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Fig. 9.34 The Ni 2p 3/2 and 2p 1/2 core level spectra for (a) [Ni 2 (EtCS 2 ) 4 I] 1 (8), (b) [Ni 2 ( n -
PrCS 2 ) 4 I] 1 (9), and (c) [Ni 2 ( n -BuCS 2 ) 4 I] 1 (10). The solid lines are the deconvoluted and sum
of the components [ 38 ]
Table 9.5 Binding energy (eV) and width of the peaks from the XPS Data for 7-10 and
corresponding [Ni 2 (RCS 2 ) 4 ]
Compound
Ni 2+ 2p 3/2
Ni 3+ 2p 3/2
Ni 2+ 2p 1/2
Ni 3+ 2p 1/2
853.8 (1.8) a
[Ni 2 (MeCS 2 ) 4 ][ 82 ]
[Ni 2 (EtCS 2 ) 4 ][ 38 ]
854.09 (1.53)
871.29 (2.08)
[Ni 2 ( n -PrCS 2 ) 4 ][ 38 ]
854.05 (1.53)
871.18 (2.03)
[Ni 2 ( n -BuCS 2 ) 4 ][ 38 ]
854.22 (1.56)
871.38 (1.98)
854.04 (1.8) a
855.0 (1.8) a
[Ni 2 (MeCS 2 ) 4 I] 1 (7)[ 82 ]
[Ni 2 (EtCS 2 ) 4 I] 1 (8)[ 38 ]
854.04 (1.53)
855.21 (1.68)
871.37 (2.18)
872.61 (2.23)
[Ni 2 ( n -PrCS 2 ) 4 I] 1 (9)[ 38 ]
854.16 (1.55)
855.26 (1.59)
871.47 (2.15)
872.65 (2.21)
[Ni 2 ( n -BuCS 2 ) 4 I] 1 (10)[ 38 ]
853.86 (1.53)
854.90 (1.53)
871.26 (2.20)
872.50 (2.20)
Full width at half-maximum values (fwhm) for peaks are given in parentheses
These values were corrected against the C 1s peak using a value of 284.6 eV
a Only Ni 2p 3/2 values were reported [ 82 ].
repulsion energy U on a MM unit originating from a strong electron-electron repulsion
on the nickel atoms. Schematic energy-band structure of [Ni 2 (RCS 2 ) 4 I] 1 is also shown
in Fig. 9.35 . HOMO-LUMO gap corresponding to U is 1.97 eV. Next HOMO is
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