scholarly journals Two-color two-dimensional Fourier transform electronic spectroscopy with a pulse-shaper

2008 ◽  
Vol 16 (22) ◽  
pp. 17420 ◽  
Author(s):  
Jeffrey A. Myers ◽  
Kristin L. Lewis ◽  
Patrick F. Tekavec ◽  
Jennifer P. Ogilvie
Author(s):  
Katherine W. Stone ◽  
Kenan Gundogdu ◽  
Daniel B. Turner ◽  
Xiaoqin Li ◽  
Steven T. Cundiff ◽  
...  

2014 ◽  
Vol 140 (12) ◽  
pp. 124312 ◽  
Author(s):  
Katherine A. Kitney-Hayes ◽  
Allison A. Ferro ◽  
Vivek Tiwari ◽  
David M. Jonas

2001 ◽  
Vol 115 (14) ◽  
pp. 6606-6622 ◽  
Author(s):  
John D. Hybl ◽  
Allison Albrecht Ferro ◽  
David M. Jonas

Author(s):  
Michael K. Yetzbacher ◽  
Eric Ryan Smith ◽  
Byungmoon Cho ◽  
Katherine A. Kitney ◽  
David M. Jonas

2010 ◽  
Vol 24 (3-4) ◽  
pp. 393-397 ◽  
Author(s):  
K. L .M. Lewis ◽  
J. A. Myers ◽  
F. Fuller ◽  
P. F. Tekavec ◽  
J. P. Ogilvie

Two-dimensional electronic spectroscopy is a sensitive probe of solvation dynamics. Using a pump–probe geometry with a pulse shaper [Optics Express15(2007), 16681-16689;Optics Express16(2008), 17420-17428], we present temperature dependent 2D spectra of laser dyes dissolved in glass-forming solvents. At low waiting times, the system has not yet relaxed, resulting in a spectrum that is elongated along the diagonal. At longer times, the system loses its memory of the initial excitation frequency, and the 2D spectrum rounds out. As the temperature is lowered, the time scale of this relaxation grows, and the elongation persists for longer waiting times. This can be measured in the ratio of the diagonal width to the anti-diagonal width; the behavior of this ratio is representative of the frequency–frequency correlation function [Optics Letters31(2006), 3354–3356]. Near the glass transition temperature, the relaxation behavior changes. Understanding this change is important for interpreting temperature-dependent dynamics of biological systems.


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