scholarly journals Polyhedra and packings from hyperbolic honeycombs

2018 ◽  
Vol 115 (27) ◽  
pp. 6905-6910 ◽  
Author(s):  
Martin Cramer Pedersen ◽  
Stephen T. Hyde

We derive more than 80 embeddings of 2D hyperbolic honeycombs in Euclidean 3 space, forming 3-periodic infinite polyhedra with cubic symmetry. All embeddings are “minimally frustrated,” formed by removing just enough isometries of the (regular, but unphysical) 2D hyperbolic honeycombs {3,7}, {3,8}, {3,9}, {3,10}, and {3,12} to allow embeddings in Euclidean 3 space. Nearly all of these triangulated “simplicial polyhedra” have symmetrically identical vertices, and most are chiral. The most symmetric examples include 10 infinite “deltahedra,” with equilateral triangular faces, 6 of which were previously unknown and some of which can be described as packings of Platonic deltahedra. We describe also related cubic crystalline packings of equal hyperbolic discs in 3 space that are frustrated analogues of optimally dense hyperbolic disc packings. The 10-coordinated packings are the least “loosened” Euclidean embeddings, although frustration swells all of the hyperbolic disc packings to give less dense arrays than the flat penny-packing even though their unfrustrated analogues in H2 are denser.

Author(s):  
Wenwu Cao

Domain structures play a key role in determining the physical properties of ferroelectric materials. The formation of these ferroelectric domains and domain walls are determined by the intrinsic nonlinearity and the nonlocal coupling of the polarization. Analogous to soliton excitations, domain walls can have high mobility when the domain wall energy is high. The domain wall can be describes by a continuum theory owning to the long range nature of the dipole-dipole interactions in ferroelectrics. The simplest form for the Landau energy is the so called ϕ model which can be used to describe a second order phase transition from a cubic prototype,where Pi (i =1, 2, 3) are the components of polarization vector, α's are the linear and nonlinear dielectric constants. In order to take into account the nonlocal coupling, a gradient energy should be included, for cubic symmetry the gradient energy is given by,


1978 ◽  
Vol 3 ◽  
pp. 479-501 ◽  
Author(s):  
E. Du Trémolet de Lacheisserie ◽  
P. Morin ◽  
J. Rouchy

2021 ◽  
Vol 60 (16) ◽  
pp. 9009-9014
Author(s):  
George Serghiou ◽  
Hans Josef Reichmann ◽  
Nicholas Odling ◽  
Kristina Spektor ◽  
Anna Pakhomova ◽  
...  
Keyword(s):  
Group Iv ◽  

2021 ◽  
Vol 47 (1) ◽  
pp. 7-13
Author(s):  
S. V. Gudina ◽  
A. S. Bogolubskiy ◽  
V. N. Neverov ◽  
K. V. Turutkin ◽  
N. G. Shelushinina ◽  
...  

2021 ◽  
Vol 103 (12) ◽  
Author(s):  
Nazir Khan ◽  
Danil Prishchenko ◽  
Mary H. Upton ◽  
Vladimir G. Mazurenko ◽  
Alexander A. Tsirlin
Keyword(s):  

Author(s):  
R. Ya. Rasulov ◽  
V. R. Rasulov ◽  
I. Eshboltaev ◽  
R. R. Sultonov

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