APS March Meeting 2013
Volume 58, Number 1
Monday–Friday, March 18–22, 2013;
Baltimore, Maryland
Session G41: Attosecond Physics and Optics
11:15 AM–2:15 PM,
Tuesday, March 19, 2013
Room: 350
Sponsoring
Unit:
DAMOP
Chair: Stephen Eckel, National Institute of Standards and Technology
Abstract ID: BAPS.2013.MAR.G41.7
Abstract: G41.00007 : Attosecond view of the photoelectric effect and optical-field-induced current in dielectrics
12:51 PM–1:27 PM
Preview Abstract
Abstract
Author:
Ralph Ernstorfer
(Fritz-Haber-Institut der Max-Planck-Gesellschaft)
Fundamental electronic processes in condensed matter like electron transport
on atomic length scales, the plasmonic response in metals or the dielectric
response in insulators occur on attosecond time scales. In the first part of
my talk, I discuss how a streak camera operating at optical frequencies
provides a time-resolved view of the photoelectric effect [1].
Photoelectrons emitted from metal surfaces by an attosecond extreme
ultraviolet laser pulse are time-stamped by a few-cycle
visible/near-infrared laser pulse. This technique allows for measuring the
relative emission time of valence and core electrons with a precision of
tens of attoseconds, thereby addressing the intrinsic dynamics of the
photoemission. I present recent studies of a free-electron metal [2] as well
as of oxygen-covered tungsten single crystals. The origin of the observed
attosecond delays in the emission of photoelectrons from different initial
states is discussed.
In the second part of the talk, I report on electric current in dielectrics
induced and controlled by ultrashort optical fields [3]. For very short
periods of time, electric fields exceeding 10 V/nm, i.e. fields
significantly beyond the threshold for dc dielectric breakdown, can be
applied to insulators. In this regime, insulators exhibit a highly nonlinear
dielectric response, resulting in an increase in conductivity by many orders
of magnitude. Applying 1.5-cycle laser pulses to unbiased
metal-dielectric-metal nanogaps, we demonstrate the generation of directly
measurable photocurrents whose magnitude and directionality can be
controlled with the carrier-envelope phase of the laser pulse, i.e. by the
shape of the laser electric field. Such currents can be switched on and off
on sub-femtosecond timescales as evidenced by employing two cross-polarized
and time-delayed pulses. The ultrafast field-controlled current generation
in a dielectric nanostructure may represent a first step towards the
realization of optical-field-controlled electronics.\\[4pt]
References:\\[0pt]
[1] A.L. Cavalieri et al., Nature 449, 1029 (2007).\\[0pt]
[2] S. Neppl et al., Phys. Rev. Lett. 109, 087401 (2012). \\[0pt]
[3] A. Schiffrin et al., Nature (2013), doi:10.1038/nature11567.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2013.MAR.G41.7