DE1464350A1 - Method for generating electromagnetic radiation for therapeutic purposes and device for carrying out this method - Google Patents

Description

DIPL-ING. HORST ROSE DIPL-ING. PETER KOSEL PATENTANWÄLTE 1464 35 Q

3353 Bad Gandersheim, September 4, 1968 »HKsHflcacflMBKKiac Hohenhöfen 5

Telephone (05387) 2842

Telegram address: Siedpatent Bod Gondenheim

PH 64 350.6
Antoine Priore

Method for generating electromagnetic radiation for therapeutic purposes and device for carrying out this method

The invention relates to a method for generating electromagnetic radiation for therapeutic purposes Purposes and to a device for carrying out such a method.

Such electromagnetic radiation for therapeutic purposes is used in living organic tissue penetrate in order to produce certain intended effects there without affecting important components of the tissue , e.g. the enzymes would be destroyed.

It is known to apply electromagnetic radiation to living tissue in order to achieve therapeutic effects different wavelengths or with bundles of rays from electrically charged particles or simultaneously to irradiate with electromagnetic radiation and such particle beams, in the latter Pall the Particles emitted by a radioactive body or by an electronic cathode ray generator will.

The invention is based on the object i to a process for generating electromagnetic radiation specify that a particularly good therapeutic efficacy on the connecting tissue to be irradiated with a large adaptability to the type of tissue to be irradiated.

2352/1 pc

M / .Q * 3 ο

nkltonlo: Braunsdiwaigisch "Staatsbank, Filiole Bod Gandersheim, account no. 22.118.970 · Posljcheckkonlo: Hannover «715

H64350

This is achieved according to the invention in that a beam of electrically charged particles and thereof separately a directed electromagnetic radiation in the cm-wave range are generated, this particle and Wave radiation are superimposed on each other, the radiation mixture is directed onto the surfaces of plague bodies, a gas discharge plasma generated in the volume range of these plague surfaces and an electromagnetic radiation in the m-wave range irradiated into the volume of the gas discharge plasma will. In this way, through the interaction between the cm-wave radiation and the ionized Molecules of the environment or of the plasma and a resulting electromagnetic radiation from the radiation of the m-wave radiation Radiation is generated whose wavelength is between the wavelengths of the m-wave radiation and the wavelengths visible radiation. Such electromagnetic radiation is special in therapeutic treatment effective and beneficial. The resulting radiation is preferably a unidirectional magnetic field great strength superimposed, which is advantageously pulsed in a rhythm of 30 to 120 oscillations / min, and in further improving the invention in a rhythm that corresponds to the heart rhythm of the resulting Radiation corresponds to the living being to be treated.

Experiments have shown that the resulting electromagnetic radiation when applied to living Tissue allows therapeutic effects to be achieved that are not possible with the known radiation generating devices could be obtained.

It appears that the invention in the treatment of diseases of live (vegetable or animal) cells can be attributed to certain phenomena, which are detailed below should be explained, but this explanation is not intended to limit the invention.

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Depending on its electromagnetic physicochemical structure, which consists of core and protoplasm cell structure is equipped with an electrical conductivity-ion exchange conditions is in direct proportion with the ones caused by the metabolic phenomena He _T. The presence of an accumulation of electricity at potentials which vary according to the different cell densities of these tissues is observed in the tissues, ^x

The work of Renshaw, Forbes, Morison, Amassian, De Vito, Buser, Albe-Fessard, ropes, Adrian and others have with the help of microelectrodes been able to demonstrate the existence of an electric g elemental activity in slow oscillations inside the cells, and the rhythm control or Propulsion can be seen as being realized by the oscillating electromagnetic system that is formed by the cell nucleus. This core is in fact essentially composed of tubular threads made of the chitin-related insulating material, which inside contain a salty liquid which conducts electricity, and it can be assumed that these threads, which are entangled in themselves, form small oscillating circles.

The last work of Warson in America as well as those Polonsky, Donzou and Sadron was brought by Professor Francis Perrin "on 05.16.1960 in the Academie des Sciences to lecture by French scholars, of which j is a work of Men (Recueil des comptes-rendus hebdomadaires , Vol. 250, no. 20, pages 34H-3416), have emphasized the fact that the examined samples of solid DNA show properties analogous to those known in ferroelectric bodies. This makes the hypothesis very likely that that there is a potential difference between the nucleus and the periphery of the cells. "Some older theories go even further and compare the cell with an electronic receiver and transmitter device which, in its normal state, functions in frequency coherence with the surrounding media. The system formed by the cell nucleus, that with muffled waves

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• ohwlagt, would · iioB damn according to ita Gesetien rtr hold, dinin dit semiconductor bodies are subject to.

The applicant is iu dtr conviction fakoaeta, dal dar Xellkern generally has a normal electrophyeical state of equilibrium and one positive charge folarization analog · BraohaiSfuiftB can last from a negative overload «

Di · Irfindung traösehen baaondara daa tob diaaar Oa * reversal of their electrical potentials affected organs, In particular, in particular cases of pathological negative overloads, tone cancerous nuclei, their initial risk to find again.

The wavelength of the ca-skin radiation is chosen roreugaweiee Bwiechen 3 oa and 80 whether * The Anaelder has featgeateilt that penetration and in particular that Healing effects are significantly ererbeesert if aan this electromagnetic radiation ia om wave range Frequents are determined depending on the organ or tissue to be penetrated or treated For example, a wavelength of 14 ca is suitable for the liver and a wavelength of 19 »5 oa for the mils.

The radiation from the electrically charged particles is accelerated as a precaution in a particle accelerator in order to reinforce the durometer penetration force,

It is often advantageous to modulate or rhythmise the radiation of the particles by means of variable magnetic and / or alactriaohar fields in such a way that the penetrating force is intensified.Especially in aedisinic applications, this rhythm is preferably based on the natural period of the penetrating tissue or the neighboring tissue , beiapieleweiae of muscles, tuned. These natural periods are known in the liedIbin and are used in particular in diathermy. They are generally in the range of wavelengths from 1 to 50 a, in particular from 1 to 18 ι.

β Oi β 43/0430 SAD ORIGINAL

The invention further relates to a device sur implementation of the described procedure! after Finding.

Further features and parts of the goal of the invention result eich from the patent claims la connection with the following description

Ib of the reference are several execution examples the device according to the invention shown. The method according to the invention is based on this drawing explained.

Xa der Äichnung seigern ™

Fig, 1 soheaatisoh one device on suction and SaleeioB an electromagnetic field of charge,

Pig. 2 are the end of the cathode, la Fig. 1 tob rsoats seen

Fig * 3 is a similar view neoh dsr line IZI-ZZX dsr Fig. T, -

4 shows the electrical supply Current to the respective components,

Figure 5 ia a · · Figure 1 ähnlionen considers other sins g Aueführungeform dsr device naohdsr invention,

Fig. 6 shows a similar view of the line VI-VI dsr Pig. 5,

Fig. 7 schematically shows a device sum pulsing the electric current,

8 shows the circuit diagram of an amplifier which enables the device according to FIG Hersene su operate,

Fig. 9 daa circuit diagram of an oscillator, dsr enables the electrical current after a between 1 and 18 m to modulate lying wavelength

909843 / OUO ^{BAD 0RIGINAL}

The in fig. Represented 1 × device, a device 1, daa electrically charged particles 2 ineinen Hohlraun or a line 3 is emitted, as well as a particle accelerator umfaflt similar to a cyclotron 4, the * the Teilch - accelerated 2 and "chiokt in a conduit forming Hohlraun 5, in into which another cavity 6 opens, which forms a wave guide for electromagnetic radiation with a cm wavelength, dis duroh sin magnetron? is emitted. The line 8 formed by the union of the line 5 and the wave guide 6 opens into a) tube 9 in which the resulting radiation is sucked in. Bas inside the cavity formed by the entirety of the elements 1, 3 _f 5, 6, 8 and 9 contains argon enter a pressure tone of 2 mm of mercury column

The particle generator 1 consists of a device * ta » lioh a sheet metal gun, an anode 10 and a

Has cathode 11.

Sis cathode 11 is preferably made as "molybdenum and has duroh SWSL aligned epeiohenartige webs 11b which is connected to a hub-shaped central portion 11e in Fig. 1 and 2 shown particular form * Hn Anlenkkrans 11a has a bore 11d for the axis XI ¹ · How ^ ig. 1 selgt, the jib crane 11a consists of swsi parts which, for example, are connected to one another by bolts . The articulated crane 11a is provided with an inner annular groove 11e through which several bores 11f pass, which are distributed parallel and uniformly to the axis ZX *. Inside the annular groove 11e of the filament 12 is arranged, which is connected to let the power supply wires 12a.

The best results are achieved with a cathode 11 made of molybdenum. A cathode made of tungsten also gives satisfactory, but less than good results. It has been found that molybdenum, and to a lesser extent tungsten, are metals whose valency approximates the average valency of the chemical molecules which the

Ö098A3 / 0430 _BAD original

leiMadea (camouflages especially the aeneous tissue balls. Ma · koaat · Tersuohen, based on this finding Al · occurrence aAea surrenders can be explained scientifically, but Al · invention is not to be limited by any scientific explanation. With regard to the la Asr device available under low pressure It is to be noted that the best results are old Argoa will be held. With other oases that too Among the rare oases, the results were satisfactory, but the results were not as good.

Sund, among other things, the Sohr, which forms the Kalseionskaaaer, are arranged I am at the level of the cathode Blektroaagnet 13, which is a magnetic · Feldgrofler strength erseugt, old "of a winding 13a as well as windings 14 and 15t ale sua condensation of the bundle of rays 2 determined • lad. Sund ua Ale lines 3, 5 and 8 are also further windings 14, 15 and 16 eur compression and Among other bays of the beam of rays 2 arranged.

The two semicircular housings 4a of the particle accelerator 4 are in the usual way between the Poles of the jacket · arranged, the τοη the windings 4b ubA 4o UBBChloesen 1st.

The magnetron 7 1st τοη known type and aufi be flfclg, ia Aen Hohlraua 3 a ca wave radiation ait elaer adjustable wavelength τοη 30 to 80 ca tu eaittleren.

The bore 9 generally has a lower cathode 17 similar to the cathode and a filament 17a. The cathode 17 is carried roughly by a hollow suture 18, which, as a matter of consent, is generally exposed to the bottom of the eye with bores 18a. The attachment 18 is ait elaea Sohr 18b la connection, which ends in the axis of a rotatable component 19, which has two cranes made of graphite plates 19a, which are inclined at 45 ° on the vertical, inter alia. The axle 19b of the rotatable component 19 is rotatably mounted in the elaea holder 20, the inside of the

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Tube 9 is attached. The axis 19b carries at the upper end magnetic flyweights 19c, which set the axis in rotation while they are bit magnetic flyweights 21a cooperate, which are firmly connected to the shaft 21b of a motor 21. The lower end of the rotatable component is formed by a part 19d consisting of molybdenum or tungsten in the form of a pyramid, the apex of which Opposite opening of the tube 18b. The lower part of the holder 20 forms the anode 22 of the tube 9.

The hollow extension 18 and the tube 18b can be made from one ^ Borosilicate glass with a low expansion coefficient exist, which is commercially available under the name "Pyrex". But they can also consist of quartz · The Tube 9 itself can be made from "Pyrex ^ glass or from another usually used to manufacture τοη electron tubes consist of glass. The bottom 9a of the tube through which however, the resulting radiation passes is advantageously made of quartz.

The line 8 opens into the tube 9 alt several lines 8a and 8b, which in vertical planes at a certain angle, which is advantageously approximately 22.5 °, are directed against the plates 19a. In the tolumen area of these plates 19a, which form the solid surfaces, * the interaction occurs swisohen the om-wave radiation and the gas discharge plan which is generated by the beam 2 · Around the cathode 17 is a Electromagnet 23 arranged, the electromagnet 13 of the Tube 1 corresponds. Windings 24 are also arranged around the tube 9. The tube 9 is also at the in The point indicated in the drawing with three electrodes 25, 25a and 25b, the τοη windings 26, 26a and 26b These electrodes are used to get into the eye 9 to introduce electromagnetic radiation in the m-wave area in order to irradiate the tolumen with the (Jas discharge plasma. This results in its electromagnetic radiation Radiation whose wavelength is between the wavelengths of the

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m-wave range and the wavelengths of visible radiation and which emerges from the tube 9 at the base. This resulting radiation is superimposed on the high strength magnetic field created by the electromagnet which improves the therapeutic effects. The feed lines 17b, 17c are also shown in the drawing for the cathode and its filament as well as the supply line 22a for the anode.

The printiρ of the supply of the electric current is shown eohematisoh in FIG. The section 27 supplied with songs voltage alternating a first branch ä line, in which a rectifier 28 is located (eg, a diode), whose rectified current in an adjustable rhythm 30-120 Sohwingungen / min, voriugsweise the rhythm of hersens of the subject, is modulated by a resistor 29, the control device of which is described below in connection with FIGS. The current modulated in this way is sent into the electromagnets 13 and 23 so that they generate a unidirectional modulated magnetic field of 10,000 to 20,000 Gauss at the location of the cathodes 11 and 17. These magnetic fields modulate, on the one hand, the emission of the partial beam 2 and, on the other hand, the field or the resulting radiation that emerges at the base of the I tube 9, preferably in the rhythm of the living being to whom the radiation is to be applied *

The section 27 also feeds a variometer 30, which the current of this section in a controllable rhythm modulated from 30 to 120 oscillations. The one on this Wisely modulated current feeds the remainder of the device, viz

a) the magnetron 7 »

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b) a converter group 31, the excitation of which is modulated to a controllable frequency of 300 to 900 Hz. Man In this way, receives a double modulated direct current (namely initially at a rate of 30 to 120 Vibrations / min and then to the frequency of 300-900 Hz), which feeds the windings 15, 16 and 26,

c) another group of converters 32, which generates low-voltage direct current that is generated by the variometer 30 in the The rhythm is modulated from 30 to 120 oscillations / min. This current feeds the motor 21 as well as the motors, which drive the variometer 30 and the control device of the resistor 29.

The current generated by the converter 32 also feeds a voltage-increasing device 33, which consists of an interrupter with a subsequent transformer and rectifier and which generates a direct current, the voltage of which changes in the rhythm imposed by the variometer from 30 to 120 vibrations / min changed. The maximum value of the The voltage generated by the device 33 is, for example, 300,000 V. However, this value can vary depending on change more or less the service that is to be brought into effect

The current generated by the voltage-increasing device 33 feeds the windings 4b of the particle accelerator and the windings 24 of the tube 9 as well as one Rheostat 34, which allows the voltage on a between 5000 and 70,000 V. rules. This voltage is applied to an oscillating circuit 35 and gives it oscillations with a frequency adjustable between the wavelengths of 1 to 18 m, the frequency at the output terminals 35a, The current available 35b of the resonant circuit is therefore a high-voltage current that rises to 30 to 120 for the first time Vibrations / min (by the variometer 30) and modulated a second time to a wavelength of 1 to 18m.

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This current spits out foci 40 and 14 bit electrodes 25a and 25b are old connected to the rails 35a and 35b, while the electrode 25Mt is connected to a central point 35c. The electrodes 25 »25a, 25b generate eo in the Tube 9 an electromagnetic radiation, whose wavelength «Wiecheη 1 ■ and 18 ■ is chosen, and this radiation itself is pulsating in a rhythm of between 30 and 120 vibrations / oin.

The cathodes 11 and 17 ″ the housing parts 4a of the Particle accelerator 4 and the anodes 10 and 22, which in the scheme of Flg. 4 are not specified, are marked with the (( Output of the voltage-increasing gate direction 33 connected, while the heating current for the filaments 11e and 17a is supplied through the resistor 29

IM using the device becomes the controller of the resistor 29 and the variometer set to the desired rhythm, which in medical applications advantageous is the rhythm of the heart of the object. This rhythm becomes that way of the whole device imposed. The cathode 11 emits radiation from positively charged particles 2 to the left, which radiation is concentrated by the electromagnet 13 and through the windings 14, 15, 16 and accelerated by the particle accelerator 4. | This radiation of the particles is in the line 8 the electromagnetic radiation of the magnetron 7 superimposed, which is regulated to the wavelength which experience has shown is most favorable for the cells to be penetrated, such as to the wavelength of 14 cm for the liver and to the wavelength of 19 »5 cm for the spleen. The resulting radiation is directed into the tube 9, as shown and the resulting formed in the stir Radiation falls through the bottom of the tube onto the area to be penetrated.

It should be noted that the unidirectional magnetic field of the windings 15, 16 and 26 is adjusted to a frequency of between 300 and 900 Hk by means of the converter group 31.

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sequence is modulated. The effect of this modulation is to concentrate the particles, i.e. them from the To detach the walls of the lines, and also enables a significant weight saving of the iron core of the windings

The unidirectional magnetic fields of the windings 4-e of the particle accelerator 4 and the windings 14 are modulated by the oscillating electric circuit 35, the Frequency of the wavelength of the electrodes 25, 25a and 2bb emitted electromagnetic radiation! is equivalent to. This wavelength is chosen between 1 m and 18 m. In medical applications in particular, the wavelength becomes * selected which is best suited for the organ to be treated or the neighboring files, such as the muscles. As mentioned earlier, the experience gained in diathermy allows for the most suitable wavelength to determine.

5 and 6 illustrate another embodiment of the device according to the invention, the Parts which have the same function are denoted by the same reference numerals as in Figs. 1 and 3, the but are marked with a '.

In FIG. 5, the arrangement of the lines relative to the tubes 1 'and 9 * ι to the magnetron 7' and to the particle accelerator 4 * is different from that according to FIG. 1 and has been successfully used by the applicant. The wave guide 6 'of the magnetron 7' opens into the end of the tube 1 ·, and the line 3 ', which conveys the resulting radiation, splits into two lines, namely into the line 36, which feeds this radiation directly to the tube 9 ″ , and into the line 37, which conveys the radiation to the particle accelerator 4 *, which holds back the electromagnetic radiation and accelerates the radiation of the particles, which is fed ^{through the line 38 to the tube 9 1.}

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This arrangement can bit of the particles emitting tube and used with an accelerating and directing Rohr · which the tubes 1 and 9 of the previous figures similar eind _f The tubes 1 'and 9' of Figures 5 and 6, however, aind respect to their cathodes, and Anodes designed differently *

The tube 1 'has a first electrode 11 ·, which the Cathode 11 is similar to the tube, and a second identical electrode 39, which is provided with a "filament 39 '" The tube 9 * (? I§, 6) has the lower part a first Electrode 17 'has its "hot filament 17a" and a "wide, identical electrode 40 bits of its hot filament 40a.

In normal operation, i.e. generating radiation which is identical to that which in relation to fig. 1 to 1, the electrode 11 * serves as a cathode, and the electrode 39 is subjected to a positive potential and plays the role of the anode 10 of Fig. 1, wherein the hot thread 39 »is not handled. The electrode 40 and their heat threads 4.0a are switched off from the circuit. The cathode 17 * and the anode 22 »are fed as in FIG.

Ub received a particularly penetrating radiation, the polarities are reversed ι The electrode 11 'becomes the I. The anode and its filament 11e * is switched off from the circuit, while the electrode 39 is fed as a cathode and its filament 39a is heated. The electrode 17 * (their Filament 17a * is disconnected from the circuit) and electrode 22 'becomes anodes, while electrode 40 becomes Cathode fed and its filament 40a is heated. For example, a potential difference of 250,000 Y between 40 and 17 'and from 50,000 V between 40 and 22' produce. Under these conditions, the cathode emits a radiation of electrons to the left, which is concentrated, modulated and accelerated in the particle accelerator 4 'by the various windings and their polarities naturally set in the appropriate sense

• 09tO / 0il0 · "« «« «■

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will have to. The letron radiation is transmitted with the the magnetron 7 * emitted centimeter radiation combined, and it results in the tube 9 '"ine very hard and on the selected frequencies modulated emission of X-rays that correspond to the centimeter radiation of the desired frequency are combined

The device of FIGS. 5 and 6 therefore enables either this very hard X-radiation or as desired to obtain the radiation described with reference to the previous figures

The following description of FIGS. 7 to 9 refers to some peculiarities of the devices that are used to modulate the electrical Currents · to achieve.

Fig. 7 shows the control device in a cheaper way de · Wideretand ·· 29 and the variometer · 30. The variable · resistor 29 is provided with a graphite spiral 29a, which is immersed in a conductive liquid 29b is, in which an electrode 29c is partially immersed, dl also consists of (Jraphit and dl · by a handlebar 41a is moved back and forth, which is articulated to a flywheel 41 »This is set in rotation via a worm gear transmission 41b by means of a shaft 42, which either via a double clutch 42a, 42b can be driven by a motor 43 or by the shaft 30a of the variometer · Da · variometer 30 becomes Driven by a motor 44 via a worm gear transmission 44a

When the flywheel 41 is driven by the motor 43 with the corresponding rotary tool, the Resistor 29 feeds the electromagnet · 13 and (Fig. 1 and 4) in the selected rhythm, which is between 30 and 120 vibrations / min and which can be regulated by means of a tachometer, which is shown schematically at 45 is indicated. In this case, the motor 44 of the variometer 30 can be stopped and the remaining part of the device is therefore not rhythmized. However, if that

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Flywheel 41 is engaged at 42b and disengaged at 42a, the motor 44 actuates the variometer 30 and the Resistance 29 in the chosen rhythm

The speed of the motors 43 or 44 can be controlled to the appropriate speed, which corresponds essentially to the heart rhythm of the object, by adding to the excitation these motors by means of a manually adjustable rheostat is acted upon. However, if you prefer, the speed of the motors 43 or 44 directly by the Uerzrhythm To regulate the object, a device as shown schematically in FIG. 8 can be used. At i 46 a contact microphone is branched off, which is arranged on the heart of the object and which generates vibrations. These are amplified in the circuit shown and made to act on an electromagnet 47, the movable core of which actuates a rheostat, which regulates the excitation current of motors 43 or 44 «

9 shows schematically the principle of the oscillating current circuit 35. The rectified voltage, which can be regulated between 5,000 and 70,000 V by means of the rheostat 34 (FIG. 4), is brought into effect between the terminals 48 and 48a. The terminal 35e (which on the other hand is connected to the electrode 25, Figs. 2 and 4) is connected to the neutral i point on the high-voltage side of the transformer, which forms an element of the step-up device 33 (Fig. 4). The terminals 49 and 49 a receive the heating current that is generated by the resistor 29. The variable capacitors 50 and 50a allow the current available at the output terminals 25a and 25b of the oscillator shown to the desired W _e llenlänge to regulate, which is between 1 to 18 m.

The described embodiments are successful have been tried, "but of course they are only given as examples and various modifications can be made without departing from the scope of the invention."

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In particular, the device 1 or 1 'could be replaced by any other electrically charged particle emitting device can be replaced.

Patent attorney « Dipl.-Ing. Horst Rose Dipl.-Ing. Peter Kosei

COPY Ö09843 / QA3Ö

Claims (20)

DIPL-ING. HORST ROSE DIPL-ING. PETER KOSEL PATENT LAWYERS 1 / C / O C Π 3353 Bad Gandersheim, September 4, 1968 ακ «******» * »: Hohenhöf en 5 'T phone! (05382) 28 « Telogram address: Siedpa'ent Bad Gandersheim P 14 64 350.6
Antoine Priore Claims 1 · Method of generating an electromagnetic Radiation for therapeutic purposes, characterized in that a beam (2) of electrically charged Particles and, separately therefrom, a directed electromagnetic radiation (7) in the cm wave range is generated These particle and wave radiation are superimposed on each other, the radiation mixture on solid surfaces (19a) is directed, a gas discharge plasma in the volume region (9) of these solid body surfaces and an electromagnetic radiation in the m-wave range into the volume of the gas discharge plasma is irradiated. 2. The method according to claim 1, characterized in that that a unidirectional magnetic field of great strength to the volume of the gas discharge plasma Effect is brought about (23). 3. The method according to claim 2, characterized in that a further unidirectional magnetic field the same strength on the area (1), in which the particle radiation is generated, is brought into effect. 4. The method according to claim 2 or 3, characterized in that the one or more unidirectional magnetic fields (13 and / or 23) pulsates at a rhythm of 30 to 120 oscillations / min, preferably in the rhythm of the heart of the person to be treated ( 29) become · ■ .. · i torlaflon '■ *''"■; _t ir« mj **. Θ098Λ3 / ΟΑ30 2352/1 Eq. Bonkkonlo: BraunschweieiKfce Slaol.bank, Bad Ga "drh [m, Ko-Nr. M.ll «.» 70 · PchAedckcnto: Hannover «715 H64350 5. The method according to claim 2, 3 or 4, characterized in that the generation of the particle radiation (1) and the cm wave radiation (7) in the same rhythm as the unidirectional magnetic fields (13 and / or 23) are modulated « 6. The method according to claim 5, characterized in that that the particle radiation is accelerated, compressed and directed by electric fields (4) and magnetic Fields (H, 15, 16, 4b, 4c) that are in the same rhythm as the unidirectional magnetic fields of great strength (13 and / or 23) can be modulated. P 7. The method according to claims 1 to 6, characterized in that that the wavelength of the cm wave radiation is about 3 to 80 cm. 8. The method according to claim 7, characterized in that the wavelength of the cm radiation is set to a value which is best suited for the tissue to be irradiated, e.g. 14 cm for the liver and 19.5 cm for the spleen. 9. The method according to claims 1 to 8, characterized in that the wavelength of the m-welen radiation (25, 25a, 25b) is selected between approximately 1 m and approximately 50 m, preferably between 1 m and 18 m 10. The method according to claim 9, characterized in that that this wavelength is chosen in the same size as in diathermy, according to the or to be irradiated the adjacent tissue. 11. The method according to claims 1 to 10, characterized in that the particle radiation by electrical Fields is accelerated (4) of the kind used in particle accelerators. 12, method according to claims 1 to 11, characterized in that the compression and direction of the Particle radiation magnetic fields (14, 15, 16, 4b, 4c) are applied * ÖQ9843 / 043Ö 13. The method according to claim 12, characterized in that that at least certain of the compressing and directing magnetic fields (15, 16) with a frequency between 300 and 900 Hz can be modulated. 14. The method according to claim 12 or 13, characterized in that that certain of the compressing and directing magnetic fields (4c, 14) with a frequency within the m-wave range (25, 25a, 25b) are modulated. 15. The device for carrying out the method according to claim 1, characterized in that it has an electron gun-like device (1) for generating the beam from electrically charged particles, which in% is a cavity (3.5 or 3'j 36, 37, 38 ) and has an anode (10) located at one end of the cavity and a hollow cathode (11) downstream from the anode, with an electromagnet (13 »13a) surrounding the cathode for generating a high strength electromagnetic field in order to ensure an emission of the beam of particles in the cavity downstream of the cathode, and that the cavity also serves as a wave guide for the cm-wave radiation emitted ^{by a magnetron or a similar device (17, 7 1).} 16 · The apparatus of claim 15, characterized ä, that the cathode has an outer rim (11a) which is connected with a hub-shaped middle part (11c) via at least two spoke-like connecting webs (11b), that the outer rim with a Hing space (11e) for Receiving a heating coil (12) and that this annular space is connected to a number of holes (Hf) which penetrate the outer rim transversely. 17 · Device according to claim 15 or 16, characterized in that the metal forming the cathode is tungsten or especially molybdenum. 909843 / 0A3Ö U6A350 18. Device according to claims 15 to 17, characterized characterized in that the cavity contains a noble gas, in particular argon, under a vacuum of the order of 2 mm Contains mercury. 19. Device according to claims 15 to 18, characterized characterized in that the volume containing the solid body surfaces (19a) is formed by a tube (9), in which the cavity (8a, 8bj 36, 38) opens and which contains: A) in the area in which the electromagnetic radiation that can be used for therapeutic treatment is to emerge, a hollow cathode (17), the ^ is surrounded by an electromagnet, similar to the Cathode (11) and the electromagnet (13, 13a) the emission device for the particle beam, B) an anode (22) in the area of the tube opposite to A), G) in the intermediate area of the tube: a) electrodes (25,25a, 25b) for irradiating the electromagnetic radiation in the m-wave range and b) a number of plates (19a) which form the solid body surfaces and on the periphery k of a rotatingly driven support body (19) are arranged, wherein the plates (19a) are further opposite the inlet ports (8c, 8b; 36,38) arranged for the confluence of the cavity in the tube (9) and to the axis of the Tube are inclined. 20. Apparatus according to claim 19, characterized in that that the electrodes (2J, 25a, 25b) of coils (26, 26a, 26b), which generate a magnetic field modulated at a frequency of 300 to 900 Hz, wherein the cavity into which the particle beam emits is, preferably surrounded by coils (15, 16), the magnetic fields modulated with the same frequency produce· 909843/0430