In modern nanoelectronics, the density of transis tors arranged on a chip has reached a high level such that a key problem of further development of integra tion is related not as much to the transistor physics as to the conditions of signal transfer in the scheme, since the spacing of conductors is small so that the unavoid able parasitic capacitance between them significantly retards the signal propagation [1]. In addition, the level of power dissipation due to leakage currents and dynamic scattering (proportional to the parasitic capacitance) has also increased. In order to solve this problem, it is necessary to possible reduce the parasitic capacitance, which can be achieved by radically decreasing the dielectric permittivity of an insulator on which the electric connections are supported.An optimum solution of this task would be the introduction of pores into the insulator-in particu lar, into a silica substrate [2]. Since porous silica (por SiO 2 ) is a new material, it is necessary to develop a cor responding special technology of growing thin films on these substrates. As is known [3,4], the properties of thin films strongly depend on both the material and surface state of a substrate. In this context, the present investigation was aimed at studying the influence of porosity on the structure of thin films synthesized on por SiO 2 substrates using the example of thin alumina (Al 2 O 3 ) films of various thicknesses grown by atomic layer deposition (ALD). Alumina was selected to be the film material because (i) this compound remains chemically stable during deposition onto various sub strates and (ii) the technology of Al 2 O 3 synthesis on traditional substrates is well developed and gives repro ducible results. For comparison, we have also studied alumina films grown on crystalline silicon (c Si) and those covered by a thermal SiO 2 layer.The porous silica substrates were prepared from a liquid phase using the spin coating technique followed by drying in an infrared furnace. The average pore size in as prepared samples was about 2 nm. Alumina films were synthesized by ALD on these por SiO 2 substrates at a temperature of 280°C. The ALD cycle consisted of two steps, in which the precursors were trimetylalumi num Al(CH 3 ) 3 and water vapor at a reactant tempera ture of 22°C.The samples were studied by X ray reflection spec troscopy using s polarized synchrotron radiation. The measurements were performed on a Reflectometer setup of D 08 1B2 Optics Beamline at BESSY II [5, 6]. The energy resolution at 85 eV (near the AlL 2,3 absorption edge) was better than 20 meV, and the accuracy of photon energy determination was about 10 meV. The reflected signal was detected by a GaAsP Schottky diode and a Keithley 617 electrometer. A total working diode area of 4 × 4 mm 2 allowed the entire reflected beam to be detected. The measured reflection spectra were used to calculate the spectra of absorption based on the Kramers-Kronig relation and a method that has been described in detail elsewhere [7]. Figure 1a shows the ...