permission from the Modelica Association under the Modelica License 2 Copyright © 1998–2011, Modelica Association, see the license conditions (including the disclaimer of warranty) at http://www.modelica.org/modelica-legal-documents/ModelicaLicense2.html. Licensed by Modelica Association under the Modelica License 2.

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Copyright © 2011 by the Institute of Electrical and Electronics Engineers, Inc.

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Library of Congress Cataloging-in-Publication Data:

Introduction to adaptive lenses / Shin-Tson Wu, Hongwen Ren.

p. cm.

Includes bibliographical references and index.

ISBN 978-1-118-01899-6 (hardback)

1. Lenses. 2. Optics, Adaptive. I. Ren, Hongwen, 1964- II. Title.

QC385.W83 2012

621.36—dc22

2011042254

Preface

A lens is an important optical device. It has been widely used in imaging processing, optical communication, information storage, beam steering, vision correction, 3D displays, and other scientific applications. The market of optical lenses is huge, and the demand of optical lenses has been growing continually. For a conventional solid lens, its focal length is fixed. To get a variable focal length, a lens system is required. The focal length of the lens system is changed by tuning the distance of the adjacent lenses. However, the lens system has some drawbacks: It is inconvenient, inefficient, bulky, and costly. In comparison, an adaptive lens can function as a lens system with the advantages of compact structure, high efficiency, easy operation, light weight, and low cost. On the other hand, the development of novel optical and electronic products has evoked a new concept lens. Conventional solid lenses are insufficient due to their inherent shortcomings. Due to these reasons, adaptive lenses have been investigated extensively in recent decades. Currently, various approaches for adaptive lenses have been demonstrated. Tunable-focus adaptive lenses have potential applications in cellular phone cameras, webcams, mini projectors, machine vision, eyeglasses, 3D displays, and other lab-on-a-chip devices. There is no doubt that adaptive lenses will play an increasingly more important role in the era of optical technology.

Currently, we have not found a book that systematically introduces various adaptive lenses. A few book chapters have been published, but only about a specific topic, such as liquid crystal lenses. The main objective of this book is to provide a textbook about various adaptive lenses. Through this book, readers will learn the basic science of operation mechanism, fabrication methods, device performances, and potential applications of each type of adaptive lens. This book will serve as an important reference book for research scientists, optical engineers, graduate students, and senior undergraduates who are interested in adaptive lenses and adaptive optics. The book is organized as follows: In Chapter 1 we introduce conventional solid lenses and the human eye. In comparison to solid lenses, the human eye is a perfect example of an adaptive lens. To develop adaptive lenses inspired by the human eye, we then introduce elastic membrane lenses in Chapter 2, electrowetting lenses in Chapter 3, dielectric lenses in Chapter 4, other special liquid lenses in Chapter 5, and liquid crystal lenses in Chapter 6. For each type of lens, we introduce the basic operation principles, device structures, fabrication methods, actuation approaches, and optical performances. We try our best to cover all the major topics in adaptive lenses we know. We hope the readers will find this book useful and stimulating.

We are grateful to the reviewers of our book proposal for their useful suggestions and comments. We would like to thank our previous group members Drs. Yun-Hsing Fan, Yi-Hsin Lin, and James Lin, for generating new knowledge included in this book. Special thanks go to Ph.D. student Ms. Su Xu for providing us drawings and her latest experimental results. We are also indebted to our colleagues and friends for their stimulating discussions and to our funding agencies (DARPA, AFOSR, and NRF of Korea) for the financial support. Finally, we are grateful to our family members (Guiying Jin, Daqiu Ren, David Ren, Choyan Wu, Janet Wu, and Benjamin Wu) for their spiritual support, understanding, and constant encouragement.

Hongwen Ren

Shin-Tson Wu

Chapter 1

Optical Lens

1.1 Introduction

Figure 1.1 Property of light as (a) a wave and (b) particles.

To human eyes, the visible wavelength of a light wave is distributed in a range from ∼ 380 to ∼ 780 nm. Each color has a different wavelength. Red has the longest wavelength and violet has the shortest wavelength. When all the waves are seen together, they make white light.

When light interacts with matter, several phenomena could take place, such as reflection, refraction, absorption, diffraction, interference, and polarization (2). In order to control or modulate light to achieve these optical properties, various optical devices have been developed. For example, we have mirrors to reflect light, eyeglasses to see better, telescopes to see farther, and microscopes to see objects hundreds or thousands of times larger than they actually are. Light can also be used for medicine and communication. The light from a laser can be used to perform tissue surgery. Many internet and telephone cables are now being replaced by optical fibers, which carry an enormous amount of information in a small space (3).

Many different optical devices have been developed. There is no doubt that the lens is the most widely used optical device. The lens has been studied and developed for a long history. The oldest man-made lens can be dated back to 3000 years ago. It may have been used as a magnifying glass, or as a burning glass to start fires by concentrating sunlight. Lenses have become indispensible devices in many areas. Owing to the development of optical materials, fabrication techniques, and new operation mechanisms, the performances of lenses have been improved significantly. A typical lens is made of glass, plastic, polymer, or polycarbonate. From the aspect of geometrical structure, a lens has two refraction surfaces with a perfect or approximate axial symmetry; at least one surface is a segment of a sphere. Conventional lenses are used to form images by converging or diverging the incident beam. They are used in building various optical devices and instruments, such as cameras, telescopes, microscope, projectors, optical readers, laser scanners, laser printers, fiber optical switches, and many more. Optical lenses are now the key elements in image processing, information storage, optical communication, vision correction, three-dimensional (3D) displays, and other scientific applications. The market of optical lenses is huge, and the demand of optical lenses has been growing continually. On the other hand, the development of novel optical and electronic products has evoked new concept lens. Thus, conventional solid lenses are insufficient due to their inherent shortcomings.

In this chapter, we will introduce the operation mechanism of a solid lens based on the law of light refraction. Through a lens or a lens system, the relationship between image and object are given. The merits and demerits of the lens or lens system are discussed. Inspired from the structure of human eye and human eye's operation mechanism, two possible ways of realizing an eye-like lens are anticipated.

1.2 Conventional Lens

1.2.1 Refraction of Light

Figure 1.2 The refraction of light at the interface of two different mediums.

The angles of incidence and refraction are measured relative to a line perpendicular to the boundary between the media called the normal. The media that the light passes from and to are transparent. The light will bend based on the following relationship, called Snell's law:

1.1

where n1 is the refractive index of medium 1, θi is the angle of incidence between the incident ray and the normal, n2 is the refractive index of medium 2, and θr is the angle of refraction between the refracted ray and the normal.

When a beam of light with parallel rays enters medium 2 at a tilted angle, the rays are bent with the same refraction angle without crossing, as shown in Figure 1.3a. As a comparison, if the surface is polished with a spherical shape, then the parallel rays of the beam are refracted with different refraction angles. Let us suppose n1 < n2, the rays come together at a point in the medium on the axis, as shown in Figure 1.3b. The point where the rays focus together is called the focal point. The distance from the focal point to the apex O of the curved surface is called the focal length. The medium has the ability to focus light because of its curved surface. Similarly, an optical lens has the ability to focus light because it employs at least one curved surface.

Figure 1.3 A beam of light passing through a medium with (a) a flat surface and (b) a spherical surface.

1.2.2 A Simple Lens

A simple lens or singlet lens is a lens consisting of a single element. A simple lens has two refraction surfaces with a perfect or approximate axial symmetry. Several types of lenses, such as spherical lens, gradient index of refraction (GRIN) lens, ball lens, and Fresnel lens, have been used in building optical instruments (2, 4). Among them, the spherical lenses are the most commonly used ones. For a spherical lens, at least one of its surfaces exhibits a spherical shape. According to the curvature of the surfaces, they can be classified into five basic types: plano-convex, bi-convex, plano-concave, bi-concave, and convex–concave (meniscus), as shown in Figure 1.4. Plano-convex and bi-convex lenses have positive optical power. They will converge a parallel input beam into a real focal point at some distance behind the lens. Plano-concave and bi-concave elements have negative power. They will diverge a parallel input beam from a virtual point in front of the lens element. Convex–concave lenses can be either positive or negative, depending on the two surface curvatures and the thickness of the element. The operation principle of a lens (either by converging or diverging a beam of light) can be explained by Snell's law. Here, we choose a bi-convex lens, as an example, for locating an image and giving the lens focus equation. To get a perfect geometrical image, the bi-convex lens is considered as a thin lens and the rays satisfy the paraxial condition. Figure 1.5 illustrates the method of locating the image of an object placed in front of the lens. The distance between the object and the lens is SO. One can locate the image by just tracing ray 1 and ray 2 from the top of the object. Ray 1 from the top of the object is parallel to the principal axis. After the ray is refracted through the lens, this ray passes through the focal point of the lens. Ray 2 is the undeviated ray through the center of the lens. This ray

intersects with ray 1 at a point at the top of the image. This intersection point of ray 1 and ray 2 shows the location of the image on the principal axis at I. The distance from the image to the lens center is SI. In Figure 1.5, the focal length f is a function of the object distance SO and the image distance SI from the lens center. Their relationship is expressed by

1.2

Equation (1.2) is the basic equation for thin lenses. It applies to other single lenses shown in Figure 1.4. Considering that the lens is a thin lens, the focal length of the lens is dependent on the lens geometrical structure and the refraction index of the lens material.

Figure 1.4 Five basic shapes of simple lenses.

Figure 1.5 Object and image location for a thin lens.

Figure 1.6 shows a bi-convex lens with the defined geometrical surface. The index of refraction of the lens material is n, the radius of the left surface curvature is R1, and the radius of the right surface curvature is R2. If the lens is thin enough (d → 0), then using Gaussian's approximation, we have the very useful thin lens equation (f), often referred to as the Lensmaker's formula:

1.3

Figure 1.6 A bi-convex lens with marked parameters.

1.2.3 A Compound Lens

From equation (1.3), both surface curvature and refraction index of the lens cannot be changed arbitrarily. To get a variable focal length, a compound lens is required. A compound lens is a collection of at least two simple lenses which are arranged one after another with a common axis. The compound lenses are commonly found in cameras and other optical instruments. Figure 1.7 shows a compound lens with two convex lenses separated by a distance d, where F1 is the focal point of lens L1 and F2 is the focal point of lens L2. Such a compound lens still obeys the law of refraction. If the two lenses are separated in the air by a distance d which is not too much greater than the sum of the two focal lengths, then this combination behaves as a single lens. One can use an effective focal length f to express the focal length of the two lenses. The effective focal length for the combined system is given by

1.4

where f1 and f2 are the focal lengths of lens (L1) and lens (L2), respectively. From equation (1.4), when the distance d is varied, the effective focal length f will be changed correspondingly. Considering the optical performance of the compound system, the distance d cannot be changed in a wide range. As a result, the associated change in focal length is rather limited. For practical applications, three or more lenses are necessary to get a wide range of focal length change by adjusting the distances among them.

Figure 1.7 A compound lens system.

1.3 Aberration and Resolution

1.3.1 Paraxial Optics

When an object is placed in front of a medium that has a spherically curved surface, an image is formed because the light rays are focused by the curved surface. To get a clear image, some conditions should be satisfied. To study what these conditions are, let us analyze the medium with the simplest structure as Figure 1.3b shows. To define the parameters clearly, we redraw the figure as Figure 1.8. In Figure 1.8,

C is the center of the spherical surface.

S is the position of the point source.

P is the position of the image.

S

o

is the distance of the object from the surface along the optical axis.

S

i

is the distance from the surface to the image.

Figure 1.8 Refraction at a spherical surface.

A ray from the point source S strikes the curved surface at A. If n1 < n2, the light enters the medium and is bent toward the normal. If θi and θR are small and satisfy sinθ ≈ θ (paraxial approximation), then equation (1.1) can be simplified as

1.5

1.6

1.7

where R is the radius of the curvature. Equation (1.7) is called Gauss's equation. If Si → ∞, then So is at the focal point, and the focal length f can be written as

1.8

1.9

1.10

From equations (1.3), (1.9), and (1.10), the sum of equation (1.9) and equation (1.10) is the same as equation (1.3). From the above deduction, paraxial optics applies when rays are close to the optical axis, that is, the paraxial rays. Based on paraxial approximation, one can determine their points of convergence. In principle, these points coincide with the points of convergence of an aberration-free system. Gaussian approximation does not provide direct information about image aberrations, so it is easy for us to find the location of the paraxial focus of an optical surface, or element. While deriving equation (1.5), we only keep the first-order terms during Taylor's expansion. Thus, paraxial optics is also called first-order optics.

1.3.2 Aberration

Based on Gauss's approximation, one can construct images by using graphical methods. From Figure 1.8, point S forms a “perfect” image without any aberration. But in reality it is not exactly true, because the paraxial approximation, sinθ ≈ θ, is somewhat unsatisfactory if rays from the periphery of a lens are considered. Images formed by real lenses are never exactly identical to the predictions of the simple paraxial ray methods mentioned above. According to Snell's law, equation (1.1) can be expanded by the following form (5):

1.11

From equation (1.11), the paraxial approximation only keeps the θ terms (first-order optics). If the θ3 terms are included, then equation (1.7) will have a more complicated form:

1.12

The additional terms in the brackets of equation (1.12) represent the deviation from the first-order theory, and quantify the aberration of the lens. By using a monochromatic light, the aberrations are usually divided into following five broad groups (2, 6).

1.3.2.1 Spherical Aberration (SA)

Spherical aberration (SA) is an image imperfection that is due to the spherical lens shape. For a lens made with spherical surfaces, rays that are parallel to the optic axis but at different distances from the optic axis fail to converge to the same point. The peripheral light rays are bent more than the central ones as shown in Figure 1.9. For a single, convex lens, light that strikes the lens close to the optical axis is focused at position a. The light that traverses the margins of the lens comes to a focus at a position b closer to the lens. The difference between the focal points for rays that are close to the axis and for rays that strike the lens near its edge is called spherical aberration. Positive spherical aberration means that rays near the edge of the lens have an effective focal point that is closer to the lens than rays that strike the lens near the axis. Negative spherical aberration means that rays near the edge of the lens have an effective focal point that is at a greater distance from the lens than rays that strike the lens near the axis.

Figure 1.9 Schematic representation of spherical aberration.

Since the effective focal point determines the position of the image for any object, if the rays are separated into concentric zones, rays in different zones will have different focal points on its principal axis; thus several images can be formed by the lens. When these images are received in one screen, the images are overlapped and the observed image is blurred. Spherical aberration obviously increases with the diameter of the lens, and it can be minimized by limiting the opening of the lens so that only rays in the paraxial region can pass through it.

1.3.2.2 Coma

Coma aberration is similar to spherical aberration. It is an image degrading aberration associated with a point even a short distance from the axis. When parallel rays pass through a lens at an oblique angle (θ), as shown in Figure 1.10, the rays cannot be focused as a point, but as a comet-shaped image. Coma can be improved by stopping down the lens.

Figure 1.10 Schematic representation of coma.

1.3.2.3 Astigmatism

Astigmatism is an aberration of off-axis rays that causes radial and tangential lines in the object plane to focus sharply at different distances in the image space. This effect is explained in Figure 1.11. Let us consider P as the object point. Four rays from the P point strike on the lens border. The top ray is labeled PA and the bottom ray is labeled PB. The APB plane containing both the chief ray and the optical axis is called tangential (or meridianal) plane. Rays in the tangential plane converge to a sharp image PT if spherical aberration is corrected. The right ray is labeled PC and the left ray is labeled PD. The CPD plane containing the chief ray is called the sagittal plane. This plane is perpendicular to the tangential plane. For the rays in the CPD plane, they produce a sharp image PS if coma is not considered. Light rays lying in the tangential and sagittal planes are refracted differently and both sets of rays intersect the chief ray at different image points, termed the tangential line segment PT (tangential focal plane) and the sagittal line segment PS (sagittal focal plane). These rays fail to produce a sharp focused point.

Figure 1.11 Schematic description of astigmatism aberration.

1.3.2.4 Field Curvature

Even if all of the aforementioned aberrations could be eliminated, this effect would remain. It arises because the image plane is not really a plane but a spherical surface. Figure 1.12 illustrates this effect. When a straight object PQ is placed in front of a lens, the formed image P′Q′ is curved. This is because the outer ray has a closer focus than the inner ray, causing the rays through the center of the lens to intersect the rays through the foci as shown. Constructing intermediate points between P and Q and their images subsequently shows curvature. When field curvature is present, close objects seem to have an inward curve, and far away objects seem to have an outward curve. It is possible to correct this effect using a combination of a positive lens and a negative lens that are positioned closely, and this is usually done in camera lenses.

Figure 1.12 Schematic representation of field curvature.

1.3.2.5 Distortion

This effect is caused by variation in magnification of the image across the field of view. When the magnification of a lens differs at the edge of the lens and at the center, the image of a square object will be abnormally curved. Figure 1.13 illustrates two kinds of distortion.

Figure 1.13 Two types of distortion. (a) Pincushion and (b) barrel.

In Figure 1.13a, the lens has too much magnification at its edges, causing a surfeit of magnification of the square at the corners. This is commonly called pincushion distortion, or positive distortion. In Figure 1.13b, the lens has too little power at its edges, causing a barrel, or negative distortion.

Except for the aforementioned five aberrations using a monochromatic light, when a light contains multiple wavelengths, the lens will produce chromatic aberration. When this kind of light propagates in a medium, the refractive index is wavelength-dependent; that is, the shorter wavelengths will bend more than the longer one. Therefore, a lens will not focus different colors in exactly the same place. It is possible to minimize this aberration by using two lenses made of different materials so that variation in the refractive index of one lens is canceled by the opposite variation of the other one.

1.3.3 Resolution

The observed image as shown in Figure 1.5 is not perfect due to the lens aberration. In a normal case, aberrations always exist in a simple lens or a compound lens system. The lens aberration will degrade the quality of the image. As mentioned above, spherical aberration, coma, astigmatism, field curvature, and distortion are the main aberrations for a monochromatic light. If the light contains multiple wavelengths, then the lens will produce chromatic aberration. In most cases, it does not make much sense by just evaluating only one kind of aberration. On the other hand, it will be complicated and sometimes it is impossible to evaluate all the aberrations for a lens or a compound lens at the same time, especially when the lens aperture is very small or micro-sized.

Nowadays, the quality of most optical systems is judged by the physical measures of diffraction pointed spread function (PSF), phase transfer function (PTF), or modulation transfer function (MTF). Since MTF is a direct measure of how well the various details in the object are produced in the image, MTF has become the most widely accepted criterion for specifying and judging an image quality. MTF is a quantity representing a relationship between the sample and the resultant image. To define MTF, rectangular black and white bars with specified frequency is chosen, as shown in Figure 1.14.

Figure 1.14 Black and white gratings with low (left) and high frequencies (right).

The frequency content is measured in line pairs/mm. One cycle contains one black line and one white line. We can measure the amount of light coming from each. The maximum amount of light will come from the white bars, and the minimum amount will from the black bars. If the light is measured in terms of radiances, the modulation (or contrast) M of a spatial frequency (ν) is given by

1.13

where Imax and Imin stand for the maximum and minimum radiance. When modulation is defined in terms of light, it is frequently referred to as Michelson contrast. Now, let us assume that we have a square-wave grating of a specific frequency (v) and modulation, and this stimulus is passed through a lens. The modulation of the image can now be measured. The MTF is defined as the ratio of image modulation to object modulation, or

1.14

Figure 1.15 MTF plot as a function of spatial frequency for three different cases.

To measure MTF, a resolution test target (such as the US Air Force three-bar test target) is widely used as the object. The pattern of one resolution test target is shown in Figure 1.16 as an example. The left-hand chart with a white background is called positive version. The right-hand chart with a black background is called the negative version. The target consists of “six” groups in three layers of patterns. The largest groups, forming the first layer, are located on outer sides. The smaller layers repeat the same pattern but are progressively smaller toward the center. Each group consists of six elements. An element consists of two patterns at right angles for testing both tangential and sagittal resolution. Each pattern consists of three black lines and two white lines of equal width, with line length five times the width. Element size decreases geometrically as the sixth root of two, causing the spatial frequency to double for six element size reductions. The resolution is defined by the group and element just before the black and white bars start blending together. The resolution is expressed as

1.15

At the scale of the original target, the spatial frequencies range from 0.25 line pairs/mm to 228 line pairs/mm. In the following chapters, MTF (or resolution) will be the frequently used parameter to evaluate the performance of various adaptive lenses.

Figure 1.16 US Air Force 1951 three-bar resolution test target.

1.4 Merits and Demerits of Solid Lens

Optical lenses made of solid materials usually exhibit very good optical performances. Some key features are highlighted as follows:

Solid lenses have several other advantages, such as broadband, high transmittance by coating a transmissive film on the lens surfaces, and high stability without the concerns of temperature change and mechanical vibration. However, solid lens has some inherit issues. For instance, the surface profile of a singlet lens is fixed once the lens is produced. To change the focal length, two or more lenses are required, thus the system is bulky and heavy. It is inefficient to adjust the focal length of the compound lens system. The dynamic response is not fast. The driving mechanism of the camera lens system is mainly mechanical.

1.5 Adaptive Optical Lenses

For humans, the eye is the window to the world. When light rays travel inside the eyes, we can see objects both far and near. The eye is the most important sense organ to us. Approximately 90% of information received is through the eyes. The human eye is enormously complicated—a perfect and interrelated system of about 40 individual subsystems. To know how it works and what the performances it has, we need to know the human eye structure first.

1.5.1 Eye Structure

Figure 1.17 shows a simplified diagram of the human eye. The human eye is about 2.5 cm in diameter, and the pressure of the fluid within it maintains its near-spherical shape. The eye as a whole behaves like a thick lens. We consider here only the physics of various parts of the eye.

Figure 1.17 Side-view structure of the human eye.

The major parts of the human eye are cornea, pupil, iris, lens, ciliary body, vitreous humor, retina, and optic nerve (7, 8). When the eye focuses on an object, light passes through the cornea and is regulated by the pupil opening. Light then passes through the pupil, to the lens, and further to the vitreous humor. Subsequently, the light reaches the retina. The iris is used to control the size of the pupil, so that the amount of light enters to the lens can be tuned. The retina is the light-sensitive part of the eye. Its surface is coated with millions of rods and cones (9). The rods are sensitive to very low levels of light, but are monochromatic and cannot detect color. The cones contain three types of cones that can detect red, green, and blue lights, respectively. When these rods and cones are struck by light, they undergo a chemical reaction.

A person can view a wide range of colors because these cones work collectively to combine their respective colors to produce new colors. As these cones work together, colored signals are sent to the optic nerve and the eye's duty is finished. As the information is passed on to the optic nerve, it produces sensations of color in the visual centers of the brain.

1.5.2 Lens Character

From Figure 1.17, the lens has a bio-convex shape. It is located just behind the iris. It is held in position by zonules extending from an encircling ring of muscle. When the ciliary muscle is relaxed, the diameter of the lens curvature increases. As a result, the zonules are under tension, and the lens is flattened. When the ciliary muscle contracts, the diameter of the lens curvature decreases, the zonules relax, and the lens becomes more convex. The changes of the lens shape enable the eye to adjust its focus between far objects and near objects. The lens with changed shape for distance vision and close vision is briefly illustrated in Figure 1.18. We can see that a singlet lens can change its focal length adaptively. Such a lens functions as a compound lens or a lens system.

Figure 1.18 Lens for far object (left) and near object (right) vision by changing the lens shape.

1.5.3 Performances

A healthy human eye perform the following functions:

A.Broadband A typical human eye responds to wavelengths from about 390 to 750 nm. In terms of frequency, this corresponds to a band in the vicinity of 400–790 THz. A light-adapted eye generally has a relatively high light transmittance in the 500- to 700-nm range (9).

B.Accommodation The ability of the eye to adjust its focal length is known as accommodation (10). In the eyeball, light rays passing through the cornea are bent by its curvature toward the pupil. The lens flexes to change its curvature and finish the focusing process. When an object is located at infinity, the focal length, or the distance from the lens to the retina, is about ∼ 24 mm. When the distance between the object and the eye is shorter than 25 cm, the focal length cannot be adjusted so as to form a clear image on the retina. This distance is known as the least distance of clear vision. In this case, the focal length of the lens is ∼ 22 mm.

C.Resolution Visual acuity is often measured in cycles per degree (CPD), which measures an angular resolution, or how much an eye can differentiate one object from another in terms of visual angles. Resolution in CPD can be measured by bar charts of different numbers of white/black stripe cycles. For a human eye with excellent acuity, the maximum theoretical resolution would be 1.2 arc-minute per line pair, or a 0.35 mm/line pair, at 1 m.

D.Response Time The response time means the reaction time of accommodation responding to sudden changes in focus. Research results show that the average values obtained for movement time are 0.64 sec for far-to-near accommodation and 0.56 sec for near-to-far accommodation.

E.Efficiency When a human eye moves its focus from one object to another, the adjusted focal length is very accurate without obvious defocus. In comparison with a conventional lens system which is operated mechanically, such as a camera lens system, the focal length adjustment exhibits high efficiency. The operation of the human eye belongs to adaptive focus rather than mechanical focus.

In addition to the above mentioned properties, the human eye has some other unique properties, such as multiple axes, rotatable movement, and wide field of vision angle (greater than 90° in the temporal field) (7).

1.5.4 The Eye-Inspired Lens

A healthy human eye exhibits high optical performances. It is a wonderful optical device. Such an optical device has inspired many scientists to develop eye-like adaptive lenses. One example is modern cameras that operate on the same basic principle as our eyes. In the past decades, various adaptive lenses have been developed. They can be roughly classified into two categories: surface profile change and refractive index change.

1.5.4.1 Surface Profile Change

Like a human eye, most diverging or converging light of adaptive lenses is due to the shape deformation. Usually the material used for the lens is elastic solid or fluidic liquid. Figure 1.19 shows the side-view structures of two different approaches for deforming the shape of a lens. Suppose the lens is placed in horizontal direction and its center locates on x axis. In Figure 1.19a, the volume of the lens keeps constant. In the original state, the aperture (diameter) of the lens is ab (the dashed line). After deformation, the aperture of the lens becomes a′b′ (the solid line). For this kind of lens, both surface curvature and the lens aperture change. For example, an aperture stretchable elastomeric solid lens (11, 12), an electrowetting lens (13), and a dielectric liquid lens (14, 15) are this kind of lens. In Figure 1.19b, the aperture of the lens (ab) does not change, but the volume of the lens increases (the solid curve) or decreases (the dashed curve). Therefore, the shape of the lens surface will change accordingly. Conventional elastic membrane lens belongs to this kind of lens. In Chapters 2, 3, and 4, we will describe some important lenses that work based on these two principles.

Figure 1.19 Two basic approaches for deforming a lens shape.

1.5.4.2 Refractive Index Change

Unlike the lens with a shape change, a lens can also exhibit a variable focal length due to the change of refractive index. Figure 1.20 depicts the variable refractive index of the lens material across the lens aperture. Let us assume that the refractive index of the material can be varied by an external voltage. In the original state, the material gives a uniform refractive index distribution across the lens aperture, the flat line as Figure 1.20 shows. When an external voltage is applied to the material, it gives a refractive index with gradient distribution across the lens aperture, as shown in the curved line in Figure 1.20. Devices with such a refractive index change will behave as a lens. Liquid crystal (LC) is the material that can realize such a refractive index distribution (16, 17). In Chapter 6, we will describe the performances of tunable focus LC lenses based on the principle of refractive index redistribution.

Figure 1.20 Distribution of refraction index across the lens aperture.

In summary, light has wave and particle dual natures. Light manifests in many forms, such as reflection, refraction, diffraction, interference, or polarization when it enters a new medium. According to Snell's law, when the surface of a new medium is curved, light will converge or diverge depending on whether its refractive index is larger or smaller than that of the previous medium. A lens can converge or diverge light because it has at least one curved surface.

Solid lenses made of glass, plastic, polymer, or polycarbonate have a fixed focal length. To change the focal length, a compound lens with two or more lenses is required. The focal length of the lens system can be adjusted by varying the distance between the lenses. Such a lens system offers high image quality, but it is bulky, heavy, inefficient, and costly.

Aberrations are commonly present with a lens or a lens system. To evaluate the lens performance, a convenient method is to use the resolution target to test the image quality.

The human eye is a naturally formed adaptive optic lens. A healthy human eye can arbitrarily vary its focal length and also exhibits many advantages over a conventional solid lens. Inspired by the human eye, various adaptive lenses based on the shape change of a surface profile and refractive index change of the lens material have been demonstrated. Some examples will be given in detail in the following chapters.

1.6 Homework Problems

References

1. A. C. Melissinos, Experiments in Modern Physics, Academic Press, New York, 1966.

2. E. Hecht, Optics, 4th ed., Addison Wesley, Reading, MA, 2002.

3. A. Al-Azzawi, Photonics, Principles and Practices, CRC Press, New York, 2006.

4. J. W. Blaker, Optics I: Lenses, Mirrors, and Optical Instruments, Barnes & Noble, New York, 1969.

5. P. Dienes, The Taylor Series; An Introduction to the Theory of Functions of a Complex Variable, Dover, New York, 1957.

6. R. R. Shannon, The Art and Science of Optical Design, Cambridge University Press, New York, 1977.

7. D. D. Atchison and G. Smith, Optics of the Human Eye, Oxford University Press, New York, 2000.

8. C. H. Graham, Vision and Visual Perception, Wiley, New York, 1965.

9. S. J. Williamson and H. Z. Cummins, Light and Color in Nature and Art, Wiley, New York, 1983.

10. F. M. Toates, Accommodation function of the human eye, Physiol. Rev. 52, 828 (1972).

11. R. A. Schachar, Variable focus lens by small changes of the equatorial lens diameter, US patent 6,493,151 (2002).

12. J. M. Choi, H.-M. Son, and Y.-J. Lee, Biomimetic variable-focus lens system controlled by winding-type SMA actuator, Opt. Express 17, 8152 (2009).

13. F. Mugele and J. C. Baret, Electrowetting: from basics to applications, J. Phys. Condens. Matter 17, R705 (2005).

14. C. C. Cheng, C. A. Chang, and J. A. Yeh, Variable focus dielectric liquid droplet lens, Opt. Express 14, 4101 (2006).

15. H. Ren, H. Xianyu, S. Xu, and S. T. Wu, Adaptive dielectric liquid lens, Opt. Express 16, 14954 (2008).

16. S. Sato, Liquid-crystal lens-cells with variable focal length, Jpn. J. Appl. Phys. 18, 1679 (1979).

17. D. K. Yang and S. T. Wu, Fundamentals of Liquid Crystal Devices, Wiley, Hoboken, NJ, 2006.

Chapter 2

Elastomeric Membrane Lens

A lens made of liquid but with at least one elastomeric membrane as its flexible boundary or all-soft elastomeric material is referred to as an elastic memb rane lens. When the volume of the lens is changed or redistributed, the shape of the lens surface profile can be changed accordingly. As a result, the reshaping of the lens surface causes the focal length of the lens to change without physical motion. The change of the lens surface is exhibited in a manner analogous to that of a human eye. The development of elastic membrane lens has been going for more than four decades. The earliest patent regarding the liquid lens with variable focal length was issued in 1968 (1). Since then, various actuation approaches, such as syringe (2–6), servo motor (7–9), piezoelectric (10–13), artificial muscle (14), and voice coil actuator (VCA) (15, 16) have been proposed to deform the shape of the lens surface.

In this chapter, we will first introduce the device structures and properties of the elastic membrane lenses. Next, we will compare the merits and demerits of each approach. The applications of the elastic membrane lenses will also be described. Finally, the remaining technical challenges of the membrane liquid lenses will be summarized.

2.1 Polydimethylsiloxane (PDMS) Membrane

In an elastomeric membrane lens, the elastic (or distensible) membrane is a key part of the lens. An ideal membrane material should have following properties:

1.High Transmission The membrane should have high transmittance and small color dispersion in the entire visible spectral region. Meanwhile, the membrane surface should be very smooth in either relaxed or stretched states.

2.Large Distension When a pressure is exerted on the membrane surface, its surface can be stretched and bulged largely without any damage. By removing the force, the distensible membrane can well recover to its original shape.

3.Chemical Property The membrane should not react with the chosen liquid. Moreover, it will not be damaged by the exposure of UV light. The lifetime of the membrane should not be a concern.

4.Physical Property When the membrane is bonded to the lens periphery, the surface of the membrane can be uniformly stressed without distortion. The material for the membrane has high melting point, no order, and nontoxicity. It will not swell or shrink under high humidity conditions. The membrane can remain stable when the surrounding temperature changes over a wide range.

Over the past years, many polymer materials have been proposed for preparing elastic membranes. However, polydimethylsiloxane (PDMS) is the preferred one for elastic membranes. Numerous reports and many patents have been disclosed for designing optical devices using PDMS. PDMS elastomers have been widely used not only in academic research, but also in practical applications because of their desirable physical and chemical properties.

2.1.1 PDMS Chemical Structure

PDMS SYLGARD_184 (Dow-Corning product) is the most common material for preparing elastomeric membranes. Sylgard 184 is a heat-curable PDMS supplied as a two-part kit consisting of pre-polymer (base) and cross-linker (curing agent) components. The manufacturer recommends that the pre-polymer and cross-linker be mixed at a 10:1 weight ratio. The base monomer is vinyl-terminated, while curing agents (cross-linking monomers) are methyl-terminated and contain silicon hydride, –OSiHCH3–, units. Mixing the two resin compounds together leads to a cross-linked polymerization. During the thermal curing process, PDMS monomers are cross-linked together to establish Si–CH2–CH2–Si linkages by reactions between the vinyl groups in the monomer and silicon hydride groups in the cross-linker. The two parts and the finally cross-linked chemical structures of PDMS are shown in Figure 2.1. After fully polymerization and cross-linking, the PDMS material is flexible and highly transparent.

Figure 2.1 Chemical structure of the PDMS polymer due to cross-linking of part A and part B.

2.1.2 Basic Material Properties

After cross-linking, the PDMS elastomers usually exhibit following properties, as listed in Table 2.1. PDMS materials have some other merits: The physical and chemical properties of PDMS remain stable over a wide temperatures range from − 50°C to + 200°C; the surface of PDMS membrane can be very smooth, with only tens of nanometers of surface roughness.

Table 2.1 Physical Properties of PDMS Elastomer

2.1.3 Optical Transmission

Optical transmission of PDMS elastic membrane is an important factor determining the performance of a liquid lens. PDMS is commonly employed in membrane lenses because of its high optical transparency, large elongation, and biocompatibility.