The transient theory of stimulated Brillouin scattering (SBS) in optical fibers is used to investigate the effects of weak feedback of incident broadband laser fields exhibiting different spectral shapes. The proper boundary conditions are given for the forward- and backward-propagating electric fields inside the fiber with a finite amount of reflectivity at the fiber ends. When the linewidth of the laser approaches the Brillouin frequency shift, a weak reflection of the laser field overlaps with the SBS gain and can be amplified in the fiber, resulting in an apparent reduction in SBS threshold. It is shown that the spectral shape of the incident field and its overlap with the SBS gain spectrum affects the SBS signal. Numerical examples are presented for incident laser fields that (1) simulate a pulsed, multilongitudinal-mode laser and (2) are a constant amplitude with a sinusoidal phase modulation. For the pulsed field with mode spacing much less than the Brillouin linewidth, calculations show that an end reflection of 0.01% (−40 dB) of the laser field with a linewidth equal to 0.75 of the Brillouin frequency shift can reduce the effective SBS threshold by a factor of 1.5. When the incident laser field is constant amplitude and phase modulated with a sinusoid, calculations predict sharp and distinct enhancement of the reflected power when the ratio of the Brillouin frequency shift to the modulation frequency is an integer for end reflections as low as 0.001% (−50 dB). Experiments performed with a sinusoidal phase modulated signal confirm the theoretical predictions. These results have implications on the design of high-power fiber laser systems that utilize spectral broadening to suppress SBS.
The transient theory of stimulated Brillouin Scattering (SBS) in optical fibers is used to investigate the effects of feedback of an incident periodic phase-modulated laser field. Phase modulation with a single sine wave and a pseudo-random binary sequence (PRSB) are investigated. It is shown that a reflection as small as 0.001% (-50 dB) of a laser field from the fiber end can lead to enhancement in the reflected power and effectively reduce the SBS threshold if the laser optical spectrum overlaps with the SBS gain spectrum. These results have implications on the design of high power fiber laser systems that utilize periodic phase modulation techniques for broadening the laser field to suppress SBS.
We report a master-oscillator/power-amplifier laser system featuring a polarizing and coilable 40-micron-core Yb-doped
photonic crystal fiber as the final-stage amplifier. The laser source generates 3.4 ns pulses at a repetition rate 19 kHz,
with maximum pulse energy 1.2 mJ, maximum average power 22.8 W, near diffraction-limited (M2 < 1.1) beam quality, and 20% electrical to optical efficiency in a compact package. This pulsed-fiber laser flight system provides high pulse energy, average power, peak power, diffraction limited beam quality, and high efficiency all in a thermally and
mechanically stable compact package.
The transient theory of stimulated Brillouin Scattering (SBS) in optical fibers is used to investigate the effects of weak
feedback of an incident broadband laser field. When the linewidth of the laser approaches the Brillouin frequency shift,
a weak reflection of the laser field overlaps with the SBS gain and can be amplified in the fiber resulting in an apparent
reduction in SBS threshold. We show that a reflection of 0.01% (-40 dB) of a laser field with a linewidth equal to the
Brillouin shift can reduce the SBS threshold by a factor of 2. These results have implications on the design of high
power fiber laser systems that utilize spectral broadening to suppress SBS.
We describe a pulsed blue (485 nm) laser source based on frequency quadrupling a pulsed Tm fiber laser. Up to 1.2 W at 485 nm was generated with an M2 of 1.3. At 10 kHz pulse repetition frequency, the output pulse at 485 nm was 65 ns FWHM resulting in an estimated peak power of 1.8 kW. We anticipate further improvements in power scaling with higher power Tm fiber lasers and improved conversion efficiency to the blue with optimized AR coatings and nonlinear optical crystals.
High-speed, high-resolution materials processing strongly benefits from optical sources that deliver high peak power in
short, high-repetition-rate pulses of excellent beam quality. These sources are also of interest for achieving high average
power at nonlinearly-generated wavelengths. Until recently, high peak power, high-repetition-rate pulses have only been
available from solid-state lasers. Fiber lasers and amplifiers offer significant advantages over solid-state lasers in terms
of size and wall-plug efficiency. This paper presents a fiber-based master-oscillator/power-amplifier (MOPA) source at
1064nm featuring 84-μm-core, polarization-maintaining Yb-doped photonic crystal fiber that generates ~20ps - 100ps
pulses at variable pulse repetition frequencies (PRFs), from 10kHz to 100MHz. The flexibility in pulse format allows the
source to be tailored to the application. Where peak power is critical, the PRF is reduced to achieve maximum peak
power. Where average power is needed, the PRF is increased to achieve high average power. Peak powers of ~4MW
have been achieved at reduced PRF (100kHz), and average powers greater than 172W have been demonstrated at high
PRF (100MHz) in a linearly-polarized output beam.
We report on an eye safe fiber laser generating >5 Watts of average power at 50 kHz packaged in a
cylinder measuring 6" in diameter and 3.75" in length to show compatibility with advanced seeker
concepts. To our knowledge, this represents the highest average power per unit volume from an eye
safe pulsed fiber laser generating multi-Watts of average power.
We report on the development of a multi-channel all-fiber based laser system for
LADAR applications. Two design pathways for the multi-channel laser system were
investigated: (i) multiple externally triggered single channel MOPA (SCMOPA) systems
and (ii) a single master-oscillator/multiple power-amplifier (SMOMPA) system. We
designed and tested a single channel MOPA system that consists of a seed source, two
single mode amplifiers and a power amplifier. With this system we were able to achieve
up to 195&mgr;J/pulse at 6kHz with a pulse duration of 3ns. For evaluating the SMOMPA
approach we built a bread board based on the single channel results with one master
oscillator and 4 power amplifiers. With this breadboard we achieved pulse energies from
each of the four power amplifiers of 120±4&mgr;J at 6kHz and 78-90&mgr;J at 18kHz. The
temporal line-shapes emitted from each power amplifier were identical within the signal-to-noise level of the temporal traces and have a FWHM=2.2ns.
All-fiber contained laser systems play a key role, in the development of rugged, compact, and highly
efficient eye-safe laser sources that can generate high peak and average powers and short (<5 ns)
pulses. Application of such laser systems include spectroscopy, LIDAR, free-space
communications, materials processing and nonlinear optics.
In this paper we present further improvement on a novel high power all-fiber-based master
oscillator power amplifier (MOPA) laser system operating in the C-band with <5 ns pulses and a
repetition rate range of 6kHz − 200kHz. The system was optimized for performance of repetition
rates between 6kHz and 18kHz. With this system, pulse energies of 322 μJ with a peak power of
170kW and an average power of 1.9W were generated using a custom designed Er:Yb co-doped
double-clad fiber. The spectral output of the amplified pulses shows no spectral broadening due to
Four-Wave-Mixing or Stimulated Raman scattering for pulse energies with less than 260μJ.
Additionally, a beam quality M2=2.1+/-0.1 was achieved. The physical performance parameters of
the all-fiber laser system make it very suitable for a variety of applications. The performance of the
MOPA system and the experimental data are presented and discussed. To our knowledge the
combination of the presented pulses energies, peak power, average power are the highest ever
recorded in an all fiber system.
In order to develop an efficient eye-safe laser, operating in the 1.53 μm region, we have written software that models the performance of a passively Q-switched Er:Yb:glass laser with a divalent cobalt Co2+:spinel saturable absorber. At present a 0D model, which uses a plane-wave approximation, has been completed. The model is based on a set coupled first order differential equations that describe the laser dynamics. These equations represent a two-level Yb3+ diode pump scheme, a five-level Er3+ gain medium, and a four-level Co2+ Q-switch. The model takes into account cooperative upconversion and excited state absorption (ESA) in both the gain and absorber media. Solutions to the rate equations and optimization examples are presented.
We present a novel high power all-fiber-based master oscillator power amplifier (MOPA) laser system operating in the C-band (1.5 mm) with pulses <5ns and a repetition rate range of 200 kHz. This system generates >4 Watts of average power and a maximum pulse energy of 20 mJ and peak power of 5 kW at 200 kHz using custom designed Er:Yb co-doped double-clad fibers. This system was also operated at reduced repetition rates of 6 kHz and pulse energy of 165 mJ was generated with a peak power of 28 kW. By shortening the seed pulses a peak power of up to 33.9 kW with a pulse energy of 73 mJ was achieved at 20 kHz. A beam quality of M2=1.2 was achieved, which makes this system very suitable for scanning lidar applications.
In order to develop an efficient eye-safe laser, operating in the 1.53μm region, we have written software that models the performance of a passively Q-switched Er:Yb:glass laser with a divalent cobalt Co2+:spinel saturable absorber. At present we have completed a 0D model for which we developed a set of coupled first order differential equations to describe the laser dynamics. These equations represent a two-level Yb3+ diode pump scheme, a five-level Er3+ gain medium, and a three-level Co2+ Q-switch. The model takes into account cooperative upconversion and excited state absorption (ESA) in both the gain and absorber media. Input parameters for the rate equations such as ion concentrations, cross sections, and lifetimes are obtained from experimental and published data. These parameters can be easily varied via a graphical user interface (GUI) that was developed for the model. A study comparing laser characteristics such as pulse energies, peak power, and pulsewidths (FWHM) is carried out between our model and experimental data. Future work will focus on a 1D model which introduces the spatial variation of the pump and laser beam within the cavity.
We have developed public domain numerical models of nonlinear three-wave mixing in birefringent crystals that include diffraction and dispersion. They are suitable for detailed and realistic modeling of mixing for both a single crystal pass and for multiple passes appropriate for a crystal in a resonant cavity. We routinely compare our models with laboratory devices, usually achieving excellent agreement.
In this paper we report on the performance of a modular single mode pulsed fiber laser system operating in the C-band. With off-the-shelf telecom components and specialty-designed electronics, 3 kW peak power can be generated in a short (1 ns) pulse at 10 kHz at 1545 nm; however, the onset of nonlinear optical effects (SRS, FWM, and SPM) is observed at a 1kW peak power level. Using highly doped erbium fibers, peak powers up to 13kW and pulse energies of up to 20μJ have been generated with a pulse duration range of 0.6-5 nsec, repetition rates between 3kHz to 1 MHz, and at a wavelength of 1545.3nm and 1567.5 nm before the onset of nonlinear effects became noticeable. Therefore, with the use of highly doped erbium fiber, the onset of nonlinear effects can be increased by an order of magnitude. For narrowband amplification, stimulated Brillouin scattering (SBS) is the limiting nonlinear process. In this regime we recorded the onset of SBS at 8μJ/pulse with a duration of 2.5 nsec. Depending on the pulse shape and pulse duration, self phase modulation (SPM) was also observed, which spectrally broadens the output centered at the signal wavelength; however, the spectral broadening due to SPM is only minor compared to SRS and FWM. It was also demonstrated that pulse steepening is minimized with an appropriate seed waveform. A 3 ns, shaped, input pulse nearly maintained its pulse duration after amplification. Without pulse shaping, the pulse shortened to 1.1 ns.
Single frequency laser sources, which also provide tunability, have wide use in spectroscopy and remote sensing as well as for other applications such as optical pumping. Optical parametric oscillators (OPOs) offer the potential for broadly tunable output in spectral regions inaccessible by conventional laser sources. We report here on the design and use ot an OPO architecture developed to produce pulsed, tunable, single-frequency output in the mid-infrared spectral region and used for optical pumping of gas. Design information about two separate OPOs that were developed will be presented along with experimental details of the optical pumping of CO on the (3-0) band around 1.57 μm and on the (2-0) band around 2.3 μm.
The propagation of high power narrowband laser pulses in multimode fibers and the limitations due to SBS are presented. An injection seeded pulsed Nd:YAG laser operating at 10 Hz was used to pump undoped step index fibers to determine the SBS threshold under various conditions. Measurements on 50μm core diameter fibers with various fiber lengths and pulse durations at 1064 nm were performed and simulated with a computer code. The code considers the time dependent coupling between the pump wave, the Stokes wave, and the acoustic wave. The experimental results are in good agreement with the numerical predictions. Our results quantify the limitations of high power narrowband pulse transmission in multimode fibers.
A tandem PPLN and ZGP optical parametric oscillator (OPO) has demonstrated the generation of multiple wavelength output in the mid-infrared. A pulsed Nd:YVO4 laser, oeprating at 1.342 microns, pumped a PPLN OPO that generated 2.12 microns and 3.66 microns. 8.4W of 1.342 microns was available at the PPLN. The PPLN OPO produced 2.6W at 2.12 microns, of which 2.35W was available to pump the ZGP OPO. The ZGP OPO generated a total combined output of 0.85W at 3.9 microns and 4.6 microns. The threshold of the ZGP OPO was measured to be 60 micro-Joules (10.6 MW/cm2, ~18 ns FWHM pulse).
We have developed a computer model calculating bare cavity transverse eigenmodes for super-gaussian unstable resonators, including aperture diffraction in the gain medium. This generalized simulation, based on the Fox and Li Power Method, reduces the input parameters to five: rod longitudinal position, cavity magnification, super-gaussian order of the output coupler reflectivity, and Fresnel numbers for the cavity and rod apertures. Using two-dimensional FFT's to discretize the Huygen-Fresnel numbers, the output fields at the plane of the rod aperture and exiting the output coupler were subjected to beam quality (M2) and extraction efficiency (Xeff) analysis. Beam quality was found to be the most sensitive to cavity magnification, with M2 values varying as much as 30% or more with 3% shifts in magnification, which can occur during rod lensing. Avoiding peaking M2 values is demonstrated with design curves for two different cavity Fresnel numbers, and super-gaussian orders. The cavity Fresnel number and the super-gaussian order are shown to only weakly affect beam quality, although extraction efficiency varies strongly with the latter. Finally, optimized rod longitudinal position was explored for promising combinations of the other four parameters, and it was found to be near the high reflector (HR) end of the cavity, in terms of M2 analysis.
Laser radar systems are required for various military applications including obstacle detection, target recognition, and terrain mapping. Each application requires different system parameters such as pulse energy, repetition rate, and field of view. This paper presents a review of a multifunction laser radar system developed and tested for the Cooperative Eyesafe Laser Radar Program (CELRAP) of the U.S. Army CECOM Night Vision and Electronic Sensors Directorate.
Laser radar systems are required for various military applications including obstacle detection, target recognition, and terrain mapping. Each application requires different system parameters such as pulse energy, repetition rate, and field of view. This paper presents a review of a multifunction laser radar system under construction for the Cooperative Eyesafe Laser Radar Program (CELRAP) of the U.S. Army CECOM Night Vision and Electronic Sensors Directorate.
We describe a computationally efficient numerical simulation model of optical parametric oscillators (OPOs) appropriate for the simulation of high energy pulsed OPOs using unstable resonators. The model calculations are time dependent and include the effects of diffraction and pump depletion in the parametric amplification process. The computational time required to solve the model equations for unstable resonator OPOs is reduced by applying a coordinate transformation to the paraxial three-wave mixing equations. An essential characteristics of this transformation is that it allows for the extraction of the geometric curvature from the intracavity fields resulting in the propagation of approximately collimated fields. We demonstrate the utility of this new model by presenting the results of a detailed numerical study of a high energy, non-critically phase matched KTA OPO using unstable resonators. Our results predict that an optimally designed confocal unstable resonator can produce near diffraction limited output at high pulse energies.
A design, as well as verification measurements, are presented for an end pumped, 20 Watt output power, single frequency, Tm:YAG laser driver for pumping a HBr mid-IR laser. Efficient end pumping of the Tm:YAG is achieved by `close lens coupling' 15 Watt average power, room temperature, 785 nm diode bars to several Tm:YAG rods. The Tm:YAG laser is operated single frequency (injection seeded) in order to couple efficiently its output to the narrow absorption band of HBr. A 2 micron laser operating multi-line, but with a bandwidth less than 1 - 2 GHz, is also under consideration using a HBr laser with increased pump absorption characteristics obtained by increasing the pressure or by placing the HBr laser inside the 2 micron laser using intra-cavity 2 micron pumping.
A novel computer model of an injection-seeded pulsed CO2 laser is used to predict the intrapulse frequency chirp as a function of laser resonator and gain medium parameters. A new mechanism for causing intrapulse frequency sweeping is predicted. It is found that nonuniform and time-varying gain saturation changes the transverse distribution of the intracavity electric field during the laser pulse, which leads to a change in the oscillator frequency. This mechanism is predicted to be much more pronounced in low-magnification graded-reflectivity unstable resonators as compared to low-Fresnel-number stable resonators. It is also shown that to obtain quantitative estimates of chirp in large aperture unstable resonators lasers, it is necessary to couple the intracavity electric field with realistic laser kinetics and index-changing mechanisms.
Access to the requested content is limited to institutions that have purchased or subscribe to SPIE eBooks.
You are receiving this notice because your organization may not have SPIE eBooks access.*
*Shibboleth/Open Athens users─please
sign in
to access your institution's subscriptions.
To obtain this item, you may purchase the complete book in print or electronic format on
SPIE.org.
INSTITUTIONAL Select your institution to access the SPIE Digital Library.
PERSONAL Sign in with your SPIE account to access your personal subscriptions or to use specific features such as save to my library, sign up for alerts, save searches, etc.