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Quantum Dynamics of Polaron Formation
Quantum Dynamics of Polaron Formation
Li-Chung Ku1,2 and S. A. Trugman1
1 Theoretical Division, Los Alamos National Laboratory,
3
0 Los Alamos, New Mexico 87545, U.S.A.
0
2 2Department of Physics, University of California,
t
c Los Angeles, California 90024, U.S.A.
O
9 (Dated: February 2, 2008)
] Abstract
l
e
r- The formation of a polaron quasiparticle from a bare electron is studied in the framework of
t
s
t. the Holstein model of electron-phonon coupling. Using Schrodinger’s¨ formalism, we calculate the
a
m time evolution of the distribution of the electron and phonon density, lattice deformation, and the
-
d electron-phonon (el-ph) correlation functions in real space. The quantum dynamical nature of the
n
o phonons is preserved. The polaron formation time is related to the dephasing time of the continuum
c
[
of unbound phonon excited states in the spectral function, which depends on the phonon frequency
1
v and the el-ph coupling strength. As the el-ph coupling increases, qualitative changes in polaron
6
2 formation occur when the one-phonon polaron bound state forms. In the adiabatic regime, we find
2
0 that a potential barrier between the quasi-free and heavy polaron states exists in both 2D and 3D,
1
3 which is crucial for polaron formation dynamics. We compare to recent experiments.
0
/
t
a
m PACS numbers: 71.38.-k, 63.20-e, and 78.47.+p
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d
n
o
c
:
v
i
X
r
a
1
The polaron formation problem not only bears fundamental inte
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