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Journal of Magnetism and Magnetic Materials

Specific heat critical amplitudes and the approach to bulk criticality in parallel plate geometries

Marcelo M. Leite, A. M. Nemirovsky, Mauricio D. Coutinho-Filho

Published Feb 1, 1992• 6 citations
Publisher
DOI
10.1016/0304-8853(92)90756-e

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•Jan 1, 2000•0 citations
We present analytical and numerical results for the specific heat and susceptibility amplitude ratios in parallel plate geometries. The results are derived using field-theoretic techniques suitable to describe the system in the bulk limit, i.e., $(L/{\ensuremath{\xi}}_{\ifmmode\pm\else\textpm\fi{}})\ensuremath{\gg}1,$ where L is the distance between the plates and ${\ensuremath{\xi}}_{\ifmmode\pm\else\textpm\fi{}}$ is the correlation length above (+) and below $(\ensuremath{-})$ the bulk critical temperature. Advantages and drawbacks of our method are discussed in the light of other approaches previously reported in the literature.
The present work investigates the influence of real boundary conditions on the critical behaviour of confined system close to the temperature of a second order phase transition of the bulk. This is done analytically by applying the methods of the field theory of critical phenomena to a half-space geometry with a completely suppressed order parameter on the surface, the so-called Dirichlet boundary conditions. For the first time the surface specific heat is calculated to next to leading order in a fixed dimension both above and below the critical temperature. The results are compared with the data of recent experiments on Helium in plate geometry close to the lambda transition. Apart from the experimentally known bulk amplitudes no adaptable parameters are used. Above the critical temperature a semi-quantitative agreement of theory and experiment is found, whereas the experimental data cannot be explained below the lambda point. Possible reasons for this discrepancy are discussed. Secondly a new method to approximate Dirichlet boundary conditions in Monte Carlo simulations of lattice spin systems is presented. In comparison with established realizations both a better suppression of the order parameter on the boundary and the theoretically predicted scaling behaviour is achieved. Data generated with the new method shows agreement with theory within the expected errors.