Z. Nie, Yipeng Wu, Chaojie Zhang, W. Mori, C. Joshi, W. Lu, C. Pai, J. Hua, Jyhpyng Wang
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We show that sub-joule, terawatts, single-cycle terahertz (2-12 THz, or 150-25 $\\mu$m) pulses can be generated by replacing the drive laser with a picosecond 10 $\\mu$m CO$_2$ laser and a different shaped plasma structure. The second plasma technique employs frequency upshifting by colliding a CO$_2$ laser with a rather sharp relativistic ionization front created by ionization of a gas in less than half cycle (17 fs) of the CO$_2$ laser. Even though the electrons in the ionization front carry no energy, the frequency of the CO$_2$ laser can be upshifted due to the relativistic Doppler effect as the CO$_2$ laser pulse enters the front. The wavelength can be tuned from 1-10 $\\mu$m by simply changing the electron density of the front. While the upshifted light with $5 <\\lambda(\\mu$m$)< 10$ propagates in the forward direction, that with $1 <\\lambda(\\mu$m$)< 5$ is back-reflected. 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The first plasma technique utilizes frequency downshifting of the drive laser pulse in a nonlinear plasma wake. Based on this technique, we have proposed and demonstrated that in a tailored plasma structure multi-millijoule energy, single-cycle, long-wavelength IR (3-20 $\\\\mu$m) pulses can be generated by using an 810 nm Ti:sapphire drive laser. Here we extend this idea to the THz frequency regime. We show that sub-joule, terawatts, single-cycle terahertz (2-12 THz, or 150-25 $\\\\mu$m) pulses can be generated by replacing the drive laser with a picosecond 10 $\\\\mu$m CO$_2$ laser and a different shaped plasma structure. The second plasma technique employs frequency upshifting by colliding a CO$_2$ laser with a rather sharp relativistic ionization front created by ionization of a gas in less than half cycle (17 fs) of the CO$_2$ laser. Even though the electrons in the ionization front carry no energy, the frequency of the CO$_2$ laser can be upshifted due to the relativistic Doppler effect as the CO$_2$ laser pulse enters the front. The wavelength can be tuned from 1-10 $\\\\mu$m by simply changing the electron density of the front. While the upshifted light with $5 <\\\\lambda(\\\\mu$m$)< 10$ propagates in the forward direction, that with $1 <\\\\lambda(\\\\mu$m$)< 5$ is back-reflected. 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引用次数: 4
摘要
本文讨论了10 $\mu$ m红外激光器在$\lambda$ =1-150 $\mu$ m ($\nu$ =300-2太赫兹)的整个波长(频率)范围内,采用两种不同的等离子体技术实现频率降移和升移的数值和实验结果。第一种等离子体技术是利用非线性等离子体尾迹中驱动激光脉冲的降频。基于该技术,我们提出并证明了在定制等离子体结构中,使用810 nm Ti:蓝宝石驱动激光器可以产生多毫焦耳能量,单周期,长波红外(3-20 $\mu$ m)脉冲。这里我们将这个想法扩展到太赫兹频率范围。我们展示了亚焦耳,太瓦,单周期太赫兹(2-12太赫兹,或150-25 $\mu$ m)脉冲可以通过用皮秒10 $\mu$ m CO $_2$激光器和不同形状的等离子体结构代替驱动激光器产生。第二种等离子体技术通过CO $_2$激光与CO $_2$激光在不到半周期(17 fs)的时间内电离气体产生的相当尖锐的相对论性电离锋相碰撞,利用频率上移。尽管电离前沿的电子不携带能量,但当CO $_2$激光脉冲进入电离前沿时,由于相对论多普勒效应,CO $_2$激光的频率可以上移。波长可以从1-10 $\mu$ m通过简单地改变前面的电子密度。当含有$5 <\lambda(\mu$ m $)< 10$的上移光向前传播时,含有$1 <\lambda(\mu$ m $)< 5$的上移光向后反射。这两种等离子体技术似乎非常有希望覆盖整个分子指纹区域。
Ultra-short pulse generation from mid-IR to THz range using plasma wakes and relativistic ionization fronts
This paper discusses numerical and experimental results on frequency downshifting and upshifting of a 10 $\mu$m infrared laser to cover the entire wavelength (frequency) range from $\lambda$=1-150 $\mu$m ($\nu$=300-2 THz) using two different plasma techniques. The first plasma technique utilizes frequency downshifting of the drive laser pulse in a nonlinear plasma wake. Based on this technique, we have proposed and demonstrated that in a tailored plasma structure multi-millijoule energy, single-cycle, long-wavelength IR (3-20 $\mu$m) pulses can be generated by using an 810 nm Ti:sapphire drive laser. Here we extend this idea to the THz frequency regime. We show that sub-joule, terawatts, single-cycle terahertz (2-12 THz, or 150-25 $\mu$m) pulses can be generated by replacing the drive laser with a picosecond 10 $\mu$m CO$_2$ laser and a different shaped plasma structure. The second plasma technique employs frequency upshifting by colliding a CO$_2$ laser with a rather sharp relativistic ionization front created by ionization of a gas in less than half cycle (17 fs) of the CO$_2$ laser. Even though the electrons in the ionization front carry no energy, the frequency of the CO$_2$ laser can be upshifted due to the relativistic Doppler effect as the CO$_2$ laser pulse enters the front. The wavelength can be tuned from 1-10 $\mu$m by simply changing the electron density of the front. While the upshifted light with $5 <\lambda(\mu$m$)< 10$ propagates in the forward direction, that with $1 <\lambda(\mu$m$)< 5$ is back-reflected. These two plasma techniques seem extremely promising for covering the entire molecular fingerprint region.