Generator of a harmonic of laser light
FIELD OF THE INVENTION 
     The invention relates to a generator of the harmonic of laser light and is destined for application particularly in the equipment for spectrometric measurements carried out with the laser technique, but also can be effectively used in all cases in which the laser technique may be applied. 
     TECHNICAL BACKGROUND 
     The known generators of the harmonic of the laser light are built at least of two dispersive elements, in particular of glass prisms with resulting zero dispersion, focusing lenses, a non-linear crystal and an outlet lens. The necessary condition for the installation of systems generating the harmonic of laser light is the identity of the light dispersion of the assembled dispersive elements, in particular glass prisms. These known systems are characterized by a long optic route of laser light, in particular between dispersive elements. In order to reduce the size of the generator, in some solutions the optic route is twice or even several times refracted through an adequate arrangement of mirrors. 
     The inconvenience of the application of other known solutions results from the fact that the manipulation with each of the elements of such a set requires special precision. This induced constructors to apply in some known generators complicated electro-mechanical systems for the control of these manipulations. 
     However, independently of the complicated service which results from long optic routes, the known generators are characterized by an unadequate light polarization and by a low capacity. 
     SUMMARY OF THE INVENTION 
     The substance of the invention is the fact that the optic route in the generator of the harmonic of the laser light may be many times shortened owing to an replacement of the system of dispersive elements, in particular of glass prisms with a resulting zero dispersion, by at least one dispersive element of great dispersion, in particular by a rutile prism. 
     As it unexpectedly resulted from investigations and experiments, the application of at least one dispersive element of a great dispersion in combination with a system reversing the polarization surface by 90°, in particular with a 90° polarization rotator of a half-wave plate, permits to shorten, even twenty times, the optic route of light in the system of the generator of harmonic. Consequently, it permits to reduce drastically the size of the equipment without a necessity of using mirrors. 
     According to the invention, the generator of the harmonic of laser light consists of a lens adapting the laser light to the system, further of at least one dispersive element of a great dispersion, in particular a rutile prism, a system reversing polarization surface by 90°, a focusing lens or lenses, a non-linear crystal and an outlet lens. 
    
    
     EXPLANATION OF THE DRAWING 
     A practical example of the generator according to the invention is shown on the drawing which represents the scheme of the optical system of the generator. 
    
    
     EXAMPLE 
     The generator of the harmonic of laser light contains a chassis--not shown on the drawing--in which along the optic route of light the following elements are successively mounted: a lens 1 adapting the laser light to the system, a rutile prism 2 as dispersive element, 90° polarization rotator 3 as a system reversing the polarization surface by 90°, a focusing lens 4, a non-linear crystal 5 and an outlet lens 6. The relative position of the particular elements of the generator system corresponds to the following interrelations: the sum of the reciprocal value of the distance between the dispersive element 2 and the focusing lens 4 and of the reciprocal value of the distance between the focusing lens 4 and the non-linear crystal 5 is equal to the reciprocal value of the focus of focusing lens 4, and, moreover, the ratio of the derivative with respect to wave length of the deviation angle of light beam, produced by the dispersive element 2, to the derivative with respect to wave length of the phase matching angle of the non-linear crystal 5 is equal to the product of the refraction coefficient of the non-linear crystal 5 and the ratio of the distance between the dispersive element 2 and the focusing lens 4 to the distance between the focusing lens 4 and the non-linear crystal 5.