Zuerch Lab
Zuerch Lab


In our laboratory we perform cutting-edge experiments using state-of-the art laser-driven attosecond sources in the extreme ultraviolet and soft X-ray range. We employ transient absorption/reflection spectroscopy in combination with transient X-ray scattering as methods to study fastest processes in real-time. Further, we perform experiments at facilities such as free-electron lasers to study dynamics using nonlinear X-ray spectroscopies, which will allow accessing dynamics at surfaces and interfaces.

Open research projects include

  • Measuring ultimate electronic switching times in technology-relevant semiconductor nanostructures by high-resolution femtosecond time-resolved imaging
  • Timing valley-specific carrier and spin localization in two-dimensional semiconductors
  • Multimodal probing of ultrafast spin dynamics in magnetic nanomaterials using attosecond diffraction spectroscopy
  • Surface-sensitive nonlinear diffraction spectroscopy of nanostructured quantum materials (at free-electron laser)

  • With an optical parametric amplification (OPA) system following an 800 nm Ti:Sapphire laser, we generate few-femtosecond, carrier-envelope phase (CEP) stabilized laser pulses throughout the visible and infrared regions in order to subsequently make high-harmonic generated (HHG) attosecond x-ray pulses spanning 20-600 eV. Combinations of such pulses are employed to perform core-level pump-probe experiments with high spatiotemporal resolution and atom-specificity where samples can remain under ultrahigh vacuum and ultracold temperature conditions.

    Fig. 1. A moirè lattice consisting of two hexagonal 2D layers twisted relative to one another by an angle θ gives rise to a periodic potential of quantum wells with depths on the order of 100 meV.

    We are specifically interested in studying and controlling charge carrier and spin dynamics in novel superlattice structures. We are specifically interested in moirè lattices of twisted van Der Waals 2D materials because they provide a highly-ordered, tunable, and periodic platform for localized excitons, spins, and charged particles (Fig. 1). Such materials are of interest for quantum information, spintronics, and optoelectronics applications, as well as for the study of canonical models of phase transitions, symmetry-breaking, and electron correlations in condensed matter and many-body physics.

    We actively collaborate with materials scientists, theorists, and FEL facilities around the world to answer questions like, what is the influence of the moirè potential on the band structure and optoelectronic properties? Can we manipulate the spatiotemporal dynamics of quasiparticles in the superlattice structures in real time? What kinds of couplings exist between the spin, orbit, charge, and lattice degrees of freedom? Can we control how long these couplings persist before decoherence sets in?


    Yu, H.; Liu, G. bin; Tang, J.; Xu, X.; Yao, W. Moiré Excitons: From Programmable Quantum Emitter Arrays to Spin-Orbit–Coupled Artificial Lattices. Science Advances 2017, 3 (11), 1–8. https://doi.org/10.1126/sciadv.1701696.

    Tran, K.; Moody, G.; Wu, F.; Lu, X.; Choi, J.; Kim, K.; Rai, A.; Sanchez, D. A.; Quan, J.; Singh, A.; et al. Evidence for Moiré Excitons in van Der Waals Heterostructures. Nature 2019, 567 (7746), 71–75. https://doi.org/10.1038/s41586-019-0975-z.

    Jin, C.; Regan, E. C.; Yan, A.; Iqbal Bakti Utama, M.; Wang, D.; Zhao, S.; Qin, Y.; Yang, S.; Zheng, Z.; Shi, S.; et al. Observation of Moiré Excitons in WSe2/WS2 Heterostructure Superlattices. Nature 2019, 567 (7746), 76–80. https://doi.org/10.1038/s41586-019-0976-y.

    Seyler, K. L.; Rivera, P.; Yu, H.; Wilson, N. P.; Ray, E. L.; Mandrus, D. G.; Yan, J.; Yao, W.; Xu, X. Signatures of Moiré-Trapped Valley Excitons in MoSe 2 /WSe 2 Heterobilayers. Nature 2019, 567 (7746), 66–70. https://doi.org/10.1038/s41586-019-0957-1.

    Bloch, I. Ultracold Quantum Gases in Optical Lattices. Nature Physics 2005, 1 (1), 23–30. https://doi.org/10.1038/nphys138.

    Wu, F.; Lovorn, T.; Macdonald, A. H. Theory of Optical Absorption by Interlayer Excitons in Transition Metal Dichalcogenide Heterobilayers. 2018, 035306, 1–10. https://doi.org/10.1103/PhysRevB.97.035306.

  • Solids can be used as a medium to generate harmonics of an intense laser pulse. While gas-phase higher harmonic generation (HHG) is widely used in generating attosecond pulses, recently, solid state higher harmonic generation (sHHG) has gained attention. Compared to HHG, sHHG has richer dynamics due to the periodic structure of the dense medium. Rather than the well-established semi-classical tunnel ionization description that explains HHG (c-d), sHHG process involves tunnel ionization followed by interactions of the charge carriers with the periodic lattice potentials. Therefore, sHHG contains valuable information about the band structure of solids (a-b). Uniquely equipped with a CEP stabilized tunable source and synchronized OPA’s, we are aiming to elucidate interband and intraband dynamics in solids at the strong field regime. We want to develop sHHG as a solid-state spectroscopy tool capable of answering questions about ultrafast dynamics. On this front, we are interested in several classes of materials such as semiconductors, 2D materials and perovskites.

  • Free electron lasers (FELs) generate high intensity, ultrafast and coherent X-Ray pulses that are tunable to the elemental edges of interest. We develop and use nonlinear X-Ray techniques at FELs to investigate ultrafast dynamics in solids. Specifically, X-Ray Second Harmonic Generation (XUV-SHG) has been our main spectroscopic tool. In principle, XUV-SHG is particularly attractive as it unites the core-level specificity of X-Ray spectroscopies with the unique properties of second harmonic generation.
    We have studied bulk non-centrosymmetric crystals using XUV-SHG [1,2]. In these crystals due to ion displacements in the unit cell, emergent order such as ferroelectricity appears which makes them an ideal candidate for XUV-SHG studies. In the case of the polar ferroelectric LiOsO3, we demonstrated that the polar phase establishes as a result of Li ion displacements, while by investigating the polarization of XUV-SHG emitted from a well-studied ferroelectric, LiNbO3, we established that the long-accepted theories of angular anisotropy in optical SHG is applicable to XUV-SHG. Along with these studies, we also contributed to the investigation of tabletop sources that achieve XUV-SHG [3] and demonstrated the capability of XUV-SHG to investigate challenging buried interfaces [4].

    1-E. Berger, S. Jamnuch, C. Uzundal, C. Woodahl, H. Padmanabhan, P. Manset, Y. Hirata,I. Matsuda, V. Goplan, Y. Kubota,et al., “Direct observation of symmetry-breaking in a ‘ferroelectric’ polar metal,” (2020), arXiv:2010.03134.

    2-C. B. Uzundal, S. Jamnuch, E. Berger, C. Woodahl, P. Manset, Y. Hirata, T. Sumi, A. Amado, H. Akai, Y. Kubota, et al., “Polarization-Resolved Extreme Ultraviolet Second Harmonic Generation from LiNbO3” (2021), arXiv:2104.01313

    3-T. Helk, E. Berger, S. Jamnuch, L. Hoffmann, A. Kabacinski, J. Gautier, F. Tissandier, J. P. Goddet, H.-T. Chang, J. Oh, C. D. Pemmaraju, T. A. Pascal, S. Sebban, C. Spielmann, M. Zuerch. “Table-top Nonlinear Extreme Ultraviolet Spectroscopy” (2021), arXiv:2009.05151

    4-C. P. Schwartz, S. L. Raj, S. Jamnuch, C. J. Hull, P. Miotti, K. Lam, D. Nordlund, C. B.Uzundal, C. D. Pemmaraju, L. Foglia,et al., “Angstrom-resolved Interfacial Structure in Organic-Inorganic Junctions,” (2020), arXiv:2005.01905.

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