Tunable terahertz waves from 4-dimethylamino-N′-methyl-4′-stibazolium tosylate pumped with dual-wavelength injection-seeded optical parametric generation

We developed a widely tunable terahertz (THz)-wave source covering the sub-THz frequency by difference frequency generation using a 4-dimethylamino-N′-methyl-4′-stibazolium tosylate (DAST) crystal. Near-infrared waves generated by dual-wavelength injection-seeded β-BaB2O4 optical parametric generation (is-BBO-OPG) were used for pumping the DAST crystal, which had separated wavelengths in the spectrum with a difference frequency of sub-THz. Furthermore, the non-collinear phase-matching condition was designed to compensate the walk-off effect of the BBO crystal. Consequently, tunable THz-waves from 0.3 to 4 THz were generated by tuning the wavelength of one of the seeding beams. The generated sub-THz-waves were monochromatic (dν < 33 GHz) with a maximum energy of 80 pJ at 0.65 THz.

S ub-terahertz (sub-THz) frequencies exist between the frequency of 1 THz and millimeter waves. In this frequency region, electromagnetic waves have high transparency to materials such as bio-materials because of less absorption than that above the 1 THz region. Also the waves of this frequency have higher directivity in propagation owing to the wavelength being shorter than that of microwaves. These benefits have attracted great interest for applications such as nondestructive imaging [1][2][3] and remote sensing of the atmosphere. 4) For sub-THz-wave-source development, both electronics and photonics technologies are useful. In electronics, high-electron-mobility transistors (HEMTs) 5) and resonant-tunneling diodes (RTDs) 6) have been developed to have fundamental oscillation reaching sub-THz and higher frequencies. In photonics, nonlinear optical wavelength conversion [7][8][9][10][11][12][13][14][15][16][17] and the quantum cascade structure in semiconductor lasers have been explored in the midinfrared region down to the frequencies of around 1 THz. 18) Among these sources, there is no tunable source operating in the sub-THz frequency range with high output power. Nonlinear optical wavelength conversion is an attractive way to develop a sub-THz-wave source because of its benefits of wide tunability, room-temperature operation, and high conversion efficiency. Such a THz-wave source will realize seamless frequency-tuning between sub-THz and 10 THz order, which will be beneficial to applications.
Over the past years, we have developed tunable THz-wave sources by optical parametric generation (OPG) 7,8) and difference frequency generation (DFG). [9][10][11] In particular, using DFG in organic nonlinear optical crystals, an ultrawidely tunable THz-wave source of 1-30 THz has been demonstrated. 11) The tunability of that source was attributable to the wide acceptance of phase-matching of the nonlinear crystals and the wide tunability of the dual-wavelength optical parametric oscillator (dual-wavelength OPO) as a near-infrared (NIR) pump source. In previous methods, however, the lowest generated THz-wave frequency was limited to approximately 1 THz, because it was difficult to prepare two NIR waves at approximately 1300 nm with a small wavelength difference of less than 6 nm for sub-THz-wave generation. In the case of the dual-wavelength OPO, this limitation was attributable to a wide tolerance in the oscillation spectrum by the cavity mode and the high gain of the nonlinear crystal. Consequently, the dual-wavelength OPO is inappropriate as a pump source for sub-THz-wave generation.
In this paper, we proposed a 1300 nm injection-seeded β-BaB 2 O 4 -OPG (is-BBO-OPG) without a cavity structure to generate spectrally separated wavelengths with difference frequency down to the sub-THz range. Moreover, to improve the conversion efficiency of is-BBO-OPG, an efficient walkoff compensation in the BBO crystal was designed and demonstrated. Using this is-BBO-OPG as a dual-wavelength pump source for 4-dimethylamino-N A-methyl-4A-stibazolium tosylate (DAST)-DFG, we demonstrated widely tunable THz-wave generation from 0.3 to 4 THz. A wide phasematching condition as a function of frequency in the BBO and DAST crystals enabled tunability to be controlled merely by tuning the wavelength in one of the injection-seeding beams. Thus, frequency agility was accomplished with no mechanical motion or temperature control of the crystal. Furthermore, the output of is-BBO-OPG had additional peaks in the spectrum, that are expected to induce cascade DFG for highly efficient THz-wave generation, as reported in a previous paper. 17) The present source has potential to extend the tunability to tens of THz by improving the tuning range of injection-seeding beams.
An organic nonlinear optical crystal of DAST has low dispersion of the refractive index from the THz to NIR frequencies, which provides various collinear phase-matching conditions. Additionally, it has a high nonlinear coefficient (1010 pm=V at 1300 nm), 19) which yields a high conversion efficiency of DFG. Consequently, the DFG configuration is suitable for tunable and efficient THz-wave generation. As a pumping source for DAST-DFG, dual-wavelength sources with wavelengths of approximately 1300 nm are necessary to satisfy the optimal phase-matching condition. 9,12,19) To generate a tunable dual-wavelength output at around 1300 nm, we applied a BBO crystal. A BBO crystal is generally used because of its wide tunability and high nonlinear conversion efficiency. 20) We applied a type-I phase-matching condition because the effective nonlinear coefficient is larger than that under the type-II phase-matching condition. With 532-nm-wave pumping, an idler wave of 1300-1400 nm is generated, with the cogeneration of a signal wave at around 900 nm. Figures 1(a) and 1(b) depict two types of phasematching conditions: non-collinear and collinear phasematching in the BBO crystal, respectively. The vectors k p , k i , and k s respectively signify the wave vectors of the pump, idler, and signal beams. S p and S i respectively represent the Poynting vectors of the pump and idler beams. α, β, and γ respectively denote the angles of the pump, idler, and signal beams measured from the c-axis under the phase-matching condition. In collinear phase-matching, the wave vectors of all three beams are parallel but the Poynting vectors are not parallel. Because of the birefringence, the Poynting vector of the pump beam with extraordinary polarization (e-polarization) is not parallel to that of the idler beam with ordinary polarization (o-polarization). The degree of overlap of the two beams decreases with propagation. Thereby, the optical parametric gain decreases even if phase-matching is satisfied. Here, the polarization of the signal beam is ordinary. To achieve better overlap between the pump beam and idler beam, the non-collinear phase-matching configuration is applicable. Non-collinear phase-matching is effective for increasing the degree of overlap between these beams by compensating the walk-off effect. 21) As shown in Fig. 1(a), the design of non-collinear phase-matching in our is-OPG is depicted for parallel Poynting vectors of the pump and idler beams. In this configuration, the walk-off angle ( ρ) and the tilt angle of the idler from the pump beam ( β − α) are equal, which allows parallel overlap. For this configuration, the following two equations must be satisfied.
In these equations, λ i , λ s , and λ p respectively denote the idler, signal, and pump beam wavelengths, where 1=λ i + 1=λ s = 1=λ p . Also, n o and n e are the refractive indices of the BBO crystal in an ordinary wave and an extraordinary wave, respectively. Angles α, β, and γ are portrayed in Figs. 1(a) and 1(b).
Equation (1) represents non-collinear phase-matching in Type-I BBO. Equation (2) represents the parallel propagation of pump and idler beams owing to the walk-off effect. Using experimental values, 22) the solutions for α, β, and γ are listed in Table I for the pump and idler beam wavelengths of 532 and 1330 nm, respectively. The values for collinear phase-matching are also listed in Table I for comparison. In collinear phase-matching, the deviation angle of the Poynting vector of the pump beam from that of the idler beam (α + ρ) − β is 3.2°, but it is zero in non-collinear phase-matching. The calculated results showed that parallel propagation of the pump and idler beams is possible in BBO-OPG owing to the non-collinear phase-matching configuration. Figures 1(c) and 1(d) depict calculated tuning curves of non-collinear phase-matching satisfying Eqs. (1) and (2), where the pump and idler beams propagate in parallel. The results indicate that a wide tuning range (δλ = 50 nm) is possible with a fixed pump angle because the difference in the phase-matching angle is within 0.16°in the tuning range; this value is less than the divergence angle of the pump beam. The corresponding tuning range of the maximum difference frequency is approximately 8 THz.
The tuning curve of collinear phase-matching is also depicted in Figs. 1(c) and 1(d) for comparison. Figure 2 presents the overall experimental setup comprising a Nd:YAG µ-chip laser master oscillator and power amplifier (MOPA) system with a second-harmonic (SH) generation system, an is-BBO-OPG, and a THz-wave-generation part based on DAST-DFG. In the is-BBO-OPG, a BBO crystal was used: θ = 22.6°; ϕ = 0°; dimensions of 5 × 5 × 10 mm 3 . Both surfaces of the BBO crystal were antireflectioncoated for wavelengths in the 1300 nm (idler) region. The reflection of 532 nm (pump) and 900 nm (signal) waves is about 3%. The original pump beam was the output from the µ-chip laser (wavelength, 1064 nm; frequency linewidth < 3 GHz) with about 0.4 mJ=pulse, which is less energy for the latter optical system. Then, the laser output was increased by the MOPA, and an output energy of 30 mJ=pulse, pulse duration of 600 ps, and repetition rate of 30 Hz were achieved. To excite OPG, the pump beam was converted to an SH beam (532 nm) by an LBO crystal (θ = 90°, ϕ = 11.4°, 3 × 3 × 15 mm 3 ). Eventually, the maximum output energy of the SH beam became 11 mJ=pulse. The SH beam was loosely focused into the BBO crystal through a planoconvex lens with a  600 mm focal length. The power intensity at the crystal was 4.8 GW=cm 2 . The incident angle of the pump beam to the crystal was individually adjusted to satisfy the non-collinear or collinear phase-matching condition. To inject seeding beams for the idler beam, two O-band external cavity laser diodes (ECLDs) (6324, New focus; tuning range of λ = 1270-1330 nm; frequency linewidth of <300 kHz) were coupled with the pump beam, so that the injection beams satisfied the non-collinear phase-matching condition and the collinear phase-matching condition, which were measured to compare the performances. The output power of each seeding beam was increased to 6 mW using optical semiconductor amplifiers. The generated idler outputs with a dual wavelength showed a narrow frequency linewidth and wide wavelength tunability in the O-band range by controlling the wavelengths of the ECLDs independently. Figures 3(a) and 3(b) show spectra of the OPG outputs without (blue) and with seeding (red) of λ 1 = 1323 nm and λ 2 = 1326 nm, under the (a) non-collinear phase-matching condition and (b) collinear phase-matching condition. The spectra were measured using a spectral analyzer (ANDO AQ6315A, minimum wavelength resolution of 0.05 nm). In non-collinear phase-matching, the suppression of optical parametric fluorescence by seeding was 8 dB. Efficient seeding produced a higher signal-to-noise ratio of about 30 dB between the peak intensity and residual fluorescence intensity. In collinear phase-matching, the suppression of fluorescence was only about 2 dB and the signal-to-noise ratio was 15 dB. In comparison, the suppression of fluorescence intensity was about twice as high under the noncollinear phase-matching condition than that under the collinear phase-matching condition. The walk-off compensation increased the overlap of pump and seed beams, resulting in the greater suppression of fluorescence intensity. Additionally, the higher signal-to-noise ratio in non-collinear phase-matching is important for efficient THz-wave generation in the latter DFG process. The energy of is-BBO-OPG was measured with a power meter (OPHIR 3A). The CW power of seeding beams was subtracted from the measured energy of is-BBO-OPG. The values of the maximum energy of is-BBO-OPG were, respectively, 0.44 and 0.21 mJ under non-collinear and collinear phase-matching conditions. The conversion efficiencies from the pump to the idler output were 4.0 and 1.8% under non-collinear and collinear conditions, respectively. Figure 3(c) shows the spectrum of the idler output in noncollinear phase-matching measured with the higher wavelength resolution. The spectrum had five clearly separated peaks equally spaced with a frequency of 0.47 THz, which exactly equals the frequency difference between the two seeding beams. A multiple-wavelength output was measured in the entire tuning range, where the peaks are equally spaced at intervals equivalent to the difference frequency of the two seeding beams. The generation of multiple wavelengths resulted from the four-wave mixing 23) of λ 1 and λ 2 with a high gain of the BBO crystal. The multiple wavelength output is expected to induce the cascade DFG process for highly efficient THz-wave generation.
For the generation of THz-waves, the NIR output of is-BBO-OPG was focused onto a 9 × 9 × 0.8 mm 3 DAST crystal by a planoconvex lens with a 100 mm focal length. The polarization of the NIR beam was aligned to the a-axis of the DAST crystal under the type-0 phase-matching condition to make use of the high nonlinearity and broadband tunability. After the NIR beam pumped the DAST crystal, the residual beam was absorbed by the IR filter, which only transmitted the THz-wave. The THz-wave from the DAST crystal was collimated by a Tsurupica lens with a 50 mm focal length. The THz-wave was detected by a 4 K Si bolometer with a black polyethylene film on the window to remove the rest of the IR wave in order to transmit only the THz-wave. A far-infrared filter with a cutoff frequency of 3.6 THz was also inserted to remove the stray light. The output voltage of the Si bolometer was measured using an oscilloscope. During measurements, optical paths of the THz-wave were purged with dry N 2 gas to prevent absorption loss by water vapor in air. with different dynamic ranges in the oscilloscope, because the THz-wave output changed greatly by two orders of magnitude depending on the frequency. Data of three ranges of frequency were merged for seamless and continuous connection of the graph. Tuning of the THz-wave frequency was achieved by changing the wavelength of one seeding beam in the range of λ 1 = 1302 to 1325 nm with a resolution of 17 GHz, while the wavelength of the other seeding beam λ 2 was fixed at 1326 nm. The results of the bolometer output showed that the THz-wave output was widely tunable from 0.3 to 4 THz. The maximum energy of sub-THz-waves was 80 pJ at 0.65 THz, corresponding to a peak power of 0.8 W, where the pulse width of 100 ps was inferred from the results of an earlier experiment. The sensitivity of the bolometer was measured using a calibrated pyrometer. The conversion efficiency of energy from NIR to sub-THz-waves was approximately 5 × 10 −7 . The highest THz-wave frequency was limited by the cutoff frequency of the mid-infrared filter inserted in the bolometer. Figure 4(b) shows the wavelength measurement of the THz-wave generated by the scanning Fabry-Perot etalon. The etalon was placed in front of the bolometer. The etalon was formed of two Si plates, where one of the Si plates was set on a mechanically movable stage. The free spectral range (FSR) and finesse of the etalon were estimated to be 75 GHz and 2.3, respectively. The wavelengths of the seeding beams were fixed at 1323 and 1326 nm, respectively. The periodical intensity peaks were measured by increasing the distance between the two Si plates. The distance between two adjoining peaks is 320 µm, which is half-the wavelength of the input THz-wave and corresponds to the frequency of 0.47 THz, which matches the difference frequency of the two seeding beams. The frequency linewidth of the sub-THzwave was estimated to be 33 GHz by fitting analysis of these data. The measured results showed the generated sub-THzwave to be monochromatic. Therefore in the DFG process, only the nearest pair of peaks in the multiple-wavelength pump beam was efficient for the generation.
In conclusion, we demonstrated widely tunable and monochromatic THz generation by DAST-DFG pumped by the NIR-wave output of is-BBO-OPG. We developed dualwavelength is-BBO-OPG seeded by two seeding beams with a narrow spectrum. For is-BBO-OPG, we designed noncollinear phase-matching to optimize the overlap of the pump beam and the idler beam. In the designed configuration, effi-cient seeding and high conversion efficiency were achieved. The is-OPG generated a spectrum with peaks separated by a sub-THz difference frequency. By pumping DAST-DFG by is-OPG, a widely tunable THz-wave of 0.3-4 THz was generated and was fully controlled by the seeding beam wavelength. The output THz-wave was monochromatic. The noncollinear phase-matching configuration proposed herein is expected to be applicable for other crystals possessing a walkoff effect, such as KTP, KTA, KDP, BiBO, LBO, CLBO, LiTaO 3 , and LiNbO 3 . Moreover, the technique of generating clearly separated wavelengths in the developed NIR source is expected to be applicable to other pumping sources for exciting nonlinear crystals reported in the literature related to THz-wave generation, such as organic crystals of BNA, DASC, BDAS-TP, DSTMS, and OH1 and semiconductor crystals of GaP, GaSe, ZnSe, and ZnTe. The developed DAST-DFG system pumped by is-BBO-OPG is anticipated to be a promising system for a widely tunable THz-wave source covering the sub-THz frequency region, and should be applicable for nondestructive imaging, remote sensing, or the calibration of sensitivity in novel sub-THz-wave detectors.