Antenna device

Abstract: To provide an antenna device where radiated electromagnetic wave is efficiently used in communication, a radiating conductor film (112) having two ends adjacent to each other and connecting the two ends in a loop-like shape, is formed on an upper face of a dielectric base body (111) in a rectangular parallelepiped shape having the upper face and a lower face in a square shape in parallel with each other, a grounding conductor film (113) extending in a planar shape is formed on the lower face of the dielectric base body (111) and feeding conductor films (114) and (115) respectively connected to the two ends of the radiating conductor film (112), extending in the up and down direction in parallel with each other one of which is connected to the grounding conductor film (113), is formed on a side face of the dielectric base body (111).

Description: BACKGROUND OF THE INVENTION .Field of the Invention The present invention relates to an antenna device used in a portable communication device or the like. Description of the Related Art An antenna device which is small-sized, having high gain, fabricated at low cost and easy to mount has been requested as an antenna device used in a portable communication device. However, a conventionally used linear antenna such as a dipole antenna or a monopole antenna or the like has a large volume, which hampers downsizing of a communication device and further, such an antenna is not easy to mount to a main body of a communication device and is difficult to use in a portable communication device or the like which has been requested to downsize. Several antennas have been proposed to resolve such a problem. JP-A- 0350901 discloses an antenna device according to the preamble of claim 1. Fig. 65 is a perspective view showing an antenna device proposed in Japanese Unexamined Patent Publication No. JP-A-7-235825. A radiating conductor film 992 is formed on the entire upper face of a dielectric substrate 991 constituting an antenna device 990. A grounding film 993 is formed on the lower face of the dielectric substrate 991. The grounding conductor film 993 has a shape where a portion of one of two short sides is notched and an exciting conductor film 994 is formed at the notched portion. A feed electrode 995 is formed at a side face of the dielectric substrate 991 and the feed electrode 995 is connected to the exciting conductor film 994. Ground electrodes 996 and 997 are formed to interpose the feed electrode 995 at the side face of the dielectric substrate 991 and the ground electrodes 996 and 997 are connected to the grounding conductor film 993. Further, a through hole 998 having a conductor at an inner wall thereof is formed in the dielectric substrate 991, and the radiating conductor film 992 and a front end portion of the exciting conductor film 994 are electrically connected by the through hole 998. The antenna device 990 constituted as described above is mounted on the surface of a circuit board incorporated in the main body of a communication device, high frequency power is supplied from the main body of the communication device to the radiating conductor film 992 via the feed electrode 995, the exciting conductor film 994 and the through hole 998 and electromagnetic wave is radiated to air from the radiating conductor film 992 by an electromagnetic coupling between the exciting conductor film 994 and the radiating conductor film 992. Fig. 66 is a perspective view showing an antenna device proposed by Japanese Unexamined Patent Publication No. JP-A-7-283639. A through hole 1102 constituting a radiating conductor film at its inner wall is formed in a dielectric base body 1101 constituting an antenna device 1100. A surface electrode 1103 is formed on the surface of the dielectric base body 1101 and a connector external conductor plate 1104 is attached to the rear face thereof. The surface electrode 1103 and the connector external conductor plate 1104 are electrically connected by the radiating conductor film formed on the inner wall of the through hole 1102. Further, a coaxial connector 1105 is attached to a face of the connector external conductor plate 1104 opposed to a face thereof on which the dielectric base body 1101 is attached. An external conductor and an internal conductor of the coaxial connector 1105 are electrically connected to the connector external conductor plate 1104 and the radiating conductor film in the through hole 1102, respectively. The antenna device 1100 constituted as described above is arranged to the main body of a communication device by connecting the coaxial connector 1105 to a connector installed to the main body of the communication device, high frequency power is supplied from the main body of the communication device to the antenna device 1100 via the coaxial connector 1105 and electromagnetic wave is radiated from the radiating conductor film formed on the inner wall of the through hole 1102. Fig. 67 is a perspective view showing an antenna device proposed by Japanese Unexamined Patent Publication No. JP-A-7-221537. A through hole 1212 constituting a radiating conductor film at its inner wall is formed in a dielectric substrate 1211 constituting an antenna device 1210 in a direction of long side of the dielectric substrate 1211. A side face electrode 1213 is formed on an entire face of an end face of the dielectric substrate 1211, a feed electrode 1214 is formed at a central portion of the other end face and the side face electrode 1213 and the feed electrode 1214 are electrically connected by the radiating conductor film formed on the inner wall of the through hole 1212. Further, side face electrodes 1215 and 1216 are formed to interpose the feed electrode 1214 on a face of the dielectric substrate 1211 where the feed electrode 1214 is formed. The antenna device 1210 constituted as described above is mounted to a circuit board incorporated in the main body of a communication device, high frequency power is supplied from the main body of the communication device to the antenna device 1210 via the feed electrode 1214 and electromagnetic wave is radiated from the radiating conductor film at the inner wall of the through hole 1212. According to the antenna device 990 shown by Fig. 65, the frequency band of electromagnetic wave must be narrowed to enhance gain and therefore, when frequencies of electromagnetic waves for transmission and receiving are different from each other as in a portable telephone, it is difficult to use the antenna device 990 as an antenna both for transmission and receiving. The antenna devices 1100 and 1210 shown by Fig. 66 and Fig. 67, are nondirectional in respect of a face expanding perpendicularly to a direction of extending the through hole where the radiating conductor film is formed. When such antenna devices are mounted to, for example, a portable telephone, a portable telephone generally transmits and receives electromagnetic wave of a vertically polarized wave and therefore, the antenna device is mounted to the main body of a portable telephone such that a direction of extending the through hole coincides with a longitudinal direction of the main body of the portable telephone. When a person actually uses a portable telephone mounted with such an antenna device, since the antenna device is nondirectional in respect of a face perpendicular to a direction of extending the through hole, a portion of electromagnetic wave transmitted from the antenna device is radiated toward a human body. The electromagnetic wave radiated toward a human body is not used in communication. SUMMARY OF THE INVENTION It is an object of the present invention in view of the above-described situation to provide an antenna device where electromagnetic wave is efficiently used in communication. In order to achieve the above-described object, an antenna device according to claim 1 is provided. According to the antenna device of the present invention, the radiating conductor film having the two ends adjacent to each other and connecting the two ends in a loop-like shape, is formed on the upper face of the dielectric base body and the grounding conductor film extending in a planar shape is formed on the lower face of the dielectric base body. Therefore, electromagnetic wave having the resonance frequency of the length of the radiating conductor film is radiated such that the maximum gain is obtained in a direction perpendicular to a loop face of the radiating conductor film and the electromagnetic wave radiated from the radiating conductor film and progressing toward the grounding conductor film is reflected by the grounding conductor film. That is, the electromagnetic wave having the maximum gain is radiated from the antenna device in a direction perpendicular to a plane including the radiating conductor film and directed from the grounding conductor film to the radiating conductor film. Therefore, the antenna device having high directivity and high gain can be obtained. When the antenna device is attached to, for example, a portable telephone, if the grounding conductor film is disposed between a person and the radiating conductor film when the person uses the portable telephone, electromagnetic wave is not radiated toward the side of the person and radiated electromagnetic wave has the maximum gain in the direction directed from the grounding conductor film to the radiating conductor film by which the antenna device can be efficiently used in communication. According to the antenna device of the present invention, it is not necessary in forming the radiating conductor film to constitute a through hole in a dielectric base body by which reduction in fabrication cost is achieved. It is preferable that the feeding conductor films of the antenna device also serve as electrodes in mounting onto a surface of a circuit board. The antenna device can be easily mounted on the circuit board when the feeding conductor films also serve as electrodes in mounting the antenna device onto the face of the circuit board. The radiating conductor film turning horizontally around the side faces may be formed on the side faces and the grounding conductor film extending in a planar shape is formed on the lower face. Accordingly, electromagnetic wave having the maximum gain is radiated from the radiating conductor film in a direction perpendicular to a plane including the radiating conductor film and electromagnetic wave progressing toward the grounding conductor film among radiated electromagnetic waves, is reflected by the grounding conductor film. That is, the electromagnetic wave having the maximum gain is radiated from the antenna device in a direction perpendicular to the plane including the radiating conductor film and directed from the grounding conductor film to the radiating conductor film. Therefore, when the antenna device is attached to, for example, a portable telephone, if the grounding conductor film is disposed between a person and the radiating conductor film when the person uses the portable telephone, electromagnetic wave is not radiated to the side of the person and electromagnetic wave is efficiently used in communication with maximum gain in a direction directed from the grounding conductor film to the radiating conductor film. The radiating conductor film making a turn in a loop-like shape on a horizontal plane may be formed at the inner portion of the antenna device and the grounding conductor film extending in a planar shape is formed on the lower face. Therefore, electromagnetic wave having the maximum gain is radiated from the radiating conductor film in a direction perpendicular to a plane including the radiating conductor film and electromagnetic wave progressing toward the grounding conductor film among radiated electromagnetic waves, is reflected by the grounding conductor film. That is, the electromagnetic wave having the maximum gain is radiated from the antenna device in a direction perpendicular to the plane including the radiating conductor film and directed from the grounding conductor film to the radiating conductor film. Accordingly, when the antenna device is attached to, for example, a portable telephone, if the grounding conductor film is disposed between a person and the radiating conductor film when the person uses the portable telephone, electromagnetic wave is not radiated to the side of the person and radiated electromagnetic wave can efficiently be used in communication with the maximum gain in a direction directed from the grounding conductor film to the radiating conductor film. Meanwhile, when a wavelength of electromagnetic wave in air is compared with a wavelength of electromagnetic wave in a dielectric body in the case of the electromagnetic waves having the same frequency, the wavelength of the electromagnetic wave in the dielectric body is shorter. Accordingly, when a case where a radiating conductor film is formed at an inner portion of a dielectric base body, is compared with a case where the radiating conductor film is formed on a surface of the dielectric base body in radiating electromagnetic waves having the same frequency, the length of the loop of the radiating conductor film can be shortened further in the case where the radiating conductor film is formed at the inside of the dielectric base body. When the length of the loop of the radiating conductor film can be shortened in this way, the dimension of the dielectric base body can be downsized. Accordingly, downsizing of the antenna device of the present invention where the radiating conductor film is formed at the inner portion of the dielectric base body can be realized. Fig. 1 is an explanatory view for explaining the operation of an antenna device having a loop antenna structure. Fig. 1 is a top view of an antenna device 10. A radiating conductor film 12 where two ends 12a and 12b adjacent to each other are opposed to each other via a gap and which connect the two ends 12a and 12b by making a turn in a circular loop shape with a point O as center, is formed on the surface of a dielectric base body 11 constituting the antenna device 10. The length of the radiating conductor film 12 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission and receiving. Further, point A designates a point indicating the position of the two ends 12a and 12b and points B, C and D are points at positions which is rotated from point A clockwisely by 90°, 180° and 270° with point O as center, respectively. According to an antenna device 10 constituted as described above, when voltage is applied between the two ends 12a and 12b, current is supplied from the two ends 12a and 12b to the radiating conductor film 12, a standing wave is generated in the radiating conductor film 12 and current flowing in the radiating conductor film 12 is maximized at point A and point C and becomes almost 0 at point B and point D. At point A and point C where the maximum current flows, the direction of current is in a direction along a line connecting point B and point D. Accordingly, the polarized wave direction is in a direction along the line connecting point B and point D. Fig. 2 is an explanatory view explaining the operation of an antenna device instead of the radiating conductor film shown by Fig. 1 in which a feed point is provided also at the position of point C shown by Fig. 1 and radiating conductor films constituting a loop-like shape as a whole are adopted. According to an antenna device 20 constituted as described above, when currents having the same amplitude and the same phase are supplied from point A and point C, standing waves are generated in radiating conductor films 22 and currents flowing in the radiating conductor films 22, are maximized at point A and point C and become almost 0 at point B and point D similar to the antenna device 10 shown by Fig. 1. The direction of currents is in a direction along a line connecting point B and point D at point A and point C where the maximum current flows. Accordingly, a polarized wave direction is in a direction along the line connecting point B and point D similar to the antenna device 10 shown by Fig. 1. Fig. 3 is an explanatory view for explaining the operation of an antenna device constituted by adopting radiating conductor films forming a loop-like shape as a whole where feed points are provided also at positions of point B and point D shown by Fig. 2 in place of the radiating conductor films shown by Fig. 2. According to an antenna device 30 constituted as described above, in respect of radiating conductor films 32 constituting the antenna device, the loop is cut off at positions of point B and point D where current becomes almost 0. Accordingly, when currents having the same amplitude and the same phase are supplied from point A and point C, similar to the antenna device 20 shown by Fig. 2, standing waves are generated in the radiating conductor films 32 and currents flowing in the radiating conductor film 32 are maximized at point A and point C and become 0 at point B and point D. The direction of current is in a direction along a line connecting point B and point D at point A and point C where the maximum current flows. Accordingly, similar to the antenna device 20 shown by Fig. 2, the polarizing direction is in a direction along the line connecting point B and point D. Meanwhile, when currents having the same amplitude and the same phase are supplied from point B and point D in place of point A and point C, standing waves are generated in the radiating conductor films 32 and currents flowing in the radiating conductor films 32 are maximized at point B and point D and becomes 0 at point A and point C. The direction of current is in a direction along a line connecting point A and point C at point B and point D where the maximum current flows and the polarized wave direction is in a direction along the line connecting point A and point C. Accordingly, when a state where currents having the same amplitude and the same phase are supplied to point A and point C-and a state where currents having the same amplitude and the same phase are supplied to point B and point D, can be switched freely, an antenna device having the gain capable of switching to polarized wave directions perpendicularly intersecting with each other, is provided. The four radiating conductor films extending in the horizontal direction, contiguous ends of which are opposed to each other via gaps and making a turn by forming four of the gaps at equal intervals as a whole, are constituted as shown by Fig. 3 and accordingly, electromagnetic waves in polarized directions perpendicularly intersecting with each other can be transmitted and received. The radiating conductor film may be a radiating conductor film in a closed loop shape making a turn on the upper face of the dielectric base body or turning around side faces of the dielectric base body. Further, the radiating conductor film may be a radiating conductor film in a closed loop shape making a turn on a horizontal plane at the inside of the dielectric base body. When a wavelength of electromagnetic wave in air is compared with a wavelength of electromagnetic wave in a dielectric body with respect to electromagnetic waves having the same frequency, the wavelength of the electromagnetic wave in the dielectric body is shorter and therefore, the length of the loop of the radiating conductor film can be shortened when the radiating conductor film is formed at an inner portion of the dielectric base body. Accordingly, the dimensions of dielectric base body can be downsized and downsizing of the antenna device is achieved. Here, it is preferable that the antenna device of the present invention further includes in addition to the radiating conductor film, a second radiating conductor film in a closed loop shape making a turn horizontally at a position of the dielectric base body different from the position where the radiating conductor film is formed, and a second pair of feeding conductor films extending in the up and down direction in parallel with each other via positions of a side face of the dielectric base body different from the positions where the pair of feeding conductor films are formed and connected to the second radiating conductor film. When the pair of feeding conductor films and the second pair of feeding conductor films are formed via positions of the side face of the dielectric base body, which are different from each other, polarized directions of transmitted and received electromagnetic waves at the radiating conductor film connected to the pair of feeding conductor films and the second radiating conductor films connected to the second pair of feeding conductor films, are different from each other. An explanation will be given of the reason why polarized directions of transmitted and received electromagnetic waves are different from each other with respect to the radiating conductor films as follows. Fig. 4 is an explanatory view therefor. Fig. 4 is a top view of an antenna device 40. A radiating conductor film 42 in a circular closed loop shape making a turn horizontally along a circumference of an upper face with point O as center, is formed on the surface of a dielectric base body 41 in a cylindrical shape constituting an antenna device 40. Further, point A is a point for connecting to the radiating conductor film 42 with a pair of feeding conductor films, not shown, and points B, C and D are points at positions which are rotated clockwisely from point A by 90°, 180° and 270°, respectively, with point O as center. According to the antenna device 40 constituted as described above, since the radiating conductor film 42 in a closed loop shape is formed, it has a single wavelength loop antenna structure and when current is supplied from point A to the radiating conductor film 42, a standing wave is generated in the radiating conductor film 42 and current flowing in the radiating conductor film 42 is maximized at point A and point C and becomes almost 0 at point B and point D. The direction of the current is in a direction along a line connecting point B and point D at point A and point C where the maximum current flows and polarized direction is in a direction along the line connecting point B and point D. Accordingly, when current is supplied from, for example, point B to the radiating conductor film 42 instead of supplying current from point A to the radiating conductor film 42, the polarized direction is in a direction along a line connecting point A and point C. When a case where current is supplied from point A to the radiating conductor film 42, is compared with a case where the current is supplied from point B to the radiating conductor film 42, the polarized directions become perpendicular to each other. As described above, the pair of second feeding conductor films connected to the second radiating conductor film are formed via positions different from positions via which the above-described pair of feeding conductor films connected to the radiating conductor film are formed. Therefore, when the radiating conductor film is compared with the second radiating conductor film, points for supplying current are different from each other in respect of a horizontal plane. Accordingly, it is known from the explanation in reference to Fig. 4 that the polarized direction of electromagnetic wave transmitted and received by the radiating conductor film and polarized direction of electromagnetic wave transmitted and received by the second radiating conductor film, are different from each other. Accordingly, when the pair of feeding conductor films and the second pair of feeding conductor films are formed via positions on the side faces of the dielectric base body, which are different from each other, electromagnetic waves having the polarized directions different from each other can be transmitted and received by the single antenna device. Here, a total of four pairs of feeding conductor films connected to the radiating conductor films at one of positions equally dividing by four an interval turning around the radiating conductor films and extending in the up and down direction in parallel with each other, may be formed including the pair of feeding conductor films. Although an explanation has been given of the case where current is supplied from point A to the radiating conductor film 42 in reference to Fig. 4, when a case where currents having the same amplitude and the same phase are supplied from point A and point C to the radiating conductor film 42, is considered, similar to the case where current is supplied from point A to the radiating conductor film 42, the currents flowing in the radiating conductor film 42 are maximized at point A and point C and becomes almost 0 at point B and point D and the direction of current becomes a direction along a line connecting point B and point D at point A and point C where the maximum current flows. That is, the polarized direction becomes a direction along the line connecting point B and point D. Accordingly, when currents having the same amplitude and the same phase are supplied from point B and point D to the radiating conductor film 42 instead of supplying currents having the same amplitude and the same phase from point A and point C to the radiating conductor film 42, the polarized direction is in a direction along a line connecting point A and point C. When the case where currents having the same amplitude and the same phase are supplied from point A and point C to the radiating conductor film 42, is compared with the case where currents having the same amplitude and the same phase are supplied from point B and point D to the radiating conductor film 42, the polarized directions become perpendicular to each other. As described above, since four pairs of the feeding conductor films are formed at positions equally dividing by four the radiating conductor films and accordingly, when the state where currents having the same amplitude and the same phase are supplied to two pairs of the feeding conductor films formed at positions equally dividing in two an interval turning around the radiating conductor films, and the state where currents having the same amplitude and the same phase are supplied to remaining two pairs of the feeding conductor films, can be switched freely, the antenna device having the gain capable of freely switching to polarized directions perpendicular to each other can be provided. Fig. 5 through Fig. 7 are explanatory views for explaining the function of an antenna device of the present invention. Fig. 5 is a perspective view showing an antenna device where two feeding conductor films are formed on one side face of a dielectric base body having four side faces and Fig. 6 is a horizontal sectional view thereof. An antenna device 60 shown by Fig. 5 is provided with a dielectric base body 61 in a rectangular parallelepiped shape. A radiating conductor film 62 having two ends 62a and 62b adjacent to each other and connecting the two ends 62a and 62b along four sides of the upper face in a loop-like shape, is formed on the upper face of the dielectric base body 61 and the length of the radiating conductor film is adjusted to become the resonance wavelength of electromagnetic wave that is an object of transmission. A grounding conductor film 63 extending in a planar shape is formed on the lower face of the dielectric base body 61 and the grounding conductor film 63 is provided with a shape where a portion of a side is notched. As shown by Fig. 6, feeding conductor films 64 and 65 having a coplanar line structure are formed on the side face of the dielectric base body 61. The feeding conductor films 64 and 65 are respectively connected to the two ends 62a and 62b of the radiating conductor film 62 and extended in the up and down direction in parallel with each other. The feeding conductor film 65 that is one of the feeding conductor films 64 and 65, is connected also to the grounding conductor film 63 and the other one of the feeding conductor film 64 reaches the lower face of the dielectric base body 61. Power is supplied from the two ends 62a and 62b (hereinafter, two ends 62a and 62b are referred to as feed points) to the radiating conductor film 62 of the antenna device 60 shown by Fig. 5 via the feeding conductor films. Generally, when the feed points of power in the radiating conductor film are points adjacent to each other in the case of a single wavelength loop antenna, the antenna is provided with high impedance of 100 Ω or higher and therefore, it is difficult to efficiently supply power to the radiating conductor film. Accordingly, in order to efficiently supply power to the radiating conductor film by reducing impedance, if the antenna device is provided with the feeding conductor films having a coplanar line structure as shown by Fig. 5, a distance between the feed points of the radiating conductor film is adjusted, that is, the gap width between the feeding conductor films is adjusted. By adjusting the gap width, the impedance is reduced and power can efficiently be supplied to the radiating conductor film. Further, the impedance of the radiating conductor film and the impedance of the feeding conductor films must be matched with each other. The impedance Z of the feeding conductor films having the coplanar line structure as shown by Fig. 5, can be represented by the following equation when the gap width of the feeding conductor films is designated by notation 2W and the width of the feeding conductor film is designated by S. Z ∝ { (1-/ε reff ) }k where ε reff is effective dielectric constant, k=W/(W+S) Here, the effective dielectric constant ε reff is represented by the following equation by determining the dielectric constant of air as 1 since electric fields are generated from the feeding conductor film at the inside of the dielectric base body and in air. ε reff = (ε r +1)/2 where ε r is dielectric constant of dielectric base body. Meanwhile, in order to reduce the impedance to efficiently supply power to the radiating conductor film, there is a case where the gap length 2W between the feeding conductor films must be widened. In this case, when the impedance Z of the feeding conductor films is intended to match with impedance of the radiating conductor film, since notation k in the equation of the impedance Z of the feeding conductor film represented by Equation (1), is defined by Equation (2), when the gap width 2W is widened, the width S of the feeding conductor film must be widened in accordance therewith. Since a sum of the gap width of the feeding conductor film and the width of the two feeding conductor films is 2W+2S, when the width of the side face of the dielectric base body is smaller than 2W+2S, the impedance of the feeding conductor films cannot be matched with the impedance of the radiating conductor film. Accordingly, when the feeding conductor films are formed on the side face of the dielectric base body, the width S of the feeding conductor film is restricted, the impedance of the feeding conductor film may not be set to a desired value and impedance of the radiating conductor films may not be matched with the impedance of the feeding conductor film. Fig. 7 is a horizontal sectional view of an antenna device where a feeding conductor film is formed at each of both sides of a side extending vertically on side faces of a dielectric base body. An antenna device 70 shown by Fig. 7 is provided with a dielectric base body 71 in a rectangular parallelepiped shape and each of feeding conductor films 72 and 73 is formed at each of both sides of a side 71a among four sides extending in the up and down direction on side faces of the dielectric body. Accordingly, when a sum of a distance from the side 71a to the feeding conductor film 72 and a distance from the side 71a to the feeding conductor film 73, is designed to be equal to the distance between the feeding conductor films shown by Fig. 5 and Fig. 6, the antenna device shown by Fig. 7 has a shorter distance between the two feeding conductor films than that in the antenna device shown by Fig. 5 and Fig. 6 by which the effective dielectric constant ε reff defined by the above-described Equation (3) is increased. Accordingly, when the antenna device of Fig. 5 and Fig. 6 is compared with the antenna device of Fig. 7, in the case where the value of notation W in Equation (2) is equal, if both of the impedances Z of the feeding conductor films are adjusted to Z=Z 1 , the value of notation k in Equation (1) must be increased, due to the fact that the effective dielectric constant ε reff is larger in the antenna device of Fig. 7. The increase in the value of k amounts to further narrowing the width S of the feeding conductor film of the antenna device shown by Fig. 7 than the width S of the feeding conductor film of the antenna device shown by Fig. and Fig. 6. Therefore, according to the antenna device of Fig. 7, impedance can be matched even if the width of the feeding conductor film is narrower than that of the antenna device shown by Fig. 5 and Fig. 6. That is, even if the gap width of the feeding conductor film is wide, the impedance of the radiating conductor film can be matched with the impedance of the feeding conductor film. Further, the antenna device has a single wavelength loop antenna structure since the radiating conductor film in a loop-like shape is formed on the upper face of the dielectric base body and electromagnetic wave radiated from the radiating conductor film is electromagnetic wave having the maximum gain in a direction perpendicular to a plane including the radiating conductor film. Further, since the grounding conductor film is formed on the lower face of the dielectric base body, electromagnetic wave progressing toward the grounding conductor film among electromagnetic waves radiated from the radiating conductor film, is reflected by the grounding conductor film. That is, the electromagnetic wave having the maximum gain is radiated from the antenna device in a direction perpendicular to the plane including the radiating conductor fi-lm and directed from the grounding conductor film to the radiating conductor film. Accordingly, when the antenna device of the present invention is attached to, for example, a portable telephone, if the grounding conductor film is disposed between a person and the radiating conductor film when the person uses the portable telephone, electromagnetic wave is not radiated to the side of the person and radiated electromagnetic wave is provided with the maximum gain in the direction directed from the grounding conductor film to the radiating conductor film and is efficiently used in communication. The radiating conductor film may be provided with an open loop shape where points of connecting the two feeding conductor films to the radiating conductor film, are electrically opened or a closed loop shape where in respect of the radiating conductor film, a conductor film in a strip-like shape turns around. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a top view of a loop antenna having one feed point; Fig. 2 is a top view of a loop antenna having two feed points; Fig. 3 is a top view of a loop antenna having four feed points; Fig. 4 is a top view of a loop antenna where a radiating conductor film having a closed loop shape is formed; Fig. 5 is a perspective view showing an antenna device where feeding conductor films are formed on the same side face; Fig. 6 is a horizontal sectional view of the antenna device as shown by Fig. 4; Fig. 7 is a horizontal sectional view of an antenna device where one feeding conductor film is formed at each of both sides of a side extending longitudinally on side faces of a dielectric base body; Fig. 8 is a view showing an antenna device according to Embodiment 1 of the present invention; Fig. 9 is a top view of the antenna device as shown by Fig. 8; Fig. 10 is a side view of the antenna device as shown by Fig. 8; Fig. 11 is a bottom view of the antenna device as shown by Fig. 8; Fig. 12 is a view showing an antenna device according to Embodiment 2 of the present invention; Fig. 13 is a view showing a state where the antenna device shown by Fig. 8 is mounted on a circuit board; Fig. 14 is a perspective view showing a first example of an antenna device not being part of the present invention; Fig. 15 is a top view of an antenna device as shown by Fig. 14; Fig. 16 is a bottom view of the antenna device as shown by Fig. 14; Fig. 17 is a side view of the antenna device as shown by Fig . 4; Fig. 18 is a side view showing a second example of an antenna device not being part of the present invention; Fig. 19 is a view showing dimensions of a pattern printed on an upper face of a dielectric base body; Fig. 20 is a view showing dimensions of a pattern printed on a lower face of the dielectric base body; Fig. 21 is a view showing dimensions of a pattern printed on a side face of the dielectric base body; Fig. 22 is a view used in explaining the gain characteristic of an antenna device; Fig. 23 is a view showing the gain characteristic of an antenna device; Fig. 24 is a perspective view showing an antenna device according to Embodiment 3 of the present invention; Fig. 25 is a bottom view showing the antenna as shown by Fig. 24; Fig. 26 is a view showing dimensions of a dielectric base body, a radiating conductor film and feeding conductor films; Fig. 27 is a perspective view showing an antenna device according to Embodiment 4 of the present invention; Fig. 28 is a view showing a state where the antenna device shown by Fig. 24 is mounted on a circuit board; Fig. 29 is a perspective view showing an antenna device according to Embodiment 5 of the present invention; Fig. 30 is a top view of the antenna device as shown by Fig. 29; Fig. 31 is a bottom view of the antenna device as shown by Fig. 29; Fig. 32 is a side view of the antenna device as shown by Fig. 29; Fig. 33 is a view showing a length and a width of a dielectric base body and dimensions of radiating conductor film and inner feeding conductor films; Fig. 34 is a view showing a thickness of the dielectric base body and dimensions of side feeding conductor films; Fig. 35 is a view showing an antenna device according to Embodiment 6 of the present invention; Fig. 36 is a view showing a state where the antenna device shown by Fig. 29 is mounted on a circuit board; Fig. 37 is a perspective view of an antenna device according to Embodiment 7 of the present invention; Fig. 38 is a top view of the antenna device as shown by Fig. 37; Fig. 39 is a sectional view taken from a line A-A' of the antenna device as shown by Fig. 37; Fig. 40 is a bottom view of the antenna device as shown by Fig. 37; Fig. 41 is a view showing a side face of the antenna device as shown by Fig. 37 where first feeding conductor films are formed; Fig. 42 is a view showing a side face of the antenna device as shown by Fig. 37 where second feeding conductor films are formed; Fig. 43 is a view showing a length and a width of the dielectric base body and dimensions of a first loop radiating conductor film; Fig. 44 is a view showing dimensions of a second loop radiating conductor film; Fig. 45 is a view showing a thickness of the dielectric base body and dimensions of first feeding conductor films; Fig. 46 is a view showing a thickness of the dielectric base body and dimensions of a second feeding conductor film; Fig. 47 is a perspective view showing an antenna device according to Embodiment 8 of the present invention; Fig. 48 is a view showing a drive circuit for driving the antenna device as shown by Fig. 47; Fig. 49 is a perspective view showing an antenna device according to Embodiment 9 of the present invention; Fig. 50 is a perspective view showing an antenna device according to Embodiment 10 of the present invention; Fig. 51 is a perspective view showing an antenna device according to Embodiment 11 of the present invention; Fig. 52 is a view showing an antenna device according to Embodiment 12 of the present invention; Fig. 53 is a bottom view of the antenna device as shown by Fig. 52; Fig. 54 is a view showing an antenna device according to Embodiment 13 of the present invention; Fig. 55 is a view showing an antenna device according to Embodiment 14 of the present invention; Fig. 56 is a view showing an antenna device according to Embodiment 15 of the present invention; Fig. 57 is a view showing an antenna device according to Embodiment 16 of the present invention; Fig. 58 is a view showing an antenna device according to Embodiment 17 of the present invention; Fig. 59 is a view showing an antenna device according to Embodiment 18 of the present invention; Fig. 60 is a top view of the antenna device as shown by Fig. 59; Fig. 61 is a bottom view of the antenna device as shown by Fig. 59; Fig. 62 is a view showing a side face of the antenna device as shown by Fig. 59 where one of two feeding conductor films is formed; Fig. 63 is a view showing a side face of the antenna device as shown by Fig. 59 where a feeding conductor film different from the feeding conductor film shown by Fig. 62 is formed; Fig. 64 is a view showing an antenna device according to Embodiment 19 of the present invention; Fig. 65 is a perspective view showing an antenna device proposed in Japanese Unexamined Patent Publication No. JP-A-7-235825; Fig. 66 is a perspective view showing an antenna device proposed in Japanese Unexamined Patent Publication No. JP-A-7-283639; and Fig. 67 is a perspective view showing an antenna device proposed in Japanese Unexamined Patent Publication No. JP-A-7-221537. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An explanation will be given of embodiments of the present invention as follows. Fig. 8 is a perspective view showing an antenna device according to Embodiment 1 of the present invention, Fig. 9 is a top view thereof, Fig. 10 is a bottom view thereof and Fig. 11 is a side view thereof. An antenna device 110 shown by Fig. 8 is provided with a dielectric base body 111 in a shape of a rectangular parallelepiped having an upper face and a lower face in a square shape in parallel with each other. As shown by Fig. 9, a radiating conductor film 112 having two ends 112a and 112b which are adjacent to each other and connecting in a loop shape the two ends 112a and 112b to extend along four sides of the upper face, is formed on the upper face of the dielectric base body 111 and the length of the radiating conductor film is adjusted to constitute a resonance wavelength of electromagnetic wave that is an object of transmission. As shown by Fig. 10, a grounding conductor film 113 is formed on the lower face of the dielectric base body 111 and the grounding conductor film 113 has a shape where a portion of one side is notched. As shown by Fig. 11, feeding conductor films 114 and 115 respectively connected to the two ends 112a and 112b of the radiating conductor film 112 and extending in the up and down direction in parallel, are formed on one side of the piezoelectric base body 111. The feeding conductor film 115 that is one of the feeding conductor films 114 and 115, is connected also to the grounding conductor film 113 and the other one of the feeding conductor film 114 reaches the lower face of the dielectric base body 111. Further, portions of the feeding conductor films 114 and 115 on the side of the grounding conductor film 113, also serve as feeding electrodes 116 and 117 which are electrodes for mounting onto the surface of a circuit board. The antenna device 110 constituted as described above has a structure of a single wavelength loop antenna since it has the radiating conductor film 112. A single wavelength standing wave is formed by supplying current to the radiating conductor film 112 via the feeding electrode 116 and the feeding conductor film 114, electromagnetic wave is radiated from the radiating conductor film 112 in a direction perpendicular to a face of the dielectric base body 111 where the radiating conductor film 112 is formed and the electromagnetic wave progressing toward the grounding conductor film 113 is reflected by the grounding conductor film 113. That is, the electromagnetic wave having the maximum gain is irradiated from the antenna device 110 in a direction perpendicular to a plane including the radiating conductor film 112 and progressing from the grounding conductor film 113 to the radiating conductor film 112. Therefore, the antenna device having high directivity and high gain is provided by which the radiated electromagnetic wave is efficiently used in communication. Further, it is not necessary to form a through hole at the inside of the dielectric base body 111 and accordingly, reduction in fabrication cost can be achieved. According to the antenna device 110 of Embodiment 1 of the present invention, the feeding conductor film 115 is grounded to the grounding conductor film 113. Fig. 12 is a view showing an antenna device according to Embodiment 2 of the present invention. A dielectric base body 151 in a cylindrical shape is adopted in an antenna device 150 as shown by Fig. 12, in place of the dielectric base body 111 having a rectangular parallelepiped shape of the antenna device 110 shown by Fig. 8 through Fig. 11, whereby with respect to the radiating conductor film, a radiating conductor film 152 in a circular loop shape is formed and with respect to the grounding conductor film, a circular grounding conductor film 153 is formed. In this way, the shape of the dielectric base body is arbitrary so far as it has an upper face and a lower face in parallel to each other. Fig. 13 is a view showing a state where the antenna device shown by Fig. 8 through Fig. 11 is mounted on a circuit board. The antenna device 110 is mounted on a circuit board 163 where an electricity feed line 161 and a grounding conductor layer 162 are formed and respective pairs of the electricity feed line 161 and the feeding conductor film 114, and the grounding conductor layer 162 and the feeding conductor film 115 are soldered to each other by solders 164. In this way, the antenna device 110 is mounted on the circuit board 103. An explanation will be given of a fabrication method of the antenna device 110 shown by Fig. 8 through Fig. 11 as follows. First, a material of the dielectric base body 111 is selected. A material where the dielectric constant is stabilized to substantially 10 through 100 in a frequency band of transmitted and received electromagnetic wave, is preferably used as the material of the dielectric base body 111. For example, a Sr(Ni 1/3 Nb 2/3 )O 3 group ceramic is preferable. The material has the dielectric constant of 30 when the frequency of transmitted and received electromagnetic wave is 6 GHz and the Q value is 1000. Next, dimensions of the radiating conductor film 112 and the feeding conductor films 114 and 115 will be determined. The dimensions can be determined as follows. When the length of radiating conductor film 112 is designated by notation λ, λ can be expressed by the following equation. λ = λ 0 / (ε reff ) where λ 0 is a wavelength of electromagnetic wave in vacuum and ε reff is an effective dielectric constant. Further, the direction of propagating electromagnetic wave radiated from the radiating conductor film shown by Fig. 8, is a direction intersecting perpendicularly with the face of the dielectric base body where the radiating conductor film is formed and since electric fields are present in both of the dielectric base body and air, the effective dielectric constant ε reff can be represented by the following equation. ε reff = ( ε r + 1)/2 where ε r is the dielectric constant of the dielectric base body. Therefore, λ can be calculated by calculating the effective dielectric constant ε reff by using Equation (5) and substituting the calculated ε reff for Equation (4). When the resonance frequency of electromagnetic wave is set to 1.9 GHz, λ=40.11 mm and accordingly, in order to form the radiating conductor film 112 shown by Fig. 8, the length of one side of the radiating conductor film 112 is determined as 10.03 mm. Further, the impedance of a single wavelength loop antenna is generally as high as 100 Ω or higher, however, the electricity feed efficiency can be promoted by lowering the impedance by adjusting the width of the radiating conductor film or the interval between the two ends. For example, in order to set the impedance to 50 Ω, the width of the radiating conductor film 112 is set to 2 mm and the interval between the two ends 112a and 112b is set to 1 mm. It has been reported that a desired transmission impedance can be provided by adjusting the width of a feeding conductor film and the interval between feeding conductor films in "C.P. Wen: 'Coplanar Waveguide: A Surface Strip Transmission Line Suitable for Nonreciprocal Gyromagnetic Device Applications', IEEE Trans. MTT, Vol. MTT-17, No. 12, Dec. 1969". In this report, the width of the feeding conductor films 114 and 115 is set to 3.09 mm and the interval between the feeding conductor films is set to 1 mm in order to set the transmission impedance to 50 Ω. Next, the dielectric base body 111 is fabricated by setting both of the length and the width of the dielectric base body 111 to 12.03 mm in accordance with the radiating conductor film 112 the dimensions of which has determined as described above and setting the thickness to 7.21 mm corresponding to a quarter of the wavelength of the electromagnetic wave having the resonance frequency of 1.9 GHz in the dielectric base body 111. Next, patterns of the radiating conductor film 112, the feeding conductor films 114 and 115 and the grounding conductor film 113 each having above-described dimensions, are printed by the thick film printing process by using a copper paste and sintered in a reducing atmosphere. After subjecting to the fabrication procedure, the antenna device 110 shown by Fig. 8 is manufactured. Fig. 14 is a perspective view showing a first example of an antenna device not being part of the present invention, Fig. 15 is a top view thereof, Fig. 16 is a bottom view thereof and Fig. 17 is a side view thereof. An antenna device 210 shown by Fig. 14 is provided with a dielectric base body 211 and the dielectric base body 211 has an upper plane and a lower plane both in a square shape in parallel to each other and has a through hole 212 extending perpendicularly to the upper plane and the lower plane. The thickness of the dielectric base body 211 is adjusted to correspond to a quarter of the resonance wavelength of electromagnetic wave that is an object of transmission in the dielectric base body 211 and a quarter wavelength monopole antenna structure is constituted by filling the through hole 212 with a monopole conductor 213. A film-like loop conductor 214 having two mutually adjacent ends 214a and 214b and connecting the two ends 214a and 214b in a loop to extend along four sides of the upper face, is formed on the upper face of the dielectric base body 211 as shown by Fig. 15. The length of the loop conductor 214 is adjusted to constitute the resonance wavelength of electromagnetic wave which is the object of transmission. A coupling line 215 is formed on the upper face to connect the end 214b of the loop conductor 214 to the monopole conductor 213. As shown by Fig. 16, a film-like grounding conductor 216 extending in a channel-like shape to surround an end of the monopole conductor 213, is formed on the lower face of the dielectric base body 211. Further, a signal line 217 one end of which is connected to the monopole conductor 213 and which has gaps 231, 232, 233 at intermediaries with respect to the grounding conductor 216 and forms coplanar lines along with the grounding conductor 216, is formed on the lower face. As shown by Fig. 17, a feed terminal 218 is formed at a side face of the dielectric base body 211 and the feed terminal 218 is connected to the signal line 217 as shown by Fig. 14. Ground terminals 219 and 220 are formed on a side face the same as the side face where the feed terminal 218 is formed, to interpose the feed terminal 218 and the ground terminals 219 and 220 are connected to the grounding terminal 216 as shown by Fig. 14. The antenna device 210 constituted as described above, is provided with the film-like loop conductor 214 having a single wavelength loop antenna structure and has the monopole conductor 213 having a quarter length monopole antenna structure. Therefore, when electric current is supplied to the loop conductor 214 via the feed terminal 218, electromagnetic wave is radiated from the loop conductor 214 perpendicularly to a face of the dielectric base body 211 where the loop conductor 214 is formed and electromagnetic wave progressing toward the grounding conductor 216 is reflected by the grounding conductor 216. Meanwhile, electromagnetic wave having the maximum gain is radiated from the monopole conductor 213 in parallel with the face where the loop conductor 214 is formed. Accordingly, when the antenna device 210 is attached, for example, to a portable telephone, if it is attached such that the grounding conductor is disposed between a person and the loop conductor when the person uses the portable telephone, the electromagnetic wave is not radiated to the side of the person but the electromagnetic wave is effectively radiated to directions other than the direction toward the person. Further, the antenna device 210 is provided with the signal line 217 forming coplanar lines along with the grounding conductor 216 and a desired line impedance is provided by fabricating the antenna device 210 where the width of the signal line 217 and the width of the gap between the signal line 217 and the grounding conductor 216 are adjusted. The antenna device 210 can be easily mounted to a circuit board by soldering or the like since the feed terminal 218 and the grounding terminals 219 and 220 are formed. Fig. 18 is a side view showing a second example of an antenna device not being part of the present invention. In Embodiment 4 shown by Fig. 18, elements corresponding to elements of the first example shown by Fig. 14 through Fig. 17, are attached with the same notations. On the upper face of the dielectric base body 211 constituting an antenna device 250 as shown by Fig. 18, the loop conductor 214 and the coupling line 215 the same as those on the upper face (refer to Fig. 15) of the antenna device 210 shown by Fig. 14 through Fig. 17, are provided and the monopole conductor 213 is filled in the through hole 212 of the dielectric base body 211. Further, the grounding conductor 216 is extended on the lower face of the dielectric base body 211 except a portion of the lower end of the monopole conductor 213. According to the antenna device 250, a coaxial connector 253 is fixed to the lower face of the dielectric base body 211. The coaxial connector 253 is provided with a central conductor 251 and a grounding conductor 252, the central conductor 251 is inserted into the through hole 212 of the dielectric base body 211 and is connected to the monopole conductor 213 and the grounding conductor 252 is extended in a planar shape and is connected to the grounding conductor 216 formed on the lower face of the dielectric base body 211. Since the antenna device 250 is provided with the coaxial connector 253, the antenna device 250 is connected to a circuit board or the like via a coaxial cable, not illustrated, coupled to the coaxial connector 253. An explanation will be given of a procedure of fabricating the antenna device 210 shown by Fig. 14 through Fig. 17 in reference to Fig. 14, Fig. 19, Fig. 20 and Fig. 21. Fig. 19, Fig. 20 and Fig. 21 show dimensions of patterns printed on an upper face, a bottom face and a side face of a dielectric substrate, respectively. An explanation will be given thereafter of a result provided by measuring the gain of the antenna device 210. First, a material of dielectric base body 211 is selected. A material where the dielectric constant is stabilized to substantially 10 through 100 in a frequency band of transmitted and received electromagnetic wave is preferably used as the material of the dielectric base body 211 and in this case, a Sr(Ni 1/3 Nb 2/3 )O 3 group ceramic is selected. According to the material, the dielectric constant is 31 when the frequency of transmitted and received electromagnetic wave is 3.8 GHz and the Q value is 1800. Next, the dimensions of the film-like loop conductor 214, the dimensions of the signal line 217 and the width of the gaps 231, 232 and 233 between the signal line 217 and the grounding conductor 216, are determined. These values are determined as follows. When the length of the loop conductor 214 is designated by notation λ, λ can be represented by Equation (4). Equation (4) is shown below. λ = λ 0 / (ε reff ) where λ 0 is wavelength of electromagnetic wave in vacuum and ε reff is effective dielectric constant. Further, the effective dielectric constant ε reff can be represented by the following equation in consideration of the fact that the electromagnetic wave radiated from the film-like loop conductor 214 as shown by Fig. 14, is propagated perpendicularly to the face of the dielectric base body 211 where the film-like loop conductor 214 is formed and electric fields are generated on the inner side and the outer side of the loop conductor 214. ε reff = ( ε r + 3) /4 where ε r is dielectric constant of dielectric substrate. Accordingly, λ can be calculated by calculating the effective dielectric constant ε reff by using Equation (6) and substituting the calculated value of ε reff for Equation (5). In this case, the resonance frequency of electromagnetic wave is set to 1.9 GHz and accordingly, λ is determined as λ=54.11 mm and in order to form the loop conductor 214 as shown by Fig. 14, the length of a side of the loop conductor 214 is determined to be 13.54 mm as shown by Fig. 19. Here, the broken line shown in Fig. 19 designates center lines of the respective sides of the loop conductor 214. Although the impedance of a single wavelength loop antenna is generally as high as 100 Ω or higher, the impedance can be lowered by adjusting the width of the loop conductor and an interval between the two ends of the loop conductor by which the electricity feed efficiency can be promoted. Here, in order to set the impedance to 50 Ω, the width of the loop conductor 214 is determined to be 2 mm and the interval between two ends 214a and 214b is determined to be 1 mm as shown by Fig. 19. Further, as shown by Fig. 14, the signal line and the grounding conductor constitute the coplanar lines and therefore, line impedance can be adjusted by adjusting the width of the signal line and the width of the gap between the signal line and the grounding conductor. In this case, in order to set the line impedance to 50 Ω, the width of the signal line is set to 1 mm and all of the widths of the gaps 231, 232 and 233 are determined to be 3.02 mm as shown by Fig. 20. Next, both of the length and the width of the dielectric base body 211 are determined to be 15.54 mm in accordance with the dimensions of the loop conductor 214 determined as described above. The thickness of the dielectric base body 211 is determined to be 7.09 mm corresponding to a quarter of a length of electromagnetic wave having the resonance frequency of 1.9 GHz in the dielectric base body 211. Thereby, the dielectric base body 211 having the above-described dimensions and having the through hole 212 having the diameter of 1 mm in the thickness direction of the dielectric base body, is fabricated. Next, respective patterns of the film-like loop conductor 214, the signal line 218, the coupling line 215, the grounding conductor 216, the feed terminal 218 and the ground terminals 219 and 220 are printed by the thick film printing process by using a copper paste. The film-like loop conductor is printed to have the above-described dimensions whereas the coupling line 215 is printed with the width of 1 mm as shown by Fig. 19, the grounding conductor 216 is printed with the width of 4.25 mm as shown by Fig. 20, the feed terminal 218 is printed with the width and the length of 1 mm as shown by Fig. 21, and the ground terminals 219 and 220 are printed with the width and the length of 1 mm and 4.25 mm, respectively, as shown by Fig. 21. Further, a copper paste is filled in the through hole 212 of the dielectric base body 211. Next, the dielectric base body 211 where a copper paste is printed and filled as mentioned above, is sintered in a reducing atmosphere. In this way, the antenna device 210 shown by Fig. 14 was fabricated. Next, an explanation will be given of the gain characteristic of the antenna device 210 fabricated as described above in reference to Fig. 22 and Fig. 23. Here, as the gain characteristic of the antenna device 210, as shown by Fig. 22, the gain characteristic in a plane 291 in parallel with the side face of the antenna device 210 where the feed terminal 218, and the ground terminals 219 and 220 are formed, and including the monopole conductor 213, is obtained. Further, X-axis, Y-axis and Z-axis shown by Fig. 22 intersect with each other by 90°, X-axis is an axis included in the plane 291 and in parallel with the loop face of the loop conductor 214, Y-axis is an axis perpendicular to the face 291 and Z-axis is an axis included in the plane 291 and directed in a direction the same as a direction of extending the monopole conductor 213. Further, an arrow mark W is an arrow mark with a point of intersection of X-axis, Y-axis and Z-axis as an origin and included in the plane 291 and angle  is an angle made by the arrow mark W and Z-axis. X-axis, Z-axis and angle  shown in Fig. 23, explained below, respectively correspond to X-axis, Z-axis and angle  shown by Fig. 22. Further, a direction directing from the center of Fig. 23 perpendicularly to paper face and directing to this side, corresponds to Y-axis shown by Fig. 22. Fig. 23 is a diagram showing the gain characteristic of the antenna device and the bold line designates the gain in a direction designated by the arrow mark in a range of 0°≤≤360° in the face 291 shown by Fig. 22 of the antenna device 210 shown by Fig. 14 which has been fabricated after being subjected to the above-described fabrication procedure and the broken line shows the gain in a direction the same as the direction designated by the arrow mark W in the range of 0°≤≤360° shown by Fig. 22 in an antenna device having only the single wavelength loop antenna structure provided by the antenna device 210 shown by Fig. 14. As shown by Fig. 23, the maximum gain 26 dB is indicated when =0° in either of the antenna devices, however, in the range of  of 30° through 90° or 270° through 330°, the antenna device shown by Fig. 14 has a higher gain and particularly, in the range of  of 270° through 300°, the antenna device shown by Fig. 14 has a gain 5 dB or more higher than the gain of the antenna device having only the loop antenna structure. In this way, it is known that the antenna device 210 shown by Fig. 14 is provided with the gain higher than that of the antenna device having only the loop antenna structure. Fig. 24 is a perspective view showing an antenna device according to Embodiment 3 of the present invention and Fig. 25 is a bottom view thereof. An antenna device 310 shown by Fig. 24 is provided with the dielectric base body 311 in a rectangular parallelepiped shape having an upper face of a square shape and a lower face of a square shape, a grounding conductor film 312 extending in a planar shape is formed on the lower face of the dielectric base body 311 as shown by Fig. 25 and the grounding conductor film 312 is provided with the shape where a portion of a side is notched. As shown by Fig. 24, two adjacent left and right ends 313a and 313b are provided to a side face of the dielectric base body 311 and a radiating conductor film 313 connecting the two ends 313a and 313b by making a turn on side faces along four sides of the upper face of the dielectric base body 311. The length of the radiating conductor film 313 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission. Further, two feeding conductor films 314 and 315 which are extended in the up and down direction in parallel to each other, one of which is connected to the one end 313a in the two ends 313a and 313b of the radiating conductor film 313 and the other one of which is connected to the end 313b, are formed at the side face of the dielectric base body 311. The feeding conductor film 315 is connected to the grounding conductor film 312 and the feeding conductor film 314 reaches the lower face of the dielectric base body 311 as shown by Fig. 25. Further, portions of the feeding conductor films 314 and 315 on the side of the grounding conductor film 312, also serves as feed electrodes 316 and 317 which are electrodes in mounting to the surface of a circuit board. Since the antenna device 310 constituted as described above, is provided with the radiating conductor film 313 having a single wavelength loop antenna structure, when electric current is supplied to the radiating conductor film 313 via the feed electrode 316, electromagnetic wave having the maximum gain is radiated from the radiating conductor film 313 perpendicularly to the upper face of the dielectric base body 311 and electromagnetic wave progressing toward the grounding conductor film 312 is reflected by the grounding conductor film 312. That is, the electromagnetic wave having the maximum gain is radiated from the antenna device 310 perpendicularly to the plane including the radiating conductor film 313 and in a direction directing from the grounding conductor film 312 to the radiating conductor film 313. Accordingly, the antenna device which has high gain and in which radiated electromagnetic wave is efficiently used in communication, is provided. Further, it is not necessary to form a through hole in the dielectric base body 311 and accordingly, reduction in fabrication cost can be achieved. An explanation will be given of the fabrication method of the antenna device 310 having the structure shown by Fig. 24 and Fig. 25 in reference to Fig. 26 indicating dimensions of the dielectric base body, the radiating conductor film and the feeding conductor film. First, a material of the dielectric base body 311 is selected. A material in which the dielectric constant is stabilized to substantially 10 through 100 in a frequency band of transmitted and received electromagnetic wave, is preferably used as the material of dielectric base body 311. For example, a Sr(Ni 1/3 Nb 2/3 )O 3 group ceramic is preferable. The dielectric constant of the material is 31 when the frequency of transmitted and received electromagnetic wave is 4 GHz and the Q value is 1000. Next, dimensions of the radiating conductor film 313, the feeding conductor films 314 and 315 and the dielectric base body 313 are determined. These dimensions can be determined as follows. When the length of the radiating conductor film 313 is designated by notation λ, λ can be represented by Equation (4) mentioned above. Equation (4) is shown as follows. λ = λ 0 / (ε reff ) where λ 0 is wavelength of electromagnetic wave in vacuum and ε reff is effective dielectric constant. Further, the effective dielectric constant ε reff can be represented by the following equation in consideration of the fact that electromagnetic wave radiated from the radiating conductor film 313 as shown by Fig. 26 is propagated perpendicularly to the upper face of the dielectric base body 311 and electric fields are generatedo n the inner side and the outer side of the radiating conductor film 313. ε reff = (ε r + 3)/4 where ε reff is dielectric constant of dielectric base body. Accordingly, λ can be calculated by calculating the effective dielectric constant ε reff by Equation (8) and substituting the calculated value of ε reff for Equation (7). When the resonance frequency of electromagnetic wave is set to 1.9 GHz, λ is determined as λ=54.16 mm and the length of a side of the radiating conductor film 313 is set to 13.54 mm in order to form the radiating conductor film extending along four sides of the upper face in a square shape of the dielectric base body 311 as shown by Fig. 26. Further, although the impedance of a single wavelength loop antenna is generally as high as 100 Ω or higher, the impedance can be lowered by adjusting the width of the radiating conductor film and the interval between two ends of the radiating conductor film by which the electricity .feed efficiency can be promoted. For example, in order to set impedance to 50 Ω, a width of the radiating conductor film 313 is set to 2 mm and the interval between the two ends is set to 0.5 mm as shown by Fig. 26. Both of the length and the width of the dielectric base body 311 is set to 13.54 mm in accordance with the dimensions of the radiating conductor film 313 determined as described above. Further, the thickness of the dielectric base body 311 is determined as follows. The efficiency of the antenna device having the loop antenna structure as shown by Fig. 26, is maximized when the distance between the radiating conductor film and the grounding conductor film formed on the lower face of the conductor base body, is a distance corresponding to a quarter of the resonance wavelength of electromagnetic wave in the dielectric base body. Accordingly, when the resonance frequency of electromagnetic wave is set to 1.9 GHz, the distance between the radiating conductor film and the grounding conductor film for maximizing the efficiency of the antenna device, is set to 7.09 mm corresponding to a quarter of the resonance wavelength of electromagnetic wave having the resonance frequency of 1.9 GHz in the dielectric base body as-shown by Fig. 26. Here, the one-dotted chain line as shown by Fig. 26 designates centers of respective sides of radiating conductor film 313. Further, since the width of the radiating conductor film 313 is set to 2 mm as shown by Fig. 26, the thickness of the dielectric base body 311 is determined as 8.09 mm. Accordingly, the length, the width and the thickness of the dielectric base body 311 are respectively 13.54 mm, 13.54 mm and 8.09 mm. Further, the desired transmission impedance is obtained by adjusting the width of the feeding conductor film and the interval between the feeding conductor films. In this case, both of the widths of the feeding conductor films 314 and 315 are set to 0.97 mm and the interval between the feeding conductor films 314 and 315 is set to 0.5 mm as shown by Fig. 26 in order to set the transmission impedance to 50 Ω. Next, the dielectric base body 311 having the above-described dimensions is fabricated, patterns of the grounding conductor film 312, and the radiating conductor film 313 and the two feeding conductor films 314 and 315 both having the above-described dimensions, are printed on the dielectric base body 311 by the thick film printing process by using a copper paste and sintered in a reducing atmosphere. In this way, the antenna device 310 is fabricated. Fig. 27 is a view showing an antenna device according to Embodiment 4 of the present invention. A dielectric base body 341 having a cylindrical shape is adopted in an antenna device 340 shown by Fig. 27 in place of the dielectric base body 311 in a rectangular parallelepiped shape of the antenna device 310 shown by Fig. 24 and Fig. 25 whereby with respect to a radiating conductor film, a radiating conductor film 343 in a circular loop shape is formed and with respect to a grounding conductor film, a circular grounding conductor film 342 is formed. As described above, the dielectric base body may be in a cylindrical shape. Fig. 28 is a view showing a state where the antenna device shown by Fig. 24 and Fig. 25 is mounted on a circuit board. A feed line 352 and a grounding conductor layer 353 are formed on the surface of a circuit board 351 and pairs of the feed line 352 and the feed electrode 316 of the antenna device 310, and the grounding conductor layer 353 and the feed electrode 317 of the antenna device 310, are connected to each other respectively by solders 354. In this way, the antenna device 310 is mounted to the circuit board 351. Fig. 29 is a perspective view showing Embodiment 5 of an antenna device according to the present invention, Fig. 30 is a top view thereof, Fig. 31 is a bottom view thereof and Fig. 32 is a side view thereof. A radiating conductor film 412 having two left and right adjacent ends 412a and 412b and connecting the two ends 412a and 412b by making a turn in a loop-like shape on a horizontal face as shown by Fig. 30, is formed at the inside of a dielectric base body 411 in a rectangular parallelepiped shape constituting an antenna device 410 shown by Fig. 29 and the length of the radiating conductor film 412 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission in the dielectric base body 411. Further, inner feeding conductor films 413 and 414 connected respectively to the two ends 412a and 412b of the radiating conductor film 412 and exposed on a side face of the dielectric base body 411, are formed in a plane including the radiating conductor film 412 at the inside of the dielectric base body 411. A gap 415 is provided between the inner feeding conductor films 413 and 414 and coplanar lines are formed therebetween. As shown by Fig. 31, a grounding conductor film 416 is formed on the lower face of the dielectric base body 411 and the grounding conductor film 416 is provided with a shape where a portion of a side is notched. As shown by Fig. 32, side feeding conductor films 418 and 419 forming coplanar lines therebetween, which are extended in the up and down direction in parallel to each other to constitute a gap 417 therebetween and which are respectively connected to portions of the inner feeding conductor films 413 and 414 exposed on the side face as shown by Fig. 29, are formed on the side face of the dielectric base body 411. One of the side face feeding conductor films 418 and 419, or the side face feeding conductor film 419 is connected also to the grounding conductor film 416 and the other one thereof, or the side face feeding conductor film 418 reaches the lower face of the dielectric base body 411. Further, portions of the side face feeding conductor films 418 and 419 on the side of the grounding conductor film 416, also serve as feed electrodes 420 and 421 which are electrodes in mounting to the surface of a circuit board. The antenna device 410 constituted as described above, is provided with the radiating conductor film 412 having a single wavelength loop antenna structure and therefore, when electric current is supplied to the radiating conductor film 412 via the feed electrode 420, electromagnetic wave having the maximum gain is radiated from the radiating conductor film 412 in a direction perpendicular to a plane including the radiating conductor film 412 and electromagnetic wave progressing toward the grounding conductor film 416 is reflected by the grounding conductor film 416. That is, the electromagnetic wave having the maximum gain is radiated from the antenna device 410 in a direction directing from the grounding conductor film 416 to the radiating conductor film 412. Accordingly, the antenna device which has high gain and in which radiated electromagnetic wave is efficiently used in communication, is obtained. Further, the antenna device 410 is provided with the inner feeding conductor films 413 and 414 forming coplanar lines therebetween and the side face feeding conductor films 418 and 419 forming coplanar lines therebetween and a desired transmission impedance can be provided by fabricating the antenna device 410 where the widths of the respective inner feeding films 413 and 414, the widths of the side face feeding conductor films 418 and 419, the gap width of the gap 415 between the inner feeding conductor films 413 and 414, the gap width of the gap 417 between the side face feeding conductor films 418 and 419 and the like are adjusted. According to the antenna device 410, the radiating conductor film 412 is formed at the inside thereof whereby downsizing can be realized. Also, the portions of the feeding conductor films 418 and 419 on the side of the grounding conductor film 416, also serve as the feed electrodes 420 and 421, respectively, and therefore, they can easily be mounted onto a circuit board by soldering or the like. An explanation will be given of the fabrication method of the antenna device 410 shown by Fig. 29 in reference to Fig. 29, Fig. 33 and Fig. 34. Fig. 33 is a top view of the antenna device 410 showing the length and the width of the dielectric base body and the dimensions of the radiating conductor film and the inner feeding conductor films and Fig. 34 is a side view of the antenna device 410 showing the thickness of the dielectric base body and the dimensions of the side face feeding conductor films. First, the material of the dielectric base body 411 is selected. A material in which the dielectric constant is stabilized to substantially 10 through 100 in a frequency band of transmitted and received electromagnetic wave, is preferably used as the material of the dielectric base body 411. Further, according to the antenna device 410, the radiating conductor film 412 is formed at the inside of the dielectric base body 411 as shown by Fig. 29 and therefore, a material capable of being sintered at low temperatures is preferable. For example, a material of a Sr(Ni 1/3 Nb 2/3 )O 3 group ceramic added with glass is preferable. According to the material, the dielectric constant is 25 when the frequency of transmitted and received electromagnetic wave is 6 GHz, the Q value is 1000 and the sintering temperature is 1000 °C. Next, the dimensions of the radiating conductor film 412, the inner feeding conductor films 413 and 414, the side face feeding conductor films 418 and 419 and the dielectric base body 411 are determined. These dimensions are determined as follows. When the length of the radiating conductor film 412 is designated by notation λ, λ can be represented by the above-described Equation (4). Equation (4) is shown below. λ = λ 0 / (ε reff ) where λ 0 is wavelength of electromagnetic wave in vacuum and ε reff is effective dielectric constant. According to the antenna device 410, ε reff coincides with the dielectric constant ε r of the dielectric base body 411 since the radiating conductor film 412 is formed at the inside of the dielectric base body 411. Accordingly, λ is represented by the following equation. λ = λ 0 / (ε r ) When the resonance frequency of electromagnetic wave is set to 1.9 GHz, λ is determined as λ=31.56 mm and in order to form the radiating conductor film 412 shown by Fig. 33, the length of one of sides of the radiating conductor film 412 is set to 7.89 mm. Here, the one-dotted chain line shown by Fig. 33 designates center lines of the respective sides of the radiating conductor film 412. Further, although impedance of a single wavelength loop antenna is generally as high as 100 Ω or higher, the impedance is lowered by adjusting the width of the radiating conductor film and the interval between the two ends of the radiating conductor film by which the electricity feed efficiency can be promoted. For example, in order to set the impedance to 50 Ω, the width of the radiating conductor film is set to 2 mm and the interval between the two ends is set to 0.4 mm as shown by Fig. 33. In order to form the radiating conductor film of which dimensions have been determined as described above such that, for example, a distance from the side face of the dielectric base body 411 to an outer peripheral edge of the radiating conductor film 412 is set to 1 mm as shown by Fig. 33, both of the length and the width of the dielectric base body 411 are set to 11.89 mm. Further, the thickness of dielectric base body is determined as follows. The gain of the antenna device having the loop antenna structure as shown by Fig. 29, is maximized when a distance between the radiating conductor film and the grounding conductor film formed on the lower face of che dielectric base body, is a distance corresponding to a quarter of the resonance wavelength of electromagnetic wave which is an object of transmission and receiving in the dielectric base body. Accordingly, when the resonance frequency of the electromagnetic wave is set to 1.9 GHz, in order to maximize the gain of the antenna device, the distance between the radiating conductor film and the grounding conductor film is set to 7.89 mm corresponding to a distance of a quarter of the resonance wavelength of the electromagnetic wave having the resonance frequency of 1.9 GHz in the dielectric base body as shown by Fig. 34. When the radiating conductor film 412 is formed such that, for example, the distance between the radiating conductor film 412 to the upper face of the dielectric base body 411 is set to 2 mm, the thickness of the dielectric base body is set to 9.89 mm as shown by Fig. 34. That is, the length, the width and the thickness of the dielectric base body 411 are respectively set to 11.89 mm, 11.89 mm and 9.89 mm. Further, a desired transmission impedance is obtained by adjusting the width of the inner feeding conductor film, the gap width of the gap between the inner feeding conductor films, the width of the side face feeding conductor film and the gap width of the gap between the side face feeding conductor films. For example, in order to set the transmission impedance to 50 Ω, both of the widths of the inner feeding conductor films 413 and 414 are set to 0.35 mm and the gap width of the gap 415 is set to 0.40 mm as shown by Fig. 33 and both of the widths of the side face feeding conductor films 418 and 419 are set to 1.69 mm and the gap width of the gap 417 is set to 0.40 mm as shown by Fig. 34. Next, patterns of the radiating conductor film 412 and the inner feeding conductor films 413 and 414 having the above-described dimensions are printed at the inside of the dielectric base body 411 having the above-described dimensions by the thick film printing process by using a copper paste, patterns of the side face feeding conductor films 418 and 419 having the above-described dimensions are printed on the side face of the dielectric base body 411 by the thick film printing process by using a copper paste, and patterns of the feed electrode 420 and the grounding conductor film 416 are printed on the lower face of the dielectric base body 411 by the thick film printing process by using a copper paste, and the assemblage is sintered in a reducing atmosphere. The antenna device 410 is fabricated in this way. Fig. 35 is a view showing an antenna device according to Embodiment 6 of the present invention. A dielectric base body 471 in a cylindrical shape is adopted in an antenna device 470 shown by Fig. 35 in place of the dielectric base body 411 in a rectangular parallelepiped shape of the antenna device 410 shown by Fig. 29 through Fig. 32 whereby with respect to a radiating the conductor film, a radiating conductor film 472 in a circular loop shape is formed and with respect to a grounding conductor film, a circular grounding conductor film 476 is formed. As described above, the dielectric base body may be in a cylindrical shape. Fig. 36 is a view showing a state where the antenna device shown by Fig. 29 through Fig. 32 is mounted on a circuit board. A feed line 482 and a grounding conductor layer 483 are formed on the surface of a circuit board 481 and pairs of the feed line 482 and the feed electrode 420 of the antenna device 410, and the grounding conductor layer 483 and the feed electrode 421 of the antenna device 410 are respectively connected to each other by solders 484. In this way, the antenna device 410 is mounted onto the circuit board 481. Fig. 37 is a perspective view showing an antenna device of Embodiment 7 of the present invention, Fig. 38 is a top view thereof, Fig. 39 is a sectional view taken from a line A-A' of Fig. 37, Fig. 40 is a bottom view thereof, Fig. 41 is a view showing a side face of the antenna device shown by Fig. 37 where first feeding conductor films are formed and Fig. 42 is a view showing a side face of the antenna device shown by Fig. 37 where second feeding conductor films are formed. An antenna device 510 shown by Fig. 37 is provided with a dielectric base body 511 in a rectangular parallelepiped shape having an upper face and a lower face in a square shape. A first loop radiating conductor film 513 is formed on the upper face of the dielectric base body 511 to extend along four sides of the upper face. The first loop radiating conductor film 513 makes a turn on the upper face to form two ends 513a and 513b opposed to each other via a first gap 512 as shown by Fig. 38 and the length of the loop is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission and receiving. Further, a second loop radiating conductor film 515 which makes a turn on a horizontal face in a square shape, is formed at the inside of the dielectric base body 511. As shown by Fig. 39, the second loop radiating conductor film 515 makes a turn on a horizontal plane to form two ends 515a and 515b opposed to each other via a gap 514. As shown by Fig. 37, the direction of the second gap 514 in respect of the loop of the second loop radiating conductor film 515, is adjusted in a direction that is different from the direction of the first gap 512 in respect of the loop of the first loop radiating film 513 by 90° in the horizontal plane. Further, the length of the loop of the second loop radiating conductor film 515 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission and receiving in the dielectric base body 511. As shown by Fig. 40, a grounding conductor film 516 is formed on the lower face of the dielectric base body 511 and is provided with a shape where portions of respective two sides in the four sides of the film are notched. As shown by Fig. 41, two of first feeding conductor films 518 and 519 opposed to each other via a gap 517, are formed on one of four side faces of the dielectric base body 511. As shown by Fig. 42, two of second feeding conductor films 521 and 522 opposed to each other via a gap 520 are formed on other one of the four side faces. As shown by Fig. 37, the two first feeding conductor films 518 and 519 shown by Fig. 41 are respectively connected to the two ends 513a and 513b of the first loop radiating conductor film 513, extended in parallel with each other via the side face of the dielectric base body 511. The feeding conductor film 519 that is one of the two feeding conductor films 518 and 519, is connected to the grounding conductor film 516 and the other one of the feeding conductor film 518 reaches the lower face of the dielectric base body 511. Further, portions of the two feeding conductor films 518 and 519 on the side of the grounding conductor film 516, also serve as feed electrodes 518a and 519a which are electrodes for mounting to the surface of a circuit board, respectively. Meanwhile, as shown by Fig. 37, similar to the first feeding conductor films 518 and 519, the two second feeding conductor films 521 and 522 shown by Fig. 42, are respectively connected to two ends 515a and 515b of the second loop radiating conductor film 515 and extended in parallel with each other via the side face of the dielectric base body 511. The feeding conductor film 522 that is one of the two feeding conductor films 521 and 522, is connected to the grounding conductor film 516 and the other one of the feeding conductor film 521 reaches the lower face of the dielectric base body 511. Also, portions of the two feeding conductor films 521 and 522 on the side of the grounding conductor film 516, also serve as feed electrodes 521a and 522a which are electrodes for mounting onto the surface of a circuit board, respectively. According to the antenna device 510 constituted as described above, the first loop radiating conductor film 513 and the second loop radiating conductor film 515, the directions of the gaps of which are different from each other by 90° with respect to a horizontal face, are formed and therefore, polarized wave directions of electromagnetic wave received by the first and the second loop radiating conductor films 513 and 515, are different from each other by 90° on the horizontal plane. Accordingly, electromagnetic wave can efficiently be received by the antenna device 510 irrespective of whether the electromagnetic wave is a vertically polarized wave or a horizontally polarized wave. Also, according to the antenna device 510, portions of the first feeding conductor films 518 and 519 at a vicinity of the grounding conductor film 516 and portions of the second feeding conductor films 521 and 522 at a vicinity of the grounding conductor film 516, also serve as feed electrodes and therefore, the antenna device 510 can easily be mounted on a circuit board by soldering or the like. Incidentally, although according to the antenna device 510, with respect to the first and the second loop radiating conductor films 513 and 515, the direction of the gap of the first loop radiating conductor film 513 and the direction of the gap of the second loop radiating conductor film 515 are different from each other by 90° in respect of a horizontal face, the directions of the gaps may be different from each other by, for example, 45° and when the directions of the gaps are different from each other, electromagnetic waves having different polarized wave directions can be received by a single antenna. An explanation will be given of a fabrication method of an antenna device 510 shown by Fig. 37 through Fig. 42 in reference to Fig. 37 and Fig. 43 through Fig. 46. Fig. 43 is a top view of the antenna device 510 shown by Fig. 37 and is a view showing the length and the width of the dielectric base body and the dimensions of the first loop radiating conductor film. Fig. 44 is a sectional view taken from a line A-A' of the antenna device 510 shown by Fig. 37 and is a view showing the length and the width of the dielectric base body and the dimensions of the second loop radiating conductor film. Fig. 45 is a view showing a side face of the antenna device 510 where the first feeding conductor films are formed and is a view showing the thickness of the dielectric base body and the dimensions of the first feeding conductor films. Fig. 46 is a view showing a side face of the antenna device 510 where the second feeding conductor films are formed and is a view showing the thickness of the dielectric base body and the dimensions of the second feeding conductor film. First, the material of the dielectric base body 511 is selected. A material where the dielectric constant is stabilized to substantially 10 through 100 in a frequency band of transmitted and received electromagnetic wave, is preferably used as the material of the dielectric base body 511 and, for example, a Sr(Ni 1/3 Nb 2/3 )O 3 group ceramic is preferable. According to the material, the dielectric constant is 31 when the frequency of transmitted and received electromagnetic wave is 3.8 GHz and the Q value is 1800. Next, the dimensions of the first and the second loop radiating conductor films, the first and the second feeding conductor films and the dielectric base body, are determined. The dimensions can be determined as follows. When the lengths of the loops of the first and the second loop radiating conductor films 513 and 515 are respectively designated by notation λ 1 and λ 2 , λ 1 and λ 2 can be represented by Equation (4) described above, respectively. Equations for calculating respectively λ 1 and λ 2 are shown below. λ 1 = λ 0 / (ε reff-1 ) λ 2 = λ 0 / (ε reff-2 ) where λ 0 is wavelength of electromagnetic wave in vacuum and ε reff-1 and ε reff-2 are effective dielectric constants. Here, the effective dielectric constant ε reff-1 in Equation (11) can be represented by the following equation in consideration of the fact that the first loop radiating conductor film 513 is formed on the upper face of the dielectric base body 511, electromagnetic wave radiated from the first loop radiating conductor film 513 is radiated perpendicularly to a face of the dielectric base body 511 where the first loop radiating conductor film 513 is formed and electric fields are generated at the inside and the outside of the first loop radiating conductor film 513. ε reff-1 = (ε r +3)/4 where ε r is dielectric constant of dielectric base body. Further, the effective dielectric constant ε reff-2 in Equation (12) can be represented by the following equation in consideration of the fact that the second loop radiating conductor film 515 is formed at the inside of the dielectric base body 511, electromagnetic wave radiated from the second loop radiating conductor film 515 is radiated perpendicularly to a face of the dielectric base body 511 where the first loop radiating conductor film 513 is formed and electric fields are generated at the inside and the outside of the second loop radiating conductor film 515. ε reff-2 = (ε r +1)/2 where ε r is dielectric constant of dielectric base body. Accordingly, by substituting respectively the effective dielectric constants ε reff-1 and ε reff-2 calculated by Equation (13) and Equation (14) for Equation (11) and Equation (12), the lengths λ 1 and λ 2 of the first and the second loop radiating conductor films 513 and 515 can be calculated. When the resonance frequency of electromagnetic wave is set to 1.9 GHz, λ 1 and λ 2 are determined as λ 1 =54.16 mm and λ 2 =39.47 mm. As shown by Fig. 43 and Fig. 44, in forming the first and the second loop radiating conductor films 513 and 515, the length of each side of the first loop radiating conductor film 513 is determined to be 13.54 mm and the length of each side of the second loop radiating conductor film 515 is determined to be 9.87 mm. Here, the one-dotted chain lines shown in Fig. 43 and Fig. 44 designate center lines of the respective sides of the first and the second loop radiating conductor films 513 and 515. Further, although impedance of a single wavelength loop antenna is generally as high as 100 Ω or higher, the impedance can be lowered by adjusting the width of the loop radiating conductor film and the gap width of the gap between two ends of the loop radiating conductor film by which the electricity feed efficiency can be promoted. For example, in order to set the impedance to 50 Ω, as shown by Fig. 43 and Fig. 44, the widths of the loop radiating conductor films are set to 1 mm and the gap widths are set to 0.6 mm. As shown by Fig. 43 and Fig. 44, both of the length and the width of the dielectric base body 511 are set to 14.54 mm in accordance with the dimensions of the radiating conductor films which have been determined as described above. Further, with respect to the thickness of the dielectric base body 511, the thickness of the dielectric base body 511 is set to 14.18 mm as shown by Fig. 45 and Fig. 46 in order to set both of a distance from the first loop radiating conductor film 513 to the second loop radiating conductor film 515 and a distance from the second loop radiating conductor film 515 to the grounding conductor film 516, to 7.09 mm corresponding to a quarter of the resonance wavelength of electromagnetic wave having the resonance frequency of 1.9 GHz in the dielectric base body. Further, a desired line impedance can be provided by adjusting the widths of the feeding conductor films and the gap widths of the gap between the feeding conductor films. For example, in order to set the line impedance to 50 Ω, as shown by Fig. 45 and Fig. 46, the widths of the feeding conductor films are set to 1.16 mm and the gap lengths are set to 0.6 mm. Next, the dielectric base body 511 having the above-described dimensions is fabricated. The loop radiating conductor film is formed also at the inside of the dielectric base body 511 as shown by Fig. 37 and therefore, two pieces of dielectric materials each having the length, the width and the thickness of 14.54 mm, 14.54 mm and 7.09 mm, respectively, are fabricated and the two dielectric materials are laminated thereby forming the dielectric base body 511. Next, a pattern of the first loop radiating conductor film 513 having the dimensions shown by Fig. 43, is printed on an upper face of one of the fabricated two dielectric materials by the thick film printing process by using a copper paste. Further, a pattern of the second loop radiating conductor film 515 having the dimensions shown by Fig. 44 is printed on an upper face of the other dielectric material by the thick film printing process by using a copper paste and further, a pattern of the grounding conductor film 516 is printed on a lower face of the other dielectric material by the thick film printing process by using a copper paste. Furthermore, patterns of the first and the second feeding conductor films having the dimensions shown by Fig. 45 and Fig. 46 are printed on the side faces of the respective dielectric materials by the thick film printing process by using a copper paste. Thereafter, the dielectric materials printed with the respective patterns are laminated, dried and sintered in a reducing atmosphere. In this way, the antenna device 510 is fabricated. Fig. 47 is a perspective view showing an antenna device according to Embodiment 8 of the present invention. An antenna device 640 shown by Fig. 47 is provided with a dielectric base body 641 in a rectangular parallelepiped shape having an upper face and a lower face in a square shape. Four radiating conductor films 642, 643, 644 and 645 are formed on the upper face of the dielectric base body 641 to extend along the respective sides of the upper face. The radiating conductor films 642, 643, 644 and 645 are extended in the horizontal direction, contiguous ends thereof are opposed to each other via gaps 646, 647, 648 and 649 and the radiating conductor films make a turn as a whole by forming the four gaps 646, 647, 648 and 649 at equal intervals. The length of a total of the radiating conductor films 642, 643, 644 and 645 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission and receiving. Further, a grounding conductor film 650 is formed on the lower face of the dielectric base body 641 and the grounding conductor film 650 has a shape where the respective corners are notched. Feeding conductor films 651, 652, 653, 654, 655, 656, 657 and 658 are formed on side faces of the dielectric base body 641 along sides of the side faces extending in the up and down direction. The feeding conductor films 651 and 652 are connected to respective ends of the radiating conductor film 642, the feeding conductor films 653 and 654 are connected to respective ends of the radiating conductor film 643, the feeding conductor films 655 and 656 are connected to respective ends of the radiating conductor films 644, and the feeding conductor films 657 and 658 are connected to respective ends of the radiating conductor film 645. Portions of the respective feeding conductor films 651, 652, 653, 654, 655, 656, 657 and 658 on the lower end sides, respectively serve as feed electrodes 651a, 652a, 653a, 654a, 655a, 656a, 657a and 658a. Further, two ground electrodes 659 and 660 are formed at the lower portions of the side faces of the dielectric base body 641 and both of the ground electrodes 659 and 660 are connected to the grounding conductor film 650. According to the antenna device 640 constituted as described above, the four radiating conductor films 642, 643, 644 and 645 having a single wavelength loop antenna structure as a whole, are formed. Therefore, when electric currents having the same amplitude and the same phase are supplied to the radiating conductor films 642, 643, 644 and 645 via the feed electrodes 656a, 657a, 652a and 653a, electromagnetic waves having a directivity in a direction perpendicular to the upper face of the dielectric base body 641 and polarized in a direction in which a straight line connecting the gap 649 and the gap 647 is extended, are radiated from the four radiating conductor films 642, 643 644 and 645. Meanwhile, when electric currents having the same amplitude and the same phase are supplied to the radiating conductor films 642, 643, 644 and 645 via the feed electrodes 658a, 651a, 654a and 655a, electromagnetic waves having a directivity in a direction perpendicular to the upper face of the dielectric base body 641 and polarized in a direction in which a straight line connecting the gap 648 and the gap 646 is extended, are radiated from the four radiating conductor films 642, 643, 644 and 645. Accordingly, the antenna device capable of freely switching the polarizing direction is provided. According to the antenna device 640, the four radiating conductor films 642, 643, 644 and 645 having a single wavelength loop antenna structure as a whole, are formed and therefore, the electromagnetic waves radiated from the four radiating conductor films 642, 643, 644 and 645, are electromagnetic waves having the maximum gain in a direction perpendicular to a plane including the four radiating conductor films 642, 643, 644 and 645. Further, the grounding conductor film 650 is formed on the lower face of the dielectric base body 641 and therefore, electromagnetic waves progressing toward the grounding conductor film 650 among the electromagnetic waves radiated from the four radiating conductor films 642, 643, 644 and 645, are reflected by the grounding conductor film 65. That is, electromagnetic waves having the maximum gain are radiated from the antenna device 640 in a direction from the grounding conductor film 650 toward the four radiating conductor films 642, 643, 644 and 645. Accordingly, when the antenna device 640 is attached to, for example, a portable telephone, if the grounding conductor film 650 is disposed between a person and the four radiating conductor films 642, 643, 644 and 645 when the person uses the portable telephone, electromagnetic waves are not radiated toward the side of the person and the electromagnetic waves can efficiently be used in communication with a maximum gain in a direction from the grounding conductor film 650 to the four radiating conductor films 642, 643, 644 and 645. An explanation will be given of the fabrication method of the antenna device 640 shown by Fig. 47. First, the material of the dielectric base body 641 is selected. A material in which the dielectric constant is stabilized to substantially 10 through 100 in a frequency band of transmitted and received electromagnetic wave, is preferably used as the material of the dielectric base body 641 and, for example, a Sr(Ni 1/3 Nb 2/3 )O 3 group ceramic is preferably used. According to the material, the dielectric constant is 31 when the frequency of transmitted and received electromagnetic wave is 4 GHz and the Q value is 1000. Next, the dimensions of the radiating conductor films 642, 643, 644 and 645 are determined. The dimensions are determined as follows. When the length of the loop formed by the four radiating conductor films 642, 643, 644 and 645 is designated by notation λ, λ can be represented by Equation (4). Equation (4) is shown as follows. λ = λ 0 / (ε reff ) where λ 0 is wavelength of electromagnetic wave in vacuum and ε reff is effective dielectric constant. Further, the effective dielectric constant ε reff can be represented by the following equation in consideration of the fact that electromagnetic waves radiated from the four radiating conductor films 642, 643, 644 and 645 as shown by Fig. 47, are radiated perpendicularly to the face where the four radiating conductor films 642, 643, 644 and 645 are formed and electric fields are generated on the inner sides and the outer sides of the four radiating conductor films 642, 643, 644 and 645. ε reff = (ε r +3)/4 where ε r is dielectric constant of dielectric base body. Accordingly, the effective dielectric constant ε reff is calculated by Equation (16) and λ can be calculated by substituting the calculated value of ε reff for Equation (15). When the resonance frequency of electromagnetic wave is set to 1.9 GHz, λ is determined as λ=54.16 mm and in order to form the radiating conductor films as shown by Fig. 47, the lengths of the respective radiating conductor films 642, 643, 644 and 645 are set to 13.54 mm. Further although the impedance of a single wavelength loop antenna is generally as high as 100 Ω or higher, impedance can be lowered by adjusting the widths of the radiating conductor films and the gap widths of the gaps between the respective radiating conductor films by which the electricity feed efficiency can be promoted. For example, in order to set the impedance to 50 Ω, the widths of the respective radiating conductor films are set to 2 mm and the gap widths of the respective gaps are set to 0.5 mm. Next, in respect of the dimensions of the dielectric base body 641, both of the length and the width are set to 15.54 mm from the dimensions of the radiating conductor films which have been determined as described above and the thickness is set to 7.09 mm corresponding to a quarter of the wavelength of electromagnetic wave having the resonance frequency of 1.9 GHz in the dielectric base body thereby fabricating the dielectric base body. Next, patterns of the feeding conductor films, the grounding conductor film, the ground electrodes and the radiating conductor films having the above-described dimensions, are printed by the thick film printing process by using a copper paste and are sintered in a reducing atmosphere. The antenna device 640 shown by Fig. 47 is fabricated after being subjected to such a fabrication procedure. Fig. 48 is a view showing a drive circuit driving the antenna device shown by Fig. 47. A drive circuit 670 is provided with two power sources 671 and 672, the power source 671 supplies current to four terminals 673, 674, 675 and 676 and the power source 672 supplies current to four terminals 677, 678, 679 nd 680. When the terminals 673, 674, 675 and 676 of the drive circuit 670 are connected to the feed electrodes 656a, 657a, 652a, 653a of the antenna device 640 shown by Fig. 47, respectively whereas the terminals 677, 678, 679 and 680 of the drive circuit 670 are respectively connected to the feed electrodes 658a, 651a, 654a and 655a of the antenna device 640, the antenna capable of freely switching the polarized directions is obtained by deactivating the power source 672 when the power source 671 is operated and deactivating the power source 671 when the power source 672 is operated. Fig. 49 is a perspective view showing an antenna device according to Embodiment 9 of the present invention. According to the antenna device shown by Fig. 49, a dielectric base body 691 having a cylindrical shape is adopted in place of the dielectric base body 641 in a rectangular parallelepiped shape of the antenna device 640 shown by Fig. 47 whereby radiating conductor films 692, 693, 694 and 695 having a circular loop shape as a whole, are formed and a circular grounding conductor film 696 is formed for the grounding conductor film. As described above, the dielectric base body may have a cylindrical shape. Fig. 50 is a perspective view showing an antenna device according to Embodiment 10 of the present invention. An antenna device 700 shown by Fig. 50 is provided with a dielectric base body 701 in a rectangular parallelepiped shape having an upper face and a lower face in a square shape. A grounding conductor film 702 is formed on the lower face of the dielectric base body 701 and the grounding conductor film 702 is provided with a shape where the respective corners are notched. Four radiating conductor films 703 are formed at the upper portions of side faces of the dielectric base body 701 along respective sides of the top face of the dielectric base body 701. The radiating conductor films 703 are extended in the horizontal direction, contiguous ends thereof are opposed to each other via gaps and the radiating conductor films make a turn by forming the four gaps at equal intervals. The length of a total of the four radiating conductor films 703 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission and receiving. Eight feeding conductor films 704 are formed on side faces of the dielectric base body 701 along respective sides extending in the up and down direction and the respective feeding conductor films 704 are connected to respective ends of the radiating conductor films 703. Also, portions of the respective feeding conductor films 704 on the lower end sides, also serve as feed electrodes 704a. Ground electrodes 705 are formed to connect to the grounding conductor film 702 at the lower portions of the respective side faces of the dielectric base body 701. The radiating conductor films may be formed on the side faces of the dielectric base body in this way. Fig. 51 is a perspective view showing an antenna device according to Embodiment 11 of the present invention. An antenna device 710 shown by Fig. 51 is provided with a dielectric base body 711 in a rectangular parallelepiped shape having an upper face and a lower face in a square shape. Four radiating conductor films 712 in an L-like shape are formed on the upper face of the dielectric base body 711 along sides of the upper face. The four radiating conductor films 712 make a turn by forming gaps at central portions of the respective sides of the top face of the dielectric base body 711. The length of a total of the four radiating conductor films 712 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission and receiving. A grounding conductor film 713 is formed on the lower face of the dielectric base body 711 and the grounding conductor film 713 is provided with a shape where central portions of respective sides are notched. Eight feeding conductor films 714 extending in the up and down direction are formed at side faces of the dielectric base body 711 and the respective feeding conductor films 714 are connected to respective ends of the radiating conductor films 712. Further, portions of the respective feeding conductor films 714 on the lower end sides, also serve as feed electrodes 714a. Ground electrodes 715 are formed to connect to the grounding conductor film 713 at corners of two parallel side faces on the side of the grounding conductor film 713 among four side faces of the dielectric base body 711. The feeding conductor films and the radiating conductor films may be connected to each other at central portions of the respective sides of the top face of the dielectric base body in this way. Fig. 52 is a view showing an antenna device according to Embodiment 12 of the present invention and Fig. 53 is a bottom view of the antenna device shown by Fig. 52. An antenna device 820 shown by Fig. 52 is provided with a dielectric base body 821 in a rectangular parallelepiped shape having a top face and a bottom face in a square shape. A radiating conductor film 822 in a closed loop shape making a turn horizontally along four sides of the top face, is formed on the top face of the dielectric base body 821 and the length of the radiating conductor film 822 is adjusted to be the resonance wavelength of electromagnetic wave that is an object of transmission. Further, a grounding conductor film 823 extending horizontally is formed on the lower face of the dielectric base body 821 as shown by Fig. 53 and the grounding conductor film 823 is provided with a shape where a portion of one side is notched. As shown by Fig. 52, a pair of feeding conductor films 824 extending in the up and down direction in parallel with each other and connected to the radiating conductor film 822, are formed on a side face of the dielectric base body 821, a feeding conductor film 826 that is one of the pair of the feeding conductor films 824, is also connected to the grounding conductor film 823 and a feeding conductor film 825 that is the other of the pair of feeding conductor films 824, reaches the lower face of the dielectric base body 821 as shown by Fig. 53. According to the antenna device 820 constituted as described above, the radiating conductor film 822 in a closed loop shape is formed on the upper face of the dielectric base body 821 and accordingly, it has a single wavelength loop antenna structure and electromagnetic wave radiated from the radiating conductor film 822 is electromagnetic wave having the maximum gain in a direction perpendicular to a plane including the radiating conductor film 822. Further, the grounding conductor film 823 extending horizontally is formed on the lower face of the dielectric base body 821 and therefore, electromagnetic wave progressing toward the grounding conductor film 823 among electromagnetic waves radiated from the radiating conductor film 822, is reflected by the grounding conductor film 823. That is, electromagnetic wave having the maximum gain is radiated from the antenna device 820 in a direction perpendicular to a plane including the radiating conductor film and progressing from the grounding conductor film to the radiating conductor film. Accordingly, when the antenna device 820 is attached to, for example, a portable telephone, if the grounding conductor film 823 is disposed between a person and the radiating conductor film 822 when the person uses the portable telephone, electromagnetic wave is not radiated to the side of the person and radiated electromagnetic wave can efficiently be used in communication. It is not necessary to form a through hole in forming the radiating conductor film 822 by which reduction in fabrication cost is achieved. The radiating conductor film may be in a closed loop shape as shown by Fig. 52. An explanation will be given of a fabrication method of the antenna device 820 as follows. First, the material of the dielectric base body is selected. A material where the dielectric constant is stabilized to substantially 10 through 100 in a frequency band of transmitted and received electromagnetic wave, is preferably used as the material of the dielectric base body and, for example, a Sr(Ni 1/3 Nb 2/3 )O 3 group ceramic is preferably used. According to the material, the dielectric constant is 30 when the frequency of transmitted and received electromagnetic wave is 6 GHz and the Q value is 1000. Next, dimensions of the radiating conductor film and the feeding conductor film are determined. The dimensions can be determined as follows. When the length of the loop of the radiating conductor film is designated by notation λ, λ can be represented by Equation (4). Equation (4) is shown below. λ = λ 0 / (ε reff ) where λ 0 is wavelength of electromagnetic wave in vacuum and ε reff is effective dielectric constant. Here, the direction of propagating electromagnetic wave radiated from the radiating conductor film in a loop shape shown by Fig. 52, is in a direction intersecting perpendicularly with a face of the dielectric base body where the radiating conductor film is formed and the effective dielectric constant ε reff can be represented by the following equation in consideration of the fact that electric fields are generated from the radiating conductor film both at the inside of the dielectric base body and in air. ε reff = (ε r +1)/2 where ε r is dielectric constant of dielectric base body. Accordingly, the effective dielectric constant ε reff is calculated by Equation (18) and λ can be calculated by substituting the calculated value of ε reff for Equation (17). When the resonance frequency of electromagnetic wave is set to 1.9 GHz, λ is determined as λ=40.11 mm and the length of one side of the radiating conductor film is set to 10.03 mm when the radiating conductor film is formed as shown by Fig. 52. Although the impedance of a single wavelength loop antenna is generally as high as 100 Ω or higher, the impedance can be lowered by adjusting the width of the radiating conductor film and an interval between a portion of the radiating conductor film that is connected to one of the feeding conductor films and a portion of the radiating conductor film that is connected to the other one of the feeding conductor films by which the electricity feed efficiency can be promoted. For example, in order to set the impedance to 50 Ω, the width of the radiating conductor film is set to 2 mm and the interval between the feeding conductor films is set to 1 mm. It has been reported that a desired transmission impedance is obtained by adjusting a width of a feeding conductor film and an interval between feeding conductor films in "C.P. Wen: 'Coplanar Waveguide: A Surface Strip Transmission Line Suitable for Nonreciprocal Gyromagnetic Device Applications', IEEE Trans. MTT, Vol. MTT-17, No. 12, Dec. 1969". In order to set the interval between the feeding conductor films to 1 mm, the width of the feeding conductor film is set to 3.09 mm for setting the transmission impedance to 50 Ω. Next, with respect to dimensions of the dielectric base body, both of the length and the width are determined to be 12.03 mm in accordance with the radiating conductor film of which dimensions have been determined as described above and the thickness is determined to be 7.21 mm corresponding to a quarter of the wavelength of electromagnetic wave having the resonance frequency of 1.9 GHz in the dielectric base body by which the dielectric base body is fabricated. Next, a pattern of the grounding conductor film and patterns of the radiating conductor film and the feeding conductor films having the above-described dimensions, are printed by the thick film printing process by using a copper paste and are sintered in a reducing atmosphere. The antenna device 820 shown by Fig. 52 is fabricated in this way. Fig. 54 is a perspective view showing Embodiment 13, of an antenna device according to the present invention. An antenna device 830 shown by Fig. 54 is provided with a dielectric base body 831 in a cylindrical shape, a radiating conductor film 832 in a closed loop shape making a turn horizontally along the circumference of an upper face is formed on the upper face of the dielectric base body 831 and the length of the radiating conductor film 832 is adjusted to be the resonance wavelength of electromagnetic wave that is an object of transmission. Further, a circular grounding conductor film 833 extending horizontally is formed on the lower face of the dielectric base body 831 and the grounding conductor film 833 is provided with a shape where a portion of the circumference is notched. A pair of feeding conductor films 834 extending in the up and down direction in parallel with each other and connected to the radiating conductor film 832, are formed on the side face of the dielectric base body 831. The feeding conductor film 836 that is one of the pair of feeding conductor films 834, is also connected to the grounding conductor film 833 and a feeding conductor film 835 which is the other one thereof reaches the lower face of the dielectric base body 831. As described above, the dielectric base body may be in a cylindrical shape. Fig. 55 is a perspective view showing an antenna device according to Embodiment 14 of the present invention. An antenna device 840 shown by Fig. 55 is provided with a dielectric base body 841 having a rectangular parallelepiped shape and a radiating conductor film 842 in a closed loop shape turning around horizontally side faces along four sides of the upper face of the dielectric base body 841, is formed on the upper portions of the side faces of the dielectric base body 841. The length of the radiating conductor film 842 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission. A grounding conductor film 843 extending horizontally is formed on the lower face of the dielectric base body 841 and the grounding conductor film 843 is provided with a shape where a portion of a side is notched. Further, a pair of feeding conductor films 844 extending in the up and down direction in parallel with each other and connected to the radiating conductor film 842 are formed on a side face of the dielectric base body 841. A feeding conductor film 846 that is one of the pair of feeding conductor films 844 is also connected to the grounding conductor film 843 and a feeding conductor film 845 that is the other one thereof reaches the lower face of the dielectric base body 841. The radiating conductor film may be formed on the side faces of the dielectric base body as described above. Fig. 56 is a perspective view showing an antenna device according to Embodiment 15 of the present invention. An antenna device 850 shown by Fig. 56 is provided with a dielectric base body 851 in a rectangular parallelepiped shape, a radiating conductor film 852 in a closed loop shape making a turn on a horizontal face at an inner portion of the dielectric base body 851 is formed and the length of the radiating conductor film 852 is adjusted to a length the same as the resonance wavelength of electromagnetic wave that is an object of transmission at the inside of the dielectric base body 851. Further, a pair of inner feeding conductor film 853 extending in a horizontal direction in parallel with each other, connected to the radiating conductor film 852 and exposed on a side face of the dielectric base body 851, are formed on a plane including the radiating conductor film 852 formed at the inner portion of the dielectric base body 851. A grounding conductor film 856 extending horizontally is formed on the lower face of the dielectric base body 851 and the grounding conductor film 856 is provided with a shape where a portion of a side is notched. A pair of side face feeding conductor films 857 extending in the up and down direction in parallel with each other are formed on the side face of the dielectric base body 851. An upper end and a lower end of a side face feeding conductor film 859 of the pair of side face feeding conductor films 857, are respectively connected to the feeding conductor film 855 and the grounding conductor film 856. An upper end of a side face feeding conductor film 858 that is the other one thereof is connected to the inner feeding conductor film 854 and a lower end thereof reaches the lower face of the dielectric base body 851. According to the antenna device 850 constituted as described above, the radiating conductor film 852 is formed at the inside of the dielectric base body 851. When the antenna device 850 is compared with an antenna device in which a radiating conductor film is formed on the surface of a dielectric base body, in the case where the respective antenna devices transmit and receive electromagnetic wave of the same frequency, since the wavelength of the electromagnetic wave is shorter at the inside of a dielectric base body than at the outside of the dielectric base body, the length of the loop of the radiating conductor film can be shortened if the radiating conductor film is formed at the inside of the dielectric base body. Accordingly, dimensions of the dielectric base body can be downsized by which downsizing of an antenna device is achieved. Fig. 57 is a perspective view showing an antenna device according to Embodiment 16 of the present invention. An antenna device 860 shown by Fig. 57 is provided with a dielectric base body 861 in a rectangular parallelepiped shape. A first radiating conductor film 862 in a closed loop shape making a turn horizontally along four sides of the upper face of the dielectric base body 861 is formed on the upper face of the dielectric base body 861. Also, a second radiating conductor film 863 in a closed loop shape making a turn on a horizontal face in a square shape at the inside of the dielectric base body 861 is formed at an inner portion of the dielectric base body 861. A grounding conductor film 864 is formed on the lower face of the dielectric base body 861 and the grounding conductor film 864 is provided with a shape where respective portions of two sides among four sides are notched. A pair of first feeding conductor films 865 extending in the up and down direction in parallel with each other and connected to the radiating conductor film 862 are formed on one side face among four side faces of the dielectric base body 861. A feeding conductor film 867 that is one of the pair of first feeding conductor films 865, is also connected to the grounding conductor film 864 and a feeding conductor film 866 that is the other one thereof reaches the lower face of the dielectric base body 861. Further, a pair of second feeding conductor films 868 extending in the up and down direction in parallel with each other and connected to the second radiating conductor film 863, are formed on a side face contiguous to the side face where the pair of first feeding conductor films 865 are formed. A feeding conductor film 870 is one of the pair of second feeding conductor films 868, is connected to the grounding conductor film 864 and a feeding conductor film 869 that is the other one thereof reaches the lower face of the dielectric base body 861. According to the antenna device 860 constituted as described above, since the pair of first feeding conductor films 865 and the pair of second feeding conductor films 868 are formed on the side faces contiguous to each other, the direction of the contact point where the first radiating conductor film 862 and the pair of first feeding conductor films 865 are brought into contact with each other, with respect to a loop of the first radiating conductor film 862, and the direction of the contact point where the second radiating conductor film 863 and the pair of second feeding conductor films 868 are brought into contact with each other, in respect of a loop of the second radiating conductor film 863, are different from each other by 90° in respect of a horizontal plane. Accordingly, polarizing directions of electromagnetic waves received by the first and the second radiating conductor films 862 and 863 are different from each other by 90° in respect of a horizontal plane by which the antenna device 860 can receive electromagnetic wave efficiently irrespective of whether the electromagnetic wave is a vertically polarized wave or a horizontally polarized wave. Fig. 58 is a perspective view showing an antenna device according to Embodiment 17 of the present invention. An antenna device 880 shown by Fig. 58 is provided with a dielectric base body 881 in a rectangular parallelepiped shape. A radiating conductor film 882 in a closed loop shape turning around side faces horizontally along four sides of the upper face of the dielectric base body 881, is formed at the upper portion of the side faces of the dielectric base body 881. Further, a grounding conductor film 883 is formed on the lower face of the dielectric base body 881 and the grounding conductor film 883 is provided with a shape where the respective corners are notched. Further, ground electrodes 884 are formed to connect to the grounding conductor film 883 at the lower portions of the respective side faces of the dielectric base body 881. A total of four pairs of feeding conductor films 885 extending in the up and down direction in parallel with each other, each of which is formed on both sides of each of sides of four sides on side faces are formed at positions of the side faces of the dielectric base body 881 dividing equally by four a periphery turning around the radiating conductor film 882 by four sides of the side faces extending in the up and down direction. According to the antenna device 880 constituted as described above, a total of the four pairs of feeding conductor films 885 are formed at positions equally dividing the radiating conductor film 882. Therefore, when a state where currents having the same amplitude and the same phase are supplied to two pairs of the feeding conductor films formed at positions equally dividing by two the periphery turning around the radiating conductor film 882, and a state where currents having the same amplitude and the same phase are supplied to residual two pairs of the feeding conductor films, are switched freely, an antenna device having gains which can freely be switched in the polarizing directions perpendicularly intersecting with each other, is provided. Fig. 59 is a perspective view showing an antenna device according to Embodiment 18 of the present invention, Fig. 60 is a top view thereof, Fig. 61 is a bottom view thereof, Fig. 62 is a view showing a side face of an antenna device shown by Fig. 59 where one of two feeding conductor films is formed and Fig. 63 is a view showing a side face of the antenna device shown by Fig. 59 where the other one of the feeding conductor films is formed. An antenna device 920 shown by Fig. 59 is provided with a dielectric base body 921 in a rectangular parallelepiped shape having an upper face and a lower face in a square shape. Two ends 922a and 922b adjacent to each other as shown by Fig. 60 are provided on the upper face of the dielectric base body 921 and a radiating conductor film 922 connecting two ends 922a and 922b in a loop-like shape are formed along four sides of the upper face. The radiating conductor film 922 is of an open loop shape where the two ends 922a and 922b are electrically opened and the length of the loop is adjusted to a length of the resonance wavelength of electromagnetic wave that is an object of transmission. A grounding conductor film 923 extending on the lower face as shown by Fig. 61 is formed on the lower face of the dielectric base body 921 and the grounding conductor film 923 is provided with a shape where a portion of one side is notched. Further, as shown by Fig. 62 and Fig. 63, two feeding conductor films 924 and 925 are formed on the side faces of the dielectric base body 921. As shown by Fig. 59, the two feeding conductor films 924 and 925 are formed to extend in the up and down direction in parallel with each other respectively on both sides of a side 926 that is shown on this side of Fig. 59 among four sides partitioning vertically the side faces. The feeding conductor films 924 and 925 are respectively connected to the ends 922a and 922b of the radiating conductor film 922. The feeding conductor film 925 is connected to the grounding conductor film 923 and the feeding conductor film 924 reaches the lower face of the dielectric base body 921 as shown by Fig. 61. The antenna device 920 constituted as described above, is provided with a single wavelength loop antenna structure since it has the radiating conductor film 922. Therefore, electromagnetic wave having the maximum gain is radiated from the radiating conductor film 922 perpendicularly to the upper face of the dielectric base body 921. The radiating conductor film 922 is formed on the upper face of the dielectric base body 921 and the grounding conductor film 923 is formed on the lower face of the dielectric base body 921 and therefore, electromagnetic wave progressing toward the grounding conductor film 923 among the electromagnetic waves radiated from the radiating conductor film 922, is reflected by the grounding conductor film 923. Accordingly, the electromagnetic wave having the maximum gain is irradiated from the antenna device 920 in a direction from the grounding conductor film 923 to the radiating conductor film 922 by which electromagnetic wave can efficiently be used in communication. Further, according to the antenna device 920, the two feeding conductor films 924 and 925 are formed respectively on both sides of the side 926 of the side faces of the dielectric base body 921 and accordingly, a distance between the feeding conductor films becomes shorter than that between two feeding conductor films formed on the same side face by which the effective dielectric constant can be enhanced. Accordingly, in respect of the antenna device 920, compared with an antenna device where two feeding conductor films are formed on the same side face, the width S of the feeding conductor film in Equation (2) can be narrowed whereby even in the case where the gap width between the two feeding conductor films 924 and 925 is wide, the impedance of the radiating conductor film can be matched with the impedance of the feeding conductor films. An explanation will be given of the fabrication method of the antenna device 920 shown by Fig. 59 through Fig. 63. First, the material of the dielectric base body 921 is selected. A material where the dielectric constant is stabilized to substantially 10 through 100 in a frequency band of transmitted and received electromagnetic wave, is preferably used as the material of the dielectric base body 921 and in this embodiment, a Sr(Ni 1/3 Nb 2/3 )O 3 group ceramic is used. According to the material, the dielectric constant is 31 when the frequency of transmitted and received electromagnetic wave is 3.8 GHz and the Q value is 1800. Next, dimensions of the radiating conductor film 922, the two feeding conductor films 924 and 925 and the dielectric base body 921 are determined. The dimensions can be determined as follows. When the length of the loop of the radiating conductor film 922 is designated by notation λ, λ can be represented by Equation (4). Equation (4) is shown below. λ = λ 0 / (ε reff ) where λ 0 is wavelength of electromagnetic wave in vacuum and ε reff is effective dielectric constant. Here, the effective dielectric constant ε reff in Equation (19) can be represented by the following equation in consideration of the fact that the radiating conductor film 922 is formed on the upper face of the dielectric base body 921, electromagnetic wave radiated from the radiating conductor film 922 is radiated perpendicularly to the upper face of the electromagnetic base body 921 and electric fields are generated at the inside and the outside of the radiating conductor film 922. ε reff = (ε r +3)/4 where ε r is dielectric constant of dielectric base body. Therefore, the length λ of the radiating conductor film 922 can be calculated by substituting the effective dielectric constant ε reff calculated by Equation (20) for Equation (19). Here, in order to set a resonance frequency of electromagnetic wave to 1.9 GHz, the length λ of the loop of the radiating conductor film 922 is determined as λ =54.16 mm. Further, although impedance of a single wavelength loop antenna is generally as high as 100 Ω or higher, the impedance can be lowered by adjusting the width of a radiating conductor film and the gap width between two ends of the radiating conductor film by which electricity feed efficiency can be promoted. In this case, in order to set the impedance to 50 Ω, the width of the radiating conductor film 922 is set to 1.5 mm and the gap width is set to 0.75 mm. Both of the length and the width of the dielectric base body 921 are set to 14.54 mm in accordance with the dimensions of the radiating conductor film which has been determined as described above. With respect to the thickness of the dielectric base body 921, a distance from the radiating conductor film 922 to the grounding conductor film 923 is set to 7.09 mm corresponding to a quarter of the resonance wavelength of electromagnetic wave having the resonance frequency of 1.9 GHz in the dielectric base body. Further, a desired impedance of the feeding conductor film can be provided by adjusting the width of the feeding conductor film and the gap width between the feeding conductor films. In this case, the width of the feeding conductor film is set to 2.0 mm and the gap width is set to 0.75 mm. Next, the dielectric base body 921 having the above-described dimensions are fabricated and a pattern of the grounding conductor film 923 and patterns of the radiating conductor film 922 and the two feeding conductor films 924 and 925 having the above-described dimensions, are printed on the dielectric base body 921 by the thick film printing process by using a copper paste and sintered in a reducing atmosphere. The antenna device 920 is fabricated in this way. Fig. 64 is a view showing an antenna device according to Embodiment 19 of the present invention. The same numbers are attached to constituent elements the same as the constituent elements of the antenna device 920 shown by Fig. 59 through Fig. 63 and an explanation will be given of only differences therebetween. A radiating conductor film 931 in a closed loop shape where a strip-like conductor film turns around along four sides of the upper face of the dielectric base body 921, is formed on the upper face of the dielectric base body 921 constituting an antenna device 930 shown by Fig. 64. In this way, the radiating conductor film may be of a closed loop shape where the strip-like conductor film turns around. As has been explained, according to the antenna device of the present invention, radiated electromagnetic wave can efficiently be used in communication.

Claims: An antenna device (110; 310; 410; 510; 820; 920) for transmission and receiving electromagnetic wave comprising: a dielectric base body (111; 311; 411; 511; 821; 921) having a lower face; a radiating conductor film (112; 313; 412; 513; 822; 922) having two ends (112a, 112b; 313a, 313b; 412a, 412b; 513a, 513b; 822a, 822b; 922a, 922b) adjacent to each other and connected in a loop-like shape so as to define a single plane on or inside the dielectric base body, the plane being parallel to and spaced apart from the lower face of the dielectric base body, a pair of feeding conductor films (114, 115; 314, 315; 418, 419; 518, 519; 825, 826; 924, 925), each of the pair of feeding conductor films formed on at least one side face of the dielectric base body, each connected to one end of the radiating conductor film, the pair of feeding conductor films extending in an up and down direction in parallel with each other between a grounding conductor film and the radiating conductor film, one of said feeding conductor films being connected to the grounding conductor film; characterized by the length of the radiating conductor film being a length the same as the wavelength of the electromagnetic wave which is an object of transmission and receiving in the dielectric body; said grounding conductor film (113; 312; 416; 516; 823; 923) formed essentially on the whole lower face of the dielectric base body and extending in a planar shape; a distance between said radiating conductor film and said grounding conductor film formed on the lower face of the dielectric bases body is a distance corresponding to a quarter of the resonance wavelength of an electromagnetic wave which is an object of transmission and receiving in the dielectric body. The antenna device (110) according to claim 1, wherein: the dielectric base body (111) has an upper face in parallel with the lower face and a plurality of side faces; the radiating conductor film (112) is formed on the upper face of the dielectric base body (111); and the feeding conductor films (114, 115) are formed on the same side face of the dielectric base body. The antenna device according to claim 2, further comprising: a second radiating conductor film in a closed and horizontal planar loop shape, the second radiating conductor film having two ends adjacent to each other that are connected in the loop shape and being formed on or inside the dielectric base body, the horizontal plane of the second radiating conductor film positioned to be spaced apart from the first radiating conductor film and from the lower face of the dielectric base body; and a second pair of feeding conductor films; in the antenna device each of the pair of feeding conductor films is formed on a side face of the dielectric base body, each is connected to one end of the second radiating conductor film, and the second pair of feeding conductor films extends in an up and down direction in parallel with each other between the grounding conductor film and the second radiating conductor film, and is spaced apart from the first pair of feeding conductor films. The antenna device according to claim 3, wherein a total of four pairs of feeding conductor films is formed, each pair of feeding conductor films being connected to one of the radiating conductor films at positions so that the loop of the radiating conductor film is equally divided by four, and each feeding conductor film of a respective one of the pairs extends in an up and down direction in parallel with each other. The antenna device (310) according to claim 1, wherein: the dielectric base body (311) has a plurality of side faces; the radiating conductor film (313) is formed on the side faces and has two ends (313a, 313b) adjacent to each other in a left and right direction and connected in a horizontal loop-like shape around the side faces. The antenna device (410) according to claim 1, wherein the radiating conductor film (412) is formed at an inner portion of the dielectric base body (411), inner feeding conductor films (413, 414) are formed at an inner portion of the dielectric base body (411) and connect respectively the two ends (412a, 412b) of the radiating conductor film with a side face of the dielectric base body; and each of the pair of feeding conductor films (418, 419) formed on the side face of the dielectric base body (411) is connected to one of the inner feeding conductor films (413, 414). The antenna device (510) according to claim 1, wherein: the dielectric base body (511) has an upper face and the lower face extends horizontally; the radiating conductor film (513) is formed on the upper face of the dielectric base body and makes a turn on the upper face such that the two ends (513, 513b) are formed opposite each other via a predetermined first gap; a second radiating conductor film is formed at an inner portion of the dielectric base body, the second radiating conductor film having two ends connected in a loop-like shape so as to define a single horizontal plane, the two ends (515a, 515b) being formed opposite each other via a second gap having a direction different from a direction of the first gap in respect of the loop-like shape of the first radiating conductor film (513); a second pair of feeding conductor films (521, 522) is provided, each of the second pair of feeding conductor films is formed on a side face of the dielectric base body, each connected to one end of the second radiating conductor film, the feeding conductor films of the second pair extending in parallel with each other. The antenna device according to claim 7, wherein the direction of the first gap is different from the direction of the second gap by being offset by 90° in the horizontal plane. The antenna device (820; 840; 850) according to claim 1, wherein: the ends of the radiating conductor film (822) are further connected so that the radiating conductor film forms a closed loop shape. The antenna device (820) according to claim 9, wherein the radiating conductor film (822) is formed on an upper face of the dielectric base body (821). The antenna device (840) according to claim 9, wherein the radiating conductor film (842) is formed horizontally around the at least one side face of the dielectric base body (841). The antenna device (850) according to claim 9, wherein the radiating conductor film (852) is formed within a horizontal plane at an inner portion of the dielectric base body (851). The antenna device (920) according to claim 1, wherein: the dielectric base body (921) has an upper face and a plurality of side faces partitioned by a vertically extending edge (926); the radiating conductor film (922) is formed on the upper face of the dielectric base body; the pair of feeding conductor films (924, 925) is formed on the side faces of the dielectric base body such that one of said pair is formed on each side of the edge (926). The antenna device (920) according to claim 13, wherein the radiating conductor film (922) is provided with an open loop shape where points of connecting the ends of the radiating conductor film to the two feeding conductor films (924, 925) are electrically opened with respect to each other. The antenna device (920) according to claim 14, wherein the radiating conductor film (922) is provided with a strip-like shape. The antenna device according to any of claims 2, 5, 6 or 7, wherein the feeding conductor films also serve as electrodes for mounting onto a surface of a circuit board. The antenna device according to any one of the preceding claims, wherein one of the feeding conductor films is connected to the grounding conductor film. The antenna device according to any one of the preceding claims, wherein the radiating conductor film extends along the periphery of the dielectric base body.

Inventors: ASO T, GOTO NAOHISA, TANIDOKORO H, ASO, T., GOTO, NAOHISA, TANIDOKORO, H., Aso, T., Electronics Technology Research Center,, Tanidokoro, H., Electronics Tech. Research Center,
Applicants: MITSUBISHI MATERIALS CORP, MITSUBISHI MATERIALS CORPORATION
Application year: 1997
Main classification: H01Q1
IPC codes: H01Q1, H01Q9, H01Q7