scholarly journals Two-dimensional electronic spectroscopy signatures of the glass transition

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.

2008 ◽  
Vol 16 (22) ◽  
pp. 17420 ◽  
Author(s):  
Jeffrey A. Myers ◽  
Kristin L. Lewis ◽  
Patrick F. Tekavec ◽  
Jennifer P. Ogilvie

2017 ◽  
Vol 139 (41) ◽  
pp. 14733-14742 ◽  
Author(s):  
Yumin Lee ◽  
Saptaparna Das ◽  
Roy M. Malamakal ◽  
Stephen Meloni ◽  
David M. Chenoweth ◽  
...  

2020 ◽  
Vol 15 (13) ◽  
pp. 1996-2004
Author(s):  
Xuan Leng ◽  
Thanh Nhut Do ◽  
Parveen Akhtar ◽  
Hoang Long Nguyen ◽  
Petar H. Lambrev ◽  
...  

2014 ◽  
Vol 140 (8) ◽  
pp. 084701 ◽  
Author(s):  
Justin R. Caram ◽  
Haibin Zheng ◽  
Peter D. Dahlberg ◽  
Brian S. Rolczynski ◽  
Graham B. Griffin ◽  
...  

1976 ◽  
Vol 54 (14) ◽  
pp. 1454-1460 ◽  
Author(s):  
T. Tiedje ◽  
R. R. Haering

The theory of ultrasonic attenuation in metals is extended so that it applies to quasi one and two dimensional electronic systems. It is shown that the attenuation in such systems differs significantly from the well-known results for three dimensional systems. The difference is particularly marked for one dimensional systems, for which the attenuation is shown to be strongly temperature dependent.


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