Two-photon IR pumped UV-Vis transient absorption spectroscopy of Dirac fermions in the 2D and 3D topological insulator Bi2Se3

TL;DR

This study reveals that in Bi2Se3 topological insulators, two-photon IR pumping significantly contributes to electron excitation even at low laser powers, due to the nonlinear response of Dirac surface states, as shown by UV-Vis transient absorption spectroscopy.

Contribution

It demonstrates the coexistence of one-photon and two-photon pumping regimes in Bi2Se3 and attributes high two-photon absorption efficiency to the nonlinearity of Dirac fermions.

Findings

Two-photon pumping occurs at low IR laser powers in Bi2Se3.

Two absorption bleaching mechanisms are identified and linked to phase-space filling and Pauli blocking.

Two-photon excitation involves Dirac surface states, not just bulk states.

Abstract

It is often taken for granted that in pump-probe experiments on the topological insulator (TI) Bi2Se3 using IR pumping with a commercial Ti:Sapphire laser [~800 nm (1.55 eV photon energy)], the electrons are excited in the one-photon absorption regime, even when pumped with absorbed fluences in the mJ cm-2 range. Here, using UV-Vis transient absorption (TA) spectroscopy, we show that even at low-power IR pumping with absorbed fluences in the mkJ cm-2 range, the TA spectra of the TI Bi2Se3 extend across a part of the UV and the entire visible region. This observation suggests unambiguously that the two-photon pumping regime accompanies the usual one-photon pumping regime even at low laser powers applied. We attribute the high efficiency of two-photon pumping to the giant nonlinearity of Dirac fermions in the Dirac surface states (SS). On the contrary, one-photon pumping is associated with the excitation of bound valence electrons in the bulk into the conduction band. Two mechanisms of absorption bleaching were also revealed since they manifest themselves in different spectral regions of probing. These two mechanisms were assigned to the filling of the phase-space in the Dirac SS and bulk states and the corresponding Pauli blocking.