Preface |
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xix | |
Acknowledgments |
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xxv | |
Author Brief Biography |
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xxvii | |
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1 | (18) |
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1.1 An Early History of Optical Systems and Optics |
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1 | (7) |
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1.1.1 Early History of Mirrors |
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1 | (1) |
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1.1.2 Early History of Lenses |
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1 | (1) |
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1.1.3 Early History of Glass Making |
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2 | (1) |
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1.1.4 Ancient History of Optics in Europe, India and China |
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2 | (1) |
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1.1.5 Optics Activities in the Middle East in 10th Century CE |
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3 | (1) |
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1.1.6 Practical Optical Systems of the Early Days |
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3 | (1) |
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1.1.7 Reading stones and Discovery of Eyeglasses |
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4 | (1) |
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1.1.8 Revival of Investigations on Optics in Europe by Roger Bacon in the 13th century CE |
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4 | (1) |
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1.1.9 Optics during Renaissance in Europe |
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4 | (1) |
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1.1.10 Invention of Telescope and Microscope |
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5 | (1) |
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1.1.11 Investigations on Optics and Optical Systems by Johannes Kepler |
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6 | (1) |
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1.1.12 Discovery of the Laws of Refraction |
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6 | (1) |
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1.1.13 Discovery of the phenomena of Diffraction, Interference and Double Refraction |
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7 | (1) |
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1.1.14 Newton's Contributions in Optics and Rømer's Discovery of Finite Speed of Light |
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7 | (1) |
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1.1.15 Contributions by Christian Huygens in Instrumental Optics and in Development of the Wave Theory of Light |
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8 | (1) |
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1.2 Metamorphosis of Optical Systems in the Late Twentieth Century |
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8 | (1) |
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1.3 Current Definition of Optics |
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9 | (1) |
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1.4 Types of Optical Systems |
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10 | (2) |
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1.5 Classification of Optical Systems |
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12 | (1) |
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1.6 Performance Assessment of Optical Systems |
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12 | (1) |
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1.7 Optical Design: System Design and Lens Design |
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13 | (1) |
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13 | (1) |
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14 | (5) |
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2 From Maxwell's Equations to Thin Lens Optics |
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19 | (42) |
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19 | (1) |
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20 | (3) |
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2.3 Characteristics of the Harmonic Plane Wave Solution of the Scalar Wave Equation |
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23 | (4) |
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2.3.1 Inhomogeneous Waves |
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26 | (1) |
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2.4 Wave Equation for Propagation of Light in Inhomogeneous Media |
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27 | (3) |
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2.4.1 Boundary Conditions |
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28 | (2) |
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2.5 Vector Waves and Polarization |
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30 | (4) |
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2.5.1 Polarization of Light Waves |
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31 | (3) |
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2.6 Propagation of Light in Absorbing/Semi-Absorbing Media |
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34 | (4) |
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2.7 Transition to Scalar Theory |
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38 | (1) |
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2.8 `Ray Optics' Under Small Wavelength Approximation |
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39 | (3) |
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2.8.1 The Eikonal Equation |
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39 | (1) |
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2.8.2 Equation for Light Rays |
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40 | (2) |
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2.9 Basic Principles of Ray Optics |
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42 | (12) |
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2.9.1 The Laws of Refraction |
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43 | (1) |
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2.9.1.1 A Plane Curve in the Neighbourhood of a Point on It |
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44 | (1) |
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2.9.1.2 A Continuous Surface in the Neighbourhood of a Point on It |
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44 | (1) |
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2.9.1.3 Snell's Laws of Refraction |
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45 | (3) |
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2.9.2 Refraction in a Medium of Negative Refractive Index |
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48 | (1) |
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2.9.3 The Case of Reflection |
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49 | (1) |
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2.9.3.1 Total Internal Reflection |
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49 | (1) |
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49 | (2) |
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2.9.5 The Path Differential Theorem |
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51 | (1) |
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2.9.6 Malus-Dupin Theorem |
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52 | (2) |
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2.10 Division of Energy of a Light Wave Incident on a Surface of Discontinuity |
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54 | (2) |
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2.10.1 Phase Changes in Reflected and Transmitted Waves |
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55 | (1) |
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56 | (1) |
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2.11 From General Ray Optics to Parabasal Optics, Paraxial Optics and Thin Lens Optics |
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56 | (2) |
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58 | (3) |
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61 | (54) |
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3.1 Raison d'etre for Paraxial Analysis |
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61 | (1) |
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3.2 Imaging by a Single Spherical Interface |
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62 | (1) |
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63 | (1) |
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3.4 Paraxial Approximation |
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64 | (11) |
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64 | (2) |
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3.4.1.1 Power and Focal Length of a Single Surface |
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66 | (1) |
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3.4.2 Extra-Axial Imaging |
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67 | (3) |
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3.4.3 Paraxial Ray Diagram |
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70 | (1) |
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3.4.4 Paraxial Imaging by a Smooth Surface of Revolution about the Axis |
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71 | (4) |
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3.5 Paraxial Imaging by Axially Symmetric System of Surfaces |
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75 | (4) |
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75 | (1) |
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3.5.2 Paraxial Ray Tracing |
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75 | (3) |
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3.5.3 The Paraxial Invariant |
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78 | (1) |
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3.6 Paraxial Imaging by a Single Mirror |
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79 | (2) |
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3.7 The General Object-Image Relation for an Axisymmetric System |
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81 | (4) |
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3.7.1 A Geometrical Construction for Finding the Paraxial Image |
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84 | (1) |
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3.7.2 Paraxial Imaging and Projective Transformation (Collineation) |
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85 | (1) |
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3.8 Cardinal Points in Gaussian Optics |
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85 | (14) |
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3.8.1 Determining Location of Cardinal Points from System Data |
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86 | (2) |
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88 | (1) |
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3.8.2.1 A Single Refracting Surface |
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88 | (1) |
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3.8.2.2 A System of Two Separated Components |
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89 | (2) |
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3.8.2.3 A Thick Lens with Different Refractive Indices for the Object and the Image Spaces |
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91 | (5) |
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3.8.2.4 A Thin Lens with Different Refractive Indices for the Object and the Image Spaces |
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96 | (1) |
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3.8.2.5 Two Separated Thin Lenses in Air |
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97 | (2) |
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3.9 The Object and Image Positions for Systems of Finite Power |
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99 | (2) |
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3.10 Newton's Form of the Conjugate Equation |
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101 | (1) |
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102 | (2) |
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104 | (1) |
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3.13 Geometrical Nature of Image Formation by an Ideal Gaussian System |
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105 | (3) |
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3.13.1 Imaging of a Two-Dimensional Object on a Transverse Plane |
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105 | (1) |
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3.13.2 Imaging of Any Line in the Object Space |
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106 | (2) |
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3.13.3 Suitable Values for Paraxial Angle and Height Variables in an Ideal Gaussian System |
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108 | (1) |
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3.14 Gaussian Image of a Line Inclined with the Axis |
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108 | (2) |
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3.15 Gaussian Image of a Tilted Plane: The Scheimpflug Principle |
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110 | (2) |
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3.15.1 Shape of the Image |
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111 | (1) |
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3.16 Gaussian Image of a Cube |
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112 | (1) |
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112 | (3) |
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4 Paraxial Analysis of the Role of Stops |
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115 | (42) |
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4.1 Aperture Stop and the Pupils |
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115 | (5) |
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4.1.1 Conjugate Location and Aperture Stop |
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117 | (3) |
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4.2 Extra-Axial Imagery and Vignetting |
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120 | (3) |
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122 | (1) |
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4.3 Field Stop and the Windows |
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123 | (6) |
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123 | (1) |
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4.3.2 Field Stop, Entrance, and Exit Windows |
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124 | (1) |
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4.3.2.1 Looking at an Image Formed by a Plane Mirror |
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124 | (1) |
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4.3.2.2 Looking at Image Formed by a Convex Spherical Mirror |
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124 | (1) |
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4.3.2.3 Imaging by a Single Lens with a Stop on It |
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125 | (1) |
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4.3.2.4 Imaging by a Single Lens with an Aperture Stop on it and a Remote Diaphragm in the Front |
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125 | (1) |
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4.3.2.5 Appropriate Positioning of Aperture Stop and Field Stop |
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126 | (1) |
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4.3.2.6 Aperture Stop and Field Stop in Imaging Lenses with No Dedicated Physical Stop |
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127 | (1) |
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4.3.2.7 Imaging by a Multicomponent Lens System |
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128 | (1) |
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4.3.2.8 Paraxial Marginal Ray and Paraxial Pupil Ray |
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129 | (1) |
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4.4 Glare Stop, Baffles, and the Like |
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129 | (1) |
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4.5 Pupil Matching in Compound Systems |
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130 | (1) |
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4.6 Optical Imaging System of the Human Eye |
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131 | (6) |
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4.6.1 Paraxial Cardinal Points of the Human Eye |
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132 | (1) |
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4.6.1.1 Correction of Defective Vision by Spectacles |
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133 | (1) |
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4.6.1.2 Position of Spectacle Lens with Respect to Eye Lens |
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133 | (1) |
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4.6.2 Pupils and Centre of Rotation of the Human Eye |
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133 | (1) |
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4.6.2.1 Position of Exit Pupil in Visual Instruments |
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133 | (3) |
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4.6.3 Visual Magnification of an Eyepiece or Magnifier |
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136 | (1) |
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4.7 Optical (Paraxial) Invariant: Paraxial Variables and Real Finite Rays |
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137 | (7) |
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4.7.1 Different Forms of Paraxial Invariant |
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138 | (1) |
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4.7.1.1 Paraxial Invariant in Star Space |
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138 | (1) |
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4.7.1.2 A Generalized Formula for Paraxial Invariant H |
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139 | (1) |
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4.7.1.3 An Expression for Power K in Terms of H and Angle Variables of the PMR and the PPR |
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139 | (1) |
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4.7.2 Paraxial Ray Variables and Real Finite Rays |
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140 | (1) |
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4.7.2.1 Paraxial Ray Variables in an Ideal Gaussian System |
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140 | (1) |
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4.7.2.2 Paraxial Ray Variables in a Real Optical System |
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141 | (1) |
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4.7.2.3 Choice of Appropriate Values for Paraxial Angles u and u |
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142 | (2) |
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4.8 Angular Magnification in Afocal Systems |
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144 | (1) |
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4.9 F-number and Numerical Aperture |
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145 | (3) |
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4.10 Depth of Focus and Depth of Field |
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148 | (5) |
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4.10.1 Expressions for Depth of Focus, Depth of Field, and Hyperfocal Distance for a Single Thin Lens with Stop on It |
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148 | (3) |
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4.10.2 General Expressions for Depth of Focus, Depth of Field, and Hyperfocal Distance for an Axisymmetric Imaging System |
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151 | (2) |
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153 | (1) |
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4.12 Stops in Illumination Systems |
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154 | (2) |
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154 | (1) |
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4.12.2 The Kohler Illumination System in Microscopes |
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155 | (1) |
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156 | (1) |
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5 Towards Facilitating Paraxial Treatment |
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157 | (22) |
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5.1 Matrix Treatment of Paraxial Optics |
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157 | (8) |
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5.1.1 The Refraction Matrix and the Translation/Transfer Matrix |
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158 | (1) |
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159 | (2) |
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5.1.3 The Conjugate Matrix |
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161 | (1) |
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5.1.4 Detailed Form of the Conjugate Matrix in the Case of Finite Conjugate Imaging |
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162 | (1) |
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5.1.4.1 Location of the Cardinal Points of the System: Equivalent Focal Length and Power |
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163 | (2) |
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5.2 Gaussian Brackets in Paraxial Optics |
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165 | (4) |
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5.2.1 Gaussian Brackets: Definition |
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166 | (1) |
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5.2.2 Few Pertinent Theorems of Gaussian Brackets |
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166 | (1) |
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5.2.3 Elements of System Matrix in Terms of Gaussian Brackets |
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167 | (2) |
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5.3 Delano Diagram in Paraxial Design of Optical Systems |
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169 | (7) |
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5.3.1 A Paraxial Skew Ray and the y, y Diagram |
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170 | (1) |
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5.3.2 Illustrative y, y Diagrams |
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171 | (1) |
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172 | (2) |
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174 | (1) |
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175 | (1) |
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176 | (3) |
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6 The Photometry and Radiometry of Optical Systems |
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179 | (16) |
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6.1 Radiometry and Photometry: Interrelationship |
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179 | (3) |
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6.2 Fundamental Radiometric and Photometric Quantities |
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182 | (4) |
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6.2.1 Radiant or Luminous Flux (Power) |
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182 | (1) |
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6.2.2 Radiant or Luminous Intensity of a Source |
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183 | (1) |
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6.2.3 Radiant (Luminous) Emittance or Exitance of a Source |
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183 | (1) |
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6.2.4 Radiance (Luminance) of a Source |
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184 | (1) |
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6.2.4.1 Lambertian Source |
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184 | (1) |
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6.2.5 Irradiance (Illuminance/Illumination) of a Receiving Surface |
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185 | (1) |
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6.3 Conservation of Radiance/Luminance (Brightness) in Optical Imaging Systems |
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186 | (1) |
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6.4 Flux Radiated Into a Cone by a Small Circular Lambertian Source |
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187 | (1) |
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6.5 Flux Collected by Entrance Pupil of a Lens System |
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188 | (1) |
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6.6 Irradiance of an Image |
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189 | (1) |
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6.7 Off-Axial Irradiance/Illuminance |
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190 | (2) |
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6.8 Irradiance/Illuminance From a Large Circular Lambertian Source |
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192 | (1) |
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6.8.1 Radiance (Luminance) of a Distant Source |
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193 | (1) |
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193 | (2) |
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7 Optical Imaging by Real Rays |
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195 | (66) |
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7.1 Rudiments of Hamiltonian Optics |
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195 | (8) |
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7.1.1 Hamilton's Point Characteristic Function |
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197 | (1) |
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7.1.1.1 Hamilton-Bruns' Point Eikonal |
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198 | (2) |
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7.1.2 Point Angle Eikonal |
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200 | (1) |
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7.1.3 Angle Point Eikonal |
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200 | (1) |
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201 | (1) |
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7.1.5 Eikonals and their Uses |
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202 | (1) |
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202 | (1) |
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7.2 Perfect Imaging with Real Rays |
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203 | (24) |
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7.2.1 Stigmatic Imaging of a Point |
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203 | (1) |
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204 | (1) |
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7.2.2.1 Finite Conjugate Points |
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204 | (2) |
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7.2.2.1.1 Real Image of an Axial Object Point at Infinity |
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206 | (3) |
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7.2.2.1.2 Virtual Image of an Axial Object Point at Infinity |
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209 | (1) |
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7.2.2.2 Cartesian Mirror for Stigmatic Imaging of Finite Conjugate Points |
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209 | (2) |
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7.2.2.2.1 Parabolic Mirror for Object/Image at Infinity |
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211 | (1) |
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7.2.2.2.2 Perfect Imaging of 3-D Object Space by Plane Mirror |
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212 | (1) |
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7.2.3 Perfect Imaging of Three-Dimensional Domain |
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212 | (1) |
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7.2.3.1 Sufficiency Requirements for Ideal Imaging by Maxwellian `Perfect' Instrument |
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213 | (2) |
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7.2.3.2 Impossibility of Perfect Imaging by Real Rays in Nontrivial Cases |
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215 | (1) |
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7.2.3.3 Maxwell's `Fish-Eye' Lens and Luneburg Lens |
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216 | (2) |
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7.2.3.3.1 A Polemic on `Perfect Imaging' by Maxwell's Fish-Eye Lens |
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218 | (1) |
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7.2.4 Perfect Imaging of Surfaces |
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219 | (1) |
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7.2.4.1 Aplanatic Surfaces and Points |
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219 | (3) |
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7.2.5 Stigmatic Imaging of Two Neighbouring Points: Optical Cosine Rule |
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222 | (1) |
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7.2.5.1 Abbe's Sine Condition |
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223 | (2) |
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7.2.5.2 Herschel's Condition |
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225 | (1) |
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7.2.5.3 Incompatibility of Herschel's Condition with Abbe's Sine Condition |
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226 | (1) |
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227 | (11) |
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227 | (1) |
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7.3.1.1 A Derivation of the Skew Ray Invariance Relationship |
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228 | (1) |
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7.3.1.2 Cartesian Form of Skew Ray Invariant |
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229 | (1) |
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7.3.1.3 Other Forms of Skew Ray Invariant |
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230 | (1) |
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7.3.1.4 Applications of the Skew Invariant |
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231 | (1) |
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7.3.1.4.1 The Optical Sine Theorem |
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231 | (1) |
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7.3.1.4.2 Relation between a Point and a Diapoint via a Skew Ray from the Point |
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232 | (1) |
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7.3.1.4.3 Sagittal Magnification Law |
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233 | (1) |
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7.3.1.4.4 Feasibility of Perfect Imaging of a Pair of Object Planes Simultaneously |
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233 | (2) |
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7.3.2 Generalized Optical Invariant |
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235 | (1) |
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7.3.2.1 Derivation of Generalized Optical Invariant |
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236 | (2) |
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7.4 Imaging by Rays in the Vicinity of an Arbitrary Ray |
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238 | (14) |
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7.4.1 Elements of Surface Normals and Curvature |
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239 | (1) |
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7.4.1.1 The Equations of the Normals to a Surface |
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239 | (1) |
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7.4.1.2 The Curvature of a Plane Curve: Newton's Method |
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240 | (1) |
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7.4.1.3 The Curvatures of a Surface: Euler's Theorem |
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241 | (2) |
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7.4.1.4 The Normals to an Astigmatic Surface |
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243 | (3) |
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7.4.2 Astigmatism of a Wavefront in General |
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246 | (1) |
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7.4.2.1 Rays in the Neighbourhood of a Finite Principal Ray in Axisymmetric Systems |
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247 | (1) |
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7.4.2.2 Derivation of S and T Ray Tracing Formulae |
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247 | (4) |
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7.4.2.3 The Sagittal Invariant |
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251 | (1) |
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7.5 Aberrations of Optical Systems |
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252 | (1) |
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253 | (8) |
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8 Monochromatic Aberrations |
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261 | (52) |
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8.1 A Journey to the Wonderland of Optical Aberrations: A Brief Early History |
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261 | (1) |
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8.2 Monochromatic Aberrations |
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262 | (26) |
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8.2.1 Measures of Aberration |
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262 | (3) |
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8.2.1.1 Undercorrected and Overcorrected Systems |
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265 | (1) |
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8.2.2 Ray Aberration and Wave Aberration: Interrelationship |
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265 | (3) |
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8.2.3 Choice of Reference Sphere and Wave Aberration |
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268 | (1) |
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8.2.3.1 Effects of Shift of the Centre of the Reference Sphere on Wave Aberration |
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268 | (2) |
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8.2.3.1.1 Longitudinal Shift of Focus |
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270 | (3) |
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8.2.3.1.2 Transverse Shift of Focus |
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273 | (2) |
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8.2.3.2 Effect of Change in Radius of the Reference Sphere on Wave Aberration |
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275 | (1) |
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8.2.3.2.1 Wave Aberration and Hamilton-Bruns' Eikonal |
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276 | (1) |
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8.2.3.2.2 Wave Aberration on the Exit Pupil |
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276 | (1) |
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8.2.4 Caustics and Aberrations |
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277 | (1) |
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8.2.5 Power Series Expansion of the Wave Aberration Function |
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278 | (4) |
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8.2.5.1 Aberrations of Various Orders |
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282 | (4) |
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8.2.5.2 Convergence of the Power Series of Aberrations |
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286 | (1) |
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8.2.5.3 Types of Aberrations |
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286 | (2) |
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8.3 Transverse Ray Aberrations Corresponding to Selected Wave Aberration Polynomial Terms |
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288 | (11) |
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8.3.1 Primary Spherical Aberration |
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288 | (1) |
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289 | (2) |
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291 | (2) |
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8.3.3 Primary Astigmatism |
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293 | (3) |
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296 | (2) |
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298 | (1) |
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8.3.6 Mixed and Higher Order Aberration Terms |
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298 | (1) |
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8.4 Longitudinal Aberrations |
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299 | (4) |
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8.5 Aplanatism and Isoplanatism |
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303 | (5) |
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8.5.1 Coma-Type Component of Wave Aberration and Linear Coma |
|
|
304 | (1) |
|
8.5.2 Total Linear Coma from Properties of Axial Pencil |
|
|
304 | (3) |
|
8.5.3 Offence against Sine Condition (OSC) |
|
|
307 | (1) |
|
8.5.4 Staeble -- Lihotzky Condition |
|
|
307 | (1) |
|
8.6 Analytical Approach for Correction of Total Aberrations |
|
|
308 | (1) |
|
|
308 | (5) |
|
|
313 | (30) |
|
|
313 | (1) |
|
9.2 Dispersion of Optical Materials |
|
|
313 | (8) |
|
9.2.1 Interpolation of Refractive Indices |
|
|
315 | (2) |
|
|
317 | (1) |
|
9.2.3 Generic Types of Optical Glasses and Glass Codes |
|
|
318 | (3) |
|
|
321 | (17) |
|
9.3.1 A Single Thin Lens: Axial Colour and Lateral Colour |
|
|
321 | (3) |
|
9.3.2 A Thin Doublet and Achromatic Doublets |
|
|
324 | (2) |
|
9.3.2.1 Synthesis of a Thin Lens of a Given Power Kd and an Arbitrary V# |
|
|
326 | (1) |
|
9.3.3 Secondary Spectrum and Relative Partial Dispersion |
|
|
327 | (3) |
|
9.3.4 Apochromats and Superachromats |
|
|
330 | (1) |
|
9.3.5 `Complete' or `Total' Achromatization |
|
|
331 | (1) |
|
9.3.5.1 Harting's Criterion |
|
|
332 | (1) |
|
9.3.6 A Separated Thin Lens Achromat (Dialyte) |
|
|
333 | (2) |
|
9.3.7 A One-Glass Achromat |
|
|
335 | (1) |
|
9.3.8 Secondary Spectrum Correction with Normal Glasses |
|
|
336 | (1) |
|
9.3.9 A Thick Lens or a Compound Lens System |
|
|
337 | (1) |
|
9.4 Chromatism Beyond the Paraxial Domain |
|
|
338 | (1) |
|
|
338 | (5) |
|
10 Finite or Total Aberrations from System Data by Ray Tracing |
|
|
343 | (26) |
|
10.1 Evaluation of Total or Finite Wavefront Aberration (Monochromatic) |
|
|
344 | (17) |
|
10.1.1 Wave Aberration by a Single Refracting Interface in Terms of Optical Path Difference (OPD) |
|
|
344 | (1) |
|
10.1.2 Rays' Own Focus and Invariant Foci of Skew Rays |
|
|
345 | (2) |
|
10.1.3 Pupil Exploration by Ray Tracing |
|
|
347 | (3) |
|
10.1.4 A Theorem of Equally Inclined Chords between Two Skew Lines |
|
|
350 | (1) |
|
10.1.5 Computation of Wave Aberration in an Axi-Symmetric System |
|
|
350 | (10) |
|
10.1.6 Computation of Transverse Ray Aberrations in an Axi-Symmetric System |
|
|
360 | (1) |
|
10.2 Measures for Nonparaxial Chromatism |
|
|
361 | (5) |
|
|
362 | (1) |
|
10.2.2 Conrady Chromatic Aberration Formula |
|
|
363 | (2) |
|
10.2.3 Image Space Associated Rays in Conrady Chromatic Aberration Formula |
|
|
365 | (1) |
|
10.2.4 Evaluation of Exact Chromatic Aberration using Object Space Associated Rays |
|
|
365 | (1) |
|
|
366 | (3) |
|
11 Hopkins' Canonical Coordinates and Variables in Aberration Theory |
|
|
369 | (28) |
|
|
369 | (1) |
|
11.2 Canonical Coordinates: Axial Pencils |
|
|
370 | (1) |
|
11.3 Canonical Coordinates: Extra-Axial Pencils |
|
|
371 | (3) |
|
11.4 Reduced Pupil Variables |
|
|
374 | (1) |
|
11.5 Reduced Image Height and Fractional Distortion |
|
|
375 | (1) |
|
|
375 | (5) |
|
11.6.1 Entrance Pupil Scale Ratios ρs and ρτ |
|
|
378 | (1) |
|
11.6.2 Exit Pupil Scale Ratios ρ's and ρ'τ |
|
|
379 | (1) |
|
11.7 Ws and Wτ from S and T Ray Traces |
|
|
380 | (5) |
|
11.8 Local Sagittal and Tangential Invariants for Extra-Axial Images |
|
|
385 | (6) |
|
11.9 Reduced Coordinates on the Object/Image Plane and Local Magnifications |
|
|
391 | (1) |
|
11.10 Canonical Relations: Generalized Sine Condition |
|
|
392 | (3) |
|
|
395 | (2) |
|
12 Primary Aberrations from System Data |
|
|
397 | (20) |
|
|
397 | (1) |
|
12.2 Validity of the Use of Paraxial Ray Parameters for Evaluating Surface Contribution to Primary Wavefront Aberration |
|
|
398 | (2) |
|
12.3 Primary Aberrations and Seidel Aberrations |
|
|
400 | (1) |
|
12.4 Seidel Aberrations in Terms of Paraxial Ray Trace Data |
|
|
401 | (10) |
|
12.4.1 Paraxial (Abbe's) Refraction Invariant |
|
|
401 | (1) |
|
12.4.2 Seidel Aberrations for Refraction by a Spherical Interface |
|
|
402 | (2) |
|
12.4.3 Seidel Aberrations in an Axi-Symmetric System Consisting of Multiple Refracting Interfaces |
|
|
404 | (1) |
|
12.4.4 Seidel Aberrations of a Plane Parallel Plate |
|
|
404 | (2) |
|
12.4.5 Seidel Aberrations of a Spherical Mirror |
|
|
406 | (2) |
|
12.4.6 Seidel Aberrations of a Refracting Aspheric Interface |
|
|
408 | (1) |
|
12.4.6.1 Mathematical Representation of an Aspheric Surface |
|
|
408 | (2) |
|
12.4.6.2 Seidel Aberrations of the Smooth Aspheric Refracting Interface |
|
|
410 | (1) |
|
12.5 Axial Colour and Lateral Colour as Primary Aberrations |
|
|
411 | (4) |
|
|
415 | (2) |
|
13 Higher Order Aberrations in Practice |
|
|
417 | (12) |
|
13.1 Evaluation of Aberrations of Higher Orders |
|
|
417 | (1) |
|
13.2 A Special Treatment for Tackling Higher Order Aberrations in Systems With Moderate Aperture and Large Field |
|
|
418 | (2) |
|
13.3 Evaluation of Wave Aberration Polynomial Coefficients From Finite Ray Trace Data |
|
|
420 | (5) |
|
|
425 | (4) |
|
|
429 | (28) |
|
14.1 Primary Aberrations of Thin Lenses |
|
|
429 | (2) |
|
14.2 Primary Aberrations of a Thin Lens (with Stop on It) in Object and Image Spaces of Unequal Refractive Index |
|
|
431 | (7) |
|
14.3 Primary Aberrations of a Thin Lens (with Stop on It) With Equal Media in Object and Image Spaces |
|
|
438 | (1) |
|
14.4 Primary Aberrations of a Thin Lens (with Stop on It) in Air |
|
|
439 | (6) |
|
14.5 Structural Aberration Coefficients |
|
|
445 | (1) |
|
14.6 Use of Thin Lens Aberration Theory in Structural Design of Lens Systems |
|
|
446 | (1) |
|
14.7 Transition from Thin Lens to Thick Lens and Vice Versa |
|
|
447 | (5) |
|
14.8 Thin Lens Modelling of Diffractive Lenses |
|
|
452 | (1) |
|
|
452 | (5) |
|
15 Stop Shift, Pupil Aberrations, and Conjugate Shift |
|
|
457 | (26) |
|
15.1 Axial Shift of the Aperture Stop |
|
|
457 | (6) |
|
15.1.1 The Eccentricity Parameter |
|
|
457 | (2) |
|
15.1.2 Seidel Difference Formula |
|
|
459 | (2) |
|
15.1.3 Stop-Shift Effects on Seidel Aberrations in Refraction by a Single Surface |
|
|
461 | (1) |
|
15.1.4 Stop-Shift Effects on Seidel Aberrations in an Axi-Symmetric System |
|
|
462 | (1) |
|
15.1.5 Stop-Shift Effects on Seidel Aberrations in a Single Thin Lens |
|
|
463 | (1) |
|
|
463 | (1) |
|
|
463 | (12) |
|
15.2.1 Relation between Pupil Aberrations and Image Aberrations |
|
|
466 | (5) |
|
15.2.2 Effect of Stop Shift on Seidel Spherical Aberration of the Pupil |
|
|
471 | (3) |
|
15.2.3 Effect of Stop Shift on Seidel Longitudinal Chromatic Aberration of the Pupil |
|
|
474 | (1) |
|
15.2.4 A Few Well-Known Effects of Pupil Aberrations on Imaging of Objects |
|
|
474 | (1) |
|
|
475 | (6) |
|
15.3.1 The Coefficients of Seidel Pupil Aberrations After Object Shift in Terms of the Coefficients of Seidel Pupil Aberrations Before Object Shift |
|
|
477 | (1) |
|
15.3.2 The Coefficients of Seidel Pupil Aberrations Before Object Shift in Terms of Coefficients of Seidel Image Aberrations Before Object Shift |
|
|
478 | (1) |
|
15.3.3 The Coefficients of Seidel Image Aberrations After Object Shift in Terms of Coefficients of Seidel Pupil Aberrations After Object Shift |
|
|
478 | (1) |
|
15.3.4 Effects of Conjugate Shift on the Coefficients of Seidel Image Aberrations |
|
|
479 | (2) |
|
15.3.5 The Bow--Sutton Conditions |
|
|
481 | (1) |
|
|
481 | (2) |
|
16 Role of Diffraction in Image Formation |
|
|
483 | (38) |
|
16.1 Raison d'etre for `Diffraction Theory of Image Formation' |
|
|
483 | (2) |
|
16.2 Diffraction Theory of the Point Spread Function |
|
|
485 | (10) |
|
16.2.1 The Huygens--Fresnel Principle |
|
|
485 | (3) |
|
16.2.2 Diffraction Image of a Point Object by an Aberration Free Axi-Symmetric Lens System |
|
|
488 | (5) |
|
16.2.3 Physical Significance of the Omitted Phase Term |
|
|
493 | (2) |
|
16.2.4 Anamorphic Stretching of PSF in Extra-Axial Case |
|
|
495 | (1) |
|
|
495 | (6) |
|
16.3.1 Factor of Encircled Energy |
|
|
499 | (2) |
|
16.4 Resolution and Resolving Power |
|
|
501 | (15) |
|
16.4.1 Two-Point Resolution |
|
|
503 | (1) |
|
16.4.2 Rayleigh Criterion of Resolution |
|
|
503 | (2) |
|
16.4.3 Sparrow Criterion of Resolution |
|
|
505 | (2) |
|
16.4.4 Dawes Criterion of Resolution |
|
|
507 | (1) |
|
16.4.5 Resolution in the Case of Two Points of Unequal Intensity |
|
|
508 | (1) |
|
16.4.6 Resolution in the Case of Two Mutually Coherent Points |
|
|
508 | (2) |
|
16.4.7 Breaking the Diffraction Limit of Resolution |
|
|
510 | (1) |
|
16.4.7.1 Use of Phase-Shifting Mask |
|
|
510 | (2) |
|
16.4.7.2 Superresolution over a Restricted Field of View |
|
|
512 | (2) |
|
16.4.7.3 Confocal Scanning Microscopy |
|
|
514 | (1) |
|
16.4.7.4 Near Field Superresolving Aperture Scanning |
|
|
515 | (1) |
|
|
516 | (5) |
|
17 Diffraction Images by Aberrated Optical Systems |
|
|
521 | (42) |
|
17.1 Point Spread Function (PSF) for Aberrated Systems |
|
|
521 | (9) |
|
17.1.1 PSF of Airy Pupil in Different Planes of Focus |
|
|
522 | (2) |
|
17.1.2 Distribution of Intensity at the Centre of the PSF as a Function of Axial Position of the Focal Plane |
|
|
524 | (1) |
|
17.1.3 Determination of Intensity Distribution in and around Diffraction Images by Aberrated Systems |
|
|
524 | (2) |
|
|
526 | (4) |
|
17.2 Aberration Tolerances |
|
|
530 | (8) |
|
17.2.1 Rayleigh Quarter-Wavelength Rule |
|
|
531 | (1) |
|
|
532 | (1) |
|
17.2.3 Strehl Ratio in Terms of Variance of Wave Aberration |
|
|
533 | (2) |
|
17.2.3.1 Use of Local Variance of Wave Aberration |
|
|
535 | (1) |
|
17.2.3.2 Tolerance on Variance of Wave Aberration in Highly Corrected Systems |
|
|
536 | (1) |
|
17.2.3.3 Tolerance on Axial Shift of Focus in Aberration-Free Systems |
|
|
537 | (1) |
|
17.2.3.4 Tolerance on Primary Spherical Aberration |
|
|
538 | (1) |
|
17.3 Aberration Balancing |
|
|
538 | (10) |
|
17.3.1 Tolerance on Secondary Spherical Aberration with Optimum Values for Primary Spherical Aberration and Defect of Focus |
|
|
540 | (2) |
|
17.3.2 Tolerance on Primary Coma with Optimum Value for Transverse Shift of Focus |
|
|
542 | (1) |
|
17.3.3 Tolerance on Primary Astigmatism with Optimum Value for Defect of Focus |
|
|
543 | (2) |
|
17.3.4 Aberration Balancing and Tolerances on a FEE-Based Criterion |
|
|
545 | (3) |
|
17.4 Fast Evaluation of the Variance of Wave Aberration from Ray Trace Data |
|
|
548 | (2) |
|
17.5 Zernike Circle Polynomials |
|
|
550 | (6) |
|
17.6 Role of Fresnel Number in Imaging/Focusing |
|
|
556 | (1) |
|
17.7 Imaging/Focusing in Optical Systems with Large Numerical Aperture |
|
|
556 | (1) |
|
|
557 | (6) |
|
18 System Theoretic Viewpoint in Optical Image Formation |
|
|
563 | (74) |
|
18.1 Quality Assessment of Imaging of Extended Objects: A Brief Historical Background |
|
|
563 | (2) |
|
18.2 System Theoretic Concepts in Optical Image Formation |
|
|
565 | (4) |
|
18.2.1 Linearity and Principle of Superposition |
|
|
566 | (1) |
|
18.2.2 Space Invariance and Isoplanatism |
|
|
566 | (2) |
|
18.2.3 Image of an Object by a Linear Space Invariant Imaging System |
|
|
568 | (1) |
|
|
569 | (9) |
|
18.3.1 Alternative Routes to Determine Image of an Object |
|
|
570 | (1) |
|
18.3.2 Physical Interpretation of the Kernel of Fourier Transform |
|
|
570 | (2) |
|
18.3.3 Reduced Period and Reduced Spatial Frequency |
|
|
572 | (2) |
|
18.3.4 Line Spread Function |
|
|
574 | (1) |
|
18.3.5 Image of a One-Dimensional Object |
|
|
575 | (1) |
|
18.3.6 Optical Transfer Function (OTF), Modulation Transfer Function (MTF), and Phase Transfer Function (PTF) |
|
|
575 | (3) |
|
18.3.7 Effects of Coherence in Illumination on Extended Object Imagery |
|
|
578 | (1) |
|
18.4 Abbe Theory of Coherent Image Formation |
|
|
578 | (2) |
|
18.5 Transfer Function, Point Spread Function, and the Pupil Function |
|
|
580 | (24) |
|
18.5.1 Amplitude Transfer Function (ATF) in Imaging Systems Using Coherent Illumination |
|
|
581 | (2) |
|
18.5.1.1 ATF in Coherent Diffraction Limited Imaging Systems |
|
|
583 | (1) |
|
18.5.1.2 Effects of Residual Aberrations on ATF in Coherent Systems |
|
|
584 | (1) |
|
18.5.2 Optical Transfer Function (OTF) in Imaging Systems Using Incoherent Illumination |
|
|
585 | (7) |
|
18.5.2.1 OTF in Incoherent Diffraction Limited Imaging Systems |
|
|
592 | (3) |
|
18.5.2.2 Effects of Residual Aberrations on OTF in Incoherent Systems |
|
|
595 | (2) |
|
18.5.2.3 Effects of Defocusing on OTF in Diffraction Limited Systems |
|
|
597 | (2) |
|
18.5.2.4 OTF in Incoherent Imaging Systems with Residual Aberrations |
|
|
599 | (2) |
|
18.5.2.5 Effects of Nonuniform Real Amplitude in Pupil Function on OTF |
|
|
601 | (1) |
|
18.5.2.6 Apodization and Inverse Apodization |
|
|
602 | (2) |
|
18.6 Aberration Tolerances based on OTF |
|
|
604 | (4) |
|
18.6.1 The Wave Aberration Difference Function |
|
|
604 | (2) |
|
18.6.2 Aberration Tolerances based on the Variance of Wave Aberration Difference Function |
|
|
606 | (2) |
|
18.7 Fast Evaluation of Variance of the Wave Aberration Difference Function from Finite Ray Trace Data |
|
|
608 | (1) |
|
|
609 | (1) |
|
18.9 Interrelationship between PSF, LSF, ESF, BSF, and OTF |
|
|
610 | (6) |
|
18.9.1 Relation between PSF, LSF, and OTF for Circularly Symmetric Pupil Function |
|
|
611 | (1) |
|
18.9.2 Relation between ESF, LSF, and OTF |
|
|
612 | (4) |
|
|
616 | (1) |
|
18.10 Effects of Anamorphic Imagery in the Off-Axis Region on OTF Analysis |
|
|
616 | (5) |
|
18.11 Transfer Function in Cascaded Optical Systems |
|
|
621 | (1) |
|
18.12 Image Evaluation Parameters in Case of Polychromatic Illumination |
|
|
621 | (5) |
|
18.12.1 Polychromatic PSF |
|
|
622 | (1) |
|
18.12.2 Polychromatic OTF |
|
|
622 | (4) |
|
18.13 Information Theoretic Concepts in Image Evaluation |
|
|
626 | (2) |
|
|
628 | (9) |
|
|
637 | (30) |
|
19.1 Statement of the Problem of Lens Design |
|
|
637 | (1) |
|
19.2 Lens Design Methodology |
|
|
638 | (3) |
|
19.3 Different Approaches for Lens Design |
|
|
641 | (1) |
|
19.4 Tackling Aberrations in Lens Design |
|
|
642 | (3) |
|
19.4.1 Structural Symmetry of the Components on the Two Sides of the Aperture Stop |
|
|
642 | (1) |
|
19.4.2 Axial Shift of the Aperture Stop |
|
|
643 | (1) |
|
19.4.3 Controlled Vignetting |
|
|
643 | (1) |
|
19.4.4 Use of Thin Lens Approximations |
|
|
643 | (1) |
|
19.4.5 D-number and Aperture Utilization Ratio |
|
|
644 | (1) |
|
19.5 Classification of Lens Systems |
|
|
645 | (5) |
|
|
645 | (1) |
|
19.5.2 Telephoto Lenses and Wide-Angle Lenses |
|
|
645 | (1) |
|
19.5.3 Telecentric Lenses |
|
|
646 | (1) |
|
|
647 | (1) |
|
19.5.5 Lenses with Working Wavelength beyond the Visible Range |
|
|
647 | (3) |
|
19.5.6 Unconventional Lenses and Lenses using Unconventional Optical Elements |
|
|
650 | (1) |
|
19.6 A Broad Classification of Lenses based on Aperture, Field of View, Axial Location of Aperture Stop, Image Quality, and Generic Type of Lens Elements |
|
|
650 | (1) |
|
19.7 Well-Known Lens Structures in Infinity Conjugate Systems |
|
|
651 | (5) |
|
19.8 Manufacturing Tolerances |
|
|
656 | (2) |
|
|
658 | (9) |
|
20 Lens Design Optimization |
|
|
667 | (44) |
|
20.1 Optimization of Lens Design: From Dream to Reality |
|
|
667 | (5) |
|
20.2 Mathematical Preliminaries for Numerical Optimization |
|
|
672 | (12) |
|
20.2.1 Newton--Raphson Technique for Solving a Nonlinear Algebraic Equation |
|
|
672 | (1) |
|
20.2.2 Stationary Points of a Univariate Function |
|
|
673 | (1) |
|
20.2.3 Multivariate Minimization |
|
|
673 | (1) |
|
|
673 | (2) |
|
20.2.3.2 The Method of Steepest Descent |
|
|
675 | (1) |
|
|
676 | (1) |
|
20.2.4 Nonlinear Least-Squares |
|
|
677 | (3) |
|
20.2.4.1 The Gauss--Newton Method |
|
|
680 | (1) |
|
20.2.4.2 The Levenberg--Marquardt Method |
|
|
681 | (1) |
|
20.2.5 Handling of Constraints |
|
|
682 | (2) |
|
20.3 Damped Least-Squares (DLS) Method in Lens Design Optimization |
|
|
684 | (14) |
|
20.3.1 Degrees of Freedom |
|
|
684 | (1) |
|
20.3.2 Formation of the Objective Function |
|
|
685 | (2) |
|
20.3.3 Least-Squares Optimization with Total Hessian Matrix |
|
|
687 | (1) |
|
20.3.4 General Form of the Damping Factor λr |
|
|
688 | (1) |
|
20.3.5 The Scaling Damping Factor λr |
|
|
688 | (1) |
|
20.3.6 Truncated Defect Function |
|
|
689 | (2) |
|
20.3.7 Second-Derivative Damping Factor λr |
|
|
691 | (2) |
|
|
693 | (1) |
|
20.3.9 Global Damping Factor λ |
|
|
694 | (3) |
|
20.3.10 Control of Gaussian Parameters |
|
|
697 | (1) |
|
20.3.11 Control of Boundary Conditions |
|
|
697 | (1) |
|
20.3.11.1 Edge and Centre Thickness Control |
|
|
697 | (1) |
|
20.3.11.2 Control of Boundary Conditions Imposed by Available Glass Types |
|
|
698 | (1) |
|
20.4 Evaluation of Aberration Derivatives |
|
|
698 | (3) |
|
|
701 | (10) |
|
21 Towards Global Synthesis of Optical Systems |
|
|
711 | (22) |
|
21.1 Local Optimization and Global Optimization: The Curse of Dimensionality |
|
|
711 | (1) |
|
21.2 Deterministic Methods for Global/Quasi-Global Optimization |
|
|
711 | (4) |
|
21.2.1 Adaptive/Dynamic Defect Function |
|
|
712 | (1) |
|
21.2.2 Partitioning of the Design Space |
|
|
712 | (1) |
|
21.2.3 The Escape Function and the `Blow-Up/Settle-Down' Method |
|
|
713 | (1) |
|
21.2.4 Using Saddle Points of Defect Function in Design Space |
|
|
713 | (1) |
|
21.2.5 Using Parallel Plates in Starting Design |
|
|
714 | (1) |
|
21.3 Stochastic Global Optimization Methods |
|
|
715 | (4) |
|
21.3.1 Simulated Annealing |
|
|
715 | (1) |
|
21.3.2 Evolutionary Computation |
|
|
716 | (1) |
|
21.3.3 Neural Networks, Deep Learning, and Fuzzy Logic |
|
|
717 | (1) |
|
21.3.4 Particle Swarm Optimization |
|
|
718 | (1) |
|
21.4 Global Optimization by Nature-Inspired and Bio-Inspired Algorithms |
|
|
719 | (2) |
|
21.5 A Prophylactic Approach for Global Synthesis |
|
|
721 | (3) |
|
21.6 Multi-Objective Optimization and Pareto-Optimality |
|
|
724 | (1) |
|
21.7 Optical Design and Practice of Medicine |
|
|
725 | (1) |
|
|
726 | (7) |
Epilogue |
|
733 | (2) |
Index |
|
735 | |