Inorganic Chemistry
and [1][PF ] were recorded in a spectral range from 250 to
6
Figure 5. Averaged temperature-dependent magnetic susceptibility
data of three independently synthesized samples of 1 (green trace)
and [1][PF ] (red trace), plotted as μ vs T (right).
6
eff
properties for tri- and tetravalent coordination complexes of
32
uranium. The average effective magnetic moment (μ ) for
eff
trivalent 1 is temperature-dependent and varies from 2.35 μ at
B
3
00 K to 0.80 μB at 2 K. The low-temperature value is
3
33−36
unusually low for an f complex.
the relation 4μeff = (g1 + g2 + g ) with the experimentally
However, by applying
2
2
2
2
35
3
determined effective g values (Figure 1), the resulting value for
μ is calculated to be 0.96 μ , which is in excellent agreement
eff
B
with the experimentally determined magnetic moment of μ =
eff
2
0
.95 μ at 9 K. Notably, while characteristic for U(IV) f
B
32
complexes, even in nearly the same ligand environments, the
magnetic moment of 1 at 300 K is higher than that of its f
+
3
Figure 4. UV/vis/NIR electronic absorption spectra for 1 in toluene
analogue and was determined to be 2.81 μ . Also, typical for
U(IV) complexes, the temperature dependence is markedly
stronger, which is characteristic of temperature-independent
B
(
green trace) and [1][PF ] in methylene chloride (red trace) at 25
6
°C. Breaks in the NIR spectra are due to cutouts of the solvent
absorptions.
paramagnetism (TIP), with a typical μeff of 0.52 μ at 2 K or
B
even lower; this is in agreement with the complex’s
3
36
dominated by intense absorption bands, and due to their
unusually large molar extinction coefficients (ε), these bands
are assigned to metal−ligand charge-transfer transitions (either
metal-to-ligand or vice versa). Notably, trivalent 1 possesses a
well-resolved absorption band centered at 344 nm (ε = 61200
nonmagnetic H ground state.
4
A computational analysis by DFT was performed in order to
37
further elucidate the electronic structure of 1. Optimizations
of the structural parameters were subsequently performed,
where the aryl substituents were truncated by methyl groups
(BP86/DKH-def2-SVP). The obtained U−N bond lengths as
well as the nacnac N−U−N bond angles were in good
agreement with the structural parameters from the solid-state
structure; the mean deviation from the solid-state, single-
crystal XRD structure was 0.006 Å and 2.2° for the bond
lengths and angles, respectively. Molecular orbitals were then
obtained from single-point calculations at the B3PW91/DKH-
def2-TZVPP//BP86/DKH-def2-SVP level of theory. The
−
1
−1
M
cm ) with a shoulder at 429 nm (Figure 4, top, green
trace). The spectral region between 600 and 2100 nm (Figure
4
, bottom) shows a broad band of relatively high intensity
centered at 770 nm (εmax = 1060 M− cm ), which is often
1
−1
seen for trivalent uranium complexes, albeit at slightly higher
1
4,27−30
energy (500−700 nm),
and this band could be assigned
30
to Laporte-allowed f → d transitions. A number of less-
intense, less-resolved Laporte-forbidden f → f transitions are
observed on the band’s bathochromic flank. The UV/vis
3
calculations suggest an f electron configuration with moderate
spectrum of [1][PF ] (Figure 4, top, red trace) shows multiple
overlapping charge-transfer transitions between 280 and 600
(Lowdin spin population at uranium of 2.6 electrons)
̈
6
delocalization of the spin density onto the nacnac ligands
(Figure 6, top). Very little, if any, discrepancy was observed in
the spin densities using various levels of theory, but the BP86-
D3/DKH-def2-TZVPP//BP86-D3/DKH-def2-SVP and
BP86/DKH-def2-TZVPP//BP86/DKH-def2-SVP levels of
theory showed the least difference for truncated and
nontruncated models (Table S2). The molecular orbitals
obtained from the truncated model system were essentially
equivalent to those obtained without truncation. Plotting the
three singly occupied molecular orbitals associated with the f-
nm, with molar extinction coefficients of ε = 49000 to 18000
−
1
−1
M
cm . Characteristic for tetravalent uranium complexes,
the NIR region features several sharp f → f transitions with
−
1
−1
molar extinction coefficients up to ε = 55 M cm (Figure 4,
middle, red trace).
30,31
The magnetic properties of 1 and [1][PF ] were determined
6
by SQUID magnetization measurements in the temperature
range from 2 to 300 K and with an applied magnetic field of 1
2
2
orbitals indicates the mixing of one orbital, namely f
,
y(3x ‑y )
the averaged data plotted as μ vs T are shown in Figure 5.
The pair of complexes 1/1 shows characteristic magnetic
with some π-orbitals derived from the β-diketiminate ligands.
The other two orbitals are essentially metal centered fyz and
eff
+
2
D
Inorg. Chem. XXXX, XXX, XXX−XXX