Book contents
- Frontmatter
- Contents
- Preface
- Part one Preview
- Part two Geometrical optics
- Part three Paraxial optics
- Part four Waves in homogeneous media
- Part five Wave propagation through lenses
- Part six Aberrations
- Part seven Applications
- 28 Gaussian beams
- 29 Concentric systems
- 30 Thin lenses
- 31 Mock ray tracing
- 32 Diffractive optical elements
- Appendix 1 Fourier transforms
- Appendix 2 Third order calculations
- Appendix 3 Ray tracing
- Appendix 4 Eikonals and the propagation kernels
- Appendix 5 Paraxial eikonals
- Appendix 6 Hints and problem solutions
- Bibliography
- Index
29 - Concentric systems
Published online by Cambridge University Press: 22 September 2009
- Frontmatter
- Contents
- Preface
- Part one Preview
- Part two Geometrical optics
- Part three Paraxial optics
- Part four Waves in homogeneous media
- Part five Wave propagation through lenses
- Part six Aberrations
- Part seven Applications
- 28 Gaussian beams
- 29 Concentric systems
- 30 Thin lenses
- 31 Mock ray tracing
- 32 Diffractive optical elements
- Appendix 1 Fourier transforms
- Appendix 2 Third order calculations
- Appendix 3 Ray tracing
- Appendix 4 Eikonals and the propagation kernels
- Appendix 5 Paraxial eikonals
- Appendix 6 Hints and problem solutions
- Bibliography
- Index
Summary
Basic properties
A concentric system is constructed of spherical surfaces, refracting or reflecting, that all have a common center. A solid sphere is a simple example; two other examples are shown in fig. 29.1. A concentric lens is insensitive to rotations around its center; this high degree of symmetry determines the special properties of concentric systems.
For any incident ray the plane containing the ray and the center of the system divides the lens into two symmetric halves. There is no reason for the ray to prefer one of these halves over the other; so the ray will remain in the symmetry plane as it traverses the lens. It follows that every ray travels in a plane containing the center.
As long as the lens is not afocal the angle eikonal W(L, M, L′, M′) can be used. We choose any straight line through the center as the axis, and locate both the (x, y) reference plane in the object space and the (x′, y′) reference plane in the image space right in the center of the system. Then the angle eikonal is the optical distance from the projection P of the center onto the ray in the object space to the projection P′ of the center onto the ray in the image space. On account of the spherical symmetry of the lens a rotation of the entire ray around the center has no effect on the value of the eikonal function.
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- The Ray and Wave Theory of Lenses , pp. 320 - 333Publisher: Cambridge University PressPrint publication year: 1995