Abstract

Recently we have demonstrated a new nonlinear optical effect in the THz interval of frequencies. The latter is based on the use of femtosecond optical pulses and intense, sub-ps, broadband terahertz (THz) pulses to generate a THz-optical four- and five-wave mixing in the investigated material. The spectrum of the generated signal is resolved in time and wavelength and displays two pronounced frequency sidebands, Stokes and anti-Stokes, close to the optical second harmonic central frequency 2, where is the optical central frequency of the fundamental beam, thus resembling the spectrum of standard hyper-Raman scattering, and hence we named this effect ‘THz hyper-Raman’—THYR. We applied this technique to several crystalline materials, including α-quartz and gallium selenide. In the first material, we find that the THYR technique brings spectroscopic information on a large variety of low-energy excitations that include polaritons and phonons far from the Γ-point, which are difficult to study with standard optical techniques. In the second example, we show that this new tool offers some advantages in detecting ultra-broadband THz pulses. In this paper we review these two recent results, showing the potentialities of this new THz technique.

Highlights

  • The Terahertz electromagnetic spectrum ranges in the frequency window from ~100 GHz to~30 THz, i.e., in between the microwave and the far-infrared domains

  • In the absence of resonances, the THz hyper-Raman (THYR) 3D-spectrum may be used under some circumstances for a phase-sensitive detection of the THz optical field, as we have demonstrated in crystalline GaSe [17]

  • In this paper we reviewed our recent results on a new nonlinear optical effect in the THz interval of frequencies, which we

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Summary

Introduction

The Terahertz electromagnetic spectrum ranges in the frequency window from ~100 GHz to. A great progress for the detection of THz pulses has been achieved by the introduction of the so-called electro-optic sampling (EOS) technique, which uses part of the laser pulse generating the THz field to sample the latter This advancement has led to the development of the so-called THz time-domain spectroscopy (THz-TDS) [1]. We have demonstrated a new nonlinear optical effect in crystalline quartz (α-SiO2 ) that we have named THz hyper-Raman (THYR) [16] It makes use of femtosecond infrared (IR) pulses and intense, sub-ps, broadband THz pulses to generate a four- and five-wave-mixing (FFWM) in the investigated material. When material resonances lie in the THz band of the THYR signal these show up in the THYR 3D-spectrum as temporal oscillations The latter may be solved in the frequency domain by applying a numerical fast Fourier transform (FFT). For a comprehensive review on the latter we remind to Ref. [10]

Theory
Semiclassical Model of THYR SPECTROSCOPY χ
Materials and Methods
Discussion
Application of THYR for the Detection of THz Pulses
Application of named
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