Control of the Trajectories of Positively and Negatively Charged Particles by Reflection from a Chain of Bent Single Crystals

2020 ◽  
Vol 65 (5) ◽  
pp. 820-825
Author(s):  
V. A. Maisheev ◽  
M. Yu. Chesnokov
Keyword(s):  
Single Crystals ◽  
Charged Particles ◽  
A Chain

scholarly journals Ratchet transport for a chain of interacting charged particles

2005 ◽  
Vol 71 (1) ◽  
Author(s):  
S. I. Denisov ◽  
E. S. Denisova ◽  
Peter Hänggi
Keyword(s):  
Charged Particles ◽  
A Chain

Die Struktur des Rubidiumtrimolybdathydrats Rb2Mo3O10 · H2O / The Structure of the Rubidiumtrimolybdate Hydrate Rb2Mo3O10 · H2O

1980 ◽  
Vol 35 (2) ◽  
pp. 242-244 ◽  
Author(s):  
Hans-Ulrich Kreusler ◽  
Achim Förster ◽  
Joachim Fuchs
Keyword(s):  
Structural Analysis ◽  
Single Crystals ◽  
Oh Groups ◽  
Primary Precipitate ◽  
A Chain ◽  
First Time ◽  
Identity Period ◽  
Oxygen Atoms

Abstract For the first time single crystals of trimolybdate were obtained through a slow trans-formation of the primary precipitate in a slightly acidified solution of rubidium molybdate at a temperature of 70 °C. A structural analysis of Rb2Mo3O10 · H2O revealed that the anion forms a chain with a hexameric identity period built up from MoO6 octahedra. Each Mo atom is bonded with two terminal oxygen atoms. The anion doesn't contain OH groups.

scholarly journals Crystal structure of chain silicate Cs3LuSi3O9

2021 ◽  
Vol 77 (12) ◽  
Author(s):  
Hiromitsu Kimura ◽  
Hisanori Yamane
Keyword(s):  
Crystal Structure ◽  
Single Crystals ◽  
Title Compound ◽  
Three Dimensional ◽  
Unit Cell ◽  
Single Chain ◽  
Orthorhombic Space Group ◽  
Space Group ◽  
Chain Silicate ◽  
A Chain

A caesium lutetium(III) silicate, Cs3LuSi3O9, was synthesized by heating a pelletized mixture of Cs2CO3, Lu2O3 and SiO2 at 1273 K. Single crystals of the title compound were grown in a melted area of the pellet. Cs3LuSi3O9 is a single-chain silicate (orthorhombic space group Pna21) with a chain periodicity of six and is isostructural with Cs3 RE IIIGe3O9 (RE = Pr, Nd and Sm–Yb). The two symmetry-dependent [Si6O18]12− chains in the unit cell lie parallel to the [011] direction. The Lu3+ ions are octahedrally coordinated by O atoms of the silicate chains, generating a three-dimensional framework. Cs+ ions are located in the voids in the framework.

Comments on the scattering of charged particles by single crystals I. The general case

1971 ◽  
Vol 10 (1-2) ◽  
pp. 33-42 ◽  
Author(s):  
C. S. Newton ◽  
L. T. Chadderton
Keyword(s):  
Single Crystals ◽  
Charged Particles

scholarly journals The Twin Physics Interpretation of Gravitational Waves

2017 ◽  
Vol 10 (1) ◽  
pp. 23 ◽  
Author(s):  
Anna C.M. Backerra
Keyword(s):  
Black Holes ◽  
Black Hole ◽  
Gravitational Waves ◽  
Charged Particles ◽  
Solid Particles ◽  
Mathematical Language ◽  
Particle Pairs ◽  
A Chain ◽  
The Relationship ◽  
Oppositely Charged

Gravitational waves may originate in two approaching black holes, circling around each other until they merge together. This phenomenon is considered by using twin physics, based upon a complementary mathematical language, after fitting Einstein’s idea about the relationship between time and space into it. According to the description obtained, the two black holes are annihilated as soon as they touch each other; only after a rearrangement of the constituent Heisenberg-units, these being units of potential energy, one new black hole is generated. During this rearrangement, a pair of oppositely charged particles appears, which is considered to be the birth of electromagnetism. This occurs during a period of time which is principally too short to measure, which seems to be the reason for the apparent merging of the black holes. The expectation is that extraordinarily large signals will be repeatedly received, related to a chain of annihilations of black solid particle pairs and subsequent generations of single black solid particles. We suppose that these signals represent gravitational waves.

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