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Bipolaron Characteristics in a Cylindrical Quantum DotTable of Contents:
We consider the motion of the electron in the z -axis direction to be bounded by an infinite high rectangular potential well and bounded on the oxy-plane by a transversal parabolic potential. System HamiltonianThe Hamiltonian of the system is written in the form:
Here, V(z) is the confinement potential (infinite high rectangular potential well) in the direction of the oz-axis. The state of the electron is described by the variational wave function that has a large spread compared to the ground state wave function:
Averaging the Lagrangian 18.534 by the wave function 18.535 we have ч /
Here,
The model Lagrangian of the transversal motion: Model System Action FunctionalFrom the model Lagrangian 18.538 we have the model action functional
Following the procedure of path integration seen earlier then Equation of Motion / Normal ModesThe equations of motion for the transversal motion are
For normal modes we substitute the following
Solving for the eigenmodes we have ![]() with
The bipolaron effective mass is conveniently obtained from the eigenmode equations: Lagrangian DiagonalizationTo diagonalize the model Lagrangian, we move to normal coordinates:
Substituting these equations into the equation of motion and also considering the conservation of the kinetic energy in any representation then
and the model diagonalized Lagrangian in normal coordinates:
It shows that in the motion of the bipolaron we have four oscillators indicating four internal motions. Bipolaron Partition FunctionThe bipolaron partition function can be obtained from the equation: ![]() or
The Coulomb interaction can be written in the form: Bipolaron Generating FunctionWe find now (Svia the generating function:
Letting,
then
where Bipolaron EnergyWe again observe all the formulae in the bipolaron problem have the same dependence on the quantity |r -
where,
and
with
For Л0» 1 then
18.19 Polaron Characteristics in a Quasi-OD Cylindrical |
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