according to fig1 an object penetration determination device 1 includes a light bundle generation medium 2 for generation of a temporally variable reference light bundle 3 and an object light bundle 4 , a light receiver 5 , on which object and reference light bundles 3 , 4 are superimposed , a selection unit 6 for selection of individual beams to be evaluated in the light bundles 3 , 4 superimposed on the light receiver 5 , as well as an evaluation unit 7 for evaluation of object penetration . the light bundle generation medium 2 includes an optical resonator formed by means of highly reflecting mirrors 2 a 1 , 2 a 2 , in which an amplification medium 2 b and an acousto - optical modulator 2 c are arranged . the acousto - optical modulator 2 c receives high frequency energy from a frequency generator 2 d in a range between 0 . 1 mhz and 500 mhz , which results in a temporal variability of the radiated light , as is to be explained later . a beam splitter 8 is provided in the output light bundle 2 e of the light bundle generation medium 2 , which splits the output light beam 2 e into a partial bundle directed at an object 10 and a reference light bundle 3 . in the beam path of the reference light bundle 3 a back reflector is arranged at a fixed reference distance , which , by means of the beam splitter 8 , reflects back the reference light bundle 3 to the light receiver 5 , while the partial bundle directed at object 10 is reflected back by said back reflector and as object light bundle 4 the beam splitter 8 is also continuously emitted to light receiver 5 , to be precise , in such a way that object light bundle 4 and reference light bundle 3 are superimposed there . the light receiver 5 is built as a cmos - element field out of a matrix of m × n cmos elements ( i , j ), which are individually addressable by means of their indices j i , i i . from each element ( i , j ) of the cmos field of light receiver 5 a line 5 a goes to the selection unit 6 , which is designed as a multiplexer and switches signals either of only one or a small number of detection elements to a demodulation unit 7 a . the demodulation unit is designed for the purpose of analyzing the temporal variability of the output light bundle 2 e in the superimposition of reference light bundle 3 and object light bundle 4 for the individual elements caused by acousto - optical modulation by means of the acousto - optical modulator 2 c and specifying a representative size for the beat of the same . the output of the demodulation unit 7 a is fed to an input of a central data processing unit 7 b , which also has input medium 7 c and output medium 7 d , and with which in particular the frequency fa which is to be preselected at the frequency generator 2 d driving to the acousto - optical modulator 2 c can be determined as well as those matrix elements i , j of the cmos array of the light receiver 5 , whose signal is fed to the demodulation unit 7 a . in the beam path between the beam splitter 8 and the light receiver 5 a partially transparent mirror 11 is additionally provided , with which light from object 10 can be reflected onto an imaging receiver 12 developed here for example as a ccd matrix . the output signal of all elements ( i ii , j ii ) of the imaging receiver 12 is also fed to the central data processing unit . an allocation unit is provided there , which allocates those cmos elements ( i , j ) to the ccd elements that detect the same object range . for the purpose of explaining the function of the arrangement reference is first made to the fig2 a through 2 d , which illustrate the emission behavior of the light bundle generation medium as well as the signals resulting from the temporal variability of the light bundles and their superimposition and their evaluation . fig2 a shows the amplification profile of the amplification medium 2 b above first as an oscillated curve . a light amplification by light waves flowing into the amplification medium only takes place for those frequencies for which the amplification is greater than 1 , that is , between the frequencies v a and v b . with all other frequencies the light is weakened as usual . the optical resonator now has , similar to an oscillating string , preferred frequencies , so - called resonator modes . those resonator modes for which the amplification of the amplified medium is greater than 1 are preferably emitted . if the acousto - optical modulator is now excited , a grid of variably dense areas results by means of the material oscillation ; light passing through is diffracted at this grid , whereby the interaction of the light photons with the oscillation modes of the acousto - optical modulator characterizing phonons shifts the frequency of the light diffracted at the density grid by the excitation frequency of the acousto - optical modulator . this results in a slight shifting of the laser modes over time . this is only indicated for a single laser mode from the 1 st to the 2 nd image and from the 2 nd to the 3 rd image for variable times , where it is to be recognized that the frequency of a mode changes with time ; this however applies for all modes that begin oscillating in the resonator . in the process it goes without saying that , depending on how far above the amplification 1 the amplification profile runs , the intensities of the individual oscillating modes are variable and that the mode intensity changes with the frequency . fig2 b shows the trend of the variable modes of the resulting frequency comb over time . it is to be recognized that the frequencies change over time for all modes in the same manner , thus possessing the same pitch when applied to the time . the diagram of fig2 b implies that light that is emitted at different times will possess different frequencies . if light beams now arrive at an area which are irradiated at variably long optical paths , that is , were also emitted at different times from the light bundle generating medium 2 , there must be a frequency difference between the two . this frequency difference is represented in fig2 c for differing runtime differences and different modes in the resonator . it can be detected as a beat frequency on a cmos element . the frequency shift between object light beam and reference light bundle is first dependent only on the runtime difference , provided a corresponding linearity of the acousto - optical modulator is assumed and the acousto - optical modulation frequency is fixed . the same dependency results for all modes . ( the beat parts originating from the individual modes add up accordingly .) the frequency shift is further dependent on which frequency the acousto - optical modulator is excited . if the excitation frequency of the acousto - optical modulator is changed , the pitch of the curve changes and the distance of the individual “ teeth ”, that is of those levels for which a given optical path length difference results in a null frequency shift again . against this background the arrangement of fig1 is used in the following way : first an object 10 is arranged in the field of vision of the split part of the output light bundle 2 a in such a way that it is illuminated . then an optical projected image of the object is taken with the image receiver 12 and specific places whose penetrations are to be specified are selected , for example places a and b . the selection of these places can occur under consideration of the optical projected image using the input medium 7 c . the elements ( i i , j i ) allocated to places a and b on the light receiver 5 are selected at the selection unit 6 for signal evaluation . this results in a signal being given to the demodulation unit 7 a by the selected cmos elements ( i i , j i ). in the case of element i i , j i , a single beam of the object light bundle 4 is superimposed with a single beam of the reference light bundle 3 ; in this connection beam means “ a small area of an expanded bundle ”. in the demodulation unit 7 a the beat frequency δv is determined for the array element i i , j i and a corresponding signal is fed to the central data processing unit . the central data processing unit 7 b now changes the excitation frequency f a of the acousto - optical modulator successively step by step in prime steps and determines the resulting beat frequencies on array element i , j . from the total signals gained thereby it is then determined which multiple of a frequency shift is actually present and the corresponding path length difference of the reference and object light beams is determined for this array element i i , j i . then the actual coordinates ( x , y , z ) of object 10 can be inferred using the geometric method from the path length difference and the position . by selecting suitable points a , b , etc ., the object can be measured at characteristically important places . the measuring can take place very rapidly , so that more than 30 , for example currently up to about 2 , 000 points can easily be created in real time without greater switching expenditure . with a correspondingly high modulation frequency precisions in the acousto - optical modulator in the micrometer range or submicrometer range can easily be achieved , which with the high time resolutions makes measurements possible on rapidly moved shafts , tool parts , loudspeaker diaphragms etc . in the process the simultaneous recording of an optical image gives information for a user that is particularly easy to evaluate . it is to be pointed out that both ring resonators and also linear resonators can be used as resonators for the fsf laser . it is further to be pointed out that in place of cmos element fields for the detection or the transfer of selected beams of different , sufficiently fast light receivers and / or detector fields can also be used as available in the state of the art .