Method and system for down-converting an electromagnetic signal, and transforms for same, and aperture relationships

• US 7,515,896 B1
• Filed: 04/14/2000
• Issued: 04/07/2009
• Est. Priority Date: 10/21/1998
• Status: Expired due to Fees

• Current Assignee: ParkerVision, Inc.
• Original Assignee: ParkerVision, Inc.
• Inventors: Cook, Robert W., Rawlins, Gregory S., Bultman, Michael J., Sorrells, David F., Moses, Charley D. Jr., Looke, Richard C., Rawlins, Michael W.
• Primary Examiner(s): Bhattacharya; Sam
• Application Number:
  US09/550,644
• Time in Patent Office: 3,280 Days
• Field of Search: 455/313, 455/118, 455/323, 455/131, 455/130, 455/350, 455/76, 455/260, 455/191.1, 455/91, 455/182.1, 455/112, 327/113, 375/130, 375/152, 375/142, 375/143, 375/150, 375/316, 375/343
• US Class Current: 455/313
• CPC Class Codes: H03D 7/00 Transference of modulation from one carrier to another, e.g. frequency-changing H03D9/00, H03D11/00 take precedence; dielectric amplifiers, magnetic amplifiers, parametric amplifiers used as a frequency-changers H03F

Abstract

Methods, systems, and apparatuses, and combinations and sub-combinations thereof, for down-converting an electromagnetic (EM) signal are described herein. Briefly stated, in embodiments the invention operates by receiving an EM signal and recursively operating on approximate half cycles (½, 1½, 2½, etc.) of the carrier signal. The recursive operations can be performed at a sub-harmonic rate of the carrier signal. The invention accumulates the results of the recursive operations and uses the accumulated results to form a down-converted signal. In an embodiment, the EM signal is down-converted to an intermediate frequency (IF) signal. In another embodiment, the EM signal is down-converted to a baseband information signal. In another embodiment, the EM signal is a frequency modulated (FM) signal, which is down-converted to a non-FM signal, such as a phase modulated (PM) signal or an amplitude modulated (AM) signal.

Claims

1. A method for down-converting an electromagnetic signal, comprising the steps of:

(1) simultaneously down-converting and performing a matched filtering/correlating operation on a portion of an initially received carrier signal, wherein said down-converting and said performing a matched filtering/correlating operation are performed in a single operation;

(2) accumulating the result of the matched filtering/correlating operation of step (1); and

(3) repeating steps (1) and (2) for additional portions of the carrier signal,

wherein step (1) comprises the step of convolving an approximate half cycle of the carrier signal with a representation of itself.

2. The method according to claim 1, wherein step (1) comprises the step of multiplying said approximate half cycle of the carrier signal by itself over a predetermined time interval and integrating over the predetermined time interval.

3. The method according to claim 1, where S₀(t) is an output of the matched filtering/correlating operation, k is a constant, S_i(t) is said approximate half cycle of the carrier signal, and t₀−

0 is a predetermined time interval, and wherein step (1) comprises the step of processing said approximate half cycle of the carrier signal in accordance with;

$S_0<br><br>\left(t\right)=k<br><br>{\int <br><br>}_0^{t_0}<br><br>S_i^2<br><br>\left(t\right)<br><br><br><br>d<br><br>t.$

4. The method according to claim 1, where S₀(t) is an output of the matched filtering/correlating operation, k is a constant, kS_i(t₀−

τ

) is an impulse response of a matched filtering/correlating operator, to is a predetermined observation time, u(τ

) is a step function, and S_i(t−

τ

) is said approximate half cycle of the carrier signal, and wherein step (1) comprises the step of processing the approximate half cycle of the carrier signal in accordance with;

$S_0<br><br>\left(t\right)={\int <br><br>}_0^{\mathrm{\infty <br><br>}}<br><br>\left({\mathrm{kS}}_i<br><br>\left(t_0-\mathrm{\tau <br><br>}\right)<br><br>u<br><br>\left(\mathrm{\tau <br><br>}\right)\right)<br><br>S_i<br><br>\left(t-\mathrm{\tau <br><br>}\right)<br><br><br><br>d<br><br>\mathrm{\tau <br><br>}.$

5. The method according to claim 1, wherein step (2) comprises the step of transferring a portion of the energy contained in said approximate half cycle of the carrier signal to an energy storage device.

6. The method according to claim 1, wherein step (2) comprises the step of transferring a portion of the energy contained in said approximate half cycle of the carrier signal to a capacitive storage device.

7. The method according to claim 1, further comprising the step of:

(4) passing on the accumulation result of step (2) to a reconstruction filter.

8. The method according to claim 1, further comprising the step of:

(4) passing on the accumulation result of step (2) to an interpolation filter.

9. The method according to claim 1, wherein step (3) comprises the step of repeating steps (1) and (2) at a sub-harmonic rate of the carrier signal.

10. The method according to claim 1, wherein step (3) comprises the step of repeating steps (1) and (2) at an off-set of a sub-harmonic rate of the carrier signal.

11. The method according to claim 1, further comprising the step of:

(4) performing steps (1), (2), and (3) for positive approximate half cycles of the carrier signal and for inverted negative approximate half cycles of the carrier signal.