The problem of chemical and biological sensing, i.e., identification of components of various media and measuring their concentrations, is of extreme importance in science, technology, medicine, environmental monitoring, etc.Principally, the problem could be solved by means of purely optical methods, particularly, tunable diode laser spectroscopy [1]. Due to the spectral resolution by an order or two of magnitude higher than Doppler width of spectral lines, it provides ideal selectivity and suitable sensitivity in gas sensing. However, such techniques require bulk, expensive laboratory equipment and qualified personnel. This results in a very high cost of analysis and makes the method unsuitable from the commercial standpoint.A known alternative approach to the problem of media analysis is sensing by microelectronic tools, mainly, through change of resistance or capacitance of semiconducting bulk or thin film samples [2J. Such sensors are rather sensitive, cheap, batch-fabricated, relatively simple in operating and, hence, are most advantageous from a practical point of view. But the problems of selectivity, stability and reproducibility of the microelectronic sensors seem to be hardly solved in the near future.In this connection, the development of new principles of sensors is an urgent need. One of the most powerful tools for both chemical and biological sensing is surface plasmon resonance (SPR) technique. Surface plasmon (SP) is a TM polarized electromagnetic wave which exists at a conductor -dielectric interface and can be optically excited in a resonant manner by means of either a prism in the total internal reflection (TIR) configuration or a grating on the conductor surface [3]. The wave decays exponentially to both sides from the interface and the conditions of SP excitation (angle of incidence of exciting radiation or its wavelength) are extremely sensitive to the properties of a medium near the interface.During the last decade, the Kretschmann technique [4] of SP excitation in the TIR arrangement has been widely used as a base of various sensors. In the work by Liedberg et. al.[5], gas sensors and biosensors based on SPR were proposed. In this method, the position of the intensity minimum of radiation reflected by a metal film covering a prism and contacting with a tested medium is measured. The capability of monitoring media changes corresponding to its refraction index shift in as small as iO was reported. In a case of a sucrose solution testing, the resolution as high as 24 -65 ppm (\n at the level of 106) was achieved [6].However, a sensor relied on the TIR technique of SPs exciting is, substantially, a purely optical one with all intrinsic drawbacks of its practical applications. In particular, one of disadvantages is the necessity of a reflecting beam registration. Such a sensor has to include either a mechanical angular scanning system with a reflected light spot displacement compensation or a photodetector matrix registering the divergent reflected beam passed through a special optics. It makes...