Mendeleev Commun., 2018, 28, 208–210
Table 1 Selected bond distances, angles and structural parameters.
0
0
.3
.2
2
1
Compound P=X/Å
MeTpp
C–P–C/deg
Fe–Naverage/Å SFea
100.06(7), 105.14(7),
9
6.19(7)
1.9506(16) 107.53(19), 105.8(2),
03.16(19)
.9507(16) 106.49(19), 104.17(19),
05.4(2)
102.62(18), 104.78(17),
.9283(14) 101.68(17)
.9268(12) 104.45(15), 101.43(15), 2.017(3)
02.74(15)
103.61(7), 102.80(7),
03.11(7)
SFe is the sum of the deviation from 90° of the 12 cis-angles of the FeN6
octahedron.
MeTppS
0.1
1
1
0
.0
1
0
50
100 150 200 250 300
1
T/K
1
1
2.009(3)
21.5
17.6
Figure 3 Temperature dependence of cMT plots for complexes (1) 1 and
(2) 2.
1
2
1.9348(6)
2.0150(14)
18.7
ii
1
state of the Fe ion in 1 and 2 is the LS state, which is in accordance
a
with the magnetic data (see below). The P=X bond lengths in the
Fe complexes (1.927 and 1.928 Å for 1 and 1.935 Å for 2) are
ii
shorter than those in the free MeTppS ligand (1.951 Å), whereas
the C–P–C angles of the complexes are 101.7–104.8°, comparable
to 103.2–107.5° in the free MeTppS ligand.
Magnetic susceptibility measurements in a 1000 Oe field
were performed in a temperature range of 2–300 K (Figure 3).
(a)
S(1)
(b)
S(1)
P(1)
P(1)
The c T values of 1 and 2 did not change as the temperature
M
N(1)
N(3)
N(2)
N(3)
N(1)
increased from 30 to 300 K to show a tendency to the LS state
stabilization, which is very similar to that observed for related
N(2)
Fe(1)
Fe(1)
ii
Fe complex systems chelating bis-tripodal ligands exhibiting no
N(3)
N(2)
N(1)
22,23
N(2)
temperature dependence (LS state) in the test temperature range.
N(1)
N(3)
3
–1
In addition, the c T values of 1 and 2 are 0.20 cm mol K at
M
3
0 K, indicating that about 5% of iron(ii) ions still remain in the
P(1)
S(1)
P(1)
S(1)
high-spin states, with the non-zero value being due to second
order Zeeman contributions from the t2g configuration possibly
augmented by some remnant HS form.
6
15–17,24
This is in accordance
with structure analysis (the coordination bond lengths in 1 and 2
are slightly longer than those of the {Fe[(TppO) ] } (1.982 Å)
2 2
Figure 2 Molecular structure of complexes (a) 1 and (b) 2. Anions, solvent
molecules and hydrogen atoms are omitted for clarity.
2
+
based on the tris(2-pyridyl)phosphine oxide ligand). The decrease
1
5–17,25,26
Note that the coordination bond lengths in 1 (av. 2.01 Å) and
of c T below 30 K is due to zero-field splitting.
In
M
ii
2
(av. 2.02 Å) (Table 1, Figure 2) are slightly longer than those
general, Fe complexes exist in either a high spin or a low spin
state depending on the nature of the ligand field on the metal
ions. We devote ourselves to select and change the ligands with
different electron-donating groups in order to get intermediate
ligand field, however spin transition from low-spin to the high-
spin state is not detected between 2 and 300 K in two complexes.
In summary, two mononuclear iron(ii) complexes with the
tris(2-pyridyl)phosphine sulfide ligands in a N,N',N''-tripodal mode
have been successfully synthesized. Although a spin transition
from low-spin to high-spin state was not detected at 2–300 K in
the two complexes, we believe that our results will have some
impact on the preparation of novel SCO molecular materials.
2
+
2+
of the {Fe[N(py) ] } (1.982 Å), {Fe[CH(py)3]2} (1.949 Å),
3
2
2
+
2+
{
Fe[MeC(py) ] } (1.973 Å) and {Fe[(TppO) ] } (1.982 Å)
based on a tris(2-pyridyl)phosphine oxide ligand.
3 2
2 2
1–23
2
In addition,
the S values are 21.5 and 17.6° for 1 or 18.7° for 2. Thus, the spin
§
Crystal data for MeTpp. C H N P, M = 307.32, monoclinic, space
18
18
3
group P2 /n, a = 11.1546(17), b = 12.1839(19) and c = 13.133(2) Å,
1
3
–3
b = 113.981(2)°, V = 1630.8(4) Å , Z = 4, d = 1.252 g cm , m(MoKa) =
0.753 mm , T = 296(2) K, 17449 reflections measured, 4940 independent
calc
–1
=
reflections (Rint = 0.0471), final R = 0.0694 [I > 2s(I)], wR = 0.1567,
1
2
GOF = 1.045.
Crystal data for MeTppS. C H N PS, M = 339.38, monoclinic, space
18
18
3
group P2 /n, a = 14.023(3), b = 8.4045(18) and c = 30.400(6) Å,
1
3
–3
This work was supported by the Educational Commission of
Hubei Province of China (project no. B2017141), the National
Undergraduate Training Program for Innovation and Entrepreneur-
ship (project no. 201613256001), the Open Fund of Hubei Key
Laboratory of Pollutant Analysis & Reuse Technology (project
no. PA160209) and the Key Fund of the School of Art and
Science of Hubei Normal University (project no. Ky201701).
b = 98.391(3)°, V = 3544.5(13) Å , Z = 8, d = 1.272 g cm , m(MoKa) =
calc
–1
=
0.275 mm , T = 296(2) K, 25914 reflections measured, 6193 independent
reflections (Rint = 0.0731), final R = 0.0834 [I > 2s(I)], wR = 0.1897,
1
2
GOF = 1.045.
Crystal data for 1. C H Cl N O P S Fe, M = 983.54, triclinic, space
35
38
2
8
10 2 2
–
group P1, a = 12.4325(14), b = 12.9046(14) and c = 14.5901(16) Å, a =
3
=
97.769(2)°, b = 105.062(2)°, g = 92.435(2)°, V = 2232.2(4) Å , Z = 2,
–3
–1
dcalc = 1.463 g cm , m(MoKa) = 0.684 mm , T = 296(2) K, 22066
reflections measured, 8686 independent reflections (Rint = 0.0594), final
R = 0.0719 [I > 2s(I)], wR = 0.2073, GOF = 1.077.
Online Supplementary Materials
1
2
Crystal data for 2. C H Cl N O P S Fe, M = 983.54, triclinic, space
Supplementary data associated with this article can be found
in the online version at doi: 10.1016/j.mencom.2018.03.034.
48
54
2
12
8 2 2
–
group P1, a = 11.2851(10), b = 11.5247(10) and c = 11.8662(11) Å, a =
3
=
88.1050(10)°, b = 80.6610(10)°, g = 64.3540(10)°, V = 1371.6(2) Å ,
–3
–1
Z = 1, dcalc = 1.428 cm , m(MoKa) = 0.569 mm , T = 100(2) K, 15996
reflections measured, 6551 independent reflections (Rint = 0.0333), final
R = 0.0373 [I > 2s(I)], wR = 0.1070, GOF = 1.052.
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–
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