Phased array antenna and its phase calibration method
US-8957808-B2 · Feb 17, 2015 · US
US10601141B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10601141-B2 |
| Application number | US-201515315889-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jun 4, 2015 |
| Priority date | Jun 4, 2014 |
| Publication date | Mar 24, 2020 |
| Grant date | Mar 24, 2020 |
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An artificial magnet conductor includes a dielectric medium, basic cells, each being formed on a side of a front surface of the dielectric medium, and including a conductive patch pattern and a conductive loop pattern formed with a predetermined gap with the conductive patch pattern, a frequency selective surface on which the basic cells are periodically arranged on the front surface of the dielectric medium, and a conductive layer formed on a side of a rear surface of the dielectric medium. A phase change from an incident wave to a reflected wave with respect to the dielectric medium is set as an addition value in which a first phase change in the gap is added to a second phase change between the basic cell of the dielectric medium and the conductive layer. A thickness of the dielectric medium is calculated using the addition value.
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The invention claimed is: 1. An artificial magnet conductor comprising: a dielectric medium; basic cells, each being formed on a side of a front surface of the dielectric medium, and including a conductive patch pattern and a conductive loop pattern that is formed with a predetermined gap with the conductive patch pattern; a frequency selective surface on which the basic cells are periodically arranged on the front surface of the dielectric medium; and a conductive layer that is formed on a side of a rear surface of the dielectric medium, wherein a phase change from an incident wave to a reflected wave with respect to the dielectric medium is set as an addition value in which a first phase change in the gap is added to a second phase change between the basic cell of the dielectric medium and the conductive layer, and a thickness of the dielectric medium is set based on the addition value, and the thickness of the dielectric medium is greater than a distance of the gap when the thickness is calculated. 2. The artificial magnet conductor according to claim 1 , wherein the dielectric medium is a dielectric substrate. 3. The artificial magnet conductor according to claim 1 , wherein the thickness of the dielectric medium is set by a predetermined expression using the addition value. 4. The artificial magnet conductor according to claim 1 , wherein the addition value is an addition phase change amount in which the second phase change which is a phase rotation amount is added to the first phase change caused by capacitance which is formed by the gap. 5. The artificial magnet conductor according to claim 3 , wherein the predetermined expression is an expression that subtracts the first phase change from a phase change amount which is obtained based on an S parameter of the frequency selective surface and is required for the dielectric medium, calculates the second phase change which is obtained as the subtraction results, and calculates the thickness of the dielectric medium from the second phase change. 6. The artificial magnet conductor according to claim 1 , wherein the frequency selective surface is formed such that one of the conductive patch pattern and the conductive loop pattern has inductive reactance, and the other has capacitive reactance, at a predetermined frequency bandwidth. 7. The artificial magnet conductor according to claim 1 , wherein the thickness of the dielectric medium is set such that the artificial magnet conductor has frequency characteristics corresponding to a plurality of frequencies, change curves of a dielectric thickness and a phase in each of the plurality of frequencies are obtained, and the phase is within ±45° of the entirety of the plurality of frequencies. 8. The artificial magnet conductor according to claim 1 , wherein the conductive patch pattern is formed in a polygon, and the frequency characteristics of the frequency selective surface are adjusted by further increasing the number of apexes by cutting regions of apex portions of the polygon in a direction perpendicular to a line connecting the apexes to a center of the polygon. 9. An antenna reflector comprising: the artificial magnet conductor according to claim 1 , which is used as a reflection plate. 10. The antenna reflector according to claim 9 , wherein the artificial magnet conductor is provided to be detachable. 11. A method for calculating a thickness of a dielectric medium of an artificial magnet conductor including a dielectric medium; basic cells, each being formed on a side of a front surface of the dielectric medium, and including a conductive patch pattern and a conductive loop pattern that is formed with a predetermined gap with the conductive patch pattern; a frequency selective surface on which the basic cells are periodically arranged on the front surface of the dielectric medium; and a conductive layer that is formed on a side of a rear surface of the dielectric medium, the method comprising: setting a phase change from an incident wave to a reflected wave with respect to the dielectric medium, as an addition value in which a first phase change in the gap is added to a second phase change between the basic cell of the dielectric medium and the conductive layer; and calculating the thickness of the dielectric medium based on the addition value, wherein the thickness of the dielectric medium is greater than a distance of the gap when the thickness is calculated. 12. The method according to claim 11 , wherein the dielectric medium is a dielectric substrate. 13. The method according to claim 11 , wherein the thickness of the dielectric medium is set by a predetermined expression using the addition value. 14. The method according to claim 11 , wherein the addition value is an addition phase change amount in which the second phase change which is a phase rotation amount is added to the first phase change caused by capacitance which is formed by the gap. 15. The method according to claim 13 , wherein the predetermined expression is an expression that subtracts the first phase change from a phase change amount which is obtained based on an S parameter of the frequency selective surface and is required for the dielectric medium, calculates the second phase change which is obtained as the subtraction results, and calculates the thickness of the dielectric medium from the second phase change. 16. The method according to claim 11 , wherein the frequency selective surface is formed such that one of the conductive patch pattern and the conductive loop pattern has inductive reactance, and the other has capacitive reactance, at a predetermined frequency bandwidth. 17. The method according to claim 11 , wherein the thickness of the dielectric medium is set such that the artificial magnet conductor has frequency characteristics corresponding to a plurality of frequencies, change curves of a dielectric thickness and a phase in each of the plurality of frequencies are obtained, and the phase is within ±45° of the entirety of the plurality of frequencies. 18. The method according to claim 11 , wherein the conductive patch pattern is formed in a polygon, and the frequency characteristics of the frequency selective surface are adjusted by further increasing the number of apexes by cutting regions of apex portions of the polygon in a direction perpendicular to a line connecting the apexes to a center of the polygon.
formed by a conductive layer on an insulating support {(patch antennas H01Q9/0407; microstrip dipole antennas H01Q9/065; microstrip slot antennas H01Q13/106; transmission line microstrip antennas H01Q13/206; manufacturing reflecting surfaces using insulating material for supporting the reflecting surface H01Q15/142)} · CPC title
Substantially flat resonant element parallel to ground plane, e.g. patch antenna (dipole H01Q9/285; monopole H01Q9/40) · CPC title
Earthing means; Earth screens; Counterpoises · CPC title
Selective devices having photonic band gap materials or materials of which the material properties are frequency dependent, e.g. perforated substrates, high-impedance surfaces · CPC title
said selective devices being reconfigurable or tunable, e.g. using switches or diodes · CPC title
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