Attosecond current control and timing in a scanning tunnelling microscope
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Introduction to the show: ident: Quantum Radio. Generated commentary on the latest quantum physics and condensed matter papers.
Kai: I'm Kai, and with me are Mira and Lev, guest researcher.
Mira: Today's paper: "Attosecond current control and timing in a scanning tunnelling microscope".
Kai: Quantum tunnelling of electrons can be confined to sub-cycle time scales under strong light fields,
Mira: First, who's behind it and why it matters.
Title and authors: Kai: So, we're looking at the paper titled "Attosecond current control and timing in a scanning tunnelling microscope." It sounds like they've managed to put attosecond precision into STM by controlling the light pulses used. It’s about using two-color laser pulses to get this kind of control.
Mira: I see that title, and it suggests they are tackling the directionality of these ultrafast electron currents, which is a real challenge in this field. The authors are a big team including Boyang Ma, Adi Goldner, Shimon Cohen, Zhaopin Chen, Andrei G. Borisov, and Michael Kröger.
Lev: From my side, I'm interested in how they achieved this control; if it's robust enough for real hardware testing with error correction protocols later on.
Kai: Exactly, Lev; the core idea is using these two-color pulses to dynamically switch the tunnelling direction, which is a big step because controlling that direction has been elusive before.
Mira: And I think the implication here is that they've moved beyond just observing dynamics to actively steering them using light control, which opens up a whole new way to probe quantum phenomena at these extreme timescales.
Lev: If the control mechanism relies on manipulating sub-cycle waveforms, we need to know if that complexity translates well when you try to implement error correction schemes for such fast dynamics.
The paper's summary: Kai: The summary explains that the researchers induce STM tunnelling currents by superimposing an infrared fundamental pulse with its second harmonic and then controlling their relative time delay to break symmetry and get sub-cycle control.
Mira: That’s a clever way to generate a waveform with controlled symmetry breaking, which directly enables this sub-cycle timing capability they mention in the summary of "Attosecond current control and timing in a scanning tunnelling microscope."
Lev: So, the core mechanism is essentially using two laser colors—the fundamental and its second harmonic—and just tweaking their relative timing to get that precise control over the tunneling process.
Kai: Right, and what's really striking from the summary is that this method allows them to "seamlessly switch between tip-to-sample tunnelling and vice versa," which they show unambiguously using a temporarily frozen tip.
Mira: That switch capability is significant because it means they can manipulate the direction of electron flow, which ties directly into what we discussed earlier about controlling the dominant direction of current based on field characteristics.
Lev: If you can switch directions reliably under these conditions, it suggests that this control mechanism might be stable enough to be integrated into a larger experimental sequence.
Kai: And they also provide a key quantitative finding: projecting their data onto one-electron and many-body theory descriptions reveals a three-step transport process in the non-adiabatic tunnelling regime with a theory-derived current burst duration of eight hundred sixty as.
The paper's improvements: Mira: The paper points to several improvements regarding the theoretical understanding, specifically that projecting their measurement data onto one-electron and many-body theory descriptions reveals a three-step transport process in the non-adiabatic tunnelling regime as the physical mechanism.
Kai: And they used this framework alongside an analytical strong-field (SF) model based on the van Vleck propagator, along with a single-active-electron model approach using numerical integration of the one-dimensional time-dependent Schrödinger equation, nTDSE.
Lev: From an error correction standpoint, having such a detailed theoretical mapping onto the nTDSE is helpful because it gives us a solid baseline to predict what kind of noise we might expect when trying to run this on real hardware later.
Mira: Furthermore, they also used many-body time-dependent density functional theory, or TDDFT, which successfully reproduces the three-step model of ultrafast STM: (one) tunnelling through a barrier thinned by the strong light field and concomitant energy gain, (two) further acceleration inside the junction, and (three) transmission into the sample.
Kai: It's impressive that they managed to get a theory-derived current burst duration of eight hundred sixty as from these models, which is a specific number derived from their analysis.
Lev: That specific duration is useful; for us on hardware, knowing the characteristic timescale helps us set appropriate time bins or coherence requirements for any measurement we attempt with this setup.
Conclusion: Mira: To wrap up, the paper concludes that they've shown robustness in their results, demonstrating that the sub-femtosecond confinement of waveform-controlled bursts remains robust against reasonable variations of experimental parameters like peak field strength, intensity ratio of SH to fundamental, junction width, and tip workfunction.
Kai: And they suggest a future path where replacing two-color pulses with single-cycle drivers could lead to a single isolated attosecond electron burst with waveform-controlled timing and direction.
Lev: If we can move toward those single-cycle drivers, that would simplify the experimental setup considerably for realizing any kind of actual quantum computation or error correction on this phenomenon.
Mira: The implications are huge because it suggests we could eventually achieve real-time observation of coherent electron-hole dynamics by combining these bursts with all-optical readout.
Kai: So, in summary, the paper "Attosecond current control and timing in a scanning tunnelling microscope" shows how two-color laser pulses can be used to dynamically control the direction of ultrafast tunnelling currents with sub-angstrom sensitivity under ambient conditions without thermal artifacts.
Lev: I just want to say that having this level of control is what makes it viable for any kind of complex, coherent operation we'd hope to build on top of these dynamics.
Mira: It’s a solid piece of work because it links the fundamental quantum dynamics directly to experimental control methods in a way that's very practical for next-generation microscopy.
Department of Physics, Technion—Israel Institute of Technology · Solid State Institute, Technion—Israel Institute of Technology · The Helen Diller Quantum Center · Institut des Sciences Mol´eculaires d’Orsay (ISMO), CNRS, Universit´e Paris-Saclay · Donostia International Physics Center
quant-ph
Submitted: 2025-07-14
Updated: 2026-09-30
Comments: 23 pages, 4 figures, Supplementary Information (SI). In this minor revision, we adjust the title to reflect the final title of the published manuscript. Please note that further minor revisions in the publishing process cannot be included in this ArXiv version and we refer the reader to the published version (see DOI below)
Journal ref: Nat. Photon. (2026)
DOI: 10.1038/s41566-026-02021-y
License: http://creativecommons.org/licenses/by/4.0/
Importance score: 90/100
The gist: Quantum tunnelling of electrons can be confined to sub-cycle time scales under strong light fields, and this work demonstrates robust attosecond directional control of ultrafast tunnelling currents
Key concepts
- Two-colour Laser Pulses
- The experiment uses an infrared fundamental pulse and its second harmonic (SH). By precisely controlling the time delay between these two pulses, the researchers create a specific waveform that breaks symmetry. This controlled asymmetry is what allows them to achieve sub-cycle timing of the tunnelling current.
- Sub-cycle Control
- This means controlling the tunnelling current dynamics on timescales shorter than one cycle of the driving laser field. The technique successfully enables seamless switching between tip-to-sample tunnelling and vice versa by exploiting the symmetry breaking caused by superimposing the two laser pulses.
- Three-step Transport Process
- The study models ultrafast STM as a three sequential steps: first, tunnelling through a barrier thinned by the light field with energy gain; second, acceleration inside the junction; and third, transmission into the sample. This model is confirmed by numerical simulations using time-dependent Schrödinger equation methods.
- Ambient Conditions Measurement
- Measurements were conducted at room temperature without thermal artifacts. This was achieved by using a sinusoidal modulation of the two-colour delay at 3.7 kHz to isolate laser-induced currents from static tunnelling, ensuring the observed dynamics are purely driven by the light field.
Terminology
Summary
Quantum tunnelling of electrons can be confined to sub-cycle time scales under strong light fields, and this work demonstrates robust attosecond directional control of ultrafast tunnelling currents in an STM junction using two-colour laser pulses. This capability enables triggering and imaging ultrafast charge dynamics at the spatio-temporal microscopy frontier, achieving sub-angstrom topographic sensitivity while operating under ambient conditions without thermal artifacts.
Core Methodology
The researchers induce STM tunnelling currents using two-colour laser pulses—an infrared fundamental pulse and its second harmonic (SH)—by superimposing them and controlling their relative time delay. This technique is employed to achieve a pronounced symmetry breaking of the resulting waveform, which enables sub-cycle control. Specifically, they employ an infrared laser pulse with its second harmonic in the same polarization plane and change their relative time delay.
The two-colour pulses lead to field waveforms with controlled symmetry breaking and enable sub-cycle control,
allowing them to seamlessly switch between tip-to-sample tunnelling and vice versa, as shown unambiguously and directly by measurements with a temporarily frozen tip.
Measurement Techniques
The experiment is conducted at ambient conditions (room temperature) using an electropolished Pt:Ir nanotip on a gold substrate. The microscope operates in constant-current measurement mode, where a static bias field drives the tunnelling current. To isolate the laser-induced currents from the static tunnelling current, they utilize a sinusoidal modulation
of the two-colour delay at an angular frequency of 3.7 kHz, which avoids artifacts associated with conventional lock-in approaches. This modulation allows them to measure the laser-induced current independently of the microscope feedback loop operating at a locking bandwidth below 500 Hz, thereby avoiding thermal artifacts.
Theoretical Framework and Analysis
The measurement data are projected onto several theoretical models: (i) an analytical strong-field (SF) model based on the van Vleck propagator; (ii) a single-active-electron model approach based on a numerical integration of the one-dimensional time-dependent Schrödinger equation (nTDSE); and (iii) many-body time-dependent density functional theory (TDDFT). The nTDSE successfully reproduces the three-step transport process in the non-adiabatic tunnelling regime, revealing a theory-derived current burst duration of 860 as.
Furthermore, they analyze power scaling, observing that the current scales approximately like a power law with order 3.8 at low powers and exhibits a soft kink
signature indicating the transition to the strong-field tunnelling regime.
Key Findings on Dynamics
The study reveals that the direction of the current is governed by the two-colour delay, as demonstrated by direct measurements with a frozen tip at zero bias. The reconstructed laser-induced current shows that Positive currents indicate that the asymmetric waveform of the two-colour field drives electrons in sub-cycle bursts from the nanotip to the sample.
They also demonstrate that peaks in the signal are correlated with small topographic protrusions,
suggesting an effective lateral spatial resolution of around 2 nm.
The analysis using TDDFT and nTDSE confirms a three-step model of ultrafast STM: (1) Tunnelling through a barrier thinned by the strong light field and concomitant energy gain, (2) further acceleration inside the junction, and (3) Transmission into the sample.
Robustness and Future Outlook
The results show that the sub-femtosecond confinement of waveform-controlled bursts remains robust against reasonable variations of experimental parameters,
including peak field strength, intensity ratio of SH to fundamental, junction width, and tip workfunction. The research suggests that replacing two-colour pulses with single-cycle drivers will lead to a single isolated attosecond electron burst with waveform-controlled timing and direction.
Future work envisions combining these bursts with all-optical readout for real-time observation of coherent electron-hole dynamics. Furthermore, they discuss the potential for bias-dependent measurements and combining quasi-static THz fields with near-infrared driving fields to further modulate the barrier shape.
The gist
In this work, two-colour laser pulses are used to induce and dynamically control the direction of ultrafast tunnelling currents in an STM junction, achieving sub-angstrom topographic sensitivity without thermal artifacts. The resulting measurements reveal a three-step transport process with a burst duration of 860 as, confirming that the sub-cycle waveform of the light pulse governs ultrafast electric current dynamics.
How it works
-
Two-colour pulses (fundamental and second harmonic) are superimposed, and their relative time delay is controlled using an interferometric setup with a linear delay stage and a piezo-mounted mirror modulated at 3.7 kHz to generate a lock-in signal without thermal artifacts.
Improvements for AI systems
As a fastidious and diligent researcher, I have analyzed this cutting-edge work on attosecond control of STM currents. The core breakthrough lies in achieving sub-angstrom spatial resolution (2 nm lateral) while dynamically controlling the direction of attosecond electron bursts using two-color laser pulses in an STM junction, all under ambient conditions without thermal artifacts.
Here are the specific improvements to AI systems that can be derived from this research:
) Improvements to AI Systems and Capabilities
-
A new class of
Attosecond Quantum Dynamics Simulators
capable of predicting electron transport in complex nanoscale junctions. -
Enhanced materials informatics for designing novel quantum devices based on predicted current asymmetry.
-
A real-time, closed-loop feedback system for attosecond charge manipulation in next-generation microscopy platforms.
) Specific Improvements and System Capabilities
-
The paper provides a robust theoretical framework (nTDSE, SF model, TDDFT) that accurately models the three-step non-adiabatic tunnelling process (tunnelling, acceleration, transmission).
-
The AI system can be trained on this framework to perform high-fidelity simulations of electron dynamics in arbitrary nanoscale junctions defined by varying geometry and material properties (e.g., tip/sample work functions).
-
The experimental results demonstrate that the directionality of the current is governed by two key controllable parameters:
a) The relative time delay between two laser colors (fundamental vs. second harmonic) to break symmetry.
b) The polarization angle of the combined field, which dictates the alignment with the nanotip geometry for maximum near-field enhancement.
- The AI system can be used to map
current directionality landscapes
across a parameter space defined by:
a) Junction width and material work functions (e.g., comparing Pt:Ir/Gold vs. other combinations).
b) Laser intensity ratios (SH/Fundamental ratio).
c) Field polarization angle.
- The AI system can predict the resulting current burst duration and its spatial profile (the
attosecond signature
) based on the input parameters, with quantified uncertainty estimates derived from NTDSE/TDDFT error analysis.
) What the Improved AI System Can Do
-
Predict optimal laser pulse configurations (two-color delay, polarization angle) required to achieve a specific electron transport direction (e.g., tip-to-sample vs. sample-to-tip current).
-
Design novel STM junction geometries that are predicted to exhibit desired sub-cycle current asymmetry or reversal based on the AI's predictive modeling of work function and geometric effects (as hinted in Fig 4a and S15).
-
Develop
digital twins
of experimental setups, allowing researchers to simulate the effect of ambient conditions, mechanical vibrations, and feedback loop bandwidth limitations on attosecond measurements before physical experimentation. -
Perform automated data analysis on STM current maps to rapidly identify sub-angstrom topographic features correlated with specific laser-induced current signatures (as seen in Fig 1d), enabling faster characterization of surface morphology at the atomic scale.
Abstract
Quantum tunnelling of electrons can be confined to the sub-cycle time scale of strong light fields, contributing decisively to the extreme time resolution of attosecond science. Because tunnelling also enables atomic-scale spatial resolution in scanning tunnelling microscopy (STM), integrating STM with light pulses has long been a key objective in ultrafast microscopy, spanning the picosecond and femtosecond domains, with first signatures of attosecond dynamics. However, while sub-cycle dynamics on the attosecond time scale are routinely controlled and determined with high precision, controlling the direction of attosecond currents and determining their duration have remained elusive in STM. Here, we induce STM tunnelling currents using two-colour laser pulses and dynamically control their direction, relying solely on the sub-cycle waveform of the pulses. Projecting our measurement data onto one-electron and many-body theory descriptions reveals a three-step transport process in the non-adiabatic tunnelling regime as the physical mechanism, with a theory-derived current burst duration of 860 as. Despite working under ambient conditions but free of thermal artifacts, we achieve sub-angström topographic sensitivity and a lateral spatial resolution of 2 nm. This unprecedented capability to directionally control attosecond bursts will enable triggering and imaging ultrafast charge dynamics at the spatio-temporal microscopy frontier of lightwave electronics.
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