TY - JOUR
T1 - Thermodynamic and Kinetic Origins of Lithiation-Induced Amorphous-to-Crystalline Phase Transition of Phosphorus
AU - Jung, Sung Chul
AU - Han, Young Kyu
N1 - Publisher Copyright:
© 2015 American Chemical Society.
PY - 2015/6/4
Y1 - 2015/6/4
N2 - (Figure Presented). Despite its fundamental importance, real-time observation of atomic motions during phase transition is challenging because the transition processes usually occur on ultrafast time scales. Herein, we directly monitored a fleeting and spontaneous crystallization of Li3P from amorphous LixP phases with x ∼ 3 at room temperature via first-principles molecular dynamics simulations. The crystallization is a collective atomic ordering process continued for 0.4 ps and it is driven by the following key impetuses: (1) the crystalline Li3P phase is more stable than its amorphous counterpart, (2) the amorphous LixP phase corresponds thermodynamically to the local minimum energy state at x ∼ 3, which enables its crystallization under an electrochemical equilibrium condition without net flux of lithium ions in the host material, (3) the crystalline and amorphous structures of Li3P are so similar that the average displacement of the mobile Li atoms during crystallization is only 0.56 Å, and (4) highly lithiated materials with all isolated host elements, such as the amorphous Li3P phase, are advantageous for crystallization because the isolation induces a kinetically favorable low-barrier transition without complicated multistep P-P bond breaking/forming processes.
AB - (Figure Presented). Despite its fundamental importance, real-time observation of atomic motions during phase transition is challenging because the transition processes usually occur on ultrafast time scales. Herein, we directly monitored a fleeting and spontaneous crystallization of Li3P from amorphous LixP phases with x ∼ 3 at room temperature via first-principles molecular dynamics simulations. The crystallization is a collective atomic ordering process continued for 0.4 ps and it is driven by the following key impetuses: (1) the crystalline Li3P phase is more stable than its amorphous counterpart, (2) the amorphous LixP phase corresponds thermodynamically to the local minimum energy state at x ∼ 3, which enables its crystallization under an electrochemical equilibrium condition without net flux of lithium ions in the host material, (3) the crystalline and amorphous structures of Li3P are so similar that the average displacement of the mobile Li atoms during crystallization is only 0.56 Å, and (4) highly lithiated materials with all isolated host elements, such as the amorphous Li3P phase, are advantageous for crystallization because the isolation induces a kinetically favorable low-barrier transition without complicated multistep P-P bond breaking/forming processes.
UR - http://www.scopus.com/inward/record.url?scp=84930959532&partnerID=8YFLogxK
U2 - 10.1021/acs.jpcc.5b02095
DO - 10.1021/acs.jpcc.5b02095
M3 - Article
AN - SCOPUS:84930959532
SN - 1932-7447
VL - 119
SP - 12130
EP - 12137
JO - Journal of Physical Chemistry C
JF - Journal of Physical Chemistry C
IS - 22
ER -