Polarized fluorescence of a crystal having uniaxially oriented molecules by a carbazole-diyl-bridged macrocage

CrystEngComm ◽  
2019 ◽  
Vol 21 (26) ◽  
pp. 3910-3914 ◽  
Author(s):  
Hikaru Hashimoto ◽  
Yusuke Inagaki ◽  
Hiroyuki Momma ◽  
Eunsang Kwon ◽  
Kentaro Yamaguchi ◽  
...  

An axially oriented π-electron system is achieved in a single crystal of a macrocage molecule, and polarized fluorescence of the single crystal was observed.

1978 ◽  
Vol 69 (8) ◽  
pp. 3639-3646 ◽  
Author(s):  
Michel Lamotte ◽  
Salomon Risemberg ◽  
Anne‐Marie Merle ◽  
Jacques Joussot–Dubien

1979 ◽  
Vol 70 (4) ◽  
pp. 2050-2050
Author(s):  
Michel Lamotte ◽  
Salomon Risemberg ◽  
Anne‐Marie Merle ◽  
Jacques Joussot‐Dubien

2016 ◽  
Vol 94 (20) ◽  
Author(s):  
T. Eknapakul ◽  
I. Fongkaew ◽  
S. Siriroj ◽  
R. Vidyasagar ◽  
J. D. Denlinger ◽  
...  

1998 ◽  
Vol 108 (17) ◽  
pp. 7327-7333 ◽  
Author(s):  
M. Muccini ◽  
E. Lunedei ◽  
A. Bree ◽  
G. Horowitz ◽  
F. Garnier ◽  
...  

1986 ◽  
Vol 41 (12) ◽  
pp. 1490-1494 ◽  
Author(s):  
Christian Robl ◽  
Armin Weiss

Abstract In SrC4O4-3H2O (type I), Sr2+ has CN 8. It is surrounded by 3 water molecules and 5 oxygen atoms of 4 different squarate dianions. The C-O and C-C bond lengths are typical of extensive delocalization of the π-electron system. The connection of Sr2+ and C4O42- leads to infinite layers, obviously interlinked by hydrogen bonding.The oxygens of the squarate behave differently: two are Sr-chelating, but simultaneously bound to two additional Sr2+, one is connected with one Sr2+ only, and the fourth is not bound to any Sr2+. The single crystal character remained in principle unchanged during dehydration to SrC4O4 · 1 H2O and subsequent rehydration to the trihydrate. Grinding of a crystal treated in this way led to a new modification of SrC4O4 ·3 H2O.


Author(s):  
Akira Tanaka ◽  
David F. Harling

In the previous paper, the author reported on a technique for preparing vapor-deposited single crystal films as high resolution standards for electron microscopy. The present paper is intended to describe the preparation of several high resolution standards for dark field microscopy and also to mention some results obtained from these studies. Three preparations were used initially: 1.) Graphitized carbon black, 2.) Epitaxially grown particles of different metals prepared by vapor deposition, and 3.) Particles grown epitaxially on the edge of micro-holes formed in a gold single crystal film.The authors successfully obtained dark field micrographs demonstrating the 3.4Å lattice spacing of graphitized carbon black and the Au single crystal (111) lattice of 2.35Å. The latter spacing is especially suitable for dark field imaging because of its preparation, as in 3.), above. After the deposited film of Au (001) orientation is prepared at 400°C the substrate temperature is raised, resulting in the formation of many square micro-holes caused by partial evaporation of the Au film.


Author(s):  
L. E. Murr ◽  
G. Wong

Palladium single-crystal films have been prepared by Matthews in ultra-high vacuum by evaporation onto (001) NaCl substrates cleaved in-situ, and maintained at ∼ 350° C. Murr has also produced large-grained and single-crystal Pd films by high-rate evaporation onto (001) NaCl air-cleaved substrates at 350°C. In the present work, very large (∼ 3cm2), continuous single-crystal films of Pd have been prepared by flash evaporation onto air-cleaved (001) NaCl substrates at temperatures at or below 250°C. Evaporation rates estimated to be ≧ 2000 Å/sec, were obtained by effectively short-circuiting 1 mil tungsten evaporation boats in a self-regulating system which maintained an optimum load current of approximately 90 amperes; corresponding to a current density through the boat of ∼ 4 × 104 amperes/cm2.


Author(s):  
D. J. Barber ◽  
R. G. Evans

Manganese (II) oxide, MnO, in common with CoO, NiO and FeO, possesses the NaCl structure and shows antiferromagnetism below its Neel point, Tn∼ 122 K. However, the defect chemistry of the four oxides is different and the magnetic structures are not identical. The non-stoichiometry in MnO2 small (∼2%) and below the Tn the spins lie in (111) planes. Previous work reported observations of magnetic features in CoO and NiO. The aim of our work was to find explanations for certain resonance results on antiferromagnetic MnO.Foils of single crystal MnO were prepared from shaped discs by dissolution in a mixture of HCl and HNO3. Optical microscopy revealed that the etch-pitted foils contained cruciform-shaped precipitates, often thick and proud of the surface but red-colored when optically transparent (MnO is green). Electron diffraction and probe microanalysis indicated that the precipitates were Mn2O3, in contrast with recent findings of Co3O4 in CoO.


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