7 Redox Properties of Polymetallic Systems THOMAS J. MEYER
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University of North Carolina, Chapel Hill, N. C. 27514
The redox properties of three classes of polymetallic systems were studied. In compounds with strong metal-metal bonds, multiple oxidation state properties are found for metal clusters and in compounds where bridging ligands reinforce the metal-metal bond. Compounds with weak interactions between metal ion sites have electronic and chemical properties that are essentially those of isolated monomeric complexes. Electronic interactions between metal centers, electrostatic effects, and statistical effects affect reduction potential values. In systems more complicated than dimers, there are ambiguities about the site of oxidation. In mixed -valence ions, intervalence transfer bands appear; their energies and intensities are functions of both bridging and non-bridging ligand effects. When metal-metal interactions across a bridging ligand are sufficiently strong, the system is delocalized and chemical and electronic properties are significantly modified. ecent w o r k has l e d to the synthesis of a v a r i e t y of c o m p o u n d s i n w h i c h m e t a l atoms or ions are h e l d i n close p r o x i m i t y b y c h e m i c a l linkages. T h e s e p o l y m e t a l l i c c o m p o u n d s represent a n e w class of m a t e rials that h a v e d i s t i n c t i v e c h e m i c a l a n d p h y s i c a l properties, a n d i n some systems the p r o p e r t i e s c a n be v a r i e d s y s t e m a t i c a l l y b y c h e m i c a l synthesis. T h e c o m p o u n d s are of interest because of possible c o o p e r a t i v e
chemical
a n d electronic interactions b e t w e e n the c h e m i c a l l y l i n k e d m e t a l centers. I n the f u t u r e i t m a y p r o v e p o s s i b l e :
(a)
to create s o l i d state m a t e r i a l s
that h a v e c o n t r o l l a b l e , a n d p e r h a p s u n u s u a l , e l e c t r i c a l c o n d u c t i v i t y p r o p erties; ( b ) to p r e p a r e p o l y m e r i c c o m p l e x e s w h i c h i n s o l u t i o n h a v e p r o p erties that are i n t e r m e d i a t e b e t w e e n those of s o l i d state materials a n d those of s i m p l e m o n o m e r i c complexes; a n d ( c ) to devise c h e m i c a l systems i n w h i c h cooperative c h e m i c a l interactions l e a d to net, m u l t i p l e - e l e c t r o n r e d o x processes, or to s i m u l t a n e o u s , t w o - or m o r e site reactions. 73 In Inorganic Compounds with Unusual Properties; King, R.; Advances in Chemistry; American Chemical Society: Washington, DC, 1976.
74
INORGANIC
COMPOUNDS
WITH
UNUSUAL
PROPERTIES
M y i n t e n t i o n is to d e v e l o p , as s y s t e m a t i c a l l y as possible, t h e r e d o x properties
of
polymetallic
systems
i n solution.
A n understanding
of
r e d o x p r o p e r t i e s a n d of m e t a l - m e t a l interactions is essential i n o r d e r to e x p l o i t p o l y m e t a l l i c systems. findings
M o s t of the examples
are b a s e d
on
the
of m y o w n r e s e a r c h g r o u p w i t h t h r e e different classes of c o m
p o u n d s w h i c h differ i n the n a t u r e a n d / o r the extent of the m e t a l - m e t a l interaction. Strong, Direct Metal-Metal
Bonding
A m e t a l - m e t a l b o n d has a p r o f o u n d effect o n the p r o p e r t i e s of t h e
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l i n k e d m e t a l centers
(I).
W i t h a metal-metal bond:
(a)
absorption
b a n d s are present w h i c h c a n b e assigned to transitions b e t w e e n b o n d i n g a n d a n t i b o n d i n g m e t a l - m e t a l o r b i t a l s (2, 3, 4);
(b)
multiple oxidation
state properties c a n a p p e a r that are b a s e d o n the m e t a l - m e t a l b o n d
or
b o n d s ; a n d ( c ) c h e m i c a l p r o p e r t i e s are s t r o n g l y m o d i f i e d . A s a n e x a m p l e of the latter, H u g h e y a n d B o c k d e m o n s t r a t e d that
[(7r-C Hr,)Mo(CO) ]2 s
and
3
induced homolytic
fission
related
(Reaction
b y flash p h o t o l y s i s
compounds
undergo
the m o n o m e r i c
1);
fragments
are p r o d u c e d react r a p i d l y w i t h a v a r i e t y of substrates u n d e r i n w h i c h t h e p a r e n t c o m p o u n d is u n r e a c t i v e (4,
[ ( π - 0 , Η ) M o ( C O ),] ο Γ>
hv — lOMO^AT
that
conditions
6).
2 G r - C H ) M o (CO) 5
sec'
1
(5) light-
5
(1)
8
1
R e d o x processes i n r e l a t i v e l y s i m p l e m e t a l - m e t a l b o n d s l e a d to a breakdown solvent
i n p r i m a r y structure
a n d R e a c t i o n 2b
(9)1.
R e a c t i o n 2a (7,
[see
However, 2e
reversible
•2U-C H )Fe(CO) S 5
[(ir-C H )Fe(C0) ] — s
2
5
+
2
2
+
where
8)
electron
5
2
2
2e"
(
7 r
n o n a q u e o u s solvents (CO)]
4
(10,11)
b y b r i d g i n g (1). revealed
5
2
reinforce
V o l t a m m e t r i c experiments
that the
( F i g u r e 1)
(2b)
-C H )Fe(CO) 5
cluster systems
and [ ( ^ C H ) F e S ] 5
5
(10)
4
5
and
[(^C H5)FeS]4 5
".
5
5
5
5
5
5
4
2 +
/ °/+ /
4
5
and
[(ΤΓ-0 Η )-
(13)
and
(12)
5
FeS] -[(7r-C H )FeS] (PF6)-[(7r-C H5)FeS] (PF6) 4
5
remain intact
T h e s t r u c t u r a l details of the c o m p o u n d s
[(7r-C H )Fe(CO)]4-[(7r-C H )Fe(CO)]4(PFe) 5
in
[(7r-C H )Fe-
i n s e v e r a l different m o l e c u l a r o x i d a t i o n states : [ ( 7 r - C H ) F e ( C O ) ] 3 + / 2 + / + / 0 /
=
(2a)
+
S
c a n o c c u r i n m e t a l clusters a n d i n c o m p o u n d s w h e r e l i g a n d s the m e t a l - m e t a l b o n d
S
transfer
4
2
n e t i c field M o s s b a u e r d a t a f o r [ ( ^ C H ) F e ( C O ) ] ( P F e ) 5
5
4
5
(14)
5
mag
are c o n
sistent w i t h a m o d e l i n w h i c h r e d o x properties are c a r r i e d , at least i n p a r t ,
In Inorganic Compounds with Unusual Properties; King, R.; Advances in Chemistry; American Chemical Society: Washington, DC, 1976.
7.
Polymetallic Systems
MEYER
75
Inorganic Chemistry
Figure 1. Structure of the [(TT-CsH^FeiCO)'], cluster unit (14)
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b y delocalized m e t a l - m e t a l bonding a n d antibonding orbitals. T h e clusters a p p e a r to u n d e r g o f a c i l e e l e c t r o n transfer C h e m i c a l l y reversible
electron
(15).
transfer processes h a v e
also
been
r e p o r t e d for l i g a n d - b r i d g e d complexes of C r , M o , W , M n , F e , R u , C o , a n d N i b y D e s s y a n d co-workers i n 1,2-dimethoxyethane
who used electrochemical
for di-ter£-phosphine-bridged d e r i v a t i v e s of C5H )Fe(CO)] (Ph P(CH )3PPh ) 5
2
2
2
2
2 + / + / 0
techniques
S i m i l a r b e h a v i o r was
(16, 17, 18, 19).
reported
[(7r-C H )Fe(CO)2]2; 5
(20,
21).
[(w-
5
The multiple oxida-
t i o n state b e h a v i o r i n l i g a n d - b r i d g e d systems also seems to arise b e c a u s e of b o n d i n g or a n t i b o n d i n g m e t a l - m e t a l o r b i t a l s . a n d f r o z e n s o l u t i o n E P R d a t a for the o n c e - o x i d i z e d Fe(CO)] (m-Ph PCH=CHPPh ) 2
2
2
Fe- - -
( F i g u r e 2)
F o r example, f o r m of
ESCA
[(7r-C H )5
indicate that
5
oxidation
-Fe
Ph Ph"" ^ ç — ç /
Figure 2. Proposed structure of [(Tr-C H )Fe (CO)] (cis-Ph PCH= CHPPh )
^Ph
5
2
5
2
2
+
occurs at i r o n a n d that the u n p a i r e d e l e c t r o n resides i n a m e t a l - m e t a l o r b i t a l (22, 23). (CO)SR]
2
+ / 0
occurs f r o m
F r o m s t r u c t u r a l studies of the system
, Connelly and D a h l concluded an antibonding
metal-metal bond
(24).
F e - F e orbital
[(7r-C H )Fe5
that one-electron that also
gives a
H o w e v e r , i n m a n y of these systems,
i n f o r m a t i o n is n e e d e d a b o u t the electronic structure.
5
oxidation partial detailed
I t is c o n c e i v a b l e
that i n s o m e cases t h e o b s e r v e d r e d o x b e h a v i o r is c a r r i e d b y
orbitals
w h i c h are l a r g e l y l i g a n d b a s e d , a n d i n r e l a t e d systems i t is n o t a l w a y s clear w h e t h e r the m e t a l - m e t a l i n t e r a c t i o n occurs p r i m a r i l y t h r o u g h s p a c e or t h r o u g h a b r i d g i n g l i g a n d (see
below).
In Inorganic Compounds with Unusual Properties; King, R.; Advances in Chemistry; American Chemical Society: Washington, DC, 1976.
76
INORGANIC
COMPOUNDS WITH
UNUSUAL
PROPERTIES
T h e l i g a n d - b r i d g e d systems a r e a t t r a c t i v e i n terms o f r e d o x
proper
ties because of c h e m i c a l v e r s a t i l i t y a n d t h e p o s s i b i l i t y of p r e p a r i n g polymeric compounds.
T h e c o m p o u n d s are also of interest e l e c t r o n i c a l l y
since, f o r a g i v e n m e t a l , t h e o r b i t a l c h a r a c t e r of t h e m e t a l - m e t a l i n t e r a c t i o n c a n b e v a r i e d . F o r e x a m p l e , t h e ions Ph PCH=CHPPh ) 2
2
a n d d -d?
+
[(7r-C H )Fe(CO)] (cis5
and [ ( 7 r - C H 5 ) F e ( C O ) S C H ] 2 5
3
+
2
5
are f o r m a l l y d - d 6
7
cases, r e s p e c t i v e l y , b u t i n b o t h ions there is a p a r t i a l m e t a l -
5
metal bond.
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Weak Interactions between Metals through a Bridging
Ligand
W h e n m e t a l - m e t a l interactions t h r o u g h a c o n n e c t i n g l i g a n d b r i d g e are w e a k , t h e m e t a l centers h a v e t h e e l e c t r o n i c a n d c h e m i c a l p r o p e r t i e s of i s o l a t e d , m o n o m e r i c
c o m p l e x e s except f o r c e r t a i n s p e c i a l effects.
If
a p p r o p r i a t e m o n o m e r i c c o m p l e x e s u n d e r g o r e v e r s i b l e e l e c t r o n transfer, a r e l a t e d l i g a n d - b r i d g e d system w i l l u n d e r g o a series of e l e c t r o n transfer steps i n w h i c h e a c h of t h e m e t a l sites i n t u r n u n d e r g o e s o x i d a t i o n o r Figure 3. Structure of the Ι,Γ-polyferrocenes. η = 0: Biferrocene (FcFc), η = I : Ι,Γ-terferrocene (Fc-Fc-Fc) and η = 2: Ι,Γ-quatreferrocene (Fc-Fc-Fc-Fc) 9
reduction. 3), Fc)
Examples
are k n o w n
for the
Ι,Ι'-polyferrocenes
(C H5)Fe(C H4-C5H )Fe(C H4-C5H )Fe(C H5) 5
5
3 + / 2 V V 0
]
4
5
4
(bipy) ClRu(pyz)Ru(bipy) (pyz)RuCl(bipy) 2
bipy =
5
( 2 5 ) , a n d for ligand-bridged 2
2,2'-bipyridine)
( 2 6 , 2 7 , 28).
complexes 2
7 + / 6 + / 5 + / 4 +
(Figure [Fc-Fc-
3 + / 2 + / + / 0
of r u t h e n i u m ,
(pyz =
pyrazine,
R e d u c t i o n potentials w i l l
e l e c t r o n i c effects ( r e s o n a n c e a n d i n d u c t i v e )
i f t h e y are large
reflect enough,
a n d they w i l l b e affected b y s i m p l e electrostatic effects. A s a n e x a m p l e of t h e latter, i n t h e c o m p l e x :
t h e m e t a l centers are e l e c t r o n i c a l l y i s o l a t e d , a n d y e t t h e y are o x i d i z e d at s l i g h t l y h i g h e r potentials t h a n r e l a t e d m o n o m e r i c c o m p l e x e s b e c a u s e of t h e h i g h e r c h a r g e o n t h e d i m e r ( 2 9 , 30). I f there is s y m m e t r y , s t a t i s t i c a l effects a p p e a r .
T o m , Creutz, and
T a u b e n o t e d that i n t h e e q u i l i b r i u m i n R e a c t i o n 3 ( w h e r e 4 , 4 ' - b i p y
=
4 , 4 ' - b i p y r i d i n e ) , t h e m i x e d - v a l e n c e i o n is f a v o r e d b y a statistical f a c t o r of 4 e v e n i n t h e absence of other effects (31).
W h e n o n e compares t h e
In Inorganic Compounds with Unusual Properties; King, R.; Advances in Chemistry; American Chemical Society: Washington, DC, 1976.
7.
Polymetallic
MEYER
77
Systems
(NH3)5Ru(4,4'-bipy)Ru(NH3)5
+
6 +
( N H ) R u (4,4'-bipy) R u ( N H ) 3
5
3
*± 2 ( N H ) R u ( 4 , 4 ' - b i p y ) R u ( N H ) 3
5
3
5
5
4 +
(3)
5 +
r e d u c t i o n potentials for the h a l f - r e a c t i o n s 4 a n d 5 ( w h e r e F c represents ferrocene a n d a f e r r o c e n y l g r o u p ) , t h e b i f e r r o c e n e c o u p l e d i s f a v o r e d b y a statistical factor of 2 or 0.018 V [(RT/nF)
(Fc-Fc) In 2 =
since there are t w o w a y s of f o r m i n g ( F c - F c ) — F c - F c a n d F c - F c +
Fc
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0.018] (25).
+
+ e -> Fc
+
(Fc-Fc)
+
(4) (5)
+ e -» F c - F c
+
is
+ / 0
F o r systems m o r e c o m p l i c a t e d t h a n d i m e r s , there are a m b i g u i t i e s r e g a r d i n g the site of o x i d a t i o n . F o r e x a m p l e , i n the Ι,Ι'-polyferrocenes, Fc
n
(n — 3, 4 ) ( F i g u r e 3 ) , a n d i n l i g a n d - b r i d g e d r u t h e n i u m complexes,
(bipy) ClRu(pyz)[Ru(bipy) pyz]nRuCl(bipy) 2
2
2
( n — 1-4)
( 2 n + 2 ) +
(25,
26, 2 7 ) , there are c h e m i c a l l y different sites. O x i d a t i o n gives a series of o x i d a t i o n state isomers w h i c h differ i n t h e site of o x i d a t i o n ( 2 5 ) . example, for ( l , l ' - t e r f e r r o c e n e ) isomers
( F c - F c - F c and F c - F c - F c ) +
a n d one
+
(Fc-Fc -Fc).
non-equivalent
differences
between
dominant.
It w a s e s t i m a t e d t h a t i n s o l u t i o n the free e n e r g y
between F c - F c - F c +
isomers m a y be l a r g e a n d a s i n g l e i s o m e r m a y
m
be
difference
a n d F c - F c - F c is ~ 0.12 V ( 2 5 ) a n d t h a t b e t w e e n
+
+
+
(NH ) Ru (pyz)Ru Cl(bipy) 5
isomer
D e p e n d i n g o n differences i n l i g a n d e n v i r o n m e n t s , e n e r g y
+
3
For
there are t w o e n e r g e t i c a l l y e q u i v a l e n t
+
n
is ~ 0.30 V (29,30).
2
4 +
and
(NH ) Ru 8
B
I I
(pyz)Ru a(bipy)2 m
4 f
I f a n o r b i t a l p a t h w a y exists b e t w e e n m e t a l centers,
t h e different isomers are accessible b y t h e r m a l - a n d l i g h t - i n d u c e d i n t r a m o l e c u l a r e l e c t r o n transfer processes. It is i m p o r t a n t to r e a l i z e that the assignment of o x i d a t i o n
states
b a s e d o n s o l u t i o n i n f o r m a t i o n m a y not a p p l y to the s o l i d state. A l t h o u g h a mixed valence ion like ( b i p y ) C l R u ( p y z ) R u C l ( b i p y ) 2
2
3 +
m a y be favored
i n s o l u t i o n , there is no guarantee t h a t it is f a v o r e d i n the s o l i d state o v e r a s t o i c h i o m e t r i c m i x t u r e of the t w o adjacent ions RuCl(bipy)
2
2 +
and
(bipy) ClRu(pyz)RuCl(bipy) 2
2
(bipy) ClRu(pyz)2
4 +
.
I n m i x e d - v a l e n c e complexes, w e a k metal—metal i n t e r a c t i o n s l e a d t o intervalence regions (25). (NH )5Ru 3
n i
transfer
(IT)
bands,
usually i n the visible or near
IR
I n a n I T t r a n s i t i o n , l i g h t - i n d u c e d e l e c t r o n transfer occurs N Ο
NRu Cl(bipy) n
2
4 +
.«ι (NH ) Ru N 3
5
n
NRu Cl(bipy) **
Ο V ^
m
'
2
/
In Inorganic Compounds with Unusual Properties; King, R.; Advances in Chemistry; American Chemical Society: Washington, DC, 1976.
78
INORGANIC
COMPOUNDS WITH
b e t w e e n m e t a l sites i n different o x i d a t i o n states
UNUSUAL
PROPERTIES
(Reaction
6).
I n the
i m m e d i a t e p r o d u c t of l i g h t - i n d u c e d e l e c t r o n transfer, the m e t a l sites are i n n o n - e q u i l i b r i u m v i b r a t i o n a n d s o l v a t i o n states since n u c l e a r
motion
is s l o w c o m p a r e d w i t h e l e c t r o n m o t i o n ( F r a n c k - C o n d o n p r i n c i p l e ) . The potential energy-configurational H u s h to d e s c r i b e
I T transitions ( 3 2 )
grams s h o w i n g I T 34)
and 8 (33)]
transitions for b o t h s y m m e t r i c a l
3
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diagrams used i n F i g u r e 4. [Reactions
by Dia
7
(31,
a n d u n s y m m e t r i c a l ( R e a c t i o n 6 ) m i x e d - v a l e n c e ions are
(NH )5Ru(4,4'-bipy)Ru(NH )5 3
hv -» (NH ) Ru(4,4 -bipy)Ru(NH )5 * (7)
5 +
Fc-Fc given.
coordinate
are p r e s e n t e d
3
r
5
5 +
3
-» Fc -Fc*
+
(8)
+
T h e t r a n s i t i o n i n R e a c t i o n 6 is at h i g h e r e n e r g y t h a n t h a t for a
s y m m e t r i c a l system b e c a u s e the e l e c t r o n transfer process is e n e r g e t i c a l l y unsymmetrical.
T h e product,
(NH ) Ru (pyz)Ru ^l(bipy) 3
n
5
n
is a t h e r m a l l y e q u i l i b r a t e d m i x e d - v a l e n c e b e c a u s e the o x i d a t i o n state c o n f i g u r a t i o n state
(29,
30).
figurations Fc-Fc)
Similar
(in
1:1
v:v
2
2
certain oxidation is at a h i g h e r
3
+
(\
+
Hush
+
hv -» Fc -Fc -Fc
developed a theoretical
+
+
treatment
for
T h e w o r k of H u s h a n d t h a t of R o b i n a n d D a y ( 3 5 ) t h e y relate the p r o p e r t i e s
of
which
disfavored ground
state
I T bands
energy
con (Fc(A
m a x
5.26 k K ) b e c a u s e the t r a n s i
max
t i o n is also e n e r g e t i c a l l y u n s y m m e t r i c a l ( R e a c t i o n 9 )
Fc -Fc-Fc
\
T h e I T b a n d o b s e r v e d for
CH C1 -CH CN)
5.99 k K ) t h a n the I T b a n d for F c - F c
state, is
4
is r e v e r s e d f r o m t h e
effects o c c u r for
of the Ι , Γ - p o l y f e r r o c e n e s .
2 +
excited
2
(25).
* IT
(9) transitions
(32).
is i m p o r t a n t b e c a u s e
to the extent
of
metal-metal
i n t e r a c t i o n a n d to the rate of t h e r m a l e l e c t r o n transfer b e t w e e n m e t a l sites. T h e r e l a t i o n s h i p s are d e p i c t e d d i a g r a m m a t i c a l l y i n F i g u r e 4 w h e r e E p and E
Ul
0
are the energies for the o p t i c a l a n d t h e t h e r m a l
transfer processes, r e s p e c t i v e l y .
electron
O r b i t a l o v e r l a p b e t w e e n m e t a l sites is
t h e o r i g i n of the s p l i t t i n g b e t w e e n surfaces
a n d of the i n t e n s i t y of
IT
bands. Recent
w o r k on dimeric ruthenium complexes demonstrated
that
there is reasonable agreement b e t w e e n e x p e r i m e n t a l d a t a a n d t h e b a n d w i d t h a n d solvent d e p e n d e n c e p r e d i c t d b y H u s h for I T b a n d s
(29,
30,
31 ). T h e w o r k w i t h r u t h e n i u m c o m p l e x e s also r e v e a l e d that the energies a n d intensities of I T b a n d s v a r y s y s t e m a t i c a l l y as a f u n c t i o n of b r i d g i n g a n d n o n b r i d g i n g l i g a n d effects (29, 30,31,
34).
N o I T b a n d was observed
In Inorganic Compounds with Unusual Properties; King, R.; Advances in Chemistry; American Chemical Society: Washington, DC, 1976.
7.
Polymetallic
MEYER
79
Systems
for t h e i o n :
[(NH )5Ru 3
n i
N
0 / - C H
2
C H
2
- Y O
NRu Cl(bipy) ] I I
2
4 +
b e c a u s e t h e o r b i t a l p a t h w a y b e t w e e n m e t a l centers is b l o c k e d b y t h e saturated - C H - C H - linkage. I T bands appear for pyrazine, 4,4-bipyri2
2
d i n e , a n d i r a n s - l , 2 - b i s ( 4 - p y r i d y l ) ethylene as t h e b r i d g i n g l i g a n d s w h e r e there is a n i n t a c t π system.
T h e bands are at h i g h e r energies f o r t h e
l o n g e r b r i d g i n g l i g a n d s ( i n a c e t o n i t r i l e : 10.4 k K f o r p y r a z i n e , ~ 1 4 . 4 k K
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for 4 , 4 ' - b i p y r i d i n e , a n d ~ 14.7 k K f o r f r a n s - l , 2 - b i s ( 4 - p y r i d y l ) e t h y l e n e (29, 30) Ru
i n
-Ru
because t h e i n t e r s e c t i o n r e g i o n b e t w e e n n
the R u
I ] L
Ru
m
and
surfaces ( F i g u r e 4 ) a n d therefore t h e energy of t h e I T t r a n s i
t i o n are functions of the d i s t a n c e b e t w e e n t h e m e t a l centers. T h e i n t e n s i t y of t h e b a n d f o r t h e p y r a z i n e - b r i d g e d d i m e r is c o n s i d e r a b l y greater t h a n that f o r t h e other d i m e r s ; this i n d i c a t e s a stronger m e t a l - m e t a l i n t e r a c t i o n .
Ru (H)-Ru (lll) a
a
RuaOlO-RuaOl)
A
Ο UJ Ζ
CONFIGURATIONAL COORDINATE
Ru (ll)-Ru (IH) b
a
Ru^llO-RuJII)
Β
Figure 4. Potential energy-configurational coordinate diagrams for symmetrical (A) and unsymmetncal (B) cases. IT transi tions are indicated by the arrows.
In Inorganic Compounds with Unusual Properties; King, R.; Advances in Chemistry; American Chemical Society: Washington, DC, 1976.
80
INORGANIC
COMPOUNDS
WITH
UNUSUAL
PROPERTIES
N o n b r i d g i n g l i g a n d s c a n affect the e n e r g y a n d a p p a r e n t l y also the i n t e n s i t y of I T b a n d s . and ( N H ) 5 R u
(34)
3
i n
I n the d i m e r s
( N ^ H R u ^ P y z J R u ^ N ^ ^
(pyz)Ru X(bipy)2 n
4 +
(29, 30),
5
*
the e n e r g y of the
I T b a n d increases as v a r i a t i o n s i n L or X increase the energy a s y m m e t r y b e t w e e n the t w o ends. F o r the m i x e d - v a l e n c e d i m e r RuCl(bipy)
2
3 +
(bipy) ORu(pyz)2
, E S C A studies d e m o n s t r a t e d t h a t there are discrete R u ( I I )
a n d R u ( I I I ) sites (36).
I n r e c e n t w o r k , C a l l a h a n a n d M e y e r (37)
a n I T b a n d for t h e i o n ( A
1300 n m , c =
m a x
found
450 i n a c e t o n i t r i l e ) w h i c h has
the a p p r o x i m a t e b a n d w i d t h a n d solvent d e p e n d e n c e t h a t w e r e p r e d i c t e d by Hush.
I R d a t a are consistent w i t h l o c a l i z e d valences.
T h e properties
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of this i o n differ m a r k e d l y f r o m those of t h e C r e u t z a n d T a u b e (NH ) Ru(pyz)Ru(NH3)5 3
with
5
a much
system
stronger
(33),
5 +
a n d the differences
are
m e t a l - m e t a l i n t e r a c t i o n i n the
ion
consistent
pentaammine
(37).
Strong Interactions between Metals through a Bridging
Ligand
W i t h s t r o n g m e t a l - m e t a l i n t e r a c t i o n s across a b r i d g i n g l i g a n d , t h e v a l e n c e r e d o x o r b i t a l s are d e l o c a l i z e d m o l e c u l a r o r b i t a l s b o t h m e t a l a n d l i g a n d i n c h a r a c t e r . I n m i x e d - v a l e n c e c o m p o u n d s , different, discrete o x i dation
states d o
not exist since the site of
o x i d a t i o n is
delocalized.
S t r o n g l y c o u p l e d systems are l i k e m e t a l - m e t a l b o n d s i n t h a t t h e i r elec t r o n i c a n d c h e m i c a l p r o p e r t i e s are s i g n i f i c a n t l y m o d i f i e d f r o m those of related monomeric
complexes.
As w i t h m e t a l - m e t a l bonds, such
com
p o u n d s c a n h a v e a n extensive m u l t i p l e o x i d a t i o n state c h e m i s t r y b a s e d on delocalized molecular orbitals. S t r o n g c o u p l i n g is e x p e c t e d
w h e n the b r i d g i n g d i s t a n c e is short,
e s p e c i a l l y for s e c o n d - a n d t h i r d - r o w metals a n d for metals i n l o w o x i d a t i o n states w h e r e d o r b i t a l extension is great a n d s t r o n g π o v e r l a p c a n occur.
S e v e r a l o x o - b r i d g e d complexes of r u t h e n i u m ( I I I ) ,
RuX(AA) ] 2
[(AA) XRuO2
( w h e r e A A is 2 , 2 - b i p y r i d i n e or 1,10-phenanthroline
2 +
/
and
X is C I or N 0 ) , h a v e u n u s u a l s p e c t r a l , r e d o x , a n d c h e m i c a l p r o p e r t i e s 2
I n the salt [ ( b i p y ) ( N 0 ) R u O R u ( N 0 ) ( b i p y ) ] ( C 1 0 ) ,
(38).
2
2
2
2
4
2
the
R u - O - R u a n g l e is