Abstract

We demonstrate ultrafast terahertz (THz) field emission from a tungsten nanotip enabled by local field enhancement. Characteristic electron spectra which result from acceleration in the THz near-field are found. Employing a dual frequency pump–probe scheme, we temporally resolve different nonlinear photoemission processes induced by coupling near-infrared (NIR) and THz pulses. In the order of increasing THz field strength, we observe THz streaking, THz-induced barrier reduction (Schottky effect) and THz field emission. At intense NIR-excitation, the THz field emission is used as an ultrashort, local probe of hot electron dynamics in the apex. A first application of this scheme indicates a decreased carrier cooling rate in the confined tip geometry. Summarizing the results at various excitation conditions, we present a comprehensive picture of the distinct regimes in ultrafast photoemission in the near- and far-infrared.

Highlights

  • Terahertz (THz) radiation with a photon energy of few millielectron-volts is commonly regarded as being non-ionizing, and finds widespread applications in imaging, sensing and spectroscopy [1,2,3]

  • We demonstrate THz field emission enabled by the high field enhancement at tungsten nanotips

  • The THz field strength is controlled by rotation of the BBO crystal (figure 2(g)), and the pulses are coupled into an high vacuum chamber (10−8 mbar range) through a 500 μm thick, Brewster-angled silicon window

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Summary

Introduction

Terahertz (THz) radiation with a photon energy of few millielectron-volts (meV) is commonly regarded as being non-ionizing, and finds widespread applications in imaging, sensing and spectroscopy [1,2,3]. The linear fielddependence of the kinetic energy cutoff maps the THz focus (blue, figure 1(e)), whereas the corresponding electron yield (red) demonstrates a higher localization due to the tunneling nonlinearity [15]. Assisted by optical field enhancement at the tungsten tip [30], the short NIR-pulse generates photoelectrons localized to the apex [19, 27, 29, 31,32,33,34,35,36,37,38], which are accelerated in the momentary THz potential.

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