Abstract
Poly(μ 2-l-alanine-μ 3-sodium nitrate (I)), p-LASN, crystals have been grown by slow evaporation at room temperature. The nominal size of the crystals obtained by the method was of 500 nm. The UV-Vis spectrum shows a wide range, where absorption is lacking around 532 nm, which is required in order to have the second harmonic emission, when an incident radiation of 1064 nm strikes on the crystal. This guarantees the possible use of the crystal in visible light applications. The transparent nature of the crystal in the visible and infrared regions within the transmission spectrum confirms the nonlinear optical properties of the crystal. Additionally, Fourier transform infrared spectroscopy displays its functional groups which correspond to the poly(μ 2-l-alanine-μ 3-sodium nitrate (I)), where the presence of nitrates in the lattice generally can be identified by their characteristic signature within the 1660–1625, 1300–1255, 870–833 and 763–690 cm−1 range. Single crystal diffraction was carried out in order to determine atomic structure and lattice parameter. Structural parameters were a = 5.388(9) Å, b = 9.315(15) Å and c = 13.63(2) Å. The structure of poly(μ 2-l-alanine-μ 3-sodium nitrate (I)) shown by single crystal diffraction shows an asymmetric unit consisting of one sodium and one nitrate ion and one l-alanine molecule. The coordination geometry around the sodium atom was trigonal bipyramidal, with three bidentate nitrate anions coordinating through their oxygen atoms and two l-alanine molecules, each coordinating through one carboxyl oxygen atom. Electronic structure was obtained by using the Becke-Lee-Yang-Part and Hartree-Fock approximations with hybrid exchange-correlation three-parameter functional and G-311**G(dp) basis set. Theoretical and experimental results were compared and discussed as having an excellent agreement among them.
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Ambujam K, Selvakumar S, Prem A D, Mohamed G and Sagayaraj P 2006 Cryst. Res. Tech. 41 671
Bernal J D Z. Kristallogr. 78 363
Hernández-Paredes J, Glossman-Mitnik D, Esparza-Ponce H E, Alváres-Ramos M E and Duarte-Moller A 2008 J. Mol. Struct. 875 295
Kristof V H, Els C, Tatjana Parac-Vogt N, Christiane G W and Luc Van M 2007 Acta Cryst. E63 m2354
Lydia Caroline M, Sankar R, Indirani R M and Vasudevan S 2009 Mater. Chem. Phys. 114 490
Meera K, Muralidharan R, Dhanasekaran R, Prapun M and Ramasamy P 2004 J. Cryst. Growth 263 510
Mohankumar R, Rajanbabu D, Jayaraman D, Jayavel R and Kitamura K 2005 J. Cryst. Growth 275 1935
Narayan Bhat M and Dharmaprakash S 2002 J. Cryst. Growth 236 376
Ostroverkhov V, Ostroverkhova O, Petschek R G, Singer K D, Sukhomlinova L, Twieg R J, Wang S-X and Chien L C 2000 Chem. Phys. 257 263
Ramesh Kumar G, Gokul Raj S, Mohan R and Jeyavel R 2006 Cryst. Growth Des. 6 1308
Razzetti C, Ardoino M, Zanotti L, Zha M and Paorici C 2002 Cryst. Res. Technol. 37 456
Rodrigues J, Misoguti L, Nunes F D, Mendonca C R and Zilo S C 2003 Opt. Mater. 22 235
Sethuraman K, Ramesh Babu R, Gopalakrishnan R and Ramasamy P 2008 Cryst. Growth Des. 8 1863
Simpson H J Jr and Marsh R E 1966 Acta Cryst. 8 550
Vijayan N, Rajasekaran S, Bhagavannarayana G, Ramesh Babu R, Gopalakrishnan R, Palanichamy M and Ramasamy P 2006 Cryst. Growth Des. 6 2441
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Duarte Moller, A. Electronic structure and first hyperpolarizability of poly(μ 2-l-alanine-μ 3-sodium nitrate (I)) crystals. Bull Mater Sci 37, 1471–1476 (2014). https://doi.org/10.1007/s12034-014-0098-y
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DOI: https://doi.org/10.1007/s12034-014-0098-y