Author Affiliations
Abstract
1 Shenzhen University, College of Physics and Optoelectronic Engineering, Shenzhen Key Lab of Micro-Nano Photonic Information Technology, Shenzhen, China
2 Shenzhen University, College of Electronic Information Engineering, Shenzhen, China
3 Institut National de la Recherche Scientifique, Centre Énergie Matériaux Télécommunications, Laboratory of Applied Computational Imaging, Varennes, Québec, Canada
We report a framing imaging based on noncollinear optical parametric amplification (NCOPA), named FINCOPA, which applies NCOPA for the first time to single-shot ultrafast optical imaging. In an experiment targeting a laser-induced air plasma grating, FINCOPA achieved 50 fs-resolved optical imaging with a spatial resolution of ~83 lp / mm and an effective frame rate of 10 trillion frames per second (Tfps). It has also successfully visualized an ultrafast rotating optical field with an effective frame rate of 15 Tfps. FINCOPA has simultaneously a femtosecond-level temporal resolution and frame interval and a micrometer-level spatial resolution. Combining outstanding spatial and temporal resolutions with an ultrahigh frame rate, FINCOPA will contribute to high-spatiotemporal resolution observations of ultrafast transient events, such as atomic or molecular dynamics in photonic materials, plasma physics, and laser inertial-confinement fusion.
ultrafast imaging spatiotemporal resolution frame rate noncollinear optical parametric amplification 
Advanced Photonics
2020, 2(5): 056002
Author Affiliations
Abstract
1 Shenzhen Key Laboratory of Micro-Nano Photonic Information Technology, College of Physics and Optoelectronics Engineering, Shenzhen University, Shenzhen518060, China
2 College of Electronic and Information Engineering, Shenzhen University, Shenzhen518060, China
A tunable ultrafast intensity-rotating optical field is generated by overlapping a pair of 20 Hz, 800 nm chirped pulses with a Michelson interferometer (MI). Its rotating rate can be up to 10 trillion radians per second ($\text{Trad}/\text{s}$), which can be flexibly tuned with a mirror in the MI. Besides, its fold rotational symmetry structure is also changeable by controlling the difference from the topological charges of the pulse pair. Experimentally, we have successfully developed a two-petal lattice with a tunable rotating speed from $3.9~\text{Trad}/\text{s}$ up to $11.9~\text{Trad}/\text{s}$, which is confirmed by our single-shot ultrafast frame imager based on noncollinear optical-parametric amplification with its highest frame rate of 15 trillion frames per second (Tfps). This work is carried out at a low repetition rate. Therefore, it can be applied at relativistic, even ultrarelativistic, intensities, which usually operate in low repetition rate ultrashort and ultraintense laser systems. We believe that it may have application in laser-plasma-based accelerators, strong terahertz radiations and celestial phenomena.
noncollinear optical-parametric amplification rotating rate ultrafast frame imager ultrafast intensity-rotating optical field 
High Power Laser Science and Engineering
2020, 8(1): 010000e3
Author Affiliations
Abstract
1 Key Lab of Optoelectronic Devices and Systems of Ministry of Education/Guangdong Province, College of Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, China
2 College of Information Engineering, Shenzhen University, Shenzhen 518060, China
We provide the first demonstration of pure red emission in the visible light region via three-photon excitation in monodisperse Na3ZrF7:Er nanoparticles (NPs) by using a laser operating in the telecommunication band. NPs of 22 nm in diameter are synthesized at 260°C by the thermal decomposition method. The experimental results reveal that the Na3ZrF7:Er NPs exhibit pure red emission in the visible region under 1480 nm laser excitation, and the emission intensity is significantly influenced by the Er3+ ion concentration. The decay times of the S3/24F415/2 and F9/24F415/2 transitions of the Er3+ ions at 540 and 655 nm, respectively, are reduced by increasing the Er3+ ion concentration in the 160.2540 Fluorescent and luminescent materials 160.4760 Optical properties 
Chinese Optics Letters
2017, 15(1): 011601
作者单位
摘要
1 深圳大学 光电子器件与系统(教育部/广东省)重点实验室, 广东 深圳518060
2 深圳大学 信息工程学院, 广东 深圳518060
3 深圳大学 物理科学与技术学院, 广东 深圳 518060
研制了基于电子束时间展宽技术和微通道板(microchannel plate, MCP)选通技术的时间展宽分幅相机。相机有三条厚度80 nm、宽度8 mm的微带阴极, 阴极上加载斜率为2.1 V/ps的高压斜坡脉冲, 使得先发射的电子较后面的电子速度快, 经过50 cm的漂移区后, 电子束产生时间展宽, 从而提高相机时间分辨率。阴极和MCP均加载了脉冲电压, 因此, 需要精确同步光脉冲、阴极脉冲和MCP选通脉冲, 分析了完整的同步过程。当阴极仅加直流电压, 无电子束时间展宽时, 获得相机的时间分辨率为78 ps。当阴极加载高压斜坡脉冲时, 电子束时间展宽技术将系统的时间分辨率提高至12 ps。改变延时, 将光脉冲分别同步在斜坡脉冲不同位置, 获得了时间分辨率与同步位置的关系。
分幅相机 时间展宽 时间分辨率 惯性约束聚变 Z箍缩 framing camera time dilation temporal resolution inertial confinement fusion Z-pinch 
红外与激光工程
2016, 45(12): 1206001
作者单位
摘要
1 深圳大学光电子器件与系统(教育部/广东省)重点实验室,广东 深圳 518060
2 深圳大学信息工程学院,广东 深圳 518060
3 深圳大学物理科学与技术学院,广东 深圳 518060
研制了无增益微通道板(Microchannel plate, MCP)选通X射线分幅相机,由无增益MCP变像管、成像针孔阵列、皮秒选通脉冲发生器及CCD构成。对相机时间分辨率进行了测量,当无增益MCP加载-1.5 kV、145 ps的选通脉冲和-300 V的直流偏置时,测得相机的时间分辨率为59 ps。改变MCP直流偏置电压,获得了时间分辨率、输出信号强度与MCP偏置电压的关系。实验结果表明,随着MCP偏置电压的减小,时间分辨率提高,但输出信号强度降低。
X射线光学 分幅相机 无增益微通道板 时间分辨率 惯性约束聚变 X-ray optics framing camera non-gain microchannel plate temporal resolution inertial confinement fusion 
红外与激光工程
2015, 44(S): 0109
作者单位
摘要
1 深圳大学光电子器件与系统教育部重点实验室, 广东 深圳 518060
2 西安交通大学电力设备电气绝缘国家重点实验室, 陕西 西安 710049
3 西北电网有限公司, 陕西 西安 710048
4 深圳大学信息工程学院, 广东 深圳 518060
研制了电子束时间聚焦和时间准直系统,由时间聚焦器、时间准直器、条纹变像管、脉冲发生器和CCD 等组成。测量了系统对电子束的时间压缩比,当聚焦脉冲斜率为800 mV/ps 时,测得系统的时间压缩比为3.4∶1。研究了时间压缩比与聚焦脉冲斜率的关系,实验结果表明时间压缩比随着聚焦脉冲斜率的增大而提高。
X射线光学 条纹相机 时间聚焦 时间准直 时间分辨率 
激光与光电子学进展
2015, 52(10): 100401
赵鑫 1,2,3,4,*蔡厚智 1,2刘进元 1谢维信 2
作者单位
摘要
1 深圳大学光电子器件与系统教育部重点实验室, 广东 深圳 518060
2 深圳大学信息工程学院,广东 深圳 518060
3 西安交通大学电力设备电气绝缘国家重点实验室,陕西 西安 710049
4 西北电网有限公司,陕西 西安 710048
为了补偿条纹变像管阴极和栅极之间的电子渡越时间弥散,提出了电子束时间聚焦和时间准直系统。系统中,时间聚焦器用来压缩补偿电子束团在加速过程中产生的时间宽度展宽,压缩补偿后的电子束团再通过时间准直器,时间准直器用来使输出的电子具有相同的能量,这样电子束团在后面的传输过程中就不会产生新的时间弥散。采用蒙特卡罗方法和有限差分法对系统进行了理论模拟。模拟结果表明,500 fs的电子脉冲经过时间聚焦器作用后,时间宽度变为131 fs,时间压缩比为3.8:1,此后由于时间准直器的作用,电子脉冲宽度保持在131 fs左右,时间准直性为16.8%。
X射线光学 条纹相机 时间聚焦 时间准直 时间分辨率 
中国激光
2015, 42(s1): s117001

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