Device for wide-band spectral analysis of a signal of interest
View Patent ↗A wideband device for the spectral analysis of a signal of interest includes a source designed to generate the signal of interest; an optical splitter element designed to spatially split the signal of interest into a first signal and a second signal; a first frequency-shifting optical cavity comprising a first frequency shifter designed to shift the optical frequency of the first signal by a first frequency f 1 per round trip in the first cavity, the first cavity having a first trip time τ 1 ; a second frequency-shifting optical cavity comprising a second frequency shifter designed to shift the optical frequency of the second signal by a second frequency f 2 per round trip in the second cavity, the second cavity having a second trip time τ 2 ; the first and the second optical cavity being designed such that a maximum number of round trips of the signal in the first and the second cavity is equal to predetermined N; a detector designed to coherently detect the first signal transmitted by the first cavity and the second signal transmitted by the second cavity and generate a photocurrent proportional to a luminous intensity detected by the detector, an analog low-pass filter designed to filter frequencies of the photocurrent that are lower than min (f 1 /2, f 2 /2) a processor configured to compute a square modulus of the photocurrent filtered by the low-pass filter, from which a temporal representation of frequency information of the signal of interest is determined.
1. A wideband device (D) for the spectral analysis of a signal of interest comprising:
a source(S) designed to generate said signal of interest (Si);
an optical splitter element (ES) designed to spatially split said signal of interest into a first signal (V 1 ) and a second signal (V 2 );
a first frequency-shifting optical cavity (DBDF, BDF 1 ) comprising a first frequency shifter (AOM 1 ) designed to shift the optical frequency of the first signal by a first frequency f 1 per round trip in said first cavity, said first cavity having a first trip time τ 1 ;
a second frequency-shifting optical cavity (DBDF, BDF 2 ) comprising a second frequency shifter (AOM 2 ) designed to shift the optical frequency of the second signal by a second frequency f 2 per round trip in said second cavity, said second cavity having a second trip time τ 2 ;
the first and the second optical cavity being designed such that a maximum number of round trips of said signal in the first and the second cavity is equal to predetermined N;
a detector (PD) designed to coherently detect the first signal (W 1 ) transmitted by the first cavity and the second signal (W 2 ) transmitted by the second cavity and generate a photocurrent (Tr) proportional to a luminous intensity detected by said detector, a low-pass filter (LP) designed to filter frequencies of the photocurrent that are lower than min (f 1 /2, f 2 /2),
a processor (UT) configured to compute a square modulus of the photocurrent filtered by said low-pass filter, from which a temporal representation of frequency information of said signal of interest is determined, said frequency information being:
a real part of a fractional Fourier transform of said signal of interest, an order of said fractional Fourier transform being set by the value f 1 ×τ 1 −f 2 ×τ 2 when the first cavity and the second cavity are configured to verify the condition f 1 ×τ 1 +f 2 ×τ 2 , modulo 1 or
a power spectrum of said signal of interest when the first cavity and the second cavity are configured to verify the condition f 1 ×τ 1 =f 2 ×τ 2 modulo 1.
2. The device as claimed in claim 1 , wherein said source comprises a monochromatic continuous-wave laser (CW), an RF source (AM) designed to generate an RF signal s(t), and a modulator (Mod) designed to amplitude-modulate or phase-modulate, using said RF signal s(t), laser radiation generated by said continuous-wave laser, so as to form said signal of interest.
3. The device as claimed in claim 1 , wherein the analog low-pass filter (LP) is designed to filter frequencies of said photocurrent that are lower than min [N×|f 1 −f 2 |; f 1 /2; f 2 /2], when the first cavity and the second cavity are configured to verify the condition f 1 ×τ 1 =f 2 ×τ 2 modulo 1.
4. The device as claimed in claim 1 , wherein the first and the second cavity respectively comprise a first and a second amplifier (EDFA, EDFA 1 , EDFA 2 ) designed to compensate for the losses induced respectively by the first and the second cavity.
5. The device as claimed in claim 1 , wherein the first frequency shifter is a first acousto-optic modulator excited by a first local oscillator (OL 1 ) designed to vary said first shift frequency and wherein the second frequency shifter is a second acousto-optic modulator excited by a second local oscillator (OL 2 ) designed to vary said second shift frequency.
6. The device as claimed in claim 1 , wherein the first cavity comprises a first controllable delay line (DL 1 ) designed to vary the first trip time τ 1 and wherein the second cavity comprises a second controllable delay line (DL 2 ) designed to vary the second trip time τ 2 .
7. The device as claimed in claim 6 , comprising a single ring cavity (BDF), said device furthermore comprising:
a first coupler (C 1 ) designed to inject said first signal (V 1 ) into said single cavity in a first direction,
a second coupler (C 2 ) designed to inject said second signal (V 2 ) into said single cavity in a second direction,
said first cavity corresponding to the single cavity into which the first signal is injected in the first injection direction,
said second cavity corresponding to the single cavity into which the second signal is injected in the second injection direction,
said single ring cavity comprising:
a first circulator (CO 1 ) designed to direct the first signal to a first controllable delay line (DL 1 ) designed to vary the first trip time τ 1 and comprising said first frequency shifter (AOM 1 ),
a second circulator (CO 2 ) designed to direct the second signal to a second controllable delay line (DL 2 ) designed to vary the second trip time τ 1 and comprising said second frequency shifter (AOM 2 ),
a doped fiber amplifier (EDFA),
an optical bandpass filter (BP) configured to set said maximum number N of round trips.
8. The device as claimed in claim 1 , wherein the first and the second cavity are fiber ring cavities (BDF 1 , BDF 2 ) comprising respectively a first and a second doped fiber amplifier (EDFA 1 , EDFA 2 ) and a first and a second optical bandpass filter (BP 1 , BP 2 ) configured to set said maximum number N of round trips in the first and the second cavity.
9. The device as claimed in claim 8 , comprising stabilizing means (ST) for stabilizing the first and the second cavity that are designed to maintain, over time, the coherence of said first signal transmitted by the first cavity with said second signal transmitted by the second cavity.
10. The device as claimed in claim 1 , wherein the first and the second cavity are configured such that 1/|τ 1 −τ 2 |≥40 GHz.
11. The device as claimed in claim 1 , wherein the first and the second cavity are configured such that N is greater than 200.
12. A method for the spectral analysis of a signal of interest (Si) using a first frequency-shifting optical cavity (BDF 1 ) comprising a first frequency shifter (AOM 1 ) having a first trip time τ 1 and a second frequency-shifting optical cavity (BDF 2 ) comprising a second frequency shifter (AOM 2 ) having a second trip time τ 2 , a maximum number of round trips of said signal of interest in the first and the second cavity being equal to predetermined N, said method comprising the following steps:
A. generating said signal of interest;
B. spatially splitting said signal of interest into a first signal (V 1 ) and a second signal (V 2 );
C. injecting said first signal into the first frequency-shifting optical cavity (BDF 1 ) and shifting the optical frequency of the first signal by a first frequency f 1 per round trip in said first cavity;
D. injecting said second signal into the second frequency-shifting optical cavity (BDF 2 ) and shifting the optical frequency of the second signal by a second frequency f 2 per round trip in said second cavity;
E. coherently detecting the first signal transmitted by the first cavity (W 1 ) and the second signal (W 2 ) transmitted by the second cavity and generating a photocurrent (Tr) proportional to a detected luminous intensity,
F. filtering frequencies of the photocurrent that are lower than min (f 1 /2; f 2 /2),
G. computing a square modulus of the filtered photocurrent and determining a temporal representation of frequency information of said signal of interest, said method comprising a step prior to step A, denoted step A 0 , of:
adjusting the first or the second cavity in order to set a difference f 1 ×τ 1 -f 2 ×τ 2 to a desired non-zero value, in order to compute, in step G, a specific order of a real part of a fractional Fourier transform of the signal of interest, or
adjusting the first or the second cavity in order to cancel out a difference f 1 ×τ 1 -f 2 ×τ 2 , in order to compute, in step G, a power spectrum of said signal of interest.