2010
DOI: 10.1007/s00723-010-0178-0
|View full text |Cite
|
Sign up to set email alerts
|

EPR Study of 5-Chlorosalicylate-Cu(II)-3-Pyridylmethanol Ternary Complex Systems in Frozen Water–Methanol Solutions

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2011
2011
2021
2021

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 5 publications
(1 citation statement)
references
References 24 publications
0
1
0
Order By: Relevance
“…The rhombicity of the Cu site arises from having an approximate D 2 h symmetry that allows for d z 2 mixing into the d x 2 – y 2 ground state; from the g x and g y values for mode I and the ternary mode I-like complex, ≈2% of d z 2 mixing can be estimated, with minimal tetrahedral distortion according to the f factor (Table ). In both cases, a superhyperfine pattern is evident in the second derivative of the EPR spectrum that can be simulated by considering the coupling of four N nuclei (Figure S10 and Table S4). However, EPR simulations reveal that the slight differences in the N superhyperfine patterns of the two complexes are due to having different N superhyperfine coupling values: while mode I can be simulated with two sets of two magnetically equivalent N atoms with N A iso = 45 and 28 MHz, the ternary mode I-like species requires different couplings for each N (Table S4).…”
Section: Discussionmentioning
confidence: 90%
“…The rhombicity of the Cu site arises from having an approximate D 2 h symmetry that allows for d z 2 mixing into the d x 2 – y 2 ground state; from the g x and g y values for mode I and the ternary mode I-like complex, ≈2% of d z 2 mixing can be estimated, with minimal tetrahedral distortion according to the f factor (Table ). In both cases, a superhyperfine pattern is evident in the second derivative of the EPR spectrum that can be simulated by considering the coupling of four N nuclei (Figure S10 and Table S4). However, EPR simulations reveal that the slight differences in the N superhyperfine patterns of the two complexes are due to having different N superhyperfine coupling values: while mode I can be simulated with two sets of two magnetically equivalent N atoms with N A iso = 45 and 28 MHz, the ternary mode I-like species requires different couplings for each N (Table S4).…”
Section: Discussionmentioning
confidence: 90%