Advances in single crystals and thin films of chiral hybrid metal halides

Author(s):  
Zhihang Guo ◽  
Junzi Li ◽  
Rui Chen ◽  
Tingchao He
2019 ◽  
Vol 7 (36) ◽  
pp. 20733-20741 ◽  
Author(s):  
Mehri Ghasemi ◽  
Miaoqiang Lyu ◽  
Md Roknuzzaman ◽  
Jung-Ho Yun ◽  
Mengmeng Hao ◽  
...  

The phenethylammonium cation significantly promotes the formation of fully-covered thin-films of hybrid bismuth organohalides with low surface roughness and excellent stability.


1997 ◽  
Vol 70 (11) ◽  
pp. 1468-1470 ◽  
Author(s):  
R. Gaffney ◽  
C. Hucho ◽  
J. R. Feller ◽  
M. J. McKenna ◽  
B. K. Sarma ◽  
...  

2002 ◽  
Vol 507-510 ◽  
pp. 223-228 ◽  
Author(s):  
L. Plucinski ◽  
T. Strasser ◽  
B.J. Kowalski ◽  
K. Rossnagel ◽  
T. Boetcher ◽  
...  

2013 ◽  
Vol 117 (50) ◽  
pp. 26675-26679 ◽  
Author(s):  
Reza Kakavandi ◽  
Sabine-Antonia Savu ◽  
Andrea Caneschi ◽  
Maria Benedetta Casu

2013 ◽  
Vol 84 (12) ◽  
pp. 123905 ◽  
Author(s):  
Anand Kamlapure ◽  
Garima Saraswat ◽  
Somesh Chandra Ganguli ◽  
Vivas Bagwe ◽  
Pratap Raychaudhuri ◽  
...  

2016 ◽  
Vol 1 (1) ◽  
pp. 19-32
Author(s):  
V.N Praveen ◽  
◽  
R Sakthi Sudar Saravanan ◽  
M Meena ◽  
◽  
...  

2003 ◽  
Vol 784 ◽  
Author(s):  
A. K. Tagantsev ◽  
P. Muralt ◽  
J. Fousek

ABSTRACTA simple theory for the shape of the piezoelectric hysteresis loops (piezoelectric coefficient d vs. applied electric field E) is developed for the case of non-ferroelelastic 180° switching in ferroelectrics. The theory provides explanations for specific features of piezoelectric hysteresis loops, which have been observed in single crystals, thin films and in ceramics in particular. The piezoelectric coefficient may show a “hump”, i.e. when E decreases from the tip of the loop down to zero, d passes through a maximum, and a “nose”, i.e. a self-crossing of the loop close to its tips. The theory also explains the difference in the coercive fields seen in the polarization and piezoelectric loops.


2004 ◽  
Vol 829 ◽  
Author(s):  
Ali N. Rashid ◽  
Donald C. Craig

Tris-(8-hydroxyquinoline) aluminum III (Alq3) is a stable metal chelate that has received a great deal of attention over the past years due to its use in the fabrication of organic light emitting diodes (OLED).[1,2] Despite all the interest in this remarkable material very little information on its' solid-state properties and packing exists. Nearly all of the available information comes from studies that have been carried out on vacuum deposited thin films.[1]


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