Collective vibrational modes in molecular assembly of DNA and its application to biological systems. Low frequency Raman spectroscopy

1985 ◽  
Vol 82 (1) ◽  
pp. 531-535 ◽  
Author(s):  
Hisako Urabe ◽  
Hideyuki Hayashi ◽  
Yasunori Tominaga ◽  
Yoshifumi Nishimura ◽  
Kenji Kubota ◽  
...  
2017 ◽  
Vol 19 (47) ◽  
pp. 32099-32104 ◽  
Author(s):  
Alexander Krylov ◽  
Alexander Vtyurin ◽  
Petko Petkov ◽  
Irena Senkovska ◽  
Mariia Maliuta ◽  
...  

Raman spectroscopy and Molecular Dynamic simulations were applied to study low-frequency vibrations of a flexible metal–organic framework DUT-8(Ni).


1995 ◽  
Vol 407 ◽  
Author(s):  
R. Sommer ◽  
J. Toulouse ◽  
H. Jain

ABSTRACTWe have performed a study on low frequency modes in several alkali silicate glasses by Raman spectroscopy. The Boson peak region is analyzed with a single parameter ω0 which is believed to characerize the density of states of the system. Analysis of the dependence of ω0 on the nature and concentration of the alkali suggests that the position of the Boson peak is essentially governed by the ratio “force constant” over “mass” of localized oscillator modes. At lower frequency (below 30 cm−1), the “excess” intensity can be explained by considering secondorder processes of the same vibrational modes, superimposed on other (possibly relaxational) modes.


2006 ◽  
Vol 55 (8) ◽  
pp. 4091
Author(s):  
Ma Shi-Hua ◽  
Shi Yu-Lei ◽  
Xu Xin-Long ◽  
Yan Wei ◽  
Yang Yu-Ping ◽  
...  

1994 ◽  
Vol 269 (49) ◽  
pp. 31047-31050
Author(s):  
S Jeyarajah ◽  
L M Proniewicz ◽  
H Bronder ◽  
J R Kincaid

Soft Matter ◽  
2021 ◽  
Author(s):  
Brian Tighe ◽  
Karsten Baumgarten

We determine how low frequency vibrational modes control the elastic shear modulus of Mikado networks, a minimal mechanical model for semi-flexible fiber networks. From prior work it is known that...


1995 ◽  
Vol 398 ◽  
Author(s):  
A.R. Guo ◽  
C.-S. Tu ◽  
Ruiwu Tao ◽  
R.S. Katiyar ◽  
Ruyan Guo ◽  
...  

ABSTRACTThe longitudinal (LO) and transverse (TO) A1 vibrational modes have been measured between 30-1200 cm−1 as a function of temperature (30–1240 K) for CsTiOAsO4 (CTA). The frequencies for all corresponding Raman components shifted to lower frequencies on increasing the temperature, however, there is no typical soft-mode like behavior observed in the measured frequency range. The relative intensities of the low frequency bands increase dramatically with increasing temperature due to high mobility of Cs+ ion. A higher symmetry structure taking place above 940K has been confirmed by changes in the phonon spectra.


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