BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a view showing an example of a waveguide apparatus in the case where the vibration directions of input/output polarized waves of waveguides are horizontal to each other;
FIG. 2 is a view showing an example of a waveguide apparatus in the case where the vibration directions of input/output polarized waves of waveguides are perpendicular to each other;
FIG. 3 is a view showing an exemplary embodiment of a waveguide apparatus of the present invention in the case where the vibration directions of input/output polarized waves of waveguides are horizontal to each other;
FIG. 4 is a view showing another exemplary embodiment of the waveguide apparatus of the present invention in the case where the vibration directions of input/output polarized waves of the waveguides are perpendicular to each other;
FIG. 5 is a perspective view of the waveguide apparatus of the present invention shown in FIG. 3 when viewed from the direction of A;
FIG. 6 is a perspective view of the waveguide apparatus of the present invention shown in FIG. 4 when viewed from the direction of B;
FIG. 7 is a view showing the result in which the reflection characteristic of an electric field horizontally polarized wave in an exemplary embodiment shown in FIG. 3 is measured; and
FIG. 8 is a view showing the result in which the reflection characteristic of an electric field vertically polarized wave in an exemplary embodiment shown in FIG. 4 is measured.
EXEMPLARY EMBODIMENT
Referring to FIG. 3, there is illustrated waveguide apparatus comprising waveguide 101 serving as a first waveguide, waveguide 102 serving as a second waveguide, and polarization transformation circuit 103. Moreover, polarization transformation circuit 1021 is embedded within waveguide 102. In this case, waveguides 101 and 102 are disposed so that the vibration directions of polarized waves that passed through the respective waveguides are horizontal to each other, and respective waveguides 101 and 102 are connected through polarization transformation circuit 103.
Referring to FIG. 4, there is illustrated the waveguide apparatus, which has a configuration similar to the FIG. 3, and which comprises waveguide 101 serving as the first waveguide, waveguide 102 serving as the second waveguide, and polarization transformation circuit 103. Moreover, polarization transformation circuit 1021 is embedded within waveguide 102. In this case, waveguides 101 and 102 are disposed so that the vibration directions of polarized waves that passed through respective waveguides 101 and 102 are perpendicular to each other, and the respective waveguides are connected through polarization transformation circuit 103.
Polarization transformation circuit 1021 shown in FIGS. 3 and 4 is embedded within waveguide 102 in the state rotated in advance at a suitable angle where impedance matching between waveguides 101 and 102 can be performed only by rotating polarization transformation circuit 103 at a suitable angle. The angle where polarization transformation circuit 1021 is rotated in advance is based on the reflection coefficients of waveguides 101 and 102. Thus, even in the case where waveguides 101 and 102 as shown in FIG. 3 are disposed so that the vibration directions of polarized waves that passed through respective waveguides 101 and 102 are horizontal to each other, it is possible to perform impedance matching between waveguides 101 and 102. Moreover, even in the case where waveguides 101 and 102 as shown in FIG. 4 are disposed so that the vibration directions of polarized waves that passed through the respective waveguides are perpendicular to each other, it is possible to perform impedance matching between waveguides 101 and 102. Namely, as a result of the fact that polarization transformation circuit 1021 is embedded within waveguide 102 in the state rotated in advance at a suitable angle, this is sufficient for performing impedance matching in an electric field horizontally polarized wave and in an electric field vertically polarized wave in order to only rotate polarization transformation circuit 103.
In this example, the lengths of polarization transformation circuit 103 and polarization transformation circuit 1021 are set in advance to ¼ of the waveguide wavelength. Thus, the phase difference at reflection becomes equal to 180 degrees so that the reflection characteristic becomes satisfactory. Moreover, even in the case where the length of polarization transformation circuit 103 is set to ¼ of the waveguide wavelength and the length of polarization transformation circuit 1021 is set to ¾ of the waveguide wavelength, phase difference at reflection becomes equal to 180 degrees so that the reflection characteristic becomes satisfactory. Further, even in the case where the lengths of polarization transformation circuit 103 and polarization transformation circuit 1021 are set to ¾ of the waveguide wavelength, phase difference at reflection becomes equal to 180 degrees so that the reflection characteristic becomes satisfactory.
An angle rotated when polarization transformation circuit 1021 shown in FIGS. 3 and 4 is embedded within waveguide 102 will now be described.
As shown in FIG. 5, when the waveguide apparatus of the present invention shown in FIG. 3 is viewed from the direction of A, polarization transformation circuit 1021 is embedded within waveguide 102 in the state rotated at an angle θ1 relative to waveguide 101, polarization transformation circuit 103 and waveguide 102.
As shown in FIG. 6, when the waveguide apparatus of the present invention shown in FIG. 4 is viewed from the direction of B, polarization transformation circuit 1021 is embedded in the state rotated at an angle of θ1 relative to waveguide 102. Moreover, an angle that polarization transformation circuit 1021 and polarization transformation circuit 103 form is assumed to be θ2. Further, polarization transformation circuit 103 is rotated at an angle θ3 relative to waveguide 101.
In FIGS. 5 and 6, respective angles θ1 to θ3 are set based on the reflection characteristic which will be described later. As an angle for obtaining reflection characteristic which will be described later,
θ3:θ2:θ1=1:√2:1
is mentioned as an example. In this case, θ1=about 26°, θ2=about 38° and θ3=about 26° are respectively optimum angles.
In the reflection characteristics of the electric field horizontally polarized wave in an exemplary embodiment shown in FIG. 3, as shown in FIG. 7, within the range from 0.95 f0 to 1.05 f0 in which the frequency band has a relative bandwidth 10% of polarization frequency f0, the reflection coefficient is below −30 dB which is the target value in the present invention. From this result, it is seen that sufficient reflection characteristics can be obtained in the electric field horizontally polarized wave. In this example, angle θ1 shown in FIG. 5 is set to about 26°. In this case, the abscissa indicates the frequency (GHz) of the polarized wave, and the ordinate indicates the reflection coefficient (dB).
In the reflection characteristic of the electric field vertically polarized wave in an exemplary embodiment shown in FIG. 4, as shown in FIG. 8, within the range from 0.95 f0 to 1.05 f0 in which the frequency band has a relative bandwidth 10% of the polarization frequency f0, the reflection coefficient is below −30 dB which is the target value in the present invention. From this result, it is seen that sufficient reflection characteristics can be obtained also in the electric field vertically polarized wave. In this example, angles θ1, θ2 and θ3 shown in FIG. 6 are respectively set to about 26°, about 38° and about 26°. In this case, the abscissa indicates the frequency (GHz) of the polarized wave, and the ordinate indicates the reflection coefficient (dB).
It is to be noted that the relative bandwidth which is the range for determining whether or not the reflection coefficient is suitable can be expanded depending upon the conditions such as the frequency used and the lengths of waveguides 101, 102, etc. For this reason, the above-described suitable angles also vary in accordance with such conditions. Namely, it is necessary to set, as an optimum angle, angles in which the reflection coefficient in the relative bandwidth that correspond to the use condition of the waveguide apparatus at that time is suitable.
As explained above, in the present invention, from among two polarization transformation circuits 103, 1021 which connect waveguides 101 and 102, polarization transformation circuit 1021 is embedded within waveguide 102 in the state rotated at an angle set, based on the reflection coefficient within the waveguide. For this reason, in the case where the vibration direction of a polarized wave that passed through waveguide 101 and the vibration direction of a polarized wave that passed through waveguide 102 are horizontal to each other, it is possible to perform impedance matching between waveguides 101 and 102 just by rotating polarization transformation circuit 103 by a suitable angle. Moreover, also in the case where the vibration direction of a polarized wave that passed through waveguide 101 and the vibration direction of a polarized wave that passed through waveguide 102 are perpendicular to each other, it is possible to perform impedance matching between waveguides 101 and 102 just by rotating polarization transformation circuit 103 by a suitable angle. Thus, the number of parts can be reduced through the integration of parts and polarization wave switching work can be facilitated.
Moreover, any other polarization transformation circuit may be disposed between waveguides 101 and 102.
Further, a polarization transformation circuit whose length is set to the length of ¼ of each waveguide wavelength of waveguides 101 and 102 may be embedded within waveguide 102, and the length of the other polarization transformation circuit may be set to ¼ of each waveguide wavelength of waveguides 101 and 102.
Further, a polarization transformation circuit whose length is set to the length of ¾ of each waveguide wavelength of waveguides 101 and 102 may be embedded within waveguide 102, and the length of the other polarization transformation circuit may be set to ¼ of each waveguide wavelength of waveguides 101 and 102.
In addition, a polarization transformation circuit whose length is set to the length of ¾ of each waveguide wavelength of waveguides 101 and 102 may be embedded within waveguide 102, and the length of the other polarization transformation circuit may be set to ¾ of each waveguide wavelength of waveguides 101 and 102.
While an exemplary embodiment of the present invention has been described in specific terms, such description is for illustrative purpose only, and it is to be understood that changes and variations may be made without departing from the spirit or scope of the following claims.
Patent Application
20080068274
