Lanthanides are routinely incorporated into quantum dots
to act
as down-shifting and up-converting phosphors in display and lighting
applications due to their high photoluminescence quantum yields (PLQY).
Recent efforts in the field have demonstrated that trivalent lanthanide,
Ln(III), incorporated into ZnAl2O4 spinel nanocrystals
can achieve PLQYs of 50% for down-shifting nanophosphors using earth
abundant materials. The high PLQY is surprising as the Al(III) site
in a spinel is centrosymmetric, which should lead to poor performance
for these nanophosphors. However, spinels are prone to formation of
an admixture of inverse and normal spinel lattices when the cation
size ratio is not optimal. Such behavior can produce local cation
disorder that can influence the phosphor performance. Herein, we describe
the use of Tb(III) as an optical probe to evaluate the fractional
population of the inverse and normal spinel structures within Tb
x
ZnAl2‑x
O4. The experimental data exhibits a Tb(III) concentration
dependent change in the fractional population that results in a maximum
PLQY of 37% with 3.56% Tb(III) incorporation. A decrease in the degree
of inversion (cation disorder) leads to larger amounts of the cubic Fd
m phase resulting
in the observed photoluminescence behavior. The correlation of NMR,
pXRD, and optical methods provides direct insight into the high PLQY
behavior for this class of nanophosphor.
Latva’s empirical rule states that the energy
separation
between a molecular sensitizer and a lanthanide ion excited state
must lie within 2000 to 4000 cm–1 for optimal energy
transfer. At energies below 2000 cm–1, back energy
transfer will impact the process resulting in the reduction of the
photoluminescence quantum yield (PLQY). The role of excited triplet
state (3π*) energy and intralanthanide ion energy
hopping is assessed for a series of β-diketonate molecular sensitizers
coordinated to the surface of a 2 nm 3.56% Tb(III):ZnAl2O4 nanospinel. It is observed that energy transfer from
the β-diketonate to a 2 nm nanospinel lies within the critical
radii for energy transfer and the presence of efficient energy hopping
minimizes back energy transfer contributions. In contradiction to
Latva’s rule, the highest PLQY of 39% is achieved following
sensitization by hexafluoroacetylacetonate, with an energy difference
(3π*-5D4) of only 1534 cm–1. The measured PLQY is consistent with other reports
of Tb(III) doped nanocrystal hosts lattices, suggesting that energy
hopping within the lattice enhances the Tb(III) phosphor performance.
Although not measured, the energy gap plot suggests that a PLQY approaching
58% may be achievable by ligand design.
A new three dimensional lanthanide-containing coordination polymer assembled from 2,2′-bithiophene-5,5′-dicarboxylic acid ([Ln2(C10H4O4S2)3(H2O)6]n, Ln = Sm–Yb) was solvothermally synthesized and used as a sensor to detect nitroaromatic compounds via luminescence quenching.
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