Abstract
A one-dimensional (1D) field theory that ascribes an energy to any given contour much in the way that it is done for polymers and self-repelling polymers is presented. The structure of this theory involves averages that have to be calculated with respect to the same Hamiltonian.
Original language | English |
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Pages (from-to) | 1283-1286 |
Number of pages | 4 |
Journal | Physical Review Letters |
Volume | 86 |
Issue number | 7 |
DOIs | |
State | Published - 12 Feb 2001 |