- NANO EXPRESS
- Open Access
Droplet etching of deep nanoholes for filling with self-aligned complex quantum structures
© Küster et al. 2016
- Received: 13 April 2016
- Accepted: 23 May 2016
- Published: 3 June 2016
Strain-free epitaxial quantum dots (QDs) are fabricated by a combination of Al local droplet etching (LDE) of nanoholes in AlGaAs surfaces and subsequent hole filling with GaAs. The whole process is performed in a conventional molecular beam epitaxy (MBE) chamber. Autocorrelation measurements establish single-photon emission from LDE QDs with a very small correlation function g (2)(0)≃ 0.01 of the exciton emission. Here, we focus on the influence of the initial hole depth on the QD optical properties with the goal to create deep holes suited for filling with more complex nanostructures like quantum dot molecules (QDM). The depth of droplet etched nanoholes is controlled by the droplet material coverage and the process temperature, where a higher coverage or temperature yields deeper holes. The requirements of high quantum dot uniformity and narrow luminescence linewidth, which are often found in applications, set limits to the process temperature. At high temperatures, the hole depths become inhomogeneous and the linewidth rapidly increases beyond 640 °C. With the present process technique, we identify an upper limit of 40-nm hole depth if the linewidth has to remain below 100 μeV. Furthermore, we study the exciton fine-structure splitting which is increased from 4.6 μeV in 15-nm-deep to 7.9 μeV in 35-nm-deep holes. As an example for the functionalization of deep nanoholes, self-aligned vertically stacked GaAs QD pairs are fabricated by filling of holes with 35 nm depth. Exciton peaks from stacked dots show linewidths below 100 μeV which is close to that from single QDs.
- Droplet etching
- Quantum dot
We fill the nanoholes with GaAs to fabricate strain-free quantum dots (QDs) . These QDs exhibit controlled and uniform size , clear excitonic features , and small excitonic fine-structure splitting . So far, shallow nanoholes with depth of 10 to 15 nm are used as template for fabrication of QDs with narrow optical linewidth.
Recently, LDE of nanoholes with depth above 100 nm was demonstrated  by increasing the droplet material coverage θ and process temperature T. Such deep holes would allow the self-aligned fabrication of more complex coupled quantum structures stacked into a single hole. A prominent example are quantum dot molecules (QDM) where the nanoholes can be filled with two QDs separated by a tunnel barrier. QDMs are interesting, e.g., for studies of the tunnel coupling between quantum objects [11–15]. A further interesting example are hybrids composed of a single QD and a metallic nanostructure, which allow to study near-field radiative coupling between single-photon emitters and plasmonic modes [16, 17]. Here, nanoholes can be filled with a QD, a thin cap layer, and a metallic nanostructure.
As a precondition for the above functionalizations, the QD optical quality must be maintained also for filling of deep droplet-etched nanoholes. In a previous approach for deep nanohole creation, an optimized As background pressure of about 8 ×10−7 Torr, a droplet material coverage θ = 3.2 ML (monolayers), and a process temperature T = 620 °C were used. Nanoholes with 20–30 nm depth have been created  which is already sufficient for QDM fabrication. However, single QDs or stacked QD pairs filled into these nanoholes turned out to have very broad excitonic linewidth of several meV, i.e., more than one order of magnitude broader compared to QDs created in shallow holes . Therefore, we study here different fabrication conditions with As pressure below 10−7 Torr and varied θ (1.0 Ml ≤θ≤ 2.4 Ml) as well as temperature T (600 °C ≤T≤ 690 °C). As a key result, we demonstrate the fabrication of single and vertically stacked QDs with linewidth below 100 μeV using 35 nm deep LDE nanoholes as template.
A schematic of a LDE process is sketched in Fig. 1. All samples are created on (001) GaAs wafers using solid source MBE. After growth of a 120 nm thick Al x Ga1−x As (x = 0.33) buffer layer, 1.0 ML up to 2.4 ML Al are deposited (Fig. 1 a) at strongly reduced As pressure F As < 10 −7 Torr and a process temperature varied from 600 up to 690 °C. The As pressure is at least hundred times smaller compared to typical MBE growth condition for planar GaAs or AlGaAs. The Al deposition results in the formation of low-density Al droplets (Fig. 1 a) in Volmer-Weber growth mode . During a subsequent annealing time t of 180 s, the initial droplets transform (Fig. 1 b) into nanoholes surrounded by walls (Fig. 1 c, e). Central processes for nanohole etching are the diffusion of As from the substrate into the liquid droplet material, a resulting liquefaction of the substrate at the interface to the droplet , and the spreading of the droplet material over the substrate surface . An example of an AlGaAs surface with droplet etched nanoholes is shown in Fig. 1 d, e. The structural features of the nanoholes are characterised using atomic force microscopy (AFM) in tapping mode.
The basic optical characterization of single QDs is done with microphotoluminescence spectroscopy (PL) at liquid Helium temperature. Individual QDs are selected using a focused helium-neon laser (λ = 632.8 nm) or a green diode laser (λ = 532 nm) for excitation. A combination of grating spectrometer and liquid nitrogen cooled CCD is used to disperse and detect the luminescence signal. The resolution limit of this setup is about 40 μeV. The measurements of the exciton fine-structure splitting (FSS) were taken using a combined measurement and fitting procedure [22, 23]. A linear polarizer was placed at the entrance of the spectrometer, and linear polarization components were analyzed by rotating emitted light with a half waveplate installed before the polarizer. A set of measured exciton spectra were fitted by the Lorentzian function and the peak centers plotted as a function of a half-waveplate angles. The amplitude of the obtained sinusoid corresponds to the value of FSS.
Autocorrelation curve was measured using a standard Hanbury Brown and Twiss setup: exciton transition was filtered by the monochromator, split by a non-polarizing 50:50 beamsplitter and sent to two avalance photo diodes (APD) coupled to multimode fibers. One APD was used to start the photon counting module, the other, delayed, to stop: an obtained histogram of the measured time intervals is directly proportional to the second-order correlation
Quantum dots optical properties
For quantum dot fabrication, the LDE nanoholes are partially filled by deposition of a GaAs amount corresponding to a 0.5 nm thin GaAs layer on a plane (001) AlGaAs surface. For the present QDs, we determine heights of 5–7 nm by assuming that the part of the GaAs flux impinging on the area of the nanohole opening migrates downwards and fills up the hole starting from its bottom . In detail, the thickness of the GaAs filling layer and the hole opening diameter define the size of the GaAs QDs. The such determined height agrees with AFM measured profiles, where a large number of unfilled nanoholes is compared to holes after filling with QDs. Finally, the QDs are capped with 80 nm AlGaAs.
As the most important finding here, Fig. 5 c demonstrates that the requirement of small luminescence linewidth sets a further upper limit to the process temperature. For temperatures up to 640 °C, the single-dot PL spectra show a clear exciton (X) peak together with higher excitonic complexes at lower emission energy. An example is plotted in Fig. 5 d. The linewidth of the exciton peaks is 70–80 μeV in the temperature range of T = 600–640 °C. An only slight increase of the process temperature to 650 °C yields QDs with substantially different optical properties. Now, the single-dot PL spectra show a very broad peak with linewidth of several meV. A typical spectrum with such broad PL peak is shown in Fig. 5 e. We assume that the exciton and biexciton lines are strongly broadened and merge to one broad peak. From this broad peak, we cannot determine the linewidth of the individual excitonic lines. The linewidth is rather determined for the overall peak, marked as stars in Fig. 5 c. We note that this abrupt PL peak broadening is in contrast to the continuous behavior of the hole depth and ground-state energy (Fig. 5 a, b). Also, the shape of the nanoholes as recorded before GaAs deposition shows no significant changes between T = 630–660 °C (Fig. 2 b, c). So far, the reason for the PL peak broadening is not clear. We speculate that the abrupt peak broadening might be caused by a material decomposition at high process temperatures.
Figure 6c shows an example of a polarization angle-dependent measurement of the QD exciton emission energy. From a sinus-type fit, a neutral exciton FSS of 4.8 μeV is determined. In Fig. 6 d, e, the FSS from several type I and type II QDs are compared. For type I QDs, the data show a few QDs with FSS larger than 10 μeV and a bunching of FSS values around a mean value of 4.6 μeV. For type II dots, the FSS values are more widely spread with one QD having a large FSS of 53 μeV and a bunching around a mean FSS value of 7.9 μeV. The increasing FSS for the type II dots might be caused by a stronger asymmetry  of the deeper holes. These data suggests the present QDs for the field of quantum cryptography, where a small FSS is a key prerequisite for the generation of entangled photons [27, 28].
Vertically stacked quantum dots
A comparison of AlGaAs and AlAs tunnel barriers yields much smaller linewidth for samples with an AlAs barrier. QD pairs with AlGaAs tunnel barrier have typically a linewidth of several 100 μeV, whereas those with an AlAs barrier have linewidth below 100 μeV. As an example, a PL spectrum of a QD pair with AlAs barrier is plotted in Fig. 7. We can clearly separate emission peaks from the first (bottom) and the second (top) dots. The first QD has a ground-state emission at 1.585 eV which agrees with the emission energy of a single type II QD. The difference between p- and s-shell emission is 11.7 meV, which is much smaller than the energy separation of 68 meV between both QDs. Our identification is supported by the systematic behavior of the emission energies in samples prepared with different filling pulse numbers. If the filling of the first dot is kept constant and the filling of the second dot is increasing the high-energy luminescence lines shift to lower energy. The second dot emits at significantly higher energy 1.652 eV which is caused by the smaller extent in growth direction and the, thus, higher quantization energy. The energy difference between both dots can be adjusted by the respective nanohole filling levels. For both QDs, the exciton peaks have the highest energy, while multiexcitonic peaks are red-shifted. As most important point here, the FWHM of the excition lines are 90 and 70 μeV for the first and second dots, respectively. This indicates that QD pairs fabricated by filling of LDE nanoholes show no additional peak broadening in comparison to single QDs. Furthermore, the linewidths are sufficiently small for investigations of molecule-resonant states in such quantum dot molecules.
Additional experiments, not shown here, use a gate voltage for tuning the energy levels of a QD pair into resonance. The data exhibit anticrossings, which is a clear proof for tunnel coupling and the presence of molecule-resonant states.
With our results, we expand the possibilities of the local droplet etching method. So far, nanoholes with depth of 10–15 nm have been used as template for fabrication of QDs with narrow PL linewidth. This work demonstrates the generation of uniform QDs with narrow exciton peak linewidth below 100 μeV also in up to 40 nm depth holes. The deeper holes allows filling with more complex heterostructures like coupled quantum systems. As a first application of the deep droplet-etched nanoholes, self-aligned vertically stacked quantum dot pairs are successfully fabricated by hole filling. The quantum dot pairs establish exciton peaks with small linewidths of 70–90 μeV which is close to that from separated QDs. The narrow linewidths allow studies of molecule resonances in these systems. As an important advantage of the present method, the size of the individual QDs as well as the tunnel barrier thickness can be adjusted individually by the respective filling layer.
The authors would like to thank Sandra Schnüll for sample growth and the Deutsche Forschungsgemeinschaft for financial support via HA 2042/6-1 and GrK 1286 and Science Foundation Ireland under grants 12/RC/2276 and 10/IN.1/I3000.
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