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Subcycle observation of lightwave-driven Dirac currents in a topological surface band


Harnessing the carrier wave of light as an alternating-current bias may enable electronics at optical clock rates1. Lightwave-driven currents have been assumed to be essential for high-harmonic generation in solids2,3,4,5,6, charge transport in nanostructures7,8, attosecond-streaking experiments9,10,11,12,13,14,15,16 and atomic-resolution ultrafast microscopy17,18. However, in conventional semiconductors and dielectrics, the finite effective mass and ultrafast scattering of electrons limit their ballistic excursion and velocity. The Dirac-like, quasi-relativistic band structure of topological insulators19,20,21,22,23,24,25,26,27,28,29 may allow these constraints to be lifted and may thus open a new era of lightwave electronics. To understand the associated, complex motion of electrons, comprehensive experimental access to carrier-wave-driven currents is crucial. Here we report angle-resolved photoemission spectroscopy with subcycle time resolution that enables us to observe directly how the carrier wave of a terahertz light pulse accelerates Dirac fermions in the band structure of the topological surface state of Bi2Te3. While terahertz streaking of photoemitted electrons traces the electromagnetic field at the surface, the acceleration of Dirac states leads to a strong redistribution of electrons in momentum space. The inertia-free surface currents are protected by spin–momentum locking and reach peak densities as large as two amps per centimetre, with ballistic mean free paths of several hundreds of nanometres, opening up a realistic parameter space for all-coherent lightwave-driven electronic devices. Furthermore, our subcycle-resolution analysis of the band structure may greatly improve our understanding of electron dynamics and strong-field interaction in solids.

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Fig. 1: Concept of subcycle time-resolved ARPES.
Fig. 2: Energy streaking of the photoelectrons by p-polarized THz radiation.
Fig. 3: Acceleration of the electrons within the surface band by s-polarized THz radiation.
Fig. 4: Dynamics of electric current within the surface band.

Data availability

The data that support the findings of this study are available from the corresponding authors on request.


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We thank R. Höfer for discussions. The work in Marburg was supported by the Deutsche Forschungsgemeinschaft (DFG) through SFB 1083 and grant number HO 2295/7 (SPP 1666). Work in Regensburg was supported by the DFG through grant numbers HU 1598/2-1 and SFB 1277 (Project A05) and by the European Research Council through grant number 305003 (QUANTUMsubCYCLE). O.E.T. and K.A.K. were supported by the Russian Science Foundation (project number17-12-01047). A.K. was financially supported by KAKENHI number 17H06138.

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Nature thanks I. Katayama, S. Zhou and the other anonymous reviewer(s) for their contribution to the peer review of this work.

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Authors and Affiliations



J.G., U.H. and R.H. conceived the study. J.R., S.S., C.P.S., F.L., S.B. and J.G. carried out the experiment. K.A.K., O.E.T. and A.K. provided the samples and performed the transport measurements. J.R., C.L., J.G. and U.H. carried out the theoretical modelling. All authors analysed the data, discussed the results and contributed to writing the manuscript.

Corresponding authors

Correspondence to U. Höfer or R. Huber.

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Extended data figures and tables

Extended Data Fig. 1 Optical set-up.

a, THz generation via tilted pulse fronts in lithium niobate (LiNbO3). After the laser beam from the titanium:sapphire amplifier system has been reduced in diameter by a reflective telescope, a grating (G) induces a pulse front tilt. Cylindrical lenses (CL) image and focus the beam into a cryogenically cooled LiNbO3 crystal, where optical rectification generates intense THz radiation. A pair of wire-grid polarizers (P) controls the polarization state. b, Electro-optically detected THz waveform after transmission through the fused silica window of the vacuum chamber. Inset, amplitude spectrum of the transient shown in a. c, Set-up for generating UV pulses for photoemission. A lens (L; focal length, 1 m) gently focuses the fundamental titanium:sapphire pulses. A beam splitter (BS) separates 90% of the intensity for second-harmonic generation in a BBO crystal (SHG-BBO). Subsequent dispersion and polarization control is employed using a birefringent calcite plate and a dual-half-wave plate (Dual-λ/2). The third harmonic is generated in another BBO crystal (THG-BBO), separated from the fundamental pulses with a beam splitter (BS), and spatially and temporally (Delay) overlapped with the remaining fundamental pulses to generate the sum-frequency at the fourth harmonic (FHG-BBO). d, The resulting spectrum of the fourth harmonic is centred at λc = 201 nm with a full-width at half-maximum (FWHM) of 2.8 nm, corresponding to a Fourier limit of 22 fs.

Extended Data Fig. 2 Determination of the reflectivity of Bi2Te3.

a, Electro-optically detected THz transients after reflection off a Bi2Te3 (red) and a gold reference (blue) surface kept at a temperature of 77 K. b, Amplitude spectra of the field traces in a normalized to the amplitude of the gold spectrum. c, Reflection coefficient rp (black spheres) for parallel incidence obtained by dividing the amplitude spectra from Bi2Te3 and gold. The orange curve describes the reflection coefficient rp calculated using the corresponding Fresnel formula with a Drude–Lorentz model for the dielectric function of Bi2Te3 (see equation (1)). d, Transmission coefficient ts calculated using the modelled dielectric function.

Extended Data Fig. 3 Comparison of scattering mechanisms.

al, Calculated distribution functions at different delay times t for the experimental THz waveform with an amplitude of 2.4 kV cm−1. Experimental broadening is not accounted for. The Boltzmann equation used to compute these results includes only the relaxation term (af) or only the effective backscattering term (gl).

Extended Data Fig. 4 Broadening of the electron distribution.

ac, Experimental distribution functions (red and blue circles) for different delay times t compared to the equilibrium Fermi–Dirac distribution (solid black line).

Extended Data Fig. 5 Local current density in Bi2Te3.

a, Calculated current density j (colour scale) as a function of the delay time t and the electron excursion in the surface layer of Bi2Te3. The excursion was evaluated using the extracted scattering times of the charge carriers within the topologically protected surface state. The intense THz fields coherently drive Dirac fermions over several hundred nanometres before they undergo scattering. b, The red solid curve shows the simulated current dynamics calculated for scattering times of \({\tau }_{{\rm{R}}}={\tau }_{k\bar{k}}=1\hspace{2.22144pt}{\rm{ps}}\); the THz electric field is depicted as a dashed black curve.

Supplementary information

Video 1

Time-domain video of THz-accelerated Dirac fermions in the surface 2 bands of Bi2Te3. a, Angle-resolved photoemission spectra of the topologically protected surface band in Bi2Te3 as a function of the delay time, t, between an s-polarized THz field and the UV probe. The THz electric field directly accelerates Dirac fermions within the bands, transiently inducing an asymmetric occupation in momentum space and a net electron current flowing on the sample surface. b, THz waveform ETHz as retrieved via momentum streaking of the photoemitted electrons. The blue sphere traces the delay time of the respective photoemission spectrum shown in a.

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Reimann, J., Schlauderer, S., Schmid, C.P. et al. Subcycle observation of lightwave-driven Dirac currents in a topological surface band. Nature 562, 396–400 (2018).

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  • Dirac Current
  • Topological Surface States
  • Angle-resolved Photoemission Spectroscopy (ARPES)
  • Bi 2Te 3
  • Three-dimensional Topological Insulator

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