Compact non-lethal optical disruption device

1 . An optical disruptor, comprising:

a. a laser system;

b. a rangefinder, wherein said rangefinder provides a real-time distance to a target;

c. control electronics; and

d. dynamically-controlled output optics, wherein said dynamically-controlled output optics are actuated by said control electronics to provide a divergence in real-time of an output of said laser system, wherein said real-time divergence is according to said real-time distance to said target.

2 . The optical disruptor of claim 1 , wherein said laser system comprises at least two wavelength-stabilized pump laser diodes having laser diode outputs directed through free-space delivery optics to pump a solid-state laser medium to generate said laser system output.

3 . The optical disruptor of claim 2 , wherein said free-space delivery optics comprise a birefringent crystal, wherein said birefringent crystal receives a first pump beam along an axis of said laser system output and receives a second pump beam parallel to said first pump beam, wherein said first pump beam comprises a first polarization and said second pump beam comprises a second polarization, wherein said second polarization is disposed to converge said second pump beam to said first pump beam as said pump beams traverse said birefringent crystal.

4 . The optical disruptor of claim 3 , wherein said birefringent crystal is selected from the group consisting of calcite, YVO 4 (vanadate), crystalline quartz, and LiNbO 3 (lithium niobate), MgF 2 , sapphire (Al 2 O 3 ), and zircon (ZrSiO 4 ).

5 . The optical disruptor of claim 3 further comprises an optical retarder, wherein said optical retarder is disposed along a beam path of said second diode pump laser and between said second diode pump laser and said birefringent crystal.

6 . The optical disruptor of claim 3 further comprises a first converging lens disposed between said first diode pump laser and said birefringent crystal and a second converging lens disposed between said second diode pump laser and said birefringent crystal.

7 . The optical disruptor of claim 3 further comprises a converging lens disposed between said birefringent crystal and said solid-state laser medium.

8 . The optical disruptor of claim 2 , wherein said free-space delivery optics comprise a polarizing beam splitter, wherein said polarizing beam splitter receives a first pump beam along an axis of said solid-state laser medium and receives a second pump beam at an angle normal to said solid-state laser medium, wherein said first pump beam comprises a first polarization and said second pump beam comprises a second polarization.

9 . The optical disruptor of claim 8 , wherein a first converging lens is disposed between said first diode pump laser and said polarizing beam splitter and a second converging lens is disposed between said second diode pump laser and said polarizing beam splitter.

10 . The optical disruptor of claim 2 , wherein said free-space delivery optics comprise a first converging lens disposed in a beam path of a first said diode pump laser, a second converging lens disposed in a beam path of a second said diode pump laser, a third converging lens disposed between said converging lenses and said solid-state laser medium and disposed between said second converging lens and said solid state laser medium.

11 . The optical disruptor of claim 2 , wherein said free-space delivery optics comprise a first converging lens disposed along a beam path of a first said diode pump laser and between said first diode pump laser and said solid-state laser medium, and further comprising a second converging lens disposed along a beam path of a second said diode pump laser and between said second diode pump laser and said solid-state laser medium, wherein said first diode pump laser beam path is disposed normal to said solid-state laser medium and said second diode pump laser beam path is disposed normal to said solid-state laser medium.

12 . The optical disruptor of claim 1 , wherein said dynamically-controlled output optics comprise at least one electrically-variable or liquid lens, wherein said electrically-variable or liquid lens adjusts said divergence of said laser system output.

13 . The optical disruptor of claim 1 , wherein said controller electronics comprise a switching buck regulator, and a switching current source and temperature switching circuit.

14 . The optical disruptor of claim 1 , wherein said control electronics comprises an optical output regulator.

15 . The optical disruptor of claim 1 , wherein said optical disruptor is battery-powered.

16 . The optical disruptor of claim 1 , wherein said solid-state laser medium is selected from the group consisting of Nd:YVO 4 (vanadate), Nd:YAG, Yb:YAG, Yb:glass, Er:glass, Nd:YLF, ND:GGG, and Nd:YGdO 4 .

17 . The optical disruptor of claim 1 , wherein an output from said solid-state laser medium is frequency multiplied using a frequency multiplying medium selected from the group consisting of KTP, KTA, KDP, KD*P, LN, LT, BBO, BIBO, cPPLN, sPPLN, cPPLT, and sPPLT or any of their Mg-doped equivalents.

18 . The optical disruptor of claim 1 , wherein said laser system output is a pulsed mode or a continuous-wave mode.

19 . The optical disruptor of claim 1 , wherein said laser system comprises an operating temperature over a range of −20° C. to 60° C.

20 . The optical disruptor of claim 1 , wherein current is provided to at least one said pump laser diode at all times during operation of said laser system.

21 . The optical disruptor of claim 1 , wherein said pump laser diodes are controlled according to a condition of said laser system output, wherein said laser output condition is sampled and fed back to said controller by an optical sampler and feedback loop.