Synthetic heterodyne demodulator circuit
AssigneeLitton Systems, Inc.
InventorMichael R. Layton
Life of this patent
Estimating the term…
Abstract
An improved synthetic heterodyne demodulator circuit. The circuit is arranged to accept the output signal s(t) from an interferometric sensor with large amplitude sinusoidal phase modulation (phase-generated carrier). The phase modulation amplitude is adjusted such that a selected pair of odd and even carrier harmonics are equal. The quadrature signal components are first extracted from the phase-generated carrier using standard homodyne techniques. The quadrature signal components are then used to AM-modulate a pair of equal-amplitude quadrature carrier components at an arbitrary frequency .omega..sub.c, and summed. The result is a conventional PM modulated carrier which can be demodulated using standard FM techniques, followed by integration, to recover with high fidelity the sensed information.
Claims21
A method for recovering the phase modulated sideband .psi.(t) of the output signal s(t) from an interferometric fiber sensor with large amplitude carrier phase modulation, said signal being of the form s(t)=S.sub.o (1+.gamma.cos(Bsin .omega..sub.m t+.psi.(t))) where:
- S.sub.o =a dimensional constant;
- .gamma.=fringe visibility of the interferometer;
- B=phase modulation amplitude;
- and
- .omega..sub.m =phase modulation angular frequency comprising steps of:
- a) forming the in-phase and quadrature components of said signal;
- then
- b) lowpass filtering said in-phase and quadrature components to remove all modulation at .omega..sub.m ;
- then
- c) mixing said filtered quadrature component with a signal of the form sin .omega..sub.c t where .omega..sub.c is an arbitrary frequency;
- and
- d) mixing said filtered in-phase component with a signal of the form cos .omega..sub.c t;
- then
- e) summing said last-named signals to form a modulated signal;
- and
- f) demodulating said modulated signal to obtain .psi.(t).
A method for recovering the phase modulated sideband .psi.(t) of the output signal s(t) from an interferometric fiber sensor with large amplitude carrier phase modulation, said signal being of the from s(t)=S.sub.o (1 +.gamma.cos(Bsin .omega..sub.m t+.psi.(t))) where:
- S.sub.o =a dimensional constant;
- .gamma.=fringe visibility of the interferometer;
- B=phase modulation amplitude;
- and
- .omega..sub.m =phase modulation angular frequency comprising the steps of:
- a) removing the d.c. component of said signal;
- then
- b) mixing said signal with an AM modulated carrier of the form sin(N.omega..sub.m t)sin .omega..sub.c t where N is an odd integer and .omega..sub.c is arbitrary to create a first mixed signal;
- and
- c) mixing said signal with an AM modulated carrier of the form cos(M.omega..sub.m t)cos .omega..sub.c t where M is an even integer to create a second mixed signal;
- then
- d) summing said first and second mixed signals to form a modulated signal;
- then
- e) applying said modulated signal to a bandpass filter centered at .omega..sub.c ;
- and then
- f) demodulating said filtered modulated signal to obtain .psi.(t).
A method for recovering the phase modulated sideband .psi.(t) of the output signal s(t) from an interferometric fiber sensor with large amplitude carrier phase modulation, said signal being of the from s(t)=S.sub.o (1+.gamma.cos(Bsin .omega..sub.m t+.psi.(t))) where:
- S.sub.o =a dimensional constant;
- .gamma.=fringe visibility of the interferometer;
- B=phase modulation amplitude;
- and
- .omega..sub.m =phase modulation angular frequency comprising the steps of:
- a) removing the d.c. component of said signal;
- then
- b) mixing said signal with a phase-shift keyed carrier of the form sgn(sin N.omega..sub.m t)sin .omega..sub.c t where N is an odd integer and .omega..sub.c is arbitrary to create a first signal;
- and
- c) mixing said signal with a phase shift keyed carrier of the form sgn(cos M.omega..sub.m t)cos .omega..sub.c t where M is an even integer to create a second signal;
- then
- d) summing said first and second signals to form a modulated signal;
- then
- e) applying said modulated signal to a bandpass filter centered at .omega..sub.c ;
- and then
- f) demodulating said filtered modulated signal to obtain .psi.(t).
A method for recovering the phase modulated sideband .psi.(t) of the output signal s(t) from an interferometric fiber sensor with large amplitude carrier phase modulation, said signal being of the form s(t)=S.sub.o (1+.gamma.cos(Bsin .omega..sub.m t+.psi.(t))) where:
- S.sub.o =a dimensional constant;
- .gamma.=fringe visibility of the interferometer;
- B=phase modulation amplitude;
- and
- .omega..sub.m =phase modulation angular frequency comprising the steps of:
- a) removing the d.c. component of said signal;
- then
- b) mixing said signal with an AM modulated carrier of the form cos M.omega..sub.m t cos .omega..sub.c t+sin N.omega..sub.m t sin .omega..sub.c t where N is an odd integer, M is an even integer and .omega..sub.c is arbitrary to form a modulated signal;
- then
- c) applying said modulated signal to a bandpass filter centered at .omega..sub.c ;
- and then
- d) demodulating said filtered modulated signal to obtain .psi.(t).
Apparatus for recovering the phase modulated sideband .psi.(t) of the output signal s(t) from an interferometric fiber sensor with large amplitude carrier phase modulation, said signal being of the form s(t)=S.sub.o (1+cos(Bsin .omega..sub.m t+.psi.(t))) where:
- S.sub.o =a dimensional constant;
- .gamma.=fringe visibility of the interferometer;
- B=phase modulation ampilitude;
- and
- .omega..sub.m =phase modulation angular frequency comprising, in combination:
- a) means for receiving said signal;
- b) means engaged to said last-named means for forming the in-phase and quadrature components of said signal;
- c) means for removing all .omega..sub.m modulation from said in-phase and quadrature components;
- d) means for mixing said first quadrature component with a signal of the form sin .omega..sub.c t where .omega..sub.c is an arbitrary frequency;
- e) means for mixing said in-phase component with a signal of the form cos .omega..sub.c t;
- f) means for summing said last-named signals to form a modulated signal;
- and
- g) means for demodulating said modulated signal to obtain .psi.(t).
Apparatus for recovering the phase modulated deband .psi.(t) of the output signal s(t) from an interferometric fiber sensor with large amplitude carrier phase modulation, said signal being of the form s(t)=S.sub.o (1+.gamma.cos(Bsin .omega..sub.m t+.psi.(t))) where:
- S.sub.o =a dimensional constant;
- .gamma.=fringe visibility of the interferometer;
- B=phase modulation amplitude;
- and
- .omega..sub.m =phase modulation angular frequency comprising, in combination:
- a) means for receiving said signal;
- b) means for removing the d.c. component of said signal;
- c) means for mixing said signal with an AM modulated carrier of the form sin N.omega..sub.m tsin .omega..sub.c t where N is an odd integer and .omega..sub.c is an arbitrary frequency to form a first mixed signal;
- and
- d) means for mixing said signal with an AM modulated carrier of the form cos M.omega..sub.m t cos .omega..sub.c t where M is an even integer to form a second mixed signal;
- e) means for summing said first and second mixed signals;
- f) a bandpass filter centered at .omega..sub.c arranged to accept said summed signal;
- and
- g) means for demodulating said filtered signal to obtain .psi.(t).
Apparatus for recovering the phase modulated sideband .psi.(t) of the output signal s(t) from an interferometric fiber sensor with large amplitude carrier phase modulation, said signal being of the form s(t)=S.sub.o (1+.gamma.cos(Bsin .omega..sub.m t+.psi.(t)) where:
- S.sub.o =a dimensional constant;
- .gamma.=fringe visibility of the interferometer;
- B=phase modulation amplitude;
- and
- .omega..sub.m =phase modulation angular frequency comprising, in combination:
- a) means for receiving said signal;
- b) means for removing the d.c. component of said signal;
- c) means for mixing said signal with a phase-shift keyed carrier of the form sgn(sin N.omega..sub.m t)sin .omega..sub.c t where N is an odd integer and .omega..sub.c is an arbitrary frequency to form a first signal;
- and
- d) means for mixing said signal with a phase-shift keyed carrier of the form sgn(cos M.omega..sub.m t)cos .omega..sub.c t where M is an even integer to form a second signal;
- e) means for summing said first and second signals;
- f) a bandpass filter centered at .omega..sub.c arranged to accept said summed signal;
- and
- g) means for demodulating said filtered signal to obtain .psi.(t).
Apparatus for recovering the phase modulated sideband .psi.(t) of the output signal s(t) from an interferometric fiber sensor with large amplitude carrier phase modulation, said signal being of the form s(t)=S.sub.o (1+.gamma.cos(Bsin .omega..sub.m t+.psi.(t))) where:
- S.sub.o =a dimensional constant;
- .gamma.=fringe visibility of the interferometer;
- B=phase modulation amplitude;
- and
- .omega..sub.m =phase modulation angular frequency comprising, in combination:
- a) means for receiving said signal;
- b) means for removing the d.c. component of said signal;
- c) means for mixing said signal with an AM modulated carrier of the form sin N.omega..sub.m tsin .omega..sub.c t+cos M.omega..sub.m tcos .omega..sub.c t where N is an odd integer, M is an even integer and .omega..sub.c is an arbitrary frequency, to create modulated signal;
- and
- d) a bandpass filter centered at .omega..sub.c arranged to accept said modulated signal;
- and
- e) means for demodulating said modulated signal to obtain .psi.(t).
Dependencies are inferred from the claim text.