WO2011030703A1

WO2011030703A1 - Inverse-l shaped antenna

Info

Publication number: WO2011030703A1
Application number: PCT/JP2010/064903
Authority: WO
Inventors: 光雄田口; 徹也山下
Original assignee: 国立大学法人長崎大学
Priority date: 2009-09-14
Filing date: 2010-09-01
Publication date: 2011-03-17
Also published as: JP2011082951A

Abstract

Provided is an inverse-L shaped antenna that has a shape suited for making the size of the antenna compact, making impedance matching easy, and achieving high-gain. The inverse-L shaped antenna is configured to be provided with: a grounding conductor face (10) provided on the front-side or back-side, and having a ground electric potential; an outer conductor (26) that has the base-end section (21) thereof connected to a prescribed section of that grounding conductor face (10); and an inner conductor (24) that is surrounded by that outer conductor (26), arranged so as to have a gap between the inner conductor and the outer conductor (26), and that has the tip thereof elongating further than the outer conductor. The inverse-L shaped antenna is also configured so that the outer conductor (26) and the inner conductor (24) are bent at a place (22) separated at a prescribed distance from the place where the conductors are connected to the grounding conductor face (10), then arranged in proximity and parallel to the grounding conductor face (10), and so that electricity is fed to the inner conductor (24).

Description

Inverted L antenna

More specifically, the present invention relates to an ultra-low profile inverted L antenna that can be impedance-matched with high gain and disposed on a finite conductor plate.

Conventionally, if a horizontal dipole antenna is arranged in the vicinity of a conductor plate, it has been theorized that electromagnetic waves are not radiated because of an image element made of a conductor plate. In contrast, in the technique described in Non-Patent Document 1, if a half-wave dipole antenna placed at a position of 1/30 wavelength in height on an infinite conductor plate is fed at two opposite points at equal distances from both ends, It has been clarified that the input impedance is 50Ω and a high directivity gain of 8 dB or more can be obtained.

FIG. 1 is a configuration example of an antenna based on the technique described in Non-Patent Document 1.
The antenna configuration shown in FIG. 1 will be described. Two coaxial cables 5 and 6 are connected in proximity to the conductor plate 4 and are parallel to the surface direction of the conductor plate 4 at a location slightly away from the connection point. It is bent by 90 °. When this bending is performed, the coaxial cables 5 and 6 are arranged so that the ends of the coaxial cables 5 and 6 face away from each other, and the length between the ends is set to be approximately half the wavelength of the signal to be transmitted and received. The height from the conductor plate 4 to the bending position is, for example, a distance of about 1/30 wavelength.

The coaxial cables 5 and 6 are composed of a center conductor and an outer conductor, and the outer conductor is electrically connected to the conductor plate 4 which is a ground potential portion. The center conductor is not electrically connected to the outer conductor. In each of the coaxial cables 5 and 6, the peripheral conductor is cut off from the tip by a certain length, and this point becomes a feeding point. The

center conductors

5a and 6a are exposed at the tip.

In the antenna power supply configuration shown in FIG. 1, the output of the signal source 1 (for example, a signal with a frequency of 2 GHz) is supplied to the coupler 2, and the oscillation signal as it is (0 ° signal). , A signal delayed in phase by 90 ° (a signal of −90 °) is obtained. Further, the −90 ° signal is supplied to the phase shifter 3 and is further delayed by 90 ° (−180 ° signal), and the 0 ° signal and the −180 ° signal whose phases are reversed are obtained. obtain.
The 0 ° signal obtained in this way is supplied to the central conductor of the coaxial cable 5, and the −180 ° signal is supplied to the central conductor of the coaxial cable 6, and the two coaxial cables are fed in reverse phase.

As an antenna having a simpler configuration than the horizontal dipole antenna shown in FIG. 1, for example, an inverted L-type antenna shown in FIG. 2 is known. This inverted L-type antenna is obtained by attaching an inverted L-type element 8 on a conductor plate 7. The inverted L-shaped element 8 formed of a conductor is bent at a location 8b having a predetermined height h from the connection point 8a, and is arranged in parallel with the conductor plate 7 from the bent location 8b to the tip 8c. For example, the conductive plate 7 is configured to supply power to the inverted L-type element 8 at the connection point 8a as a ground potential.

Non-Patent Document 1 shows that the antenna configuration shown in FIG. 1 makes it possible to obtain an input impedance of 50Ω and a high directivity gain of 8 dB or more. In the case of the antenna configuration shown in FIG. 1, the length of the antenna needs to be ½ wavelength, and there is a problem that the total length of the antenna becomes long. Further, as shown in FIG. 1, it is necessary to generate and feed two signals having opposite phases, and there is a problem that the configuration for feeding is complicated.

The present invention has been made in view of these points, and an object of the present invention is to provide an antenna shape suitable for miniaturization, easy impedance matching, and high gain.

The inverted L-type antenna of the present invention includes a finite conductor plate having a surface ground potential, an outer conductor having a base end connected to a predetermined portion of the finite conductor plate, and a gap between the outer conductor and the outer conductor. And an inner conductor whose tip extends beyond the outer conductor.
And the outer L conductor and the inner conductor are bent at a predetermined distance from the place connected to the finite conductor plate, arranged in parallel in close proximity to the finite conductor plate, and an inverted L-type antenna configured to feed the inner conductor; It is a thing.
The predetermined distance to the part to be bent is a distance of about 1/30 of one wavelength of a signal having a specific frequency. The length from the bent portion of the inner conductor to the tip is set to about 1/4 of one wavelength of a signal having a specific frequency. Then, the impedance value of the feeder is matched with the setting of the length of the inner conductor and the length from the bent portion of the outer conductor to the tip of the outer conductor.
The ground conductor surface has a length in a direction parallel to the longitudinal direction of the inner conductor, a length from a predetermined location to one end portion toward the distal end side of the inner conductor, and a side from the predetermined location toward the distal end side of the inner conductor. The length to the other end on the opposite side was set so that current would flow in the direction from the bent portion of the inner conductor toward the tip.

According to the present invention, a conductor having a short length of about a quarter wavelength is disposed on a finite conductor plate or in the same plane as the finite conductor plate, thereby reducing the size of the inverted L A type antenna can be constructed. According to this configuration, it is possible to directly perform impedance matching with the feed line without providing an impedance matching device, and a high gain antenna can be realized with a simple configuration.

It is explanatory drawing which showed the example of the conventional horizontal dipole antenna. It is explanatory drawing which showed the example of the conventional inverted L type | mold antenna. It is a perspective view which shows the example of an antenna structure by the 1st Embodiment of this invention. FIG. 4 is a cross-sectional view taken along line AA in FIG. 3. It is explanatory drawing which shows the example of the electric current generation state of the antenna by the 1st Embodiment of this invention. It is the characteristic view which showed the electric current and voltage distribution on an antenna. It is the characteristic view which showed the input impedance characteristic (FIG. 7A) and the return loss characteristic (FIG. 7B) of the antenna by the 1st Embodiment of this invention compared with the conventional inverted L type | mold antenna. FIG. 8A is a characteristic diagram showing a radiation field directivity pattern example of the antenna according to the first embodiment of the present invention, FIG. 8A is a radiation field directivity pattern on the xz plane, and FIG. 8B is a radiation field directivity pattern on the yz plane. is there. FIG. 9A is a characteristic diagram showing an example of a radiation field directivity pattern of a conventional inverted L-type antenna. FIG. 9A is a radiation field directivity pattern on the xz plane, and FIG. 9B is a radiation field directivity pattern on the yz plane. It is a perspective view which shows the example of an antenna structure by the 2nd Embodiment of this invention. It is a perspective view which shows the example of an antenna structure by the 3rd Embodiment of this invention. It is a perspective view which shows the example of an antenna structure by the 4th Embodiment of this invention. It is a top view which shows the example of an antenna structure by the 4th Embodiment of this invention. It is a perspective view which shows the example of an antenna structure by the 5th Embodiment of this invention. It is a perspective view which shows the example of an antenna structure by the 6th Embodiment of this invention. It is the characteristic view which showed the return loss characteristic of the antenna by the 6th Embodiment of this invention. It is a perspective view which shows the example of an antenna structure by the 7th Embodiment of this invention. FIG. 19 is a characteristic diagram showing a directivity gain (FIG. 18A) and a return loss characteristic (FIG. 18B) of an antenna according to a seventh embodiment of the present invention. It is a perspective view which shows the example of an antenna structure by the 8th Embodiment of this invention. It is the characteristic view which showed the return loss characteristic and axial ratio characteristic of the antenna by the 8th Embodiment of this invention. FIG. 21A is a characteristic diagram showing calculated values of the radiation field directivity pattern of the antenna according to the eighth embodiment of the present invention, FIG. 21A is a radiation field directivity pattern on the xz plane, and FIG. 21B is a radiation field directivity pattern on the yz plane. It is. It is explanatory drawing which shows the example of arrangement | positioning of the antenna by each embodiment of this invention. It is explanatory drawing which shows the example of the location which arrange | positions the antenna by each embodiment of this invention to an airplane.

Hereinafter, examples of embodiments of the present invention will be described in the following order.
1. Example of the first embodiment (FIGS. 3 to 9)
2. Example of second embodiment (FIG. 10)
3. Example of third embodiment (FIG. 11)
4). Example of the fourth embodiment (FIGS. 12 to 13)
5. Example of fifth embodiment (FIG. 14)
6). Example of sixth embodiment (FIGS. 15 and 16)
7). Example of seventh embodiment (FIGS. 17 and 18)
8). Example of the eighth embodiment (FIGS. 19 to 21)
9. Application example of antenna of each embodiment (FIGS. 22 and 23)

[1. Example of First Embodiment (FIGS. 3 to 9)]
FIG. 3 is a diagram illustrating an antenna configuration of the example of the first embodiment. In this embodiment, it is configured as an ultra-low profile inverted L-type antenna. The configuration will be described with reference to FIG. 3. A conductor plate 10 as a finite conductor having a predetermined rectangular size is used as an antenna. The conductor plate 10 has at least the surface as a ground potential portion. The size of the conductor plate 10 will be described later.

A connection point 21 connecting one end of the coaxial cable 20 is provided at a predetermined position on the surface of the conductor plate 10. The coaxial cable 20 includes a center conductor 24 and an outer conductor 26. As shown in cross section in FIG. 4, the coaxial cable 20 has an insulator (dielectric material) 25 disposed so as to surround the outside of the central conductor 24 disposed at the center, and surrounds the outside of the insulator 25. The outer conductor 26 is arranged on the front side. The coaxial cable 20 is electrically connected to the outer conductor 26 and the surface of the conductor plate 10 serving as a ground potential portion at a connection point 21 with the conductor plate 10, and the outer conductor 26 serves as a ground potential portion. .

The coaxial cable 20 having one end connected to the connection portion 21 is bent at a position away from the surface of the conductor plate 10 by a predetermined distance h as a bent portion 22, and the distal end side of the bent coaxial cable 20 is They are arranged so as to be parallel to the surface of the conductor plate 10. The distance h separating the surface of the conductor plate 10 and the center of the coaxial cable 20 is, for example, about 1/30 of one wavelength of a signal transmitted and received by the antenna of this example.

Coaxial cable bent at bent portion 22 extends parallel to the conductive plate 10 20 Yes stretched only the center conductor 24 to the center conductor end portion 24a to a length L _0, the outer conductor 26, the length L The position of the length L ₁ shorter than ₀ is set as the outer conductor end portion 23. At the position of the outer conductor end 23, the insulator 25 is also cut as an end. The position where the outer conductor 26 is cut becomes the feeding point of the antenna.
The length L ₀ from the bent portion 22 to the center conductor end 24a is, for example, about ¼ of one wavelength of a signal transmitted / received by this antenna. Outer conductor 26 of the thus stretched central conductor 24 and the length L ₁ functions as an antenna device having an inverted L antenna of the present embodiment. The length L ₁ of the outer conductor 26, the impedance of the antenna is set to be (50 [Omega in this case) the desired value. That is, in such a configuration, the impedance can be set to an arbitrary value by setting the length of the center conductor 24 as the inner conductor and the length from the bent portion 22 to the tip 23 of the outer conductor 26. Here, this impedance is matched with the power supply line so as to match the impedance value of the power supply line. Specific examples of these values will be described later.

As shown in FIG. 4, the coaxial cable connecting portion 21 of the conductor plate 10 is provided with a hole 20a penetrating from the front surface to the back surface, and the central conductor 24 of the coaxial cable 20 is passed through the hole 20a. At this time, for example, the insulator 25 is also passed through the hole 20a so that the central conductor 24 is not in electrical contact with the surface of the conductor plate 10 or the like.
Power is supplied using the outer conductor 26 and the center conductor 24 drawn out to the back side of the conductor plate 10. A broken-line arrow from the back surface side of the conductor plate 10 shown in FIG. 3 toward the coaxial cable connection portion 21 indicates a state where power is supplied from the back surface side, and when transmitting, a transmission signal is supplied and received. In this case, the received signal is taken out.

Next, with reference to FIG. 5, the radiation principle of the inverted L-type antenna of this example and the size of the conductor plate 10 will be described.
FIG. 5 shows the direction of current flowing through the conductor plate 10 and the coaxial cable 20 of this example. If the current phase of each part is constant, the current I _{2 in the} horizontal direction (y-axis direction in FIG. 5) parallel to the longitudinal direction of the antenna element on the surface of the conductor plate 10, the center conductor 24 and the outer conductor 26 constituted current I ₁ of the surface of the horizontal elements cancel each other become opposite, the radiation is reduced.

Moreover, in this example, about the direction (x-axis direction in FIG. 5) orthogonal to the longitudinal direction of an antenna element (center conductor 24) on the surface of the conductor board 10, it is one edge part from the coaxial cable connection part 21. And the length pxp from the coaxial cable connecting portion 21 to the other end are equal. By doing so, the currents I3 in the x-axis direction shown in FIG. 5 cancel each other, and radiation by the current I3 is suppressed. However, making the length pxm and the length pxp equal is one example, and the currents I3 in the x-axis direction may cancel each other out in the same manner with the x-axis direction being unequal.
Then, by adjusting the lengths pym and pyp of the conductor plate 10 in the y-axis direction, the current in the y-axis direction on the conductor plate is adjusted to flow in the + y-axis direction. Here, the + y-axis direction is a direction from the coaxial cable connecting portion 21 toward the central conductor end portion 24a. The length pyp in the y-axis direction is the length from the connection point 21 to the end of the conductor plate 10 in the direction in which the antenna element (center conductor 24) extends, and the length pym in the y-axis direction is the connection point 21. To the end in the opposite direction to the x-axis direction.

The direction of the current during transmission / reception will be described in more detail. Inside the coaxial cable 20, a reverse current flows through the center conductor 24 and the outer conductor 26. And since the coaxial cable 20 of the position where the outer conductor 26 is arrange | positioned is shielded by the outer conductor 26, electromagnetic waves are not radiated | emitted.
On the other hand, by extending the central conductor 24 from the outer conductor end 23 to the outside, a current flows out therefrom. An equal amount of current flows from the surface of the outer conductor 26 into the coaxial cable 20. If the central conductor 24 is not extended from the outer conductor end 23, the electromagnetic field radiated from the outer conductor end 23 is almost zero.
When receiving by an antenna, current is induced on the surface of the central conductor 24 extended from the outer conductor end 23 and the outer conductor 26 of the coaxial cable 20. As a result, a potential difference (voltage) is generated between the center conductor 24 and the outer conductor 26 at the outer conductor end 23, whereby current flows into the coaxial cable 20 and reception is performed.

According to FIG. 5, in the region of y <0, the current is reflected at the end y = −pym of the conductor plate, and the current in the + y axis direction and the current in the −y axis direction cancel each other. In the region of y> 0, the current on the conductor plate is rapidly attenuated as the distance from the base of the inverted L antenna increases. It should be noted that the currents on the horizontal element and the conductor plate immediately below the horizontal element have substantially opposite phases.

Here, FIG. 7 to FIG. 9 show examples of specific shapes of the antennas of this embodiment and characteristics calculated by the shapes.
The antenna shape parameters were set as follows.
As the radius of the coaxial cable constituting the antenna element, the radius from the connection point 21 to the outer conductor end 23 (feed point) is 1.095 mm, and the radius of the center conductor 24 from the feed point to the tip is 0.255 mm. .
Further, the length in the x-axis direction shown in FIG. 3 is set to pxm = pxp = 15 mm, and the length in the y-axis direction is set to pym = 10 mm and pyp = 50 mm.
Further, the length and height of the antenna element are L ₀ = 31.6 mm, L ₁ = 22.8 mm, and h = 4.0 mm.

After setting this parameter, the center frequency handled by this antenna was set to 2.45 GHz, and the characteristics were obtained.
As for the obtained antenna characteristics, the calculated value of the frequency bandwidth with a return loss of 10 dB or more, the measured value was 2.71%, and the calculated value of the directivity gain was 4.14 dBi.

Moreover, the input impedance of the antenna of this example can be set to 50Ω by setting the lengths L0 and L1 of the antenna element described above. The value of this input impedance can be adjusted by setting the position of the outer conductor end 23 of the coaxial cable 20 (that is, the position of the feeding point).
The point that the input impedance can be adjusted by adjusting the position of the feeding point will be described.
FIG. 6 shows a current / voltage distribution of a general inverted L antenna. In FIG. 6, the current distribution is indicated as Iα, and the voltage distribution is indicated as Vα. As shown in FIG. 6, in order to operate the inverted L-type antenna in which the element 24 is disposed on the conductor plate 10, a large current must be passed through the antenna. When the horizontal element length of the element 24 of the inverted L-shaped antenna is approximately a quarter wavelength, the current becomes maximum. When power is supplied at a certain point on the antenna, the voltage difference (potential difference) between both ends of the power supply point becomes large if the lengths at both ends are different. If the feeding point is at the tip of the antenna, the voltage is maximized. The input impedance at the feeding point is defined by the following equation.
Input impedance at the feed point = voltage / current at the feed point Therefore, if power is fed at the base of the inverted L antenna, the input resistance is small and increases toward the tip.

Using this characteristic, in the example of the present embodiment, the antenna input impedance is set to 50Ω, which is equal to the impedance of the feeder line, by setting the lengths L ₀ and L ₁ of the antenna element.

Next, an ultra-low profile inverted L-type antenna (unbalanced feeding inverted L-type antenna) of the example of the present embodiment and a conventional inverted L-type antenna (as shown in FIG. The characteristics of the antenna shown will be described below.
The antenna shape parameters here are as follows.
Length in the x-axis direction pxm = pxp = 15 mm, length from the connection point in the y-axis direction to one end pym = 10 mm, length from the connection point in the y-axis direction to the other end pyp = 50.0 mm, length L ₀ from the bending position of the antenna element to the tip, 31.6 mm, length L ₁ of the outer conductor in the unbalanced feed inverted L antenna = 22.8 mm, height h = 4.0 mm It is.
Further, the radius of the coaxial cable constituting the element of the unbalanced feed inverted L-type antenna of the example of the present embodiment is 1.095 mm from the feed point having the outer conductor to the feed point from the center conductor only to the tip. It shall be 0.255 mm. Furthermore, the radius of the radiating element of the conventional inverted L-type antenna as a comparative example is 1.095 mm.

FIG. 7 shows the input impedance characteristics (FIG. 7A) and the calculated return loss characteristics (FIG. 7B) of the unbalanced feed inverted L antenna of the example of this embodiment and the inverted L antenna of the comparative example. ).
7A and 7B, the characteristic a is the characteristic of the unbalanced feed inverted L antenna of the example of the present embodiment, and the characteristic b is the characteristic of the inverted L antenna of the comparative example.
As can be seen from FIGS. 7A and 7B, the input resistance of a normal inverted L-type antenna is several Ω, whereas the input resistance of an unbalanced feed inverted L-type antenna is 50Ω at a design frequency of 2.45 GHz. Yes.

FIG. 8 shows the radiation field directivity pattern calculation values of the unbalanced feed inverted L antenna with the same parameter settings as in FIG. FIG. 9 shows a radiation field directivity pattern calculation value of the inverted L-type antenna of the comparative example with the same parameter setting as that of FIG. FIG. 8 and FIG. 9 show the patterns seen on the xz plane (FIGS. 8A and 9A) and the patterns seen on the yz plane (FIGS. 8B and 9B), and are indicated by Eφ and Eθ.
Both radiation electric field directivity patterns are almost the same. However, in an inverted L-type antenna, the input impedance at the feed point is not matched with the characteristic impedance of the feed line. Therefore, in the case of transmission, the power supplied to the antenna is reduced, and electromagnetic waves are radiated from the antenna. Get smaller. In the case of reception, it becomes difficult to extract received power from the antenna.
On the other hand, in the case of the unbalanced feed inverted L antenna of the example of the present embodiment, the input impedance at the feed point is 50Ω matched with the characteristic impedance of the feed line, so that the power supplied to the antenna during transmission is small. The received power can be efficiently extracted from the antenna during reception.

As described above, according to the inverted L-type antenna of the example of the present embodiment, it is possible to obtain a smaller, simpler and more efficient structure than the conventional low-profile horizontal dipole antenna shown in FIG. More efficient than conventional conventional inverted L-type antennas. In other words, the length of the horizontal arrangement of the central conductor 24, which is an antenna element, may be 1/4 wavelength, which is 1/2 wavelength of the conventional low-profile horizontal dipole antenna shown in FIG. About half is sufficient. Further, it is only necessary to supply power to one central conductor 24, and a simple power supply configuration that does not require a phase shifter can be achieved.
In addition, the gain is also high, and the impedance can be set to 50Ω according to the cable to be connected. Conventionally, an impedance matching circuit that was necessary when connecting the antenna to the circuit is required. Thus, an efficient antenna can be obtained with a simple configuration.

Here, Table 1 and Table 2 show examples of changes in antenna characteristics when the shape of the ground conductor of the antenna and the height of the antenna element in the example of the present embodiment are changed.

Table 1 shows characteristic examples when the height h of the antenna element and the ground potential conductor is changed. Table 1 shows an example in which pxp = pxm = 15 mm, pym = 10 mm, pyp = L ₀ +18.4 mm as parameters other than the height h.
As can be seen from Table 1, by reducing the height h between the antenna element and the ground potential conductor and narrowing the distance between them, the coupling between the antenna element and the ground potential conductor is strengthened, and the band in which wireless communication is possible However, the gain is increased. On the other hand, by increasing the height h and increasing the spacing, the coupling is weakened and the band for wireless communication is widened, but the gain is reduced. As shown in Table 1, when 4.0 mm, which is 1/30 of one wavelength λ, a return loss of −10 dB and a bandwidth (Bandwidth) of 2.71% are secured, and a directivity gain is obtained. It can be seen that (Gain) 4.14 dBi is secured, and a relatively wide band and a good gain are secured. Incidentally, the entire antenna element length L ₀ and the length L ₁ of the ground element is one in which the impedance showed a value that is a 50Ω when the respective values.

Table 2 shows an example of characteristics when pxp = pxm, which is the length of the ground conductor in the direction orthogonal to the longitudinal direction of the antenna element, is changed. Table 2 shows an example in which h = 4.0 mm, pym = 10 mm, and pyp = L ₀ +18.4 mm as parameters other than the height h.
As can be seen from Table 2, when the values of pxp and pxm are the smallest 5.0 mm, the bandwidth is the widest and the gain is low, and the bandwidth is narrowed and the gain is increased as the value is increased. I understand that. Also in Table 2, the entire antenna element length L ₀ and the length L ₁ of the ground element is one in which the impedance showed a value that is a 50Ω when the respective values.

Here, the high efficiency of the antenna of this embodiment will be described.
In the case of the conventional low profile inverted L-type antenna shown in FIG. 2, the power supplied to the antenna is small, and as a result, the power radiated from the antenna is small. In order to use the antenna efficiently, it is important to resonate the antenna, that is, increase the current and increase the power supplied to the antenna. In order to increase the power supplied to the antenna, it is first necessary to bring the input impedance at the antenna feeding point close to the characteristic impedance of the feeding line (50Ω in this example). The input impedance is defined by “line voltage at feeding point / feeding point current”. Since the current is zero at the tip and maximum at the center of the antenna element, the input resistance (real part of the input impedance) is as low as several ohms at the center, and the input resistance increases if the feed position is moved from the center to the tip. The maximum power can be supplied at a point that matches the characteristic impedance of the feeder line.
Therefore, if the feeding position can be arbitrarily changed as in the antenna of the present embodiment, the impedance can be adjusted. As a result, the power supplied to the antenna can be increased, and a highly efficient antenna can be obtained. can do. Further, the configuration can be simplified as compared with a conventional antenna that requires impedance matching.

[2. Example of Second Embodiment (FIG. 10)]
Next, an example of the second embodiment of the ultra-low profile inverted L antenna of the present invention will be described with reference to FIG.
In the example of the first embodiment shown in FIGS. 3 to 5, the central conductor of the coaxial cable constituting the antenna element is arranged on the surface of the conductor plate 10 in parallel with the surface. In the example, the central conductor of the coaxial cable is arranged in parallel with the end face of the conductor plate 10, and the conductor constituting the antenna element is arranged in the same plane as the conductor plate.

That is, as shown in FIG. 10, a connection point 21 of the coaxial cable 20 is provided at a predetermined location on the end surface 11 of the conductor plate 10 ′, and the coaxial cable 20 attached to the connection point 21 is bent 90 ° at a bending location 22. Thus, the central conductor 24 and the like are arranged in parallel with the end face 11 at a certain interval.
The interval is, for example, about 1/30 of one wavelength of a signal to be transmitted / received. About length py2 from the bending location 22 to the front-end | tip of the center conductor 24, let it be about 1/4 of 1 wavelength of the signal transmitted / received, for example.
Also in the coaxial cable 20 in this case, as shown in FIG. 10, only the center conductor 24 is exposed on the tip side, and the outer conductor 26 is cut halfway. The outer conductor 26 of the coaxial cable 20 is electrically connected to the end face 11 of the conductor plate 10 'serving as a ground potential portion, and the outer conductor of the coaxial cable 20 is used as the ground potential portion similarly to the end face and surface thereof. .

The coaxial cable 20 attached to the end face 11 of the conductor plate 10 ′ is configured to feed power by pulling out only the central conductor 24, for example, on the back surface of the conductor plate 10 ′ as in the example of FIG. Alternatively, a circuit component for antenna connection may be arranged on the surface of the conductor plate 10 ', and the circuit component may be connected to the central conductor 24 in a state insulated from the ground potential portion.
In FIG. 10, the configuration in which the central conductor 24 is drawn from the feeding point is omitted.
The length py in the y-axis direction and the length px in the x-axis direction of the conductor plate 10 'in the case shown in FIG. 10 and the length py2 from the bent portion 22 to the tip of the central conductor 24 are also shown in FIG. The antenna is configured to have a size similar to the current characteristic of the antenna shown.

Also in the case of the ultra-low profile inverted L antenna having the configuration of the second embodiment shown in FIG. 10, the impedance can be adjusted by setting the length of the central conductor 24 and the length of the outer conductor 26 of the coaxial cable 20. Yes, it can be 50Ω suitable for connection to a communication circuit. Therefore, the same good characteristics as the antenna of the first embodiment can be obtained, and a simple configuration that does not require a matching circuit can be realized.

[3. Example of Third Embodiment (FIG. 11)]
Next, an example of the third embodiment of the ultra-low profile inverted L antenna of the present invention will be described with reference to FIG.
The ultra-low profile inverted L-type antenna of the example of the third embodiment shown in FIG. 11 has a ground conductor plate and an antenna element formed on a surface 31 of a substrate 30 that is a dielectric in a planar manner. As an example, a coplanar line is used instead of a coaxial cable.
That is, as shown in FIG. 11, a ground potential portion 40 having a relatively large area is provided on the surface 31 of the substrate 30, and the ground potential portion 40 is provided at one end (right end side in FIG. 11) of the ground potential portion 40. The surface 31 is provided with no part.

Conductive patterns

41 and 42 connected by the ground potential portion 40 and the

connection locations

40a and 40b are arranged in parallel at a location where the ground potential portion 40 is not present, and between the two ground potential

conductive patterns

41 and 42. In addition, the conductive pattern 51 constituting the antenna element is disposed.

Each of the

conductive patterns

41, 42, 51 is bent 90 ° at the

bent portions

41 a, 42 a, 51 a and arranged parallel to the end surface of the ground potential portion 40. And the front-end | tip part 51b of the conductive pattern 51 which comprises an antenna element is made longer than the front-end | tip

parts

41b and 41b of the

conductive patterns

41 and 42 of the both sides.
The conductive pattern 51 constituting the antenna element is connected to an antenna connection circuit (not shown) at a connection location 51c close to the ground potential portion 40. For example, an antenna connection circuit unit is disposed on the front surface 31 or the back surface of the substrate 30 and connected to the conductive pattern 51 at the circuit unit and the connection location 51c.

The conductive pattern 51 is configured in this way, and the distance h between the end surface of the ground potential portion 40 and the conductive pattern 51 is set to the same value as the height h in the first embodiment, and forms the antenna element. the length L0 arranged parallel to and a length L ₁ arranged parallel to the conductive pattern 41 and a ground potential, adjusted in the same manner as the length L _0, L ₁ of the first embodiment Thus, the impedance can be set to 50Ω or the like. The length L ₀ is, for example, about ¼ of one wavelength of a signal to be transmitted / received.
Note that the length pym to the one end of the connection portion 51c of the conductive pattern 51 and the ground potential portion 40 and the length pyp to the other end also have the same relationship as the length described in the first embodiment. It is preferable to do so.

Also in the case of the configuration of the third embodiment, good characteristics similar to those of the antenna of the first embodiment can be obtained, and a simple configuration that does not require a matching circuit can be realized. In the case of the configuration of the third embodiment, each conductive pattern is configured on the same surface on the surface 31 of the substrate 30, so that the ground potential portion 40 and each of the

conductive patterns

41, 42,. 51 can be configured. For example, an antenna having good characteristics can be easily arranged on a circuit board of various cards (such as a PC card and a memory card) to be installed in a card slot of a personal computer device.

[4. Example of Fourth Embodiment (FIGS. 12 to 13)]
Next, an example of a fourth embodiment of the ultra-low profile inverted L-type antenna of the present invention will be described with reference to FIGS. FIG. 12 is a perspective view, and FIG. 13 is a plan view seen from above.
The ultra-low profile inverted L-type antenna of the example of the fourth embodiment shown in FIGS. 12 and 13 basically has an antenna element beside the ground conductor on the substrate, as in the third embodiment. However, the ground potential portion is on the back side of the substrate and the antenna element side is on the front side of the substrate.
That is, as shown in FIG. 12, a microstrip line 70 having a predetermined pattern is arranged on a surface 61 of a substrate 60, and the microstrip line 70 is extended to the end of the substrate 60 to form an antenna element portion 71. is there. The antenna element portion 71 is provided with a bent portion 71a in the middle, and is bent 90 ° at the bent portion 71a.

On the back surface 62 side of the substrate 60, a ground potential portion 80 having a relatively large area is disposed as shown by a broken line, and a conductive pattern 81 connected to the ground potential portion 40 is disposed in parallel so as to be conductive. The pattern 81 is also bent by 90 ° at the bent portion 81a.
Then, as shown in a plan view in FIG. 13, a conductive pattern 71 constituting the antenna element is arranged in the center of the conductive pattern 81 at the ground potential. The length L ₀ from the bent portion 71 a to the tip end portion 71 b of the conductive pattern 71 is longer than the length L ₁ from the tip end portion 81 b of the conductive pattern 81, and the impedance can be determined to be 50Ω by adjusting the length. Value. The length L ₀ is, for example, about ¼ of one wavelength of a signal to be transmitted / received.
The distance h between the end face of the ground potential portion 80 and the conductive pattern 71 is set to the same value as the distance h in the third embodiment, and one of the bent portion 71a of the conductive pattern 71 and the ground potential portion 80 is set. It is preferable that the length pym to the end and the length pyp to the other end have the same relationship as the length described in the first embodiment.
Also in the case of the configuration of the fourth embodiment, the same good characteristics as those of the antenna of the third embodiment can be obtained, and a simple configuration that does not require a matching circuit can be realized. The arrangement state of the microstrip line 70 connected to the conductive pattern 71 shown in FIG. 12 is an example, and various arrangement states can be considered according to the arrangement state of the circuit components to be connected.

[5. Example of Fifth Embodiment (FIG. 14)]
Next, an example of the fifth embodiment of the ultra-low profile inverted L antenna of the present invention will be described with reference to FIG.
In the ultra-low profile inverted L-type antenna of the example of the fifth embodiment shown in FIG. 14, a ground conductor plate is disposed on the surface 31 of the substrate 90, which is a dielectric, and only a height h from the ground conductor plate. In this example, conductive patterns are arranged at positions separated in the thickness direction of the substrate.
That is, as shown in FIG. 14, a ground potential portion 92 having a relatively large area is provided on almost the entire surface 91 of the substrate 90, and two conductors connected to the ground potential portion 92 are provided at predetermined positions of the ground potential portion 92. The

conductive patterns

94 and 95 are arranged in parallel in an upright state, and the conductive pattern 93 constituting the antenna element is arranged in an upright state between the two grounded

conductive patterns

94 and 95.

The

conductive patterns

94 and 95 are directly connected to the ground potential portion 92 at

connection portions

94c and 95c. The connection portion 93c of the conductive pattern 93 is not connected to the ground potential portion 92 but is connected to the communication circuit portion or the like by a coplanar line (not shown).
The

conductive patterns

93, 94, and 95 are bent at

bent portions

93a, 94a, and 95a so as to be parallel to the surface direction of the ground potential portion 92 at a height h. Furthermore, the

leading end portions

94 b and 95 b of the

conductive patterns

94 and 95 are shorter than the leading end portion 93 b of the conductive pattern 93.

With this configuration, as shown in FIG. 14, the length L ₀ from the connection portion 93 c of the conductive pattern 93 to the tip end portion 93 b of the conductive pattern 93 and the

tips

94 b and 95 b of the

conductive patterns

94 and 95 are set. adjust the length L _1, it can be adjusted impedance 50Ω like. The length L ₀ is, for example, about ¼ of one wavelength of a signal to be transmitted / received. Also, good characteristics can be obtained by setting the sizes pym, pyp, pxm, pxp of the ground potential portion 92. However, in the case of this example, the lengths pxm and pxp in the x-axis direction orthogonal to the longitudinal direction of the conductive pattern 93 are not equal, and the length in the x-axis direction is not uniform so that there is no deterioration in characteristics. It is necessary to select each parameter appropriately.

In the antennas of the embodiments described above, the antenna characteristics are improved by controlling the current on the conductor plate, for example, by providing a slit on the surface of the conductor plate at the ground potential. It may be.

[6. Example of sixth embodiment (FIGS. 15 and 16)]
Next, an example of a sixth embodiment of the ultra-low profile inverted L antenna of the present invention will be described with reference to FIGS. 15 and 16. In the sixth embodiment, the ground potential portion is not flat but has a structure in which conductor bars are assembled, and the configuration of the coaxial cable is the same as that in the example of FIG.

That is, as shown in FIG. 15, the parallel conductor frame 310 is configured by three ground conductor bars 311, 312, 313 and the ground conductor bars 314 orthogonal to each other. The three

ground conductor rods

311, 312, and 313 have the same length. Then, one end of the coaxial cable 320 is connected with an intersection of the ground conductor rod 311 and the ground conductor rod 314 of the parallel conductor frame 310 as a connection point 315. The coaxial cable is penetrated at a connection point 315 and further extended downward (not shown) to connect a transmission / reception circuit (not shown). At this connection location 315, the outer conductor 324 of the coaxial cable 320 is connected to the ground conductor rod 311 side to be at the ground potential. The center conductor 322 is connected to a power feeding unit of a transmission / reception circuit (not shown).

The coaxial cable 320 is bent at 90 ° at a bent portion 323 so that the tip side is parallel to the ground conductor bar 311. The coaxial cable 320 parallel to the ground conductor bar 311 has a configuration in which the central conductor 322 extends from the end 321 of the outer conductor 324.
The antenna in the example of FIG. 15 has the distance (height) h between the center conductor 322 and the ground conductor bar 311 of the coaxial cable 320 and the lengths L0, L1, pyp, pym, pxp, pxm in FIG. Set under the same conditions as. 2a is the diameter (a is a radius) of each of the conductor rods 311 to 314.

An example of each length of the antenna of FIG. 15 is shown as pxp = pxm = 35.0 mm, pyp = 115.0 mm, pym = 23.0 mm, h = 9.0 mm, L0 = 72.2 mm, L1 = 39. 3 mm, a = 1.5 mm, outer conductor 324 radius 1.095 mm, and central conductor 322 radius 0.255 mm.

FIG. 16 shows an example of the return loss characteristic of the antenna shown in FIG. 15 manufactured with this size. The horizontal axis represents frequency (GHz) and the vertical axis represents return loss characteristics (dB). The example of FIG. 16 is an example in the case of being configured as an antenna having characteristics with a center frequency around 1.06 GHz.
As in the antenna of FIG. 15, the ground potential portion is not flat and a structure in which the conductor rods are assembled can also provide good characteristics.

[7. Example of seventh embodiment (FIGS. 17 and 18)]
Next, an example of the seventh embodiment of the ultra-low profile inverted L-type antenna of the present invention will be described with reference to FIGS. The seventh embodiment is an example in which the antenna of the sixth embodiment is further developed as an antenna for receiving digital terrestrial television broadcasts.
That is, as shown in FIG. 17, the parallel conductor frame 410 is constituted by the

ground conductor rods

411, 412, 413 arranged in parallel with the ground conductor rods 414 orthogonal to each other. The three ground conductor bars 411, 412, and 413 have the same length. Then, one end of the coaxial cable 420 is connected with an intersection of the ground conductor rod 411 and the ground conductor rod 414 of the parallel conductor frame 410 as a connection point 415. At this connection location 415, the outer conductor 424 of the coaxial cable 420 is connected to the ground conductor rod 411 side to obtain a ground potential. The center conductor 422 is connected to a power feeding unit of a receiving circuit (not shown).

The coaxial cable 420 is bent at 90 ° at a bent portion 423 so that the tip end side is parallel to the ground conductor bar 411. The coaxial cable 420 parallel to the ground conductor rod 411 has a configuration in which the center conductor 422 is extended from the end 421 of the outer conductor.
Up to this point, the configuration is the same as that of the antenna shown in FIG. 15. However, in this embodiment, the waveguide 431 and the reflector 432 are arranged in the front and rear. That is, the waveguide 431 is disposed with the ground conductor rod 411 and the distance Dz in the z-axis direction shown in FIG. 17, and the reflector 432 is disposed with the ground conductor rod 411 and the distance Rz in the opposite direction to the z-axis direction. It is. The director 431 and the reflector 432 are fixed to the parallel conductive wire frame 410 side by a support (not shown). When viewed from the position where the ground conductor rod 411 is disposed, the side on which the director 431 is disposed is the transmitting station side of terrestrial digital television broadcasting.
In FIG. 17, the length of the director 431 is Dy, and the length of the reflector 432 is Ry.

FIG. 17 shows an example of the length of each antenna. As an example of receiving a signal having a broadcast frequency of 470 MHz to 710 MHz, pxp = pxm = 40 mm, pyp = 210 mm, pym = 44 mm, h = 24.5 mm, L0 = 130 mm, L1 = 41 mm, a = 1.5 mm, Dy = 208 mm, Dz = 80 mm, Ry = 320 mm, Rz = 82 mm.

FIG. 18A shows the directivity characteristics of the antenna of FIG. 17, and FIG. 18B shows the calculated values of the return loss characteristics.
As can be seen from the characteristics of FIGS. 18A and 18B, a sufficient gain is obtained in the transmission frequency band of terrestrial digital television broadcasting in Japan, which is 470 MHz to 710 MHz.
In the example of FIG. 17, one waveguide 431 and one reflector 432 are disposed. However, for example, a plurality of waveguides 431 may be disposed at a predetermined interval. . Alternatively, a plurality of reflectors 432 may be arranged.
Moreover, you may comprise the parallel conducting wire frame 410, the waveguide 431, and the reflector 432 with a conductor board.

[8. Example of Eighth Embodiment (FIGS. 19 to 21)]
Next, an eighth embodiment of the ultra-low profile inverted L antenna of the present invention will be described with reference to FIGS. 19 to 21. FIG. The eighth embodiment is an example of a circularly polarized antenna for an RFID (Radio Frequency IDentification) reader / writer, for example, an antenna that handles a circularly polarized signal in the 2.4 GHz band.
A conductor plate 510 having a ground potential portion on the surface is prepared, and a connection point 521 connecting one end of the coaxial cable 520 is provided at a predetermined position on the surface of the conductor plate 510. The coaxial cable 520 includes a center conductor 524 and an outer conductor 527, and the outer conductor 527 is electrically connected to the ground potential portion.

The coaxial cable 520 having one end connected to the connection portion 521 is bent 90 ° with a predetermined distance h away from the surface of the conductor plate 510 as a bent portion 522, and the end of the bent coaxial cable 520 is bent. The side is arranged so as to be parallel to the surface of the conductor plate 510.

The coaxial cable 520 that is bent at the bent portion 522 and extends in parallel with the conductor plate 510 extends by extending only the center conductor 524 from the outer conductor end 523, and further, a bent portion 525 in the middle of the drawn center conductor 524. The center conductor tip 526 is bent at 90 ° horizontally. By being bent horizontally, the central conductor 524 ahead of the outer conductor end 523 is in a state where the parallelism with the conductor plate 510 is maintained. In FIG. 19, the length from the bent portion 525 to the center conductor tip 526 is a.

In addition to the coaxial cable 520, one end of the conductor rod 530 is connected to the connection portion 531 of the conductor plate 510. The conductor rod 530 is electrically connected to the ground potential portion on the surface of the conductor plate 510.
The conductor bar 530 is bent at 90 ° horizontally at the bent portion 532, and the tip of the bent portion 532 is parallel to the distal end portion 526 of the center conductor 524 with the parallel portion 533. The height at which the conductor rod 530 is bent at the bent portion 532 is set equal to the height h of the coaxial cable 520, for example. The length from the bent portion 532 to the tip of the parallel portion 533 and _{L 2,} a parallel portion 533, the distance between the tip portion 526 of the center conductor 524 and _{C 1.}

An example of each length of the antenna of FIG. 19 is shown as pxp = 23.0 mm, pxm = 31.2 mm, pyp = 46.0 mm, pym = 6.0 mm, h = 5.5 mm, L ₀ = 27. 5 mm, L ₁ = 19.5 mm, L ₂ = 25.2 mm, a = 3.5 mm, and C ₁ = 12.5 mm.

FIG. 20 shows an example of the return loss characteristic and the axial ratio characteristic of the antenna shown in FIG. 19 manufactured with this size. The horizontal axis is frequency (GHz), the left side of the vertical axis is the return loss characteristic (dB), and the right side of the vertical axis is the axial ratio characteristic (dB). The thin solid line in the figure shows the return loss characteristic obtained by calculation, the thick solid line shows the measured return loss characteristic, and the broken line shows the calculated axial ratio characteristic.
FIG. 21 shows a calculated value of the radiation electric field directivity pattern at 2.45 GHz. RHCP represents right-hand circular polarization, and LHCP represents left-hand circular polarization. As can be seen from these characteristics, a circularly polarized antenna with good characteristics can be obtained.

[6. Application example of antenna of each embodiment (FIGS. 22 and 23)]
22 and 23 are diagrams showing the arrangement state of the low-position inverted L-shaped antenna of each example of the present embodiment.
FIG. 22 shows an example applied to an antenna device provided in a wireless LAN base station.
In the case of the example of FIG. 42, the wireless LAN base station antenna 100 is assumed to be composed of a cylindrical portion 110 and a plurality of protruding plate portions 120 arranged around the cylindrical portion 110. At this time, the coaxial cable 111 is arranged around the cylindrical portion 110 in the state shown in FIG. 3 and the like, the central conductor 112 is exposed, and is arranged in parallel with the circumference of the cylindrical portion 110. This arrangement state is, for example, the arrangement state shown in FIG.
Further, the coaxial cable 121 is disposed on the end surface of the protruding plate portion 120 so that the central conductor 122 is exposed, and is disposed in parallel with the end surface of the protruding plate portion 120. This arrangement state is, for example, the arrangement state shown in FIG.
With this configuration, it is possible to arrange a plurality of antennas around the wireless LAN base station antenna 100. In the case of the example shown in FIG. 22, the same configuration may be used instead of each coaxial cable, such as a Copnar line or a microstrip line.

FIG. 23 shows an example of positions where the antennas of each example of the present embodiment are arranged on the airplane 200.
In the example shown in FIG. 23, the antenna mounting positions 201 and 202 on the upper and lower sides of the fuselage of the airplane 200 and the antenna mounting positions 203 and 204 on the tip of the main wing or tail wing may be used. Or you may install in another position.
22 and 23 show preferred examples of application examples, and it goes without saying that the antenna of the example of this embodiment can be applied to other various wireless communication antennas.

DESCRIPTION OF SYMBOLS 1 ... Signal source, 2 ... Coupler, 3 ... Phase shifter, 4 ... Conductor plate, 5, 6 ... Coaxial cable, 5a, 6a ... Center conductor, 7 ... Conductor plate, 8 ... Inverted L-type element, 10 ... Conductor plate 11 ... Conductor plate end face, 20 ... Coaxial cable, 20a ... Hole, 21 ... Connection point, 22 ... Bending point, 23 ... Outer conductor end, 24 ... Center conductor, 24a ... Center conductor tip, 25 ... Insulator, 26 ... outer conductor, 30 ... substrate (dielectric), 31 ... surface, 40 ... ground potential part, 40a, 40b ... connection place, 41, 42 ... conductive pattern (ground potential part), 41a, 42a ... bent part, 41b , 41b ... tip part, 51 ... conductive pattern, 51a ... bent part, 51b ... tip part, 51c ... connection part, 60 ... substrate, 61 ... surface, 62 ... back surface, 70 ... microstrip line, 71 ... antenna element part, 71a ... bent portion, 71b ... tip, 8 ... ground potential part, 80a, 80b ... connection place, 81 ... conductive pattern (ground potential part), 81a ... bent part, 81b ... tip part, 90 ... substrate, 91 ... surface, 92 ... ground potential part, 93, 94, 95 ... conductive pattern, 93a, 94a, 95a ... bent portion, 93b, 94b, 95b ... tip, 93c, 94c, 95c ... connection location, 100 ... base station antenna for wireless LAN, 110 ... cylindrical portion, 111 ... coaxial cable , 112 ... center conductor, 120 ... projecting plate part, 121 ... coaxial cable, 122 ... center conductor, 200 ... airplane, 201, 202, 203, 204 ... antenna mounting position, 310 ... parallel conductor frame, 311, 312, 313 314, ground conductor bar, 315, connection location, 320, coaxial cable, 321, outer conductor end, 322, center conductor, 323, bent point. 324 ... Outer conductor, 410 ... Parallel conductor frame, 411, 412, 413, 414 ... Ground conductor bar, 415 ... Connection point, 420 ... Coaxial cable, 421 ... Outer conductor end, 422 ... Center conductor, 423 ... Bending point 424 ... outer conductor, 431 ... waveguide, 432 ... reflector, 510 ... conductor plate, 520 ... coaxial cable, 521 ... connection point, 522 ... bent point, 523 ... outer conductor end, 524 ... center conductor, 525 ... bent portion, 526 ... tip portion, 530 ... conductor rod, 531 ... connection portion, 532 ... bent portion, 533 ... parallel portion

Claims

In an inverted L-type antenna that is connected to a feeder line of a predetermined impedance value and performs transmission or reception in a frequency band centered on a specific frequency,
A ground conductor surface provided on the front surface or the back surface;
An outer conductor having a base end connected to a predetermined portion of the ground conductor surface, and an inner conductor sandwiched between the outer conductors and disposed with a gap between them and having a distal end extending from the outer conductor. ,
The outer conductor and the inner conductor are bent at a predetermined distance away from a predetermined location on the ground conductor surface, and are arranged in parallel near the ground conductor surface,
The power supply is configured by connecting the power supply line to the inner conductor,
The predetermined distance is a distance of about 1/30 of one wavelength of the signal of the specific frequency,
The length from the bent portion of the inner conductor to the tip is set to about ¼ of one wavelength of the signal of the specific frequency, and from the length of the inner conductor and the bent portion of the outer conductor. In setting with the length to the tip of the outer conductor, to match the impedance value of the feeder line,
The grounding conductor surface has a length in a direction parallel to the longitudinal direction of the inner conductor, a length from the predetermined location to one end toward the tip end side of the inner conductor, and from the predetermined location to the inner conductor. An inverted L-type antenna in which the length to the other end on the side opposite to the tip side is set so that a current flows in a direction from the bent portion of the inner conductor toward the tip.
The inverted L-shaped antenna according to claim 1,
The outer conductor and the inner conductor are inverted L-type antennas configured by a coplanar line or a microstrip line in which an inner conductor and an outer conductor are arranged at a predetermined interval.
The inverted L-shaped antenna according to claim 1,
The said outer conductor and the said inner conductor are reverse L type antennas comprised by the outer conductor and inner conductor of a coaxial cable.
The inverted L-type antenna according to any one of claims 1 to 3,
An inverted L-shaped antenna in which a predetermined portion connecting the ground conductor surface and the outer conductor is an end surface of the ground conductor surface.
The inverted L-shaped antenna according to claim 1,
An inverted L-type antenna in which the length from the predetermined portion to one end and the other end is made equal as the length of the ground conductor surface in a direction orthogonal to the longitudinal direction of the inner conductor.
The inverted L-shaped antenna according to claim 1,
An inverted L-shaped antenna configured by combining a plurality of conductor rods as the ground conductor surface.
The inverted L-shaped antenna according to claim 6,
An inverted L-type antenna in which a director and a reflector are arranged at positions in front of and behind a ground conductor surface configured by combining a plurality of conductor rods.
The inverted L-shaped antenna according to claim 1,
An inverted L-type antenna in which a tip of the inner conductor is bent horizontally and a conductor different from the outer conductor and the inner conductor is arranged in parallel with the bent inner conductor.