- Main
Classical Limit on Quantum Mechanics for Unbounded Observables
- Tong, Pun Wai
- Advisor(s): Driver, Bruce K
Abstract
This dissertation is divided into two parts. In Part I of this dissertation--- On the Classical Limit of Quantum Mechanics, we extend a method introduced by Hepp in
1974 for studying the asymptotic behavior of quantum expectations in the limit
as Plank's constant ($\hbar$) tends to zero. The goal is to allow for
unbounded observables which are (non-commutative) polynomial functions of the
position and momentum operators. [This is in contrast to Hepp's original paper
where the "observables" were, roughly speaking, required to be bounded functions
of the position and momentum operators.] As expected the leading order
contributions of the quantum expectations come from evaluating the "symbols" of the observables along the classical trajectories while the next order contributions (quantum
corrections) are computed by evolving the $\hbar=1$ observables by a linear canonical
transformations which is determined by the second order pieces of the quantum mechanical Hamiltonian.
Part II of the dissertation --- Powers of Symmetric Differential Operators is devoted to operator theoretic properties of a class of linear symmetric differential operators on the real line. In more detail, let $L$ and $\tilde{L}$ be a linear symmetric differential operator with polynomial coefficients on $L^{2}\left(m \right) $ whose domain is the Schwartz test function space, $\mathcal{S}.$ We study conditions on the polynomial coefficients of $L$ and $\tilde{L}$ which implies operator comparison inequalities of the form $\left( \overline{\tilde{L}}+\tilde{C}\right) ^{r}\leq C_{r}\left( \bar{L}+C\right) ^{r}$
for all $0\leq r<\infty.$ These comparison inequalities (along with their generalizations
allowing for the parameter $\hbar>0$ in the coefficients) are used to supply a
large class of Hamiltonian operators which verify the assumptions needed for
the results in Part I of this dissertation.
Main Content
Enter the password to open this PDF file:
-
-
-
-
-
-
-
-
-
-
-
-
-
-