Source: https://www.jove.com/video/56861/all-electronic-nanosecond-resolved-scanning-tunneling-microscopy
Timestamp: 2019-04-22 20:15:57+00:00

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We demonstrate an all-electronic method to observe nanosecond-resolved charge dynamics of dopant atoms in silicon with a scanning tunneling microscope.
Rashidi, M., Vine, W., Burgess, J. A., Taucer, M., Achal, R., Pitters, J. L., Loth, S., Wolkow, R. A. All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics. J. Vis. Exp. (131), e56861, doi:10.3791/56861 (2018).
The miniaturization of semiconductor devices to scales where small numbers of dopants can control device properties requires the development of new techniques capable of characterizing their dynamics. Investigating single dopants requires sub-nanometer spatial resolution, which motivates the use of scanning tunneling microscopy (STM). However, conventional STM is limited to millisecond temporal resolution. Several methods have been developed to overcome this shortcoming, including all-electronic time-resolved STM, which is used in this study to examine dopant dynamics in silicon with nanosecond resolution. The methods presented here are widely accessible and allow for local measurement of a wide variety of dynamics at the atomic scale. A novel time-resolved scanning tunneling spectroscopy technique is presented and used to efficiently search for dynamics.
Scanning tunneling microscopy (STM) has become the premier tool in nanoscience for its ability to resolve atomic-scale topography and electronic structure. One limitation of conventional STM, however, is that its temporal resolution is restricted to the millisecond timescale because of the limited bandwidth of the current preamplifier1. It has long been a goal to extend STM's temporal resolution to the scales on which atomic processes commonly occur. The pioneering work in time-resolved scanning tunneling microscopy (TR-STM) by Freeman et. al.1 utilized photoconductive switches and microstrip transmission lines patterned on the sample to transmit picosecond voltage pulses to the tunnel junction. This junction-mixing technique has been used to achieve simultaneous resolutions of 1 nm and 20 ps2, but it has never been widely adopted due to the requirement of using specialized sample structures. Fortunately, the fundamental insight gained from these works can be generalized to many time-resolved techniques; even though the bandwidth of the STM's circuitry is limited to several kilohertz, the non-linear I(V) response in STM allows faster dynamics to be probed by measuring the average tunnel current obtained over many pump-probe cycles. In the intervening years, many approaches have been explored, the most popular of which are briefly reviewed below.
Shaken-pulse-pair-excited (SPPX) STM takes advantage of the advancements in ultrafast pulsed laser technologies to achieve sub-picosecond resolution by directly illuminating the tunnel junction and exciting carriers in the sample3. Incident laser light creates free carriers that transiently enhance conduction, and modulation of the delay between the pump and probe (td) allows dI/dtd to be measured with a lock-in amplifier. Because the delay between the pump and probe is modulated rather than the laser's intensity, as in many other optical approaches, SPPX-STM avoids photo illumination-induced thermal expansion of the tip3. More recent extensions of this approach have extended the timescales over which SPPX-STM can be used to investigate dynamics by utilizing pulse-picking techniques to increase the range of pump-probe delay times4. Importantly, this recent development also provides the ability to measure I(td) curves directly rather than via numerical integration. Recent applications of SPPX-STM have included the study of carrier recombination in single-(Mn, Fe)/GaAs(110) structures5 and donor dynamics in GaAs6. Applications of SPPX-STM face some restrictions. The signal SPPX-STM measures depends on free carriers excited by the optical pulses and is best suited to semiconductors. Additionally, although the tunneling current is localized to the tip, because a large area is excited by the optical pulses, the signal is a convolution of the local properties and material transport. Finally, the bias at the junction is fixed at the measurement timescale so that the dynamics under study must be photoinduced.
A more recent optical technique, terahertz STM (THz-STM), couples free-space THz pulses focused on the junction to the STM tip. Unlike in SPPX-STM, the coupled pulses behave as fast voltage pulses allowing for the investigation of electronically driven excitations with sub-picosecond resolution7. Interestingly, the rectified current generated from the THz pulses results in extreme peak current densities not accessible by conventional STM8,9. The technique has been used recently to study hot electrons in Si(111)-(7x7)9 and image the vibration of a single pentacene molecule10. THz-pulses naturally couple to the tip, however, the necessity to integrate a THz source to an STM experiment is likely to be challenging to many experimenters. This motivates the development of other widely applicable and easily implementable techniques.
In 2010, Loth et al.11 developed an all-electronic technique where nanosecond voltage pulses applied on top of a DC offset electronically pump and probe the system11. The introduction of this technique offered a critical demonstration of unambiguous and practical applications of time-resolved STM to measure previously unobserved physics. Although it is not as fast as junction mixing STM, which preceded it, applying microwave pulses to the STM tip permits arbitrary samples to be investigated. This technique does not require any complicated optical methodologies or optical access to the STM junction. This makes it the easiest technique to adapt to low temperature STMs. The first demonstration of these techniques was applied to the study of spin-dynamics where a spin-polarized STM was used to measure the relaxation dynamics of spin-states excited by the pump pulses11. Until recently, its application remained limited to magnetic adatom systems12,13,14 but has since been extended to the study of carrier capture rate from a discrete mid-gap state15 and charge dynamics of single arsenic dopants in silicon15,16. The latter study is the focus of this work.
Measurements are performed on selected DBs on a hydrogen terminated Si(100)-(2x1) surface. A dopant depletion region extending approximately 60 nm below the surface, created via thermal treatment of the crystal30, decouples the DB and the few remaining near-surface dopants from the bulk bands. STM studies of DBs have found that their conductance is dependent on global sample parameters, such as the concentration of dopants and the temperature, but individual DBs also show strong variations depending on their local environment16. During an STM measurement over a single DB, the current flow is governed by the rate at which electrons can tunnel from the bulk to the DB (Γbulk) and from the DB to the tip (Γtip) (Figure 1). However, because the conduction of the DB is sensitive to its local environment, the charge state of nearby dopants influences Γbulk (Figure 1B), which can be inferred by monitoring the DB's conductance. As a result, the conductance of a DB can be used to sense the charge states of nearby dopants, and can be used to determine the rates at which the dopants are supplied electrons from the bulk (ΓLH) and lose them to the STM tip (ΓHL). To resolve these dynamics, TR-STS is performed around the threshold voltages (Vthr) at which the tip induces ionization of near-surface dopants. The role of the pump and probe pulses is the same in the three time-resolved experimental techniques presented here. The pump transiently brings the bias level from below to above Vthr, which induces dopant ionization. This increases the conductance of the DB, which is sampled by the probe pulse which follows at a lower bias.
The techniques described in this paper will benefit those wishing to characterize dynamics occurring on the millisecond to nanosecond timescale with STM. While these techniques are not limited to studying charge dynamics, it's crucial that the dynamics are manifested via transient changes in the conductance of states that can be probed by STM (i.e., states on or near the surface). If the conductance of the transient states does not differ significantly from the equilibrium state, such that the difference between the transient and equilibrium currents multiplied by the probe pulse duty cycle is smaller than the systems noise floor (typically 1 pA), the signal will be lost in the noise and will not be detectable by this technique. Because the experimental modifications of commercially available STM systems required to perform the techniques described in this paper are modest, it's anticipated these techniques will be widely accessible to the community.
Begin with an ultrahigh vacuum cryogenic-capable STM and associated control software. Cool the STM to cryogenic temperatures.
NOTE: Throughout this report, ultrahigh vacuum refers to systems that achieve <10 x 10-10 Torr. The STM should be cooled to cryogenic temperatures; this is especially important when investigating the charge dynamics of dopants, which are thermally activated at modest temperatures. Other chambers may be at room temperature.
Ensure that the STM tip is equipped with high-frequency wiring (~500 MHz).
Connect an arbitrary function generator with at least two channels to the tip (Figure 2), which will be used to prepare the cycles of voltage pulse pairs used for pump-probe experiments.
Configure the arbitrary function generator so that the pump and probe voltage pulses are generated independently and summed before being fed into the tip.
Apply the DC bias voltage used for imaging and conventional spectroscopy to the sample (VDC).
Connect two radio frequency switches to the arbitrary function generator's output channels.
Configure the switches so that the tip will be grounded during STM imaging and conventional spectroscopy, and the effective bias is VDC + Vtip during pump-probe experiments (Figure 4A).
Collect the tunneling current for all measurements through a preamplifier connected to the sample.
Cleave a sample from a 3-4 mΩ·cm n-type arsenic doped Si(100) wafer by scratching the back of the wafer with a silicon carbide scriber and gently snapping the sample off the wafer with glass microscope slides.
Affix the sample to an STM sample holder and introduce it to an ultrahigh vacuum chamber adjacent to the STM chamber.
Degas the sample by resistively heating it to 600 °C (a pyrometer can be used to monitor the sample's temperature) and holding it at that temperature for at least 6 h in ultrahigh vacuum.
NOTE: The pressure will initially rise as the sample and sample holder degas, but should stabilize near the base pressure (<10-10 Torr) after several hours.
Allow the sample to cool to room temperature before continuing.
Degas a tungsten filament in the same chamber as the sample by resistively heating the filament to 1800 °C and waiting for the system to recover to base pressure. Turn off the filament before continuing.
NOTE: The sample can remain in the chamber during this step because it is passivated by the native oxide layer at its surface, and any contamination of the sample surface caused from this step will be removed subsequently. The filament's temperature will have to be calibrated to a specific current/voltage applied to the filament using a pyrometer.
Remove the oxide from the sample surface by flashing the sample to 900 °C and holding it at that temperature for 10 s before cooling it to room temperature. The pressure will increase several orders of magnitude from the base pressure during the flashing procedure. After each of the flashes found throughout this procedure, wait for the sample to cool to room temperature and the system to recover to base pressure before continuing.
NOTE: Flashing is defined within this report as heating and cooling the sample with high ramp rates, on the order of 100 °C/s.
Progressively flash the sample to higher temperatures while attempting to reach a final flash of 1250 °C. Abort any flash where the pressure rises above 9x10-10 Torr to prevent the sample surface from getting contaminated. Record the voltage/current used to achieve the 1250 °C flash (the light given off by the heated filament in step 2.6 will prevent a pyrometer from giving an accurate reading of the sample's temperature, and thus this setpoint should be used). On the final flash, determine the voltage/current required to heat the sample to 330 °C as the crystal is cooled, then let the sample cool to room temperature, and let the system recover to base pressure before continuing.
Leak H2 gas into the chamber at a pressure of 1x10-6 Torr and heat the tungsten filament to 1800 °C.
NOTE: This has the effect of cracking the H2 to atmoic hydrogen32.
Hold the sample in these conditions for 2 min before flashing the sample to 1250 °C, holding it at that temperature for 5 s, and cooling it to 330 °C.
After 1 min of exposure at 330 °C, simultaneously close the H2 leak valve, turn off the tungsten filament, and let the sample cool to room temperature.
NOTE: These high flash temperatures affect the distribution of dopants in the sample. Heating to 1250 °C has been found to induce a ~60 nm dopant depletion region near the sample surface30.
Verify the sample's quality by taking STM images of the surface.
NOTE: Good samples will have large (>30 nm x 30 nm) terraces with a defect rate of <1% (dangling bonds, adsorbed molecules, adatoms, etc.) and will demonstrate the classic Si(100)-(2x1) reconstruction32, which features dimer rows running antiparallel to one another across step edges (Figure 3B).
Approach the STM tip to the sample surface by engaging the current feedback controller with a current setpoint of 50 pA and a sample bias of -1.8 V.
NOTE: Under these conditions, the tip is estimated to be <1 nm from the sample surface. The STM tip used in this work was produced by chemically etching polycrystalline tungsten. It was sharpened further using a nitrogen etching procedure, which is well described in Rezeq et al.33.
Look for an area on the sample surface free from large surface defects by taking large area scans (e.g., 50 nm x 50 nm).
Position the STM tip over an H-Si on the surface, which appear as the dimer rows in STM images (Figure 3B).
Set VDC to -1.0 V, Vpump to -0.5 V, Vprobe to -0.5 V, the width of the pump and probe pulses to 200 ns, and the rise/fall time of the pulses to 2.5 ns (Figure 4A).
Send a series of trains of pump and probe pulses where the relative delay of the pump and probe is swept from -900 ns to 900 ns.
Plot the tunneling current as a function of the delay between the pump and probe. It will likely demonstrate strong ringing (oscillations in the tunneling current as a function of the relative delay between the pump and probe pulses, Figure 4B).
NOTE: Python and Origin software were used to plot, analyze, and evaluate the data collected for this manuscript.
Repeat steps 3.1–3.5, but increase the rise/fall times of the pulses. The ringing will decrease as the rise/fall times are increased.
NOTE: It's desired to eliminate ringing to provide the most accurate spectroscopic results, however, the time-resolution of these techniques is limited to the width of the pulses used. 25 ns rise times were used for this work.
Position the STM tip over a silicon DB, which appear as bright protrusions at negative tip-sample biases (Figure 3B).
Turn off the STM current feedback controller.
Send a train composed of only the probe pulse with a repetition rate of 25 kHz. Over a series of pulse trains, sweep the bias of the probe pulse over a range of 500 mV from the DC bias of -1.8 V.
NOTE: This simple experiment is analogous to conventional STS where the conductance is sampled over a range of biases.
Configure the duration of the pulse trains (each with a different bias) such that the resulting spectra have a signal to noise ratio >10.
Send a train composed of pump pulses set at a fixed bias (such that VDC + Vpump > Vthr) with a repetition rate of 25 kHz. In these experiments, set the VDC, Vpump, and Vthr to -1.8 V, 500 mV and -2.0 V, respectively.
NOTE: Pump pulses can have arbitrarily long durations (1 µs is typically sufficient).
Send a train composed of the pump pulses with the probe pulses followed by a delay of 10 ns. In these experiments, set the amplitude of the pump pulse as 500 mV and of the probe pulse sweep from 50 to 500 mV.
NOTE: In this experiment, the probe pulse is sampling the state prepared by the pump pulse, rather than the equilibrium state sampled in conventional STS.
Subtract the signal obtained when only the pump pulse was applied when displaying/evaluating the signal collected from this step.
Compare the probe only and the pump + probe signals by plotting them in the same graph. Any hysteresis in the two signals is an indication of dynamics that can be probed with time-resolved STM techniques.
NOTE: By keeping the range of the probe pulse fixed and coarsely scanning the DC offset (in 0.25 V steps, for example), one can efficiently map the entire energy range of the sample to identify dynamics accessible to the technique. Pulse durations can be modified depending on the experiment. The width of the pump pulse needs to be longer than the rate at which the dopant is ionized, such that it consistently ionizes the dopant. In general, probe durations should be of the same order as the dynamical process under study, such that the maximum signal can be measured without sampling an average of the two conductance states. When searching for energies at which dynamics exist, it is recommended that durations of the probe are minimized such that only one state of the system is measured to enhance hysteresis. As the relaxation time constants are found, the duration of the probe pulse can be increased to improve the signal to noise ratio.
Position the STM tip over a silicon DB and turn off the STM current feedback controller.
Send a train composed of pump pulses set at a fixed bias (such that VDC + Vpump > Vthr) with a repetition rate of 25 kHz. In these experiments, set the VDC, Vpump, and Vthr to -1.8 V, 400 mV and -2.0 V, respectively.
Send a train of pump and probe pulses. Ensure that the probe pulses have an amplitude smaller than the pumps and comparable to the range at which hysteresis occurs (Vprobe < Vpump, Vprobe + VDC≈Vhystersis).
Sweep the delay between the pump and probe pulse up to several tens of µs.
Subtract the signal obtained when only the pump pulse was applied. In these experiments, set the VDC, Vpump, and Vprobe to -1.8 V, 400 mV and 210 mV, respectively. Set the relative delay sweep from -5 μs to 35 μs.
NOTE: If the signal obtained from the previous step is well fit (R2 > 0.80) by a single exponential decay function, then the lifetime of the transient state prepared by the pump pulse can be extracted from the fit.
Send a train composed of pump pulses set at a fixed bias (such that greater than VDC + Vpump > Vthr) with a repetition rate of 25 kHz. In these experiments, set the VDC and Vthr to -1.8 V and -2.0 V, respectively. Set Vpump between 220 and 450 mV.
Sweep the duration of the pump pulse from several nanoseconds to several hundred nanoseconds.
Send a train of pump and probe pulses. The probe pulses should have an amplitude smaller than the pumps and comparable to the range at which hysteresis occurs (Vprobe < Vpump, Vprobe + VDC≈Vhystersis). In these experiments, set Vprobe to 210 mV.
Subtract the signal obtained when only the probe pulse was applied.
NOTE: If the signal obtained is exponential, it indicates that the pump pulse is preparing the transient state (ionized dopant) at a rate that can be extracted from the fit (R2>0.80). The protocol described above is specific to the experiments and equipment described herein. There are many potential avenues for readers to customize their own experimental setup for studies of other systems. For example, the general techniques are not limited to cryogenically cooled STMs; any tip material can be used, and they do not require nitrogen etching. Furthermore, a suitably programmed arbitrary function generator could be used to generate double-pulse waveforms, which would negate the need to sum two independent channels. Lastly, lower bandwidth cabling could be used31.
The results presented in this section of the text have been previously published15,16. Figure 3 illustrates the behavior of an example selected DB with conventional STM. A conventional I(V) measurement (Figure 3A) clearly depicts a sharp change in the conductance of the DB at Vthr = -2.0 V. This behavior is also observed in STM images taken at -2.1 V (Figure 3B, left panel), -2.0 V (middle panel), and -1.8 V (right panel), where the DB has the appearance of a bright protrusion, a speckled protrusion, and a dark depression, respectively. This transition can also be observed by looking at the tunneling current collected with the tip positioned directly on top of the DB with the z-controller turned off and the bias set to Vthr, which results in two-level telegraph noise (Figure 3C). Crucially, in these measurements, the tip of the STM was placed directly over the DB. In this arrangement, the fluctuation of the DB's charge state occurs on timescales below e/IT = 2ns, which is much faster than the switching observed. As such, the observed behavior is attributed to the charging dynamics of nearby dopants which affects the conductance of the DB. It is important to note that because the extended wave-function of DB's mid-gap energy states act as a bridge to conduct electrons from the bulk conduction band to the tip, the observed behavior is only apparent when the tip is placed directly over the DBs. As the bias was increased, the frequency of the telegraph noise also strongly increased, such that at -2.02 V, the switching behavior could no longer be resolved directly by the STM's preamplifier. This motivated the use of time-resolved scanning tunneling microscopy (TR-STM) and time-resolved scanning tunneling spectroscopy (TR-STS).
Figure 4 demonstrates a method that can be used to assess the quality of the pulses delivered to the junction. Ringing is observed when fast rise times are used for the pump and probe pulses because of the impedance mismatch between the STM circuitry and the tunnel junction. A cross-correlation of the pump and probe pulses can be generated by sweeping the relative delay of the probe pulse through zero-delay. A strong increase in tunneling current occurs when the pump and probe pulses overlap due to the characteristic non-linear behavior of I(V) measurements. Ringing is manifested through smaller amplitude oscillations in the tunneling current on both sides of the origin. By increasing the rise times on the pulses from 2.5 ns to 25 ns, a strong suppression of the ringing is observed. The relative offset of the signals generated with each pulse rise time is a result of the fact that the pulse width is measured to include the rise times of the pulses. Therefore, pulses with 2.5 ns rise times have a greater integrated area, and therefore a greater integrated current, compared to pulses with 25 ns rise times. This highlights that quantitative comparison of TR-STM measurements should only be performed when the rise times of the pulses used are equal.
Figure 5 demonstrates TR-STS. In these measurements, a pump pulse transiently brings the system above Vthr, and immediately after a probe pulse interrogates the conductance of the transient state. The conductance of the transient state can be mapped by subtracting the signal acquired with probe only from the signal obtained with pump+probe. When the pump+probe and probe only signals are compared directly, any hysteresis is indicative of dynamic processes that can be probed by TR-STS. By changing the value of the fixed DC offset bias, the dynamics of the system that can probed by TR-STS can be efficiently identified.
In TR-STS, it is important to consider the duration of the pump and probe pulses. The pump pulse should be sufficiently long to induce a steady-state of the system (i.e., pump it into the high conductance state). If the duration of the probe pulse is too long, however, then at low probe amplitudes, the conductance of the DB can relax during the measurement. In this case, the probe pulse will sample both the high and low conductance states of the DB and reduce the visibility of the hysteresis. Therefore, to maximize the visibility of the hysteresis, the duration of the probe pulse should be shorter than the relaxation rate of the high-conductance state.
Figure 6 demonstrates time-resolved measurements of dopant relaxation and excitation dynamics. As in TR-STS, the sample is set to a fixed DC offset bias below Vthr, and the pump pulses transiently bring the system above Vthr. Relaxation dynamics were probed by sweeping the relative delay of the probe pulses (Figure 6A). Fitting a plot of the probe current as a function of the relative delay (Figure 6B) with a single exponential decay permitted ΓHL to be extracted. It is important to note that this rate is never observed for a single cycle, rather ΓHL is inferred from the time-averaged tunneling current which is comprised of many events. This is analogous to optical spectroscopy, where the lifetime of an excited state can be determined from single measurements of an ensemble, except that in this case the lifetime of a single dopant can be characterized through an ensemble of measurements because it can be probed directly by the STM tip. It is important to note that the probe current observed in Figure 6B does not decay to zero, but rather to a fixed offset. This is because the pump pulse excites dynamics (observed as the millisecond-scale telegraph noise in Figure 3C) that do not decay within the measurement timeframe. This indicates that the conductance of the DB under study is gated by two dopants with distinct relaxation time constants. Figure 6C demonstrates a control experiment where the amplitude of the pump is varied from -0.25 V to -0.6 V. A change in the lifetime of the ionized state, as a function of the pump amplitude, would indicate that additional dynamical processes exist close in energy to Vthr. Because ΓHL is constant beyond -2.05 V, it's concluded that only the charge states of the two identified dopants are gating the conductance of the DB.
Excitation dynamics were probed by sweeping the width of the pump pulse (Figure 6D). ΓLH was extracted from an exponential fit of the time-averaged current as a function of the pump width (Figure 6E). When the pumped bias does not exceed Vthr, there is no observed dependence between the pump width and the tunneling current because the dopants remain neutral. When the pumped bias exceeds Vthr, an electron can tunnel from the dopant to the tip leaving the dopant ionized. By sweeping the width of the pump, the average rate at which the dopant is ionized is mapped. Figure 6F investigates the dependence of ΓLH as a function of the pump's amplitude. If a DB is gated by a single dopant, ΓLH is expected to scale exponentially with the pump's amplitude over the entire bias range16. This is expected because the dopant's ionization rate depends exponentially on the strength of the local electric field, which scales with the bias applied to the tip. DB1, which is the DB studied in all prior figures, demonstrates an exponential dependence between -2.1 V and -2.25 V, and a step at -2.05 V. This step is further evidence that DB1 is gated by two nearby dopants. An exponential dependence was observed for DB2 over the range -1.3 V to -1.6 V, indicating that a single dopant gated it. DB2 did not exhibit any dynamics beyond the millisecond timescale and therefore was not studied with the other time-resolved techniques.
Figure 1: Schematic of the system of study and its associated energy diagram. (A) The current sampled by the STM tip positioned directly on top of a silicon DB is predominantly composed of electrons passing from the bulk to the DB, and from the DB to the tip, with rates Γbulk and Γtip, respectively. Arsenic dopants, represented by green balls, also have filling (ΓHL) and emptying rates (ΓLH) that can be probed by time-resolved STM measurements. (B) The conduction band edge in the presence of an ionized dopant (green curve) is pulled down relative to when the dopant is neutral (black curve), which results in an increased conductance. The energy diagram was computed for a sample bias of -2.0 V. The blue colored area represents the filled states. This figure has been taken with permission from Rashidi et al.16 Please click here to view a larger version of this figure.
Figure 2: The required modifications that must be made to a commercial STM such that TR-STM can be performed with the methods described in this work. A DC offset bias is applied to the sample, and during STM imaging and conventional spectroscopy, the STM tip is grounded. When used for time-resolved measurements, the signals created by an arbitrary function generator with two independent channels are summed and fed to the tip of the STM, which must be equipped with high-frequency cabling. Two radiofrequency switches are used to control the pulse trains. The tunneling current is measured on the sample side. This figure has been taken with permission from Rashidi et al.16 Please click here to view a larger version of this figure.
Figure 3: The spectroscopic behavior of a selected DB with conventional STM. (A) An I(V) measurement over the DB collected at constant height. (B) Constant-current STM images of the DB beyond (-2.1 V, left), at (-2.0 V, middle), and below (-1.8 V, right) the threshold voltage. Dimer rows of the H-Si(100)-(2x1) reconstruction appear as parallel bars. (C) With the current feedback controller of the STM off a current-time trace acquired over the DB at the threshold voltage (-2.01 V) displays two-state telegraph noise on the millisecond timescale. This figure has been taken with permission from Rashidi et. al.16 Please click here to view a larger version of this figure.
Figure 4: A cross-correlation of the pump and probe pulses at the tunnel junction. (A) Schematic of the cross-correlation pulse sequences. A static DC offset bias (green bar) is applied to the sample. The relative delay between the pump pulses (red bars) and the probe pulses (blue bars) is swept through zero delay. Each pair of pump and probe pulses represents a train of pulses sent to the tip. (B) The tip is positioned over H-Si and a train of pump-probe pairs is delivered to the tunnel junction. The relative delay of the probe is measured from the trailing edge of the pump to the leading edge of the probe, and was swept from -900 ns to 900 ns. A static DC offset of -1.0 V was applied to the sample. Pump and probe amplitudes were set to -0.50 V with 200 ns widths. The rise/fall time of the pulses was set to 25 ns (black), 10 ns (red), and 2.5 ns (blue). The probe current was multiplied by a factor of twenty to account for the 5% duty cycle employed in the measurement, however, no attempt was made to correct for the fact that the integrated areas of each pulse train differ. Inset: an enlarged view of the ringing between 0 and 900 ns relative delay. Please click here to view a larger version of this figure.
Figure 5: Time-resolved scanning tunneling I(V) spectroscopy (TR-STS). (A) Schematic of the TR-STS pulse sequences. A static DC offset bias (green bar) is applied to the sample. Pump pulses (red bars) precede probe pulses (blue bars). Each pair of pump and probe pulses represents a train of pulses sent to the tip. (B) TR-STS measurement with 1 µs width pump and probe pulses. The hysteresis between the curves without the pump (red triangles) and with the pump (blue circles) overlaps the bias range where the system is bistable. The DC bias is set to -1.80 V, the pump bias is -0.50 V, and the probe bias was swept from 500 to 50 mV. The pulses have risen and fallen times of 25 ns, the relative delay between the trailing edge of the pump and the leading edge of the probe pulse is 10 ns, and the repletion rate is 25 kHz. This figure has been taken with permission from Rashidi et. al.16 Please click here to view a larger version of this figure.
Figure 6: Time-resolved measurements of dopant excitation and relaxation dynamics. (A,D) Schematics of the pulse sequences. A static DC offset bias (green bar) is applied to the sample. Pump pulses (red bars) precede probe pulses (blue bars). Each pair of pump and probe pulses represents a train of pulses sent to the tip. (B) Measurement of ΓHL is made by sweeping the relative delay of the pump and probe pulses. The pump and probe pulses have widths of 1 µs. A DC offset of -1.80 V is applied to the sample; the pump and probe pulses have amplitudes of -0.4 and -0.21 V, respectively. The solid line is a fit of the data with a single exponential function. (C) Measurements of ΓHL at different pump amplitudes. Error bars represent the standard errors of the exponential fittings. (E) Measurement of ΓLH is made by sweeping the duration of the pump. A DC offset of -1.80 V is applied to the sample and the probe pulses have an amplitude of -0.21 V. Vthr for the selected DB is -2.05 V. The solid line is a fit of the data with a single exponential function. (F) Measurements of ΓLH at different pump amplitudes for two selected DBs. DB1 (red triangles) is the DB used for all other measurements in the text. DB2 is a different selected DB and is described fully in Rashidi et al.16 Solid lines are fits of the data with a single exponential function. This figure has been taken with permission from Rashidi et al.16 Please click here to view a larger version of this figure.
The variant of TR-STS in which the pump pulse is not applied is comparable to conventional STS, except that the system is being sampled at a high frequency rather than continuously. If the durations of the probe pulses are appropriate (>ΓLH), the TR-STS signal acquired without the pump pulse can be multiplied by a constant proportional to the experiment's duty cycle to coincide exactly with a conventional STS measurement. This is only possible because the measurements are made without the use of a lock-in amplifier, which would otherwise attenuate an unknown portion of the signal due to the low-pass filtering used. This is a significant difference between the methods employed by Loth et al.11 and those presented in this work. The use of a lock-in amplifier can be used to enhance the sensitivity of the measurements, but prevents the direct comparison of TR-STS with conventional STS measurements. In systems where this sensitivity is required, it is anticipated that both methods could be used in concert, with the lock-in amplifier turned off such that experimenters can efficiently search for dynamics, and the lock-in amplifier turned on for added sensitivity during the characterization of excitation and relaxation dynamics.
The main drawback of these techniques is that their temporal resolution is currently limited to several nanoseconds. This is several orders of magnitude slower than what can be achieved with junction-mixing or optical techniques. This is a consequence of signal ringing, which occurs when voltage pulses with sub-nanosecond rise times are used, due to the impedance mismatch between the STM circuit and the tunnel junction31. Indeed, all-electronic methods have achieved time resolution as fine as 120 ps34 but have not yet been used to investigate dynamics at that resolution. An optimally designed STM would have a perfectly impedance-matched STM circuit up until the tunnel junction, which would be perfectly impedance-mismatched. This would eliminate distortion and dissipation of the pulse and would reflect the microwave power, rather than deliver it across the junction. A possible strategy to eliminate the resulting ringing would be to add extra dissipation to the STM circuit so that reflected pulses would be effectively attenuated.
In this work, the simplest approach was taken, i.e., no internal modification to the commercial STM was performed. A cross-correlation technique was used to characterize the ringing, which was then minimized by simply extending the rise times of the pulses. Because the rise time of the pulses limits the time resolution, this strategy cannot be used to characterize dynamic processes occurring on timescales at the limits of these techniques (several ns). In these situations, ringing can be actively suppressed by employing the techniques developed by Grosse et al.31, which involve shaping the pulses to account for the transfer function of the arbitrary function generator and the tunnel junction.
The all-electronic approach to TR-STM has many advantages over other prominent TR-STM approaches. Firstly, in comparison to junction-mixing STM, this approach does not require any specialized sample structures. Any samples that can be scanned with conventional STM should be amenable to these techniques. Further, the all-electronic approach does not require significant modifications to the STM or the use of ultrafast optics. Indeed, the modifications to the STM circuitry required to perform these techniques are extremely modest, as commercial STMs with high-frequency cabling are available. Additionally, the dynamics probed with the all-electronic approach are purely local, as the pulses are supplied directly to the STM tip. This contrasts with SPPX-STM, where the incident laser pulses can only be focused to several square microns. Finally, the all-electronic method permits the ability to accurately manipulate the biases of the pump and probe, allowing a direct comparison to standard STM measurements. This is central to several of the techniques described in this paper, and while it may be possible to implement similar pulse sequences in optical approaches to TR-STM, it is experimentally difficult.
The experimental techniques presented here measure charge dynamics with atomic spatial resolution and nanosecond temporal resolution. There is a wealth of new physics to be studied with this very accessible approach. For example, the dynamics of single atoms are fascinating and important technologically. Single atom dynamics were previously studied within the limitations of conventional STM, but this technique opens the door for investigating similar processes over six additional orders of magnitude (from millisecond to nanosecond). Notably, this bridges the gap from the slow events typically observed in STM, to the fundamental processes that underlie them.
We would like to thank Martin Cloutier and Mark Salomons for their technical expertise. We also thank NRC, NSERC, and AITF for financial support.
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