3211
Yan Z[ Voloshin et al[
ments into the clathrochelate cage\ as a rule\ exerts complex chromophore system than that of sym!
much more on the QS and 8 values than in the case metrical clathrochelates\ while the spectra for boron!
when a second such fragment is introduced[ The above containing axial!asymmetrical compounds closely
statements are clearly shown for a!benzydioxime in resemble those of the corresponding symmetrical com!
Table 1[
pounds[ It should be noted that the UVÐVIS spectra
A similar phenomenon was observed upon intro! for the latter with the same dioxime and di}erent
duction of glyoximate and nioximate fragments into boron!containing capping fragments are practically
the clathrochelate framework instead of a!benzyl! identical ð3\ 06Ł[ The spectrum for a mixed borontin!
dioximate and dimethylglyoximate ones[
containing ""n!C3H8#3N#ðFeNx2"BC5H4#"SnCl2#Ł cla!
For axial!asymmetrical complexes\ just like for throchelate alone essentially di}ers from that for the
symmetrical boron!containing iron"II# tris!dioximates FeNx2"BC5H4#1 complex] apart from a singlet band
ð3\ 05Ł\ distinct dependencies of QS and 8 values on about 359 nm characteristic for boron!containing
the nature of a substituent at the boron atom have compounds\ a more intense band appears about
been obtained[ꢀ The QS value in a mixed borontin! 499 nm detectable in the UVÐVIS spectrum for a tin!
containing clathrochelate is equal to zero which is in chloride tris!dioximate ðFeNx2"SnCl2#1Ł1− dianion[
agreement with the above statements too] the QS value The intensities of these bands are redistributed "Table
in the corresponding trigonal!prismatic boron!con! 2#[
taining FeNx2"BC5H4#1 complex has a positive sign\
An analogous phenomenon was also observed in
while the corresponding trigonal!antiprismatic tin! the spectra of some meridianal!asymmetrical clathro!
containing clathrochelate\ according to the data chelates "FeDm1Bd"BF#1\ FeBd1Dm2"BF#1 and
reported in ð4\ 07Ł\ is characterized by a negative QS FeBd1Nx1"BF#1#[ The intense Md:Lpꢀ charge trans!
value[ A superposition of these two contributions fer band in the UVÐVIS spectra of these compounds
gives a twist angle 8 close to 29> and\ hence\ the QS proved to be a superposition of two bands with max!
value is zero[
ima slightly shifted to the long!wavelength range as
The UVÐVIS spectra for synthesized meridianal! compared to the corresponding symmetrical com!
asymmetrical compounds in solution indicate a more plexes ""FeDm2"BF#1\ FeBd2"BF#1 and FeNx2"BF#1#\
but at an unusual and unexpected ratio of the inten!
sities of these bands takes place[
The UVÐVIS spectrum for the FeBd1Gm"BF#1 com!
one axial!asymmetrical complex "Fig[ 0# was solved ð19Ł[ plex proved also to be quite unexpected since it con!
ꢀ After sending this paper to the Editor the structure of
Single
crystals
of
the
FeBd2"BF#"Bn!
tains only one band with the intermediate value of
lmaxꢁ353 nm\ rather than two bands at approxi!
mately 339 and 379 nm[ With this complex\ maximal
tension in p!systems of di}erent dioxime fragments is
presumably observed[ Since UVÐVIS spectral charac!
teristics of FeDm2"BF#1 and FeGm2"BF#1 complexes
are identical in the visible part\ the charge transfer
band in the spectrum for an asymmetrical
FeDm1Gm"BF#1 clathrochelate is nearly the same as
C3H8# = C5H4CH2 = 0C7H05 complex were obtained by slow
1
evaporation of the saturated solution in a tolueneÐcyclooc!
tane "0]2# mixture for several weeks[ Due to the partial decay
of the sample it turned out to be impossible to get a larger
data set[ Moreover one of the phenyl rings is disordered\ the
rest were re_ned in a {{rigid!body|| approximation[ However\
the structure is the _rst example of asymmetric cla!
throchelates and the data obtained allow to analyze the coor!
dination
environment
of
the
central
atom[
C46H44B1FFeN5O5\ crystal size 9[25×9[17×9[11 mm\ that for the _rst two complexes[ In this case the band
¹
Mꢁ0904[63\ triclinic\ space group P0\ aꢁ09[741"1#\
positions of intraligand pÐpꢀ transitions di}er from
that for symmetrical compounds[
The asymmetry of the synthesized complexes mani!
fests itself in their IR and NMR spectra "Tables 2 and
Ä
bꢁ03[960"2#\ cꢁ06[949"2# A\ aꢁ76[52"2#>\ bꢁ76[35"2#>\
gꢁ79[19"2#>\ Uꢁ1450[4"8# A \ Zꢁ1\ Dcꢁ0[001 g cm−2
\
2
Ä
mꢁ9[234 mm−0\ F"999#ꢁ0919[1781 independent re~ections
were collected at 182 K on a CAD3 di}ractometer using Mo!
3#[ The C N and NÐO stretching vibrations in the
1
Ä
Ka
radiation
"lꢁ9[60962 A#
with
u:1u
scans
dioxime fragments of meridianal!asymmetrical cla!
throchelates and in the mixed borontin!containing
axial!asymmetrical complex proved to be the most
sensitive ones[ These vibrations may be assigned to the
"0[75>³u³08[87>#[ The structure was solved by the heavy!
atom method\ re_nement was made by a full!matrix least
squares an F1 for all data with anisotropic displacement
parameters for non!hydrogen atoms and isotropic for hydro!
gen atoms^ goodness!of!_tꢁ0[967\ _nal R indices "I×1s"I## corresponding dioximate groups or their fragments
R0ꢁ9[9681\ wR1ꢁ9[1003\
w−0ꢁs1"F1o#¦"9[041P#1
bound to a certain type of an capping groups[ In
particular\ the stretching vibrations of the C N band
in the spectrum of the FeDm1Gm"BF#1 complex are a
superposition of two signals] one about 0459 cm−0
which may be assigned to a glyoximate fragment "for
the FeGm2"BF#1 clathrochelate\ it is detected at
0448 cm−0# and at 0472 cm−0\ which may be assigned
¦05[863P\ Pꢁ"F1o¦1Fc1#:2[ The main parameters of the
1
Ä
iron"II# coordination polyhedron "FeÐN distance is 0[78 A
and NÐFeÐN bite "chelate# angle is 28[4># are characteristic
for macrobicyclic iron"II# tris!dioximates[ The smaller dis!
tortion angle value "8ꢁ06[8># than estimated from 46Fe
\
Mossbauer parameters "Table 0\ for analogous FeBd "BF#
Ã
2
1
complex with similar QS value distortion angle signi_cantly
higher\ 8ꢁ18[2># accounted for the electronÐdonor e}ect of
n!butyl substituent at boron atom rather than an electron!
acceptor e}ect of the ~uorine substituent[
to
dimethylglyoximate
fragments
"for
the
FeDm2"BF#1 clathrochelate\ it is detected at
0474 cm−0#[ The same vibration in the IR spectrum