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Figure 3 Hollow TiO 2 particles.
Figure 2 TEM images of hollow TiO 2 particles.
(2) Particles were adsorbed to a preexisting support film.
These minerals were also components of category 1 and 2 particles.
Figure 2 XRD pattern of SnS 2 particles at different reaction times.
Open image in new window Figure 1 SEM images of TiO 2 particles.
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Although the name is no longer appropriate, it has been retained to describe all spin-1/2 particles that do not feel the strong force.
Dirac's theory, in fact, applies to any subatomic particle with spin 1/2; therefore, all spin-1/2 particles should have corresponding antiparticles.
The PLGA composite films including Mg(OH 2 particles were prepared by a solvent casting method.
Such behaviour can be described by the Dirac equation for spin 1/2 particles [1 6].
For comparison, CNTs provide cross-linking conductive cages for Pb NO3 2 particles.
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