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A polyoxovanadium borate [Na(H2O)]2[Na(H2O)2]2[Cu(en)2][V12B18O54(OH)6]・(H3O)2・(H2O)18 1 (en=ethylenediamine) has been hydrothermally synthesized and characterized by IR, two-dimensional infrared (2D IR) correlation spectroscopy with magnetic and thermal
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30
卷
6
期
201
1.
6
结构化学
(J
IEGOU
HUAXUE)
Chinese
J.
Struct.
Chem.
Vo
l.
30
,
No.
6
785-792
A
Porous
Organic-inorganic
Hybrid
Compound
Constructed
from
Polyoxovanadium
Borate
Anions, Dinuclear N a Sites
and
Metal-organic U
nits
①
LI
Guang-Man
MEI
Hong-
Xin
CHEN
Xiang-Yi
CHEN
Yi-Ping
SUN
Yan-Qiong
ZHANG
Han-Hui
CHEN
Xiao-Ping
(D
句
partment
01
Chemis
t.
η"
Fuzhou University, Fuzhou, Fujian 350108, China)
ABSTRACT
A polyoxovanadium borate [N
a(H20)h
[Na(H20)zh[Cu(en
)z
][VI2BI80S4(OH)
6l
但
30)2.
(H
20)181
(en = ethylenediamine) has been hydrothermally synthesized and characterized
by
IR,
two-dimensional infrared (2D IR) correlation spectroscopy with magnetic and thermal
pert
旧
ba
tion, thermal
IR
spectroscopy, thermal
gravime
仕
ic
analysis and single.,.crystal X-ray
di
岱
action.
It
crystallizes in triclinic, space group
PÏ
with a = 12.981(3), b = 13.044(3), c = 14
.2
08(3)
A
,
α=
63.98(
匀
,
ß=77.17(
坷
,
y =
14.208(3
沪
,
V=
200
1.
0(8) A
3
, Z = 1,
M,.
= 2518.05,
Dc
= 2.090
g!
cm-
I
,
F(OOO)
= 1255.0,
Mu(mm
叮=
1.
756
,
λ
仙
fo
Ki
α)
= 0.71073 A, R = 0.0625 and
wR
= 0.1952. In 1, the
[V
12
B
I8
0
S4('
。而
6]8-
units are connected
by
[CU(en)2]
衍,
binu
cI
ear
Na(l)
and
Na(2) to form a
three-dimensional porous framewor
k.
Keywords:
organic-inorganic
hybrid
,
porous
framewor
k,
polyoxovanadium
borate
, 2D
IR
correlation
spectroscopy
,
thermal
IR
spectroscopy
1
剧
TRODUCTION
Recently, there has been
much
recent
interest
也
mixed organic-inorganic materials,
especially
岛
rthe
formation
of
new porous
materials[I
,
21.τ
'h
e
porous
polyoxovanadium borates developed recently
by
Haushalter, Zubieta and others[3-
8
1 have some
of
the
most interesting structural and compositional diver-
sity. Until now
, the polyoxovanadium borates con-
nected with linkers
by
covalent bond to form a
three-dimensional (3D) microsoft framework are
relatively less studied.
Thus
,也
e
preparation and
characterization
of
mixed organic-inorganic poly-
oxovanadium borates still remain challenging[9
,
I
町.
The earliest full description
of
perturbation based
Received
3
September
2010;
accepted
26
November
2010
(CCDC
756202)
dynamic
2D
correlation spectroscopy, based on a
simple sinusoidal perturbation
, was put forward in
1990
by
Noda[lll.τ
'h
en
,
the idea
of
2D correlation
coefficient maps
baséd
on
the statistical correlation
analysis introduced
by
Barton II
et
al.[12
1
, which
made the next significant advance in the
2D
cor
四
relation spectroscopy
by
removing the constraint
of
sinusoidal perturbation.
On
this basis, a major
breakthrough
in
this field occurred when the ge-
neralized
2D
correlation spectroscopy based on any
arbitrary shape
of
perturbation waveform introduced
by
Noda[
I3-
16
1.
Since then, the generalized two-
dimensional
in
企
ared
(2D
IR)
correlation spectro-
scopy has become a
verypowerful
and versat
i1
e tool
岛
r
elucidating subtle spectral changes induced by an
(Th
is
work
was
suppor
时
by
the
National
Natural
Science
Foundation
ofChina
(20873021
,
21003020)
,
Doctoral
Fund
ofMinis
町
。
f
Ed
ucation
ofChina
(20093514120002)
,
and
New
Ce
ntury
Excellent
Talent
Supported
Plan
ofFujian
Provinc
币。
XSJRC2007-21)
(
Corresponding
au
也
or.
E-mail:
ypchen007@hotmai
1.
com
786
LJ
G.
M.
et
al.: A
Porous
Organic-inorganic
Hybrid
Compound
Constructed
台
om
Polyoxovanadium
Borate
Ani
o
田,
Dinuclear
Na
Sites
andMetal-organic
Units
No.6
extemal perturbation, such as light, heat,
elec
位
icity
,
magnetism, chemistry or mechanical force.
Th
e 2D
IR correlation spectroscopy could not only enhance
the spectral resolution and identify the over-lapped
peaks but also probe the specific order
of
certain
events taking place under the i
n:fl
uence
of
a
controlled physical
variable[17-19].
Our research group has successfully introduced
the generalized 2D
IR
correlation spectroscopy to
study the polyoxometalates
(POMsf'
8,
20]
To
further enrich its application in structure identifica-
tion
, the 2D
IR
correlation spectroscopy with ther-
mal and magnetic perturbation was introduced to
explore the studies
of
1.
In addition, the 2D IR
correlation spectroscopy and thermal IR
spec
忧。"
scopy were frrst introduced to explore the
[V
12
B
18
0
S4(
。而
6]8-
cluster and obtained the dynamic
information about the structural changes
of
1.
2 EXPERIMENTAL
2. 1
Materials
and
methods
Al
l chemicals purchased were
of
reagent grade
and used without further purification.
Th
e IR
spec
仕um
was recorded
in
the range
of
4000'"'-'400 cm
-1
on a Perkin-Elmer FT -IR spectrum
2000 spectrometers using
KBr
pellets. In order to
obtain the 2D
IR
correlation spectra, a series
of
dynall
山
IR
spectra was recorded in the 4000'"'-'
400 cm-
1
range on a Perkin-Elmer FT-IR
spec
位
um
2000 spectrometers using KBr pellets.
Th
e magnetic
intensity variation was controlled
by
a homemade
magnetic intensity
controller
仕
om
2 to 20
mT
at an
interval
of
2 mT.
Th
e temperature variation was
controlled
by
a portable programmahle temperature
con
仕
oller
(Model 50-886, Love Control Corporation)
企
om
50 to
120.C
at an interval
of
10
oC.
Before
2D calculation
, each spectrum was
smoothed
岛
r13
points and baseline was corrected.
So
丘
ware
used for
ca
1c
ulation was provided
by
Tsinghua University. A
series
of
thermal
IR
spec
仕
a
was recorded in the
4000'"'-'400 cm-
1
region on a BRUKER TENSOR 27
IR
spec
位
um
2000 spectrometer with KBr pe
l1
ets.
The temperature variation was controlled by a por-
table programmahle
tempera
阳
re
controller (IR by
double sample transmission
, Xiamen Tuosi
Ins
仕
u
ment
Eq
uipment Dev
e1
0pment
Co.
,
L
创.)
in N
2
environ-
ment
企
om
50 to 550
.C
at an interval
of
10
.C.
2. 2 Synthesis
The
VOS0
4
(1.
0 mo
l/
L) was prepared by H
2
S04
(20
mL, 98 wt%), V
2
0
S
(9.1245 g, 50.0 mmol),
H
2
C
2
0
4
.2H
2
0 (7
.3
024 g, 57.9 mmol) and distilled
water in a 50
mL measuring
f1
as
k.
1 was hydrothermally synthesized under autoge-
nous pressure. A mixture
of
2.00
mL
VOS0
4
, 1.20 g
H
3
B0
3
, 0.75 g CuS04.5H20, 2.00 mL H
2
0 , 0.60 mL
en and 0.15 g H
2
C
2
0
4
.2H
2
0 was stirred
to
homogeneity and
a
司
justed
to
pH
= 9.0 with NaOH
solution (10 mo
llL)
under continuous stirring and
sealed in a
10
mL Te
f1
on-lined stainless steel
autoclave
, which was heated to 140
oC
岛
r
3 days.
Aft
er
slowly cooling to room
tempera
阳
re
,
brown
block crystalline product
of
1 was separated (yield
73% based on vanadium).
2. 3
Crystallography
X-ray intensity data
of
1 were collected on a
Rigaku R-AXIS RAPID diffractometer equipped
with a graphite-monochromatic
Mo
Kj
αradiation
(À
=
0.71073 Á) at 298 K. The structure was solved by
direct methods using SHELXS-97 and refined
by
岛
L
matrix least-squares on
F-
with
SHELXL_97[21
,
22].
All
of
the non-hydrogen atoms were refmed with
anisotropic displacement parameters except some
disordered oxygen atoms
of
water molecules and
charge-compensating H
3
0+.
Th
e selected. bond
lengths and bond angels are listed in Table
1.
3 RESULTS AND DISCUSSION
3. 1
Structural
description
of
1
ηle
[V
12B180S4(OH)6t cluster (Fig.
1)
of
1 can
be visualized most easily as being composed
of
a
puckered
[B
18
0
36
(OH)6J
丛
ring
sandwiched between
two
仕
iangul
缸
V
6 rings
of
six altemating cis and
trans edge-sharing VO
s
square pyramids. The V
-ü
hond lengths
of
the terminal oxygen atoms (V=O)
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