APS March Meeting 2017
Volume 62, Number 4
Monday–Friday, March 13–17, 2017;
New Orleans, Louisiana
Session P25: DCP Prize Session
2:30 PM–4:30 PM,
Wednesday, March 15, 2017
Room: 288
Sponsoring
Unit:
DCP
Chair: David Nesbitt, University of Colorado
Abstract ID: BAPS.2017.MAR.P25.4
Abstract: P25.00004 : Earle K. Plyler Prize Lecture: The Three Pillars of Ultrafast Molecular Science - Time, Phase, Intensity*
3:54 PM–4:30 PM
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Abstract
Author:
Albert Stolow
(University of Ottawa \& National Research Council)
We discuss the probing and control of molecular wavepacket dynamics in the
context of three main `pillars' of light-matter interaction: time, phase,
intensity.
Time: Using short, coherent laser pulses and perturbative matter-field
interactions, we study molecular wavepackets with a focus on the ultrafast
non-Born-Oppenheimer dynamics, that is, the coupling of electronic and
nuclear motions. Time-Resolved Photoelectron Spectroscopy (TRPES) is a
powerful ultrafast probe of these processes in polyatomic molecules because
it is sensitive both electronic and vibrational dynamics [1, 2]. Ideally,
one would like to observe these ultrafast processes from the molecule's
point of view -- the Molecular Frame -- thereby avoiding loss of information
due to orientational averaging. This can be achieved by Time-Resolved
Coincidence Imaging Spectroscopy (TRCIS) which images 3D recoil vectors of
both photofragments and photoelectrons, in coincidence and as a function of
time, permitting direct Molecular Frame imaging of valence electronic
dynamics during a molecular dynamics [3].
Phase: Using intermediate strength non-perturbative interactions, we apply
the second order (polarizability) Non-Resonant Dynamic Stark Effect (NRDSE)
to control molecular dynamics without any net absorption of light [4]. NRDSE
is also the interaction underlying molecular alignment and applies to
field-free 1D of linear molecules and field-free 3D alignment of general
(asymmetric) molecules [5]. Using laser alignment, we can transiently fix a
molecule in space, yielding a more general approach to direct Molecular
Frame imaging of valence electronic dynamics during a chemical reaction [6,
7].
Intensity: In strong (ionizing) laser fields, a new laser-matter physics
emerges for polyatomic systems [8] wherein both the single active electron
picture and the adiabatic electron response, both implicit in the standard
3-step models, can fail dramatically. This has important consequences for
all attosecond strong field spectroscopies of polyatomic molecules,
including high harmonic generation (HHG) [9]. We discuss an experimental
method, Channel-Resolved Above Threshold Ionization (CRATI), which directly
unveils the electronic channels participating in the attosecond molecular
strong field ionization response [10].
\textbf{[1]} Nature \underline {401}, 52, (1999). \textbf{[2]} Chemical
Reviews \underline {104}, 1719 (2004). \textbf{[3]} Science \underline
{311}, 219 (2006). \textbf{[4]} Science \underline {314}, 278 (2006).
\textbf{[5] }Physical Review Letters \underline {94}, 143002 (2005);
\underline {97}, 173001 (2006). \textbf{[6]} Science \underline {323}, 1464
(2009). \textbf{[7] }Nature Physics \underline {7}, 612 (2011). \textbf{[8]}
Physical Review Letters \underline {86}, 51 (2001); \underline {93}, 203402
(2004); \underline {93}, 213003 (2004). \textbf{[9]} Science \underline
{322}, 1207 (2008). \textbf{[10]} Science \underline {335}, 1336 (2012);
Physical Review Letters \underline {110}, 023004 (2013)
*This work was supported by the National Research Council of Canada and the Natural Sciences & Engineering Research Council.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2017.MAR.P25.4