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Aligned copper nanorod arrays for highly efficient generation of intense ultra-broadband THz pulses

Scientific Reports volume 7, Article number: 40058 (2017) | Download Citation

Abstract

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.

Introduction

Terahertz radiation is a powerful tool for imaging1 and probing various physical systems2, because of its unique nonionizing nature and transparency to many materials that are opaque to visible radiation3. It also has strong interactions with diverse materials, which allow THz radiation to probe many physical, chemical and biological systems4,5,6,7. Intense broadband THz pulses are also opening new scientific areas to explore, such as nonlinear optics in the THz domain8, as well as new technological opportunities, such as single-shot THz spectroscopy and imaging9. 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 detail10,11. For example, optical rectification sources and THz generation from air plasma12,13 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. Electron accelerators can also be used to produce energetic THz pulses either (i) by bending a beam of relativistic electrons using a strong magnetic field or (ii) by sending them through a thin metal foil, but usually they are not available at modest laboratory scales15,16,17,18. Progress in research up to now has made it clear that many laser-based methods possess an upper limit in the maximum driving laser intensity19 that could be used, which is limiting the THz yield and hence their applications to several spectroscopic purposes4,20.

High-intensity ultrafast laser-plasma interaction can also be a potential source of intense ultra-broadband THz radiation21,22,23,24. Particle-in-cell (PIC) simulations have predicted that GV/cm THz fields can be generated by such interactions via different mechanisms such as laser wakefield excitation in underdense plasma25 and coherent transition radiation with solid targets26. Intense transition radiation in the THz frequency range has been observed when energetic electrons generated by high-intensity laser-solid interaction are ejected from the target26,27. THz pulses (0.1–133 THz) with pulse energy more than 700 μJ have been demonstrated from rear side of a foil target via a different mechanism; THz generation via target normal sheath acceleration24,28. Intense THz pulses via generation of coherent transition radiation in the rear side of size limited thin targets have also been demonstrated by Liao et al.27. Being generated via energetic electrons, transition radiation could reveal the characteristics of those electron bunches produced during the laser-solid interaction and hence is very important in high-intensity laser-plasma interaction29,30.

In this work, we first study transition radiation in the THz frequency range generated by relativistic intensity laser-plasma interaction using thick copper (Cu) targets. Then, we demonstrate that aligned Cu nanorod targets, which have been used to improve the efficiency of generating highly energetic photons and particles31,32,33,34,35,36,37, can also be used to significantly enhance the THz pulse energy through transition radiation. Single-shot electro-optic measurement shows the temporal behavior as well as the coherent nature of the THz pulses generated via transition radiation.

Results

In our experiments, intense, THz pulses are generated via high-intensity laser-solid interaction (for details about the experiments, please see Method). In Fig. 1(a), we compare the THz pulse energy for medium frequencies (≤20 THz, with UHMWPE window) detected by the pyroelectric detector from polished and rough Cu thick-solid targets. The presence of small random structures on the target surface could increase the THz pulse energy by about 4 times. In Fig. 1(b), we show the THz pulse energy emitted when high-intensity femtosecond laser irradiates the aligned Cu nanorod targets with a nanorod diameter (D) of 200 nm and lengths (h) of 5 μm, 15 μm, 30 μm, 40 μm, and compare them with the THz pulse energy emitted from an optically polished Cu target.

Figure 1: THz pulse energy for different targets as a function of laser intensity on target.
Figure 1

(a) Comparison of THz pulse energy generated from thick polished and rough Cu solid targets in spectral range ≤20 THz; (b) Comparison of THz pulse energy generated from nanorod (NR) targets of different nanorod lengths (h) and diameter (D) of 200 nm in the spectral range ≤20 THz; (c) THz pulse energy generated from nanorod targets with different nanorod (NR) lengths, with high-pass window in spectral range from 20 THz to 200 THz.

Compared with polished Cu targets, we observe a 13.8 times enhancement in the THz pulse energy for h = 5 μm nanorod targets. However, we also find that the THz pulse energy decreases as nanorod length (h) increases further. This is in contrast to earlier studies on the X-ray generation, which showed enhancement in the X-ray yield with increasing nanorod length34. To investigate this difference, we repeat the experiment with a high-pass window that has lower transmission for lower frequencies (1% for ≤20 THz, ~10% transmission for ≥100 THz and ~60% for ≥130 THz). Radiation with frequencies higher than 200 THz is blocked by the HRFZ-Si filters. The results are shown in Fig. 1(c). In this measurement, the reference material is Cu tape, because the Cu nanorod targets were attached to the bulk Cu target by Cu tape, which has adhesives on both sides. For higher frequencies of electromagnetic radiation (20 THz to 200 THz), the pulse energy increases with the nanorod length (h), and the enhancement in the pulse energy reaches as high as 28 times for the case of the 60 μm long Cu nanorod target, demonstrating a large pulse energy of about 32 μJ per pulse in 0.0873 Sr solid angle.

Single-shot detection of THz pulses

Temporal profiles of the THz pulses have been measured by using single-shot electro-optic measurements38 using a reflecting echelon mirror, a technique similar to the one developed by Minami et al.39. For details about experimental scheme, please see the section Methods. The THz field profile in the temporal domain as well as in the frequency domain obtained from polished and nanorod targets are shown in Fig. 2(a) and (b). The temporal profile of the THz pulses varies from shot to shot, and so in Fig. 2(a), we show the data that has the maximum THz peak field out of 20 successive shots. Likewise, THz energy measurement from nanorod targets, THz field measurement also shows maximum for 5μm long Cu nanorod. A simple Gaussian fit provides a pulse width (FWHM) of 235±6 fs for the THz pulse obtained from 8 μm nanorod target, which is expected by the ultra-broadband nature of the THz pulses.

Figure 2
Figure 2

Comparison of THz pulses (a) in temporal domain (b) in frequency domain captured in single-shot experiment with polished and nanorod targets.

Numerical simulations

To understand our experimental results in detail, we have performed two dimensional particle-in-cell (PIC) simulations. The geometry of the simulation box is shown in Fig. 3(a). The simulation parameters are set close to those of the experiment. In the simulations, a p-polarized Gaussian beam with wavelength of 800 nm, pulse width of 40 fs and intensity of 3.5 × 1018 Wcm−2 is incident onto the target at an incidence angle of 30°. Since the prepulse contrast of the laser, which is used in the experiment is high, we have not included preplasma in the simulations. An 8 μm thick copper target is used, which is covered with Cu nanorod arrays with 200 nm diameter (D) and spacing (d0) of 200 nm. Figure 3(b) is a snapshot of the spatial distribution of the magnetic field, which is time-averaged over a laser period in order to filter out the high frequency components. Both backward and forward radiations are emitted from the target front and back sides, respectively, which can be attributed to coherent transition radiation generated by hot electrons produced in the laser-plasma interaction26,40. For polished planar targets, the THz radiation is the weakest around the specular reflection direction and strongest along the target surface direction, typical for transition radiations. The simulation shows that the nanorods have enhanced the backward THz radiation and have changed its emission direction to the specular reflection direction, significantly from that predicted for a planar target. These are more obvious from the spectra of the electromagnetic fields, which is detected 100 μm away from the laser irradiated spot in the target front, as shown in Fig. 3(c) and (d).

Figure 3
Figure 3

PIC simulation results: (a) Simulation geometry. (b) Snapshot of magnetic field Bz (averaged in a laser cycle) of the THz radiation. (c) and (d) Spectra of EM fields emitted from the target front with the nanorod length is 0.8 μm and 4 μm, respectively. (e) Intensity of THz radiation (maximum in THz range of the spectra) as a function of the nanorod length. Radiations are detected in the reflection direction (120°). (f) Total kinetic energy of hot electrons (Ek > 30 keV) as a function of the nanorod length. Energies are rescaled to that of planar target.

To check the effect of the nanorod length on the THz radiation, we have varied the nanorod length from 0 to 30 μm, which shows the presence of optimized nanorod length for THz radiation. When the nanorod length increases from 0 to 4 μm, the radiation intensity decreases along the target surface (near 0° or 180°) while it increases in the specular reflection direction (120°). As a whole, it becomes dominant on the specular reflection direction. Figure 3(e) shows that the intensity of the backward THz radiation in the specular reflection direction varies with the nanorod length, where the intensities are normalized to the maximum THz emission from polished targets. As the length increases, the radiation intensity increases until h = 4 μm, then it decreases slightly for h > 4 μm, which reaches a saturation for h > 10 μm. Because the emitted THz radiation is coherent transition radiation generated by the hot electrons, the radiation is the strongest when the absorption rate of the laser energy by electrons is the highest. The corresponding optimal nanorod length, at which the highest number of hot electrons is produced, is determined by the nanorod parameters d0 and d136. The simulations show enormous increase in both the number and total energy of hot electrons for the case of nanorod targets, when compared with polished targets. The variation in the total kinetic energy of hot electrons as a function of the nanorod length (h) is shown in Fig. 3(f). The nanorod array enhances the electron energy in both the x (Ekx) and y (Eky) directions, but much more significantly in the y (vertical) direction. We observe that Eky peaks at around h = 3 μm, although the energy in the horizontal x-direction Ekx is not the maximum. The electron energy in the y-direction (Eky) contributes more to THz emission in specular reflection direction (120°) than the electron energy in the x-direction (Ekx). This is consistent with the theory of coherent transition radiation that the radiation is mostly emitted in a large angle or nearly perpendicular to the moving direction of the electron26,40,41 when the electrons are of moderate energy. The average kinetic energy of hot electrons is normally at the order of 100 keV under the laser conditions. The maximum Eky is about 3.4 times higher than that from polished targets. The tendency of the THz intensities agrees very well with the behavior of the total energy of hot electrons in the vertical direction.

Conclusions

We have demonstrated that the THz pulse energy can be increased by using aligned Cu nanorod array targets, with a maximum enhancement of up to 13.8 times for ≤20 THz and 28 times in the spectral range between 20 THz and 200 THz. It is shown that there is an optimal nanorod length for the most efficient THz radiation. The temporal profiles of the THz pulses are also obtained by the use of a single-shot electro-optic measurement. PIC simulations reveal the mechanism behind the intense THz pulse generation by this technique, which we attribute to coherent transition radiation at THz frequencies by the energetic electrons produced by the laser plasma interactions. It also reveals that the THz radiation with nanorod array targets is distributed mainly in the specular reflection direction, which is different from that with a planar target.

The THz pulses, especially for low frequency THz radiation, are emitted in a broad angle, which is also seen in the simulation results. However, we only collect THz signal over a small solid angle of 0.0873 Sr, and thus we obviously do not collect all of the THz energy generated by the interaction. To estimate the total THz pulse energy generated by the interaction, we consider that the THz pulses are emitted in a 2π solid angle24,42 on the target front. By correcting for the small solid angle of detection, we estimate that several hundred micro-joule THz energy is generated at a frequency range (≤20 THz). Most of this THz pulse energy can easily be collected by using an ellipsoidal mirror24, which opens a roadway towards millijoule class THz sources on tabletop.

Methods

Figure 4(a) shows a schematic diagram of the experimental setup. We use 10 TW femtosecond laser pulses with high contrast (nanosecond contrast ~10−7) from the10 Hz beam line of the Advanced Laser Light Source (ALLS) facility at INRS-EMT. This laser, with incidence angle of 45 and p-polarization, is focused on to a Cu target (size: 5 cm × 5 cm × 3 cm) using an f/3 off-axis parabolic mirror, to a circular spot of 20 μm in diameter. The target is mounted on an automated XYZ translation stage inside a vacuum chamber. The 10 Hz beam line can deliver up to 240 mJ maximum pulse energy with 40 fs pulse duration after compression, with a central wavelength of 800 nm, which when focused results in a peak intensity of about 3.5 × 1018 Wcm−2. Ultra-broadband THz and infrared (IR) pulses (via the generation of coherent transition radiation) are generated as a result of laser-plasma interaction. THz pulses are then collimated by using a thick gold plated off-axis parabolic mirror, and then guided out of the vacuum chamber through a THz window made from ultrahigh molecular weight polyethylene (UHMWPE), which only transmits radiation up to 20 THz while blocking higher frequency electromagnetic radiation. The generated THz pulses are then refocused on to a calibrated pyroelectric detector (Gentec-EO, THZ5I-BL-BNC) using another off-axis parabolic mirror to measure the THz pulse energy. To remove any residual of the 800 nm driving laser, we have further used two high-resistivity float-zone silicon (HRFZ-Si) filters that have flat transmission up to the cut-off at around 1.5 μm. We take an average over 15 shots to improve the statistical error. The THz pulse energy from the optically polished target is compared with that from the aligned Cu nanorod array targets. The THz pulse energy is collected over a relatively small solid angle of 0.0873 Sr.

Figure 4
Figure 4

(a) Schematic diagram of the experimental setup. (b) X-ray diffraction (XRD) spectrum of Cu nanorods embedded in AAO template. (c), (d), (e) & (f) SEM images of Cu nanorod arrays at different magnifications: (c,d) top view; (e,f) cross-sectional view.

Nanorod target fabrication

The commercially available porous anodic aluminum oxide (AAO) membrane (pore size: 200 nm, membrane thickness: 60 μm, Whatman® Anodisc) was used as a template for the electrochemical deposition of Cu nanorod arrays43. A gold layer (300 nm) was sputtered on one side of the through-hole AAO template, serving as the working electrode in a conventional three-electrode cell for Cu electrochemical deposition, with graphite carbon and saturated calomel electrode (SCE) electrode as the counter and reference electrode, respectively. The electrolyte was 0.2 M CuSO4·5H2O + 0.1 M H3BO3 for Cu deposition. Experiments were carried out using Potentiostat (Autolab) with the constant potential of −1.20 V (vs. SCE) at room temperature. The length of the Cu nanorods can be controlled between 0 and 60 μm by adjusting the deposition time.

The crystallographic studies of Cu nanorods embedded in AAO were carried out by X-ray spectroscopy (XRD, Bruker D8 Advanced Diffractometer, Cu radiation). The XRD spectrum of the Cu nanorods, shown in Fig. 4(b), fits the standard XRD pattern very well. Three reflection peaks attributed to (111), (200), (220) are evidently noticeable, and can be completely indexed to the Cu face-centered cubic crystal structure (JCPDS 04-0836)44. There are no impurities except for the broad peaks belonging to the amorphous AAO template and the corresponding peaks of the sputtered Au electrode. For the SEM characterization, the as-prepared Cu nanorods embedded in AAO template were first immersed in the NaOH solution to dissolve the alumina membrane, and then the nanorods were washed thoroughly with distilled water and ethyl alcohol several times. Figure 4(c), (d), (e) and (f) show the SEM images of the Cu nanorods (length h = 15 μm) at different magnifications. It is clearly depicted from the SEM micrograph that a large quantity of well-aligned, dense, homogeneous in diameter, and parallel to each other Cu nanorods have been successfully fabricated by this technique.

Single-shot electro-optic measurement

The single-shot electro-optic measurement of THz pulses is setup by carefully encoding the temporal information in the spatial direction38,39,45,46. The THz pulses generated by this technique and described before are then refocused on an electro-optic crystal by using another off-axis parabolic mirror, which has a hole at the center. A 1mm thick Zinc-Telluride (ZnTe) crystal has been used as the electro-optic crystal in our case, which has spectral response up to 3 THz. The spectral sensitivity of the THz detection system is limited to 3 THz by the ZnTe crystal. A part of the main beam (~1mJ in energy), which can be time delayed by a 5 cm delay stage in the path, as shown in the Fig. 5, has been used as a probe for the electro-optic sampling. The probe energy is then reduced further below the damage threshold of the electro-optic crystal, which is placed at the focus, by a thin neutral density filter. Before interacting with the THz pulse on the ZnTe crystal, the probe beam passes through a half-wave (λ/2) plate and a thin polarizer and reflects from a nickel echelon mirror. The half-wave (λ/2) plate is used to overlap the plane of polarization between the probe beam and the generated THz beam. The thin polarizer is used to increase the polarization contrast of the input probe. The delay line in the conventional electro-optic measurement of THz pulses is replaced by the echelon mirror. The echelon mirror46 consists of a number of optically polished reflecting steps of equal dimension distributed horizontally, as shown in the left panel of Fig. 5. In our case, the echelon mirror with dimension of 10 mm × 10 mm is used, which is made with polished nickel with 500 steps of height H = 5 μm and width W = 20 μm and is placed just before the interaction with the THz pulses.

Figure 5: Schematic of the experimental setup for single-shot electro-optic measurement of THz pulses.
Figure 5

The left panel shows the working mechanism of reflective echelon mirror.

A plane wave front, after reflection from the echelon mirror, splits into several beamlets with a delay between them, thus encoding the temporal information in the spatial direction. The beamlet size and the delay between beamlets is determined by the step size of the echelon mirror. Any space resolved detector such as CCD/CMOS camera with sufficient pixel resolution can be used to extract temporal information.

After reflection from the echelon mirror, the probe beam is then focused through the central hole of the off-axis parabolic mirror and finally collinearly overlaps with the THz beam on the ZnTe crystal. After being collimated by another lens with the same focal length, the spatial profile of the probe beam is captured on a CCD camera (Point Grey: FL2-14S3M-C), which is triggered by the laser. A Glan polarizer has been placed just before the CCD camera, which works as an analyzer to capture any change in the polarization state of the probe pulse due to the electro-optic effect during interaction with the THz pulses. Initially, the temporal overlap of the 800 nm probe pulse with the attenuated 800 nm pump pulse has been performed by looking at the interference fringe at the CCD camera and with the help of a delay line incorporated in the beam path, as shown in Fig. 5. After that, THz window made from UHMWPE and HRFZ-Si filters are used in main beam path to block the IR beam and only THz beam (≤20THz) is allowed to pass. The delay stage in the probe path is then readjusted for proper positioning of the THz peak in the THz trace in the CCD image by looking at the image from the CCD camera.

Additional Information

How to cite this article: Mondal, S. et al. Aligned copper nanorod arrays for highly efficient generation of intense ultra-broadband THz pulses. Sci. Rep. 7, 40058; doi: 10.1038/srep40058 (2017).

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References

  1. 1.

    Terahertz wave imaging: horizons and hurdles. Physics in Medicine and Biology 47, 3667–3677 (2002).

  2. 2.

    , , , & Carrier dynamics in semiconductors studied with time-resolved terahertz spectroscopy. Reviews of Modern Physics 83, 543–586 (2011).

  3. 3.

    et al. THz imaging and sensing for security applications—explosives, weapons and drugs. Semiconductor Science and Technology 20, S266–S280 (2005).

  4. 4.

    Principles of Terahertz Science and Technology (Springer Science & Business Media, New York, 2009).

  5. 5.

    , & Far-infrared vibrational modes of DNA components studied by terahertz time-domain spectroscopy. Physics in Medicine and Biology 47, 3807–3814 (2002).

  6. 6.

    , & Terahertz spectroscopy and imaging - Modern techniques and applications. Laser & Photonics Reviews 5, 124–166 (2011).

  7. 7.

    , & Resonant and nonresonant control over matter and light by intense terahertz transients. Nature Photonics 7, 680–690 (2013).

  8. 8.

    et al. Nonlinear terahertz field-induced carrier dynamics in photoexcited epitaxial monolayer graphene. Physical Review B 91, 035422 (2015).

  9. 9.

    et al. Intense terahertz radiation and their applications. Journal of Optics 18, 093004 (2016).

  10. 10.

    , , & Single-cycle terahertz pulses with amplitudes exceeding 1 MV/cm generated by optical rectification in LiNbO3. Applied Physics Letters 98, 091106 (2011).

  11. 11.

    & Demonstration of a low-frequency three-dimensional terahertz bullet with extreme brightness. Nature Communications 6, 5976 (2015).

  12. 12.

    et al. Intense terahertz generation in two-color laser filamentation: energy scaling with terawatt laser systems. New Journal of Physics 15, 075002 (2013).

  13. 13.

    et al. Improved terahertz two-color plasma sources pumped by high intensity laser beam. Optics Express 17, 6044 (2009).

  14. 14.

    , & Phase-locked generation and field-resolved detection of widely tunable terahertz pulses with amplitudes exceeding 100 MV/cm. Optics Letters 33, 2767 (2008).

  15. 15.

    et al. Intense terahertz pulses from SLAC electron beams using coherent transition radiation. Review of Scientific Instruments 84, 022701 (2013).

  16. 16.

    et al. High-power terahertz radiation from relativistic electrons. Nature 420, 153–156 (2002).

  17. 17.

    & Accelerator- and laser-based sources of high-field terahertz pulses. Journal of Physics B: Atomic, Molecular and Optical Physics 46, 192001 (2013).

  18. 18.

    et al. High-Field High-Repetition-Rate Sources for the Coherent THz Control of Matter. Scientific Reports 6, 22256 (2016).

  19. 19.

    et al. Effect of extreme pump pulse reshaping on intense terahertz emission in lithium niobate at multimilliJoule pump energies. Optics Letters 39, 4333 (2014).

  20. 20.

    Cutting-edge terahertz technology. Nature Photonics 1, 97–105 (2007).

  21. 21.

    , , , & Subpicosecond, electromagnetic pulses from intense laser-plasma interaction. Physical Review Letters 71, 2725–2728 (1993).

  22. 22.

    , , , & Single-cycle strong terahertz pulse generation from a vacuum-plasma interface driven by intense laser pulses. Physical Review E 79, 046411 (2009).

  23. 23.

    et al. Effects of laser-plasma interactions on terahertz radiation from solid targets irradiated by ultrashort intense laser pulses. Physical Review E 84, 036405 (2011).

  24. 24.

    et al. Observation of Gigawatt-Class THz Pulses from a Compact Laser-Driven Particle Accelerator. Physical Review Letters 111, 074802 (2013).

  25. 25.

    , & Single-cycle powerful megawatt to gigawatt terahertz pulse radiated from a wavelength-scale plasma oscillator. Physical Review E 77, 046405 (2008).

  26. 26.

    , & High-field half-cycle terahertz radiation from relativistic laser interaction with thin solid targets. Applied Physics Letters 103, 204107 (2013).

  27. 27.

    et al. Demonstration of Coherent Terahertz Transition Radiation from Relativistic Laser-Solid Interactions. Physical Review Letters 116, 205003 (2016).

  28. 28.

    et al. Characterization of 700 μJ T rays generated during high-power laser solid interaction. Optics Letters 38, 4705 (2013).

  29. 29.

    et al. Few femtosecond, few kiloampere electron bunch produced by a laser–plasma accelerator. Nature Physics 7, 219–222 (2011).

  30. 30.

    et al. Temporal Characterization of Femtosecond Laser-Plasma-Accelerated Electron Bunches Using Terahertz Radiation. Physical Review Letters 96, 014801 (2006).

  31. 31.

    & Interpretation of the field enhancement factor for electron emission from carbon nanotubes. Journal of Applied Physics 106, 014314 (2009).

  32. 32.

    et al. Intense Picosecond X-Ray Pulses from Laser Plasmas by Use of Nanostructured “Velvet” Targets. Physical Review Letters 84, 5149–5152 (2000).

  33. 33.

    , , , & Metal Nanoplasmas as Bright Sources of Hard X-Ray Pulses. Physical Review Letters 90, 115002 (2003).

  34. 34.

    et al. Highly enhanced hard x-ray emission from oriented metal nanorod arrays excited by intense femtosecond laser pulses. Physical Review B 83, 035408 (2011).

  35. 35.

    Surface Plasmons on Smooth and Rough Surfaces and on Gratings, vol. 111 of Springer Tracts in Modern Physics (Springer Berlin Heidelberg, Berlin Heidelberg, 1988).

  36. 36.

    , & A model for the efficient coupling between intense lasers and subwavelength grating targets. Physics of Plasmas 15, 030702 (2008).

  37. 37.

    et al. Near-complete absorption of intense, ultrashort laser light by sub-λ gratings. Phys. Rev. Lett. 101, 145001 (2008).

  38. 38.

    et al. Single-shot measurement of terahertz electromagnetic pulses by use of electro-optic sampling. Optics Letters 25, 426 (2000).

  39. 39.

    , , & Single-shot measurement of a terahertz electric-field waveform using a reflective echelon mirror. Applied Physics Letters 103, 051103 (2013).

  40. 40.

    & Sub GV/cm terahertz radiation from relativistic laser-solid interactions via coherent transition radiation. Physical Review E 93, 063204 (2016).

  41. 41.

    et al. Theoretical study of transition radiation from hot electrons generated in the laser-solid interaction. Physics of Plasmas 10, 2994 (2003).

  42. 42.

    et al. Terahertz emission from two-plasmon-decay induced transient currents in laser-solid interactions. Physics of Plasmas 23, 013104 (2016).

  43. 43.

    , , , & Electrochemical synthesis of copper nanowires. Journal of Physics: Condensed Matter 14, 355–363 (2002).

  44. 44.

    , , , & Copper Nanoparticles Grafted on a Silicon Wafer and Their Excellent Surface-Enhanced Raman Scattering. Advanced Functional Materials 22, 2067–2070 (2012).

  45. 45.

    , , , & Algorithm for high-resolution single-shot THz measurement using in-line spectral interferometry with chirped pulses. Applied Physics Letters 87, 211109 (2005).

  46. 46.

    , , , & Single-shot terahertz pulse characterization via two-dimensional electro-optic imaging with dual echelons. Optics Letters 32, 1968 (2007).

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Acknowledgements

T. O. and S. S. acknowledge the financial support from the Fonds de recherche du Québec–Nature et technologies (FRQNT) and the Natural Sciences and Engineering Research Council of Canada (NSERC). Z.M.S. and J.Z. acknowledges the support by the National Basic Research Program of China (Nos 2014CB339801 and 2013CBA01504), the National Science Foundation of China (No. 11421064), a MOST international collaboration project (No. 2014DFG02330), and a Leverhulme Trust Research Grant. Q. W. acknowledges the scholarship from China Scholarship Council (CSC) and FRQNT.

Author information

Affiliations

  1. Institut national de la recherche scientifique – Centre Energie, Matériaux et Télécommunications (INRS-EMT), 1650 Lionel-Boulet, Varennes, Québec J3X 1S2, Canada

    • S. Mondal
    • , Q. Wei
    • , H. A. Hafez
    • , M. A. Fareed
    • , A. Laramée
    • , X. Ropagnol
    • , G. Zhang
    • , S. Sun
    •  & T. Ozaki
  2. A*STAR Institute of High Performance Computing, Singapore 138632

    • W. J. Ding
  3. Max Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, Germany

    • H. A. Hafez
  4. Physics Department, Faculty of Science, Helwan University, 11792, Cairo, Egypt

    • H. A. Hafez
  5. SUPA, Department of Physics, University of Strathclyde, Glasgow G4 0NG, UK

    • Z. M. Sheng
  6. Laboratory for Laser Plasmas and Department of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China

    • Z. M. Sheng
    •  & J. Zhang
  7. Collaborative Innovation Center of IFSA, Shanghai Jiao Tong University, Shanghai 200240, China

    • Z. M. Sheng
    •  & J. Zhang

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Contributions

S.M. conducted experiments with H.A.F., M.A.F., A.L., X.R. under the supervision of T.O., S.M. analyzed the results. Q.W. prepared the nanorod targets under the supervision of S.S., W.J.D. performed PIC simulation under the supervision of Z.M.S., S.M., Q.W. and W.J.D. prepared the manuscript. All authors reviewed the manuscript.

Competing interests

The authors declare no competing financial interests.

Corresponding author

Correspondence to T. Ozaki.

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