Molecular hydrodynamic theory of nonresonant Raman spectra in liquids: Third-order spectra

2002 ◽  
Vol 116 (5) ◽  
pp. 1979-1986 ◽  
Author(s):  
R. Aldrin Denny ◽  
David R. Reichman
Keyword(s):  
Raman Spectra ◽  
Hydrodynamic Theory ◽  
Third Order ◽  
Molecular Hydrodynamic

Fifth-order two-dimensional Raman spectra of CS2 are dominated by third-order cascades

1999 ◽  
Vol 111 (7) ◽  
pp. 3105-3114 ◽  
Author(s):  
David A. Blank ◽  
Laura J. Kaufman ◽  
Graham R. Fleming
Keyword(s):  
Raman Spectra ◽  
Two Dimensional ◽  
Third Order ◽  
Fifth Order

Raman spectra and third-order nonlinear optical Z-scan properties of MO-Nb2 O5 -TeO2 (M=Zn, Mg, Ca, Sr, Ba) glasses

2011 ◽  
Vol 8 (9) ◽  
pp. 2633-2636 ◽  
Author(s):  
Tomokatsu Hayakawa ◽  
Toshiki Suhara ◽  
Takeshi Fujiwara ◽  
Masayuki Nogami ◽  
Philippe Thomas
Keyword(s):  
Raman Spectra ◽  
Nonlinear Optical ◽  
Third Order

Metal oxide doping effects on Raman spectra and third-order nonlinear susceptibilities of thallium–tellurite glasses

2010 ◽  
Vol 62 (10) ◽  
pp. 806-809 ◽  
Author(s):  
Tomokatsu Hayakawa ◽  
Motohiro Koduka ◽  
Masayuki Nogami ◽  
Jean René Duclère ◽  
Andrei P. Mirgorodsky ◽  
...  
Keyword(s):  
Metal Oxide ◽  
Raman Spectra ◽  
Tellurite Glasses ◽  
Third Order ◽  
Doping Effects

scholarly journals Utilizing Microcavities To Suppress Third-Order Cascades in Fifth-Order Raman Spectra

2017 ◽  
Vol 8 (14) ◽  
pp. 3387-3391 ◽  
Author(s):  
Zhedong Zhang ◽  
Kochise Bennett ◽  
Vladimir Chernyak ◽  
Shaul Mukamel
Keyword(s):  
Raman Spectra ◽  
Third Order ◽  
Fifth Order

Probe size and 5th-order aberration

1987 ◽  
Vol 45 ◽  
pp. 134-135 ◽  
Author(s):  
Zhifeng Shao
Keyword(s):  
Electron Probe ◽  
Spherical Aberration ◽  
Wave Length ◽  
Cylindrical Symmetry ◽  
Electron Wave ◽  
Third Order ◽  
The Third ◽  
Probe Radius ◽  
Small Probe ◽  
Probe Size

A small electron probe has many applications in many fields and in the case of the STEM, the probe size essentially determines the ultimate resolution. However, there are many difficulties in obtaining a very small probe.Spherical aberration is one of them and all existing probe forming systems have non-zero spherical aberration. The ultimate probe radius is given byδ = 0.43Csl/4ƛ3/4where ƛ is the electron wave length and it is apparent that δ decreases only slowly with decreasing Cs. Scherzer pointed out that the third order aberration coefficient always has the same sign regardless of the field distribution, provided only that the fields have cylindrical symmetry, are independent of time and no space charge is present. To overcome this problem, he proposed a corrector consisting of octupoles and quadrupoles.

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