High-repetition-rate and high-power picosecond regenerative amplifier based on a single bulk Nd:GdVO4 crystal Download: 737次
1 Introduction
Compact, stable and high-power diode-pumped short-pulse laser amplifier systems with excellent spatial quality are ideal sources for high-power optical parametric chirped pulse amplification (OPCPA) and efficient laser processing[1–5]. Among various configurations, regenerative amplifiers (RAs) are routinely used to enhance the output of mode-locked oscillators because of their ability to provide gains of several orders of magnitude and a resonator structure that maintains the spatial quality of the seed[6–9].
In the past two decades, various solutions and architectures have been proposed for power scaling of regenerative amplifiers. The thin-disk geometry was particularly impressive for heat dissipation. Nubbemeyer
High-repetition-rate regenerative amplifiers are beneficial for promoting industrial throughput and reducing data accumulation or processing time in scientific applications. However, high repetition rates come with bifurcation and even chaotic pulse train dynamics, in which the pulse energy is unstable[16]. This bifurcation-termed phenomenon constitutes a major impediment for RAs operated at high repetition rates[3], where the operating parameters of the laser systems have to be carefully optimized to maintain equilibrium[17–20]. A detailed analysis concerning this problem is elaborated in the following section. For more than a decade, several methods have been proposed to eliminate this deleterious effect. The methodologies include raising the seed energy[19, 21], pumping at higher intensity[17], operating at the second operating point outside the unstable region if the effect could not be thoroughly avoided[22], or working in a bistable regime with a negligible lower bifurcation branch[23]. Consequently, efforts to optimize system parameters are necessary to achieve stable and efficient performance.
RAs based on bulk neodymium gain media show specific advantages. A high stimulated-emission cross-section simplifies the system design, and requirements such as the reflectivity for optical components are allayed. RAs based on them are generally free of CPA because of the relatively longer pulse durations. Diode-pumped RAs built with Nd:YAG or Nd:YLF crystals are commonly side-pumped for high pulse energy generation[24–29]. End-pumping schemes provide simpler structures and are always realized by neodymium-doped vanadate crystals. Lasers based on neodymium-doped vanadate crystals deliver moderate pulse energies as well as average power, but less complex cavities and pumping schemes are required. In 2013, a regenerative amplifier based on a Nd:YVO
Here we report a 100 kHz high-power regenerative amplifier based on a single bulk Nd:GdVO4 crystal. The basic properties of three Nd-doped single crystals are compared in Table
Table 1. Basic properties of three Nd-doped single crystals (see Refs. [35–42]).
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2 Numerical simulations
Looking at its working principle, one RA operation cycle can be divided into two successive stages: the pump stage and the amplification stage. No voltage is applied to the Pockels cell during the pump stage. The amplification stage starts when the seed is injected into the amplification cavity and a high voltage is applied to the Pockels cell. When the pulse energy reaches a certain level, the high voltage is switched off, the amplified pulse is ejected and the next cycle begins[20]. For continuously pumped regenerative amplifiers, this operation cycle division is justified when the amplification stage duration is considerably shorter than the inverse of the repetition rate so that the impact of the pump during amplification can be neglected. Nevertheless, for continuously pumped regenerative amplifiers, the operation cycles become interdependent when the pump stage duration becomes comparable to or even shorter than the upper state lifetime of the respective transition. Let us consider a 100 kHz RA based on a Nd:GdVO4 crystal as an example. The pump stage duration (
Numerical simulations were performed to fully exploit the system’s capability: to ensure stable operation and extract as much stored energy as possible. Diagrams presented in the parameter space are very helpful to realize this prospect[19, 20, 44]. The parameter space separatrix and curve of
The basic equations describing the pump and amplification stages are listed as Equations (
Here
Table 2. Key parameter values for simulation.
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Fig. 1. Parameter separatrix (colored blue and yellow) and curve of $\text{NRT}^{\text{MAX}}$ (colored bold black). The red star indicates the optimum working point for 100 kHz repetition rate operation.
In the simulation, the repetition rate of the RA operation range was set between 1 kHz and 150 kHz. For the seed energy, the mode mismatch between the seed and the RA in the spatial and spectral domains should be taken into account[19]. The effective seed energy was estimated to be
3 Experimental setup
The experimental setup of the regenerative amplifier system is shown in Figure
For the amplifier, the gain medium was a 0.5 at.% doped Nd:GdVO4 crystal with dimensions 4 mm (
The RA cavity comprised a dichroic mirror M7, a quarter-wave plate (QWP), a thin-film polarizer (TFP), a Pockels cell (PC) based on BBO crystal with an aperture of 5 mm, and two highly reflective concave mirrors M5 (
Fig. 2. Schematic of the experimental setup: PP, pulse picker; TFP, thin-film polarizer; FR, Faraday rotator; HWP, half-wave plate; QWP, quarter-wave plate; PC, Pockels cell. The beam inside the RA cavity propagates along the 15 mm long $a$ -axis of the Nd:GdVO4 crystal.
4 Experimental results and discussions
Continuous wave (CW) operation was first conducted to confirm the optimum cavity performance, in which the combination of TFP2 and QWP served as the output coupler and the PC driver was switched off. Figure
In the RA operation regime, the seed with 800 nJ pulse energy was injected into the RA for amplification. Its output power is depicted in Figure
Fig. 4. (a) RA regime output power versus absorbed pump power; (b) the last five intracavity signals of the RA.
The temporal characteristics of the oscillator and RA output pulse were confirmed by an intensity autocorrelator. As shown in Figure
The long-term stability of the RA system at full pump power for 30 min is characterized and presented in Figure
Fig. 6. (a) Long-term power stability measurement of the RA output. (b) RA output beam quality.
5 Conclusion
In conclusion, we have demonstrated a 100 kHz high-power continuously pumped Nd:GdVO4 regenerative amplifier. The numerical analysis of the continuously pumped high-repetition-rate RA prior to the experiment facilitated optimization of the parameters in our experiment. This helped eliminate bifurcation instability and achieve efficient energy extraction. With a single bulk crystal, a maximum output pulse energy of
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Article Outline
Jie Guo, Wei Wang, Hua Lin, Xiaoyan Liang. High-repetition-rate and high-power picosecond regenerative amplifier based on a single bulk Nd:GdVO4 crystal[J]. High Power Laser Science and Engineering, 2019, 7(2): 02000e35.