On a one-dimensional variational problem related to the Cahn–Hilliard energy in a bent strip-like domain

2001 ◽  
Vol 47 (2) ◽  
pp. 1059-1068 ◽  
Author(s):  
Kazuhiro Kurata ◽  
Masataka Shibata
2004 ◽  
Vol 83 (7) ◽  
pp. 747-756
Author(s):  
G. Cardone ◽  
A. Corbo Esposito † ◽  
V. V. Zhikov ‡

2020 ◽  
Vol 102 (1) ◽  
pp. 118-125
Author(s):  
LAURENT BÉTERMIN

We consider a deformation $E_{L,\unicode[STIX]{x1D6EC}}^{(m)}(it)$ of the Dedekind eta function depending on two $d$-dimensional simple lattices $(L,\unicode[STIX]{x1D6EC})$ and two parameters $(m,t)\in (0,\infty )$, initially proposed by Terry Gannon. We show that the minimisers of the lattice theta function are the maximisers of $E_{L,\unicode[STIX]{x1D6EC}}^{(m)}(it)$ in the space of lattices with fixed density. The proof is based on the study of a lattice generalisation of the logarithm, called the lattice logarithm, also defined by Terry Gannon. We also prove that the natural logarithm is characterised by a variational problem over a class of one-dimensional lattice logarithms.


2020 ◽  
Vol 70 (6) ◽  
pp. 1381-1412
Author(s):  
Veronika Chrastinová ◽  
Václav Tryhuk

AbstractFundamental concepts for variational integrals evaluated on the solutions of a system of ordinary differential equations are revised. The variations, stationarity, extremals and especially the Poincaré-Cartan differential forms are relieved of all additional structures and subject to the equivalences and symmetries in the widest possible sense. Theory of the classical Lagrange variational problem eventually appears in full generality. It is presented from the differential forms point of view and does not require any intricate geometry.


1968 ◽  
Vol 1 (2) ◽  
pp. 16-22 ◽  
Author(s):  
N. S. Galyun ◽  
A. N. Kraiko

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