hexagonal packing
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2021 ◽  
Author(s):  
Qian Li ◽  
Chady Moussallem ◽  
Frédéric Castet ◽  
Luca Muccioli ◽  
Marie-Anne Dourges ◽  
...  
Keyword(s):  

2021 ◽  
Author(s):  
Song Hu ◽  
Liangyu Hu ◽  
Xuefeng Zhu ◽  
Yuan Wang ◽  
Minghua Liu
Keyword(s):  

Author(s):  
Song Hu ◽  
Liangyu Hu ◽  
Xuefeng Zhu ◽  
Yuan Wang ◽  
Minghua Liu
Keyword(s):  

2021 ◽  
Vol 346 ◽  
pp. 02005
Author(s):  
Alexey Kuchugurov ◽  
Nikolay Shardakov ◽  
Inna Kovyazina ◽  
Nadezhda Lukoyanova

The technology for the formation of functional coatings from hollow glass microspheres by the self-organization method from aqueous-alcoholic suspensions is proposed. A monolayer with the closest (hexagonal) packing is shown to be formed on a solid (glass) substrate. The criterion for the ordering of a monolayer is proposed. The assessment of the influence of various technological factors on the monolayer formation rate and the degree of its ordering is given.


2020 ◽  
Vol 76 (6) ◽  
pp. 677-686
Author(s):  
Jeanine Concepcion H. Arias ◽  
Manuel Joseph C. Loquias

A linear isometry R of {\bb R}^{d} is called a similarity isometry of a lattice \Gamma\subseteq{\bb R}^{d} if there exists a positive real number β such that βRΓ is a sublattice of (finite index in) Γ. The set βRΓ is referred to as a similar sublattice of Γ. A (crystallographic) point packing generated by a lattice Γ is a union of Γ with finitely many shifted copies of Γ. In this study, the notion of similarity isometries is extended to point packings. A characterization for the similarity isometries of point packings is provided and the corresponding similar subpackings are identified. Planar examples are discussed, namely the 1 × 2 rectangular lattice and the hexagonal packing (or honeycomb lattice). Finally, similarity isometries of point packings about points different from the origin are considered by studying similarity isometries of shifted point packings. In particular, similarity isometries of a certain shifted hexagonal packing are computed and compared with those of the hexagonal packing.


2020 ◽  
Vol 101 (3) ◽  
Author(s):  
Samira Abedi ◽  
Chau-Chyun Chen ◽  
Siva A. Vanapalli

2020 ◽  
Author(s):  
Debasis Sen ◽  
Avik Das ◽  
Jitendra Bahadur ◽  
Priyanka Biswas
Keyword(s):  

2019 ◽  
Vol 50 (4) ◽  
pp. 422-427
Author(s):  
Chloe J. Pugh ◽  
Craig M. Robertson ◽  
Alexander Steiner

Abstract In the solid state diallylamine forms supramolecular helices with four molecules per pitch that are held together by hydrogen bonding. The helical structure is the result of competing length scales at which hydrogen bonding and second-neighbour Van-der-Waals interactions occur. The structure features two crystallographically independent helices and four unique molecules in the asymmetric unit (Z′ = 4). The high Z′ value is partly a consequence of the centrosymmetric pseudo-hexagonal packing of helical columns, which is incompatible with helical spacegroup symmetries. Graphic Abstract


2019 ◽  
Vol 67 (8) ◽  
pp. 5445-5457 ◽  
Author(s):  
Jesus Alberto Lopez-Fernandez ◽  
Rafael Gonzalez Ayestaran ◽  
Ignacio Santamaria ◽  
Christian Lameiro

Crystals ◽  
2019 ◽  
Vol 9 (3) ◽  
pp. 162 ◽  
Author(s):  
Yuri Yevdokimov ◽  
Sergey Skuridin ◽  
Viktor Salyanov ◽  
Sergey Semenov ◽  
Efim Kats

In this review, we compare the circular dichroism (CD) spectra of liquid-crystalline dispersion (LCD) particles formed in PEG-containing aqueous-salt solutions with the purpose of determining the packing of ds DNA molecules in these particles. Depending on the osmotic pressure of the solution, the phase exclusion of ds DNA molecules at room temperature results in the formation of LCD particles with the cholesteric or the hexagonal packing of molecules. The heating of dispersion particles with the hexagonal packing of the ds DNA molecules results in a new phase transition, accompanied by an appearance of a new optically active phase of ds DNA molecules. Our results are rationalized by way of a concept of orientationally ordered “quasinematic” layers formed by ds DNA molecules, with a parallel alignment in the hexagonal structure. These layers can adopt a twisted configuration with a temperature increase; and as a result of this process, a new, helicoidal structure of dispersion particle is formed (termed as the “re-entrant” cholesteric phase). To prove the cholesteric pattern of ds DNA molecules in this phase, the “liquid-like” state of the dispersion particles was transformed into its “rigid” counterpart.


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