Waveguide mode converter and method using same

• US 4,956,620 A
• Filed: 07/17/1989
• Issued: 09/11/1990
• Est. Priority Date: 07/17/1989
• Status: Expired due to Fees

• Current Assignee: United States Of America As Represented By The Department Of Energy
• Original Assignee: United States Department of Energy (Government of the United States of America)
• Inventors: Moeller, Charles P.
• Primary Examiner(s): Healy, Brian
• Application Number:
  US07/381,756
• Time in Patent Office: 421 Days
• Field of Search: 333/21 R, 333/242, 333/241, 350/96.10, 350/96.15, 350/96.29, 350/96.30, 350/320
• US Class Current: 333/21.00R
• CPC Class Codes: H01P 1/16 for mode selection, e.g. mode suppression or mode promotion; for mode conversion
• CPC Class Codes: H01P 3/123 with a complex or stepped cross-section, e.g. ridged or grooved waveguides H01P3/14 takes precedence

Abstract

A waveguide mode converter converts electromagnetic power being transmitted in a TE_0n or a TM_0n mode, where n is an integer, to an HE₁₁ mode. The conversion process occurs in a single stage without requiring the power to pass through any intermediate modes. The converter comprises a length of circular corrugated waveguide formed in a multiperiod periodic curve. The period of the curve is selected to couple the desired modes and decouple undesired modes. The corrugation depth is selected to control the phase propagation constant, or wavenumbers, of the input and output modes, thereby preventing coherent coupling to competing modes. In one embodiment, both the period and amplitude of the curve may be selectively adjusted, thereby allowing the converter to be tuned to maximize the conversion efficiency.

Claims

1. Waveguide mode converting apparatus for converting a first mode of transmission of electromagnetic power at a given free space wavelength to a second mode of transmission at the same wavelength, said apparatus including a length of circular corrugated waveguide of predetermined inner diameter and annular corrugations formed in a multiperiod periodic planar curve with a period substantially equal to 2π

divided by the difference in axial wavenumbers of the respective first and second modes of transmission in said waveguide.

2. Apparatus according to claim 1 wherein the physical depth of said corrugations substantially minimizes the coupling of power to modes of transmission other than said second mode of transmission.

3. Apparatus according to claim 2 wherein said physical depth of said corrugations is between 1/30 and 14/30 of said wavelength, exclusive of physical depths near 1/4 said wavelength.

4. Apparatus according to claim 3 wherein said physical depth of said corrugations is about 1/8 said wavelength.

5. Apparatus according to claim 3 wherein said physical depth of said corrugation is about 3/8 said wavelength.

6. Apparatus according to claim 1 wherein said annular corrugations are evenly spaced.

7. Apparatus according to claim 6 wherein the spacing of said corrugations is less than half said wavelength.

8. Apparatus according to any one of claims 1-7 further including an input section of circular corrugated waveguide of said predetermined inner diameter and having annular corrugations increasing in depth in the direction of transmission from zero at the input end of said input section to the depth of corrugations in said length of waveguide, and an output section of circular corrugated waveguide of said predetermined inner diameter and having annular corrugations gradually changing in depth in the direction of transmission to substantially 1/4 said wavelength at the output end of said output section from the depth of corrugations in said length of waveguide, said input section preceding and said output section following said length of waveguide in the direction of transmission.

9. Apparatus according to any one of claims 1-7 further including means for adjusting the period of said curve and its amplitude.

10. Apparatus according to claim 1 wherein said curve is cyclic with symmetric cycles.

11. Apparatus according to claim 1 wherein said curve is substantially sinusoidal.

12. A tunable waveguide mode converter comprising:

a length of circular corrugated waveguide formed into a multiperiod periodic planar curve, the periods of said multiperiod curve having a period P measured along a longitudinal axis of the waveguide, and said periodic planar curve having an amplitude A measured transverse to the longitudinal axis;

first adjustment means for selectively adjusting said period P; and

means for coupling electromagnetic power having a free space wavelength λ

in a first transmission mode to a first end of said length of circular waveguide;

said period P being adjusted with said first adjustment means to couple power of said first transmission mode to a second transmission mode and decouple power of said first transmission mode to modes other than said second transmission mode.

13. The converter as set forth in claim 12 further including second adjustment means for selectively adjusting said amplitude A, said amplitude A being adjusted with said second adjustment means to maximize the power converted to said second transmission mode from said first transmission mode.

14. The converter as set forth in claim 13 wherein said first and second adjustment means comprise:

a support bar; and

means for holding selected segments of said corrugated waveguide in respective spaced relationship relative to said support bar;

at least one of said holding means including means for adjusting the spaced relationship between its respective corrugated waveguide segment and said support bar.

15. The converter as set forth in claim 14 wherein said plurality of holding means each comprise a ring having a base, said ring having an inside diameter that snugly fits around said corrugated waveguide, said base including means for securing said ring to said support bar.

16. The converter as set forth in claim 15 wherein said inside diameter of said ring varies from a first maximum value at its ends to a second minimum value in between its ends.

17. The converter as set forth in claim 12 wherein said corrugations of said corrugated waveguide are annular corrugations having a specified physical corrugation depth, said specified physical depth being a prescribed percentage of the wavelength λ

of the electromagnetic power applied to said waveguide.

18. The converter as set forth in claim 17 wherein said prescribed corrugation depth is less than 1/4 λ

and greater than about 1/30 λ

.

19. The converter as set forth in claim 18 wherein, said prescribed corrugation depth is greater than 1/4 λ

and less than about 14/30 λ

.

20. The converter as set forth in claim 17 wherein said first transmission mode of said electromagnetic power applied to the first end of said waveguide comprises a TE₀₁ or TM₀₂ mode, and wherein said second transmission mode comprises an HE₁₁ mode.

21. A method for converting electromagnetic power at a given free space wavelength from a TE₀₁ or TM₀₂ input mode, to an HE₁₁ output mode, said method comprising applying said power in said input mode to the input end of a length of circular corrugated waveguide of given inner diameter and annular corrugations formed in a multiperiod periodic planar curve, adjusting the period of said curve to maximize power radiating from the output end of said length of waveguide in said HE₁₁ output mode, and adjusting the amplitude of said curve to minimize the power radiating from the output end of said length of waveguide in said input mode, thereby achieving maximum conversion to the HE₁₁ mode.