Reducing crosstalk in free-space optical communications

1. An apparatus, comprising:

an optical transmitter that includes a modulator, a dispersion adjustment module, and an optical amplifier, the transmitter being configured to transmit optical pulses over a free-space optical communication channel; and

wherein the modulator is configured to produce an optical carrier that is amplitude and/or phase modulated by data; and

wherein the dispersion adjustment module is connected between the modulator and the amplifier and is configured to substantially change temporal widths of optical pulses received from the modulator by changing dispersions of the received optical pulses.

2. The apparatus of claim 1 , further comprising a second dispersion adjustment module being connected to cause substantial temporal narrowing of optical pulses that have passed through the optical amplifier.

3. The apparatus of claim 2 , wherein the second dispersion adjustment module is located in the optical transmitter.

4. The apparatus of claim 2 , further comprising:

an optical receiver that is located to receive the transmitted optical pulses from the free-space optical communication channel.

5. The apparatus of claim 4 , wherein the second dispersion adjustment module is located in the optical receiver.

6. The apparatus of claim 4 , further comprising:

a third dispersion adjustment module being connected to cause substantial temporal narrowing of optical pulses that have passed through the optical amplifier, the third dispersion adjustment module being located in the optical receiver.

7. The apparatus of claim 6 , wherein the second dispersion adjustment module be configured to decrease temporal widths of optical pulses that are output by the amplifier by at least about 20 percent.

8. The apparatus of claim 1 , wherein the dispersion adjustment module is configured to change magnitudes in pico-seconds per nanometer of dispersions of optical pulses received therein to be at least [0.25×10 5 giga-bits per second][1550 nanometers)/λ] 2 over the square of the per wavelength-channel bit-rate in giga-bits per second, λ being the wavelength of the optical pulses in nanometers.

9. The apparatus of claim 2 , wherein the second dispersion adjustment module is configured to decrease temporal widths of optical pulses received therein by about 20 percent or more.

10. The apparatus of claim 2 , wherein the second dispersion adjustment module is configured to increase peak intensities of optical pulses received by the second dispersion adjustment module by about 25 percent or more.

11. A method, comprising:

producing a stream of optical pulses by producing a modulated optical carrier;

substantially changing the dispersions of the optical pulses of the stream to produce corresponding temporally broadened optical pulses;

optically amplifying the temporally broadened optical pulses to produce corresponding amplified optical pulses; and

transmitting the amplified optical pulses to an optical receiver via a free-space optical communication channel.

12. The method of claim 11 , further comprising:

substantially changing dispersions of optical pulses that have been optically amplified to produce corresponding substantially temporally narrowed optical pulses.

13. The method of claim 12 , further comprising:

demodulating a stream of data from the substantially temporally narrowed optical pulses.

14. The method of claim 11 , wherein the substantially changing the dispersions increases the temporal widths of the optical pulses of the stream by at least about 25 percent.

15. The method of claim 11 , wherein the substantially changing the dispersions causes the optical pulses of the stream to have dispersions whose magnitudes in pico-seconds per nanometer are at least [0.25×10 5 giga-bits per second][(1550 nanometers)/λ] 2 over the square of the per wavelength-channel bit-rate in giga-bits per second, λ being the wavelength of the optical pulses in nanometers.

16. The method of claim 11 , wherein the substantially changing dispersions of the optically amplified optical pulses includes decreasing temporal pulse widths of the optically amplified optical pulses by about 20 percent or more.

17. The method of claim 11 , wherein the substantially changing dispersions of the optically amplified optical pulses includes increasing peak intensities of optical pulses by about 25 percent or more.