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飞秒激光激发非线性材料是目前太赫兹的关键产生技术之一. 它由于具有超快时间分辨、超宽频谱分布等优点, 已广泛应用于太赫兹表征与测量、感知与成像等方面. 然而通过微结构等对太赫兹波的调控方法只能对太赫兹传输过程进行调控, 且面临设计困难, 工艺复杂等障碍, 难以在产业上广泛应用. 本文通过引入脉冲整形系统改变飞秒激光脉冲的时间色散, 可以直接调控飞秒激光与铌酸锂晶体的相互作用过程, 从而对太赫兹产生过程进行直接调控. 同时, 本文利用冲击受激拉曼散射模型与黄昆方程, 对太赫兹波的产生过程进行仿真模拟, 证明了利用飞秒激光脉冲时间色散调控太赫兹波的可行性. 这一结果对于未来基于铌酸锂晶体的片上太赫兹源主动调控具有重要的借鉴意义.Femtosecond laser excitation of nonlinear materials is one of the key technologies for generating terahertz waves at present. Due to its advantages such as ultrashort time resolution and ultrabroad frequency spectrum, the technology has been widely used to characterize, measure, sense and image terahertz waves. However, the methods of controlling terahertz waves through microstructures can only regulate their transmission process, but they will face obstacles such as design difficulty and complex processes, making it hard to be widely used in industry. In this work, by introducing a pulse-shaping system to change the time dispersion of femtosecond laser pulses, the interaction process between femtosecond laser and lithium niobate crystals can be directly regulated, therefore the terahertz generation process can be directly controlled. Taking the second-order time dispersion for example, the terahertz signals generated by pump light with different second-order time dispersion in lithium niobate is detected by using the pump-probe phase-contrast imaging system. Meanwhile, the generation process of terahertz waves is simulated using the impact stimulated Raman scattering model and Huang-Kun equation, demonstrating the feasibility of using femtosecond laser pulses to adjust the time dispersion of terahertz waves. The experimental and simulation results show that when the time dispersion of femtosecond laser causes the pulse width to increase, the time in which the lithium niobate lattice is subjected to the impact stimulated Raman scattering force is prolonged, and the macroscopic polarization of the lithium niobate lattice is correspondingly extended. On the one hand, the longer duration of polarization results in a wider terahertz signal in the time domain and a narrower one in the frequency domain. On the other hand, since the impact stimulated Raman scattering force is proportional to the pump light intensity and is in the same direction during the interaction time, when the Raman scattering force ends, the lattice reaches a maximum displacement. The longer Raman scattering force causes the lattice to move to one side for a longer time, and correspondingly, the subsequent vibration of one period takes a longer time, ultimately resulting in a lower center frequency. In addition, this work also points out that the modulation of terahertz signals by pump light pulse width may be affected by the thickness of the wafer, and the modulation effect on thinner media may be more obvious. This result is of great reference significance for the active regulation of on-chip terahertz sources based on lithium niobate crystals in the future.
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Keywords:
- temporal dispersion /
- terahertz generation /
- on-chip integration
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图 1 实验系统构成: (a) 泵浦探测光路; (b) 模拟中不同群时延色散的泵浦光的强度变化; (c) 实验中不同群时延色散的泵浦光的强度变化
Fig. 1. Composition of the experimental system: (a) Pump-probe optical path; (b) Intensity variation of pump light with different group delay dispersion in the simulation; (c) Intensity variation of pump light with different group delay dispersion in the experiment.
图 2 泵浦光功率一致时的时域信号: (a)—(c) 实验中不同色散泵浦光产生的THz信号及其相对峰值强度变化; (d)—(f) 模拟中不同色散泵浦光产生的THz信号及其相对峰值强度变化
Fig. 2. Time domain signal when the pump light power is consistent: (a)–(c) THz signals generated by different dispersion pump lights and their relative peak intensity changes in the experiment; (d)–(f) THz signals generated by pump lights with different dispersions and their relative peak intensity changes in the simulation.
图 3 泵浦光功率一致时的频域信号: (a), (b) 实验中不同色散泵浦光产生的THz信号; (c), (d) 模拟中不同色散泵浦光产生的THz信号
Fig. 3. Frequency domain signal when the pump light power is consistent: (a), (b) THz signals generated by pump lights with different dispersion in the experiment; (c), (d) THz signals generated by pump lights with different dispersion in the simulation.
图 4 高斯脉冲模拟泵浦产生THz波: (a)—(c)脉宽相同、峰值强度不同的泵浦光及其产生的THz信号; (d)—(f) 脉宽不同、峰值强度相同的泵浦光及其产生的THz信号
Fig. 4. Gaussian pulse simulates pumping to generate THz waves: (a)–(c) THz signals generated by pump lights with the same pulse width but different intensities; (d)–(f) THz signals generated by pump lights with different pulse widths but the same intensity
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