Abstract:
A device for measuring thin films and bulks is disclosed using slow-wave structures in electrodynamic elements to allow a decrease in frequency, an increase in sensitivity to electromagnetic parameters and accuracy of their monitoring. A method is also disclosed for monitoring of materials which includes placing an electrodynamic element near a monitored material and exciting an alternating electromagnetic field at an appropriate frequency to penetrate the monitored material concentrating in a small volume. Electromagnetic field parameters are then measured which are caused by the material parameters variation and said variations are converted to electromagnetic field parameters, the element being excited by an electromagnetic field in the form of at least one slowed electromagnetic wave.

Description:
CROSS-REFERENCE TO RELATED APPLICATION 
     This is a continuation-in-part of U.S. patent application Ser. No. 09/134,056 filed Aug. 14, 1998, by Pchehnikov et al., for Electromagnetic Method of Liquid Level Monitoring. 
    
    
     FIELD OF THE INVENTION 
     The present invention relates to the non-contact monitoring of electromagnetic parameters of thin films and bulks (conducting and non-conducting materials). More specifically, the present invention relates to an electromagnetic method and apparatus for measuring resistivity, permeability and permittivity, including artificial dielectric permittivity. The monitoring of these parameters permits the measurement of thickness of semiconductor and dielectric films and substrates, by determining the distance to a buried layer or its conductivity. This provides the possibility of non-destructive monitoring of quality in the process. 
     BACKGROUND OF THE INVENTION 
     The usefulness of application of RF or microwave field for monitoring electric parameters of different materials is recognized by the prior art. Such devices can operate with microwave excitation. When a monitored material is placed in a microwave electromagnetic field, for example inside a circular cavity resonator, the resonance frequency and Q-factor are dependent on the material permittivity and resistivity, see U.S. Pat. No. 3,458,808 Apparatus for Measuring the Properties of a Material by Resonance Techniques/N. B. Agdur, 1969. 
     Permittivity of a dielectric material can be monitored when the material is placed in the transmission line, for example a waveguide. The phase delay of a microwave signal is used for permittivity measurement, see Adrian D. Green and Wayne S. Holmes, “Dielectric Properties of Fresh Peas at Frequencies from 130 MHz to 4 GHz.”  Proceedings  31  Microwave Power Symposium,  1996, Boston, Mass., pp. 1-4. 
     The electromagnetic method of measuring resistivity in semiconductor substrates is also known. Directed by a tapered parallel plate antenna, the microwave radiation reflects from the semiconductor wafer, the reflection factor correlating with a wafer&#39;s resistivity, see S. Bothra and J. M. Borrego “Spatially Resolved Resistivity Measurements in Semiconductor Wafers Using Microwave Techniques”  Proceedings of  20 th    European Conference Vol.  1, 1990, pp. 990-994. 
     In particular, the state of the art is shown in Yu. N. Pchelnikov publications, disclosing a slow-wave structure application for permittivity measurement, see Yu. N. Pchelnikov “Possibility of Using a Cylindrical Helix To Monitor the Continuity of Media”,  Measurement Techniques, Vol.  38, # 10, 1995, pp. 1182-1184 and in the review on slow-wave structure-based sensors, see Yu. N. Pchel&#39;nikov et al “Primary Measuring Transducers Based on Retardation Systems”,  Measuring Techniques, Vol.  37, # 5, 1994, pp. 506-510. These publications show that the change in the monitored parameters in the measuring volume leads to a change in signal phase delay in the slow-wave structure. A change in a delay alteration can be converted into a change in an oscillator&#39;s frequency. 
     Slowed electromagnetic waves and slow-wave structures are also well known in the field of microwave engineering, See Dean A. Watkins “Topics in Electromagnetic Theory”, New York, John Wiley &amp; Sons, Inc., p. 1, These waves are electromagnetic waves propagating in one direction with a phase velocity ν p  that is smaller than the light velocity c in a vacuum. The relation c/ν p  is named slowing or deceleration and is designated as n. In the most practically interesting cases, slowed electromagnetic waves are formed in slow-wave structures by coiling one or two conductors (for example, into a helix, as it is shown in FIG. 1 (Prior Art), where the other conductor is a cylinder), which increases the path length traveled by the wave, or by successively connecting resonant elements or cells, energy exchange between which delays the phase of the wave, or by using an electrodynamically dense medium (usually a dielectric), or a combination of these methods. Additional deceleration was also obtained due to positive electric and magnetic coupling in coupled slow-wave structures. See V. V. Annenkov, Yu. N. Pchelnikov “Sensitive Elements Based on Slow-Wave Structures”  Measurement Techniques, Vol.  38, # 12, 1995, pp. 1369-1375. 
     Slow-wave structure-based sensitive elements are known in the art, see Yu. N. Pchelnikov, I. A. Uvarov and S. I. Ryabtsev “Instrument for Detecting Bubbles in a Flowing Liquid”,  Measurement Techniques, Vol.  22, # 5, 1979, pp. 559-560. Slowing of the electromagnetic wave leads to a reduction in the resonant dimensions of the sensitive elements, and this enables one, by using the advantages of electrodynamic sues to operate at relatively low frequencies, which are more convenient for generation and are more convenient for primary conversion of the information signal, but sufficiently high to provide high accuracy and high speed of response. The low electromagnetic losses at relatively low frequencies (a few to tens of megahertz) also help to increase the accuracy and sensativity of the measurements. The slowing of the electromagnetic wave leads also to energy concentration in the transverse and longitudinal directions which results in an increase in sensitivity, proportional to the slowing down factor n. See V. V. Annenkov, Yu. N. Pchelnikov “Sensitive Elements Based on Slow-Wave Structures”  Measurement Techniques, Vol.  38, # 12, 1995, pp. 1369-1375. 
     Most slow-wave structures were made as two-conductor periodic transmission lines (see Dean A. Watkins “Topics in Electromagnetic Theory”, John Willy &amp; Sons, Inc. Publishers). A version is possible when a slow-wave structure contains three or more different conductors. In all cases the slowed wave is excited in the electrodynamic element between different combinations of the two conductors. The coiled conductors increasing the wave path are named “impedance conductors”, and conductors with simple configuration such as rods, tapes, etc., stretched along the wave propagation direction are named “screen conductors”, see V. V. Annenkov, Yu. N. Pchelnikov “Sensitive Elements Based on Slow-Wave Structures”  Measurement Techniques, Vol.  38, # 12, 1995, pp. 1369-1375. 
     Both the prior art and the present invention measure one or more parameters of an electromagnetic field. Some of the prior methods and present invention use an electrodynamic element which is made as a section of an electromagnetic transmission line. The electrodynamic element is connected to an external RF or microwave signal generator which is used to excite an electromagnetic field. The change in, for example, resistivity, causes a shift in the characteristics of the electromagnetic field in the electrodynamic element. The shift in characteristics correlates to a change, for example, in the electromagnetic parameters of a monitored material. However, the prior art employs antennas, cavity resonators, wave-guides and two-conductor transmission lines. 
     Devices used in the prior art exhibit several problems overcome by the present invention. The previous design employs antennas, cavity resonators, wave-guides and two-conductor transmission lines. The monitoring by reflection and penetration factors measurement of the prior art requires very frequency, lying in particular, in a millimeter or an optical range, wherein measurements are possible only when optically transparent materials are involved. The electric parameters monitored by an electrodynamic element made as a section of a wave-guide in the prior art can not be made at relatively low frequency at which electromagnetic losses are small and the cost is also low. The previous methods that were based on wave-guide application are expensive, inconvenient and are not sufficiently accurate. The first is due to complexity of the microwave measuring circuits, the second is due to restricted volume inside the wave-guide; the third is due to radiation and electromagnetic losses in conductors, and due to cavity resonators&#39; frequency dependence upon the environment temperature. 
     Thus, there is a need in the art for an electromagnetic method and apparatus for monitoring thin film and bulks electric parameters that is more convenient, has better sensitivity, better resolution, greater diversity and lower cost. 
     SUMMARY OF THE INVENTION 
     The present invention employs slow-wave structures in electrodynamic elements, which allows a decrease in frequency, an increase in sensitivity to electromagnetic parameters of materials for thin films and bulks and accuracy of their monitoring. The use of these structures is followed by the cost and dimensions of transducers decreasing, the range of measured parameters increasing, and the making of the measurements more convenient to obtain. 
     The frequency decreasing is achieved due to slowing. The sensitivity increasing is achieved due to electromagnetic energy concentration near the electrodynamic element surface and due to splitting electric and magnetic fields in the monitored volume. The additional increase of sensitivity is achieved due to application of the “butterfly” design of an electrodynamic element. The measured parameters range is widened due to the wide frequency band of slow-wave structures. The application convenience is due to possibility of placing of the electrodynamic element outside the monitored material. The slow-wave structure-based electrodynamic elements are designed, as a rule, on a dielectric base, stable to temperature alteration, and its resonant frequency dependence on temperature is very small, contrary to, for example, cavity resonators. 
     The present invention teaches an electromagnetic method of measuring electric parameters of thin films and bulks, both thickness and distance, that require high resolution wherein an excited electromagnetic wave with a preset distribution of the electric and magnetic components of the electromagnetic field makes it possible to increase the sensitivity and accuracy of measurement, using relatively low frequencies. The method is implemented in an apparatus, for example, for measuring resistivity, wherein the structural form of the electrodynamic element, used as the sensing element, allows increased sensitivity and accuracy. In this invention an electrodynamic element is made as at least one section of a slow-wave structure. 
     It is known, that dielectric or conducting materials, placed in the electromagnetic field, alters its parameters, for example, its velocity, that leads to the phase delay or resonant frequency alteration. The degree of such alteration and, therefore, sensitivity S is proportional to the relation of the volume V of a material to the monitored volume V 0 , for example, a volume of a resonator, and depends on the electric and magnetic field distribution in the monitored volume 
     
       
           S ˜( V/V   0 ) F (∈, μ, σ) f,   
       
     
     where ∈ and μ are relative permittivity and permeability, σ is conductivity of a material, F(∈, μ, σ) is some function, depending on the material position in the monitored volume V 0 , and f is frequency. See V. A. Viktorov, B. V. Lunkin and A. S. Sovlukov, “Radio-Wave measurements”  Moscow: Energoatomizdatat,  1989, p. 27. If, for example, dielectric material is monitored, for the present invention, it should be placed in the electric field and its effect will be proportional to the electric field energy in the material. Since the resonant volume V 0  is smaller when the first resonant frequency f 1  is higher, the sensitivity S rises with frequency increasing. Slowing of electromagnetic wave n times leads to an n-times decrease of the resonant volume V 0  that is accomplished by the sensitivity n-times increasing 
     
       
           S ˜( V/V   0 ) nF (∈, μ, σ) f   1 . 
       
     
     The sensitivity increasing permits lower frequency and works with smaller losses, which, for example, in conductors are proportional to the square root of frequency. See: E. C. Young “The Penguin Dictionary of Electronics”, second edition, Penguin Books, p. 530. The decrease in electromagnetic losses leads to resolution increase. 
     The definition “thin film” means that film thickness is at least three times smaller than the depth of an electromagnetic field penetration into the film&#39;s material. It means that the electromagnetic field intensity does not change through the film&#39;s thickness by more than 30% of its value at the film&#39;s surface. In this case the film can be replaced by one or more surface electromagnetic parameters. If film is made from conducting material, it can be replaced by an infinitely thin film with an equivalent surface resistivity ρ □ ; if the film is made from a dielectric material, it can be replaced by an infinitely thin film with an equivalent surface permittivity ∈ □ . The magnetic film can be replaced by an infinitely thin film with an equivalent permeability μ □ see Yu. N. Pchelnikov “On the Application of Surface Permeability to the Analysis of Electrodynamic Systems”// Journal of Communications Technology and Electronics, Vol.  41, # 4, 1996, pp. 299-301. 
     The definition “bulk” means a three dimensional piece or volume of material. In some cases, when the bulk thickness exceeds the depth of the slowed field penetration in the material, the bulk can be replaced by an infinitely thin film with an equivalent surface permittivity, surface permeability or surface resistivity. 
     Thus, the slow-wave structures application makes it possible to measure thin films and bulks electromagnetic parameters (permittivity, permeability, and resistivity) with large sensitivity and higher accuracy than previous methods. 
    
    
     DESCRIPTIONS OF THE DRAWINGS 
     For further understanding of the nature and objects of the present invention, reference should be had to the following drawings in which like parts are given like reference numerals and wherein: 
     FIG. 1 illustrates a slow-wave structure of the prior art, wherein one conductor is coiled into a helix and the other conductor is a cylinder; 
     FIG. 2 illustrates an electrodynamic element of the preferred embodiments of the present invention juxtaposed with the film to be measured; 
     FIG. 3 illustrates an electrodynamic element of the preferred embodiment of the present invention mounted on the dielectric substrate adjacent the thin film; 
     FIG. 4 illustrates a measuring circuit of the preferred embodiment of the present invention; 
     FIG. 5 illustrates a second preferred embodiment of the present invention showing the measuring circuit; 
     FIG. 6 is an illustration of the electrodynamic element of the preferred embodiment of the present invention; 
     FIG. 7 is the graphic portrayal of the electric and magnetic fields near the plane slow-wave structure used with the preferred embodiment of the present invention; 
     FIG. 8 is the graphic portrayal of the electric and magnetic fields inside and outside the cylindrical slow-wave structure with the preferred embodiment of the present invention; 
     FIG. 9 shows an illustration of two-conductor slow-wave structure with an impedance conductor and screen conductor with the fields of a preferred embodiment of the present invention; 
     FIG. 10 illustrates a two-conductor slow-wave structure with impedance conductors showing opposite directed radial spirals in the fields of a preferred embodiment of the present invention; 
     FIG. 11 illustrates the electric field concentration between conductors and electric field shifting outside conductors in an in-phase type wave in the electrodynamic element of the preferred embodiment of the present invention; 
     FIG. 12 illustrates an anti-phase type wave in the electrodynamic element of the preferred embodiment of the present invention; 
     FIG. 13 shows a bifilar helix; 
     FIG. 14 illustrates interdigital combs; 
     FIG. 15 illustrates coupled meander-lines of the preferred embodiment of the present invention; 
     FIG. 16 illustrates the real component of phase ratios and imaginary part dependence upon a surface resistivity. 
     FIG. 17 illustrate the preferred circuit of the attenuation measurement of the preferred embodiment of the present invention; 
     FIG. 18 illustrates the preferred circuit of the preferred embodiment of the present invention for phase delay measurement; 
     FIG. 19 illustrates the preferred circuit of the preferred embodiment of the present invention for variation of the phase delay converting into a generator&#39;s frequency alteration; 
     FIG. 20 illustrates the preferred circuit of the preferred embodiment of the present invention to convert alteration of resonant frequency into a generator&#39;s frequency; 
     FIG. 21 illustrates a slow-wave structure with impedance and screen conductors; 
     FIG. 22 illustrates an electrodynamic element including an additional slow-wave structure  57  and terminated to an inductor  58  having a large induction; 
     FIG. 23 illustrates an electrodynamic element wherein an additional slow-wave structure is replaced by two inductors; 
     FIG. 24 illustrates an electrodynamic element wherein an additional slow-wave structure is replaced by two capacitors; 
     FIG. 25 illustrates an electrodynamic element with an additional slow-wave structure terminated to a capacitor; 
     FIG. 26 illustrates varying the distance between conductors of a slow-wave structure; 
     FIG. 27 illustrates a varying of a screen conductor width; 
     FIG. 28 illustrates a simple version of “butterfly” design of the electrodynamic element; 
     FIG. 29 illustrates the “butterfly” design of FIG. 28 with an additional conductor and having a different connections arrangement; 
     FIG. 30 shows an electric field distribution near a plane “butterfly” electrodynamic element; 
     FIG. 31 shows a magnetic field distribution near a plane “butterfly” electrodynamic element; 
     FIG. 32 illustrates the insertion of a magnetic screen diametrically opposite to the monitored film; 
     FIG. 33 illustrates a magnetic screen; 
     FIG. 34 is graph showing the dependence of normalized resonant frequency upon surface resistivity; 
     FIG. 35 illustrates typical characteristics for electromagnetic parameters of thin film monitoring; 
     FIG. 36 illustrates an electrodynamic element with a slow-wave structure made from a rectangular helix wound on a dielectric base; and 
     FIG. 37 illustrates typical characteristics of “butterfly” electrodynamic elements. 
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     As shown in FIGS. 2-3, an electrodynamic element  1  may be placed in parallel to a monitored material  2 , opposite to the material  2  as shown in FIG. 2, or separated by a dielectric substrate  3 , as shown in FIG.  3 . Element  1  is connected to the measuring circuit  4 , comprising (FIGS. 4 and 5) a generator  5  of electromagnetic oscillations at RF or microwave frequency, primary transducer  6 , converting the electrodynamic parameters of electrodynamic element  1  into an electromagnetic informative signal, for example, resonance frequency, Q-factor, etc., and converter  7 , converting electromagnetic informative signals into information about a film&#39;s electromagnetic parameter, for example permeability or thickness. Electrodynamic element  1  can be connected to the generator  5  in parallel (FIGS. 3,  4 ) or in sequence, as it is shown in FIGS. 2,  5 . 
     In some cases, when electrodynamic element  1  is placed in an aggressive environment or in vacuum it can be installed in a case  8 , shown in FIG. 2 by dotted lines, or can be covered by a dielectric layer (not shown in Figures). 
     At least one slowed electromagnetic wave is exited in the electrodynamic element  1  at a frequency at which the electromagnetic field penetrates into material  2 . The material  2  can be represented by a thin film (FIG.  2 ), can be spread on the dielectric or semiconductor plate  3 , as it is shown in the FIG. 3, or may have configuration of a bulk (not shown in Figures). 
     In all above mentioned cases the electromagnetic field excited in the electrodynamic element  1  penetrates into the monitored region, e.g. material  2 . It means that the distance b between the electrodynamic element  1  and material  2  must not exceed the thickness δ of an “area of the energy concentration” which is approximately equal to λ/2πn, where λ is a wave-length in the medium between the element  1  and film  2 , n is slowing. In FIG. 2 it is the distance between element  1  and material  2 ; in FIG. 3 it is the substrate  3  thickness. 
     The electrodynamic element  1  comprises slow-wave structure  9  (FIG.  6 ), one end of which is connected to the input  10  and the other end to the output  11 , input  10  and output  11  also being included in the electrodynamic element  1 . Depending on the quantity (number) of slow-wave structure  9  conductors (impedance conductors  12 ,  13  and a screen conductor  14 , for example, in FIG.  6 ), the input  10  and the output  11  have two or more poles connected to slow-wave structure  9 . For example, as it is shown in FIG. 6, the poles  15 ,  16  are connected to the opposite ends (input and output, respectively) of impedance conductor  12 , and the poles  17 ,  18  (input and output, respectively) are connected to the opposite ends of the other impedance conductor  13 ; the poles  19 ,  20  (input and output, respectively) are connected to the opposite ends of the screen conductor  14 . 
     One or more types of slowed waves at one frequency and much more at different frequencies can be excited in such electrodynamic element, simultaneously, their number being equal to the number of conductors minus 1. See Z. I. Taranenko, Ya. K. Trochimenko “Slow-Wave Structures”  Kiev,  1965, p. 57. 
     The excited, slowed electromagnetic wave in the electrodynamic element  1  propagates along this element penetrating into monitored material  2 . The latter having an effect on the propagation constant γ and, as a result, on the slowing n and on the attenuation factor, that leads to alteration of electromagnetic parameters of the electrodynamic element  1 , such as resonance frequency f and Q-factor. 
     Any electromagnetic wave is characterized by so called “wave coefficient”, defining electric and magnetic fields E and H dependence on time t and coordinate z in the direction of wave propagation: 
     
       
           E, H˜e   jωt+γz , 
       
     
     where ω is an angular frequency and, as mentioned above, γ is a propagation constant, which can be presented by the expression 
     
       
         γ=− jβ−α.   
       
     
     Here j is the imaginary unit, β is the phase constant (β=ω/ν p ), ν p  is the phase velocity, α is the attenuation constant, related to the specific attenuation factor K a  in decibels/meter by the relation 
     
       
           K   a =8.68 α. 
       
     
     See V. V. Annenkov, Yu. N. Pchelnikov “Sensitive Elements Based on Slow-Wave Structures”  Measurement Techniques, Vol.  38, # 12, 1995, pp. 1369-1375. 
     The slowed electromagnetic wave is excited in electrodynamic element  1  with distribution of the electric and magnetic components of the field required for the best sensitivity. Usually, the field distribution is defined by the slowing n and the frequency f. Thus, when there is no boundary surface outside the impedance conductor, the longitudinal components of the electric field E z  and the magnetic field H z  of the wave are proportional to e −xτ′ , e −xτ″  for a plane system (curves  21  and  22  in FIG.  7 ), and are proportional to modified Bessel functions I 0 (rτ′), I 0 (rτ″) inside of a cylindrical slow-wave structure (curves  23 ,  24  in FIG.  8 ), or K 0 (rτ′), K 0 (rτ″) outside it (curves  25 ,  26  in FIG.  8 ). Here x and r are the coordinates along the normal to the surfaces of the impedance conductors and τ′, τ″ are two different values of the transverse constant τ, related to the different slowing values n′, n″ and the wave number k by the relations 
     
       
         (τ′) 2   =k   2 [( n ′) 2 −1], 
       
     
     
       
         (τ″) 2   =k   2 [( n ″) 2 −1],  k=ω   2 ∈ 0 μ 0 , 
       
     
     where ∈ 0  and μ 0  are the permittivity and the permeability of the vacuum, respectively. If the frequency changes and slowing n is constant, the wave number has different values, for example, k′, k″ that leads to transverse constant changing also 
     
       
         (τ′) 2 =( k ′) 2 ( n   2 −1), 
       
     
     
       
         (τ″) 2 =( k ″) 2 ( n   2 −1). 
       
     
     It is seen from the above that the wave number k is proportional to the angular frequency ω. If the frequency changes, the wave number also changes. The wave number alteration also leads to the transverse constant alteration. For two different frequencies one has two different wave numbers k′, k″. If slowing n is a constant, one has two different transverse constants τ′, τ″ for two different frequencies. 
     In FIGS. 7 and 8 τ″=2τ′ 
     It is seen from the expressions for τ′, τ″ and is shown in FIGS. 7 and 8, that a field distribution can be changed by a slowing n change, and by angular frequency ω change also. Thus, one can obtain different distribution of the field in the same electrodynamic element, exciting, for example, two or more slowed waves at different frequencies. 
     The field distribution can be changed by the different modes of the slowed wave exciting also. For example, the field distribution in FIG. 8 for bifilar helix was calculated for in-phase excitation. In this case the potentials of both helices are identical for diametrically opposite points. This means that the field components of an in-phase wave do not alter along the azimuth coordinate and are defined by the Bessel functions of the zero order. In case of anti-phase excitation the potentials of the helices have opposite signs and field distribution is defined by the Bessel functions of the first order, the field distribution being quite different from the distribution shown in FIG.  8 . 
     One of the most important peculiarities of slowed waves is the electric and magnetic field energy splitting between electric and magnetic type waves (E- and H-modes, respectively). See Dean A. Watkins “Topics in Electromagnetic Theory”, New York, John Wiley &amp; Sons, Inc., p. 63. When the slowing n is sufficiently great, the energy of the electric field of the slowed wave is concentrated mainly in the E-mode, while the energy of magnetic field is concentrated mainly in the H-mode, both modes existing in the slowed wave only together. Because of this the electromagnetic parameters of the monitored material  2  (the conductivity, the permittivity, and the permeability) have a different effect on the E-modes and H-modes, thus manifesting their own kind of an anisotropy. See Yu. N. Pchel&#39;nikov “Anisotropy of a Semiconductor Film in the Field of a Slow Wave”,  Journal of Communications Technology and Electronics, Vol  39, # 10, 1994, pp. 66-69. This effect is due to the absence of the longitudinal component of electric field in the H-mode and due to the absence of the longitudinal component of magnetic field in the E-mode wave, that follows from Maxwell&#39;s equations. See L. N. Loshakov and Yu. N. Pchel&#39;nikov “Theory and the traveling-wave tube gain calculation”,  Sov. radio:  1964, p.p. 217-218. It leads, for example, to the H-mode insensitivity to a longitudinal conductivity and permittivity and E-mode insensitivity to a transverse conductivity and permittivity. It follows also from Maxwell&#39;s equations that the electric energy of H-mode slowed wave and the magnetic energy of E-mode wave are smaller by factor of n 2  than electric and magnetic energy accordingly, where n is the considered wave slowing. This enables one, on the one hand, to make independent measurements, for example, of the electric permittivity and magnetic permeability, while on the other hand it enables one to control the distribution of the electric and magnetic fields across the transverse section of the electrodynamic element  1 . Thus, screening by a screen conductor of the E-mode reduces the amount of the electric-field energy in the measured volume compared with the amount of the magnetic-field energy by more than a factor of n 2 . 
     As mentioned above, slowing of the electromagnetic wave leads to electric and magnetic energy splitting between E- and H-waves. It follows from this, that the E-wave is not sensitive enough to permeability and the H-wave is not sensitive enough to permittivity of the material  2 . This energy splitting makes the E-wave sensitive to small resistivity only, and makes H-wave sensitive to big resistivity only, see Yu. N. Pchel&#39;nikov “Anisotropy of a Semiconductor Film in the Field of a Slow Wave”// Journal of Communications Technology and Electronics, Vol.  39, # 10, 1994, pp. 66-69. 
     Analyzing a slow-wave structure as being replaced by a long line with an equivalent inductance L 0  and an equivalent capacitance C 0 , the first being proportional to the stored magnetic energy, the second being proportional to the stored electric energy, the slowing n in a long line is defined by formula 
     
       
         
           n={square root over (L 0   C   0 /∈ 0 μ 0 )}, 
         
       
     
     see Yu. N. Pchelnikov “On the Replacement of Slow-Wave Systems by a Three-Conductor Equivalent Line”  Journal of Communications Technology and Electronics, Vol.  39, # 3, 1994, pp. 68-74. It follows from this that a magnetic material would increase inductance, a dielectric material would increase capacitance, and both of these would increase the slowing n. The relatively big resistivity screens electric field, increasing capacitance C, and does not change the inductance L. The relatively small resistivity screens electric and magnetic fields, decreasing inductance L, and does not changes capacitance, the capacitance being maximum. To obtain maximum sensitivity one must shift electric or magnetic energy in the monitored material  2 . 
     In the simplest cases, the distribution of electric and magnetic fields is as shown in FIGS. 7 and 8 and is formed, for example, by a two-conductor slow-wave structure  9  with an impedance conductor  12  and a screen conductor  14  (FIG.  9 ). Here an electric (E) field and a magnetic (H) field are distributed between conductors  12 ,  14  and outside the impedance conductor  12 . 
     The field distribution can be changed essentially in so called coupled slow-wave structures, which impedance conductors  12 ,  13  have configuration of turned through 180°, mirror images of one another, for example, oppositely directed radial spirals, shown in FIG.  10 . Here the conductors  12 ,  13  are made as arithmetic spirals with opposite direction of winding. In such structures electric and magnetic energy can be split in transverse section of such structures, and this splitting can be controlled by exciting in-phase or anti-phase types of waves. 
     When exciting an in-phase type wave in the electrodynamic element  1  with two coupled impedance conductors  12 ,  13 , connected one to another, and a screen conductor  14 , the magnetic field energy is concentrated between conductor  12  and conductor  13  (FIG.  11 ), while an electric field energy is shied outside conductors  12 ,  13 . This can be explained by the different directions of the transverse components of currents in conductors  12 ,  13  and by equality of its potentials. The transverse components direction is perpendicular to the direction of the wave propagation. 
     In the second case (anti-phase excitation) the energy of the electric field is concentrated between impedance conductors  12 ,  13  (FIG.  12 ), while a magnetic field energy will be shifted outside conductors  12 ,  13 . It can be explained by the transverse components of the currents in conductors  12 ,  13  directions coincidence and by the opposite potentials on the conductors  12 ,  13 . In this case, if one wave is excited only, the screen conductor  14  can be absent. If both, anti-phase and in-phase waves should be excited, the electrodynamic element  1  should include impedance conductors  12 ,  13  and screen conductor  14 . 
     The distribution of electric and magnetic components of a slowed electromagnetic wave excited in the electrodynamic element  1  must be chosen depending upon electric parameters of the math (film, bulk)  2  being monitored. As it was mentioned earlier, the dielectric material&#39;s effect is proportional to the electric energy concentration in the dielectric material  2 . Thus, in the case of dielectric film  2  (non-conductive or poorly-conductive), the electric component of the slowed electromagnetic wave must be shifted into the monitored volume. If a material  2  has dielectric and ferrite properties simultaneously, for example it is ferrite, both electric and magnetic fields should be shifted in the monitored volume simultaneously or in two different electrodynamic elements  1 . If the monitored material  2  is conducting, the magnetic field will effect oppositely to that of the electric field. Thus the magnetic field should be shifted from monitored volume, as it is shown in FIG. 11 or, alternatively, the electric field should be shifted from the monitored material  2 , as it is shown in FIG. 12, depending on the material. For material  2  being conductive, the current induced on the metal surface by the magnetic field of the electrodynamic element  1  would increase this magnetic field in the region between electrodynamic element  1  and material  2 . 
     If the electrodynamic element  1  is at least hexapole (FIG.  6 ), in-phase and anti-phase waves can be excited simultaneously, or one after another. It allows more informative parameters to be obtained. Two or more resonant frequencies can be utilized, which would permit obtaining two or more informative parameters. For example, if the material  2  is thin film to be monitored, the equivalent surface permittivity ∈ □  is a multiple of the specific relative permittivity ∈ and material  2  thickness a. 
     
       
         ∈ □   =a∈   0 ∈. 
       
     
     In the case of relatively thick material when the equivalent surface permittivity depends on field penetration in this material, the surface permittivity depends also upon the frequency f i   
     
       
         ∈ □1   =G ( a, ∈   0   ∈, f   i ), 
       
     
     where G is a function, which is the same for different frequencies, i.e. is frequency independent. 
     The influence of material  2  having equivalent surface permittivity ∈ □  on a deceleration n and, as a result, on a resonant frequency f i , depends, in its turn, on the frequency f i  and the distance b between electrodynamic element  1  and the material  2 . This influence is described by some function F i  depending on a resonance number i or the type of the wave excited in electrodynamic element  1   
     
       
           f   i   =F   i (∈ □1   , b ),  i= 1, 2, 3 . . .  
       
     
     If, for example, the distance b and thickness a are unknown but constant, having results of measurements of two different frequencies f 1  and f 2 , one can exclude the distance b and thickness a from the equations 
     
       
           f   1   =F   1 (∈ □1   , b ),  f   2   =F   2 (∈ □1   ,b ), ∈ □1   =G ( a, ∈   0   ∈, f   1 ), ∈ □2   =G ( a, ∈   0   ∈, f   2 ). 
       
     
     This makes it possible to calculate ∈ □ . 
     ∈′ □ , ∈″ □  can then be calculated by having obtained two different measurements both the relative permittivity ∈ and the thickness a with help of the measurement results represented by the equations: 
     
       
           e′   □   =F ( a, f   1   , b ), 
       
     
     
       
         ∈″ □   =F ( a, f   2   , b ). 
       
     
     Analogously, if the thickness a is constant and the distance b changes, the distance b can be excluded from the two above-mentioned equations. The temperature and other parameters also can be excluded, the number of excluded influences being equal to the informative parameters number minus one. The number of informative parameters can be increased by exciting one or both types of waves at different frequencies, for example, at the first resonant frequency, second, etc. 
     In the mentioned example the distance b to a relatively well conducting film can be measured by the in phase wave, while the approximate value of the conductivity can be measured by the anti-phase wave. Comparing of the measured values allows the calculation of an accurate value of the conductivity. 
     As it was shown earlier, the degree of energy concentration near the electrodynamic element  1  depends on slowing down rate n, and frequency f, and increases as n and f increase. It is true for fields presented by the zero space harmonic. The same effect of energy concentration can be obtained by exciting an E- or H-mode wave, or both, with fields presented by the first (plus one and minus one) space harmonics. See Dean A. Watkins “Topics in Electromagnetic Theory”, New York, John Wiley &amp; Sons, Inc., p. 2, and Yu. N. Pchelnikov, V. T. Sviridov, “Microwave Electronics”  Moscow: Radio - Svjaz,  1983, p. 44. For example, the distance b to a relatively well conducting material can be measured by the in-phase wave excitation, while the equivalent surface conductivity of the monitored material can be measured by the anti-phase wave excitation. When in-phase wave is excited, the conductivity σ □  of the monitored material  2  is large enough to increase the equivalent capacitance of the electrodynamic element  1  to its maximum value and its resonant frequency f 1  depends on the equivalent inductance L which decreases with the distance b 
     
       
           f   1 =Ξ 1 ( b ), 
       
     
     where Ξ 1 (b) is a function defined for in-phase wave. When an anti-phase wave is excited the electric field outside the electrodynamic element  1  is very small and the conductivity σ □  does not influence the equivalent capacitance changing the equivalent inductance L. In this case 
       f   2 =Ξ 2 (σ □   , b ), 
     where Ξ 2 (σ □ , b) is a function defined for anti-phase wave. Solving f 1 =Ξ 1 (b) and f 2 =Ξ 2 (σ □ , b) together, one can exclude the distance b and to obtain an equation which defines value of the conductivity 
     
       
         σ □ =ψ( f   1   , f   2 ), 
       
     
     where ψ(f 1 , f 2 ) is function of measured frequencies f 1  and f 2 . As it was said earlier, the degree of energy concentration near the electrodynamic element  1  depends on slowing down rate n, and frequency, and increases as n and f increase. Indeed, the energy of electric field W e  concentration is proportional to the electric field intensity amplitude E squared, the energy of magnetic field W m  is proportional to the magnetic field intensity amplitude H squared 
     
       
           W   e =∈∈ 0   E   2 /4,  W   m =μμ 0   H   2 /4. 
       
     
     Here ∈∈ 0  and μμ 0  are absolute permittivity and absolute permeability. With the field amplitudes being proportional to exp.(−τx), the energy concentration is proportional to exp.(−2τx). It is true for fields presented by the zero space harmonic. 
     The same effect of energy concentration can be obtained by exciting an E- or H-mode wave, or both, with fields presented by the first (plus one and minus one) space harmonics. See Dean A. Watkins “Topics in Electromagnetic Theory”, New York, John Wiley &amp; Sons, Inc., p. 2, and Yu. N. Pchelnikov, V. T. Sviridov, “Microwave Electronics”  Moscow: Radio - Svjaz,  1983, p. 44. In this case the energy density is proportional, for example, to exp.(−4πx/T), where T is the period of a two stage slow-wave structure such as meander line or interdigital comb, or proportional to exp.(−2πx/T), where T is period of a one stage slow-wave structure such as bifilar helix. As a rule, 2πx/T, 4πx/T&gt;&gt;2τx and, as a result, the depth of the field penetration into the monitored volume (a thickness δ of the energy concentration area) is much smaller than in the case of zero space harmonic and is determined not by the frequency, the slowing, or the conductivity, as it is in the case of zero space harmonic, but it is determined by the period T of the slow-wave structure. 
     As it follows from the above, in the case of the first space harmonics, energy concentration near impedance conductors  12 ,  13  is greater than in case of zero space harmonic (the area of energy concentration δ is smaller). Such effect of the field concentration can be used at relatively low frequencies to increase sensitivity. 
     With the phase constant β for the first harmonics being approximately equal to π/T for symmetrical structures, for example, bifilar helix with anti-phase excitation (FIG. 13) and being approximately equal to 2π/T for two-stage structures, for example, interdigital combs (FIG. 14) with slowing N defined as β/k, where k=2π/λ (λ is a wavelength in free space), one can find out that phase velocity of the first harmonics slowing is defined as λ/T for two-stage structures or λ/2T for symmetrical structures. Taking into account that sensitivity is proportional to the slowing value: 
     
       
           S ˜( V/V   0 )λ/2 TF (∈, μ, σ) f   1 , 
       
     
     or 
     
       
           S ˜( V/V   0 )λ/ TF (∈, μ, σ) f   1 , 
       
     
     where λ is a wavelength in the vacuum. Substituting f 1 =c/λ, where c is the velocity of the light in the vacuum, we obtain 
     
       
           S ˜( V/V   0 ) c/ 2 TF (∈, μ, σ), 
       
     
     or 
     
       
           S ˜( V/V   0 ) c/TF (∈, μ, σ). 
       
     
     It is seen, that in the case of the first harmonics sensitivity S does not depend on frequency and increases with period T decreasing. 
     In most cases slowed waves are so called hybrid waves, comprising both, E- and H-mode waves, and these waves can be presented by different space harmonics. For example, the E-mode in a meander-line (FIG. 15) is presented on the whole by the zero space harmonic, while the H-mode is presented by the first harmonics. The in-phase type wave in the bifilar helix (FIG. 13) comprises E- and H-modes, which are presented by zero space harmonic; the anti-phase type wave comprises the E- and H-modes both being presented by plus one/minus one harmonics. 
     Existence of a certain distance b between electrodynamic element  1  and the monitored material  2  decreases sensitivity S approximately by a factor of exp.(−bτ) because of the lowering of the electric and magnetic field strength, so that as b increases the ability to measure the monitored material  2  electric parameters decreases. Thus it appears that good sensitivity requires the distant b to be maintained relatively small and constant. 
     In the case of thin films monitoring the dependence of the propagation constant γ upon the distance b as it follows from an analysis for relatively large slowing (when n≈τ/k), may be small. The conditions required for such small dependence may be used for the decreasing of the distance b influence. The measuring error does not exceed 3% when the distance b alteration does not exceed 30% if 
     
       
         ∈ □ &lt;0.3λ/2π n   
       
     
     
       
         ρ □ &gt;126 n   
       
     
     for E-wave and 
     
       
         μ □ &lt;0.3λ/2π n   
       
     
     
       
         ρ □ 126/ n,   
       
     
     for H-wave, where λ is wavelength in free space, n is the wave slowing down in comparison to the velocity of fight in vacuum. 
     A variation in the material  2  electromagnetic parameters and thickness causes a variation of the propagation constant γ depending on the field distribution in the slowed electromagnetic wave. For example, dielectric and magnetic materials increase the imaginary part of the propagation constant γ, phase constant β; low conductive films increase the real part of the propagation constant γ attenuation constant α; highly conductive films decrease β and increase α. 
     It follows from long line theory (see Yu. N. Pchelnikov “Comparative Evaluation of The Attenuation in Microwave elements”//Soviet Journal of Communications Technologies and Electronics, Vol. 32, # 11, 1987, pp. 74-78), that 
     
       
         β/β 0   =Re{square root over (LC/L 0   C   0 )},   
       
     
     
       
         α/β 0   =Im{square root over (LC/L 0   C   0 )},   
       
     
     where β 0  is a phase constant of the slowed wave and L, C are specific inductance and capacitance in the presence of monitored material  2 . It is important that dependence of β and α are not monotonous and have maximums (the attenuation constant α has two maximums). It is seen from FIG. 16, where the curve  27  demonstrates a real part of LC/L 0 C 0  dependence upon a surface resistivity ρ □  and the curve  28  demonstrates an imaginary part of LC/L 0 C 0  dependence, calculated for slowing n=33 for the simplest design of electrodynamic element  1 , when electric field and magnetic field in the monitored material  2  have equal intensity. Note that the ordinate of FIG. 16 is the relative values of real and imaginary of the phase constant shown in FIG.  16 . 
     The variation of the real part of the propagation constant γ is indicated by the attenuation of the slowed electromagnetic wave in the electrodynamic element  1 . The preferred circuit of the attenuation measurement is shown in FIG.  17 . Here the electromagnetic signal from the output  29  of the generator  5  (standard RF generator can be used) passes through the end  30  of the signal divider  31 , input  10  of the electrodynamic element  1 , slow-wave structure  9  and output  11 , passes through the input  32  of a standard amplitude comparator  33  and is compared with the signal from the end  34  of the signal divider  31 , connected to the input  35  of the comparator  33 . The results of this comparison in voltage are converted into a material&#39;s  2  parameter by the converter  7 , which can be standard voltmeter. Other measuring circuits can be used too. 
     The variation of the imaginary part of the propagation constant γ is indicated by the phase delay measurement. The preferred circuit is shown in FIG.  18 . Here the electromagnetic signal from output  29  of generator  5  passes through end  30  of the signal divider  31 , input  10  of the electrodynamic element  1 , slow-wave structure  9 , output  11  and to input  36  of a standard phase comparator  37  with the voltage output, its phase being compared with phase of a signal coming to the input  38  of the comparator  37  from the end  34  of the signal divider  31 . The results of this comparison in voltage are converted into a film&#39;s parameter by the converter  7 , which can be a standard voltmeter. Other measuring circuits can be used also. 
     The variation of the phase delay can be also converted into generator  5  frequency alteration Δf. It can be done, for example, by the electrodynamic element  1  sequence inserting in the feedback network  39  of amplifier  40  (FIG.  19 ). Filter circuits  41  and  42  in feedback  39  can be inserted to increase stability of the generator  5 . In this case the generator  5  takes part of the primary transducer  6  for use of measurement, converting a phase delay alteration into the frequency alteration. 
     The variation of the imaginary part of the propagation constant γ can be also indicated by the resonance frequency f i  of the electrodynamic element  1  variation. If the slow-wave structure  9  is open ended (the output  11  is open), 
     
       
           f   i   =c (2 i−l )/(4 b·n ), 
       
     
     where c is the light velocity in the vacuum, i=1, 2, . . . is a resonant frequency number, l is the length of the slow-wave structure  9 , n is a slowing down value. 
     If the slow-wave structure  9  is short ended (the end  11  is closed), then 
     
       
           f   i   =ci /(2 l·n ). 
       
     
     The resonance frequency f i  can be measured by standard net analyzer or by other devices. If electrodynamic element  1  includes a two-conductor slow-wave structure  9 , for example a bifilar helix, the preferred circuit to convert alteration to resonant frequency as the informative parameter is very simple. It combines, as it was in the previous example, the generator  5  and transducer  6  (FIG.  20 ). In FIG. 20, the pole  15  of the electrodynamic element  1  is connected to the inverting input  43  of an operational amplifier  44 ; the other pole  17  is connected to the earth. (Alternatively pole  19  could be grounded to earth if the other conductor of the slow-wave structure  1  would be screen conductor  14 ). The poles  16 ,  18  can be open ended, short ended or terminated. It depends on the monitored material  2  electric parameters. For example, if it is dielectric or low conducting material, they can be open ended or terminated with a big inductance. Simultaneously, the inverting input  43  is connected through a resistance  45  to the output  46  of amplifier  44  and the non-inverting input  47  is connected through a resistance  48  to the output  46  and is connected through a resistance  49  to the earth, forming a Schmitt trigger (see E. C. Young “ The Penguin Dictionary of Electronics”, second edition,  p. 505). The signal from the output  46  has a meander configuration, with frequency near the resonance frequency of the electrodynamic element  1 . 
     The analysis of the slow-wave structure with dielectric material shows that the slowing n growth with increases of surface permittivity and surface permeability reaches saturation, see Yu. N. Pchel&#39;nikov, A. A. Elizarov “Ferrite Plate in the Decelerated Wave Field”  Radioelectronics and Communications ions Systems  (Iz. VUZ.  Radioelektronika ), Vol. 37, # 10, 1994, pp. 44-49. It is shown in this work that electromagnetic parameters of relatively thick plates can be described by equivalent surface parameters(μ □ , ∈ □ ) Presume that saturation begins from the point on the monitored parameter if further increasing until infinity does not change the equivalent inductance L or equivalent capacitance C more than 10%. In this case, as it follows from the analysis, the saturation begins if 
     
       
         μ □ &gt;10( cthbτ−thb τ)λ/2π n   
       
     
     or 
     
       
         ∈ □ &gt;10( cthbτ−thb τ)λ/2π n,   
       
     
     where cth and th are hyperbolic cotangent and tangent, respectively. 
     The analogous conditions can be obtained for resistive film. The slowing saturation in E-wave takes place when 
      ρ □ &lt;37.7 n /( cthbτ−thb τ) 
     and in H-wave when 
     
       
         ρ □ &lt;37.7/ n ( cthbτ−thb τ). 
       
     
     The same effect takes place if the material  2  electromagnetic parameters are too small and their influence on equivalent capacitance or equivalent inductance are very low. In this case it follows from the expressions for L and C that they do not exceed L 0 , C 0  more than 10% if in E-wave 
     
       
         μ □ &lt;0.1λ(1+ thb τ)/2π n (1− thb τ), 
       
     
     or 
     
       
         ∈ □ &lt;0.1λ(1+ thb τ)/2π n (1− thb τ), 
       
     
     or 
     
       
         ρ □ &gt;3.77·10 3   n (1− thb τ)/(1+ thb τ); 
       
     
     and in H-wave when 
     
       
         ρ □ &gt;3.77·10 3 (1− thb τ)/ n (1+ thb τ). 
       
     
     It is seen from FIG. 16, that in case of resistive film there are four regions of LC/L 0 C 0  saturation, two of them for relatively small resistivity (region  50  for H-wave, and region  52  for E-wave) and two of them for relatively big resistivity (region  51  for H-wave and region  53  for E-wave). In the region  50  the film, having small resistivity, screens the electric and magnetic fields. As a result, the inductance L has its minimum value L min  and capacitance C has its maximum value C max . Any alteration of resistivity in this region doesn&#39;t change the inductance and capacitance. The further resistivity increasing is followed by the decreasing of the magnetic field screening and, hence, the inductance L increasing to its maximum value L 0 , related to the beginning of the region  51 . The capacitance C remains maximum till the resistivity values, related to the region  52  end. The further resistivity increasing leads to the capacitance C decreasing to its minimum value C 0 , related to the region  53 . 
     It is seen from FIG. 16 that when a resistive film is monitored, the imaginary part of LC measurement can be preferred if resistivity relates to regions  50 ,  51 ,  52  and  53 . 
     It can be shown that in all the above mentioned measurements there are conditions required for obtaining maximum sensitivity. The most convenient for measuring estimation is so called relative sensitivity S r , that in the case of slowing change can be defined as 
     
       
           S   r =(ξ/ n )·(∂ n /∂ξ), 
       
     
     where ξ is the monitored parameter. 
     The magneto-dielectric plate in the slowed wave analysis shows: when the surface permittivity or permeability is monitored, the relative sensitivity is maximum if 
     
       
         ∈ □ =(1+ thb τ)λ/2π n,   
       
     
     or 
     
       
         μ □ =(1+ thb τ)λ/2π n.   
       
     
     See Yu. N. Pchel&#39;nikov, A. A. Elizarov “Ferrite Plate in the Decelerated Wave Field”  Radioelectronics and Communications Systems  (Iz. VUZ:  Radioelektronika ), Vol 37, # 10, 1994, pp. 44-49. 
     As is set out above, the apparatus for materials (films and bulks) electric parameters monitoring comprises an electrodynamic element  1 , connected to a measuring circuit  4  (FIGS.  2 - 3 ), the last including a generator  5  of electromagnetic oscillations, a transducer  6 , connected to a converter  7 , converting an electric signal to indicate the measured parameters (FIGS.  4  and  5 ). Electrodynamic element  1  (FIG. 6) includes at least one slow-wave structure  9 , input  10  and output  12 , connected to the ends of the slow-wave structure  9 . In some cases the output  11  can be absent, the conductors  12 ,  13 ,  14  being open or connected one to the other. The slow-wave structure  9  includes at least two conductors, which at least one is an impedance conductor, for example conductor  12 , fashioned as a row of conducting members arranged in series in the direction of the slowed wave propagation (arrow A of FIG. 6) and connected to one another with spacing. The other conductors can be impedance conductor  13  and a screen conductor  14 , made as a tape, plate, cylinder, etc. For example, impedance conductor  12  in FIG. 21 includes conducting fingers  54  connected one to another in the direction of arrow a in FIG. 21 by a conducting base  55  with gaps  56 . The screen conductor  14  may be made as a conducting plate. 
     Also, as discussed above, slow-wave structure  9  can include two or more impedance conductors ( 12 ,  13  in FIG. 6) and, sometimes, one screen conductor  14 . From one end of slow-wave structure  9 , all its conductors are connected to the input  10 , each to one pole, for example, impedance conductor  12  in FIG. 6 is connected to the pole  15 , impedance conductor  13 —to the pole  17  and the screen conductor  14 —to the pole  19 . From the other end of the slow-wave structure all its conductors are connected to the output  11 , conductor  12 —to the pole  16 , conductor  13 —to the pole  18 , conductor  14 —to the pole  20 . The input  10  and output  11  can be standard coaxial adapters, or can be made from cable or wires. The output  11  can be absent. 
     In some cases, when the distribution of electric or magnetic field along the slow-wave structure should be homogeneous, a section of slow-wave structure  57  described below (FIGS. 22,  25 ) should be added in series to the slow-wave structure  9 . If the electrodynamic element  1  is open ended or terminated to an inductor  58  having big inductance, as it is shown in FIG. 22, the slow-wave structure  57  must have the wave impedance (characteristic impedance) Z 1  much bigger than the wave impede Z 2  of the slow-wave structure  9 . If the electric length (a phase delay φ) in both structures is the same (the preferred case), the first resonance frequency f 1  of the electrodynamic element  1  is defined by the expression (see Yu. N. Pchehnikov, A. A. Elizarov, “Quasiresonators Using Slowing Down Systems”  Radioelectronics and Communications Systems,  Vol. 34, # 10, 1991, pp. 68-72.) 
     
       
           f   1   =cφ/ 2π nl, φ≈{square root over (Z 2   /Z   1 )},   
       
     
     where c is the velocity of light in vacuum, l is the slow-wave structure  9  length, n is slowing in the slow-wave structure  9 . In this case a distribution of the electric-field energy along slow-wave structure  9  is proportional to 
      cos 2   βz, φ≧βz,   
     where β is the phase constant in the slow-wave structure  9 , z is the coordinate along the structure  9 . Thus, if the phase delay φ is smaller 0.3 (that is Z 1 /Z 2  is larger than 9), 
     
       
         cos 2   βz&gt; 0.8. 
       
     
     This means the electric-field energy decrease along the electrodynamic element  1  is smaller than 20%. 
     In the case under consideration the additional slow-wave structure  57  can be replaced by two inductors  59 ,  60  with relatively small inductance L 1  and L 2 . (FIG.  23 ). Though the preferable case is when L 1 =L 2 =Z 2 /πφ, and one inductor also can be used. 
     If electrodynamic element  1  is short ended or terminated to a big capacitance  61 , as it is shown in FIG. 25, and homogeneous distribution of the magnetic field energy along slow-wave structure  9  should he obtained, the wave resistance Z 1  of the additional slow-wave structure  57  must be chosen much smaller than the wave resistance Z 2  of the slow-wave structure  9 . In this case, if a phase delay in both slow-wave structures is the same and equal to φ, the magnetic field energy distribution along slow-wave structure  9  is proportional to 
     
       
         cos 2   βz   
       
     
     and 
      φ≈ {square root over (Z 1   /Z   2 )}.   
     If φ&lt;0.3, Than cos 2 βz&lt;0.8 and the magnetic field distribution along the electrodynamic element  1  does not alter more than 20%. The additional slow-wave structure  57  can be replaced by two capacitors  62 ,  63  with relatively big capacitance C 1  and C 2  (FIG.  24 ). Though the preferable case is when C 1 =C 2 =1/Z 2 πφ, and one capacitor also can be used. 
     The energy distribution in the monitored volume can be adjusted also by the variation of the distance d between slow-wave structure  9  conductors, for example, between impedance conductor  12  and the screen conductor  14 , as it is shown in FIG.  26 . The increasing distance between conductors  12 ,  14  leads to the energy increasing in the area  64  outside the conductor  12 . The same effect can be achieved by the conductor  14  width w altering along the structure  9 , as it is shown in FIG.  27 . The width decreasing as the distance increasing is accompanied by a screening decreasing. 
     Usually, impedance conductors  12 ,  13  of the slow-wave structure  9  have a constant period T, as it is shown in FIG.  21 . The slowing n varies approximately in inverse proportion to T. Changing the slowing n one can change the energy concentration in the material  2 , the last being approximately proportional to slowing n. It follows from this that the T variation along the slow-wave structure  9  can be used for the energy distribution adjustment. 
     When electrodynanic element  1  is used as a quarter-wavelength resonator, the potential difference between element  1  and the monitored material is equal to ¼ of the potential difference between impedance conductors  12 ,  13  and ½ of the potential difference between the impedance conductor  12  or conductor  13  and the screen conductor  14 . As a result the sensitivity decreases. This disadvantage can be eliminated in the “butterfly” design of electrodynamic element  1 . The simplest version of such design is shown in FIG. 28, where the impedance conductors  12 ,  13  are placed on the same geometrical surface, for example plane, and directed in the opposite directions A 1  and A 2 , as it shown in FIG.  28 . In this case the electrodynamic element  1  has no output  11  and the ends  65 ,  66  of the impedance conductors  12 ,  13 , opposite to that connected to poles  15 ,  17  of the input  10 , can be free, as it is shown in FIG. 28, or connected to the ends  67 ,  68  of the screen conductor  14  by connectors  69 ,  70 , as it is shown in FIG.  29 . 
     The advantages of the “butterfly” design are: 
     The relatively homogeneous distribution of electric energy along the conductors  12 ,  13 , if the ends  65 ,  66  are free (FIG.  30 ), and the relatively homogeneous distribution of magnetic energy, if ends  65 ,  66  are connected to ends  67 ,  68  of the screen conductor  14 , respectively (FIG.  31 ). It can be explained by the increasing of potential difference in the directions of A 1 , A 2 , in the first case, and the magnetic field intensity, in the second case, simultaneously with increasing of the distance between corresponding points of the conductors  12 ,  13 . 
     The potential of the monitored material  2  is equal to zero and, hence, the potential difference between element  1  and material  2  is equal to potential amplitude. 
     The screen conductor  14  can be eliminated, that leads to energy increasing in the material  2 . 
     As it follows from the results of calculation and experiment, all of the above factors permit increasing sensitivity of the “butterfly” sensors by a factor of four. 
     When permittivity or big resistivity is measured, the capacitance between the monitored material  2  and dance conductor  12  or conductor  13  or both conductors  12 ,  13  has the value of the same order as the equivalent capacitance C 0 , and that makes it possible to achieve maximum sensitivity. When permeability is measured, the equivalent inductance of slow-wave structure L 0  can be increased only by a factor of two, which does not allow good sensitivity. To increase sensitivity of the permeability measurement, one can decrease magnetic resistance, inserting magnetic screen  71  symmetrically to the monitored material  2 , for example, as it is shown in FIG. 32, where it is placed between the screen conductor  14  and the dielectric base  72 , supporting the impedance conductor  12 . If the magnetic screen  71  is made from non-conducting material, it can be used as a supporting base for slow-wave structure  9 . 
     The magnetic screen  71  can be fashioned as a row of conducting tapes  73 , arranged along the direction of the slowed wave propagation. In FIG. 33 tapes  73  are arranged along the coupled spirals&#39; radii. In this case tapes  73  should be isolated one from the other and from spirals; for example, they can be installed on a dielectric film. 
     A typical set of curves in FIG. 34 shows dependence of a normalized resonant frequency f/f 0  upon surface resistivity ρ □ , where f 0  is the resonant frequency of electrodynamic element  1  without monitored material  2 . The curve  74  represents rests of measurements, carried out with help of coupled arithmetic spirals with slowing n≈500 for thin metal films on dielectric substrate. The curve  75  represents results of measurements, carried out with help of an arithmetic spiral with a screen conductor  14 , made as a tape, for implanted semiconductor substrates. The slowing in the last case was much smaller (n≈50). The curve  76  in FIG. 34 demonstrates theoretical versus calculated for slowing n≈100. 
     A typical characteristics of a transducer for electromagnetic parameters of thin films monitoring are shown in FIG.  35 . This transducer comprises “butterfly” electrodynamic element  1  with slow-wave structure  9 , made from rectangular helix (FIG. 36) and generator  5 , made as Schmitt trigger (FIG.  20 ). The helical conductors  12 ,  13  are wound on dielectric plate  77  (FIG.  36 ). The curve  78  in FIG. 35 demonstrates the relative frequency f/f 0  of generator  5  dependence upon artificial dielectric equivalent impedance 1/ω∈ 0 ∈ □ . Here, for comparison, curve  79  demonstrates frequency f/f 0  of generator  5  dependence upon surface resistivity ρ □ . 
     Typical characteristics of“butterfly” electrodynamic element  1  with conductors  12 ,  13  made as a meander lines and the conductor  14  made as one tape, are shown in FIG.  37 . Here, curve  80  shows dependence of the element&#39;s  1  normalized resonance frequency f/f 0  of element  1  upon the resistivity ρ □  of film  2 . The curve  81  demonstrates the attenuation factor K a  dependence upon the surface resistivity ρ □ . 
     The experimental results, shown above and results of practical application show the simplicity of realization, large sensitivity, accuracy and usefulness of the invention. 
     The preferred embodiment of the invention is relative measurements of thin films&#39; electromagnetic parameters. 
     All of the features of a particular preferred embodiment of the waveguide assembly are not shown in the above disclosure in order to emphasize the generality of the disclosure. 
     Because many varying and different embodiments may be made within the scope of the invention concept taught herein which may involve many modifications in the embodiments herein detailed in accordance with the descriptive requirements of the law, it is to be understood that the details herein are to be interpreted as illustrative and not in a limiting sense.