Abstract:We investigate high-power terahertz (THz) generation in two-color laser filamentation using terawatt (TW) lasers including a 0.5 TW, 1 kHz system, as well as 2 and 30 TW systems both operating at 10 Hz. With these lasers, we study the macroscopic effect in filamentation that governs THz output energy yields and radiation profiles in the far field. We also characterize the radiation spectra at a broad range of frequencies covering radio-micro-waves to infrared frequencies. In particular, our 1 kHz THz source ca… Show more
“…This kind of density ripple can be created by different techniques (Hazra et al, 2004;Pai et al, 2005;Layer et al 2007;Liu et al, 2008). The laser propagates in the z-direction and polarized in the x-direction.…”
Section: Thz Radiation Generationmentioning
confidence: 99%
“…Experimental studies have also been done to generate intense THz pulses using two color laser filamentation using TW lasers. High-energy (>1 μJ), high average power (>1 mW), intensity (>1 MV cm −1 ), and broadband (0.01-60 THz) THz via two color filamentations have been reported (Oh et al, 2013). There are several techniques available for the study of self-focusing in the plasma.…”
The effect of self-focusing and defocusing on terahertz (THz) generation by amplitude-modulated Gaussian laser beam in rippled density plasma is investigated. A stronger transient transverse current is generated by transverse component of ponderomotive force exerted by laser on electrons that drives radiation at the modulation frequency (which is chosen to be in the THz domain) because of the variation in intensity in the direction transverse to the laser propagation. Numerical simulations indicate the enhancement of THz yield by many folds due to self-focusing of laser beam in comparison with that without self-focusing. The transient focusing of laser beam and its effect on the generated THz amplitude has also been studied.
“…This kind of density ripple can be created by different techniques (Hazra et al, 2004;Pai et al, 2005;Layer et al 2007;Liu et al, 2008). The laser propagates in the z-direction and polarized in the x-direction.…”
Section: Thz Radiation Generationmentioning
confidence: 99%
“…Experimental studies have also been done to generate intense THz pulses using two color laser filamentation using TW lasers. High-energy (>1 μJ), high average power (>1 mW), intensity (>1 MV cm −1 ), and broadband (0.01-60 THz) THz via two color filamentations have been reported (Oh et al, 2013). There are several techniques available for the study of self-focusing in the plasma.…”
The effect of self-focusing and defocusing on terahertz (THz) generation by amplitude-modulated Gaussian laser beam in rippled density plasma is investigated. A stronger transient transverse current is generated by transverse component of ponderomotive force exerted by laser on electrons that drives radiation at the modulation frequency (which is chosen to be in the THz domain) because of the variation in intensity in the direction transverse to the laser propagation. Numerical simulations indicate the enhancement of THz yield by many folds due to self-focusing of laser beam in comparison with that without self-focusing. The transient focusing of laser beam and its effect on the generated THz amplitude has also been studied.
“…Stimulated by such applications, the generation of intense THz pulses has recently been the subject of great interest, and several table-top techniques have been studied in detail1011. For example, optical rectification sources and THz generation from air plasma1213 have been the subject of many extensive efforts to scale up both THz peak electric field and energy10. THz pulses with more than 100 MV/cm peak electric field have been demonstrated by difference-frequency mixing of two parametrically amplified pulses14.…”
We demonstrate an intense broadband terahertz (THz) source based on the interaction of relativistic-intensity femtosecond lasers with aligned copper nanorod array targets. For copper nanorod targets with a length of 5 μm, a maximum 13.8 times enhancement in the THz pulse energy (in ≤20 THz spectral range) is measured as compared to that with a thick plane copper target under the same laser conditions. A further increase in the nanorod length leads to a decrease in the THz pulse energy at medium frequencies (≤20 THz) and increase of the electromagnetic pulse energy in the high-frequency range (from 20–200 THz). For the latter, we measure a maximum energy enhancement of 28 times for the nanorod targets with a length of 60 μm. Particle-in-cell simulations reveal that THz pulses are mostly generated by coherent transition radiation of laser produced hot electrons, which are efficiently enhanced with the use of nanorod targets. Good agreement is found between the simulation and experimental results.
“…Conventional THz sources were usually achieved by semiconductor photoconductive switches [11,12] or optical rectification in nonlinear crystals [13], while the THz field intensity by the two schemes is relatively low and its spectral range is narrow. Recently, as an alternative approach, two-color laser field has been proposed to generate the intense and broadband THz pulse [14][15][16]. In this two-color scheme, a fundamental femtosecond laser field combining with its second harmonic field are focused in air to generate gaseous plasma, and an intense THz pulse can be irradiated in the forward direction.…”
We theoretically demonstrate the effect of intensity ratio of the two-color laser field on the terahertz generation based on a transient photocurrent model. We show that the terahertz generation depends on the intensity ratio of the two-color laser field at a given total laser intensity, and the optimal intensity ratio for the maximum terahertz generation will decrease with the increase of the total laser intensity. We also show that the final ionization degree can be used to explain the optimal intensity ratio change at different laser intensities. Furthermore, we utilize the increasing rate of electron density and the electron drift velocity to illustrate the physical mechanism of the maximum terahertz radiation generation.
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