Synthesis, Crystal Structures, and Nonlinear Optic and Thermal Properties of Two Diiodocarbazole Derivatives

2017 ◽  
Vol 41 (2) ◽  
pp. 79-81 ◽  
Author(s):  
Gui-Mei Tang ◽  
Rui-Hai Chi ◽  
Wen-Zhu Wan ◽  
Yong-Tao Wang ◽  
Yue-Zhi Cui ◽  
...  

Two 3,6-diiodocarbazole derivatives were prepared from the iodination of the corresponding phenylcarbazole. 3,6-Diiodo-9-phenylcarbazole crystallises in the chiral space group P21 and shows good second-harmonic generation effects. Thermogravimetric analysis of the two compounds shows high thermal stabilities, in which the decomposition temperature for 1 and 2 are 273 and 308 °C, respectively.

Author(s):  
P. Raghavaiah ◽  
R. Kuladeep ◽  
D. Narayana Rao ◽  
A. Jyothi Lakshmi ◽  
P. Srujana ◽  
...  

Heterocyclic building blocks possessing ethylene spacer and amine functionality such as 1-(2-aminoethyl)piperidine (1,2-AEPi), 2-(2-aminoethyl)pyridine (2,2-AEPy) and 1-(2-aminoethyl)pyrrolidine (1,2-AEPr) were reacted with tetracyanoquinodimethane (TCNQ) to give disubstituted compounds namely bis-(1-(2-aminoethyl)piperidino)dicyanoquinodimethane (1), bis-(2-(2-aminoethyl)pyridino)dicyanoquinodimethane (2) and bis-(1-(2-aminoethyl)pyrrolidino)dicyanoquinodimethane (3). Utilization of 1,2-AEPi, 2,2-AEPy and 1,2-AEPr as disubstituents on TCNQ has resulted in interesting crystal structures. Inter- and intramolecular hydrogen-bond mediated and expanded supramolecular structures were observed in the lattices of the crystals. Strong fluorescence was observed in solids and solutions. (2) showed a strong second harmonic generation (SHG) whereas (1) and (3) were found to be SHG inactive. All compounds possess good thermal stabilities.


1998 ◽  
Vol 37 (9) ◽  
pp. 2158-2165 ◽  
Author(s):  
Géraldine Lenoble ◽  
Pascal G. Lacroix ◽  
Jean Claude Daran ◽  
Santo Di Bella ◽  
Keitaro Nakatani

1977 ◽  
Vol 55 (17) ◽  
pp. 3081-3085 ◽  
Author(s):  
K. Ann Kerr ◽  
P. M. Boorman ◽  
B. S. Misener ◽  
J. G. H. van Roode

Crystals of tricyclohexylphosphine sulphide, C18H33PS, are orthorhombic, a = 10.906(2), b = 15.836(2), c = 10.362(2) Å, Z = 4, space group Pn21a. The structure was solved by direct methods and refined by full-matrix least-squares procedures to a final Rω of 0.058 for all 1209 reflexions with sin θ/λ ≤ 0.5377.Although second harmonic generation unambiguously established the correct space group as Pn21a, parameters reported here refer to the centrosymmetric space group Pnma. The geometry at phosphorus is approximately tetrahedral with an average P—C distance of 1.838(2) Å. Angles at phosphorus range from 105.4° to 113.2°. The P=S bond length of 1.966(2) Å is one of the longest bonds of this type so far reported. Rigid body analysis of thermal parameters suggests that the 'true' bond lengths are even longer.


2019 ◽  
Vol 43 (24) ◽  
pp. 9354-9363
Author(s):  
Peng Ren ◽  
Yun Yang ◽  
Hao Li ◽  
Zhihua Yang ◽  
Shilie Pan

KCa4B3O9 and K0.59Rb0.41Ca4B3O9 crystallize in the polar space group with moderate SHG responses. Calculations were performed to elucidate the structure–property relationships.


2006 ◽  
Vol 62 (4) ◽  
pp. o1647-o1649 ◽  
Author(s):  
William T. A. Harrison ◽  
H. S. Yathirajan ◽  
B. K. Sarojini ◽  
B. Narayana ◽  
J. Indira

The geometrical parameters for the title compound, C16H13ClO2, are normal. Packing in a non-centrosymmetric space group, which is consistent with the non-zero second harmonic generation response, may be influenced by a C—H...O interaction.


RSC Advances ◽  
2017 ◽  
Vol 7 (30) ◽  
pp. 18650-18657 ◽  
Author(s):  
Ji-Han Huang ◽  
Guang-Feng Hou ◽  
Dong-Sheng Ma ◽  
Ying-Hui Yu ◽  
Wen-Hong Jiang ◽  
...  

Two pairs of Zn-based chiral coordination polymers were synthesized under hydrothermal conditions, exhibiting medium second-harmonic generation (SHG) activities and luminescent behavior.


Crystals ◽  
2021 ◽  
Vol 11 (8) ◽  
pp. 921
Author(s):  
Ilhwan Kim ◽  
Donghwa Lee ◽  
Kwang Jo Lee

The mid-infrared (mid-IR) continuum generation based on broadband second harmonic generation (SHG) (or difference frequency generation) is of great interest in a wide range of applications such as free space communications, environmental monitoring, thermal imaging, high-sensitivity metrology, gas sensing, and molecular fingerprint spectroscopy. The second-order nonlinear optic (NLO) crystals have been spotlighted as a material platform for converting the wavelengths of existing lasers into the mid-IR spectral region or for realizing tunable lasers. In particular, the spectral coverage could be extended to ~19 µm with non-oxide NLO crystals. In this paper, we theoretically and numerically investigated the broadband SHG properties of non-oxide mid-IR crystals in three categories: chalcopyrite semiconductors, defect chalcopyrite, and orthorhombic ternary chalcogenides. The technique is based on group velocity matching between interacting waves in addition to birefringent phase matching. We will describe broadband SHG characteristics in terms of beam propagation directions, spectral positions of resonance, effective nonlinearities, spatial walk-offs between interacting beams, and spectral bandwidths. The results will show that the spectral bandwidths of the fundamental wave allowed for broadband SHG to reach several hundreds of nm. The corresponding SH spectral range spans from 1758.58 to 4737.18 nm in the non-oxide crystals considered in this study. Such broadband SHG using short pulse trains can potentially be applied to frequency up-conversion imaging in the mid-IR region, in information transmission, and in nonlinear optical signal processing.


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