23 research outputs found
Transparent Infrared-Emitting CeF<sub>3</sub>:Yb−Er Polymer Nanocomposites for Optical Applications
Bright infrared-emitting nanocomposites of unmodified CeF3:Yb−Er with polymethyl-methacrylate (PMMA) and polystyrene (PS), which offer a vast range of potential applications, which include optical amplifiers, waveguides, laser materials, and implantable medical devices, were developed. For the optical application of these nanocomposites, it is critical to obtain highly transparent composites to minimize absorption and scattering losses. Preparation of transparent composites typically requires powder processing approaches that include sophisticated particle size control, deagglomeration, and dispersion stabilization methods leading to an increase in process complexity and processing steps. This work seeks to prepare transparent composites with high solids loading (>5 vol%) by matching the refractive index of the inorganic particle with low cost polymers like PMMA and PS, so as to circumvent the use of any complex processing techniques or particle surface modification. PS nanocomposites were found to exhibit better transparency than the PMMA nanocomposites, especially at high solids loading (≥10 vol%). It was found that the optical transparency of PMMA nanocomposites was more significantly affected by the increase in solids loading and inorganic particle size because of the larger refractive index mismatch of the PMMA nanocomposites compared to that of PS nanocomposites. Rayleigh scattering theory was used to provide a theoretical estimate of the scattering losses in these ceramic-polymer nanocomposites
Thermochemistry of 3D and 2D Rare Earth Oxychlorides (REOCls)
The thermodynamic stability of rare
earth (RE) materials plays
a key role in the design of separation and recycling processes for
RE elements. Thermodynamic stability is fundamentally influenced by
the lanthanide contraction, as observed in the systematic reduction
of unit cell volumes with increasing atomic number. RE materials are
found in the form of solids having primary bonds in three dimensions
(3D materials) as well as ones with primary bonds in two dimensions
(2D materials) whose layers are held together by weak van der Waals
(vdW) forces. While studies of synthesis, structure, and physical
properties of 2D RE materials are numerous, no systematic research
has compared their thermodynamic stability to that of 3D materials.
In the present work, RE oxychlorides (REOCls), which display a structural
transition from a 3D-polyhedral network (PbFCl-type) to a vdW-bonded
layered one (SmSI-type) as the RE size decreases, were all synthesized
by the flux method. High-temperature oxide melt solution calorimetry
was used to determine their formation enthalpies to enable Born–Haber
cycles to calculate lattice energies. Our results indicate that REOCl
compounds are thermodynamically stable when compared to their binary
oxides and chlorides. The lattice energies of 3D REOCls increase with
decreasing RE size yet are insensitive to unit cell volumes for 2D
REOCls. This is caused by interatomic interactions parallel and perpendicular
to layers in the SmSI-type REOCls, causing a different structure response
to the lanthanide contraction than 3D RE materials
Comprehensive Study on the Size Effects of the Optical Properties of NaYF<sub>4</sub>:Yb,Er Nanocrystals
Monodisperse
β-NaYF<sub>4</sub>:Yb,Er nanocrystals with mean
sizes of 11, 40, and 110 nm were synthesized by a thermal decomposition
solvothermal process to better understand the relationship between
particle size and optical properties. A systematic study of luminescence
intensity versus size revealed that both visible upconversion and
infrared downconversion emission intensities decrease with decreasing
nanocrystal size. The intrinsic quantum efficiency of the infrared <sup>4</sup><i>I</i><sub>13/2</sub> → <sup>4</sup><i>I</i><sub>15/2</sub> downconversion transition was studied in
great detail since this specific transition allows us to quantify
the contribution of nonradiative losses more easily than the observed
upconversion transitions. The intrinsic quantum efficiency of the <sup>4</sup><i>I</i><sub>13/2</sub>→<sup>4</sup><i>I</i><sub>15/2</sub> transition decreased from 50% (110 nm)
to 15% (11 nm). Multiphonon relaxation and −OH quenching was
studied in these materials by measuring the vibrational characteristics
of β-NaYF<sub>4</sub>:Yb,Er nanospheres. While multiphonon relaxation
exhibited increased contribution to nonradiative decay, −OH
quenching rates were calculated to be ∼4 orders of magnitude
higher than that of the multiphonon relaxation. Therefore, surface
−OH quenching effects were concluded to be primarily responsible
for the observed dependence of emission intensity versus particle
size
Thermochemical Investigation of the Stability and Conversion of Nanocrystalline and High-Temperature Phases in Sodium Neodymium Fluorides
As important upconversion materials,
sodium rare-earth fluorides
(nominally NaREF4 in composition but actually often harboring
sodium deficiency, especially in nanophase materials) have been subjected
to intensive studies, particularly in the synthesis and applications
of nanocrystals. However, the mechanisms of the conversion between
the two phases (α and β) of NaREF4 nanocrystals
during the synthesis are still controversial and lack thermodynamic
investigations, which limit the rational design, synthesis, and processing
of these materials. In this work, aiming at NaREF4 with
light rare-earth elements, the thermochemistry of the NaF–NdF3 system, including the α and β phases in nanocrystalline/nanophase
and bulk stoichiometric samples, is systematically studied by thermogravimetry
and differential scanning calorimetry and high-temperature oxide melt
solution calorimetry. With the help of compositional analysis and
structural characterization, a strong Na deficiency is found in nanocrystals
with small crystal sizes, which leads to the formation of cubic (α)
crystallographic polymorphs at the nucleation stage, possibly because
of the relative thermodynamic stability of the α phase compared
to the β phase in such compositions. After converting to the
hexagonal (β) structure, the crystal growth is accompanied by
an increase of Na content in nanocrystals with increasing energetic
stability until the formation of the stoichiometric compound (β-NaNdF4). On the contrary, the stoichiometric α phase (α-NaNdF4) is metastable at room temperature but is the intermediate
phase as the temperature increases. We show that the α →
β phase conversion in aqueous solution synthesis is distinct
from the β → α transition driven by temperature
because of composition differences
Lanthanide Clusters with Internal Ln Ions: Highly Emissive Molecules with Solid-State Cores
“Er(SePh)2.5I0.5” reacts with elemental S to give (THF)10Er6S6I6, a double cubane cluster with
one face of the Er4S4 cube capped by an additional Er2S2. Reactions with a mixture of elemental S/Se
results in the formation of (THF)14Er10S6(Se2)6I6, a cluster composed of an Er6S6 double cubane core, with
two “Er2(Se2)3” units condensed onto opposing rectangular sides of the Er6S6 fragment. This deposition of
Er2Se6 totally encapsulates the two central Er with chalcogen atoms (4 S, 4 Se) and excludes neutral THF
donors or iodides from the two primary coordination spheres. The Er10 compound is the first lanthanide
cluster to contain internal, chalcogen encapsulated Ln. This cluster shows strong fluorescence at 1544 nm
with a measured decay time of 3 ms and an estimated quantum efficiency of 78%, which
is comparable to Er doped solid-state materials. The unusual fluorescence spectral properties of
(THF)14Er10S6Se12I6 are unprecedented for a molecular Er complex and are attributed to the low phonon
energy host environment provided by the I-, S2-, and Se22- ligands
Thiolate-Bound Thulium Compounds: Synthesis, Structure, and NIR Emission
Molecular (DME)2Tm(SC6F5)3 and tetrametallic (DME)4(μ2-SPh)8Tm4(SPh)4 have been isolated in high yield and characterized by conventional methods. The fluorinated thiolate has an eight-coordinate Tm(III) ion bound to three sulfur atoms from the thiolates, four oxygen donors from the THF ligands, and a relatively weak dative Tm−F interaction with a 2.842(3)Å Tm−F separation. The benzenethiolate compound crystallizes as a tetramer with an alternating number (3, 2, 3) of thiolates connecting the nearly linear array of Tm(III) ions. Emission properties of both thiolates and the chalcogen-rich cluster (THF)6Tm4Se9(SC6F5)2 have been established. The Ph compound is significantly more emissive than either of the fluorinated species
Thiolate-Bound Thulium Compounds: Synthesis, Structure, and NIR Emission
Molecular (DME)2Tm(SC6F5)3 and tetrametallic (DME)4(μ2-SPh)8Tm4(SPh)4 have been isolated in high yield and characterized by conventional methods. The fluorinated thiolate has an eight-coordinate Tm(III) ion bound to three sulfur atoms from the thiolates, four oxygen donors from the THF ligands, and a relatively weak dative Tm−F interaction with a 2.842(3)Å Tm−F separation. The benzenethiolate compound crystallizes as a tetramer with an alternating number (3, 2, 3) of thiolates connecting the nearly linear array of Tm(III) ions. Emission properties of both thiolates and the chalcogen-rich cluster (THF)6Tm4Se9(SC6F5)2 have been established. The Ph compound is significantly more emissive than either of the fluorinated species
Lanthanide Clusters with Internal Ln Ions: Highly Emissive Molecules with Solid-State Cores
“Er(SePh)2.5I0.5” reacts with elemental S to give (THF)10Er6S6I6, a double cubane cluster with
one face of the Er4S4 cube capped by an additional Er2S2. Reactions with a mixture of elemental S/Se
results in the formation of (THF)14Er10S6(Se2)6I6, a cluster composed of an Er6S6 double cubane core, with
two “Er2(Se2)3” units condensed onto opposing rectangular sides of the Er6S6 fragment. This deposition of
Er2Se6 totally encapsulates the two central Er with chalcogen atoms (4 S, 4 Se) and excludes neutral THF
donors or iodides from the two primary coordination spheres. The Er10 compound is the first lanthanide
cluster to contain internal, chalcogen encapsulated Ln. This cluster shows strong fluorescence at 1544 nm
with a measured decay time of 3 ms and an estimated quantum efficiency of 78%, which
is comparable to Er doped solid-state materials. The unusual fluorescence spectral properties of
(THF)14Er10S6Se12I6 are unprecedented for a molecular Er complex and are attributed to the low phonon
energy host environment provided by the I-, S2-, and Se22- ligands
Lanthanide Clusters with Internal Ln Ions: Highly Emissive Molecules with Solid-State Cores
“Er(SePh)2.5I0.5” reacts with elemental S to give (THF)10Er6S6I6, a double cubane cluster with
one face of the Er4S4 cube capped by an additional Er2S2. Reactions with a mixture of elemental S/Se
results in the formation of (THF)14Er10S6(Se2)6I6, a cluster composed of an Er6S6 double cubane core, with
two “Er2(Se2)3” units condensed onto opposing rectangular sides of the Er6S6 fragment. This deposition of
Er2Se6 totally encapsulates the two central Er with chalcogen atoms (4 S, 4 Se) and excludes neutral THF
donors or iodides from the two primary coordination spheres. The Er10 compound is the first lanthanide
cluster to contain internal, chalcogen encapsulated Ln. This cluster shows strong fluorescence at 1544 nm
with a measured decay time of 3 ms and an estimated quantum efficiency of 78%, which
is comparable to Er doped solid-state materials. The unusual fluorescence spectral properties of
(THF)14Er10S6Se12I6 are unprecedented for a molecular Er complex and are attributed to the low phonon
energy host environment provided by the I-, S2-, and Se22- ligands
Heterometallic Chalcogenido Clusters Containing Lanthanides and Main Group Metals: Emissive Precursors to Ternary Solid-State Compounds
Heterometallic clusters containing lanthanides and the group 12 metals can be isolated as
crystalline compounds in high yields. These products [(py)8Ln4M2Se6(SePh)4 (Ln = Er, Yb, Lu; M = Cd,
Hg)] adopt a double cubane structure with the covalent M occupying an opposing pair of external metal
sites. Both Er/M compounds are strongly emissive materials, with emission lifetimes of 1.41 ms (Er/Cd)
and 0.71 ms (Er/Hg) and with the Er/Cd radiative quantum efficiency twice that of the Er/Hg compound.
Thermal decomposition of the Er/Cd and Yb/Cd compounds at 650 °C give the ternary solid-state materials
CdLn2Se4
