Temperature and Magnetic Field Effects on the Transport Controlled Charge State of a Single Quantum Dot
© The Author(s) 2010
Received: 25 March 2010
Accepted: 17 April 2010
Published: 5 May 2010
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© The Author(s) 2010
Received: 25 March 2010
Accepted: 17 April 2010
Published: 5 May 2010
Individual InAs/GaAs quantum dots are studied by micro-photoluminescence. By varying the strength of an applied external magnetic field and/or the temperature, it is demonstrated that the charge state of a single quantum dot can be tuned. This tuning effect is shown to be related to the in-plane electron and hole transport, prior to capture into the quantum dot, since the photo-excited carriers are primarily generated in the barrier.
Self-assembled semiconductor quantum dots (QDs) have attracted considerable attention within the nanostructure research field in recent years due to their possible optical and optoelectronic applications [1–3]. The discrete energy levels in QDs also open up novel possibilities for studies of the physics in a zero-dimensional system. The most common technique to fabricate QDs is by Stranski–Krastanow (SK) self-assembly, which is based on heteroepitaxy. The mismatch in lattice constant between the substrate material and the epitaxial material results in a highly strained layer. After growing a critical thickness, a two-dimensional continuous wetting layer (WL) can be transformed into the zero-dimensional QDs. For multiple purposes of QD structures, from integration into a sophisticated optoelectronic device to studies of fundamental properties of QDs, it is of utmost importance to understand the interaction between the QD and the WL and the surrounding matrix in which they are embedded. The reason for this is that the electrons and/or holes are normally not both generated in and extracted from the intrinsic QD states. On the contrary, the carriers are either supplied from the matrix by an external current to recombine in the QD, as in a laser or light emitting diode application, or alternatively the carriers are excited by light absorption in the QD, to give rise to an external current in the matrix/WL, as in a photo-detector or photovoltaic application. In all these cases, the carriers will be transported to or from the intrinsic QD region, via the surrounding material. For example, in structures fabricated by the SK growth mode, the QDs will coexist with the remains of the WL and it has been demonstrated by several groups that the interaction between the QD and WL states will have a significant impact on the QD characteristics [4–12]. For example, the modulation rate of a QD laser is limited by the thermal emission of carriers from the QD into the WL in differential transmission spectroscopy measurements [4, 5], and the threshold current in QD lasers was shown to significantly depend on the carrier capture mechanisms . The non-zero absorption at photo-excitation far below the WL was attributed to crossed transitions, involving one bound QD state and one delocalized WL state . The localized states of the rough WL acting as intermediate states was proposed as an explanation to the observed PL up-conversion, seen in single InAs/GaAs QDs . In our previous works, the carrier capture mechanisms into the QD via the WL were studied in the presence of a lateral electric field , an external magnetic field  and with an additional infrared (IR) laser excitation  as well as by means of temperature dependent PL .
In the current study, the transport of photo-excited carriers in the WL has been explored by micro-photoluminescence (μPL) spectroscopy of an individual QD. The combined dependence of the μPL characteristics on temperature and on the magnitude and direction of an external magnetic field has been investigated. Special attention has also been focused on the μPL of the WL itself. Our observations show that the QD charge configuration can be effectively tuned if one can control the carrier transport in the WL, in the vicinity of the QD. This carrier transport is discussed and explained within a simple model of the QD structure energy diagram.
The sample studied consists of InAs QDs grown on GaAs with Molecular Beam Epitaxy (MBE). The QDs were formed from a 1.7 monolayers thick InAs layer deposited at 530°C. A first growth interruption of 30 s was used to improve the size distribution, whereupon the QDs were covered with a thin GaAs cap layer with a thickness of 3 nm before a second growth interruption of 30 s. Finally, a 100-nm-thick GaAs layer was deposited to protect the QDs. The QDs developed in this process are lens-shaped with a height and diameter of 4.5 and 35 nm, respectively. No rotation of the substrate was used during growth, resulting in a gradient of the density of QDs across the sample. In our present investigation, a piece of the sample with a low QD density has been used for the μPL experiments where the average distance between QDs is more than 10 μm. This allows direct optical access to an individual QD without arranging apertures or mesas, which would restrict the area of the sample excited by the laser. The sample was mounted on the cold finger of a continuous-flow cryostat, which allows control of the temperature in the range from 3.8 K up to room temperature. A magnetic field could be applied either perpendicular (Faraday geometry) or parallel (Voigt geometry) to the sample surface, while the laser beam was kept at perpendicular incidence to the sample surface. A laser beam from a tunable Ti:Sp laser pumped by a solid state laser was focused to a spot diameter of 2 μm onto the sample surface with a microscope objective, hence only one QD is present within the laser spot. The resulting luminescence is collected through the same objective and mirrored into a monochromator equipped with a liquid nitrogen–cooled CCD, allowing a spectral resolution of around 0.1 meV.
As an external magnetic field, B = 5 T, is applied perpendicular to the sample, i.e. in Faraday geometry, the rate at which the WL PL intensity decreases with T is reduced in the range between 10 and 40 K (Fig. 1a). This observation is attributed to a magnetic field–induced quantization of the carrier motion, which enhances their possibility to remain longer in the WL than is the case at B = 0. To verify this explanation, the probability for carrier localization at a 5 T-field was evaluated. For this evaluation of the carrier localization due to an applied magnetic field, the conventional localization criterion, based on a comparison of the product with unity , is employed. Here, is the cyclotron frequency, is the scattering time for electrons (holes), e is the elementary charge, and is the effective mass for electrons (holes), taken as = 0.067 m 0 and = 0.5 m 0, respectively . We find that = 8.9 and = 0.29 at B = 5 T , which indicates that the electron transport is severely inhibited by the B-field (meaning that the electrons start forming cyclotron orbits in between scattering events), while the hole motion is essentially unaffected at B = 5 T. Thus, the difference between the WL PL behavior at B = 0 and 5 T (Fig. 1a) is explained in terms of a decreasing electron migration with increasing B-field, leading to an enhanced luminescence in the WL. At T > 90 K, no luminescence is monitored from either the WL or the QD, which is commonly attributed to an enhanced non-radiative recombination rate with increasing temperature .
The most striking observation in Fig. 2a is the intensity redistribution between the spectral lines with increasing B-field. At B = 0, the μPL spectrum is dominated by the X 2− emission, but its intensity decreases with increasing B-field at the expense of the appearing X 1− and X 0 lines. The redistribution of the exciton lines (Fig. 2a) indicates a B-field-induced “neutralization” of the QD charge state. In contrast, when the magnetic field is applied in Voigt geometry (Fig. 2b), no corresponding redistribution effect is observed and the QD is dominated by the X 2− emission at any B-field strength in the range employed, 0–5 T. This observation gives additional support for the quantized in-plane electron transport in the presence of a B-field in Faraday geometry, while a B-field in Voigt geometry, i.e. parallel to the transport, is unable to induce such a quantization. Additional studies have shown that for photo-excitation energy below the WL band gap energy, i.e. when no carrier transport takes place prior to capture into the QD, the redistribution effect vanishes .
At this point, it is interesting to consider the process that generally governs the in-plane carrier transport in a QD sample. It has been established, by us as well as by others, that there is a built-in electric field (F) attributed to ionized impurities, with a component directed in the QD plane (see [9, 10] and references therein). The magnitude of the electric field will differ between different QDs, but can, to some extent, be controlled either by an additional IR laser excitation or by applying a lateral bias , resulting in significant effects on the carrier transport in both cases. For the specific QD studied here, an internal field of F = 500 V/cm has been estimated . Hence, in the present study with an applied B-field, the carriers are migrating in a crossed electric and magnetic field and will consequently exhibit a motion with the drift velocity V dr = F/B directed perpendicular to both fields . An increased B-field will consequently lead to a decrease in V dr, as experimentally observed.
I PL is the integrated intensity of the X 0, X 1− and X 2−-peaks, respectively. The temperature dependence of N e at B = 0 and 5 T was measured and is given in Fig. 4. At B = 0, N e initially increases with temperature from N e ≈ 1.7 at T = 4 K to N e ≈ 2.1 at T = 10 K. On the other hand, at B = 5 T, N e ≈ 0.2 is monitored at 4 K and increases to N e ≈ 1.3 at T = 30 K. The initial increase in N e with increasing temperature in these cases is attributed to thermally activated escape of electrons out of the WL localizing potentials and suggests that the corresponding ionization energy for electrons is smaller than for holes, which is reasonable considering that the holes are ~7 times heavier than the electrons . At T > 40 K, N e is seen to decrease and to stabilize at N e ≈ 1, i.e. with two electrons occupying the QD ground state, independent of the B-field. The inset in Fig. 4 shows the calculated ratio between N e at B = 0 and 5 T, respectively, in the studied temperature range. This ratio goes toward 1 with increasing temperature, as the effect of the B-field vanishes. These results combined with the results presented in Fig. 1a indicate that the QD population dynamics at T > 60 K is primarily not determined by the transport in the barrier/WL interface, but is instead attributed to thermally assisted escape of carriers out of the discrete QD states. Specifically, for N e = 1 at T > 60 K, the escape of holes is proposed to be the reason for the observed extra electron in the QD and a decreasing QD PL intensity.
A model for the transport of photo-excited carriers in the WL plane of a QD structure was proposed and tested by exerting the structure to elevated temperatures and external magnetic fields of varying strength and direction. Localizing potentials for the carriers in the WL were shown to play a crucial role for the behavior of the QD PL. It was demonstrated that a magnetic field enhances the capture into these localizing potentials, whereas an increased temperature enhances the thermally assisted escape out of these potentials. By applying an external magnetic field in Faraday geometry, in contrast to Voigt geometry, the electron migration toward the QD is decreased. Elevated temperatures will increase the electron migration toward the QD. Hence, a temperature and magnetic field–induced charging control of an individual QD was achieved.
The authors would like to thank P. M. Petroff and W. V. Schoenfeld for providing the sample. This work was supported by grants from the Swedish Research Council (VR) and the Swedish Foundation for Strategic Research (SSF) funded Nanopto consortium.
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