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Titlebook: Geometric Optics; Theory and Design of Antonio Romano Book 20101st edition Birkhäuser Boston 2010 Hamiltonian formulation of the optical sy

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https://doi.org/10.1007/978-3-322-87277-7In Chapter 9, we formulated the fundamental laws of geometrical optics using the Lagrangian formalism. It is well known that any theory expressed in Lagrangian terms can also be (equivalently) formulated via the Hamiltonian formalism, with significant advantages. This chapter describes this new formalism together with its consequences.
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Albert Ploeger,Robert van KralingenIn Chapter 2 we presented the paraxial or Gaussian theory, which describes the propagation of light across an optical system ., but only for rays that are close to the optical axis a and that subtend small angles with it. We showed that, under these conditions, the correspondence between an . and .′ is given by the linear relations
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Gaussian Optics,In this chapter we present the Gaussian analysis of an optical system .. In particular, we introduce all of the optical characteristics of . (pupils, focal points, nodal points, principal planes, etc.). All these data can be obtained using the notebook ..
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Cameras for Astronomy,This chapter describes the cameras most commonly used for astronomical photography. The main component in these cameras is a concave mirror . that forms the image of an object at infinity on its focal plane. The image formed by such a system usually exhibits aberrations that are too large to be acceptable.
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Compound Cassegrain Telescopes,Very efficient optical configurations can be obtained for astronomical telescopes by combining one of the correctors described in the previous chapter with the Cassegrain scheme. Depending on the corrector chosen, a Schimdt–Cassegrain, Houghton–Cassegrain or Maksutov–Cassegrain telescope is obtained (see Figure 6.1).
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Hamiltonian Optics,In Chapter 9, we formulated the fundamental laws of geometrical optics using the Lagrangian formalism. It is well known that any theory expressed in Lagrangian terms can also be (equivalently) formulated via the Hamiltonian formalism, with significant advantages. This chapter describes this new formalism together with its consequences.
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