|Publication number||US7692854 B2|
|Application number||US 11/975,871|
|Publication date||Apr 6, 2010|
|Priority date||Oct 22, 2007|
|Also published as||US20090103172|
|Publication number||11975871, 975871, US 7692854 B2, US 7692854B2, US-B2-7692854, US7692854 B2, US7692854B2|
|Inventors||David Clubley, Angus Sutherland Bell|
|Original Assignee||Coherent, Inc.|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (18), Non-Patent Citations (2), Referenced by (3), Classifications (18), Legal Events (2)|
|External Links: USPTO, USPTO Assignment, Espacenet|
The present invention relates in general to repetitively pulsed lasers and pulsed optical amplifiers. The invention relates to such lasers and amplifiers in which there is a provision for maintaining a constant pulse power or pulse energy as the pulse repetition rate is changed.
In laser machining or material processing operations in which pulses of laser radiation are repetitively delivered to a workpiece it is often necessary to change the repetition frequency (PRF) of the pulses while maintaining the peak power of the pulses, or the energy per pulse, constant. In a pulsed laser or a pulsed, master oscillator power amplifier (MOPA) laser-system including a continuously pumped gain-medium a change in repetition rate can result in a change in pulse energy. This is because the interval between the delivery of pulses in a train, among other factors, determines the gain available for each pulse. Further, in a pulsed-laser that is activated to provide a pulse train after a period of inactivity in which the gain medium continues to be pumped, the power of the first pulse in a train can be much higher than any subsequent pulses.
Several techniques for providing variation of the PRF of a pulsed laser, or a pulsed laser and amplifier system while maintaining constant energy per pulse have been described in the prior-art. These techniques include operating the laser or amplifier in a continuous (CW) mode while pulses are not being delivered, allowing the laser or amplifier to operate in a CW mode between pulses in a train, and operating the laser or amplifier at a PRF much greater than the nominal PRF before a pulse train is delivered or between pulses in a train. Examples of such techniques are described in one or more of U.S. Pat. Nos. 6,038,241; 6,414,980; 6,418,154; 6,683,893; and 6,931,035, all of which are assigned to the assignee of the present invention.
The method of carrying of the techniques primarily involve certain sequences of operation of a Q-switch which is normally provided in the laser for causing the laser to operate in a pulsed mode and controlling the PRF of the laser, whether or not any measures were taken for controlling pulse energy or first pulse suppression. Such additional operations include steps in which the Q-switch must be selectively partially opened (or closed). An acousto-optic Q-switch is preferred for the operation of the lasers described. This type of Q-switch is operable in a partially open or closed mode.
Adding such Q-switch operations for pulse-energy control adds to the complexity of circuitry required to control the Q-switch as careful synchronization of the additional operations with “normal” operations is required. Certain amplifier types such as regenerative amplifiers used in ultrafast laser-amplifier systems, require a Pockels-cell type Q-switch, which operates by switching electrically induced birefringence, and does not lend itself to operation in a partially open or partially closed mode. It would be advantageous to have a method for controlling pulse energy and providing first pulse suppression that did not require complex, synchronized Q-switch operations. Preferably such a method would be primarily passive and be effective independent of the type of Q-switch in the laser.
In one aspect apparatus in accordance with the present invention for amplifying a seed pulse in response to an external trigger-signal, comprises a source of seed pulses and a primary resonator terminated by first and second mirrors and arranged to receive the seed pulses. The primary resonator includes a gain-medium and an optical switch. A pump radiation source is arranged to optically pump the gain-medium in a continuous-pumping mode, thereby providing available gain in the gain-medium. The apparatus also includes a secondary resonator including the gain-medium. The secondary resonator does not include the optical switch, but includes a selectively-variable attenuator for selectively varying losses in the secondary resonator. The optical switch and the selectively-variable attenuator are controllable such that when the gain-medium is being pumped and the seed pulse is not being amplified, the selectively-variable attenuator allows lasing to occur in the secondary resonator at a level selected to limit gain in the gain-medium to a predetermined level. The optical switch and the selectively variable attenuator are also controllable such that on receipt of the trigger signal, the selectively-variable attenuator causes lasing to cease in the secondary resonator for a predetermined time period during which gain in the gain medium is allowed to rise above the predetermined level, the optical switching causes the seed pulse to be trapped in the primary resonator and the trapped seed pulse is amplified in the primary resonator, and such that after the predetermined time period the optical switch causes the amplified seed pulse to be delivered from the primary resonator, and the selectively-variable attenuator causes lasing to occur in the secondary resonator at the level selected to limit gain in the gain-medium to the predetermined level.
The accompanying drawings, which are incorporated in and constitute a part of the specification, schematically illustrate a preferred embodiment of the present invention, and together with the general description given above and the detailed description of the preferred embodiment given below, serve to explain principles of the present invention.
Referring now to the drawings, wherein like components are designated by like reference numerals,
The primary resonator includes a birefringent gain-medium 12 that has different gain for two polarization-planes perpendicular to each other. One such gain-medium is neodymium-doped gadolinium orthovanadate Nd:GdVO4. This is a tetragonal crystal material usually arranged with an a-axis aligned with the resonator axis, with the highest gain being for light plane-polarized parallel to the c-axis. In the continuing description it is assumed that gain-medium 12 is Nd:GdVO4, but this should not be construed as limiting the present invention. In this arrangement, the axis of the primary resonator terminated by mirrors M1 and M4 is aligned with the path of the o-ray through the birefringent gain-medium, i.e., along the a-axis of the crystal
Gain-medium 12, during an operational period of apparatus 10 is continually optically pumped by radiation (pump-light) L from a diode-laser array (not shown) and delivered from the diode-laser array by an optical fiber 14. The gain-medium provides peak gain at about 1064 nm. The pump-light is focused into the gain-medium by lenses 15 and 16 through mirror M3 which has high reflection at the peak gain wavelength and high transmission at the wavelength of the pump-light. When regenerative amplifier 14 is not amplifying a pulse, a quarter-wave plate 22 cooperative with a Pockels cell 24 and polarizing beamsplitter 20 prevents radiation from being generated in the primary resonator terminated by mirrors M1 and M4.
This is achieved by setting the Pockels cell to provide net zero polarization rotation such that plane-polarized radiation that has been reflected from polarizing beamsplitter 20 and made a double pass through the quarter-wave plate 22 and the Pockels cell is polarization-rotated 90° and is now polarized in a plane indicated by arrow Pp that is transmitted by the polarizing beamsplitter of the primary resonator. Accordingly radiation can not circulate in the primary resonator and any seed pulses are not trapped. This can be described, for purposes of this description and the appended claims, as the primary resonator being in an “open” mode. In the open mode, the gain n the gain-medium would be at an indeterminate level absent any preventive measure.
This is prevented in this embodiment of the inventive apparatus by providing a secondary resonator terminated by mirror M4 and another mirror M5 and folded by mirror M2. This resonator does not include the switching arrangement provided by polarizing beamsplitter 20, quarter-wave plate 22 and the Pockels cell. The longitudinal axis of this secondary resonator is aligned with the path of the e-ray (extraordinary ray) through the birefringent gain-medium. The a-axis is the path of the ordinary ray (o-ray) through the gain medium. The longitudinal axis of the primary resonator is aligned with the path of the o-ray though the gain-medium. The axes of the primary and secondary resonators are collinear between the gain-medium and mirror M4. In the gain-medium and between the gain-medium and fold-mirror M2 the axes of the primary and secondary resonators (designated by solid and dashed lines respectively) diverge. Preferably, the face 12A of the gain-medium (the face furthest from mirror M3) is non-orthogonally aligned (wedged) with the a-axis to increase the angle between the resonator axes. A wedge angle of about 3° on face 12A of provides that there is an angle of about 0.7 degrees between the resonator axes.
CW radiation is generated in the secondary resonator for the “wrong” polarization-plane, i.e., the polarization-plane for which the gain of gain-medium 12 is least. The power of radiation generated can be controlled by selectively adjusting a tilt angle that a transparent plate 42 such as a glass or fused silica plate makes with the secondary-resonator axis as indicted by arrows A. The gain is preferably held at a level slightly higher, for example about 10% higher than the peak gain reached during delivery of a pulse train. The primary resonator is a resonator only for plane-polarized radiation having the “right” polarization-orientation in gain-medium 12, i.e., the polarization-orientation for which the gain of gain-medium 12 is greatest. An acousto-optic modulator could be used instead of plate 42 to provide active control of losses.
When it is desired to deliver a train of pulses from the regenerative amplifier, a train of seed-pulses is delivered from a mode-locked seed-pulse laser 28. Mode-locked lasers typically provide pulses having a duration of a few picoseconds or less at pulse-repetition frequencies (PRFs) of a few megahertz (MHz). The regenerative amplifier is operated at pulse-repetition frequencies of tens to hundreds of kilohertz (KHz), accordingly, only selected ones of the pulses from the seed laser are amplified. The selection mechanism is well-known to those skilled in the art but is reviewed briefly below as it pertains to the present invention.
A pulse to be amplified is directed by mirrors 30 and 32 through a Faraday isolator 34, a lens 36 and another Faraday isolator 24 and delivered to polarizing beamsplitter 20 plane-polarized in a plane that is transmitted by the polarizing beamsplitter. The seed pulse enters the primary resonator while it is in the open state. The polarization-plane of the pulse is then rotated by 90 degrees following a double pass through the quarter-wave plate and the (inactive) Pockels cell as described above and therefore will be reflected by the polarizing beamsplitter 20 into the primary resonator and towards gain-medium 12. At about this point, the Pockels cell is switched to a state such to provide a 90 degree polarization rotation on the double pass, whereby a double pass through the quarter-wave plate and the Pockels cell provides no net polarization. Accordingly the pulse is trapped and circulates in the primary resonator, being amplified as energy is extracted by the pulse from gain-medium 12. This will be referred to as the “closed” state of the primary resonator. A half-wave plate 23 rotates the polarization of the pulse to that for which gain is strongest in gain medium 12 and re-rotates the polarization plane of the pulse returning from the gain-medium into the orientation that is reflected by polarizing beamsplitter 20. Essentially as soon as this circulation begins, gain in the gain-medium is reduced below the threshold required for CW lasing in the secondary resonator, and lasing in the secondary resonator ceases.
After a predetermined time, the Pockels cell is switched back to a state such that a double-pass through quarter-wave plate 22 and the Pockels cell produce a net 90 degree polarization rotation, and the amplified pulse is transmitted out of the primary resonator via beam splitter 20. Optionally, a sample of the pulse can be obtained from a beamsplitter 40. The main output pulse is directed out of apparatus 10 along the rejection channel of Faraday isolator 24 as depicted. This pulse trapping and transmitting is repeated until the train of amplified pulses is delivered. After the final pulse in a train is delivered the gain increases until CW lasing begins in the secondary resonator as described above, and clamps the gain in gain-medium 12 until it is desired to deliver another train of pulses.
It was found that when the regenerative amplifier was operated at higher PRF, the secondary resonator became increasingly less effective at first pulse suppression. This is believed to be because the peak gain between pulses was increasingly reduced. In a with-and-without-the-secondary resonator comparison made operating the above-discussed example of apparatus 10 at a PRF of 200 KHz, it was found that the first pulse in a pulse-train with the secondary-resonator gain-clamping operative had a peak power that was about five times the average peak power of the second and subsequent pulses in the pulse-train. Without the gain-clamping, however, the peak-power in the first pulse was about 20 times the average peak power of the second and subsequent pulses in the pulse-train. It is to be expected that this frequency of dependence of the effectiveness of the present invention may be different for different gain-media.
Those skilled in the art will recognize that while the present invention has been described in the context of a particular example of a regenerative amplifier, the invention is applicable to any regenerative amplifier including a gain-medium having a polarization dependent gain and being sufficiently birefringent to allow a secondary resonator to be added according to principles of the present invention. Examples of such gain media include but are not limited to (any) ion-doped yttrium orthovanadate (X:YVO4), and ion-doped gadolinium orthovanadate (X:GdVO4).
The invention is also applicable to gain-media that have minimal birefringence and minimal polarization dependence such Ti:sapphire and Nd:YAG. By way of example,
Those skilled in the art will also recognize without further detailed description or illustration that principles of the present invention are applicable not only in a primary resonator that is operated as a regenerative amplifier but also in a primary resonator that is operated as a Q-switched laser to generate pulses. In the case of the embodiments of
Returning now to a discussion of regenerative amplifiers, apparatus 10 of
In certain applications it would be advantages to be able to change the pulse repetition rate while the amplifier is operating, and possibly even advantageous to be able to deliver pulses with arbitrary (irregular) intervals therebetween. One method for accomplishing this is described below with reference to
In a preferred method of operating apparatus 60, it is necessary to determine the maximum PRF that will be required from the amplifier. The number of round trips for optimizing amplification of a seed pulse at that repetition rate is determined. By way of example, a PRF of 60 kHz may require five round trips, after trapping the seed pulse into the amplifier before delivery of the amplified pulse to optimize output pulse energy. This number of round trips becomes a constant for the scheme. It is assumed, as will be true in most instances, that the optimized number of round trips will be sufficiently low that the gain of the amplifier can be far from saturated. This means that CW lasing in the secondary resonator can reduce the gain to well below the steady-state gain for operation at the maximum PRF.
This preferred method of operation is described below with reference to the timing diagram of
At time T1, an external trigger is supplied to controller 62 requesting a pulse from the amplifier (see top line of
The above described method provides about constant pulse energy independent of pulse repetition rate provided that the external trigger pulse is not applied faster than the maximum selected repetition rate. The amplifier is simply responding to an external trigger and the starting gain in the amplifier for each pulse is the same.
It should be noted here that controller 62 and Pockels cell and switching electronics 24 are indicated in
In summary, while the present invention is described and depicted herein in terms preferred embodiments, the invention is not limited to the embodiments described and depicted. Rather, the invention is limited only by the claims appended hereto.
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|U.S. Classification||359/348, 372/25|
|International Classification||H01S3/106, H01S3/17, H01S3/00|
|Cooperative Classification||H01S3/235, H01S3/09415, H01S3/082, H01S3/1611, H01S3/115, H01S3/1103, H01S3/1106, H01S3/1671, H01S3/106, H01S3/0816, H01S3/117|
|European Classification||H01S3/106, H01S3/23A2R|
|Dec 6, 2007||AS||Assignment|
Owner name: COHERENT, INC., CALIFORNIA
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:CLUBLEY, DAVID;BELL, ANGUS SUTHERLAND;REEL/FRAME:020220/0977
Effective date: 20071029
Owner name: COHERENT, INC.,CALIFORNIA
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:CLUBLEY, DAVID;BELL, ANGUS SUTHERLAND;REEL/FRAME:020220/0977
Effective date: 20071029
|Sep 4, 2013||FPAY||Fee payment|
Year of fee payment: 4