Abstract
We study examples of one dimensional matrix models whose potentials possess an energy spectrum that can be explicitly determined. This allows for an exact solution in the continuum limit. Specifically, step-like potentials and the Morse potential are considered. The step-like potentials show no scaling behaviour and the Morse potential (which corresponds to a {gamma} = -1 model) has the interesting feature that there are no quantum corrections to the scaling behaviour in the continuum limit. (author). 5 refs.
Citation Formats
Raju Viswanathan, R.
Exactly soluble matrix models.
IAEA: N. p.,
1991.
Web.
Raju Viswanathan, R.
Exactly soluble matrix models.
IAEA.
Raju Viswanathan, R.
1991.
"Exactly soluble matrix models."
IAEA.
@misc{etde_10113314,
title = {Exactly soluble matrix models}
author = {Raju Viswanathan, R}
abstractNote = {We study examples of one dimensional matrix models whose potentials possess an energy spectrum that can be explicitly determined. This allows for an exact solution in the continuum limit. Specifically, step-like potentials and the Morse potential are considered. The step-like potentials show no scaling behaviour and the Morse potential (which corresponds to a {gamma} = -1 model) has the interesting feature that there are no quantum corrections to the scaling behaviour in the continuum limit. (author). 5 refs.}
place = {IAEA}
year = {1991}
month = {Sep}
}
title = {Exactly soluble matrix models}
author = {Raju Viswanathan, R}
abstractNote = {We study examples of one dimensional matrix models whose potentials possess an energy spectrum that can be explicitly determined. This allows for an exact solution in the continuum limit. Specifically, step-like potentials and the Morse potential are considered. The step-like potentials show no scaling behaviour and the Morse potential (which corresponds to a {gamma} = -1 model) has the interesting feature that there are no quantum corrections to the scaling behaviour in the continuum limit. (author). 5 refs.}
place = {IAEA}
year = {1991}
month = {Sep}
}