Introduction

In modern magnetic memory bits, spin currents are driven through vertical stacks from a magnetic polarizer via a non-magnetic spacer into a recording magnet to facilitate reading and writing of the information1. Spin conservation across the spacer is an essential prerequisite for these functionalities. Recent discoveries showed that a non-magnetic layer alone can be turned into an efficient injector of the spin-current to the adjacent magnetic layer by relativistic electrical transport means, namely by the spin Hall effect2. Here the spin-conserving length-scale defines the active width of the non-magnetic layer from which the spin-current can reach the interface with the magnet. The characteristic spin-transport lengths in these vertical spin-transport devices are often limited to nanoscale by scattering from magnetic impurities or by strong spin-orbit coupling.

The limitation to nanoscale lengths can be afforded in the vertical devices comprising thin-film stacks. However, the spatial-resolution scale of common electrical or optical probes that can be used to directly measure non-local spin-transport between an injector and a detector in lateral structures is orders of magnitude larger. Correspondingly, also the fabrication of lateral spin-transistors and more complex spin-logic devices3,4,5 relies on systems with spin-conserving length-scales approaching or, ideally, exceeding microns. The long-range nature of spin-transport, in combination with the desired high speed of these devices, inherently brings not only the requirement on the long spin life-time but also implies that electrons carrying the spin information were highly mobile.

In semiconductors like GaAs, spin-polarized photo-carriers can be generated by optical spin orientation using circularly polarized light6. Scattering from magnetic impurities is then not relevant in these non-magnetic systems. Moreover, near the bottom of the conduction band of bulk GaAs, electron wavefunctions have a dominant s-orbital character which implies weak spin-orbit coupling. The key factor limiting the spin life-time of photo-electrons is then the electron-hole recombination occurring at ~100 ps time-scales. This decay mechanism can be suppressed by introducing equilibrium carriers via impurity doping7,8. When electrons from the equilibrium electron sea take part in the recombination process, the net optically-induced spin orientation can persist over ~10–100 ns after the pump pulse. The long spin life-time is achieved, however, at the expense of a low electron mobility (~103 cm2 V−1 s−1) in these bulk GaAs samples at dopings tuned close to the metal-insulator transition.

Approaching the problem from the opposite side, very high spin mobilities (~105–106 cm2 V−1 s−1) were reported9,10 in modulation doped two-dimensional electron gases (2DEGs) at GaAs/AlGaAs interfaces in which donors are introduced into the AlGaAs barrier and the electron sheet density of the GaAs two-dimensional channel can be further controlled by gating11. However, strong electric fields confining the 2DEG enhance the spin-orbit coupling which results in short spin life-times ~100 ps9,10.

Attempts to suppress spin relaxation in two-dimensional systems included growth on [110] or [111]-oriented GaAs substrates, instead of the common [001] orientation, resulting in a moderate spin life-time ~1 ns but low mobility ~103 cm2V−1 s−1 12,13. An alternative approach is based on fine-tuning competing spin-orbit fields in the confined two-dimensional systems to the so-called spin-helix state, or on quenching these fields in one-dimensional channels5,14,15. Moderate spin life-time ~1 ns and mobility ~104–105 cm2 V−1 s−1 have been achieved in these studies15.

In our undoped GaAs/AlGaAs epilayer, electrons have intrinsically high mobilty (~105 cm2 V−1 s−1 at 10 K) since no intentional impurity doping is introduced into the system. The spin decay channel due to electron-hole recombination is suppressed by a built-in electric field which drives photo-generated holes towards the GaAs surface while the photo-electrons are driven in the opposite direction towards the AlGaAs barrier. The built-in field is not strong enough to confine the electrons into a narrow two-dimensional layer and to significantly enhance their spin-orbit coupling. As a result we observe spin life-times on the scale of 10’s of ns. Our approach is reminiscent of the electron-hole separation reported in undoped, more complex structures comprising ZnSe/BeTe type-II quantum wells where, however, only a moderate spin life-time ~1 ns and mobility ~104 cm2 V−1 s−1 were reported16.

Below we present our time and spatially-resolved pump-and-probe experiments in which we detect spins at distances reaching more than ten microns from the injection point at times as short as nanoseconds after the pump pulse. The corresponding long spin life-time and high mobility are independently confirmed by local time-resolved optical experiments and by measurements of the photo-electron conductivity in a Hall-bar dc-transport device and from terahertz (THz) transient conductivity spectra.

Results

Optical time-resolved and spatially-resolved spin transport measurements

Our pump and probe experiment, schematically illustrated in Fig. 1a, is performed on an undoped GaAs/AlGaAs structure grown by molecular beam epitaxy on a [001]-oriented semi-insulating GaAs substrate. The epilayers are deposited on the substrate starting from a 100 nm thick GaAs buffer, followed by a 100 nm Al0.3Ga0.7 As barrier and a 800 nm thick top GaAs layer. A circularly polarized pump beam and a time-delayed linearly polarized probe beam are focused at normal incidence on the sample surface, kept at temperature of 10 K, using a near infrared objective to form light spots of a diameter of ~2 μm. The relative position of the pump and probe spots is varied by a piezo-tilting mirror. Absorption of the circularly-polarized pump light generates photo-electrons with out-of-plane spin-polarization. An in-plane magnetic field, B = 500 mT, is applied to induce Hanle precession of the photo-electron spins which are probed by time and spatially-resolved polar Kerr effect measurements. The time delay between two subsequent pump pulses is 12.5 ns. For more details on the optical setup see Methods and Supplementary Fig. S.2 and Note 2.

Figure 1
figure 1

Measurement of the spin life-time and spin diffusion coefficient.

(a) A sketch of the spatially resolved pump-and-probe optical experiment. Circularly polarized pump and linearly polarized probe pulses are relatively time-delayed by Δt and focused to 2 μm sized spots (full width at half maximum). The spots can be spatially separated by Δx by tilting the incident pump beam. The magnetic field B is applied in-plane along the pump-probe separation direction. The sample was kept at temperature 10 K. (b) Kerr rotation dynamics measured by the spatially resolved pump and probe technique for several Δx. The Δx-dependent increase of the signal in time is a signature of diffusive spin-transport. The non-oscillatory envelopes (gray dashed curves) are calculated from Eq. 1 using the transient and intrinsic steady-state Ds for Δt < 0.4 ns and Δt > 0.4 ns, respectively. The data were vertically shifted and upper two curves were divided by indicated factors for clarity. (c) The spatial Gaussian dependence of the amplitude of the oscillatory Kerr signal at Δt = 1, 2 and 3 ns (marked by circles, squares and triangles, respectively) and the corresponding fits using Eq. 1. The spatial profile of the pump spot is depicted by the grey area. (d) Δt dependence of the half-width of the spatial Gaussian profile of the amplitude of the oscillatory Kerr signal.

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The dynamics of the Kerr signal at varying spatial separation of the pump and probe laser spots, Δx, is shown in Fig. 1b. The spin signal is detected at distances an order of magnitude larger than the laser spot size. This implies that the apparent decay of the signal with time at Δx = 0 is only partly due to spin relaxation and that a significant contribution comes from the out-diffusion of the photo-injected spins from the area of the laser spot. Indeed, with increasing Δx, the character of the dynamic Kerr signal changes. It acquires a nearly time-independent amplitude between Δt = 1 and 3 ns for Δx = 11 μm and for larger Δx it even increases with time. Consistently, we also observe a relative increase of the dynamic signal with increasing Δx at negative times which originates from the previous pump-pulse. The spatial Gaussian evolution of amplitudes of the Kerr signal is compared to the pump beam profile in Fig. 1c. Without a detailed analysis, the measured data illustrate that the spin signal is transferred in our GaAs/AlGaAs structure over tens of microns in time intervals as short as nanoseconds.

A more quantitative information on the spin life-time τs and diffusion coefficient Ds of the photo-electrons and on the corresponding spin diffusion length ls, can be obtained by fitting our spatially and time-dependent data to a solution of the two-dimensional spin diffusion equation17,18,

Here Ns is a normalization prefactor proportional to the total number of generated spins, is the half-width of the Gaussian distribution with the initial half-width ws,0 and the spin diffusion coefficient , ω = gμBB/ħ is the precession frequency, g is the Landé g-factor, μB is the Bohr magneton and ϕ0 is a phase factor related to the initial excitation conditions. By fitting Eq. (1) to the measured spatial spin-distribution at various Δt (as shown in Fig. 1c), we obtain the dependence (Δt), plotted in Fig. 1d. This dependence is linear for Δt > 0.4 ns, indicating that is constant in time and, therefore, represents the intrinsic steady-state value Ds for this system. From the slope of (Δt) for Δt > 0.4 ns we obtain Ds = (90 ± 10) cm2 s−1. The larger slope of (Δt) for Δt < 0.4 ns is likely caused by the transient cooling of hot non-thermalized electrons18. For the purpose of the following fitting procedure we approximate this region by a linear function, characterized by an average transient  cm2 s−1. Using Ds and for their respective Δt ranges, we apply Eq. 1 to determine τs from the time-resolved dynamics. (For clarity, we show in Fig. 1b only the envelope functions without the cosine factor.) We obtain τs = (20 ± 10) ns and the corresponding spin diffusion length,  μm. From the Einstein relation, μs = eDs/kBT and the temperature T = 10 K of the experiment we can estimate the mobility of our photo-electron spins to μs ≈ 1.0 × 105 cm2 V−1 s−1. (For a more detailed discussion of the Ds vs. μs relation see Supplementary Fig. S.5 and Note 5.)

Optical measurements of the spin life-time

To confirm the large spin life-time inferred from the above non-local experiment we employ a local measurement with overlapping pump and probe light spots. The contribution from the out-diffusion of spins from the detection area is suppressed in this experiment by increasing the size of the spots to 25 μm. The typical time-dependent Kerr signal is shown in Fig. 2a (blue points). Apart from additional signal components with a sub-ns spin life-time (commented further below and discussed in detail in Supplementary Fig. S.3 and Note 3), the spin life-time of the long-lived spin-system is obtained by fitting the Kerr dynamics to the expression19,

Figure 2
figure 2

Spin life-time τs and electron-hole separation.

(a) Kerr rotation signals measured by the local pump and probe technique on the GaAs/AlGaAs/GaAs sample and three reference samples. The data were vertically shifted and bottom two curves were multiplied or divided by indicated factors for clarity. Inset: Temperature dependence of the measured spin life-time. (b) Schematics of the GaAs/AlxGa1−xAs/GaAs layer structure (sample surface is on the left side) and of the corresponding band-edge diagram. Data presented here were measured on samples with x = 0.3 and layer thicknesses 800 nm (top GaAs), 100 nm (AlxGa1−xAs) and 100 nm (bottom GaAs spacer) on 500 μm thick GaAs substrate. The band-edge diagram shows the band bending before the illumination (solid curves) due to the negatively charged surface states (square with the negative sign) and ionized unintentional impurity states in the bulk (squares with the positive signs); EF is the Fermi level. After the illumination by the pump light (ħω) the electron-hole pairs are created (e, h letters in circles) and split in the built-in electric field, resulting in the migration of photo-holes towards the surface and photo-electrons towards the barrier and in the suppression of the band bending (dotted curves). The formation of the transient electron population near the interface is depicted by the quasi-Fermi level EQF.

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where S0 is the initial amplitude of the signal for Δt = 0. From the fit we get τs = (21 ± 2) ns in agreement with the spatially-resolved measurement.

To highlight the large spin life-time observed in the GaAs/AlGaAs layer we present in Fig. 2a also a measurement on a reference sample containing just the 900 nm thick GaAs epilayer on the GaAs substrate and a measurement on the GaAs substrate alone. As expected, spin life-times in these bulk undoped GaAs samples are limited to ~100 ps time-scales by the electron-hole recombination (τs ≈ 70 ps in the sample with the GaAs epilayer and τs ≈ 350 ps in the GaAs substrate).

The large τs observed in the GaAs/AlGaAs layer is exceptional for an undoped semiconductor. Its origin is illustrated in Fig. 2b. In dark, GaAs surface states are negatively charged by electrons removed from unintentional impurity states in the bulk of the semiconductor20,21. This generates a built-in electric field whose extent depends on the density of the ionized impurities and in epitaxial GaAs typically exceeds a micron. After illumination, photo-holes are driven by the built-in field towards the GaAs surface and fill the negatively charged surface states. Photo-electrons, on the other hand, partially fill the bulk impurity states in the top GaAs layer and partly accumulate at the interface of this layer with the AlGaAs barrier (for more details see Supplementary Fig. S.1 and Note 1). The resulting transient electron doping can persist over time-scales exceeding by orders of magnitude the repetition time of the pump pulses in our optical measurements. We confirmed this by time-resolved THz conductivity measurements, discussed in the following section.

As in previous experiments on GaAs structures with equilibrium excess electrons provided by intentional donor doping, our transient electron population at the top GaAs/AlGaAs interface suppresses the effect of electron-hole recombination on the spin life-time8,11. Simultaneously, due to the absence of intentional dopants in our structure, the electron mobility is high as we independently confirm below in the dc and THz conductivity measurements. Furthermore, consistently with the discussed mechanism, the electron-hole pairs generated outside the transient electron doping region (located near the interface) contribute to the total Kerr signal with a component whose spin life-time is limited by the electron-hole recombination to sub-ns time scale (see the rapidly damped part of the Kerr signal up to Δt = 1 ns in Fig. 2a, blue points).

The temperature dependence of the large τs, shown in the inset of Fig. 2a, is consistent with the expected Dyakonov-Perel spin-dephasing mechanism dominating at higher temperatures and with hyperfine coupling to nuclear spins at low temperatures11. We also note that τs measurements as a function of the magnetic field strength confirm a uniform g-factor (|g| = 0.45 ± 0.01) in our structure which rules out a spin relaxation mechanism induced by the g-factor inhomogeneity.

The picture of the electron-hole separation and of the accumulation of electrons with large τs near the top GaAs/AlGaAs interface is further supported by measurements on a structure without the top GaAs layer. As shown in Fig. 2a, the spin life-time in this sample (epi-AlGaAs/GaAs) is again on the ~100 ps time-scale. Indeed, the photo-holes generated in GaAs underneath the AlGaAs barrier cannot drift to the surface states and, consequently, the electron-hole separation mechanism is not effective at the interface between the AlGaAs barrier and the GaAs buffer layer.

Dc-transport and THz-spectroscopy measurements of the electron mobility

In dark, the undoped GaAs/AlGaAs layer is not conductive. Upon illumination, we detect transient dc-electrical conduction through a macroscopic Hall-bar device (a 14 μm-long and 7 μm-wide transport channel) by using both pulse laser-excitation with the 12.5 ns time separation between pulses or a continuous-wave Ti:Sapphire laser (see Supplementary Fig. S.7 and Note 7 for data with cw-laser illumination). A long life-time of the electron system is independently inferred from the time-resolved THz spectroscopy experiment with 200 μs delays between pump pulses (see Methods for details). Both the dc and THz experiments, which we now discuss in more detail, reveal a high mobility of the transient electron system, consistent with the large diffusion constant observed above in the spatially-resolved spin transport measurements.

The transient dc photoconductivity in our GaAs/AlGaAs layer is characterized at low temperatures by the electron mobility μn ≈ 2 × 105 cm2 V−1 s−1 (data shown in Fig. 3a bottom panel) and density n ~ 5 × 1010 cm−2 (Fig. 3a upper panel). (For more details on the electrical characterization see Supplementary Figs S.6 and S.7 and Notes 6 and 7.) The electron mobility shows the characteristic bulk temperature dependence22 which confirms that the electric field confining the transient electron system near the GaAs/AlGaAs interface is relatively weak, as expected from the observed long spin life-time.

Figure 3
figure 3

Dc and THz transport measurements.

(a) Dc Hall measurements of the transient carrier mobility and sheet carrier concentration with pulse laser illumination of the Hall cross at wavelength 815 nm and fluence generating a photocarrier density of 4 × 1013 cm−2. (b) Time dependence of the representative value of the photoconductivity spectra (imaginary part at ω = 0.6 THz). Data correspond to photoexcitation at fluence generating a carrier density of 2.6 × 1013 cm−2 and wavelength 800 nm (closed symbols) and at fluence generating a carrier density of 5.7 × 1013 cm−2 and wavelength 400 nm (open symbols) and to the GaAs/AlGaAs/GaAs sample (black symbols) and the reference sample containing the GaAs epilayer on the GaAs substrate (red symbols). The photoconductivity at Δt = 20 ps is normalized to unity. (c) THz spectra of normalized complex photoconductivity as a function of pump photon fluence (i.e. of the density of photocarriers) at 400 nm and time delay 9.6 ns. Lines show fits by the two Drude terms from Eq. 4.

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The transient THz photoconductivity spectra Δσ(ω) were calculated from the transient wave form spectrum ΔE(ω), measured at 18 K under various excitation fluences and wavelengths, using the expression23,

where n is the THz refractive index of GaAs, z0 is the vacuum wave impedance, ϕ is the pump photon fluence absorbed in the sample and E(ω) is the Fourier transform of the THz wave form transmitted through the unexcited sample (reference wave form). Here the conductivity is normalized by the initial charge density en0, i.e., we obtain directly the conductivity per single unit charge. Note that this quantity is expressed in units of the carrier mobility and it can be understood as a yield-mobility product ξ(t)μ(ω), where μ(ω) is the THz mobility spectrum, ξ(Δt = 0) = 1 is the unity quantum yield of the free carrier photo-excitation and ξ(Δt) describes the time decay of the carrier density23.

In Fig. 3b we plot the time decay of the imaginary part of Δσ at ω = 0.6 THz for a moderate photon pump fluence in the GaAs/AlGaAs/GaAs sample and in the reference sample containing the GaAs epilayer on the GaAs substrate. Here, we first observe a significantly slower decay of the signal in the sample containing the barrier, compared to the reference sample, which indicates that the recombination process is dramatically changed when the AlGaAs barrier is present. This supports the picture of the built-in electric field affecting the electron-hole recombination channel by separating them. Measured data for photo-excitations at 800 nm and 400 nm, with the respective light penetration depths of ~750 nm and ~20 nm, also show similar time dependence of the THz conductivity which is a signature of the homogeneity of the electric field and of the similar efficiency of this mechanism for both excitation wavelengths.

Further evidence is provided by analyzing the fluence dependence of the THz spectra. Figure 3c shows an example of the spectra for Δt = 9.6 ns. We observe that the amplitude of the conductivity does not decrease with increasing pump fluence which would be the characteristics of a dominant electron-hole recombination mechanism24,25. (See Supplementary Fig. S.9 and Note 9 for the corresponding measurement in the reference bulk GaAs sample where electron-hole recombination dominates.) However, considering the life-time of electron-hole pairs in sub-ns time-scale seen in Fig. 3b, we conclude that although the electron-hole recombination is obviously affected by the built-in electric field, the electron-hole separation of this part of the photo-carriers is not efficient enough to fully suppress their recombination. Consistently, this sub-system contributes with its sub-ns life-time to the Kerr signal in Fig. 2a (blue points, data for Δt < 1 ns).

Moreover, the imaginary part of the THz conductivity becomes negative at low frequencies and, correspondingly, the real part of the conductivity exhibits a maximum at a finite frequency, as required by Kramers-Kronig relations. This is a signature of another sub-system contributing to the net signal with a high-mobility term. The observation suggests that the highly mobile long-lived electron system is present before the arrival of each pump pulse (separated from the preceding pulse by 200 μs) and, therefore, it exhibits a fully suppressed electron-hole recombination. After being temporarily disturbed by the pump, this long-lived transient electron system leaves a trace in Δσ(ω) in the form of a negative Drude term in measured spectra. The presence of this steady-state highly mobile electron layer is fully consistent with the observation of the transient effective electron doping near the upper GaAs/AlGaAs interface in the time-resolved magneto-optical experiments.

To quantify the mobility of the long-lived electron system we fitted the THz spectra by a sum of positive and a negative Drude terms,

where τ and τL and ξ(t) and ξL are the carrier scattering times and quantum yields of the respective positive and negative Drude terms. From the fits we obtain for the long-lived electron system τL = 3.3 ± 0.7 ps which corresponds to a carrier mobility μL = (1 ± 0.2) × 105 cm2 V−1 s−1. This value is consistent, within a factor of 2, with the mobilities obtained from the dc Hall measurement and agrees well with the mobility reported from the spatially-resolved optical spin transport measurement.

Discussion

We have demonstrated an exceptional combination of a long spin life-time and a high mobility of an electron system in a semiconductor structure. Photo-generated electrons with the spin life-time reaching 20 ns and mobility 1 × 105 cm2 V−1 s−1 have been demonstrated to allow for a transfer of the spin signal over distances more than ten microns in times as short as nanoseconds. The simplicity of our bare GaAs/AlGaAs structure, compared to earlier attempts focusing on more elaborate doping, gating, heterostructure, or micro-patterning designs, opens a new perspective for the research of spin transport in semiconductors. Since undoped GaAs/AlGaAs interfaces have been commonly embedded in a variety of previously studied structures, our results may also prompt revisiting earlier experiments. As we highlight below, the superior spin-transport characteristics of the undoped GaAs/AlGaAs interface is a robust and generic phenomenon.

We have confirmed that the long spin life-time and high mobility are observed over a broad range of Al concentrations in the barrier and a broad range of barrier thicknesses (for more details see Supplementary Fig. S.4 and Note 4). Remarkably, the long spin life-time signal originating from photo-carriers at the GaAs/AlGaAs heterointerface prevails even in complex structures comprising multiple-period superlattices which are commonly introduced to separate doped GaAs quantum wells from the GaAs substrate. To demonstrate this, we compare in Fig. 4 optical spin life-time measurements in a series of GaAs/AlGaAs heterostructures.

Figure 4
figure 4

Example of the robustness of the long spin life-time signal in complex heterostructures.

(a) Schematics of the studied GaAs/AlGaAs heterostructures with a 2DEG formed in a triangular quantum well depicted by the black layer. (b) Corresponding time-resolved Kerr rotation signals measured with the local pump and probe setup arrangement at same conditions as data presented in Fig. 2a. The data were vertically shifted and divided by the indicated factor for clarity.

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The structure (A) represents a common triangular quantum well system with a 2DEG residing in a GaAs layer grown underneath a doped AlGaAs barrier and separated from the GaAs substrate by an GaAs/AlAs superlattice. The time-resolved optical signal measured in this structure is more complex than in the case of the bare GaAs/AlGaAs interface. Still, the long spin life-time component with τs ~ 10 ns is clearly present in the data. On the other hand, the structure (B) comprising an identical 2DEG layer but no undoped GaAs/AlAs superlattice shows only a short spin life-time signal with τs ~ 100 ps. Inversely, the structure (C) contains only the undoped superlattice and here the long spin life-time signal is again recovered, confirming the key role of the undoped GaAs/AlGaAs interface.

Methods

Time and spatially resolved pump and probe experiment

This experimental method was employed in order to measure τs and Ds of the long-lived excess electron system. The sample was kept in an optical cryostat at temperature 10 K and subjected to in-plane magnetic field of 500 mT, provided by an electromagnet. A mode-locked Ti:Sapphire laser (Mai Tai, Spectra Physics) with repetition rate 80 MHz (i.e. time delay between two subsequent pulses of 12.5 ns) was tuned to the wavelength λ = 815 nm. The laser beam was split to pump and probe beams with intensity ratio 10:1, setting the pump beam fluence to ≈8.5 μJcm−2, i.e. light power of 5 mW. This fluence corresponds to the bulk carrier density ≈4.8 × 1017 cm−3 photo-generated in the sample, or to sheet carrier density ≈4 × 1013 cm−2. Pump and probe beams were time delayed with respect to each other using a delay line and then circularly and linearly polarized, respectively. The setup arrangement without the spatial resolution was used to determine τs. Here, the incoming beams were focused using a lens into the cryostat close to the normal incidence on the sample surface, forming ~25 μm-sized overlapped spots.

In the arrangement with the spatial resolution (primarily employed to measure Ds), the lens was replaced by a near-infrared microscopic objective with magnification 20× and numerical aperture 0.4 to create laser spots with full width at half maximum <2 μm. The pump beam focus point was movable in 2D using a piezo-tilting mirror holder. In order to suppress the reflected pump light in the detection part in this setup arrangement, the pump and probe beams were filtered using disjunctive spectral filters, resulting in central wavelengths 824 and 814 nm, respectively (more details can be found in Supplementary Fig. S.2 and Note 2). The reflected probe light was detected via an optical bridge in both arrangements.

Electrical Hall experiment and THz spectroscopy

These approaches were used in order to determine the carrier mobility of the long-lived system and to prove the spatial separation of electron-hole pairs. In the arrangement for the electrical Hall measurements, the sample was kept in an optical cryostat at temperature 18 K and the out-of-plane magnetic field of 500 mT was applied. The central detection area of the Hall cross nanopatterned on the sample surface was illuminated with the same pump laser beam and the same fluence as described in the preceding method. The electrical operation of the nominally undoped sample was possible due to the residual local optical illumination of whole sample surface (see Supplementary Note 3). The Hall cross was current-biased to 10 μA and the longitudinal and transversal voltages were sensed by dc voltmeters.

The transient time resolved THz conductivity spectra were measured on unpatterned samples using a setup based on Ti:Sapphire laser amplifier with central wavelength 800 nm and 5 kHz repetition rate (time separation of two pulses is 200 μs). One part of the laser beam was used for the THz pulse generation and its phase-sensitive detection by means of the optical rectification and electro-optic sampling in 1-mm-thick (110)-oriented ZnTe crystals, respectively. Another part of the laser beam was used for optical pumping of samples either at 800 or 400 nm, see ref. 26 for more details. The pump beam was defocused to generate photocarriers homogeneously across the sample attached to a 3 mm aperture. The pump fluence was attenuated using neutral density filters to achieve the photo-generated carrier density in the range ≈ ×1012 –1014 cm−2. An optical chopper was used in the pump beam path; this scheme ensures that we experimentally detect the photo-induced change ΔE(ω) of the THz wave form transmitted through the sample. The experiments were carried out at 18 K for both pump wavelengths. (For more information see Supplementary Fig. S.8 and Note 8.)

Additional Information

How to cite this article: Nádvorník, L. et al. Long-range and high-speed electronic spin-transport at a GaAs/AlGaAs semiconductor interface. Sci. Rep. 6, 22901; doi: 10.1038/srep22901 (2016).