Multimode Optical Amplifier As A Receiver Pre-Amplifier For Free-Space Optical Communications

Abstract

In the method for processing a signal light from free-space by amplifying said signal for free-space optical communications. wherein the improvement includes the steps of (a) pre-amplifying said signal light with low noise; and (b) coupling said signal light into a multimode filter which reduces coupling hisses compared to single mode filters.

Description

CROSS REFERENCE TO RELATED APPLICATION

This application is a divisional of U.S. application Ser. No. 12/822,404 filed Jun. 24, 2010 and claims rights under 35 USC 19(e) from U.S. Application Ser. No. 61/219,821 filed Jun. 24, 2009.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to laser communications and more particularly to for amplifying signals in laser communications.

2. Brief Description of Prior Developments

The receiver sensitivity for an atmospheric laser communications system is increased by focusing the tree-space light into a multimode fiber amplifier that pre-amplifies the received signal For laser communications in the 1500-1600 nm region, we have used a multimode erbium-doped fiber amplifier (EDFA). Other fiber amplifiers are applicable for other wavelengths. Typical systems use readily available single mode EDFAs as receiver preamps, but this arrangement typically results in a 5-10 dB coupling loss of signal into a single mode EDFA from free-space, even with the benefit of adaptive optics correction. Multimode fibers have a larger core diameter and a larger numerical aperture (NA), thus permitting the collection of aberrated free-space optical wave fronts with minimal losses. Amplifying this signal with a multimode EDFA provides increased detector sensitivity compared to a (multimode) detector with no preamp, and also better net receiver sensitivity than a single mode preamp, which has an inherently high coupling loss.

An improved method and apparatus for amplifying signals in laser communications.

SUMMARY OF INVENTION

According to the present invention, the signal light from free-space is coupled into a muitimode fiber which reduces coupling losses compared to single mode fibers, as the core diameter and NA of multimode fibers tie larger than single mode, thus allowing for a much wider acceptance angle, and also resulting in the capture of high-order modes of a distorted atmospheric wave front. To increase the sensitivity of the receiver subsystem, the signal in the multimode fiber needs to first be pre-amplified with low noise. This is accomplished for 1500-1600 nm signals in a muitimode EDFA. Since there is minimal insertion loss into multimode fiber from free-space, the signal is collected and amplified efficiently, allowing for the receiver subsystem (i.e., multimode EDFA preamp and detector) to have enhanced sensitivity compared to the detector alone.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention is further described with reference to the accompanying drawings wherein:

FIGS. 1 is a schematic drawing showing a preferred embodiment of the method and apparatus of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

Referring to FIG. 1, in the method of the present invention a co-pumped diode driver 10 and a 980 μm co-pumped diode 12 may optionally be used to drive a 1550 μm signal through a multimode er-doped fiber 14. The signal then enters a muitimode (MM) 980/1550 pump wave division multiplexer (WDM) 16 and then to an MM circulator 18 which is driven by diode driver 20 and a 1532 μm diode 32. The signal then goes to band pass filter 24 and through tap coupler 26 to detector 28. From tap coupler 26 the signal is also directed to AGC detector 30 to automatic gain control (AGC) circuit 32 and then to counter-pumped diode driver 34 and then to 980 μm counter-pump diode 16 and then back to the MM 980/550 pump WDM 16.

Those skilled in the art will appreciate that the present invention overcomes insertion loss, fading, and receiver sensitivity disadvantages listed above; tolerant of residual angle-of-arrival of optical wave front due to atmospheric propagation, aero-optic boundary layer effects, or high bandwidth uncompensated residual tracking jitter; net result is lower bit and packet error rate for a free-space laser communications link (FSO). Unique approach employs counter-pumping from the exit end of the EDFA, to provide highest inversion in the downstream portion of the EDF where the amplified signal intensity is the greatest. This optical components on a bench that must be held. The present invention also is a single-stage amplifier, which results in fewer components and a more cost-effective solution for production. This is achieved in part by using an avalanche photodiode (APD) for the detector, rather than a PIN photodiode. The APD provides a 6-10 dB sensitivity advantage over a PIN detector, which allows the EDFA to be implemented with a single stage amplifier.

While the present invention has been described in connection with the preferred embodiments of the various figures, it is to be understood that other similar embodiments may be used or modifications and additions may be made to the described embodiment for performing the same function of the present invention without deviating therefrom. Therefore, the present invention should not be limited to any single embodiment, but rather construed in breadth and scope in accordance with the recitation of the appended claims.

Claims

1. In the method for processing a signal light from free-space by amplifying said signal for free-space optical communications, wherein the improvement comprises the steps of

(a) pre-amplifying said signal light with low noise; and

(b) coupling said signal light into a multimode filter which reduces coupling losses compared to single mode filters.

2. The method of claim 1 wherein step (a) is accomplished for a signal having a wavelength of 1300 μm to 1600 μm in a multimode er-doped fiber amplifier.

3. The method of claim 2 wherein step (b) allows for an enhanced acceptance angle.

4. The method of claim 3 wherein step (b) allows for the capture of high-order modes of a distorted atmospheric wavefront.