System and method for amplifying an optical pulse and pumping laser therefor

- Coherent, Inc.

An efficient, powerful and reliable system for amplifying optical pulses. Seed-pulses are generated by a seed-pulse source and are transmitted to an optical amplifier for amplification. The power for the amplification is provided by a Q-switched, diode-pumped, intracavity-doubled pump laser.

Skip to: Description  ·  Claims  ·  References Cited  · Patent History  ·  Patent History
Description
CROSS REFERENCES TO RELATED APPLICATIONS

This application is a continuation of application Ser. No. 08/787,991, filed on Jan. 23, 1997, which issued as U.S. Pat. No. 5,790,303 on Aug. 4, 1998.

BACKGROUND OF THE INVENTION

1. Field of the Invention

This invention relates generally to the field of lasers, and more particularly to lasers for pumping optical amplifiers.

2. Description of the Background Art

Known amplifier systems employ a source laser, an amplifier, and a pump source to transfer energy to the amplifying medium, to generate amplified laser light. The source laser emits a beam of laser light that is amplified as it passes through the amplifier. The energy for the amplification is provided to the amplifier by the pump source, which is typically a laser. A pump laser generally includes a laser medium element, positioned between a high reflector and an output coupler, and a pumping means. The pumping means excites the atoms of the medium element into a metastable state. The relaxation of the excited atoms is accompanied by the emission of light, which is reflected back and fourth between the high reflector and the output coupler, and the growing reflected wave induces the emission of additional light into the reflected wave state. As the wave continues to grow, the output coupler allows a portion of the reflected light to pass as the output beam of the pump laser.

It is obviously desirable that the pump laser be efficient, powerful, reliable, and convenient to set up and operate, but often there is tension between these various design objectives. For example, diode lasers provide a very efficient pumping means and are more durable than lamps, but the output energy of known diode-pumped lasers has been too low for them to function effectively as amplifier pumping lasers. Further, some prior diode-pumped systems require that the pitch of the diode emitters be carefully matched and aligned to the optical path within the media element, reducing convenience of assembly.

More powerful pump lasers exist, but in each case the power increase comes at the expense of one of the other design objectives. For example, more power can be obtained by using gas filled lamps to excite the pump laser lasing medium, but these systems are less efficient, less reliable, and less robust. Additionally, such lasers generally have significant cooling requirements and require a special power service, as opposed to a standard 110V AC outlet.

Thus, there is a need for a laser amplifier system capable of producing an output that is orders of magnitude higher in energy than known diode-pumped systems. It is also desirable that the amplifier system be efficient, reliable, and convenient to set up and operate.

SUMMARY OF THE INVENTION

The present invention is an efficient, powerful and reliable optical amplification system. Seed-pulses are generated by a seed-pulse source and are transferred to an optical amplifier for amplification. The power for the amplification is provided by a Q-switched, diode-pumped, intracavity-doubled amplifier pump laser.

One embodiment of the amplifier pump laser includes a laser medium element that is pumped by a plurality of diode lasers to emit a beam of light at a first frequency along an optical path passing through the element. The pump laser also includes at least one reflector and an output coupler, for redirecting the beam along the optical path to establish an optical resonator. A Q-switch is disposed in the optical path to selectively frustrate or permit optical resonance, thereby enabling the laser to produce high-power output pulses, as opposed to low-power, continuous output. The output power of the pump laser is further enhanced by including a doubling crystal within the optical cavity. The doubling crystal is disposed in the optical path and converts a portion of the original oscillating wave to a new wave having twice the frequency of the original. The output coupler is highly reflective to the original frequency, but highly transmissive to the doubled frequency, and, therefore, passes the doubled frequency wave as output.

There are several specific embodiments of the amplifier pump laser of the present invention. One embodiment is characterized by a beam that is directed between two reflectors, along a folded optical path, by a beam director and an output coupler. Another embodiment is characterized by a straight optical path between one reflector and the output coupler. Finally, there are uni-directional and bi-directional ring configured embodiments.

One embodiment of the optical amplifier of the present invention is a regenerative amplifier which includes a gain medium element within an optically resonant cavity, a capturing means for switching seed-pulses into the cavity, and an ejecting means for switching amplified pulses out of the cavity. The output beam of the amplifier pump laser excites the gain medium, which amplifies the seed-pulse as it oscillates within the cavity. After amplification, the ejecting means switches the amplified pulse out of the cavity as the amplification system output.

Other embodiments of the optical amplifier include a ring configured regenerative amplifier and a multi-pass “bowtie” amplifier.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a block diagram of the preferred optical amplification system of the present invention;

FIG. 2 is a block diagram of the diode-pumped, Q-switched, intracavity-doubled pump laser of FIG. 1;

FIG. 3 shows an end view of the laser medium element of FIG. 2;

FIG. 4 is a block diagram of the optical amplifier of FIG. 1;

FIG. 5A is a block diagram of an alternate amplifier pump laser;

FIG. 5B is a block diagram of an alternative amplifier pump laser having a bi-directional, ring configuration;

FIG. 5C is a block diagram of an alternative amplifier pump laser having a uni-directional, ring configuration;

FIG. 6A is a block diagram of an alternate ring-configured optical amplifier; and

FIG. 6B is a block diagram of an alternate multi-pass optical amplifier.

 DETAILED DESCRIPTION OF A PREFERRED EMBODIMENT

The present invention provides an efficient, powerful, reliable, and convenient optical amplification system. Numerous details, such as the number of diode lasers and the use of a regenerative amplifier, are provided for the sake of clarity, but it will be obvious to those skilled in the art that the invention can be practiced apart from these specific details. In other instances, details of well known equipment and processes are omitted so as not to obscure the invention.

FIG. 1 shows an optical amplification system 100, including a seed-pulse source 110, an optical amplifier 112, and an amplifier pump laser 114. Seed-pulse source 110 generates seed-pulses and sends them via optical path 116 to optical amplifier 112. Amplifier pump laser 114 generates pump pulses which are directed along optical path 118 into amplifier 112. Amplifier 112 uses the optical energy of the pump pulses to amplify the seed-pulses and emits the amplified pulses along optical path 120.

Seed-pulse source 110 includes pump laser 122 and oscillator 124. Pump laser 122 provides optical energy, via optical path 126, which excites oscillator 124 to emit the seed-pulses along optical path 116. In the preferred embodiment, pump laser 122 is a continuous-wave laser and oscillator 124 is a titanium-sapphire oscillator. Seed-pulse sources are well known in the art, and therefore will not be discussed in greater detail.

FIG. 2 shows a detailed view of amplifier pump laser 114, including a first reflector 202, a Q-switch 204, a laser medium element 206, a plurality of diode lasers 208, a second reflector 210, an output coupler 212, a frequency altering device 214, and a third reflector 216. In the preferred embodiment, laser medium element 206 is a cylindrical rod of neodymium-doped yttrium-lithium-fluoride (YLF), but those skilled in the art will understand that the invention may be practiced with alternate active elements, such as erbium (Er) holmium, (Ho) or thorium (Th), or alternate carriers such as glass, vanadate, or yttrium-scandium-gallium-garnet (YSGG). Diode lasers 208 are disposed along the lateral surface of laser medium element 206, and when provided with electrical current emit laser light into element 206 which excites the atoms of element 206 to a metastable state. The relaxation of the excited atoms is accompanied by the emission of light of a first frequency (w), some of which travels along a folded optical path 218.

Reflectors 202 and 216 are positioned at opposite ends of optical path 218, and each respectively has a reflective surface 220 and 222 which is substantially perpendicular to an incident segment of optical path 218. Therefore, any light traveling along optical path 218 which is incident on either reflector 202 or 216 is reflected back along optical path 218. Reflector 210 and output coupler 212 fold optical path 218 to pass between reflectors 202 and 216, through Q-switch 204, laser medium element 206 and frequency altering device 214. As the light oscillates back and forth between reflectors 202 and 216, the growing reflected wave induces the emission of additional light into the reflected wave state, thus amplifying the reflected wave.

Q-switch 204 is disposed in optical path 218 between reflector 202 and laser medium element 206 and selectively frustrates or permits oscillation. When oscillation is frustrated, the excited atoms are not induced to emit light, and the number of excited atoms can, therefore, be greatly increased. Then, when Q-switch 204 permits oscillation, a powerful pulse will be generated as the large number of excited atoms drop to the lower state, emitting light as they make the transition. Many Q-switching arrangements are known, including, but not limited to, bleachable absorbers that become transparent under illumination, rotating prisms and mirrors, mechanical choppers, ultrasonic cells, and electro-optic shutters such as Kerr or Pockels cells. The present invention contemplates the use of any such switching device.

Frequency altering device 214 is disposed in optical path 218, between reflector 216 and output coupler 212. In the preferred embodiment, frequency altering device 214 is a lithium-triborate (LBO) doubling crystal, but those skilled in the art will understand that the invention may be practiced with alternative doubling crystals, including but not limited to beta-barium-borate (BBO), potassium-titanyl-phosphate (KTP) and potassium-dihydrogen-phosphate (KDP). As the light of frequency (w) emitted by laser medium element 206 travels along optical path 218 through device 214, the frequency of a portion of the beam is doubled, creating a second wave at the doubled frequency (2w). Output coupler 212 is designed to be highly reflective to the first frequency (w) but transparent to the second (2w) frequency, and therefore passes the second (2w) wave as an output pulse along optical path 118. The intracavity disposition of device 214 is advantageous over prior art systems which positioned the doubling crystal between the amplifier pump laser and the optical amplifier. Since the reflected (w) wave makes multiple passes through device 214, the doubling efficiency is greatly increased, resulting in an increase in output power.

FIG. 3 shows an end view of laser medium element 206, taken along optical path 218. The plurality of diode lasers 208 are disposed along the circumference of medium element 206 which, except for openings through which diode lasers 208 emit their light, is surrounded by a highly reflective material 310. The reflective material 310 increases efficiency by insuring that the light emitted by diode lasers 208 makes several passes through medium element 206, thus increasing the opportunity for absorption. Those skilled in the art will understand that a suitable choice of neodymium concentration in the YLF or a suitable distribution of the pump diodes around the rod could eliminate the need for the reflective material. Those skilled in the art will also understand that the laser beams emitted by diode lasers 208 are typically diverse, and are shown in FIG. 2 as narrow rays for the sake of clarity.

FIG. 4 is a block diagram detailing optical amplifier 112, which includes a gain medium element 402, first and second reflectors 404 and 406, first and second Pockels cells 408 and 410, a polarizing beam splitter 412, and first and second beam directors 414 and 416. In the preferred embodiment, gain medium element 402 is a cylindrical rod of titanium-doped sapphire (Ti:Al2O3) having a first end surface 418 and a second end surface 420, each formed by a Brewster cut. Reflectors 404 and 406 each have a highly reflective surface 422 and 424 respectively, and are positioned facing each other at opposite ends of gain medium element 402 with their reflective surfaces 422 and 424 perpendicular to an optical path 426 passing through both end surfaces 418 and 420 of gain medium element 402. First and second Pockels cells 408 and 410 are disposed in optical path 426, between gain medium element 402 and first and second reflectors 404 and 406, respectively. Polarizing beam splitter 412 is disposed in optical path 426 between gain medium element 402 and second Pockels cell 410.

During operation, seed-pulses emitted by seed-pulse source 110 along optical path 116 impinge on first end surface 418 of gain medium element 402. Although the angle appears smaller in FIG. 4 for purposes of illustration, optical path 116 forms an angle of about 114° with optical path 426. The reflected seed-pulse is polarized, and optical path 116 is oriented relative to gain medium element 402 such that the polarized seed-pulse is reflected along optical path 426 toward first Pockels cell 408. First Pockels cell 408 selectively switches a seed-pulse into optical amplifier 112, where the pulse is amplified during several passes along optical path 426 between reflectors 404 and 406.

The energy for the amplification that occurs in optical amplifier 112 is provided by amplifier pump laser 114. First beam director 414 redirects the pump light emitted from amplifier pump laser 114 along optical path 118 to impinge on first end surface 418 of gain medium element 402. The pump light passes through first end surface 418 and is absorbed by the atoms of gain medium element 402, exciting them to a metastable state. The excited atoms are induced by the oscillating seed-pulse to re-emit the absorbed light into the seed-pulse state, thereby amplifying the seed-pulse. After a number of passes between first and second reflectors 404 and 406 along optical path 426, second Pockels cell 410 ejects the amplified pulse by altering its polarization such that polarizing beam splitter 412 directs the pulse toward second beam director 416, which in turn directs the pulse along optical path 120 out of optical amplifier 112. Those skilled in the art will understand that there are many optical switching techniques that can be used to switch pulses into and out of the regenerative amplifier resonator. These include a single Pockels cell, multiple Pockels cells, a combination of a Pockels cell and a wave plate, acousto-optic cells, Faraday isolators, and a multitude of other combinations of the foregoing. The invention contemplates the use of each of these and other types of switching techniques, and is limited only by the appended claims.

While amplifier 112 of the preferred embodiment of the invention has been disclosed as a linear regenerative amplifier, it will be obvious to those skilled in the art that the invention may be practiced with other types of optical amplifiers. In fact, the invention contemplates the use of other types of amplifiers, and is limited only by the appended claims.

FIG. 5A is a block diagram of an alternate amplifier pump laser 114a characterized by a straight-line optical path 502. Alternate pump laser 114a includes a laser medium element 504, a plurality of diode lasers 506, a reflector 508, an output coupler 510, a Q-switch 512, and a frequency altering device 514. Diode lasers 506 are disposed along the lateral surface of laser medium element 504, and when provided with electrical current emit laser light into element 504 which excites the atoms of element 504 to a metastable state. The relaxation of the excited atoms is accompanied by the emission of light of a first frequency (w), some of which travels along optical path 502.

Reflector 508 and output coupler 510 are positioned to face each other at opposite ends of optical path 502. Reflector 508 and output coupler 510 each have a reflective surface 516 and 518 respectively which is substantially perpendicular to optical path 502. Therefore, any light traveling along optical path 502 which is incident on either reflector 508 or output coupler 510 is reflected back along optical path 502. As the light oscillates back and forth between reflector 508 and output coupler 510, the growing reflected wave induces the emission of additional light into the reflected wave state, thus amplifying the reflected wave.

Q-switch 512 is disposed in optical path 502 between reflector 508 and laser medium element 504 and selectively frustrates or permits oscillation. When oscillation is frustrated, the excited atoms are not induced to emit light, and the number of excited atoms can, therefore, be greatly increased. Then, when Q-switch 512 permits oscillation, a powerful pulse will be generated as the large number of excited atoms drop to the lower state, emitting light as they make the transition.

Frequency altering device 514 is disposed in optical path 502, between laser medium element 504 and output coupler 510. As the light of frequency (w) emitted by laser medium element 504 travels along optical path 502 through device 514, the frequency of a portion of the beam is doubled, creating a second wave at the doubled frequency (2w). Output coupler 510 is designed to be highly reflective to the first frequency (w) but transparent to the second (2w) frequency, and therefore passes the second (2w) wave as an output pulse along optical path 118.

FIG. 5B shows an alternate bi-directional, ring-configured amplifier pump laser 114b, which could be substituted for amplifier pump laser 114. Pump laser 114b is characterized by a triangular optical path 520, and includes a laser medium element 524, a plurality of diode lasers 526, a first beam director 528, a second beam director 530, an output coupler 532, a Q-switch 534, and a frequency altering device 536. Diode lasers 526 stimulate laser medium element 524 to emit light of a first frequency in both directions along optical path 520. As described above, Q-switch 534 pulses laser 114b, and frequency altering device 536 doubles the frequency of a portion of the light passing therethrough. Beam directors 528 and 530 are disposed at two of the vertices of optical path 520 to direct light incident from one leg of optical path 520 along the adjacent leg. Output coupler 532 is disposed at the remaining vertex of optical path 520 and is designed to reflect light of the first frequency and transmit light of the doubled frequency as output beams along optical paths 118 and 538.

It will be clear to one skilled in the art that optical path 520 need not be triangular. With the addition of an appropriate number of beam directors optical path 520 could be shaped as any multi-sided polygon. Further, additional laser medium elements may be disposed in one or more of the additional legs to create a more powerful multi-element laser. All such modifications are considered to be within the scope of the present invention.

The dual output is a result of the bi-directional operation of laser 114b. Light traveling along optical path 520 in a clockwise direction will be emitted along optical path 118, whereas light traveling along optical path 520 in a counter-clockwise direction will be emitted along optical path 538. Bi-directional operation is desirable when two output beams are required. When only one output beam is required, the second beam results in wasted power and uni-directional operation is preferred.

FIG. 5C shows an alternate uni-directional, ring-configured amplifier pump laser 114c, which could be substituted for amplifier pump laser 114. Ring laser 114c is substantially identical to ring laser 114b described above, but includes an additional uni-directional device (optical diode) 550. Typically, optical diodes include a Faraday rotator, an optically active crystal and a Brewster plate. Faraday rotators rotate the polarization of a beam in a direction of rotation that is not dependent on the direction of travel of the wave, but the direction of rotation by the optical crystal does depend on the direction of travel of the wave. Therefore, in one direction the effect of the two components combine to produce a net rotation, but in the other direction they offset, producing no net rotation. The Brewster plate then selectively introduces a loss in the direction undergoing a net rotation, frustrating oscillation in that direction. Other means for encouraging unidirectional oscillation are known to those skilled in the art, and are considered to be within the scope of the invention.

FIG. 6A shows an alternate ring-configured, regenerative optical amplifier characterized by a rectangular optical path 602 and including four beam directors 604, 606, 608, and 610, a gain media element 612, a Pockels cell 614 and a polarizing beam splitter 616. Beam directors 604, 606, 608, and 610 are each disposed at one of the vertices of optical path 602, to redirect light incident from one leg of optical path 602 along the adjacent leg. Gain element 612 has a first end surface 618 and a second end surface 620, and is disposed between beam directors 604 and 610 such that optical path 602 passes through first and second end surfaces 618 and 620 of gain element 612. Pockels cell 614 and polarizing beam splitter 616 are disposed in optical path 602 between beam directors 606 and 608, with beam splitting polarizer 616 nearer beam director 606.

A polarized seed-pulse enters amplifier 600 via optical path 622, and is reflected along optical path 602 toward beam director 610 by the second end surface 620 of gain element 612. The seed-pulse travels counter-clockwise around optical path 602, first being reflected by beam directors 610 and 608, then passing through Pockels cell 614 which alters its polarization and, thus, it passes through polarizing beam splitter 616, then being reflected by beam directors 606 and 604, and finally passing through gain element 612.

The seed-pulse is amplified as it repeats the loop around optical path 602. The power for amplification is provided by a pump laser whose output beam enters amplifier 600 via optical path 626. The pump beam passes through first end surface 618 of gain element 612 where it is absorbed by the active atoms of the gain medium, exciting them to a metastable state. The oscillating seed-pulse induces the excited atoms to re-emit the absorbed light into the seed-pulse state, thereby amplifying the seed-pulse. After a number of amplifying passes around optical path 602, Pockels cell 614 ejects the pulse by altering its polarization such that polarizing beam splitter 616 directs the pulse along optical path 624 out of optical amplifier 600. Those skilled in the art will recognize that there many techniques, for example those described above, for switching a pulse into and out of a regenerative amplifier, and the present invention contemplates the use of any such switching technique.

FIG. 6B shows an optional multi-pass optical amplifier 650, characterized by a “bow tie” shaped optical path 651, including a gain element 652 and four beam directors 654, 656, 658, and 660. A seed-pulse enters amplifier 650 along optical path 662 and passes through gain element 652 and proceeds along optical path 651 toward beam director 654. Beam director 654 redirects the pulse along the next leg of optical path 651 toward beam director 656, which in turn redirects the pulse back through gain element 652 and toward beam director 658. Beam director 658 then directs the pulse toward beam director 660, which in turn directs the pulse through gain element 652 a third time and out of amplifier 650 via optical path 664. The pulse is amplified each time it passes through gain element 652, with power provided by a pump laser beam.

Those skilled in the art will recognize that there are many variations on this type of amplifier. In its simplest form, an amplifier of this type could consist simply of a gain element and a pumping means, with the beam making only one pass (although this is not technically a multi-pass amplifier) through the element. At the other extreme, a large number of beam directors could be arranged around the gain element, greatly increasing the number of passes by the beam through the gain element.

The present invention has been disclosed with reference to a preferred embodiment and several alternate embodiments. Specific details have been set forth, such as the number of medium elements in a pump laser or amplifier, specific beam paths, and methods for switching pulses into and out of an amplifier. Those skilled in the art will understand that the invention may be practiced apart from the specific details set forth herein.

Claims

1. A method for amplifying an optical pulse in a laser comprising the steps of:

generating a pulsed light in a Q-switched, amplifier pump laser including an intracavity frequency altering device wherein said pump laser includes an elongated gain medium have a light propagation axis extending longitudinally therethrough and wherein said gain medium is pumped by at least two elongated diode laser pump sources mounted along the side of the gain medium at two circumferentially spaced apart positions;
directing the pulsed light to an optical gain element of an optical amplifier comprising a medium of optically responsive atoms;
exciting the atoms to a metastable state using the pulsed light; and
directing a seed pulse at the gain element of an said optical amplifier, thereby causing the excited atoms to emit an amplified optical pulse.; and
redirecting the amplified optical pulse through the gain element, thereby causing the excited atoms to emit a further amplified optical pulse.

2. The method of claim 1 wherein said step of generating a pulsed light includes altering a frequency of said light with a frequency altering device.

3. The method of claim 2 1 wherein said step of altering the frequency of said light utilizes intracavity frequency altering device is a frequency doubling crystal.

4. The method of claim 2 further comprising:

disposing intracavity said frequency altering device.

5. The method of claim 2 1 wherein said step of generating a pulsed light includes providing output coupler means.

6. A method for generating and amplifying an optical pulse comprising the steps of:

exciting atoms in a laser medium said laser medium being elongated and having a light propagation axis extending longitudinally therethrough and wherein said laser medium is pumped by at least two elongated diode laser pump sources mounted along the side of the gain medium at two circumferentially spaced apart positions;
causing oscillation in said laser medium using a Q-switch disposed along an optical path to produce laser light along said optical path;
altering the frequency of at least some of said laser light along said optical path using an intracavity frequency altering device;
selectively releasing laser light having the altered frequency from said optical path;
receiving the selectively released laser light at an a regenerative optical amplifier to provide optical energy to the optical amplifier; and
receiving a seed-pulse at the regenerative optical amplifier to cause the optical amplifier to emit an amplified optical pulse.

7. The method of claim 6 wherein said step of altering the frequency is performed by a an intracavity frequency doubling crystal.

8. The method of claim 7 wherein said frequency doubling crystal is intracavity disposed.

9. The method of claim 6 wherein said step of selectively releasing laser light is performed by an optical coupler.

10. The method of claim 6 wherein the steps of receiving the selectively released laser light and receiving a seed-pulse are performed by a gain medium element.

11. A system for amplifying optical pulses comprising:

a seed-pulse source for producing optical seed-pulses;
an optical amplifier disposed to receive said seed-pulses from said seed-pulse source, for receiving and amplifying said seed-pulses and for outputting amplified seed-pulses; and
an amplifier pumping laser for providing optical energy to said optical amplifier for the amplification of said seed-pulses, said amplifier pumping laser including an elongated gain medium have a light propagation axis extending longitudinally therethrough and wherein said gain medium is pumped by at least two elongated diode laser pump sources mounted along the side of the gain medium at two circumferentially spaced apart positions, an intracavity frequency altering device, and a switching means for selectively frustrating or allowing optical resonance, thereby enabling said amplifier pumping laser to emit pulses of laser light; and
a plurality of beam directors positioned to redirect each seed-pulse through a gain medium of the optical amplifier, whereby each seed-pulse makes more than one pass through the gain medium.

12. The system of claim 11 wherein said switching means comprises a Q-switch.

13. The system of claim 11 wherein said frequency altering device comprises a frequency doubling crystal.

14. A system for amplifying optical pulses, comprising:

a an elongated lasing material having a light propagation axis extending longitudinally therethrough and wherein said gain medium is pumped by at least two elongated diode laser pump sources mounted along the side of the gain medium at two circumferentially spaced apart positions;
switching means for selectively frustrating or allowing optical resonance in said lasing material;
a an intracavity frequency altering device for altering the frequency of light emitted from said lasing material;
a seed pulse source for producing optical seed-pulses; and
an a regenerative optical amplifier disposed to receive the optical seed-pulses from the seed pulse source and to receive light emitted from the frequency altering device to amplify the optical seed-pulses with optical energy from the light emitted from the frequency altering device.

15. The pumping laser system of claim 14 wherein said switching means comprises a Q-switch.

16. The pumping laser system of claim 14 wherein said frequency altering device comprises a frequency doubling crystal.

17. A system for amplifying optical pulses, comprising:

a seed pulse source for producing optical seed-pulses;
an a regenerative optical amplifier disposed to receive the seed-pulses from the seed-pulse source, for receiving and amplifying the seed pulses and for outputting amplified seed-pulses; and
an amplifier pumping laser for providing optical energy to the optical amplifier for the amplification of the seed-pulses, the amplifier pumping laser including a an elongated gain medium have a light propagation axis extending longitudinally therethrough and wherein said gain medium is pumped by at least two elongated diode laser pump sources mounted along the side of the gain medium at two circumferentially spaced apart positions, an intracavity frequency altering device and a switching device for selectively frustrating or allowing optical resonance, thereby enabling the amplifier pumping laser to emit pulses of laser light.

18. A system for amplifying optical pulses, comprising:

a seed pulse source for producing optical seed-pulses;
an optical amplifier disposed to receive the seed-pulses from the seed-pulse source, for receiving and amplifying the seed pulses and for outputting amplified seed-pulses; and
an amplifier pumping laser for providing optical energy to the optical amplifier for the amplification of the seed-pulses, the amplifier pumping laser including an intracavity frequency altering device and a switching device for selectively frustrating or allowing optical resonance, thereby enabling the amplifier pumping laser to emit pulses of laser light.

19. A system for amplifying optical pulses, comprising:

an amplifier pumping laser for providing optical energy to an a regenerative optical amplifier for the amplification of seed-pulses;
the amplifier pumping laser including an elongated gain medium have a light propagation axis extending longitudinally therethrough and wherein said gain medium is pumped by at least two elongated diode laser pump sources mounted along the side of the gain medium at two circumferentially spaced apart positions and configured to produce light, an intracavity frequency altering device configured to alter a frequency of the produced light, and a switching device for selectively frustrating or allowing optical resonance, thereby enabling the amplifier pumping laser to emit pulses of laser light.

20. The method of claim 1, further comprising:

altering a polarization of the seed-pulse, the polarization determining whether the seed-pulse is redirected through the gain element or directed as an output pulse.

21. The system of claim 11, wherein:

the plurality of beam directors directs the seed-pulse along separate paths through the gain element.

22. The system of claim 11, wherein:

the plurality of beam directors form a ring path around the gain element.

23. The system of claim 11, further comprising:

a polarizing element for altering a polarization of the seed-pulse.

24. The system of claim 23, further comprising:

a beam splitting element for directing the seed-pulse as an output pulse when the seed-pulse has a predetermined polarization.

25. A method for amplifying an optical pulse in a laser comprising the steps of:

generating a pulsed light in a Q-switched, diode-pumped, amplifier pump laser including an intracavity frequency altering device, the amplifier pump laser including a gain medium having a highly reflective material disposed about a radial outer surface thereof, the highly reflective material having at least one opening for admitting radiation from a diode laser for exciting atoms of the gain medium;
directing the pulsed light to an optical gain element comprising a medium of optically responsive atoms;
exciting the atoms to a metastable state using the pulsed light; and
directing a seed pulse at the gain element of an optical amplifier, thereby causing the excited atoms to emit an amplified optical pulse.

26. The method of claim 25 wherein the amplifier pumping laser further includes a plurality of diode lasers.

27. The method of claim 26 wherein the plurality of diode lasers are disposed along a lateral surface of the gain medium.

28. The method of claim 25 wherein radiation generated by the diode laser passes more than once through the gain medium.

29. A system for amplifying optical pulses comprising:

a seed-pulse source for producing optical seed-pulses;
an optical amplifier disposed to receive said seed-pulses from said seed-pulse source, for receiving and amplifying said seed-pulses and for outputting amplified seed-pulses; and
an amplifier pumping laser for providing optical energy to said optical amplifier for the amplification of said seed-pulses, said amplifier pumping laser including a gain medium having a highly reflective material disposed about a radial outer surface thereof, a diode laser positioned to direct radiation through an opening in the highly reflective material in order to excite atoms of the gain medium, an intracavity frequency altering device, and a switching means for selectively frustrating or allowing optical resonance, thereby enabling said amplifier pumping laser to emit pulses of laser light.

30. The system of claim 29, wherein:

the amplifier pumping laser further includes a plurality of diode lasers.

31. The system of claim 30, wherein:

the plurality of diode lasers are disposed along a lateral surface of the gain medium.

32. The system of claim 29, wherein:

radiation generated by the diode laser passes more than once through the gain medium.
Referenced Cited
U.S. Patent Documents
3731110 May 1973 Dewey, Jr.
3883752 May 1975 Davies et al.
3914709 October 1975 Pike et al.
4191928 March 4, 1980 Emmett
4227159 October 7, 1980 Barrett et al.
4603940 August 5, 1986 Shaw et al.
4653056 March 24, 1987 Baer et al.
4752931 June 21, 1988 Dutcher et al.
4756003 July 5, 1988 Baer et al.
4764731 August 16, 1988 Salour
4764739 August 16, 1988 Salour
4896119 January 23, 1990 Williamson et al.
4905247 February 27, 1990 Glessner et al.
4908832 March 13, 1990 Baer
4910740 March 20, 1990 Oka
4914663 April 3, 1990 Basu et al.
4918704 April 17, 1990 Caprara et al.
5033058 July 16, 1991 Cabaret et al.
5034951 July 23, 1991 Edelstein et al.
5084879 January 28, 1992 Suzuki et al.
5091778 February 25, 1992 Keeler
5123026 June 16, 1992 Fan et al.
5136597 August 4, 1992 Nightingale
5175664 December 29, 1992 Diels et al.
5181135 January 19, 1993 Keeler
5235606 August 10, 1993 Mourou et al.
5249190 September 28, 1993 Kortz et al.
5278852 January 11, 1994 Wu et al.
5280491 January 18, 1994 Lai
5287381 February 15, 1994 Hyuga et al.
5295144 March 15, 1994 Lawrenz-Stolz et al.
5296960 March 22, 1994 Ellingson et al.
5333145 July 26, 1994 Hyuga et al.
5343488 August 30, 1994 Guyot et al.
5406408 April 11, 1995 Ellingson et al.
5420876 May 30, 1995 Lussier et al.
5430754 July 4, 1995 Suzuki et al.
5440574 August 8, 1995 Sobottke et al.
5446749 August 29, 1995 Nighan, Jr. et al.
5450429 September 12, 1995 Klemer et al.
5463649 October 31, 1995 Ashby et al.
5469454 November 21, 1995 Delfyett, Jr.
5473626 December 5, 1995 Fan et al.
5479431 December 26, 1995 Sobottke et al.
5491707 February 13, 1996 Rieger et al.
5511085 April 23, 1996 Marshall
5521932 May 28, 1996 Marshall
5530582 June 25, 1996 Clark
5572358 November 5, 1996 Gabl et al.
5574740 November 12, 1996 Hargis et al.
5583882 December 10, 1996 Miyai et al.
5612967 March 18, 1997 Lai
5671241 September 23, 1997 Stamm et al.
5673281 September 30, 1997 Byer
5687186 November 11, 1997 Stultz
5720894 February 24, 1998 Neev et al.
5790303 August 4, 1998 Weston et al.
5805622 September 8, 1998 Brinkmann
5838701 November 17, 1998 Deutsch et al.
5880877 March 9, 1999 Fermann et al.
5909306 June 1, 1999 Goldberg et al.
5963363 October 5, 1999 Weston et al.
6122097 September 19, 2000 Weston et al.
6333485 December 25, 2001 Haight et al.
Other references
  • W. Koechner, Solid-State Laser Engineering, Chapters 2, 6, 8, and 10, Springer Series in Optical Sciences (printed in Germany 1976-1988), vol. 1, 89 pages in length.
  • User's Manuel by Spectra-Physics Lasers, “kHz Pulsed Ti:Sapphire Amplifier with Pulse Stretcher and Compressor,” (Quanta-Ray® TSA-1000), Feb. 1994, 122 page in length.
  • I.L. Bass et al., “Q-switched, intracavity doubled Nd:YAG laser side-pumped by a laser diode array,” SPIE High Power and Solid State Lasers II, vol. 1040, (1989), pp. 116-121.
  • German brochure (No. 13), “Soliton,” by Neuheiten Aus der Laser-und Messtechnik, Sep. 1996, 2 pages in length.
  • K. Lewotsk, “Multipass pumping scheme produces 13 W in Nd:YLF,” Laser Focus World, Aug. 1995, 1 page in length.
  • W.L. Nighan, Jr. et al., “DPSS lasers challenge water-cooled ion lasers,” Laser Focus World, Apr. 1996, 4 pages in length.
  • Q. Fu et al., “High-average-power kilohertz-repetition-rate sub-100-fs Ti:sapphire amplifier system,” Optics Letters, vol. 22, No. 10, May 15, 1997, pp. 712-714.
  • R. Mellish et al.,“All-solid-state diode-pumped cw femtosecond Cr:LiSrAlF6 lasers,” CLEO '94 (CLEO Convention, Wednesday Afternoon), pp. 234-235.
  • M.C. Farries et al., “Operation of Erbium-Doped Fiber Amplifiers and Lasers Pumped with Frequency-Doubled Nd:YAG Lasers,” Journal of Lightwave Technology, vol. 7, No. 10, Oct. 1989, pp. 1473-1477.
  • T. Yee Fan et al., “Diode Laser-Pumped Solid-State Lasers,” Reprinted from IEEE Journal of Quantum Electronics, vol. QE-24(6), Jun. 1988, pp. 442-457.
  • L.R. Marshall et al., “3-W continuous-wave diode-pumped 532-nm laser,” Optics Letters, vol. 17, No. 16, Aug. 15, 1992, pp. 1110-1112.
  • R. Buzyalis et al., “Amplification of Staged SS-Compressor Picosecond Single Pulses in Ti:Al2O3 Pulse Laser Pumped Amplifiers,” Litovsky fizichesky sbornik, vol. 32, No. 3, (1992), pp. 1-12.
  • C. Kim et al., “Deamplification response of a traveling-wave phase-sensitive optical parametric amplifier,” Optics Letters, vol. 19, No. 2, Jan. 15, 1994, pp. 132-134.
  • P. Georges, et al., “Candela Photo-injector: the Drive Laser” IEEE (Proceedings of the 1993 Particle Accelerator Conference), vol. 4 of 5 (1993), pp. 3053-3054.
  • W.L. Nighan, Jr. et al., “High efficiency, high energy optical amplifier for femtosecond pulses,” SPIE Applications of Ultrashort Laser Pulses in Science and Technology, vol. 1268, (1990), pp. 79-87.
  • F.P. Strohkendl et al., “Ultrastable amplification of femtosecond pulses” CLEO '94 (CLEO Convention, Tuesday Morning), May 8-13, 1994, p. 68.
  • K. Tamura et al. “Technique for obtaining high-energy ultrashort pulses from an additive-pulse mode-locked erbium-doped fiber ring laser” Optics Letters, vol. 1, p. 46, Jan. 1, 1994.
  • Donald J. Harter et al. “Short pulse amplification in tunable solid state materials” in Femtosecond to Nanosecond High-Intensity Lasers and Applications, Proceedings of the International Society for Optical Engineering, vol. 1229, p. 19, Jan. 17-18, 1990.
  • Y. Nabekawa et al. “Terawatt KrF/Ti:sapphire hybrid laser system” Optics Letters, vol. 18(22), p. 1922, Nov. 15, 1993.
  • Dan Botez et al. “The Next Generation of High-Power Semi-conductor Diode Lasers” TRW Space & Defense Quest, Winter 1991/1992, p. 21.
  • Philippe Bado et al. “Regenerative Amplification in Alexandrite of Pulses from Specialized Oscillators” IEEE Journal of Quantum Electronics, vol. 24(6), p. 1167, Jun. 1988.
  • Christopher P. Yakymyshyn et al. “Frequency-doubled, additive-pulse, mode-locked NaCl:OH- laser” Optics Letters, vol. 14(15), p. 791, Aug. 1, 1989.
  • M. Mizoguchi et al. “100-fs, 10-Hz, terawatt KrF laser” J.Opt. Soc. Am. B, vol. 9(4), p. 560, Apr. 1992.
  • John J. Zayhowski “Microchip Optical Parametric Oscillators” IEEE Photonics Technology Letters, vol. 9(7), p. 925, Jul. 1997.
  • W. J. Kozlovsky et al., “Monolithic MgO:LiNbO3 doubly resonant optical parametric oscillator pumped by a frequency-doubled diode-laser-pumped Nd:YAG laser” Optics Letters, vol. 14(1), p. 66, Jan. 1, 1989.
  • M. Gaignet et al., “High repetition rate all solid-state tunable ps source based on a diode-pumped Cr:LiSAF oscillator and a Ti:Sapphire regenerative amplifier” OSA TOPS, vol. 10, Advanced Solid State Lasers, Optical Society of America, p. 318, May 1997.
  • P. C. Becker et al. “High-intensity and high-repetition-rate Q-switched diode-pumped Nd:YLF-pumped femtosecond amplifier” Optics Letters, vol. 16(23), p. 1847, Dec. 1, 1991.
  • M. M. Choy et al. “A High-Gain, High-Output Saturation Power Erbium-Doped Fiber Amplifier Pumped at 532 nm” IEEE Photonics Technology Letters, vol. 2(1), Jan. 1990.
  • “TFR Tightly Folded Resonator User's Manual” Published by Spectra-Physics Laser Diode Systems Mountain View CA., Feb. 1992.
  • M. Lenzner et al. “Sub-20-fs, kilohertz-repetition-rate Ti:sapphire amplifier” Optics Letters, vol. 20(12), p. 1397, Jun. 15, 1995.
  • S. Backus et al. “Ti:sapphire amplifier producing millijoule-level, 21-fs pulses at 1 kHz” Optics Letters, vol. 20(19), p. 2000, Oct. 1, 1995.
  • Hamid Hemmati et al. “High Repetition-Rate Q-Switched and Intracavity Doubled Diode-Pumped Nd:YAG Laser” IEEE Journal of Quantum Electronics, vol. 28(4), Apr. 1992.
  • S. Takeuchi et al. “Highly efficient Ti:sapphire regenerative amplifier” Optics Communications, vol. 109, p. 518, 1994.
  • F. Zhou et al., “Double-side pumped Ti:sapphire regenerative pre-amplifier operating at 1.063 μm wavelength” Electronics Letters, vol. 31(13), p. 1060, Jun. 22, 1995.
  • M. Wittmann et al. “Experimental and theoretical investigation of a multipass, plane mirror, femtosecond dye laser amplifier” Applied Optics, vol. 34(24), p. 5287, Aug. 20, 1995.
  • P. F. Curley et al. “Multi-pass amplification of sub-50 fs pulses up to the 4 TW level” Optics Communications, vol. 131, p. 72, Oct. 15, 1996.
  • B. C. Stuart et al. “Chirped-Pulse Amplification in Ti:Sapphire Beyond 1 μm” IEEE Journal of Quantum Electronics, vol. 31(3), p. 528, Mar. 1995.
  • Koichi Yamakawa et al. “Generation of High Peak and Average Power Femtosecond Pulses at a 10 Hz Repetition Rate in a Titanium-Doped Sapphire Laser” IEEE Journal of Quantum Electronics, vol. 30(11), p. 2698, Nov. 1994.
  • B. Zysset et al., “High repetitiion rate femtosecond dye amplifier using a laser diode pumped neodymium:YAG laser” Appl. Phys. Lett. 54(6), p. 496, Feb. 6, 1989.
  • “Operation and Maintenance Manual” YG571C-20 Quantel International, Feb. 1986.
  • J.V. Rudd et al., “Regenerative Amplification of 55-Femtosecond Pulses at a 1 kHz Repetition Rate: Model and Experiment,” OSA Proceedings on Advanced Solid-State Lasers, 1994, vol. 20, Optical Society of America.
  • T. Joo et al., “Ti:Sapphire Regenerative Amplifier for Ultrashort High-Power Multikilohertz Pulses Without an External Stretcher,” Optics Letters, Feb. 15, 1995, vol. 20, No. 4, Optical Society of America.
  • R.P. Johnson et al., “Trident as an Ultrahigh Irradiance Laser,” SPIE, vol. 2377.
  • N.P. Barns et al., “Efficiency of Nd Laser Materials with Laser Diode Pumping,” IEEE Journal of Quantum Electronics, vol. 26(3), p. 558, Mar. 1990.
  • W.A. Clarkson et al., “High-power diode-bar end-pumped Nd:YLF laser at 1.053 μm,” Optics Letters, vol. 23(17), p. 1363, Sep. 1, 1998.
  • P.J. Hardman et al., “Energy-Transfer Upconversion and Thermal Lensing in High-Power End-Pumped Nd:YLF Laser Crystals,” IEEE Journal of Quantum Electronics, vol. 35(4), p. 647, Apr. 1999.
  • Mark D. Skeldon et al., “Quantitative Pump-Induced Wavefront Distortions in Laser-Diode- and Flashlamp-Pumped Nd:YLF Laser Rods,” IEEE Journal of Quantum Electronics, vol. 35(3), p. 381 Mar. 1999.
  • Pollinger et al., “Photoinduced Electron Transfer in Cyclophane-Bridged Porphyrin-Quinone Molecules. A Subpicosecond Transient Absorption Study”, Ber. Bunsenges. Phys. Chem., vol. 100, No. 12, 1996, pp. 2076-2080.
Patent History
Patent number: RE42499
Type: Grant
Filed: Aug 19, 2002
Date of Patent: Jun 28, 2011
Assignee: Coherent, Inc. (Santa Clara, CA)
Inventors: Jeremy Weston (San Jose, CA), William Eugene White (Campbell, CA), Leigh John Bromley (Palo Alto, CA), Frank Godwin Patterson (Danville, CA)
Primary Examiner: Mark Hellner
Attorney: Morrison & Foerster LLP
Application Number: 10/224,158
Classifications
Current U.S. Class: Particular Pumping Type (e.g., Electrical, Optical, Nuclear, Magnetic, Etc.) (359/345); Regenerative (359/348); Pump Cavity (372/72)
International Classification: H01S 3/00 (20060101);