Cargando…

A random tiling model for two dimensional electrostatics /

Part A.A Random Tiling Model for Two Dimensional Electrostatics: Introduction Definitions, statement of results and physical interpretation Reduction to boundary-influenced correlations A simple product formula for correlations along the boundary A $(2m+2n)$-fold sum for $\omega_b$ Separation of the...

Descripción completa

Detalles Bibliográficos
Clasificación:Libro Electrónico
Autor principal: Ciucu, Mihai, 1968-
Formato: Electrónico eBook
Idioma:Inglés
Publicado: Providence, R.I. : American Mathematical Society, 2005.
Colección:Memoirs of the American Mathematical Society ; no. 839.
Temas:
Acceso en línea:Texto completo
Tabla de Contenidos:
  • A random tiling model for two dimensional electrostatics 1. Introduction 2. Definitions, statement of results and physical interpretation 3. Reduction to boundary-influenced correlations 4. A simple product formula for correlations along the boundary 5. A $(2m + 2n)$-fold sum for $\omega _b$ 6. Separation of the $(2m + 2n)$-fold sum for $\omega _b$ in terms of $4mn$-fold integrals 7. The asymptotics of the $T^{(n)}$'s and $T'^{(n)}$'s 8. Replacement of the $T^{(k)}$'s and $T'^{(k)}$'s by their asymptotics 9. Proof of Proposition 7.2 10. The asymptotics of a multidimensional Laplace integral 11. The asymptotics of $\omega _b$. Proof of Theorem 2.2 12. Another simple product formula for correlations along the boundary 13. The asymptotics of $\bar {\omega }_b$. Proof of Theorem 2.1 14. A conjectured general two dimensional superposition principle 15. Three dimensions and concluding remarks B. Plane partitions I: A generalization of MacMahon's formula 1. Introduction 2. Two families of regions 3. Reduction to simply-connected regions 4. Recurrences for $\mathrm {M}(R_{\mathbf {l}, \mathbf {q}}(x))$ and $\mathrm {M}(\bar {R}_{\mathbf {l}, \mathbf {q}}(x))$ 5. Proof of Proposition 2.1 6. The guessing of $\mathrm {M}(R_{\mathbf {l}, \mathbf {q}}(x))$ and $\mathrm {M}(\bar {R}_{\mathbf {l}, \mathbf {q}}(x))$