Preface |
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xv | |
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Chapter 1 Law of Refraction: The Foundation of Geometrical Optics |
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1 | (10) |
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1 | (1) |
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1 | (2) |
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1 | (1) |
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1 | (2) |
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3 | (1) |
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1.4 Graphical Ray Tracing |
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4 | (1) |
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5 | (6) |
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1.5.1 Equations, symbols, and sign conventions |
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6 | (5) |
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Chapter 2 Best Shape for a Thin Lens |
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11 | (12) |
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11 | (1) |
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2.2 Object at Any Position |
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12 | (4) |
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2.3 Object at Infinity with Added Field of View |
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16 | (5) |
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2.3.1 Spherical aberration |
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16 | (2) |
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2.3.2 Chromatic aberration |
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18 | (1) |
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19 | (1) |
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19 | (2) |
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2.3.5 Total blur-spot size |
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21 | (1) |
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21 | (2) |
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Chapter 3 Best Shapes for Multiple Thin Lenses, Aspherizing, and the Natural Stop Position |
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23 | (10) |
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23 | (1) |
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3.2 Best Shapes for Minimum Spherical Aberration |
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23 | (3) |
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3.3 Aspherizing a Singlet to Eliminate Spherical Aberration |
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26 | (2) |
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3.4 Correcting Coma and Spherical Aberration |
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28 | (3) |
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28 | (1) |
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3.4.2 Eliminating spherical aberration |
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29 | (2) |
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3.5 Natural Stop Position |
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31 | (2) |
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Chapter 4 Transition from a Thin Lens to a Thick Lens |
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33 | (6) |
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33 | (1) |
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4.2 Adding a Thickness and Changing the Second Surface Radius |
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33 | (2) |
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4.2.1 VIS singlet with N = 1.5 |
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34 | (1) |
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4.2.2 MWIR singlet with N = 3.4 |
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35 | (1) |
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4.2.3 LWTR singlet with N = 4 |
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35 | (1) |
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4.3 Change of Spherical Aberration with Added Thickness |
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35 | (4) |
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39 | (18) |
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39 | (1) |
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5.2 Thin Achromat for the VIS Spectrum, On-Axis Performance |
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39 | (6) |
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5.2.1 Adding a field to the on-axis corrected achromat |
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43 | (2) |
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45 | (1) |
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5.3 Smith's Method of Determining the Surface Shapes |
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45 | (3) |
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5.3.1 Curvatures and inverse object distances |
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45 | (1) |
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46 | (1) |
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47 | (1) |
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5.4 Achromat for the MWTR Region |
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48 | (2) |
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5.5 Achromat for the LWIR Region |
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50 | (1) |
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5.6 Diamond-Turned Hybrid |
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50 | (7) |
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5.6.1 Hybrid for the MWIR region |
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51 | (1) |
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51 | (1) |
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52 | (1) |
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5.6.1.3 The diffractive phase profile |
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52 | (1) |
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53 | (2) |
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55 | (2) |
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Chapter 6 Systems with Two Separated Components |
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57 | (8) |
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57 | (1) |
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6.2 Dialyte---An Air-Spaced Achromat |
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57 | (5) |
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6.2.1 Example for the MWIR region |
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59 | (2) |
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6.2.1.1 Aspheric deformation coefficients of surface 3 |
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61 | (1) |
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6.2.1.2 Phase coefficients |
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61 | (1) |
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6.2.1.3 Step height at the zone transition |
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62 | (1) |
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6.3 Telephoto and Reversed Telephoto |
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62 | (3) |
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6.3.1 Examples for the MWIR and LWIR regions |
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63 | (2) |
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Chapter 7 From an Air-Spaced Doublet to a Triplet |
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65 | (4) |
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65 | (1) |
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66 | (1) |
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7.3 Example, a Conventional Triplet |
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66 | (1) |
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7.4 Hybrid Petzval Objective with a Cold Stop |
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67 | (2) |
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Chapter 8 A Hybrid for Two Wavelengths |
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69 | (4) |
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69 | (1) |
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8.2 Basic Lens Shape for the Long Wavelength |
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69 | (1) |
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8.3 Required Diffractive Profile |
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70 | (3) |
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73 | (16) |
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73 | (1) |
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9.2 Focus Shift of a Refractive Element |
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73 | (1) |
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9.3 Athermalization with a Doublet |
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74 | (1) |
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9.4 Focus Shift of a Diffractive Lens |
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74 | (4) |
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78 | (2) |
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9.5.1 Athermat with two elements in an aluminum housing |
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78 | (1) |
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9.5.2 Hybrid athermat in an aluminum housing |
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79 | (1) |
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9.6 Impact of Housing Material |
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80 | (1) |
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9.7 Athermat for the CO2 Laser Line |
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81 | (3) |
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9.8 Athermalized Achromat |
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84 | (3) |
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9.8.1 Three-element athermat in an aluminum housing |
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85 | (1) |
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9.8.2 Two-element athermat in an aluminum housing |
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86 | (1) |
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9.9 Effect of Quarter-Wave Limit without Athermalization |
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87 | (2) |
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89 | (6) |
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89 | (1) |
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10.2 Spherical Aberration |
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90 | (1) |
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91 | (1) |
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92 | (3) |
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Chapter 11 Seidel and the Pegel Diagrams |
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95 | (6) |
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95 | (1) |
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11.2 Triplet for the LWIR Region |
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95 | (3) |
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11.2.1 Surface contributions |
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96 | (1) |
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11.2.2 Pegel diagram for the triplet |
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96 | (1) |
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11.2.3 Remarks to field curvature |
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97 | (1) |
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11.3 Cassegrain Version with a Maksutov-Mangin Mirror Combination for the LWIR Region |
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98 | (3) |
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98 | (3) |
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Chapter 12 The Single-Imaging Mirror |
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101 | (12) |
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101 | (1) |
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101 | (3) |
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104 | (1) |
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104 | (3) |
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106 | (1) |
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12.4.1.1 Additional comments |
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106 | (1) |
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107 | (1) |
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107 | (2) |
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12.6 Manufacturing Remarks |
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109 | (1) |
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109 | (4) |
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Chapter 13 Eight Single Optical Elements as Imaging Objectives |
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113 | (6) |
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113 | (1) |
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113 | (1) |
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13.3 Eight Chosen Configurations |
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113 | (2) |
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13.4 Shapes of the Elements |
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115 | (1) |
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116 | (1) |
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117 | (2) |
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Chapter 14 A Progression of Performance with an Increase in Lens Complexity |
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119 | (2) |
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119 | (2) |
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Chapter 15 Two-Mirror Systems as Telescope and Microscope Objectives |
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121 | (16) |
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121 | (1) |
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15.2 Basic Cassegrain Telescope Layout |
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122 | (1) |
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123 | (1) |
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15.3 Cassegrain with Two Spherical Mirrors |
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123 | (1) |
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15.4 Classic Cassegrain System |
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124 | (1) |
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15.5 Dall-Kirkham Arrangement |
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124 | (1) |
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15.6 Ritchey-Chretien Configuration |
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125 | (1) |
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125 | (1) |
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15.8 Cassegrain with Mangin as a Secondary Reflector |
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126 | (1) |
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127 | (3) |
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15.10 Gregorian Microscope Objective |
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130 | (1) |
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15.11 Two Schwarzschild Objectives |
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131 | (5) |
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15.11.1 Prescription for the classic configuration for an object at infinity |
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133 | (1) |
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15.11.1.1 Brief historic remark about the golden ratio |
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134 | (1) |
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15.11.2 Prescription for the inverted configuration for an object at infinity |
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134 | (2) |
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15.12 Solid Microscope Objective |
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136 | (1) |
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Chapter 16 The Plane-Parallel Plate |
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137 | (10) |
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137 | (1) |
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138 | (3) |
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140 | (1) |
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141 | (2) |
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143 | (1) |
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16.4.1 Lateral displacement |
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144 | (1) |
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144 | (3) |
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Chapter 17 MTF, Limits, and Pixel Sizes |
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147 | (4) |
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147 | (1) |
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17.2 Optical Modulation Transfer Function |
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147 | (1) |
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148 | (3) |
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Chapter 18 Details of a Hybrid Lens |
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151 | (6) |
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151 | (1) |
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151 | (2) |
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18.3 Coordinates of the Combined Surface |
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153 | (4) |
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Chapter 19 From the Hoegh Meniscus to Double Anastigmats |
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157 | (12) |
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157 | (1) |
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157 | (3) |
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19.2.1 Approach and design method |
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158 | (2) |
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160 | (1) |
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19.4 Achromatic Double Lens |
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161 | (4) |
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19.4.1 Approach and design method |
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162 | (3) |
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165 | (4) |
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19.5.1 Approach and design method |
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165 | (4) |
Index |
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169 | |