Related Experiment Video
Updated: Mar 6, 2026

10:17
20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
Published on: July 12, 2017
12.1K
Active pulse shaping for end-pumped Nd:YVO4 amplifier with high gain.
Optics Letters
|March 16, 2017
Summary
We achieved active pulse shaping in a solid-state neodymium-doped yttrium orthovanadate (Nd:YVO4) amplifier, generating various pulse shapes including a flat square pulse with low amplitude variation. This method shows potential for designing high-peak-power lasers with tailored pulse characteristics.
Area of Science:
- Laser Physics and Engineering
- Nonlinear Optics
- Materials Science
Background:
- Solid-state lasers are crucial for various scientific and industrial applications.
- Controlling laser pulse shapes is essential for optimizing performance in areas like high-intensity physics and material processing.
- Neodymium-doped yttrium orthovanadate (Nd:YVO4) is a widely used gain medium for lasers.
Purpose of the Study:
- To demonstrate active pulse shaping for a solid-state Nd:YVO4 amplifier.
- To generate a variety of useful laser pulse shapes, including a highly stable square pulse.
- To propose a numerical method for designing active pulse shaping without experimental testing.
Main Methods:
- Active shaping techniques were applied to a solid-state Nd:YVO4 amplifier.
- A numerical method was developed and proposed for simulating and designing the pulse shaping process.
- Characterization of output pulse shapes and amplitude stability was performed.
Main Results:
- Achieved a high average gain of 39.2 dB.
- Generated an average output power of 8.3 W from an input power of 1 mW.
- Successfully produced a range of pulse shapes, including a very flat square pulse with root-mean-square amplitude variation below 3%.
Conclusions:
- Active pulse shaping is effectively demonstrated in a solid-state Nd:YVO4 amplifier.
- The proposed numerical method facilitates the design of lasers with desired pulse shapes and high peak power (>100 kW).
- This work paves the way for advanced laser system design with precise temporal control.
Related Concept Videos
MOSFET Amplifiers
602
The MOSFET, when operating in its active region, functions as a voltage-controlled current source. In this region, the gate-to-source voltage controls the drain current. This principle underlies the operation of the transconductance MOSFET amplifier. The output current is directed through a load resistor to convert this amplifier into a voltage amplifier. The output voltage is then obtained by subtracting the voltage drop across the load resistance from the supply voltage. This process results...
602
Biasing of FET
805
Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
805
Maximum Power Transfer
1.0K
Numerous practical applications within engineering disciplines, such as telecommunications, necessitate optimizing power delivery to a connected load. This pursuit, however, entails inherent internal losses, which can either equal or exceed the power supplied to the load. The Thevenin equivalent circuit is helpful in finding the maximum power a linear circuit can deliver to a load. It is assumed in this context that the load resistance can be adjusted.
By substituting the entire circuit with...
By substituting the entire circuit with...
1.0K
Cascaded Op Amps
1.2K
Operational amplifiers (op-amps) are versatile electronic components that can be interconnected in a cascade - one after another in a linear sequence. This cascading is possible due to their infinite input resistance and zero output resistance, allowing them to maintain their input-output relationships even when connected in series.
In a cascaded system, each op-amp is referred to as a stage. The output of one stage drives the input of the subsequent stage. As the input signal passes through...
In a cascaded system, each op-amp is referred to as a stage. The output of one stage drives the input of the subsequent stage. As the input signal passes through...
1.2K
BJT Amplifiers
1.1K
Bipolar Junction Transistors (BJTs) are pivotal components in amplifier circuits, functioning as voltage-controlled current sources in their active region. This characteristic allows them to efficiently control the collector current through variations in the base-emitter voltage. Essentially, BJTs amplify power due to their ability to take a weak input signal and output a much stronger signal.
In BJT amplifier configurations, particularly in common-emitter setups, the transistor's role...
In BJT amplifier configurations, particularly in common-emitter setups, the transistor's role...
1.1K
Biasing of P-N Junction
2.3K
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
2.3K

