Patent Publication Number: US-2012024587-A1

Title: Radiation amount reducing device

Description:
TECHNICAL FIELD 
     The present invention relates to a radiation amount reducing device. 
     BACKGROUND ART 
     In recent years, higher density and higher integration of a CPU, an LSI, a clock IC, a peripheral semiconductor and the like, which are used inside a device, and higher density of a print wiring are advancing with advancement in electronic devices including a television, a computer, a camera, and a portable telephone. The component of the frequency handled in such electronic components and the like is also becoming higher frequency. 
     Accompanied therewith, problems such as influence on human body, false operation, functional failure, characteristics degradation and the like due to radiation noise (electromagnetic wave) generated from an electronic component and conduction noise (electromagnetic wave) generated from a line pattern formed on a print substrate arise. EMC (Electro-Magnetic Compatibility), EMI (Electro-Magnetic Interference), EMS (Electro-Magnetic Susceptibility) measures are thus further being desired. 
     
       
         
           
               
            
               
                   
               
               
                 Citation List 
               
            
           
           
               
               
               
            
               
                   
                 Patent Literature 
                   
               
               
                   
                   
               
               
                   
                 Patent Literature 1:  
                 JP H7-212079A 
               
               
                   
                 Patent Literature 2:  
                 JP H11-3549669A 
               
               
                   
                 Patent Literature 3: 
                 JP H9-312489A 
               
               
                   
                 Patent Literature 4: 
                 JP 2007-95971A 
               
               
                   
                   
               
            
           
         
       
     
     SUMMARY OF INVENTION 
     Technical Problem 
     Generally, a mechanism for suppressing unnecessary electric wave and unnecessary noise radiated from an electronic device with a shield case is the main stream of a means for reducing unnecessary electric wave in the electronic device. 
     This is a method of using a metal plate having conductivity as a shield plate and sealing the radiation noise generated from a substrate by reflecting (see above Patent Literature 1). Although this method is effective in the leakage of radiation noise, the electromagnetic wave interference of the scattered radiation noises may be promoted since the radiation noise from various types of components such as IC and patterns are reflected by the shield case. Furthermore, the shield case structure becomes complicating to reduce the radiation of the electromagnetic wave such as radiation noise, which consequently leads to increase in manufacturing cost (see above Patent Literature 2). 
     When such shield case and the like are used, screw-fitting, plate spring, gasket, and the like are used to join a cover and the shield case, which configure a housing. 
     When joining by screw-fitting, a troublesome screw-fitting task is required, and the installing locations of the screw between the cover and the shield case need to be increased to enhance the shield effect. The screw-fitting task thus increases, and the assembly task efficiency significantly lowers. 
     When the plate spring is used, the task of forming the plate spring itself takes considerable time, which greatly increases the attachment man-hour, and increases the cost. 
     In a case of a gasket added with conductive metal powder or an article including an insulative soft magnetic body, the gasket and the sheet themselves are expensive, and the usage location is greatly limited due to restriction in the attachment structure. 
     Further, Patent Literature 3 above discloses a complex magnetic body that performs measures with the radiation noise from a cable and the like as one of the EMI measures. In this method, however, the conduction noise generated from the line pattern formed on the print substrate is difficult to suppress. The conductive noise that is not suppressed thus generates by power supply voltage fluctuation and the like caused by switching operation, thereby affecting the electronic device, the circuit, and the like. 
     Further, Patent Literature 4 above discloses an electromagnetic wave shielding sheet for covering a radiation unit, which radiates the electromagnetic wave. However, this sheet not only increases the manufacturing steps due to its complicating configuration but is also expensive, and thus may increase the manufacturing cost of the product. 
     Therefore, the radiation preventing method has advantages and disadvantages, and development of a ready and inexpensive method capable of appropriately suppressing the radiation noise and the conduction noise is desired. However, since the electronic circuit, in which reduction of noise is increasingly desired due to higher frequency and the like, is complicating, noises of various positions and frequencies are generated. Such noises are not uniformed, where measures by the shield case structure and the like are known to be complicating and noise reduction by the shield case is also limited. Therefore, a ready and inexpensive radiation preventing means capable of effectively reducing radiation is desired. 
     In order to solve the problem above, the present invention aims to provide a novel and improved radiation amount reducing device capable of more effectively suppressing noise (electromagnetic wave) radiated from an electromagnetic wave generation source such as an electronic circuit readily and inexpensively. 
     Solution to Problem 
     According to an aspect of the present invention in order to achieve the above-mentioned issue, there is provided a radiation amount reducing device including a metal plate for entirely covering at least one surface of an electromagnetic wave generation source for radiating an electromagnetic wave, a cover region, set within a plane of the metal plate, for covering the entire one surface, and a plurality of slits formed to a band-shape in at least the cover region, and spaced apart from each other, wherein each of the plurality of slits includes, a drawing slit formed extending towards a central part of the cover region from a ferromagnetic field position where a magnetic field generated in between the electromagnetic wave generation source by the electromagnetic wave is stronger than other positions at an outer periphery of the cover region so as to guide a circular current flowing in a peripheral direction surrounding the central part of the cover region in the central part direction of the cover region by the electromagnetic wave, and a coupling slit formed extending so as to line in parallel to another slit on one side from an end in the central part direction of the cover region in the drawing slit so as to guide the circular current guided by the drawing slit to in between the other slit adjacent on one side in the peripheral direction of the cover region. 
     2 N  slits may be formed on the metal plate, N being a positive integer. 
     The plurality of slits may be arranged point symmetrically from each other with the central part of the cover region as a reference. 
     Moreover, the cover region may be an entire region of the metal plate, the metal plate may be formed with a distance from the central part to the outer periphery unequal, and the ferromagnetic field position may be an edge position at a middle between edge positions adjacent at the outer periphery of the metal plate where the center distance is long compared to other sites. 
     Moreover, the metal plate may be formed to a polygon having 2 M  corners at an outer periphery, M being a positive integer of greater than or equal to two, and the ferromagnetic field position may be an edge position at a middle between the corners. 
     Moreover, the metal plate may be a regular polygon. 
     Moreover, the ferromagnetic field position may be a position at the outer periphery of the cover region corresponding to an edge position at a middle between the corners in one surface of the electromagnetic wave generation source. 
     Moreover, the cover region may be an entire region of the metal plate, and the metal plate may be formed to a circular shape in which a center distance from the central part to the outer periphery equal. 
     Advantageous Effects of Invention 
     According to the present invention described above, the noise (electromagnetic wave) radiated from an electromagnetic wave generation source such as an electronic circuit can be more effectively suppressed readily and inexpensively. 
    
    
     
       BRIEF DESCRIPTION OF DRAWINGS 
         FIG. 1A  is an explanatory view describing a configuration of a radiation amount reducing device according to a first embodiment of the present invention; 
         FIG. 1B  is an explanatory view describing the configuration of the radiation amount reducing device according to the embodiment; 
         FIG. 2A  is an explanatory view describing an operation example of the radiation amount reducing device according to the embodiment; 
         FIG. 2B  is an explanatory view describing an operation example of the radiation amount reducing device according to the embodiment; 
         FIG. 3A  is an explanatory view describing an operation example of the radiation amount reducing device according to the embodiment; 
         FIG. 3B  is an explanatory view describing an operation example of the radiation amount reducing device according to the embodiment; 
         FIG. 4  is an explanatory view describing an example of the radiation amount reducing device according to the embodiment; 
         FIG. 5A  is an explanatory view describing an example of the radiation amount reducing device according to the embodiment; 
         FIG. 5B  is an explanatory view describing an example of the radiation amount reducing device according to the embodiment; 
         FIG. 5C  is an explanatory view describing an example of the radiation amount reducing device according to the embodiment; 
         FIG. 6  is an explanatory view describing an example of the radiation amount reducing device according to the embodiment; 
         FIG. 7A  is an explanatory view describing an implementation example of the radiation amount reducing device according to the embodiment; 
         FIG. 7B  is an explanatory view describing an implementation example of the radiation amount reducing device according to the embodiment; 
         FIG. 7C  is an explanatory view describing an implementation example of the radiation amount reducing device according to the embodiment; 
         FIG. 7D  is an explanatory view describing an implementation example of the radiation amount reducing device according to the embodiment; 
         FIG. 7E  is an explanatory view describing an implementation example of the radiation amount reducing device according to the embodiment; 
         FIG. 7F  is an explanatory view describing an implementation example of the radiation amount reducing device according to the embodiment; 
         FIG. 8A  is an explanatory view describing a variant of the radiation amount reducing device according to the embodiment; 
         FIG. 8B  is an explanatory view describing a variant of the radiation amount reducing device according to the embodiment; 
         FIG. 8C  is an explanatory view describing a variant of the radiation amount reducing device according to the embodiment; 
         FIG. 8D  is an explanatory view describing a variant of the radiation amount reducing device according to the embodiment; 
         FIG. 8E  is an explanatory view describing a variant of the radiation amount reducing device according to the embodiment; 
         FIG. 8F  is an explanatory view describing a variant of the radiation amount reducing device according to the embodiment; 
         FIG. 9A  is an explanatory view describing another variant of the radiation amount reducing device according to the embodiment; 
         FIG. 9B  is an explanatory view describing another variant of the radiation amount reducing device according to the embodiment; and 
         FIG. 10  is an explanatory view describing a radiation amount reducing device according to a related art. 
     
    
    
     REFERENCE SIGNS LIST 
     
         
           10 ,  90  metal plate 
           11 ,  12 ,  13 ,  14  metal plate pieces 
           15 ,  16 ,  17 ,  18  metal plate pieces 
           21 ,  23  shield case 
           22  substrate 
           31  adhesive 
           100 ,  101 ,  102 ,  103 ,  104 ,  105  radiation amount reducing device 
           106 ,  107 ,  108 ,  109 ,  110 ,  111  radiation amount reducing device 
           900  radiation amount reducing device according to the related art 
         A, B region 
         Ar cover region 
         BA, BC, BB, BD ferromagnetic field position 
         D reception probe 
         H magnetic field 
         I, I 1 , I 2 , I 3 , I 4  circular current 
         R noise generation source 
         N noise 
         O central part 
         PA, PB, PC, PD parallel position 
         SA, SB, SC, SD slits 
         SE, SF, SG, SH slits 
         S 1 A, S 1 B, S 1 C, S 1 D drawing slits 
         S 1 E, S 1 F, S 1 G, S 1 H drawing slits 
         S 2 A, S 2 B, S 2 C, S 2 D coupling slits 
         S 2 E, S 2 F, S 2 G, S 2 H coupling slits 
         S 3 A, S 3 B, S 3 C, S 3 D auxiliary slits 
         S 4 A, S 4 B, S 4 C, S 4 D auxiliary slits 
         S 11 , S 12 , S 13 , S 14  auxiliary coupling slits 
         T 1  supporting plate 
         T 2  vinyl film 
         VA, VB, VC, VD, VO intense electric field position 
         X measuring target 
       
    
     DESCRIPTION OF EMBODIMENTS 
     Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the appended drawings. Note that, in this specification and the drawings, elements that have substantially the same function and structure are denoted with the same reference signs, and repeated explanation is omitted. 
     The radiation amount reducing device according to each embodiment of the present invention can be used for various electromagnetic wave generating sources. A wide variety of electromagnetic wave generating sources from various electronic elements including CPU (Central Processing Unit), LSI (Large Scale Integration), clock IC (Integrated Circuit), peripheral semiconductor, print substrate, wiring, coil, resistor, and capacitor, to an electronic device formed by combining the above may be used. The application of the radiation amount reducing device is not limited to the example of the electromagnetic wave generation source, and may be applied to various regions that emit electromagnetic wave. In this case, the radiation amount reducing device is arranged in close contact with the electromagnetic wave generation source on the direction side not desiring to propagate the electromagnetic wave radiated by the electromagnetic wave generation source, or is arranged in the vicinity thereof. The radiation amount reducing device may be arranged distant from the electromagnetic wave generation source, but is desirably arranged on the electromagnetic wave generation source side in view of shielding or attenuation efficiency of the electromagnetic wave, spatial efficiency of the entire device, and the like. The description will be made in the following order to facilitate the understanding on the radiation amount reducing device. 
     1. Radiation amount reducing device according to related art
 
2. Radiation amount reducing device according to first embodiment
 
     2-1. Configuration of radiation amount reducing device 
     2-2. Operation example of radiation amount reducing device 
     2-3. Example of radiation amount reducing device 
     2-4. Implementation example of radiation amount reducing device 
     2-5. Variant of radiation amount reducing device 
     2-6. Example of effects of radiation amount reducing device 
     1. Radiation Amount Reducing Device According to Related Art 
     First, a radiation amount reducing device according to the related art will be described with reference to  FIG. 10 .  FIG. 10  is an explanatory view describing the radiation amount reducing device according to the related art. 
     In  FIG. 10 , an example of a case in which a metal plate  90  is used as a shielding shield of the electromagnetic wave, that is, a radiation amount reducing device  900  according to the related art is shown. The metal plate  90  shown in  FIG. 10  has conductivity and is arranged to cover an electromagnetic wave generation source (hereinafter also referred to as “noise generation source R”). Although not illustrated, the noise generation source R of the same extent as or one size smaller than the outer shape (outer shape in x-y plane) at the formed surface of the metal plate  90  is arranged on the back surface (far side in plane of drawing) of the metal plate  90  shown in  FIG. 10 . 
     The electromagnetic wave (noise) generated from the noise generation source R is reflected by the radiation amount reducing device  900  according to the related art. However, the energy thereof does not attenuate, and is radiated from the outer periphery or the surface of the radiation amount reducing device  900  according to the related art or from between the noise generation source R. Such phenomenon is referred to herein as “secondary radiation”, and the secondary radiated electromagnetic wave is referred to herein as “noise N”. 
     Various circuits serve as the noise generation source R and generate electromagnetic wave, and the noise N of the secondary radiation is emitted from the radiation amount reducing device  900  according to the related art. The strong noise N of the secondary radiation is roughly divided into two types. The noise N of the first type is the main noise, and is a radiation having the metal plate  90  as a patch antenna. This noise N is mainly emitted from the surface of the metal plate  90  towards the opposite side of the noise generation source R. The noise N of the second type is emitted when an opening formed by an edge (end) of the metal plate and a GND (ground) surface in the substrate, where the noise generation source R is arranged, operate as if an electrostatic capacity antenna. 
     The generation mechanism of the secondary radiation noise N that became apparent as a result a thorough research conducted by the inventors of the present invention will be briefly described below. 
     If the metal plate  90  covering the noise generation source R is arranged as with the metal plate  90  of the radiation amount reducing device  900  according to the related art, the electric field generates as if a standing wave at the lower part of the metal plate  90 , that is, between the metal plate  90  and the noise generation source R. The position of strong electric field generated (referred to as “intense electric field position”) is shown in  FIG. 10 . As shown in  FIG. 10 , the intense electric field positions VA to VD generate at four corners of the metal plate  90 , and the intense electric field position VO generates at the middle of the metal plate  90 . The intense electric field positions are determined at least by one of either the shape of the metal plate  90  or the shape of the noise generation source R. The loop of the electric field of pseudo-standing wave generates at the intense electric field positions VA to VD, VO, where the sign of the electric field of the adjacent intense electric field positions is inverted with respect to each other. Thus, a circular current I (hereinafter also referred to as outer peripheral current) flows by the electric field. 
     The circular current I flows the outer periphery so as to surround the central part O of the metal plate  90 , and becomes smaller towards the central part O. When such circular current I flows, a magnetic field generates at the upper part and the lower part of the metal plate  90 . The magnetic field generated at the lower part of the metal plate  90  generates as if a standing wave similar to the intense electric field position of the electric field mentioned above. The position of strong magnetic field generated (referred to as “ferromagnetic field position”) is shown in  FIG. 10 . As shown in  FIG. 10 , the ferromagnetic field positions BA to BD generate at the middle of four sides of the metal plate  90 . In other words, the ferromagnetic field positions BA to BD generate at the midpoint of the intense electric field positions VA to VD. 
     The electric field and the magnetic field generated at the lower part of the metal plate  90  respectively perform an operation similar to the electric field and the magnetic field generated by the electrostatic capacity antenna between the GND in the substrate and the metal plate  90 . The electric field and the magnetic field generate noise N (noise N of second type; may not be accurate secondary radiation) through the opening between the GND in the substrate and the metal plate  90 . The magnetic field generated at the upper part of the metal plate  90  by the circular current I generates the electric field in chain reaction and generates noise N (noise N of first type). 
     Therefore, in the radiation amount reducing device  900  according to the related art simply formed with the metal plate  90 , the electromagnetic wave radiated by the noise generation source R is simply scattered in the x-y plane direction (noise N of second type) or is again radiated from the surface of the metal plate  90  (noise N of first type). 
     The inventors of the present invention who conducted a thorough research on the noise N etc. of the radiation amount reducing device  900  according to the related art clarified the generation mechanism of the noise N as described above, and completed the present invention through further researches and developments in an aim of reducing the noise N. Hereinafter, an explanation will be given on each embodiment of the present invention. It is to be understood that the generation mechanism of the noise N described herein does not limit the noise N, and that the radiation amount reducing device according to each embodiment of the present invention can reduce even the radiation amount of noise other than the two types of noise N described above. 
     2. Radiation Amount Reducing Device According to First Embodiment 
     First, an explanation will be given on a configuration of the radiation amount reducing device according to a first embodiment of the present invention with reference to  FIGS. 1A and 1B .  FIGS. 1A and 1B  are explanatory views describing the configuration of the radiation amount reducing device according to the first embodiment of the present invention. 
     2-1. Configuration of Radiation Amount Reducing Device 
     As shown in  FIG. 1A , a radiation amount reducing device  100  according to the present embodiment roughly includes a metal plate  10  and slits SA to SD. 
     In the present embodiment, a case in which the radiation amount reducing device  100  reduces the radiation amount of the electromagnetic wave radiated to the upper side of the noise generation source R will be described, as shown in  FIG. 1B , for the sake of convenience of explanation. The metal plate  10  described below is thus formed to a shape that covers the upper surface of the noise generation source R, and the radiation amount reducing device  100  is arranged near the upper surface side of the noise generation source R. The shape of the metal plate  10 , the arrangement position of the radiation amount reducing device  100 , and the like can be appropriately changed according to the noise generation source R, the direction of reducing the radiation amount, and the like. 
     The metal plate  10  is made from a material having conductivity, and includes a cover surface that can cover at least the entire upper surface (one example of one surface) of the noise generation source R (one example of electromagnetic wave generation source) for radiating the electromagnetic wave. As shown in  FIG. 1B , the metal plate  10  according to the present embodiment is entirely formed as a cover surface. However, the cover surface of the metal plate  10  may not be over the entire region of the metal plate  10 , and may be over a region of one part of the metal plate  10 . That is, the metal plate  10  can be formed to various shapes as long as it has a surface (cover surface) corresponding to the entire upper surface of the noise generation source R. The region of the metal plate  10  that becomes the cover surface is also referred to as “cover region Ar”. 
     That is, in the present embodiment, the cover region Ar is comparable to the entire region of the metal plate  10 . If the cover region Ar is comparable to the entire region of the metal plate  10 , the area of the metal plate  10  is desirably between 1 and 1.5 times, and more preferably between 1.25 and 1.5 times the area of the upper surface of the noise generation source R to be covered by the metal plate  10 . The metal plate  10 , however, may be formed much larger than the upper surface of the noise generation source R. 
     In the present embodiment, a case in which the metal plate  10  is formed to a square in correspondence to the shape of the upper surface of the noise generation source R is shown. However, the metal plate  10  may not correspond to the shape of the upper surface of the noise generation source R, and may not be a square. The metal plate  10  is desirably formed in the following order to enhance the radiation amount reducing effect and the like of the radiation amount reducing device  100 . 
     Square Regular≧polygon&gt;Polygon&gt;Ellipse&gt;Circle 
     However, other than the shapes mentioned in the example, the metal plate  10  may have, for example, a shape in which the center distance is unequal. 
     The cover region Ar is a region that is set within a plane of the meal plate  10 , and that covers the entire upper surface of the noise generation source R. As described above, the cover region Ar is set to the entire region of the metal plate  10  in the present embodiment. 
     The slits SA to SD are formed to a band-shape at least in the cover region Ar. The slits SA to SD can be formed by cutting out one part of the metal plate  10  in a band-shape (also referred to as groove) or by forming the metal plate  10  itself excluding the slits SA to SD. As shown in  FIG. 1A , the slits SA to SD are formed towards a central part O and is formed to a cross-like shape as a whole, but the slits adjacent in the peripheral direction of the metal plate  10  are not connected to each other and are spaced apart. Therefore, metal plate pieces  11  to  12  pseudo-partitioned by the slits SA to SD are connected to each other by way of the central part O to form the metal plate  10 . 
     In the present embodiment, four of such slits SA to SD are formed, as shown in  FIG. 1A . However, the number of slits SA to SD is not limited to four, and may be in plurals. However, 2 N  of such slits SA to SD is desirably formed on the metal plate  10 , where N is a positive integer. 
     As shown in  FIG. 1A , the slits SA to SD according to the present embodiment are arranged point symmetrically with the central part O of the cover region Ar (i.e., metal plate  10 ) as a reference. Each slit SA to SD is formed to a similar shape. The shape of each slit will be first described using the slit SA by way of example. 
     As shown in  FIG. 1A , the slit SA is broadly divided into a drawing slit S 1 A and a coupling slit S 2 A. 
     The drawing slit S 1 A is formed extending from the ferromagnetic field position BA at the outer periphery of the cover region Ar towards the central part O of the cover region Ar. Since the cover region Ar and the entire metal plate  10  match in the present embodiment, the drawing slit S 1 A is formed from the end of the metal plate  10 . Moreover, the ferromagnetic field position BA at the outer periphery of the cover region Ar is generated in an edge position (ends) at a middle between four corners (corner portion, intense electric field position) of the cover region Ar, as shown in  FIG. 10 , and thus the drawing slit S 1 A is formed extending in a band-shape from this edge position towards the central part O. 
     Furthermore, the drawing slit S 1 A is formed in a straight line to a band-shape from the corner towards the central part O in the present embodiment, but the drawing slit S 1 A may be curved. However, the drawing effect of the circular current I by the drawing slit S 1 A enhances, and the radiation amount reducing effect enhances if the drawing slit S 1 A is formed in a straight line as in the present embodiment. 
     The coupling slit S 2 A is formed extending from the end in the central part O direction of the cover region Ar of the drawing slit S 1 A so as to be lined in parallel to another slit SB (or slit SD) on one side in the peripheral direction of the cover region Ar. More specifically, the coupling slit S 2 A is formed extending so as to be lined in parallel to the drawing slit S 1 B of another slit SB in the present embodiment. 
     In the present embodiment, a case in which the coupling slit S 2 A is formed extending to the right side (counterclockwise direction) of the drawing slit S 1 A in the peripheral direction of the cover region Ar is shown. Therefore, each coupling slit S 2 B to S 2 D is formed extending to the right side (counterclockwise direction) at the end of the central part O direction in other drawing slits S 1 B to S 1 D as well. The coupling slits S 2 A to S 2 D, however, may be formed extending to the left side (clockwise direction) of each drawing slit in the peripheral direction of the cover region Ar. 
     The coupling slit S 2 A according to the present embodiment is formed parallel to the drawing slit S 1 B of the adjacent slit SB, and is formed with a predetermined spacing with such drawing slit S 1 B. The coupling slit S 2 A is desirably formed shorter than the lined drawing slit S 1 B so as not to be formed up to the end of the cover region Ar. The coupling slit S 2 A is desirably formed to a band-shape with a width same as or approximate to the drawing slit S 1 A. 
     The coupling slit S 2 A guides the circular current I, which is guided by the drawing slit S 1 A, substantially parallel to the lined drawing slit S 1 B to realize the coupling effect of coupling the same with the circular current I guided by the drawing slit S 1 B. 
     The drawing slit S 1 A and the coupling slit S 2 A described here respectively correspond to the slit SA, but other slits SB to SD similarly include one of each of the drawing slit S 1 B to S 1 D and the coupling slit S 2 B to S 2 D. In other words, each slit SA to SD is formed to a substantially L-shape, which L-shaped slits SA to SD are formed extending from the edge position at the middle of the four corners of the metal plate  10 . As a result, the slits SA to SD partition the metal plate  10  to four metal plate pieces  11  to  14  of a substantially cross-shape. The slits SA to SD of substantially L-shape are spaced apart from each other, and the metal plate pieces  11  to  14  forming the metal plate  10  are coupled to each other at the central part O. 
     (Regarding Intense Electric Field Position) 
     As described above, the slits SA to SD are respectively formed from the ferromagnetic field positions BA to BD towards the central part O direction. The ferromagnetic field positions BA to BD will be described. 
     As described above, the ferromagnetic field positions BA to BD are locations where a magnetic field generates with the noise generation source R due to the electromagnetic wave generated by the noise generation source R, where such magnetic field is large compared to other sites. The intense electric field positions VA to VD correspond to locations where a special impedance between the metal plate  10  and the noise generation source R is low. The ferromagnetic field positions BA to BD correspond to the midpoint position (edge position of metal plate  10  in the present embodiment) of the intense electric field positions VA to VD at the outer periphery of the cover region Ar. Accordingly, in the radiation amount reducing device  100  according to the present embodiment, the metal plate  10  is formed to a polygon (square) of the same extent as the noise generation source R or an extent of covering the same, but in this case, the spatial impedance of the corner of the metal plate  10  becomes low compared to other sites. Thus, the four corners of the metal plate  10  become the intense electric field positions VA to VD, and the edge positions at the middle of the four corners of the metal plate  10  become the ferromagnetic field positions BA to BD. In the radiation amount reducing device  100  according to the present embodiment, the slits SA to SD are respectively formed from the edge positions at the middle of the four corners. Since the ferromagnetic field positions BA to BD differ depending on the shape of the metal plate  10 , the shape of the noise generation source R, and the like, as mentioned above, the positions where the slits SA to SD are formed can be changed depending on the shape of the metal plate  10 , the shape of the noise generation source R, and the like. The intense electric field positions are the edge positions (ends), which center distance is long compared to other sites, when the metal plate  10  is formed such that the center distance from the central part O to the outer periphery unequal. The ferromagnetic field positions become the edge positions (ends) at the middle of such edge position. More specifically, the intense electric field position is a corner (corner portion) if the metal plate  10  is a polygon, and is four corners shown in  FIG. 1A  if the metal plate  10  is a square as in the present embodiment. Therefore, the ferromagnetic field position is the middle of each side if the metal plate  10  is a polygon, and is each middle of the four sides shown in  FIG. 1A  if the metal plate  10  is a square as in the present embodiment. If the metal plate  10  does not have a corner and the metal plate  10  is significantly larger than the cover region Ar, the intense electric field positions VA to VD are positions at the outer periphery of the cover region Ar corresponding to the corners of the upper surface of the noise generation source R. In this case, the ferromagnetic field positions BA to BD are positions at the outer periphery of the cover region Ar corresponding to the edge position at the middle of the intense electric field positions VA to VD, that is, at the middle between the corners of the upper surface of the noise generation source R. Therefore, in such a case, the slits SA to SB are formed from the ferromagnetic field positions corresponding to the midpoint position between the corners of the upper surface of the noise generation source R. 
     The configuration of the radiation amount reducing device  100  according to the first embodiment of the present invention has been described above. 
     The operation example of the radiation amount reducing device according to the first embodiment of the present invention will now be descried with reference to  FIGS. 2A to 3B .  FIGS. 2A to 3B  are explanatory views describing the operation example of the radiation amount reducing device according to the present embodiment. 
     2-2. Operation Example of Radiation Amount Reducing Device 
     2-2-1. Circular Current Attenuating Operation 
     First, the attenuating operation of the circular current I, which is the main generation source of noise N, will be described. 
     As described in  FIG. 10 , when the electric field and the magnetic field similar to the standing wave generates between the metal plate  10  and the noise generation source R by the electromagnetic wave generated by the noise generation source R, the circular current I circularly flows so as to surround the central part O of the cover region Ar by such electric field and magnetic field. The circular current I is the main cause of generation of the noise N of the secondary radiation and the like. 
     On the other hand, the radiation amount reducing device  100  according to the present embodiment includes a plurality of slits SA to SD formed from the ferromagnetic field positions BA to BD, as described above. In such slits SA to SD, each of drawing slits S 1 A to S 1 D is formed from the ferromagnetic field position BA to BD. The ferromagnetic field positions BA to BD are positions where the magnetic field is stronger than other sites, and a magnetic field H generates, as shown in  FIG. 2A , in the edges of the drawing slits S 1 A to S 1 D by forming the drawing slits S 1 A to S 1 D at the ferromagnetic field positions BA to BD.  FIG. 2A  schematically shows the magnetic field H as magnetic current. In other words, the radiation magnetic field component of the electromagnetic wave generated by the noise generation source R couples at the ferromagnetic field positions BA to BD to the drawing slits S 1 A to S 1 D and excites the magnetic field H. The magnetic field H is guided towards the central part O side of the cover region Ar along the drawing slits S 1 A to S 1 D while being coupled to the drawing slits S 1 A to S 1 D. The circular current I is divided by the drawing slits S 1 A to S 1 D, and is guided towards the central part O side with the magnetic field H, as shown in  FIG. 2A , with the coupling of the magnetic field H to the drawing slits S 1 A to S 1 D. As shown in  FIG. 2B , the circular current I guided towards the central part O side by the drawing slits S 1 A to S 1 D is guided to between another slit adjacent on one side in the peripheral direction by the coupling slits S 2 A to S 2 D. Therefore, the circular current I flows at the edge portion of each slit SA to SD. 
     As shown in  FIG. 2B , the circular current I flowing the edge portion of each slit SA to SD has an opposite phase to the circular current I guided by the adjacent slit. Therefore, the circular currents I of opposite phases cancel each other out at the region A and the region B where two slits SA to SD become parallel. That is, the circular current I is canceled out and attenuated at two regions A, B, as can be seen from one slit. As a result, the radiation amount reducing device  100  according to the present embodiment can reduce the noise N of the secondary radiation and the like. 
     2-2-2. Radiation Magnetic Field Component Attenuating Operation 
     The radiation magnetic field component that generates the magnetic field H by coupling to each slit SA to SD is guided along each slit SA to SD from the ferromagnetic field positions BA to BD, as described above. Each slit SA to SD couples not only the radiation magnetic field component from the ferromagnetic field positions BA to BD, but also the radiation magnetic field component at other locations and generates the magnetic field H. The magnetic field H generated in each slit SA to SD has an opposite phase, as shown in  FIG. 3B , at parallel positions PA to PD shown in  FIG. 3A , and thus cancel each other out. Therefore, the noise N of the secondary radiation by the magnetic field H generated at the respective slit SA to SD also becomes an opposite phase in the parallel positions PA to PD and cancels each other out, whereby the noise N is further reduced. 
     2-2-3. Remaining Secondary Radiation Component Attenuating Operation 
     Furthermore, still remaining secondary radiation component generates even by the circular current attenuating operation and the radiation magnetic field component attenuating operation. However, as shown in  FIG. 3A , since each slit SA to SD is formed point symmetrically in the present embodiment, the noises N generated by the opposing slits SA to SD (slit SA and slit SC or slit SB and slit SD) have substantially the same amplitude and have opposite phases. As a result, the noise N of the secondary radiation component cancels each other out even if supposedly radiated. More specifically, the secondary radiation component radiated from the parallel position PA becomes an opposite phase to the secondary radiation component radiated from the parallel position PC thereby canceling each other out, and the secondary radiation component radiated from the parallel position PB becomes an opposite phase to the secondary radiation component radiated from the parallel position PD thereby canceling each other out. The noise N is thus further reduced. 
     Therefore, the radiation amount reducing device  100  according to the present embodiment can reduce the radiation amount of noise N by realizing the circular current attenuating operation, the radiation magnetic field component attenuating operation, and the remaining secondary radiation component reducing operation with the arrangement of the slits SA to SD. Such operations, however, are merely examples and the radiation amount reducing device  100  is not limited to such operations, and the existence of operations not mentioned herein and the possibility of reducing the noise N by such operations are not to be excluded. 
     The operation examples of the radiation amount reducing device  100  according to the first embodiment of the present invention have been described above. 
     An example of the radiation amount reducing device according to the first embodiment of the present invention will now be described with reference to  FIGS. 4 to 6 .  FIGS. 4 to 6  are explanatory views for describing the example of the radiation amount reducing device according to the present embodiment. 
     2-3. Example of Radiation Amount Reducing Device 
     In measuring the radiation amount reducing effect by the radiation amount reducing device according to the present embodiment, a measurement device imitating a print substrate as shown in  FIG. 4  is prepared. More specifically, a vinyl film T 2  is arranged at the lower surface of a measuring target X, which vinyl film T 2  is arranged on a supporting plate T 1  so as to block an opening of the supporting plate T 1 . The electromagnetic wave is generated from the noise generation source R while changing the frequency, and the noise N (electric field distribution) radiated from the measuring target X is measured by a reception probe D spaced apart by 50 mm from the measuring target X. 
     As shown in  FIG. 5A , a radiation amount reducing device  900  according to the related art without slits and the radiation amount reducing devices  101 ,  102  according to the present embodiment are prepared and arranged at the position of the measuring target X, and the radiation amount of the noise N is measured by the measurement device. 
     The radiation amount reducing devices  101 ,  102  according to the present embodiment are respectively formed with the slits SA to SD of different size, as shown in  FIG. 5A . That is, the metal plate  10  is obtained by forming a copper plate having a thickness of 0.09 mm to a square of 40 mm×40 mm, and the slits SA to SD having a slit width of 0.8 mm are formed in the metal plate  10 . The material of the metal plate  10  is not particularly limited as long as it has conductivity, and effects similar to those described below can be obtained even with other materials. 
     In this case, the length of the drawing slits S 1 A to S 1 D of the radiation amount reducing device  101  is 18 mm, and the length of the coupling slits S 2 A to S 2 D is 11 mm. The length of the drawing slits S 1 A to S 1 D of the radiation amount reducing device  102  is 17.5 mm, and the length of the coupling slits S 2 A to S 2 D is 11 mm. The slit interval (i.e., interval between adjacent slits) at the parallel positions PA to PD is 0.6 mm. The angle between the drawing slit S 1 A to S 1 D and the coupling slit S 2 A to S 2 D in each slit SA to SD is 90°. The slits SA to SD have a shape rotated 90° with respect to each other (i.e. four-fold symmetry of 90°) with the central part O of the cover region Ar (i.e., metal plate  10 ) as a reference so as to be formed to a substantially cross-shape as a whole. The radiation amount reducing device  900  according to the related art uses the metal plate  90  similar to the metal plate  10 . 
       FIG. 5B  shows the measurement result in which measurement signal I 101  with respect to the radiation amount reducing device  101  according to the present embodiment is standardized with a measurement signal I 900  with respect to the radiation amount reducing device  900  according to the related art as 0 dB.  FIG. 5C  shows the result in which simulations results C 101 , C 102  with respect to the radiation amount reducing devices  101 ,  102  are standardized with a simulation result C 900  with respect to the radiation amount reducing device  900  according to the related art as 0 dB using an electromagnetic field simulator. 
     Generally, as the slits SA to SD are opened in the metal plate  10 , the electromagnetic wave leaked therefrom is added to the secondary radiation component, and thus the amount of noise N is assumed to degrade in the radiation amount reducing devices  101 ,  102  according to the present embodiment compared to the radiation amount reducing device  900  according to the related art. Therefore, the measurement signals I 101 , I 102  by the radiation amount reducing devices  101 ,  102  are generally expected to become higher than the measurement signal I 900  with respect to the radiation amount reducing device  900  according to the related art. 
     However, the radiation amount reducing devices  101 ,  102  according to the present embodiment can greatly reduce the secondary radiation component (noise N) in a wide range of electromagnetic wave frequency band, contrary to one&#39;s expectations, as apparent not only from  FIG. 5B  but also from  FIG. 5C . This is because the radiation amount reducing devices  101 ,  102  can greatly reduce the secondary radiation by drawing in the radiation component into the slits SA to SD and mutually interfering and cancelling out the same using a plurality of slits SA to SD. 
     Radiation amount reducing devices  103  to  107  (not shown) according to the present embodiment, in which the dimension of the slits SA to SD is appropriately changed in the metal plate  10  similar to the above, are prepared, and the measurement similar to the above is performed. 
     In this case, the radiation amount reducing device  103  has a slit width of 1.0 mm, the length of the drawing slits S 1 A to S 1 D of 17 mm, the length of the coupling slits S 2 A to S 2 D of 15 mm, and the slit interval at the parallel positions PA to PD of 0.4 mm. The radiation amount reducing device  104  has a slit width of 1.2 mm, the length of the drawing slits S 1 A to S 1 D of 18.5 mm, the length of the coupling slits S 2 A to S 2 D of 15 mm, and the slit interval at the parallel positions PA to PD of 0.6 mm. The radiation amount reducing device  105  has a slit width of 0.6 mm, the length of the drawing slits S 1 A to S 1 D of 17 mm, the length of the coupling slits S 2 A to S 2 D of 11 mm, and the slit interval at the parallel positions PA to PD of 0.4 mm. The radiation amount reducing device  106  has a slit width of 0.8 mm, the length of the drawing slits S 1 A to SW of 17 mm, the length of the coupling slits S 2 A to S 2 D of 13 mm, and the slit interval at the parallel positions PA to PD of 0.2 mm. The radiation amount reducing device  107  has a slit width of 1.4 mm, the length of the drawing slits S 1 A to S 1 D of 18 mm, the length of the coupling slits S 2 A to S 2 D of 12 mm, and the slit interval at the parallel positions PA to PD of 0.5 mm. 
       FIG. 6  shows the measurement results in which measurement signals I 103  to I 107  with respect to the radiation amount reducing devices  103  to  107  are standardized with the measurement signal I 900  with respect to the radiation amount reducing device  900  according to the related art as 0 dB. 
     Even if the dimensions of the slits SA to SD differ, the measurement results of  FIG. 6  also show that the radiation amount reducing devices  103  to  107  according to the present embodiment can realize the secondary radiation (noise N) reducing effect by having the slits SA to SD reliably couple the radiation component. 
     The example of the radiation amount reducing device according to the first embodiment of the present invention has been described above. 
     An implementation example of the radiation amount reducing device according to the first embodiment of the present invention will now be described with reference to  FIGS. 7A to 7F .  FIGS. 7A to 7F  are explanatory views describing an implementation example of the radiation amount reducing device according to the present embodiment. 
     2-4. Implementation Example of Radiation Amount Reducing Device 
     The radiation amount reducing device  100  according to the first embodiment of the present invention can be formed with a very simple configuration in which the slits SA to SD are formed in the metal plate  10 , as described above. In particular, the radiation amount reducing device  100  is not particularly subjected to limitation on the arrangement position and is simply arranged near the noise generation source R as it does not even need to be grounded, thereby enabling various implementations. Some of the implementation examples of the radiation amount reducing device  100  will be described below. 
     2-4-1. First Implementation Example 
       FIG. 7A  shows a case in which the radiation amount reducing device  100  according to the present embodiment is directly printed on the upper surface of the noise generation source R. In this case, the radiation amount reducing device  100  may be embedded inside the noise generation source R instead of the upper surface of the noise generation source R. The radiation amount reducing device  100  can be easily configured and the radiation amount of noise N with respect to one surface side of the noise generation source R can be greatly reduced by directly printing the radiation amount reducing device  100  on the noise generation source R. In this case, an insulating protective layer of about 0.05 mm is desirably formed between the noise generation source R and the radiation amount reducing device  100 . 
     2-4-2. Second Implementation Example 
       FIG. 7B  shows a case in which the radiation amount reducing device  100  is fixed on the upper surface of the noise generation source R with an adhesive  31  (may be seal with adhesive), as an implementation example of the radiation amount reducing device  100  integrally formed with the noise generation source R, similar to the first implementation example. In this case, a raw material having insulating property is desirably used for the adhesive  31  and the like. 
     2-4-2. Third Implementation Example 
       FIG. 7C  shows a case in which the radiation amount reducing device  100  according to the present embodiment is fixed to a shield case  23 . The noise generation source R is arranged on a substrate  22  and is covered by shield cases  21 ,  23 . The radiation amount reducing device  100  is fixed at the interior with an adhesive, a seal (not shown), and the like at a position facing the noise generation source R of the shield case  23  at the upper side. The radiation amount reducing device  100  may obviously be fixed to the upper side of the shield case  23 . The radiation amount reducing device  100  thus can be arranged near the noise generation source R in any manner since the arrangement position is not limited. Furthermore, the radiation amount reducing device  100  can be easily arranged since grounding and the like is not necessary and a fixing means is not particularly a problem. 
     2-4-2. Fourth Implementation Example 
       FIG. 7D  shows a case in which the radiation amount reducing device  100  according to the present embodiment is formed as one part of the shield case  23 . In this case, a site covering the noise generation source R of the shield case  23  is the metal plate  10 , and the position facing the noise generation source R of the metal plate  10  is the cover region Ar. The slits SA to SD are formed in the cover region Ar. In this case, the radiation amount reducing device  100  according to the present embodiment can be formed by simply forming the slits SA to SD in the shield case  23 . 
     2-4-2. Fifth Implementation Example 
       FIG. 7E  shows a case in which the radiation amount reducing device  100  according to the present embodiment is directly formed in the shield case  23  and the metal plate  10  is much larger than the cover region Ar covering the noise generation source R. similar to the fourth implementation example. In this case, same as the above fourth implementation example, since the cover region Ar and the metal plate  10  do not match, the outer periphery (corner) of the cover region Ar corresponding to the edge position in the middle of the corner of the upper surface of the noise generation source R becomes the intense electric field positions BA to BD, and the slits SA to SD are formed from the intense electric field positions BA to BD. 
     2-4-2. Sixth Implementation Example 
       FIG. 7F  shows a case in which the radiation amount reducing device  100  according to the present embodiment is directly formed in the shield case  23 , but the cover region Ar covering the noise generation source R is substantially the same extent as the metal plate  10 , different from the fifth implementation example. In this case, the corners of the metal plate  10  become the corners of the cover region Ar, and also become the ferromagnetic field positions BA to BD. Thus, the slits SA to SD are formed from the edge positions at the middle between the corners of the metal plate  10 . As shown in  FIG. 7F , the slits SA to SD are desirably formed extending to the side surface different from the metal plate  10  in the shield case  23  to more effectively guide the circular current I to the central part O. This is similar in the case of the fifth implementation example. Therefore, in the fifth implementation example, the circular current I can be more effectively guided to the central part O as the slits SA to SD of  FIG. 7E  are extended to the end of the metal plate  10  or the vicinity thereof beyond the cover region Ar. 
     The implementation examples of the radiation amount reducing device  100  according to the first embodiment of the present invention have been described above. The implementation examples described herein are merely examples, and the application of the radiation amount reducing device  100  is not to be limited to such implementation examples. As described above, various other implementations can be carried out since the radiation amount reducing device  100  is formed with a very simple configuration and the arrangement position thereof is not limited. 
     2-5. Variant of Radiation Amount Reducing Device 
     A variant of the radiation amount reducing device  100  according to the first embodiment of the present invention will now be described with reference to  FIGS. 8A to 8E .  FIGS. 8A to 8E  are explanatory views describing variants of the radiation amount reducing device according to the present embodiment. 
     2-5-1. Number of Slits and Arrangement Position 
     Point Symmetric 
     As described above, the radiation amount reducing device  100  according to the present embodiment can reduce the noise N by realizing the circular current attenuating operation, the radiation magnetic field component attenuating operation, the residual secondary radiation component attenuating operation, and the like with the arrangement of the plurality of slits SA to SD. The circular current attenuating operation and the radiation magnetic field component attenuating operation are realized when the adjacent slits draw in the circular current I or the magnetic field H of opposite phases with respect to each other in the central part O direction, as described in  FIGS. 2A ,  2 B, and  3 B. Two or more slits are to be formed to realize the circular current attenuating operation and the radiation magnetic field component attenuating operation. 
     However, as described in  FIG. 3A , the residual secondary radiation component attenuating operation is realized when the noises N generated from each slit SA to SD become opposite phases at substantially the same amplitude. To this end, the number of slits to be formed is desirably 2 N , N being a positive integer, in relation to the phase. To further enhance the cancelling effect by equalizing the amplitude of the noises N of opposite phases, the plurality of slits is desirably formed point symmetrically with the central part O of the cover region Ar as a reference. That is, describing the number of slits and the arrangement position together, 2 N  slits are formed, and the slits are desirably formed 2 N  fold symmetrically with the central part O of the cover region Ar as a reference. 
     The circular current attenuating operation, the radiation magnetic field component attenuating operation, the residual secondary radiation component attenuating operation, and the like are realized to the same extent for when the number of slits is N=2 and for when N is greater than 2. Therefore, in view of the increase in the slit forming steps due to the increase in the number of slits, and the reduction in the mechanical strength of the radiation amount reducing device  100 , the number of slits is desirably N=2, that is, four. Taking into consideration that each slit is formed point symmetrically, the slits SA to SD may be formed in a rectangular metal plate  10 , as shown in  FIG. 8A . However, the four-fold symmetric slits SA to SD as in the present embodiment shown in  FIG. 1A  are desirably formed to isotropically realize the cancelling effect by equalizing the amount of circular currents I to cancel out, the amplitude of the magnetic fields H, the amplitude of the noises N of opposite phases, and the like. 
     However, the circular current attenuating operation, the radiation magnetic field component attenuating operation, and the like can be realized even if the slit is formed in plurals other than 2 N . It is to be note that the circular current attenuating operation, the radiation magnetic field component attenuating operation, the residual secondary radiation component attenuating operation, and the like can be realized even if the plurality of slits is not formed point symmetrically, as shown in  FIG. 8B . In this case, the central part O of the cover region Ar may be an intersection of the diagonal lines of each corner of the metal plate  10  or a barycentric position of the metal plate  10 . 
     2-5-2. Shape of Metal Plate 
     Meanwhile, the slit is formed from the ferromagnetic field position of the cover region Ar towards the central part O, as described above. In this case, if the metal plate  10  significantly larger than the cover region Ar (e.g., greater than or equal to 1.5 times), the ferromagnetic field position becomes the position at the outer periphery of the cover region Ar corresponding to the edge position at the middle between the corners of the upper surface of the noise generation source R, as shown in  FIGS. 7D and 7E . However, if the cover region Ar is substantially the entire region of the metal plate  10 , the ferromagnetic field position corresponds to the edge position at the middle between the corners of the metal plate  10 . 
     The number of slits formed is desirably 2 N , N being a positive integer, in relation to the phase to sufficiently realize the residual secondary radiation component attenuating operation. Therefore, the ferromagnetic field position formed with the slit is desirably arranged by the number of the same extent. To this end, the metal plate  10  is desirably formed to a polygon in which 2 M  corners are formed at the outer periphery, where M is a positive integer of greater than or equal to two. Therefore, the metal plate  10  desirably has a 4-, 8-, 16-, 32 polygon shape etc. to sufficiently realize the residual secondary radiation component attenuating operation. Similar to desirably forming the slits point symmetrically to further enhance the cancelling effect by equalizing the amplitude of the noise N of opposite phases, the metal plate is also desirably formed point symmetrically. Furthermore, similar to desirably forming the slits SA to SD four-fold symmetrically to isotropically realize the cancelling effect, the metal plate  10  is desirably a regular polygon. 
     An example of a case in which the metal plate  10  is formed to a regular polygon is shown in  FIGS. 8C and 8D . In  FIGS. 8C and 8D , the metal plate  10  is formed to a regular octagon. In  FIG. 8C , eight slits SA to SH are formed in eight-fold symmetry to satisfy the above relationship. However, the number of slits may not match the number of corner portions of the metal plate  10 , and thus four slits SA to SD may be formed at four-fold symmetry, as shown in  FIG. 8D . 
     If the metal plate  10  does not have a corner or is formed to a shape in which the center distance from the central part O to the outer periphery is unequal as with an ellipse shown in  FIG. 8E , the ferromagnetic field positions BA, BC become edge positions at the middle between the edge positions which center distance is long compared to other sites. Therefore, in this case, the plurality of slits SA, SC are formed from the ferromagnetic field positions BA, BC, which are edge positions, as shown in  FIG. 8E . 
     If the metal plate  10  is formed without such edge position as with a circle shown in  FIG. 8F , the ferromagnetic field positions BA to BD become positions at the outer periphery of the cover region Ar (i.e., metal plate  10 ) corresponding to the edge positions at the middle between the corners of the upper surface of the noise generation source R, similar to  FIG. 7E  and the like. Therefore, in this case, the plurality of slits SA to SD are formed from the ferromagnetic field positions BA to BD, as shown in  FIG. 8F . 
     2-6. Example of Effects of Radiation Amount Reducing Device 
     The radiation amount reducing device  100  according to the present embodiment of the present invention has been described above. 
     According to such radiation amount reducing device  100 , the radiation noise component generated at the upper part of a site can be divided and acted to cancel out by simply being loaded on the upper surface of the noise generation source R. Therefore, the electromagnetic wave generated from the noise generation source R can be effectively suppressed while reducing the generation of noise N of the secondary radiation and the like. In this case, the canceled electromagnetic wave energy is absorbed as heat. 
     The radiation amount reducing device  100  can be easily arranged with an adhesive, a seal, and the like, and can be easily arranged since the task that may lower the assembly task efficiency such as screw-fitting task is not carried out. The manufacturing cost is also expected to greatly reduce since the radiation amount reducing device  100  can be formed with a simple structure. 
     As described above, the radiation amount reducing device  100  can be loaded freely without being subjected to limitation on the arrangement position since grounding is not even necessary. Therefore, the amount reducing device  100  can be appropriately arranged near a plurality of noise generation sources R, the electromagnetic wave of which is desirably reduced, and the noise can be appropriately reduced even in a state where a wide variety of noise generation sources is present. It is to be noted that use can be made by grounding to the shield case, and the like. 
     The preferred embodiments of the present invention have been described above with reference to the accompanying drawings, whilst the present invention is not limited to the above examples, of course. A person skilled in the art may find various alternations and modifications within the scope of the appended claims, and it should be understood that they will naturally come under the technical scope of the present invention. 
     For instance, in the above-described embodiment, a case of drawing in the circular current I to the central part O side by the drawing slits S 1 A to S 1 D and directly canceling out the circular currents I etc. flowing through the adjacent slits SA to SD by the coupling slits S 2 A to S 2 D has been described. However, the effect of drawing and canceling out the circular current I can be indirectly realized through auxiliary coupling slits S 11  to S 14  in place of the coupling slits S 2 A to S 2 D, as shown in  FIG. 9A . In this case, however, not only the circular current attenuating operation, but the radiation magnetic field component attenuating operation and the residual secondary radiation component attenuating operation are also suppressed low compared to the first embodiment, and thus the configuration of directly canceling out the circular currents I etc. as in the first embodiment is desirable. 
     To realize the reducing effect of the circular current I and the like with each slit SA to SD alone, auxiliary slits S 3 A to S 3 D and auxiliary slits S 4 A to S 4 D may be arranged on both sides of the coupling slits S 2 A to S 2 D, as shown in  FIG. 9B . In this case, the circular current I is guided towards the central part O side by the drawing slits S 1 A to S 1 D, and then flowed around the auxiliary slits, so that the circular current I can be reduced. In this case, however, the circular current attenuating operation and the radiation magnetic field component attenuating operation are difficult to sufficiently realize, and thus the configuration of canceling out the circular currents I etc. as in the first embodiment is desirable.