Determination of triplet-energy levels in azomethine dyes by energy-transfer measurements

1975 ◽  
Vol 97 (11) ◽  
pp. 3090-3096 ◽  
Author(s):  
W. G. Herkstroeter
Keyword(s):  
Energy Transfer ◽  
Energy Levels ◽  
Triplet Energy

The influence of triplet energy levels of bridging ligands on energy transfer processes in Ir(iii)/Eu(iii) dyads

2011 ◽  
Vol 40 (43) ◽  
pp. 11410 ◽  
Author(s):  
Weili Jiang ◽  
Bin Lou ◽  
Jianqiang Wang ◽  
Hongbin Lv ◽  
Zuqiang Bian ◽  
...  
Keyword(s):  
Energy Transfer ◽  
Energy Levels ◽  
Triplet Energy ◽  
Bridging Ligands ◽  
Transfer Processes

Definition and determination of the triplet-triplet energy transfer reaction coordinate

2014 ◽  
Vol 140 (3) ◽  
pp. 034102 ◽  
Author(s):  
Felipe Zapata ◽  
Marco Marazzi ◽  
Obis Castaño ◽  
A. Ulises Acuña ◽  
Luis Manuel Frutos
Keyword(s):  
Energy Transfer ◽  
Transfer Reaction ◽  
Reaction Coordinate ◽  
Triplet Energy ◽  
Triplet Energy Transfer

Determination of the distance for triplet energy transfer in the faujasite NaY

1995 ◽  
Vol 233 (1-2) ◽  
pp. 5-8 ◽  
Author(s):  
J.C. Scaiano ◽  
Nanci Camara de Lucas ◽  
John Andraos ◽  
Hermenegildo García
Keyword(s):  
Energy Transfer ◽  
Triplet Energy ◽  
Triplet Energy Transfer

A quantitative approach to inner shell losses

1978 ◽  
Vol 36 (1) ◽  
pp. 526-527 ◽  
Author(s):  
R.D. Leapman ◽  
P. Rez ◽  
D.F. Mayers
Keyword(s):  
Energy Transfer ◽  
Cross Section ◽  
Cross Sections ◽  
Accurate Determination ◽  
Background Intensity ◽  
Core Excitation ◽  
Quantitative Basis ◽  
Cross Section Differential ◽  
Bound Electrons

Microanalysis by EELS has been developing rapidly and though the general form of the spectrum is now understood there is a need to put the technique on a more quantitative basis (1,2). Certain aspects important for microanalysis include: (i) accurate determination of the partial cross sections, σx(α,ΔE) for core excitation when scattering lies inside collection angle a and energy range ΔE above the edge, (ii) behavior of the background intensity due to excitation of less strongly bound electrons, necessary for extrapolation beneath the signal of interest, (iii) departures from the simple hydrogenic K-edge seen in L and M losses, effecting σx and complicating microanalysis. Such problems might be approached empirically but here we describe how computation can elucidate the spectrum shape.The inelastic cross section differential with respect to energy transfer E and momentum transfer q for electrons of energy E0 and velocity v can be written as

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