Q. Shi, et al.
InorganicChemistryCommunications113(2020)107814
(acac)3(5-Br-2,2′-bpy)] (3), can be definitely assigned to the major
species [M−H]+, respectively. These observations confirm that each
binary tris-β-diketonate-Ln3+ species of the three iso-structural com-
plexes 1–3, can keep stable in the respective solution.
Dy3+ materials promising for optoelectronic devices [3] and sensing
subsequently complete energy transfer for one specific organo-Dy3+
complex, one feasible strategy to direct white-light seems highly at-
tractive after the simultaneous emissions of both Dy3+-centered blue-
The photo-physical properties of the binary tris-β-diketonate-Ln3+
complex 2–3 were examined in dilute MeCN solutions at room tem-
perature or 77 K, and summarized in Figs. 1 and 1S. In contrast to the
strong absorption bands (Fig. 1S) limited to the λab < 350 nm range
for the two (Hacac and 5-Br-2,2′-bpy) free ligands, the complex 2–3
display the similar ligands-based (248–250 and 284–287 nm) while
significantly broadened (200–400 nm) absorption spectra, in which, the
lower strong one (284–287 nm) should be assigned to the ligands-based
π-π*-transitions. Moreover, upon Ln3+coordination, the molar ab-
sorption coefficients of the complexes 2–3 at the lower energy ab-
sorption peaks are almost three orders of magnitudes larger than those
of the two (Hacac and 5-Br-2,2′-bpy) free ligands, also indicative of
their tris-β-diketonate-Ln3+ component with the enhanced π-conjuga-
tion effect. For the Dy3+-based complex 2, upon photo-excitation of the
chromohphores at the range of 200–410 nm (λex = 340 nm), as shown
in Fig. 1, the strong Dy3+-characteristic line-like emissions (484 nm
(4F9/2 → 6H15/2 transition), 578 nm (4F5/2 → 6H13/2 transition), 629 nm
light (λem = 478 nm; 4F9
→
6H15/2 magnetic dipole transition) and
yellow-light (λem = 572 nm; 4F9
→
6H13/2 electric dipole transition)
with a comparable intensity [5]. Nonetheless, due to the ligands-field
adjustment [6] just hyper-sensitive to the electric-dipole-governed
transition while insensitive to the magnetic dipole transition, the
dominated yellow-light as a universal basis, renders the Dy3+-exclusive
white-light greatly challenging [7] to one certain organo-Dy3+ com-
-
centered sharp visible emissions, does not cover the broad 400–700 nm
spectral region, also suffering from the inferior color-rendering prop-
erty [8]. By contrast, through the ligands-based residual blue-light
lecule dichromatic white-light [9] could be smoothly approached for
the specific organo-Dy3+ complex. However, this alternative strategy
still suffers from an intrinsic obstacle of having unsatisfactory white-
light efficiency (Φ < 5%) caused by the partial energy transfer.
Convincingly, the circumvention of such problem can rely on (Dy,
Gd)-[10], (Dy, Eu)-[11], (Dy, Eu, Gd)-[12], (Dy, Sm, Gd)-[13], (Dy, La,
the Ln3+-mixed stoichiometry, different color-compensatory contribu-
tions could be well balanced for efficient and high-quality white-lights.
However, despite their potential applications [3a] for white light-
emitting diodes (WLEDs), the detrimental deficiency of their processing
(vacuum-deposition or solution-process) inability, limits the utilization
in flexible white organic/polymer light-emitting diodes (WOLEDs/
WPLEDs) [3b–3d]. As a matter of fact, from the perspective of film-
forming capability necessary, the Ln3+-mixed complexes’ blending to-
ward direct white-light, does conceptually take effect on WOLEDs/
WPLEDs. Herein, in light of the color-tunable white-light of (Eu, Tb)-
mixed complexes [16] disadvantageous of unmanageable Tb3+-to-Eu3+
energy transfer, the (Dy, Gd) complexes’ blending should be more
worthy of motivation, because the patent absence of Dy3+-to-Gd3+
energy transfer is unambiguous, due to the extremely higher energy
level of Gd3+ ion [17]. Moreover, based on the yellow-plus-blue in-
tegration, one certain (Dy3+, Gd3+x) complexes’ blending is also cap-
able of direct white-light. Interestingly, with the judicious adjustment
of the (Dy3+, Gd3+x)-mixed ratio, the dichromatic white-light endowed
from the two isomeric Ln3+-complexes, can be easily realized under
single wavelength excitation.
(4F5/2
→
6H11/2 transition) and 665 nm (4F5/2
→
6H9/2 transition)) and
the weak while detectable emission peaking at λem = 388 nm, are
concurrently observed. For the dual-emissive complex 2 featuring a
bright yellow-light with the CIE (Commission International De L’E-
clairage) chromatic coordinate × = 0.400 and y = 0.401, the ligands-
based residual (λem = 388 nm) emission should be assigned to the
intra-ligands π-π* transition, and the hyper-sensitive peak at 578 nm
4
from the F5/2
→
6H13/2 transition should be resulted from its low
molecular symmetry [19]. Moreover, its dual-emitting nature, can
further be confirmed with the lifetimes-decayed combination of the
ligands-based fluorescence (τ = 1.13 ns; λem = 388 nm) and the Dy3+
-
centered phosphorescence (τ = 3.2 μs at λem = 578 nm; 4F5/2 → 6H13/2
transition) from the same chromophores. As to the Gd3+-based complex
3 in solution at room temperature, it displays the typically ligands-
based fluorescence (λem = 394 nm, τ = 1.02 ns and Φem = 4.7%) also
shown in Fig. 1, exhibiting a blue-light with the CIE chromatic co-
ordinate × = 0.203 and y = 0.202. In contrast, the Gd3+-centered
complex 3 in solution at 77 K, shows the 0–0 transition phosphores-
cence (λem = 433 nm andτ = 0.98 μs; also Fig. 1), from which, the
triplet (3π-π*) energy level of 23095 cm−1 is obtained. With regard to
the singlet (1π-π*) energy level, it (27855 cm−1) can be reasonably
estimated from the lower wavelength (359 nm) of its UV–visible ab-
sorbance edge, and thus, the first energy gap ΔE1 (1π-π* - 3π-π*,
4760 cm−1; Fig. 2S) near to the desirable 5000 cm−1, endows a rela-
tively effective ISC process according to the Reinhoudt’s empirical rule
[20]. Importantly, further checking the energy level match between the
As shown in Scheme 1, the N,N’-chelate ancillary ligand 5-Br-2,2′-
coupling reaction between 2,5-dibromopyridine and 2-(tributylstannyl)
pyridine in the presence of Pd(PPh3)4 (0) as the literature [18]. Further
through the one-pot reaction of LnCl3⋅6H2O (Ln = La, Dy, or Gd), the
N,N’-chelate ancillary ligand 5-Br-2,2′-bpyand the β-diketone ligand
Hacac treated with an equimolar amount of anhydrous NaOH, the
series of binary tris-β-diketonate-Ln3+ complexes [Ln(acac)3(5-Br-2,2′-
bpy)] (Ln = La (1); Dy (2); or Gd (3)) were self-assembled in receptive
yields of 68–75%, respectively.
4
(20830 cm−1) of Dy3+ ion, the second energy gap ΔE2 (2265 cm−1; 3π-
π*-4F5/2) is beyond the ideal 2500-–4500 range ruled by the Latva’s
empirical rule [21], and thus, the allowed back energy transfer should
be the reason to the dual emissions of the Dy3+-based complex 2.
Noticeably, the absolute quantum efficiency (Φem) of the complex 2,
characteristic of the Dy3+-endowed yellow-light, is up to 5.8%, which
is at the top level among previously reported organo-Dy3+-complexes
[3b–3d,8–9], which should be mainly due to the strengthened optical
absorbance and the effective suppression from the oscillator-induced
quenching [22] or the non-radiative deactivation by the 5-Br-2,2′-bpy-
All of the three complexes 1–3, soluble in common organic solvents,
were well characterized by EA, FT-IR, 1H NMR and ESI-MS. Especially
in the 1H NMR spectrum of the anti-ferromagnetic [La(acac)3(5-Br-2,2′-
bpy)] (1), the combined proton resonances (δ = 8.82–1.73 ppm) of
both the deprotonated ligand (acac)− and the ancillary ligand 5-Br-
2,2′-bpy are observed with a stipulated molar ratio of 3:1. Meanwhile,
the presence of the typically enolic eCH]C proton singlet peak at
In consideration of the relatively higher efficiencies for the yellow-
light of the Dy3+-based complex 2 and the blue-emitting of the isomeric
Gd3+-based complex 3, it is particular interest on their binary tris-β-
diketonate-(Dy3+, Gd3+x) complexes’ blend toward the dichromatic
white-light modulation as desirable. After adding different amounts of
δ = 5.19 ppm of the (acac)− ligand should be resulted from the La3+
-
coordination. Moreover, based on the ESI-MS results of the complexes
1–3, a strong mass peak at m/z 672.02 for [La(acac)3(5-Br-2,2′-bpy)]
(1), 695.91 for [Dy(acac)3(5-Br-2,2′-bpy)] (2)or 691.04 for [Gd
the Gd3+-based complex
3
to the Dy3+-based complex 2, the
UV–visible absorption and fluorescence titrations in MeCN solution
2