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synthetic opal
The heat capacity at constant pressure (in the range 3-50 K) and the lattice heat conductivity (from 5 to 75 K) of a single-crystal synthetic opal are measured.
      
The [111] longitudinal sound velocity (vL) in a single-crystal synthetic opal has been measured at a frequency of 10 MHz in the temperature range 4.2-300 K.
      
Erbium oxide and silicates were embedded in the pores of synthetic opal by using the chemical bath deposition technique.
      
The dominant relaxation mechanism of gallium embedded in an synthetic opal matrix changes from magnetic dipole to electrical quadrupole.
      
The Bragg diffraction spectrum of a synthetic opal with pores filled by the vanadium dioxide semiconductor (VO2) was found to be strongly affected by 0.1-μs-long YAG:Nd laser first-harmonic pulses (1.06 μm).
      
Thermal conductivity of HgSe loaded in the pore lattice of a synthetic opal single crystal
      
Thermal conductivity of NaCl loaded in regular arrays of nanovoids in a synthetic opal single crystal
      
The selective reflection spectra of films prepared from the photonic crystal, i.e., synthetic opal, are investigated.
      
Luminescence from ZnO quantum dots deposited with synthetic opal
      
Photoluminescence from ZnO layers of varied thickness deposited onto the surface of synthetic opal has been studied.
      
The spectra of transmission and reflection of synthetic opal which has 3-dimensional periodic structure were measured at different orientations of incident beam relative to the sample facets.
      
Several semiconductor materials, including TiO2, CdS, and ZnSe, were successfully used to achieve a controllable red-shift of the stop band position of synthetic opal.
      
We have studied light scattering in synthetic opal crystals infiltrated with ferroelectric sodium nitrite, NaNO2, and have analyzed simple models for the energy band structure of photonic crystals.
      
Reflection spectra of uninfiltrated and Ba(NO3)2-infiltrated synthetic opal photonic crystals
      
The reflection spectra of uninfiltrated and Ba(NO3)2-infiltrated synthetic opal crystals have been measured using a halogen lamp with a quasi-continuous near-UV through IR spectrum as the light source.
      
Our results indicate that synthetic opal crystals can be used as photon traps for studying the emission spectra of organic and inorganic materials infiltrated in opal pores.
      
We describe the fabrication of an opal-sulfur composite through vacuum infiltration of synthetic opal with molten sulfur.
      
The emission centers in synthetic opal have been tentatively identified.
      
It has been found that on exposure of specimens of synthetic opal to UV radiation, luminescence is excited in them (337 nm) that has spectral maxima at 400 and 500 nm.
      
Inverse gold photonic crystals were fabricated from synthetic opal templates composed of 290 nm silica spheres.
      
 

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