Abstract
The spatiotemporal dynamics of a surface plasmon polariton (SPP) wave packet (WP) that interacts with a plasmonic nanocavity on a metal surface are investigated via femtosecond time-resolved two-photon fluorescence microscopy and numerical calculations. The nanocavity, which consists of a metal–insulator–metal (MIM) laminar structure (longitudinal length: ∼100 nm), behaves as a subwavelength meta-atom possessing discretized eigenenergies. When a chirp-induced femto-second SPP WP is incident on the nanocavity, only the spectral component matching a particular eigenenergy is transmitted to continue propagation on the metal surface. This spectral clipping induces a spatial peak shift in the WP. The shift can be controlled by tuning the eigenenergy or chirp.
1 Introduction
In optical physics, the control of the spatiotemporal dynamics of light pulses has been a fascinating topic of study. The tunability of material dispersion and/or optical resonance has facilitated control over group velocities of light in a variety of natural materials and artificial nanostructures, including gaseous atoms [1, 2], ultracold atoms [3], optical fibers [4], ring resonators [5, 6], photonic crystals [7, 8], plasmonic Bragg gratings [9], and metamaterials [10], [11], [12], [13]. Metamaterials consist of arrayed subwavelength-scaled optical resonators, each of which provides specific shifts in the phase, amplitude, and polarization between the incident and scattered components of the light field [14]. Accordingly, light has been tailored to realize various applications such as anomalous refraction and reflection [15], vector beam formation [16], spectral filtering [17], light acceleration [18, 19], and ultrafast optical pulse shaping [20].
An established method for achieving control of the group velocity of light is the use of spectral windows in which materials exhibit abnormal dispersion responses to frequency [21], [22], [23]. In the framework of classical electrodynamics, the realization of group velocities that deviate significantly from the speed of light in vacuum, such as subluminal, superluminal, and negative group velocities in natural materials, has been interpreted as a result of the steep change in the refractive index near the absorption lines of atoms [1], [2], [3]. Slow light in photonic crystals has been caused by a large bending of the photonic band near the Brillouin zone edge [7], [8], [9]. Doubly negative phase and group velocities in metamaterials have been realized by using regions with negative values of both permittivity and permeability near the electric and magnetic resonance frequencies of the artificial resonator structure [10]. The width of the spectral window, in which these peculiar optical pulse propagations occur, is usually not very wide. Spectral widths of light pulses should be narrow enough to fit within the limited frequency range. In these cases, the instantaneous frequency of the light pulse can be assumed to be constant over the pulse duration. The envelope shape of the pulse remains similar before and after transmission through the natural materials or the artificial structures, although the amplitude would be attenuated because of the absorption by materials.
If the optical pulse has a large spectral width that exceeds the spectral window described above, and multiple resonance lines enter the spectral width, the amplitude and phase modulation of each of the frequency component of the pulse will be significantly different for each frequency. In this case, the pulse waveform of the incident light is no longer maintained, because both the envelope shape and the instantaneous carrier frequency are modulated significantly in time. This situation is rather similar to the pulse shaping of femtosecond laser pulses [20, 24].
Recently, several methods using spatio-temporal couplings (STCs) [25, 26] or space-time correlations [27, 28] of light pulses have been reported, which allow spatio-temporal control of light pulses based on a different principle rather than relying on the spectral window of materials. In these methods, the direction of wavevector is controlled for each frequency component of the light pulse. The spectral widths of light pulses are no needed to be kept narrow. By shaping the spatial distribution of the pulse in both the longitudinal and the transverse directions, the temporal evolution of the peak intensity of the optical pulse can be highly controlled. Moreover, by exploiting the degree of freedom in the temporal variation of the carrier frequency of optical pulses, advanced spatio-temporal control of light has been achieved, including a wide-range control of the light group velocity [29], [30], [31], temporal modulation of the light velocity [32, 33], bending and steering of the light direction [34], and pulses propagations in a dispersive medium without spreading [35].
We recently reported a finite-difference time-domain (FDTD) simulation study of the deformation of the temporal waveform of a surface plasmon polariton (SPP) wave packet (WP) with a femtosecond time duration and a wide spectral width transmitted through a metal–insulator–metal nanocavity (MIM-NC) [36]. The MIM-NC is a typical meta-atom used in the visible to infrared light regions [37], [38], [39], [40], [41]. The levels of eigenenergies were controlled by tuning the structural length of the MIM-NC. When an up-chirped, broadband SPP WP was incident, the spectral components overlapping the cavity eigenmodes were transmitted otherwise they were reflected. The transmitted SPP WP still maintained a femtosecond time duration due to a wide linewidth of the eigenmodes, however, the coordinate of the intensity peak showed a significant shift in time compared to a reference WP which propagated on a flat surface without the MIM-NC. The shift of the intensity peak was controlled either forward or backward by tuning the eigenenergy of the MIM-NC. If the position of the wave packet is defined as the coordinate of the maximum intensity of the envelope, then this peak shift produces an apparent velocity anomaly as the wave packet passes through the nanocavity. The temporal behavior of SPP WPs were tuned by controlling the direction of the wavevector of each frequency component using cavity resonances, which could be conceptually compared to the spatio-temporal control of light pulses using STCs. In metamaterials, the optical responses of the meta-atoms are accumulated over the spectral bandwidth and sectional area of the incident light beam to determine the complete spatiotemporal behavior of the light pulses [42]. Therefore, to realize emerging applications based on the newly developed controllability of light, it is indispensable to understand the dynamic responses of individual meta-atoms and their roles in the modulation of light pulses in terms of intensity, spatial shape, and temporal shape [43, 44].
In this study, the spatiotemporal dynamics of SPP WPs interacting with a subwavelength-scale MIM-NC were investigated by femtosecond time-resolved two-photon fluorescence microscopy (TR-2PFM). 10 fs duration and 810 nm center wavelength light pulses irradiate an Au film containing a coupler and an MIM-NC to initiate SPP WP propagation [45]. The SPP WPs were optically imaged by up-converting a small portion of the energy of the SPP field to fluorescent emission with the wavelength of about 470 nm through two-photon fluorescence process in a ∼50 nm thick dye-doped PMMA layer coated on the surface [46], [47], [48], [49]. In combination with a pump-probe technique, spatio-temporal evolution of SPP WP was dynamically visualized with 10 fs time and 0.5 μm spatial resolutions. The TR-2PFM provided time-resolved movies of SPP WPs that were similar character to those produced by time-resolved photoemission electron microscopy (TR-PEEM), which has been a representative method for revealing SPP dynamics on femtosecond timescales [50], [51], [52], [53], [54], [55], [56], [57]. Although the spatial resolution of the TR-2PFM is limited by the resolution of the objective lens of the optical microscope and thus it is inferior to that of a PEEM, the TR-2PFM has several useful characteristics: The measurements can be performed in air, and the sample material can be a variety of materials including insulators. In addition, TR-2PFM can be easily combined with a variety of light sources such as infrared lasers and vector beams.
The TR-2PFM images revealed the motion and deformation of the SPP WPs, which evolved as a function of the pump–probe delay time. The coordinates of the intensity peak of a WP showed a distinct spatial shift relative to the coordinates of a reference peak when the WP was transmitted through an MIM-NC. The spatial shifts were controlled to within several micrometers in either the forward or the rearward directions depending on the cavity eigenenergies. Simulations performed using a finite-difference time-domain (FDTD) method and an analytical model based on a complex dispersion (CD) relation of SPPs (CD model) [51, 52] revealed that for a chirp-induced SPP WP, spectral clipping by an MIM-NC induced spatial shifts.
2 Materials and methods
2.1 Sample fabrication and experimental setup
To study the optical interaction of an SPP WP with an MIM-NC, a 10 fs SPP WP was made to propagate over an Au surface containing an MIM structure. Figure 1(a) shows a schematic of the launching of an SPP WP by the incidence of femtosecond light and the interaction of the WP with an MIM-NC having a few eigenenergies near the spectral range of the SPP. The MIM-NCs were prepared by placing rectangular Au nanoblocks on an Al2O3 (thickness (h) = 16 nm)/Au (h = 100 nm) film (Figure 1(a) and (b)). The eigenenergy levels were determined as a function of the MIM-NC structure length L, which corresponds to the length of the waveguide for the SPP inside the cavity. The MIM-NCs were fabricated by sequentially changing the length L in the range of 50–220 nm. On the same Au surface, another straight MIM structure was placed 40 μm apart from the MIM-NC as a light–SPP coupler. The entire area of the surface was coated with a thin dye-doped PMMA layer to form a two-photon fluorescent layer. The dye (coumarin 343) used for the fluorescent layer has absorption and emission peaks at approximately 440 and 470 nm, respectively. The wavelength of the absorption line is shorter than that of the femtosecond laser; thus, the dye doping does not affect the linear extinction coefficient of PMMA.
2.2 Time-resolved two-photon fluorescent microscopy of SPP WP
The light source was a custom-made Ti:sapphire laser oscillator with a pulse duration of 10 fs, a spectral distribution ranging from 680 nm to 900 nm (center wavelength: 810 nm), a repetition rate of 90 MHz, and an average power of 450 mW. Light pulses were generated such that they formed coaxially aligned pump–probe pulse pairs using a Mach–Zehnder interferometer (MZI) [50, 58]. A piezoactuator-driven optical stage was used to control the length difference between the two arms of the MZI with a precision of <20 nm (<70 as) to ensure an interferometric phase correlation between the pump and probe. Then, the formed pulses were loosely focused onto an oval-shaped spot (80 × 60 μm) on the sample surface where both an MIM-NC and a light–SPP coupler were placed. The laser power per pulse on the sample surface was 0.9 μJ/mm2. P-polarized, dispersion-compensated pump–probe pulses were used to irradiate the sample at an incident angle (
where,
Time-resolved movies of the SPP WPs were obtained by taking a sequence of fluorescent images while advancing
2.3 SPP WP propagation on a surface equipped with MIM-NC
Because the SPP WPs excited at the coupler replicated the temporal waveform of the light pulse, they initially had a frequency spectrum comparable to that of the light pulse and had the narrowest temporal duration corresponding to the transform limit. Then, the SPP WPs propagated along the surface to interact with the MIM-NC while the spatial width extended and the carrier frequency up-chirped owing to the dispersion relation of the SPPs at the sample surface (Figure 1(a)). The dispersion relation of SPP was determined by the refractive indices of materials that constructing the multi-layered sample structure (see Supplementary Figure S5 for derivations of dispersion curves). This system is similar to a system consisting of an optical cavity coupled with a waveguide [59], [60], [61]. When the SPP WPs reached the MIM-NC, the wave components whose frequencies coincided with the eigenenergy of the cavity were coupled to the eigenmode. Consequently, a large part of the energy of the SPP WP was squeezed into the thin insulator layer of the MIM-NC and the intensity of the field inside the cavity was enhanced. After a propagation through the MIM-NC at a slowed group velocity corresponding to the MIM waveguiding mode, the SPP WP was released from the other end of the MIM-NC [62]. This process constituted a spectrally filtered transmission of an SPP WP through an MIM-NC. Because of the normal-dispersion character of the SPP mode on the Au surface, SPP WP causes up-chirping and thus the head and tail regions of the WP reached to the MIM-NC possesses different carrier frequencies. Therefore, the spectral filtering by MIM-NC leads to a spatial deformation of the SPP WP. Our previous FDTD studies have suggested that if an SPP WP is chirped, the transmitted SPP WP will exhibit a shift (
The transmittance spectra of an SPP through an MIM-NC were evaluated using the FDTD method for the cavity length (L) range of 10–400 nm and are plotted in Figure 1(c) together with the first- to fourth-order eigenmodes of the MIM-NC (open circles) (see Supplementary Figure S1 for details) [36]. Overall, the transmittance spectra followed the trends of the eigenmodes of the cavity. More specifically, the spectra exhibited asymmetric line shapes, with the peak energy being slightly shifted from the eigenmodes. These features are interpreted as the Fano-resonance line shape that arose as a consequence of the interference between the discretized eigenmodes of the MIM-NC and the continuous SPP mode on the surface of the MIM nanoblock structure [63], [64], [65], [66]. While the transmittance reached considerably large values (∼0.5) at the peaks, it decreased considerably (∼0.1) for L ≈ 100 nm, corresponding to a valley between the first- and second-order resonances.
3 Results
3.1 Deformation of SPP WP by transmission through MIM-NC
Figure 2(a) shows a frame of the time-resolved fluorescence movie taken for a pump–probe delay time of
where
The SPP WP launched from the coupler underwent a resonant interaction with an MIM-NC, passed through it, and continued to propagate on the metal surface at the far side of the cavity. The deformed spatial shapes of the SPP WPs were determined by analyzing the beat patterns in this area. For detail examination of the SPP WP, the oscillatory waveform constructed by the pump–probe interference was extracted by the following method: The constant phase of the pump-probe interference beat moves by
This procedure practically works well because the change in the special envelope of the pump-probe beat during an increment of
In this study, we minimized the number
where,
As similar to
Figure 2(b)–(d) shows the differential images taken at
The variations in the spatial deformations of the SPP WPs were closely related to the levels of the eigenenergies of the MIM-NC, which sensitively changed as a function of L. The MIM-NC was a plasmonic Fabry–Pérot resonator constructed by cutting an MIM plasmonic waveguide to a length that was approximately equal to multiple halves of the SPP wavelength in the MIM, i.e.,
3.2 Sequence of time-resolved movie frames of SPP WP
The spatial shifts in the intensity peaks of the SPP WPs were further investigated by examining a sequence of time-resolved images from the TR-2PFM movie. Figure 3(a) shows selected frames from the movie for
4 Discussion
4.1 Modeling of WP deformation through resonant interaction with MIM-NC
The TR-2PFM imaging of SPP WPs revealed how the waveform and intensity of the transmitted SPP WP changed significantly according to the overlap between the spectrum of the WP and the eigenenergy of the MIM-NC. When the eigenenergy was detuned from the center of the spectral distribution, the transmitted WP showed a shift in the peak intensity position compared to the case continuing the propagation on a flat surface. This result is qualitatively consistent with the recent FDTD simulation [36] and another time-resolved measurement study of SPP wave scattering by a nanohole [67]. The waveform deformation and peak shift observed in a transmitted SPP WP are attributed to the clipping of a chirped SPP WP in the temporal-frequency domain induced by an MIM-NC. Because of the normally dispersed character of the SPP mode, the instantaneous carrier frequency of an SPP WP gradually becomes up-chirped during propagation on an Au surface. Whereas the intensity peak continuously propagates at a group velocity
To obtain more detailed insights into the deformation of the WPs, model calculations were performed based on the CD relations of SPPs (CD model; see Supplementary Figures S2 and S3 for formulations and Movie 2 for simulated time-resolved movie.) [51, 52]. In this model, the temporal waveform of an SPP WP at position x,
The
Here,
The CDs of the SPP modes for the PMMA/Al2O3/Au surface and Au/Al2O3/Au waveguiding structure were independently prepared (see Supplementary Figure S5 for derivations of the CDs). The resonant interactions of the SPP WPs with the MIM-NCs were modeled by considering (1) the resonant and/or off-resonant excitations of the multiple eigenmodes of the MIM-NC associated with a phase shift in the SPP WP determined as the sum of the responses to each of the eigenmodes (1st–5th order), (2) phase accumulations in
The waveform of
The intensity of the emission of fluorescence induced through two-photon excitations was evaluated by substituting Eqs. (10) and (11) to Eq. (1).
As mentioned above, beat patterns in micrographs comprised of the pomp-probe interferences imitated the spatial shapes of SPP WPs, although the spatial widths of the envelopes were widened than that of the actual SPP WPs. This broadening happens because the excitation light was incident at an oblique angle. For the same reason, an actual spatial separation (
For the experimental condition used here, Eq. (12) provides a relation
Figure 4(a) and (b) shows the beat patterns calculated by the CD model for the reference plane and the cavity plane containing an MIM-NC with
As shown in Figure 4(e) and (f), the CD-model-calculated peak shifts (
Because the coherence lifetimes of MIM-NCs are limited to several femtoseconds, MIM-NCs possess wide linewidths and behave as low-finesse Fabry–Pérot etalons. SPP WPs sustain spectral widths that are sufficiently wide to form a WP with femtosecond time durations even after transmission through an MIM-NC. As shown in Figure 4(b) and (c), the spectral clippings by MIM-NCs did not elongate the width of the WPs or induce complicated phase retardations in the WPs. Rather, the width of the SPP WPs could be narrowed by transmission through an MIM-NC if the incident WP had a large chirp. The slow group velocity of the MIM waveguiding mode compared to that of the SPP on the metal surface induced a retardation of the SPP WP, but the retardation was only marginal; for the MIM-NC with L = 160 nm, the retardation effect was estimated to be only
4.2 External control of peak shift of WP using chirped light pulse
The control of the peak shifts of the transmitted SPP WPs can be regarded as an application of spatiotemporal coupling (STC) [25, 26]. In the abovementioned case, the STC was simply an up-chirping of the carrier wave of an SPP WP that possessed longer (shorter) wavelengths in the head (tail) region. The intensity peaks of the SPP WPs were controlled by tuning the eigenenergy of the MIM-NC such that a portion of the carrier wave was clipped, with the instantaneous frequency matching the eigenenergy. Here, another strategy for controlling the peak shifts is discussed wherein the chirp applied to the excitation light pulses is externally controlled. CD model calculations were performed to estimate the amount of shift
In conducting the CD model calculations, we assumed fused silica glass as the material [69]. The length of the MIM-NC was assumed to be L = 140 nm; the MIM-NC had a second-order resonance at 1.7 eV and was placed at
It may be useful to mention that the spatial peak shift of SPP WP would arise an apparent anomalous group velocity of the WP in MIM-NC. In MIM waveguides, SPP waves propagate at their intrinsic group velocity defined by the first derivative of the dispersion curve of the waveguiding mode as
5 Conclusions
In this study, the spatiotemporal dynamics of an SPP WP interacting with an MIM-NC possessing discretized eigenenergies near the spectral distribution range of the WP were investigated using time-resolved microscopy and numerical calculations. The spatial shape and the motion of an SPP WP launched on an Au surface by an irradiation of 10 fs, 810 nm laser pulse were imaged with 10 fs-temporal and 0.5 μm spatial resolutions. A small portion of the energy of surface electromagnetic fields was up-converted to fluorescence emissions through two-photon excitations of a thin dye-doped PMMA layer coated on the surface. Time-resolved two-photon fluorescence microscopy (TR-2PFM) revealed spatial shifts in the peak position of the WP after it passed through the MIM-NC. The transmittance spectra of an SPP WP passing through an MIM-NC were analyzed by FDTD simulations and the waveforms and spectra of the SPP WP were calculated by the CD model. The analysis results showed that the peak shifts were induced by the spatiotemporal clipping of a chirped SPP WP caused by the MIM-NC. The peak shift can be controlled to within several micrometers in either the positive or the negative direction by adjusting the eigenenergy of the MIM-NC or the chirp of an excitation pulse. The controllability of the SPP WP demonstrated here is expected to provide useful insights into the development of novel optical devices based on the complex control of light waves using optical nanostructures.
6 Methods
6.1 Sample fabrication
The sample was prepared as follows. First, an Au layer with a thickness of 100 nm and a subsequent sapphire (Al2O3) layer with a thickness of 16 nm were deposited on a silicon wafer (Si(100)) covered with a native oxide layer via sputtering and atomic layer deposition. Next, rectangular Au blocks with a transverse length of 30 μm, a thickness of 100 nm, and a longitudinal length (L) ranging from 50 nm to 220 nm were placed on the Al2O3/Au film using standard electron beam lithography and thermal evaporation methods. The entire area of the sample was coated with dye (coumarin 343)-doped poly(methyl methacrylate) (PMMA) using a standard spin-coating technique. The thickness of the PMMA layer was determined using a spectroscopic ellipsometer. To prevent unintentional loss of fluorescence intensity due to the bleaching of dye molecules, the dye-doped PMMA layer was occasionally recoated throughout the experiment. The thickness of the PMMA layers was 50 nm for the experiments shown in Figures 2 and 4 and Supplementary Movie 1, and 60 nm for Figure 3. The uncertainty of the thickness was 5 nm, including the nonuniformity of the film. The difference of 5 nm in the film thickness resulted in a difference of approximately 0.1 × 108 m/s in the group velocity of the SPPs under the experimental conditions used in the study.
Funding source: Japan Society for the Promotion of Science
Award Identifier / Grant number: JP14459290
Award Identifier / Grant number: JP16823280
Award Identifier / Grant number: JP18967972
Award Identifier / Grant number: JP20J21825
Funding source: Ministry of Education, Culture, Sports, Science and Technology
Award Identifier / Grant number: Q-LEAP ATTO
Funding source: Core Research for Evolutional Science and Technology
Award Identifier / Grant number: JPMJCR14F1
Funding source: National Institute for Materials Science
Award Identifier / Grant number: JPMXP09F-17-NM-0068
Acknowledgement
The authors thank H. T. Miyazaki and T. Kasaya for their advice, valuable discussions, and critical contributions with regard to sample fabrication. The authors also thank H. Petek for critical reading of manuscript.
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Author contribution: N.I. performed the experiments, simulations, model calculations, and wrote the draft of the manuscript; Y.O. performed the sample fabrication and developed the calculation model; A.K. conceived the experiment, supervised its execution, and finalized the manuscript.
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Research funding: This work was supported by NIMS Nanofabrication Platform in Nanotechnology Platform Project, (JPMXP09F-17-NM-0068), the JSPS KAKENHI (JP14459290, JP16823280, JP18967972, JP20J21825), JST CREST (JPMJCR14F1), and MEXT Q-LEAP ATTO (JPMXS0118068681), Japan. This study was supported by the Nanofabrication Platform of the National Institute for Materials Science and the University of Tsukuba.
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Conflict of interest statement: The authors declare no conflicts of interest regarding this article.
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