The programmed crystallization of particles into lowsymmetry lattices represents a major synthetic challenge in the field of colloidal crystal engineering. Herein, we report an approach to realizing such structures that relies on a library of low-symmetry Au nanoparticles, with synthetically adjustable dimensions and tunable aspect ratios. When modified with DNA ligands and used as building blocks for colloidal crystal engineering, these structures enable one to expand the types of accessible lattices and to answer mechanistic questions about phase transitions that break crystal symmetry. Indeed, crystals formed from a library of elongated rhombic dodecahedra yield a rich phase space, including low-symmetry lattices (body-centered tetragonal and hexagonal planar). Molecular dynamics simulations corroborate and provide insight into the origin of these phase transitions. In particular, we identify an unexpected asymmetry in the DNA shell, distinct from both the particle and lattice symmetries, which enables directional, nonclose-packed interactions.
Sublattice melting is the loss of
order of one lattice component
in binary or ternary ionic crystals upon increasing the temperature.
A related transition has been predicted in colloidal crystals. To
understand the nature of this transition, we study delocalization
in self-assembled, size-asymmetric binary colloidal crystals using
a generalized molecular dynamics model. Focusing on body-centered
cubic (BCC) lattices, we observe a smooth change from localized-to-delocalized
interstitial particles for a variety of interaction strengths. Thermodynamic
arguments, mainly the absence of a discontinuity in the heat capacity,
suggest that the passage from localization-to-delocalization is continuous
and not a phase transition. This change is enhanced by lattice vibrations,
and the temperature of the onset of delocalization can be tuned by
the strength of the interaction between the colloid species. Therefore,
the localized and delocalized regimes of the sublattice are dominated
by enthalpic and entropic driving forces, respectively. This work
sets the stage for future studies of sublattice melting in colloidal
systems with different stoichiometries and lattice types and it provides
insights into superionic materials, which have the potential for application
in energy storage technologies.
High-performance materials rely on small reorganization energies to facilitate both charge separation and charge transport. Here, we performed DFT calculations to predict small reorganization energies of rectangular silicene nanoclusters with hydrogen-passivated edges denoted by H-SiNC. We observe that across all geometries, H-SiNCs feature large electron
Utilizing density functional theory (DFT) and a complete active space self-consistent field (CASSCF) approach,we study the electronic properties of rectangular silicene nano clusters with hydrogen passivated edges denoted by H-SiNCs (n,n), with n and n representing the zigzag and armchair directions, respectively. The results show that in the n direction, the H-SiNCs prefer to be in a singlet (S = 0) ground state for n > n. However, a transition from a singlet (S = 0) to a triplet (S = 1) ground state is revealed for n > n. Through the calculated Raman spectrum, the S = 0 and S = 1 ground states can be observed by the E (G) and A (D) Raman modes. Furthermore, H-SiNC clusters are shown to have HOMO-LUMO (HL) energy gaps, which decrease as a function of n and n for S = 0 and S = 1 states. The H-SiNC with a S = 1 ground state can be potentially used for silicene-based spintronic devices.
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