Paper Menu >>
Journal Menu >>
Journal of Minerals & Materials Characterization & Engineering, Vol. 9, No.5, pp.495-507, 2010
jmmce.org Printed in the USA. All rights reserved
Synthesis, Crystal Growth, Structural, Optical, Thermal and
Mechanical Properties of Semiorganic Nonlinear Optical Material:
T. Uma Devia*, N. Lawrenceb, R. Rameshbabuc, S. Selvanayagamd , Helen Stoeckli-Evanse,
G. Bhagavannarayanaf, K. Ramamurthic
aDepartment of Physics, Government Arts College for Women, Pudukkottai –622001, India.
bDepartment of Physics, St.Joseph’s College, Tiruchirappalli –620002, India.
cSchool of Physics, Bharathidasan University, Tiruchirappalli –620024, India.
dDepartment of Physics, Kalasalingam University, Krishnan Koil - 626 190
eInstitute of Physics, University of Neuchâtel, Neuchâtel, India
fMaterials Characterization Division, National Physical Laboratory, New Delhi-110 012, India
*Corresponding author: email@example.com
L-Cystine dihydrochloride, a semiorganic nonlinear optical material, was synthesized and a
single crystal was grown from aqueous solution. Low temperature (173 K) crystal structure
measurement was carried out, and it reveals that the crystal belongs to noncentro symmetric
space group C2. The structural perfection of the grown crystal was analyzed by high-resolution
X-ray diffraction (HRXRD) rocking curve measurements. Fourier transform infrared (FTIR)
spectroscopic studies were also performed for the identification of different vibrational modes of
the fundamental groups present in the compound. The UV–vis transmission spectrum was
recorded in the range 200–1000 nm. The second harmonic conversion efficiency was determined
using the Kurtz powder technique; which is 0.35 times that of KDP. Thermal properties of L-
Cystine Dihydrochloride were studied by TGA and DTA.
Keywords: crystal st ructure, amino-acid, coordination compounds, thermal properties
Extensive studies have been made on the synthesis and crystal growth of nonlinear optical
(NLO) materials over the past decade because of their potential applications in the field of
496 T. Uma Devi, et al Vol.9, No.5
telecommunications, optical signal processing and optical switching 1,2. These applications
depend upon the various properties of the materials, such as transparency, birefringence,
refractive index, dielectric constant, thermal, photochemical and chemical stability. Organic
crystals have large nonlinear susceptibilities compared to inorganic crystals. However these
crystals have certain limitations such as increased optical absorption, narrow transparency
window and poor mechanical and thermal stability. Inorganic crystals have excellent mechanical
and thermal properties but possess relatively low optical nonlinearities because of the lack of -
electron delocalization. Combining the high optical nonlinearity and chemical flexibility of
organics with thermal stability and excellent transmittance of inorganics, semiorganic materials
have been proposed and are attracting a great deal of attention in the field of nonlinear optics 3,4.
Complexes of amino acids with inorganic salts are promising materials for optical second
harmonic generation (SHG), as they aptly fit in this context with such properties. Amino acids
are interesting materials for NLO application as they contain a proton donor carboxyl acid (-
COO) group and the proton acceptor amino (-NH2) group in them. A series of semi-organic
compounds such as l-histidinium hydrogen malate 5, L-arginine diphosphate6, L-Lysine
monohydrochloride dihydrate7, L-histidine hydrochloride monohydrate8 and L-glutamic acid
hydrochloride9 have been reported with moderately high mechanical and chemical stability. Our
laboratory is engaged in finding new materials for NLO applications and some of these were
reported recently 10-13.
L-cystine dihydrochloride (C6H12S2N2O4.2HCl) is yet another semiorganic nonlinear optical
material. L-Cystine is a sulfur containing amino acid. The chirality of L-cystine enforces non-
centrosymmetry of crystal structures of its compounds. This is an important aspect in addition to
chemical and conformational flexibility for the search for new non-centrosymmetrical materials
with certain desired physical properties, such as in the field of non-linear optics 3. In this paper,
we report for the first time on the growth of bulk crystal of L-cystine dihydrochloride
(LCDHCL) using temperature reduction method and its characterization by single crystal x-ray
diffraction (XRD), High resolution X-ray diffraction (HRXRD), Fourier Transform infrared
spectroscopy (FTIR), UV-Vis-NIR, thermal and microhardness studies.
2. EXPERIMENTAL PROCEDURE
The LCDHCL was synthesized by dissolving 1M of L-cystine in 2 M of hydrochloric acid in
double distilled water at 50 °C. The fully reacted solution was filtered and crystalline salt was
obtained by evaporation of filtered solution. The crystalline salt formed was further purified by
re-crystallization process in double distilled water. Solubility of LCDHCL in double distilled
water was determined in the temperature range of 30-55 °C.
From the knowledge of these data, saturated solution of LCDHCL was prepared at 35 °C from
recrystallized salt and this solution was filtered with microfilters and placed in a constant
Vol.9, No.5 Synthesis, Crystal Growth, Structural, Optical 497
temperature bath having an accuracy of ± 0.01 °C. One of the better quality crystals obtained
from slow evaporation of the solution at room temperature was used as the seed crystal. Single
crystal of LCDHCL was grown by the slow cooling method by reducing the temperature from 35
°C at the rate of 0.1 °C per day. Well-developed crystal of size 20×6×5 mm3, harvested in a
growth period of 10 days, is shown in Figure 1.
Figure 1. As grown crystal of LCDHCL.
3. RESULTS AND DISCUSSION
3.1. X-ray Diffraction
Data set was obtained using a Stoe Image Plate Diffraction System using Mo K graphite
monochromated radiation at 173 K using phi & omega scans method. The structure was solved
by Direct methods using the programme SHELXS97 and refined by full-matrix least squares
method using SHELXL97. The R-values of the full-matrix least squares refinement is given in
Table 1. The H-atoms could all be located in Fourier difference maps. The water H-atoms were
freely refined, while the remainder of the H-atoms were included in calculated positions and
treated as riding atoms using SHELXL default parameters. CCDC 653578 contains the
supplementary crystallographic data for the title compound. These data can be obtained from free
of charge from the Cambridge Crystallographic Data Centre via the website of
498 T. Uma Devi, et al Vol.9, No.5
The X-ray study confirmed the molecular structure and atomic connectivity for the title
compound as illustrated in Figure 2a. In the title compound the molecule resides on a
crystallographic twofold axis, which runs through the central S-S bond. The bond distance S1-
S1i of 2.040 (1) Å [symmetry code: (i) 1-x, y, 1-z] confirms the S-S single bond character. The
geometry of the cystine residues are comparable to the related literature values. Both half
molecule adopts R configuration with the atoms C2*/N1/C1/C3/H2. The molecular structure is
stabilized by strong intramolecular N-H…Cl hydrogen bond involving atoms N1-H1C…Cl1.
The crystal packing is stabilized by strong intermolecular N-H…Cl and O-H…Cl hydrogen
bonds. The Chlorine atom act as a trifurcated acceptor atom for two intermolecular and one
intramolecular hydrogen bonds involving with all the three hydrogen atoms attached to N1. Two
of these hydrogen bonds run along ‘bc’ plane and one run along ‘ac’ plane (Figure 2b). The acid
group hydrogen atom involves O2-H2O…Cl1 intermolecular hydrogen bond in the equivalent
position of x,y-1,1+z The molecules are further stabilized by weak two C-H…O intermolecular
interaction involving atoms C2-H2…O1.
Figure 2a. ORTEP of LCDHCL showing 50% probability ellipsoids and the labeling scheme.
Vol.9, No.5 Synthesis, Crystal Growth, Structural, Optical 499
Figure 2b. A view along the b axis of the crystal packing of LCDHCL.
Table 1. Single-Crystal X-ray Data of LCDHCL Crystal.
CCDC No. CCDC 653578
Formula C6 H14 Cl2 N2 O4 S2
Formula weight 313.23
Crystal System Monoclinic
Space group C2
a (Å) 18.4405(14)
b (Å) 5.2166(6)
c (Å) 7.2191(6)
V (Å3) 673.62(11)
Flack parameter -0.03(5)
500 T. Uma Devi, et al Vol.9, No.5
The freshly ground powder sample of LCDHCL was subjected to powder X-ray diffraction
analysis with a monochromated CuK radiation (=1.5406 Å). The powder XRD patterns are
indexed and shown in Figure 3.
Figure 3. Powder X-ray diffraction of LCDHCL.
Figure 4 shows the high-resolution X-ray diffraction curve (DC) recorded for a typical LCDHCL
single crystal specimen using (400) diffracting planes in symmetrical Bragg geometry by
employing the multicrystal X-ray diffractometer with MoK1 radiation. The solid line
(convoluted curve) is well fitted with the experimental points represented by the filled rectangles.
On deconvolution of the diffraction curve, it is clear that the curve contains an additional peak,
which is 57 arc s away from the main peak. This additional peak depicts an internal structural
very low angle (tilt angle 1 arc min) boundary14 whose tilt angle (misorientation angle between
the two crystalline regions on both sides of the structural grain boundary) is 59 arc s from its
adjoining region. The FWHM (full width at half maximum) of the main peak and the very low
angle boundary are respectively 52 and 46 arc s. Though the specimen contain a very low angle
boundary, the relatively low angular spread of around 300 arc s of the diffraction curve and the
low FWHM values show that the crystalline perfection is reasonably good. Thermal fluctuations
or mechanical disturbances during the growth process could be responsible for the observed very
low angle boundary.
Vol.9, No.5 Synthesis, Crystal Growth, Structural, Optical 501
Figure 4. High-resolution diffraction curve of LCDHCL.
3.2 Fourier Transform Infrared Spe ct ru m
The Fourier Transform Infrared (FTIR) spectrum of LCDHCL (Figure 5) was recorded at room
temperature in the spectral range 400 - 4000 cm-1 by KBr pellet method using the Perkin Elmer
grating Infrared spectrophotometer. The peak at 1730 cm-1 is characteristic of α-amino acid
hydrochlorides10. Presence of the functional groups of L-cystine, were identified and the
vibrational frequencies are compared in Table 2 with the corresponding frequencies of the parent
reactant of L-cystine. From Table 2 one can observe that the vibrational frequencies except CH2
wagging and C-C deformation are not modified appreciably in the LCDHCL crystal.
502 T. Uma Devi, et al Vol.9, No.5
Figure 5. FTIR spectrum of LCDHCL.
Table 2. Band assignment of FTIR spectrum of LCDHCL
Wave number (cm-1) assignments
L-cystine  LCDHCL
3429 3413 NH asymmetric stretching
3030 3020 CH broad band stretching
2096 2083 NH3+ stretching
1585 1570 NH3+deformation
1489 1503 COO– stretching
1408 1428 CH2-CO deformation
Vol.9, No.5 Synthesis, Crystal Growth, Structural, Optical 503
1342 1347 C-C stretching
1298 1221 CH2 wagging
1194 1188 C-C stretching
1126 1130 C-C stretching
1090 1082 C-C stretching
1043 1046 C-N stretching
611 582 COO- rocking
540 505 C-C deformation
3.3. Optical Transmission Spectrum
Optically transparent single crystal of thickness 2 mm was used to record the optical
transmittance spectrum by employing Varian Cary 5E UV – Vis – NIR spectrophotometer in the
range 200 and 1000 nm (Figure 6).Transmittance is about 70 % in the range of 400-1000 nm and
the lower cutoff is at 300 nm. Hence the LCDHCL crystal can be used as a potential material
for frequency doubling.
Figure 6. UV-Vis spectrum of LCDHCL.
504 T. Uma Devi, et al Vol.9, No.5
3.4. Microhardness Studies
Vicker’s microhardness values were estimated by employing REICHERT MD 4000E ULTRA
microhardness tester for different loads on the polished face of LCDHCL. Vickers
microhardness number (Hv) was calculated using the relation, Hv = 1.8544 (P/d 2) kg/mm2, where
P is the indenter load in kg and d is the diagonal length of the impression in mm. Figure 7 shows
the variation of Vickers hardness values with load. The hardness value increases up to a load of
100 g and decreases for 200 g. Cracks develop around the indentation mark above the load of
200 g. The work hardening coefficient n was calculated from Meyer’s law17. The n value
calculated by plotting log P against log d for LCDHCL crystal on (001) plane is 2. Onitsch18
inferred that a value of n lies between 1 and 1.6 for hard materials and for soft materials it is
above 1.6. Therefore calculated value of n=2 shows that LCDHCL is a soft material.
Figure 7. Variation of microhardness values with applied load
3.5. Thermal Studies
Thermogravimetric analysis of the LCDHCL crystal was carried out employing Perkin Elmer,
US, TGA7 Analyzer between 50 and 900 o C in the nitrogen atmosphere at a heating rate of 10 o
C / min (Figure 8). A small piece of crystal weighing 1.6420 mg was used for this investigation.
From the TG–DTA curves it is inferred that the melting of the material takes place in the vicinity
of 235˚C. The sharpness of this endothermic peak shows the good degree of crystallinity and
purity of the sample 19, 20. Further, it indicates no phase transition before this temperature. There
is a gradual and significant weight-loss as the temperature is increased above the melting point.
Sudden decomposition took place between 235 ˚C and 333 ˚C with a weight loss of 78 % due to
the expulsion of molecules of, SO2, NH3 and CO2 from the chain and the residual weight
obtained at 800 °C is only 2.42 %.
Vol.9, No.5 Synthesis, Crystal Growth, Structural, Optical 505
Figure 8. TG/DTA of LCDHCL.
3.6. NLO Studies
Kurtz 21 second harmonic generation (SHG) test was performed to find the NLO property of
LCDHCL crystal. The powdered crystalline sample was illuminated using Spectra Physics
Quanta Ray DHS-2. Nd: YAG laser using the first harmonics output of 1064 nm with pulse
width of 8 ns and repetition rate of 10 Hz. The green radiation of 532 nm was collected by a
photomultiplier tube (PMT- Philips Photonics - model 8563) after being monochromated
(monochromator - model Triax – 550). The optical signal incident on the PMT was converted
into voltage output at the CRO (Tektronix- TDS 3052B). The input laser energy incident on the
powdered sample was chosen to be 5.6 mJ. The result obtained shows that the powder SHG
relative efficiency of LCDHCL is about 0.34 times that of potassium dihydrogen orthophosphate
(KDP). As the second order nonlinear efficiency will vary with the particle size of the powder
sample, higher efficiencies are expected to be achieved by optimizing the phase matching 22.
Single crystals of L-cystine dihydrochloride, a semiorganic NLO material of the amino-carboxyl
acid family was grown using temperature reduction technique. Single crystal X-ray diffraction
study shows that LCDHCL crystallizes in a monoclinic system. A multicrystal X-ray
diffractometer study reveals that the crystalline perfection of the grown crystal is reasonably
506 T. Uma Devi, et al Vol.9, No.5
good. The presence of functional groups such as N–H, COO_, C–C, C–H and C–S were
identified. Optical transmission study shows that LCDHCL is transparent in the entire visible and
in NIR region. Microhardness measurements imply that the LCDHCL comes under the soft
materials category. TGA reveals that the sample is thermally stable and has relatively higher
melting point. Furthermore, its nonlinear property was investigated by the Kurtz and Perry
technique and the second harmonic conversion relative efficiency of powder LCDHCL is about
0.34 times that of KDP.
One of the authors (T. U.) acknowledges Cauvery College for Women (Reddy Educational
Trust) for providing lab facilities to carry out the research work. The authors acknowledge Prof.
P. K. Das, Department of Inorganic and Physical Chemistry, Indian Institute of Science,
Bangalore for extending the laser facilities for the SHG measurement.
 P.N. Prasad and D.J. Williams. Introduction to Nonlinear Optical Effects on Molecules
and Polymers, Wiley, New York (1991)
 D.S. Chemla and J. Zyss. In: Nonlinear Optical Properties of Organic Molecules and
Crystals Vols. 1 and 2, Academic Press, Orlando (1987).
 M. Fleck, P. Becker, L. Bayarjargal, R. Ochrombel, L.Bohatý, Cryst. Res. Technol. 2008,
 V. Siva shankar, R. Siddheswaran, T. Bharthasarathi, P. Murugakoothan,J.Cryst. Growth
2009, 311, 2709-2713
 E. de Matos Gomes, V.H. Rodrigues, M.M.R. Costa, M.S. Belsley, P.J.M. Cardoso, C.F.
Gonçalves, F. Proença, J. Solid State Chem. 2006, 179, 2521-2528
 R. Ittychan , P. Sagayaraj, J. Cryst.Growth 2002 ,243, 356 -360.
 R.Ramesh Babu, N.Vijayan, R.Gopalakrishnan, P. Ramasamy ,Cryst. Res. Technol.
2006, 41, 405 – 410.
 J. Madhavan, S. Aruna, P. C. Thomas, M. Vimalan, S. A. Rajasekar, and P. Sagayaraj,
Cryst.Res. Technol. 2007, 42, 59 – 64.
 R. Sathyalakshmi, V. Kannan, R. Bairava Ganesh, and P. Ramasamy Cryst. Res. Technol.
2007, 42, 78-83.
 T. Uma Devi , N. Lawrence, R. Ramesh Babu, K. Ramamurthi J. Cryst. Growth 2008,
 T. Uma Devi , N. Lawrence, R. Ramesh Babu, K. Ramamurthi Spectrochim. Acta A
2008, 71, 340-343
Vol.9, No.5 Synthesis, Crystal Growth, Structural, Optical 507
 T. Uma Devi , N. Lawrence, R. Ramesh Babu, S. Selvanayagam, Helen Stoeckli-Evans,
K. Ramamurthi Cryst. Growth Des. 2009, 9, 1370 –1374.
 T. Uma Devi , N. Lawrence, R. Ramesh Babu, K. Ramamurthi Mat. Res. India, 2008,5,
 G. Bhagavannarayana, R.V. Ananthamurthy, G.C.Budakoti, B. Kumar, K.S. Bartwal,
J. Appl. Cryst. 2005, 38, 768 -771.
 E. Ramachandran, S. Natarajan, Cryst. Res. Technol. 2004, 39, 308-312.
 K.Biemann, Tables of Spectral Data for Structure Determination of Organic Compounds,
Springer Verlag, Berlin Heidelberg, 1989.
 H. Li, R.C. Bradt, J. Hard Mater. 1992, 3, 403-419.
 E.M.Onitsch, Mikroskopie 1947, 2, 131 -151.
 N. Vijayan, R. Ramesh Babu, M. Gunasekaraan , R. Gopalakrishnan, R. Kumaresan,
P. Ramasamy, C. W. Lan, J. Cryst. Growth 2003, 249, 309-315.
 A.S.H. Hameed, G. Ravi, R. Dhanasekaran, P. Ramasamy, J. Crystal Growth 2000, 212,
 S.K. Kurz, T.T. Perry, J. Appl. Phys. 1968, 39, 3798 –813.
 H.J. Ravindra, M.R. Suresh Kumar, C. Rai, S.M. Dharmaprakash, J. Cryst. Growth 2006,