Multi-stage optical amplifier having photonic-crystal waveguides for generation of high-power pulsed radiation and associated method

• US 20070091948A1
• Filed: 05/27/2006
• Published: 04/26/2007
• Est. Priority Date: 07/29/2005
• Status: Active Grant

• Current Assignee: Lockheed Martin Aculight Corp. (Martin Marietta Corporation)
• Original Assignee: Aculight Corporation (Martin Marietta Corporation)
• Inventors: Di Teodoro, Fabio, Brooks, Christopher
• Granted Patent: US 7,440,175 B2
• Time in Patent Office: Days
• US Class Current: 372/39
• CPC Class Codes: C03B 37/10 Non-chemical treatment surface treatment of fibres or filaments made from glass, minerals or slags C03C25/00
• CPC Class Codes: G02B 6/02328 Hollow or gas filled core
• CPC Class Codes: G02B 6/02347 Longitudinal structures arranged to form a regular periodic lattice, e.g. triangular, square, honeycomb unit cell repeated throughout cladding
• CPC Class Codes: G02B 6/02376 Longitudinal variation along fibre axis direction, e.g. tapered holes
• CPC Class Codes: G02B 6/02385 Comprising liquid, e.g. fluid filled holes
• CPC Class Codes: G02B 6/3826 characterised by form or shape
• CPC Class Codes: G02B 6/3853 Lens inside the ferrule lensed connectors G02B6/32
• CPC Class Codes: H01S 3/005 Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping shaping laser beam for working metal or other materials B23K26/06; optical elements, systems or apparatus in general G02B
• CPC Class Codes: H01S 3/0064 Anti-reflection devices, e.g. optical isolaters absorbing layers for marking or protecting purposes in laser working B23K26/50; magneto-optical non-reciprocal devices G02F1/093, G02F1/0955
• CPC Class Codes: H01S 3/0078 Frequency filtering
• CPC Class Codes: H01S 3/06704 Housings; Packages
• CPC Class Codes: H01S 3/06708 Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering optical fibres as passive waveguides G02B6/02
• CPC Class Codes: H01S 3/06729 Peculiar transverse fibre profile
• CPC Class Codes: H01S 3/06741 Photonic crystal fibre, i.e. the fibre having a photonic bandgap
• CPC Class Codes: H01S 3/06745 Tapering of the fibre, core or active region
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/06758 Tandem amplifiers
• CPC Class Codes: H01S 3/094007 Cladding pumping, i.e. pump light propagating in a clad surrounding the active core

Abstract

A method and apparatus use a photonic-crystal fiber having a very large core while maintaining a single transverse mode. In some fiber lasers and amplifiers having large cores problems exist related to energy being generated at multiple-modes (i.e., polygamy), and of mode hopping (i.e., promiscuity) due to limited control of energy levels and fluctuations. The problems of multiple-modes and mode hopping result from the use of large-diameter waveguides, and are addressed by the invention. This is especially true in lasers using large amounts of energy (i.e., lasers in the one-megawatt or more range). By using multiple small waveguides in parallel, large amounts of energy can be passed through a laser, but with better control such that the aforementioned problems can be reduced. An additional advantage is that the polarization of the light can be maintained better than by using a single fiber core.

Claims

1. An apparatus comprising:

an optical amplifier having a segmented fiber that includes a first amplifying segment having a rare-earth-doped photonic-crystal core and a second amplifying segment having a rare-earth-doped photonic-crystal core, wherein the first segment amplifies to a higher power than the second segment and is non-contiguous with the second segment;

a master-oscillator subsystem operable to obtain a seed laser signal light and to optically couple the seed laser signal light into the second segment, and a first optical-connector subassembly operatively coupled between the second segment and the first segment.

2. The apparatus of claim 1, wherein the master-oscillator subsystem includes a first optical isolator and a first narrow-bandwidth band-pass optical filter, and is operable to obtain a narrow-linewidth, single-frequency seed laser signal having a spectrally narrow signal bandwidth of less than 20 GHz, optically coupled to the core of the second segment through the first optical isolator and the first narrow-bandwidth band-pass optical filter.

3. The apparatus of claim 1, wherein the master-oscillator subsystem includes a first optical isolator and a first long-pass optical filter, and is operable to obtain a narrow-linewidth, single-frequency seed laser signal having a spectrally narrow signal bandwidth of less than 20 GHz, optically coupled to the core of the second segment through the first optical isolator and the first long-pass optical filter.

4. The apparatus of claim 2, wherein the first optical-connector subassembly includes a second narrow-bandwidth band-pass optical filter that is operable to pass wavelengths of the narrow-linewidth, single-frequency seed laser signal having a spectrally narrow signal bandwidth of less than 20 GHz, and to at least partially block wavelengths of amplified spontaneous emission (ASE) propagating back from the first segment.

5. The apparatus of claim 1, wherein the first optical-connector subassembly includes:

a substrate;

an optical band-pass filter; and

a dichroic mirror/beamsplitter that directs pump light into the second segment in a counter-propagating direction relative to signal light, and directs signal light from the second segment to the first segment through the optical band-pass filter;

wherein the filter and the mirror/beamsplitter are affixed to the substrate to form a unitized assembly.

6. The apparatus of claim 1, wherein the first optical-connector subassembly includes:

a substrate;

an optical band-pass filter attached to the substrate;

a dichroic mirror/beamsplitter, attached to the substrate, that directs pump light into the second segment in a counter-propagating direction relative to signal light, and directs signal light from the second segment to the first segment through the optical band-pass filter; and

at least one lens attached to the substrate;

wherein at least one of the filter, the mirror/beamsplitter and the lens is laser welded to the substrate to form a unitized assembly.

7. The apparatus of claim 1, wherein the first optical-connector subassembly includes:

an enclosure having a substrate;

an optical band-pass filter attached to the substrate;

a dichroic mirror/beamsplitter, attached to the substrate, that directs pump light into the second segment in a counter-propagating direction relative to signal light, and directs signal light from the second segment to the first segment through the optical band-pass filter; and

at least one lens attached to the substrate;

wherein at least one of the filter, the mirror/beamsplitter and the lens is soldered to the enclosure to form a unitized assembly.

8. The apparatus of claim 1, wherein the first optical-connector subassembly is a non-photonic-crystal bridge fiber having a multimode core having a numerical aperture (NA) higher than either the first or second segment'"'"'s photonic-crystal core NA, and wherein a fundamental mode of the photonic-crystal cores exhibits high spatial overlap with those transverse modes in the bridge fiber that exhibit a single central maximum.

9. The apparatus of claim 1, wherein at least one of the first amplifying segment and the second amplifying segment is capable of operation with a signal-output peak power of at least 500 kW.

10. The apparatus of claim 1, wherein at least one of the first amplifying segment and the second amplifying segment is capable of operation with a signal-output peak power of at least 2 megawatts (MW).

11. The apparatus of claim 1, wherein at least one of the first amplifying segment and the second amplifying segment is capable of operation with a signal-output-beam peak power of at least 500 kW and a beam-quality M² value of less than 1.5.

12. The apparatus of claim 1, wherein at least one of the first amplifying segment and the second amplifying segment is capable of generating linearly polarized pulses having degree of polarization of at least 15 dB (wherein the degree of polarization is a value of ten times the log (base 10) of the ratio of optical power along the polarization axis to the optical power along the orthogonal axis), a beam-quality M² value of less than 1.5, and a peak power of at least about 100 kW.

13. An apparatus comprising:

an optical amplifier that includes;

first photonic-crystal means for amplifying optical signal pulses to obtain high-power optical signal pulses,

second photonic-crystal means for amplifying optical signal pulses to obtain intermediate-power optical signal pulses, wherein the second means is non-contiguous with the first means, and

means for optically coupling the intermediate-power optical signal pulses to the first amplifying means from the second amplifying means; and

means for generating optical seed signal pulses and for coupling the optical seed signal pulses into the second amplifying means.

14. The apparatus of claim 13, wherein the means for generating further comprises:

means for optically isolating the optical seed signal pulses; and

means for filtering the optical seed signal pulses before they enter the core of the second photonic-crystal means to obtain narrow-linewidth, single-frequency optical seed signal pulses having a spectrally narrow signal bandwidth of less than 20 GHz.

15. The apparatus of claim 13, wherein the means for optically coupling further comprises:

means for filtering the intermediate-power optical signal pulses and substantially passing from the second photonic-crystal means toward the first photonic-crystal means those wavelengths corresponding to the narrow-linewidth, single-frequency seed laser signal and substantially blocking other wavelengths of amplified spontaneous emission (ASE) propagating back from the first photonic-crystal means, wherein the means for filtering the intermediate-power optical signal pulses are part of a unitized assembly.

16. The apparatus of claim 13, wherein the means for optically coupling further comprises:

means for filtering the intermediate-power signal light and substantially passing from the second photonic-crystal means those wavelengths corresponding to the narrow-linewidth, single-frequency seed laser signal and substantially blocking other wavelengths of amplified spontaneous emission (ASE) propagating back from the first photonic-crystal means;

means for directing pump light into the second photonic-crystal means in a counter-propagating direction relative to signal light; and

means for directing the filtered intermediate-power signal light toward the first photonic-crystal means, wherein the means for filtering the intermediate-power optical signal pulses, the means for directing pump light, and the means for directing the filtered intermediate-power signal light are part of a unitized assembly.

17. A method comprising:

providing an optical amplifier having a segmented photonic-crystal fiber that includes a higher-power first amplifying segment having a rare-earth-doped photonic-crystal core and a lower-power second amplifying segment having a rare-earth-doped photonic-crystal core;

obtaining a seed laser signal;

optically coupling the seed laser signal into the core of the second amplifying segment;

amplifying the seed laser signal in the second amplifying segment to obtain intermediate-power signal light;

operatively coupling the intermediate-power signal light to the first amplifying segment from the second amplifying segment; and

amplifying the intermediate-power signal light in the first amplifying segment to obtain higher-power signal light.

18. The method of claim 17, further comprising:

optically isolating the seed laser signal light; and

narrow-bandwidth band-pass filtering the seed laser signal light before it enters the core of the second segment to obtain a narrow-linewidth, single-frequency seed laser signal having a spectrally narrow signal bandwidth of less than 20 GHz, and optically coupling the seed laser signal to the core of the second segment.

19. The method of claim 17, further comprising:

optically isolating the seed laser signal; and

long-pass optically filtering the seed laser signal to obtain a narrow-linewidth, single-frequency seed laser signal optically coupled to the core of the second segment.

20. The method of claim 17, further comprising narrow-bandwidth band-pass filtering the intermediate-power signal light and substantially passing from the second segment toward the first segment those wavelengths corresponding to the narrow-linewidth, single-frequency seed laser signal and substantially blocking other wavelengths of amplified spontaneous emission (ASE) propagating back from the first segment.

21. The method of claim 17, further comprising:

narrow-bandwidth band-pass filtering the intermediate-power signal light and substantially passing from the second segment toward the first segment those wavelengths corresponding to the narrow-linewidth, single-frequency seed laser signal and substantially blocking other wavelengths of amplified spontaneous emission (ASE) propagating back from the first segment;

directing pump light into the second segment in a counter-propagating direction relative to signal light; and

directing the narrow-bandwidth band-pass filtered intermediate-power signal light toward the first segment within a unitized assembly.

22. The method of claim 17, further comprising:

narrow-bandwidth band-pass filtering the intermediate-power signal light and substantially passing from the second segment toward the first segment those wavelengths corresponding to the narrow-linewidth, single-frequency seed laser signal and substantially blocking other wavelengths of amplified spontaneous emission (ASE) propagating back from the first segment;

focusing pump light into the second segment in a counter-propagating direction relative to the signal light; and

focusing the narrow-bandwidth band-pass filtered intermediate-power signal light into the core of the first segment within a unitized assembly.

23. The method of claim 17, wherein the operatively coupling the intermediate-power signal light to the first amplifying segment from the second amplifying segment is performed through a non-photonic-crystal bridge fiber having a multimode core having a numerical aperture (NA) higher than either the first or second segment'"'"'s photonic-crystal core NA, and wherein a fundamental mode of the photonic-crystal cores exhibits high spatial overlap with those transverse modes in the bridge fiber that exhibit a single central maximum.

24. The method of claim 17, wherein the amplifying of the intermediate-power signal light in the first amplifying segment generates a peak power of at least 500 kW.

25. The method of claim 17, wherein the amplifying of the intermediate-power signal light in the first amplifying segment generates a peak power of at least 2 MW.

26. The method of claim 17, wherein the amplifying of the intermediate-power signal light in the first amplifying segment generates a peak power of at least 500 kW and a beam-quality M² value of less than 1.5.

27. The method of claim 17, wherein the amplifying of the intermediate-power signal light in the first amplifying segment generates linearly polarized pulses having degree of polarization of at least 15 dB (wherein the degree of polarization is a value of ten times the log (base 10) of the ratio of optical power along the polarization axis to the optical power along the orthogonal axis), a beam-quality M² value of less than 1.5, and a peak power of at least about 100 kW.