Van der Waals materials in the form of thin sheets (1-50 nm) or single atomic layers have received a great deal of attention as a light source due to their unique mechanical, electronic and optical properties [1][2][3][4]. Particularly, their ability to conform and integrate with other material systems offer unprecedented control over their electronic and optical response [5][6][7][8]. Additionally, these material systems exhibit intriguing quantum phenomena both at the macro scale (e.g. room temperature quantum Hall effect [9], condensates [10], and superconductivity [11]) and at the nanoscale (e.g. single photon emission from color centers [12,13], and excitons [14][15][16][17]). These features have given the scientific community new ways to explore quantum phenomena while setting the stage for novel devices.
From among the many van der Waals systems presently attracting attention, in this study, we focus on hexagonal boron nitride (hBN), a semiconductor featuring a wide band gap (of approximately 6 eV [18]) and high thermal conductivity [19]. This material can be used in a wide range of applications, from catalysis [20] to electronics (e.g. as a component for atomically-thin heterostructures [21,22]). Its crystal lattice is isomorphic to graphene, with boron and nitrogen forming the basic elements for a honeycomb structure [23]. Recently, hBN was identified as the host of room temperature single photon emitters (SPE) associated with point defects in its crystal lattice. These SPEs possess properties that are needed in a single photon source (SPS), including high excitation and out-coupling efficiency, photon purity and a low Debye-Waller factor [12]. While the exact nature of the defects remains unclear, the low material cost, room temperature operation, high photon count rates, spectral tunability and narrow linewidth make these emitters highly attractive for quantum technologies [24][25][26][27][28][29][30][31].
Recent studies have shown that hBN grown via chemical vapor deposition (CVD) can contain a high density of point defects that can be "activated" (i.e. transformed into a fluorescent state) either by thermal annealing or substrate-engineering [32,33]. In this latter case, the emitter position (and, to some extent, the areal concentration [34]) can be controlled, thus providing opportunities for integration with photonic structures [35,36].
Processing information with quantum emitters requires scalable methods for deterministically placing these emitters in integrated photonic circuits and subsequently coupling to structures that can direct, amplify, and potentially modulate the emitted photons. On the one hand, small ensembles of independent emitters coupled to a cavity have recently gained attention with an eye on applications in quantum memory storage and its ability to act as entangled systems [37,38]. On the other hand, photonic structures, such as plasmonic surface lattice resonances (SLRs) supporting delocalized or propagating modes, provide one attractive route to establishing long-range interactions between electronically independent emitters so as to control emission directionality and intensity. The coupling of emitters to this class of photonic systems has recently attracted research attention due to its potential as tunable light sources and for compact lasing applications [39][40][41][42][43][44][45].
In this report, we focus on engineering the emission properties of room temperature SPSs in hBN by combining deterministic emitter activation and coupling to an optically active substrate. This is achieved by placing 20 nm-thick hBN flakes on silver nanopillar arrays that support the SLRs. Capitalizing on the unique mechanical properties of the 2D materials, we activate the quantum emitters located in a target area by suitably shaping the underlying substrate [7,8,32], and subsequently engineering their emissions both directionally and spectrally with the aid of array-supported SLR modes [39]. While the exact mechanism by which the hBN emitters are activated has not been currently isolated, a likely candidate is the strain caused by the folding of the hBN around the nanopillars, which in turn, would lead the emitter into a bright radiative state [7,8,32,46]. The number of emitters can be controlled via the size of the activated area and the intrinsic defect density [33].
In our experiments, we start with the fabrication of arrays of silver nanopillars via e-beam lithography. To this end, a PMMA film (positive resist) was patterned onto a glass substrate to produce regular, square arrays of cylindrical holes of variable diameter and separation (pitch). Then, a 100 nm layer of Ag was deposited on the patterned PMMA film via electron beam evaporation. Afterwards, a lift-off process was used to remove the Ag-coated PMMA via acetone, leaving behind arrays of silver nanopillars with different diameters and inter-site separations. Subsequently, a 10 nm conformal coating of alumina was deposited on the sample in order to passivate the Ag structure as well as to provide the spacing required to prevent silver-induced emitter quenching.
To study the interaction between the hBN emission and the plasmonic arrays, we fabricated pillar structures with pitches varying from 220 nm to 2000 nm and with pillar diameters from 50 nm to 400 nm for each pitch. Generally, pillar arrays with a pillar-to-pillar spacing of less than 100 nm were found to fuse together, hence imposing a practical limit in the type of systems we could probe. Each array was 50 × 50 μm 2 in size, large enough to allow for a collective SLR mode while still compatible with the optical inspection.
The hBN used in the experiment was a CVD-grown 20 nm-thick film that was commercially available from Graphene Supermarket. The hBN flake had an approximate size of 5 × 5 mm 2 , large enough to cover the entire patterned area with a continuous film. The hBN was deposited on the Ag pillar substrate via a wet transfer protocol described in Ref. [32].
In order to obtain angle-resolved spectra in Figures 1 and4, the Fourier image of the sample was projected onto the spectrometer slit (Princeton Instruments SpectraPro HR 750). The white light was focused on the array through the excitation objective (Exc. Obj.) and the transmitted light or PL was collected by the collection objective (Coll. Obj.) The collimated transmitted light was then focused by a tube lens (TL) to form a real image plane (IP) that was one focal distance away from the Bertrand lens (BL), which forms an image of the collection objective's back focal plane at the spectrometer slit (Det.) [47]. In this configuration, the spectrometer captures the Fourier image of the Ag pillar array, where the linear polarizer (Pol.) is used to resolve the p-and s-polarizations. For the angle-resolved transmission spectra, the sample was illuminated via a tungsten lamp (Olympus) with a 0.6 NA long-working-distance objective (Olympus SLMPLN100x). For the photoluminescence spectra in Figure 4, a beam size of ~40 μm was used to excite the majority of the pillars in a given array.
Photoluminescence (PL) spectra were collected via a high numerical aperture (.83 NA) objective (Olympus). The confocal PL experiments in Figure 3 were performed with a custom-built confocal microscope. A piezo nanostage was used to raster scan the sample across a fixed laser and collection path. The focused spot size had a diameter of ~1 μm and the collection spot was ~400 nm. The PL in Figure 3B was excited via a 510 nm, 500 fs pulsed fiber laser with a repetition rate of 80 MHz (Toptica FemtoFiber pro TVIS). The PL for the rest of the experiment was excited via a 460 nm CW diode laser.
SLRs are hybrid plasmonic diffractive modes found in one-and two-dimensional periodic arrays of plasmonic 345 nm and a pillar diameter of 150 nm. As seen from the SEM image, the pillars are slightly tapered at the top. This change in diameter can lead to broadening of the LSPR mode as it depends highly on the pillar cross section [39]. The hybridized SLR modes occur at wavelengths slightly red-shifted from the wavelengths of the RAs (the high transmittance lines crossing at ~510 nm in Figure 1C). The SLR is seen in the dispersive extinction feature from 575 nm to 700 nm. The SLR in Figure 1C probed with a broadband white source has a Fano-resonance line shape due to the interference between the scattered light from the SLR mode and the directly transmitted broadband light [49]. The relevant modes here are the so-called "out-of-plane SLRs" that correspond to the LSPRs predominantly localized near the upper and lower ends of the pillars [50,51].
For the geometry in Figure 1A, the non-dispersive LSPR mode for the 150 nm pillars, shown in Figure 1B, splits into two branches. The branch outside the 510 nm RA has two symmetrical lobes occurring between 500 nm and 560 nm centered at the original LSPR mode (indicated by the gray dotted lines in Figure 1C). These two lobes correspond to the SLR produced by the coupling of the Ag pillar LPSR to the higher energy (0, ±1) air RAs (red dotted lines). The lower energy (0, ±1) glass RA modes (white dotted lines) couple to the LSPR such that the resulting SLR (black dotted line) is continuous across normal incidence and follows the dispersion of the RA angles with gradually decreasing linewidths at larger angles. This is the typical behavior of SLRs [50]. Moreover, the quality of the mode increases at larger angles as these modes are longer lived when they become less localized at the individual Ag pillars.
The bright field microscope images of the Ag pillars arrays in Figure 2 allow us to compare the SLR's optical properties before and after hBN transfer. Aside from a ~20 nm red shift of the modes (expected from the higher index of the hBN film) and a slight decrease in the resonance quality, we find the SLRs were largely unaffected by the hBN film and retained all its core features. We fabricated Ag arrays with variable pitch and pillar diameter as seen in Figure 2A andB. This allowed us to study a large variety of SLR resonances as the hBN color centers occur across most of the visible spectrum, centered at ~570 nm [32,52]. The 345 nm-pitch, 150 nm-pillar-diameter array was found to have the highest emission contrast on and off the SLR. Figure 2E shows a confocal scan of the observed PL. The hBN shows preferential emission when on the pillar array regions, while in the partially torn regions (seen in Figure 2D) the PL intensity was drastically reduced, indicating that the hBN was the source of the observed PL.
Figure 3 displays the emission characteristics of these hybrid hBN/Ag arrays. The hBN-induced photoluminescence from isolated plasmonic particles was highly localized to individual pillars, as seen in the upper quadrants of Figure 3A andB. These arrays have a 2 μm spacing and do not support collective SLRs. The pillar locations of all four arrays are clearly identifiable in the bright field image of Figure 3A. At each pillar site, we can probe individual (or few) emitters as the pillar diameter is made sufficiently small [32]. For illustration purposes, Figure 3D shows a spectrum for a 100 nm-diameter pillar with 2 or less defects (g (2) (0) < 0.54 ± 0.04). The g (2) (0) was determined from the autocorrelation data in the inset of Figure 3D by taking the ratio between the area under the coincidence peak at t = 0 and the average area of 10 t ≠ 0 peaks. The area was determined by fitting each peak with a Lorentzian function [30]. Arrays that support SLRs (lower quadrants in Figure 3A) become collectively bright as seen in the confocal image of Figure 3B. As the pitch decreases, emitters get closer to each other and the collected fluorescence contains contributions from several defects. The latter leads to a broad dynamical emission across most of the visible spectrum (line cut in Figure 3C) with emitters blinking intermittently on a timescale of seconds (contour plot in Figure 3C).
To study the interplay between the emitter fluorescence and the SLRs, we look at the optical characteristics of the hBN-covered array already characterized in Figure 1. Aside from the slight changes pointed out above, the optical transmission spectrum in Figure 4A shows that the modes remain largely unaltered. By contrast, the blue laser excitation of the entire array (40 μm spot size) shows that the hBN emission is drastically modified via coupling into the SLR modes (Figure 4B). In particular, we observed that the PL becomes highly directional, largely mirroring the RA-induced SLR dispersion at high angles [39]. Moreover, the emission spectral band is extended by the SLR mode into the deep red, where the intensity of the defect emission is otherwise an order of magnitude weaker (red spectra of Figure 3C). These findings demonstrate good coupling between the defect center emission and the SLR modes. In the absence of an SLR mode (Figure 4C), the hBN emission shows no dispersion. This contrast with Figure 4B confirms that the dispersion of the hBN emission in Figure 4B is derived from the coupling of the hBN emitters to the SLR mode, which is supported by the 345 nm pitch Ag nanopillar array.
In summary, we presented a method for engineering room temperature quantum emission in a scalable platform where the emitters are activated at the array sites via Brought to you by | CCNY City College of New York Library Authenticated Download Date | 9/18/19 3:11 PM substrate engineering. For suitable array parameters, the defect emission couples to the optically active plasmonic substrate and undergoes a modification in its directionality and spectral intensity. The coupling of emitter systems with photonic structures that support delocalized or propagating modes permits the mutual interaction between these distinct and spatially separated color centers. Such structures could facilitate long range energy transfer between individual emitters. Future works could focus on controlling the number of emitters coupling to the SLR mode via the size of the active region; this can be done by considering the number of intrinsic defects present in the material or by conducting spectral filtering [33].