TY - JOUR
T1 - Solvent wrapped metastable colloidal crystals
T2 - Highly mutable colloidal assemblies sensitive to weak external disturbance
AU - Yang, Dongpeng
AU - Ye, Siyun
AU - Ge, Jianping
PY - 2013/12/11
Y1 - 2013/12/11
N2 - Solvent wrapped "metastable" crystalline colloidal arrays (CCAs) have been prepared by supersaturation induced precipitation and self-assembly of monodisperse particles in polar/nonpolar organic solvents. These metastable CCAs possess ordered structures but with less stability comparing with traditionally fixed colloidal crystal systems. They are stabilized by the balance between long-range attraction and electrostatic repulsion of neighboring like-charged particles. Monitoring the reflection intensity during evaporation suggests that these crystals can exist for several hours at 90 C and even longer at room temperature. Based on the evolution of particle volume fraction in whole suspension (φSiO2), crystal phase (φcrystal) , and liquid phase (φliquid), the formation of metastable CCAs can be understood as a microscopic phase separation process, where the homogeneous dispersion will separate into a "crystal phase" with orderly stacked particles and a "liquid phase" with randomly dispersed particles. Further calculation of the volume fraction of crystal phase (V crystal/Vtotal) and the ratio of particles in crystal phase (fcrystal) shows that with the increase of designed ΦSiO2, more particles precipitate to form colloidal crystals with larger sizes but the lattice spacing of the microcrystals remains constant. Unlike fixed or traditional responsive CCAs, these metastable CCAs can reversibly assemble and disassemble with great ease, because little energy is involved or required in this transformation. Therefore, they can sense weak external disturbances, including subtle motion and slight friction or shearing forces.
AB - Solvent wrapped "metastable" crystalline colloidal arrays (CCAs) have been prepared by supersaturation induced precipitation and self-assembly of monodisperse particles in polar/nonpolar organic solvents. These metastable CCAs possess ordered structures but with less stability comparing with traditionally fixed colloidal crystal systems. They are stabilized by the balance between long-range attraction and electrostatic repulsion of neighboring like-charged particles. Monitoring the reflection intensity during evaporation suggests that these crystals can exist for several hours at 90 C and even longer at room temperature. Based on the evolution of particle volume fraction in whole suspension (φSiO2), crystal phase (φcrystal) , and liquid phase (φliquid), the formation of metastable CCAs can be understood as a microscopic phase separation process, where the homogeneous dispersion will separate into a "crystal phase" with orderly stacked particles and a "liquid phase" with randomly dispersed particles. Further calculation of the volume fraction of crystal phase (V crystal/Vtotal) and the ratio of particles in crystal phase (fcrystal) shows that with the increase of designed ΦSiO2, more particles precipitate to form colloidal crystals with larger sizes but the lattice spacing of the microcrystals remains constant. Unlike fixed or traditional responsive CCAs, these metastable CCAs can reversibly assemble and disassemble with great ease, because little energy is involved or required in this transformation. Therefore, they can sense weak external disturbances, including subtle motion and slight friction or shearing forces.
UR - https://www.scopus.com/pages/publications/84890467113
U2 - 10.1021/ja405670r
DO - 10.1021/ja405670r
M3 - 文章
AN - SCOPUS:84890467113
SN - 0002-7863
VL - 135
SP - 18370
EP - 18376
JO - Journal of the American Chemical Society
JF - Journal of the American Chemical Society
IS - 49
ER -