相关实验视频
Updated: Sep 11, 2025

10:17
20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
Published on: July 12, 2017
11.6K
概括
我们开发了一种稳定,高效率的二极管送的合和正 (Nd:YVO4) 激光器. 这款紧型激光器实现了7.5W的平均输出功率和48.1%的光对光效率,证明了其实际潜力.
科学领域:
- 激光物理 激光物理
- 固态激光器 固态激光器
- 光电学是指光电子产品.
背景情况:
- 用二极管的固态激光器在效率和紧性方面具有优势.
- 模式锁定激光器对于需要高峰功率脉冲的应用至关重要.
研究的目的:
- 为了开发一个高效率,紧,稳定的二极管末端 SESAM 模式锁定 Nd:YVO4 激光.
- 分析腔镜曲率对模式锁定稳定性的影响.
- 从理论上建模并抑制更高阶波模式锁定.
主要方法:
- 使用半导体和吸收镜 (SESAM) 进行模式锁定.
- 采用多通道腔设计,以保持紧性和效率.
- 开发了一个基于速率方程的理论模型来分析多重脉冲现象.
主要成果:
- 在20.53MHz的重复率下实现了接近衍射限制的模式锁定脉冲.
- 获得了7.5W的平均输出功率,脉冲持续时间为28.8 ps,峰值功率为12.7 kW.
- 达到了48.1%的光对光效率和58.6%的斜率效率.
- 识别并理论上抑制了更高阶波模式锁定.
结论:
- 开发的Nd:YVO4激光器具有高效,紧和稳定的性能.
- 腔镜曲率显著影响模式锁定稳定性.
- 该理论模型准确地预测并提供模式锁定问题的解决方案.
相关概念视频
Oscillations In An LC Circuit
2.5K
An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
2.5K
RLC Circuit as a Damped Oscillator
1.3K
An RLC circuit combines a resistor, inductor, and capacitor, connected in a series or parallel combination.
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
1.3K
Parallel Resonance
274
The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
274
Design Example: Underdamped Parallel RLC Circuit
377
Consider designing an oscillator circuit, a crucial component in various electronic devices and systems. The objective is to create an oscillator circuit with specific characteristics: a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. To accomplish this, a parallel RLC circuit is employed, known for its ability to sustain oscillations at a resonant frequency. In this case, the damping factor is pivotal in achieving the desired performance.
Starting with a fixed...
Starting with a fixed...
377
Double Resonance Techniques: Overview
293
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
293
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences
917
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
917

