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228    J. Gaspar et al.
                           mirror profiles, yield simple projection models. In general, to obtain such a
                           system it is necessary to place the mirror at a precise location relative to
                           the camera. In 1997, Nayar and Baker [64] patented a system combining a
                           parabolic mirror and a telecentric lens, which is well described by a simple
                           model and simultaneously overcomes the requirement of precise assembly.
                           Furthermore, their system is superior in the acquisition of non-blurred images.
                              The second design involves specifying a specialised mirror profile in
                           order to obtain a particular, possibly task-specific, view of the environment.
                           In both cases, to image the greatest field-of-view the camera’s optical axis is
                           aligned with that of the mirrors’. A detailed analysis of both the standard
                           and specialised mirror designs are given in the following Sections.


                           2.1 A Unifying Theory for Single Centre of Projection Systems
                           Recently, Geyer and Daniilidis [37, 38] presented a unified projection model
                           for all omnidirectional cameras with a single centre of projection. They showed
                                                                                      3
                           that these systems (parabolic, hyperbolic, elliptical and perspective )canbe
                           modelled by a two-step mapping via the sphere. This mapping of a point in
                           space to the image plane is graphically illustrated in Fig. 1 (left). The two
                           steps of the mapping are as follows:
                            1. Project a 3D world point, P =(x, y, z)toapoint P s on the sphere surface,
                               such that the projection is normal to the sphere surface.
                            2. Subsequently, project to a point on the image plane, P i =(u, v)froma
                               point, O on the vertical axis of the sphere, through the point P s .



















                           Fig. 1. A Unifying Theory for all catadioptric sensors with asinglecentreofpro-
                           jection (left). Main variables defining the projection model of non-single projection
                           centre systems based on arbitrary mirror profiles, F(t)(right)



                            3
                             A parabolic mirror with an orthographic lens and all of the others with a standard
                             lens. In the case of a perspective camera, the mirror is virtual and planar.
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