the schematic of the process for obtaining nanoparticles by laser dispersion ( fig1 ), used in practicing the claimed method , includes a target 1 , whose molten surface layer 2 is dispersed under the action of a pulsed - periodic laser 3 to give liquid drops 4 , which , when passing the plasma zone 5 , undergo division to nanoparticles 6 . the resulting nanoparticles 6 are deposited onto a substrate 7 . the process is performed in an atmosphere of argon at a pressure of 10 − 4 - 10 − 2 pa . the installation for plasma - assisted electrodispersion , in which a stationary plasma is formed , includes ( see fig4 ) a vacuum chamber 8 in which a pointed cathode 9 , an anode with an aperture 11 , a cathode 12 with an opening 13 , and an annular anode 14 on which substrates 7 are mounted . the chamber is filled with an inert gas at a pressure of 10 − 3 - 10 − 1 pa . when an appropriate potential difference is created between the pointed cathode 9 and anode 10 , molten drops 4 emerge from the surface of the cathode 9 . when these drops pass the plasma zone 5 , they are divided to form nanoparticles 6 and coarser ( than the nanoparticles ) drops 15 . the claimed method for obtaining nanoparticles is practiced as follows . a molten material , from which nanoparticles are to be produced , is dispersed by any known method ( e . g ., by atomization with a nozzle ). the resulting liquid drops are fed into a plasma formed in an inert gas at a pressure of 10 − 4 - 10 − 1 pa . as inert gas can serve any known inert gas . the liquid nanoparticles formed in the plasma zone are cooled in the inert gas to hardening and then the resulting solid nanoparticles are deposited onto a support made of any solid material . as established by the authors , the plasma parameters should satisfy the relations : t e & gt ; 1 . 4 · 10 5 ⁢ r d ⁢ r ⁡ ( r d + r ) r d + 2 ⁢ r ( 1 ) n e 1 / 2 & gt ; 9 ⁢ τ d - 1 ⁡ ( 1 + r d r ) ( 2 ) 1 τ p + 10 3 l & gt ; 10 - 5 ⁢ t m 3 ( 3 ) where r and r are , respectively , the maximum and minimum radii of liquid drops fed into the plasma , m ; r d = 7 . 5 · 10 3 ⁢ t e n e n e is the density of the plasma , m − 3 ; τ d is the time of transit of liquid drops across the plasma zone , s ; t m is the melting point of the conducting material , k ; l is the characteristic distance along which the plasma pressure decreases by a factor of e , m . as a material that can be used to obtain nanoparticles can serve both a metal and a semiconductor or a metal oxide . it is advisable to deposit the nanoparticles obtained onto a support in an electric field whose strength vector makes a certain angle with the direction of nanoparticle motion , e . g ., in a nonuniform electric field . the claimed method for obtaining nanoparticles was practiced on the basis of laser dispersion of such metals as copper and nickel ( see fig1 ). in this case , irradiation of the surface of the metallic target 1 with a pulsed - periodic laser 3 leads to melting of the surface layer 2 of the target 1 and the material of the target 1 evaporates . as a result of an optical breakdown of the vapor formed , a plasma zone 5 with a thickness l ≧ 100 μm is formed near the surface of the molten layer 2 of the target 1 . under the action of plasma 5 , the molten surface layer 2 becomes unstable , which leads to dispersion of the metal to give liquid particles 4 from the metal of the target 1 , with the maximum and minimum radii of these particles being r = 1 μm and r = 100 nm , respectively . liquid drops 4 formed as a result of dispersion are fed into the plasma zone 5 , which is heated by absorbed laser light . in the plasma zone 5 , drops 4 are charged to the floating potential , so that their charge is mainly determined by the temperature of electrons in plasma 5 . if the amount of charge is such that coulomb repulsion forces exceed the surface tension force , then the drop 4 becomes unstable ( capillary instability ) and starts to break down into smaller drops 6 . the capillary instability develops if condition ( 1 ) is satisfied . this condition elates the electron temperature ( t e ), the density of electrons in the plasma ( n e ), and the maximum radius of particles 4 fed into the plasma zone 5 ( r ). in order for dispersed particles 4 to have enough time to obtain a charge sufficient for their transition to an unstable state , condition ( 2 ) should be satisfied . these conditions impose restrictions on the minimum electron temperature and density of plasma 5 . for particles 4 with sizes r = 1 μm and r = 100 nm , the required temperature of electrons is ˜ 30 ev , and the density of plasma 5 , n e = 10 18 cm − 3 . the necessary parameters can be obtained if the power density of laser light incident on the target exceeds 10 9 w / cm 2 and the laser pulse has such a shape that the pulse - rise time is less than 5 ns and the full pulse width exceeds 20 ns . if conditions ( 1 ) and ( 2 ) are satisfied , this ensures that all liquid drops 4 fed into the plasma zone 5 undergo division : the process occurs in the form of a cascade with successive formation of increasingly fine drops and culminates in the formation of a great number of nanosize liquid drops 6 . depending on the ratio between the plasma expantion velocity of 6 and the motion velocity of nanoparticles 6 , liquid nanoparticles 6 can either leave the region of hot plasma 5 and eventually undergo cooling and hardening , or cool down and harden because of the expansion of the plasma cloud . for nanoparticles to have an amorphous structure in the solid state , it is necessary to ensure a sufficiently high (˜ 10 7 k / s ) rate of their cooling in hardening . such a cooling rate is ensured by radiation loss if nanoparticles 6 are outside the plasma zone 5 at the instant of hardening , i . e ., if inequality ( 3 ) is satisfied . under the conditions of the experiment described , the plasma lifetime τ p = 1 μs , l ≧ 100 μm . if copper or nickel is chosen as the material of the target 1 , the motion velocity of nanoparticles 6 , v n = 3 10 4 cm / s , and the melting point falls within the range t m = 1350 - 1730 k . in this case , condition ( 3 ) is satisfied . with the above - described parameters of the process , copper and nickel nanoparticles 6 were obtained ( fig2 and 3 ). both copper and nickel nanoparticles 6 were in the amorphous state . particles 6 were deposited onto oxidized silicon substrates 7 . the size of the particles 6 was 5 nm for copper and 2 . 5 nm for nickel . the relative variance of the sizes of nanoparticles 6 , evaluated using tem images , did not exceed 20 %. in contrast to nanoparticles obtained using the prototype method , in which nanoparticles are crystalline and coagulate when coming in contact with one another , the size of the nanoparticles 6 produced by the claimed method was found to be twice smaller . this is due to the choice of the rise time of the laser light pulse , which ensures that condition ( 2 ) is satisfied . the claimed method was practiced on the basis of an installation for plasma - assisted electrodispersion , which is shown schematically in fig4 . molten metal was dispersed by applying to a metallic pointed cathode 9 with a radius of tip curvature not exceeding 10 μm an electric field with a strength at the tip apex of no less than 10 7 v / s . molten drops 4 obtained at the tip 8 are delivered to the plasma zone 5 created by a stationary or quasi - stationary discharge in an inert gas at a pressure of 10 − 3 - 10 − 1 pa , to be charged there . the electron density in stationary discharges at these pressures is on the order of n e = 10 10 - 10 11 cm − 3 , and , in accordance with condition ( 1 ), the required temperature of electrons should exceed 500 ev . to create such a temperature , the potential difference between anode 9 and cathode 10 was set to be no less than 2 kv . for drops 4 not to have enough time to be charged to the floating potential , i . e ., for condition ( 2 ) to be satisfied at a given electron density , the anode 9 and the cathode 10 are to be mounted at a certain distance from each other , in accordance with the chosen inert gas pressure ( about 5 cm ). if the above conditions are satisfied , drops 4 flying into the plasma zone 5 become unstable , which leads to the onset of their cascade fission . the lifetime of stationary or quasi - stationary plasma 5 is long , and , in contrast to the case of laser dispersion , whether or not the inequality that describes condition ( 3 ) is satisfied is determined by the choice of parameter l . in the given case , the value of this parameter is close to the size of the opening in the cathode 10 and , in view of the requirements imposed by condition ( 3 ), it should not exceed 1 cm . further , the forming nanosize drops 6 were separated from coarser drops 11 by choosing the dimensions of the annular anode 12 , on which substrates 1 are mounted . the potential difference between the anode 12 and the cathode 10 was chosen in such a way that nanosize particles 6 were directed by the electric field to the substrate 1 , and the trajectories of coarse particles 11 were not distorted . the resulting nanoparticles 6 were also in the amorphous state . thus , the claimed method yields nanosize spherical amorphous particles with a narrow size dispersion . while this invention has been particularly shown and described with references to preferred embodiments thereof , it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the scope of the invention encompassed by the appended claims .