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Pandi, S.
- Non-linear Optical Properties of α-glycine Single Crystals by Z-scan Technique
Abstract Views :474 |
PDF Views:129
Authors
Affiliations
1 Dept. of Physics, Aksheya Engineering College, Puludivakkam- 603 314, Kanchipuram Dt. Tamil Nadu, IN
2 Rajalakshmi Institute of Technology, Kunthampakkam-602 107, Kanchipuram Dt., Tamil Nadu, IN
3 Dept. of Physics, Presidency College, Chennai- 600 005, IN
1 Dept. of Physics, Aksheya Engineering College, Puludivakkam- 603 314, Kanchipuram Dt. Tamil Nadu, IN
2 Rajalakshmi Institute of Technology, Kunthampakkam-602 107, Kanchipuram Dt., Tamil Nadu, IN
3 Dept. of Physics, Presidency College, Chennai- 600 005, IN
Source
Indian Journal of Science and Technology, Vol 3, No 6 (2010), Pagination: 653-655Abstract
Single crystals of α-Glycine up to the size of 4 × 4 × 1 mm3 were grown for optical characterization by the solution growth method using methanol as a solvent. The crystal structure was studied by X-ray diffraction. The UV-visual absorption spectra indicate a good transparency between 200 and 1400 nm. The non-linear refractive index n2 and susceptibility χ (3) have been measured through the Z-scan technique. α-Glycine exhibits saturation absorption and self-focusing performance. Non-linear absorption co-efficient β is determined as 2.4763 x 10 -5 cm/W. Non-linear refractive index n2 measured at the wavelength of 632.8 nm is calculated as 2.14435 x 10-8 cm2/W. The real and imaginary pars of χ (3) have been measured at 632.8 nm and found to be 7.9732 x 10-07 esu and 8.0018 x 10-07 esu, respectively. The measured 3rd order non-linear properties confirm its suitability for non-linear optical devices such as optical switching device.Keywords
Single XRD, α-Glycine, UV Spectrum, Z-scan, Crystal GrowthReferences
- Fryad Z. Henari, Shane MacNamara, Orla Stevenson, Joesph Callagham, Declan Weldon, Werner J. Blau, (1993) Low power nonlinear optical response of C60 and C70 fullerene solutions Adv.Mater. 5, 930.-936.
- Gu G, Zhang W, Zen H, Du Y, Han Y, Dong F and Xia Y (1993) Large non-linear absorption in C60 thin films. J. Phys. B. 26, L451- L456.
- Gu G, Zhang W, Zen H, Du Y, Han Y, Dong F and Xia Y (1993) Large non-linear absorption in C60 thin films J. Phys. B 26 L451- L456.
- Henari FZ, MacNamara S, Stevenson O, Callagham J, Weldon D and Blau WJ (1993) Low power non-linear optical response of C60 and C70 fullerene solutions. Adv. Mater. 5, 930-936.
- Kurtz SK and Perry TT (1968) A powder technique for the evaluation of non-linear optical materials. J. Appl.Phys. 39, 3798-3812.
- Sheik–Bahe M, Said AA, Wei TH, Hagan DJ and Van Stryland EW (1990) Sensitive measurement of optical nonlinearities using a single IEEE. J. Quantum Electron. 26, 760-769.
- Wei TH, Hagan DJ, Sence MJ, Van Stryland EW, Perry JW and Coulter DR (1992) Direct measurements of non-linear absorption and refraction in solutions ofphthalocyanines. Appl. Phys. B. 54, 46-51.
- Yin M, Li HP, Tang SH and Ji W (2000) Determination of non-linear absortion and refraction by single Z-scan method. Appl. Phys. B. 70, 587-591.
- Zhao W and Palffy-Muhoray P (1994) Z-scan measurement of χ(3) using top- hat beams. Appl. Phys. Lett. 65, 673-675.
- Third Order Non-linear Optical Properties of Potassium Aluminium Sulphate Single Crystals by Z-scan Technique
Abstract Views :462 |
PDF Views:148
Authors
Affiliations
1 Department of Physics, Rajalakshmi Institute of Technology, Kuthampakkam – 602 107, Chennai, IN
2 Department of Physics Aksheyaa College of Engineering, Puludivakkam – 603 314, Kanchipuram Dt., IN
3 Head Department of Physics, Presidency College, Chennai – 600 005, IN
1 Department of Physics, Rajalakshmi Institute of Technology, Kuthampakkam – 602 107, Chennai, IN
2 Department of Physics Aksheyaa College of Engineering, Puludivakkam – 603 314, Kanchipuram Dt., IN
3 Head Department of Physics, Presidency College, Chennai – 600 005, IN
Source
Indian Journal of Science and Technology, Vol 3, No 6 (2010), Pagination: 656-658Abstract
Potassium aluminum sulphate dodeca hydrate crystals were grown from aqueous solution and studied by X-ray diffraction. The UV-Visual IR transmission spectra indicate a better transparency between 200 and 800 nm. The nonlinear refractive index n2 and susceptibility χ(3) have been measured through the Z-scan technique. The results indicate that the compound exhibits saturation absorption and self-focusing performance. Non-linear absorption Co-efficient β is determined as 7.6746 x 10 -4 cm/W. Non-linear refractive index n2 measured at the wavelength of 632.8 nm is calculated as 1.46412 x 10-8 cm2/W. The real and imaginary pars of χ(3) have been measured at 632.8 nm and found to be 7.84088 x 10-07 esu and 2.07218 x 10-08 esu, respectively. The measured 3rd order non-linear properties confirm its suitability for nonlinear optical devices such as optical limiting and switching.Keywords
Growth from Solution, Single XRD, UV Spectrum, Z-scanReferences
- Fryad Z. Henari, Shane MacNamara, Orla Stevenson, Joesph Callagham, Declan Weldon and Werner J. Blau (1993) Low power nonlinear optical response of C60 and C70 fullerene solutions. Adv.Mater. 5, 930-936.
- Krauss TD and Wise FW (1994) Femtosecond measurement of nonlinear absorption and refraction in CdS, ZnSe, and ZnS. Appl. Phys. Lett. 65 1739-1741.
- Kurtz SK and Perry TT (1968) A powder technique for the evaluation of nonlinear optical materials. J. Appl. Phys. 39, 3798-3812.
- Lee W. Tutt and Thomas F. Boggess (1993) A review of optical limiting mechanisms and devices using organics, fullerenes, semiconductors and other materials. Prog. Quant. Elecr. 17, 299-306.
- Li L, Yuan HJ, Hu GH and Palffy-Muthoray P (1994) A new configurational transition in inhomogeneous nematics. Liq. Cryst. 16, 703-712.
- Ma Ma H. Gomes ASL and de Araujo GB (1992) Infrared nonlinearity of commercial Cd (S, Se) glasscomposites. Opt. Commun. 87, 19-22.
- Paparo D, Maddalena P, Abbade G, Santamato E and Jannossy (1994) Wavelength Dependence of Optical Reorientation in Dye-Doped Nematics Mol. Cryst. Liq. Cryst. 251 73-84.
- Rangel-Rojo R, Kosa T, Hajito E, Ewen PJS, Owen AE, Kar AK and Whereett BS (1994) Near-infrared optical nonlinearities in amorphous chalcogenides. Opt. Commun. 109, 145-150.
- Sheik–Bahe M, Said AA, Wei TH, Hagan DJ and Van Stryland EW (1990) Sensitive measurement of optical nonlinearities using a single. IEEE J. Quantum Electron. 26, 760-769.
- Sheik-Bahe M, Wang J and Van Stryland EW (1994) Non-degenerate optical Kerr effect in semiconductors IEEE J. Quantum Electron. 30, 249-255
- Sivanesan T, Natarajan V and Pandi S (2010) Nonlinear optical properties of α-glycine single crystals by Z-Scan technique. Indian J.Sci.Technol. 3 (6), this issue. Domain name: http://www.indjst.org.
- Wei TH , Hagan DJ, Sence MJ, Van Stryland EW, Perry JW and Coulter DR (1992) Direct measurements of nonlinear absorption and refraction in solutions of phthalocyanines, Appl. Phys. B 54, 46-51.
- Yin M, Li HP, Tang SH and Ji W (2000) Determination of nonlinear absorption and refraction by single Zscan method. Appl. Phys. B 70, 587-591.
- Zhao W and Palffy-Muhoray P (1993) Z-scan technique using top-hat beams. Appl. Phys. Lett. 63, 1613-1615.
- Zhao W and Palffy-Muhoray P (1994) Z- scan measurement of χ(3) using top- hat beams. Appl. Phys. Lett. 65, 673-675.
- Synthesis, Growth, Optical and Thermal Properties of a New Organic Crystal Semicarbazone of P-anisaldehyde (SPAS)
Abstract Views :493 |
PDF Views:166
Authors
Affiliations
1 Department of Physics, Presidency College, Chennai-600 005, Tamilnadu, IN
2 Department of Materials Science and Engineering, National Chiauo Tung University, TW
3 Department of Physics, St. Xavier’s College, Polyamkottai, Tirnelveli, Tamilnadu, IN
1 Department of Physics, Presidency College, Chennai-600 005, Tamilnadu, IN
2 Department of Materials Science and Engineering, National Chiauo Tung University, TW
3 Department of Physics, St. Xavier’s College, Polyamkottai, Tirnelveli, Tamilnadu, IN
Source
Indian Journal of Science and Technology, Vol 3, No 8 (2010), Pagination: 885-889Abstract
The semicarbazone of p-anisaldehyde (SPAS) is a novel organic nonlinear optical material. The SPAS has been synthesized and the solubility studies were carried out in the temperature range 30-60 °C. Single crystals of SPAS have been grown following the slow evaporation technique and the unit cell parameters have been evaluated by single crystal X-ray diffraction technique. The UV-Visible, FT-IR and 1HNMR spectra have been recorded to characterize the grown crystal. The thermogravimetric and differential thermal analysis of the grown crystal revealed that there is no phase transformation in SPAS, and its thermal stability was found to be good. The dielectric measurement was made as a function of frequency (50 Hz - 5 MHz). The second harmonic generation in the sample was confirmed by the Kurtz powder technique.Keywords
Crystal Growth, XRD, Solution Growth, Thermal Studies, Dielectric StudiesReferences
- Boomadevi S and Dhanasekaran RD (2004) Synthesis, crystal growth and characterization of L-pyrrolidone-2-carboxylic acid (L-PCA) crystals. J. Cryst. Growth. 261,70-76.
- Bruice PY (2002) Organic chemistry, Pearson education (Singapore) Pte. Ltd., first Indian reprint, Delhi. 534–565.
- Chemla DS and Zyss J (1988) Non-linear optical properties of organic molecule and crystals. 1 & 2, Academic Press, NY.
- Elmali A, Karaka A and Unver H (2005) Non-linear optical properties of bis[(p-bromophenylsalicylaldiminato) chloro] iron(III) and its ligand N-(4-bromo)-salicylaldimine. Chem. Phys. 309, 251.
- Frazier CC, Cockerham MP, Chauchard EA and Lee CH (1987) Second-harmonic generation in aromatic organic compounds. J. Opt. Soc. Am. B. 4, 1899-1903.
- Kanis DR, Ratner MA and Marks TJ (1994) Design and construction of molecular assemblies with large second-order optical nonlinearities. Quantum chemical aspects. Chem. Rev. 94, 195-242
- Karakas A, Elmali A, Unver H, Kara H and Yahsi Y (2006a) Synthesis, structure, spectroscopic studies and ab-initio calculations on first hyperpolarizabilities of N,N’-Bis(2-hydroxy-1-naphthylmethylidene)-1- methyl-1,2-diaminoethane-N,N’,O,O’-copper(II).Z. Naturforsch. 61b, 968-974.
- Karakas A, Unver H and Elamli A (2006b) Static and dynamic second hyperpolarizabilities of [FeL(MeOH)Cl]2 (L = N-(5-methylphenyl)-3- methoxysalicylaldimine). J. Mol. Struct. (Theochem.). 774, 67-70.
- Keinan S, Ratner MA and Marks TJ (2004) Selfassembled electrooptic superlattices. A theoretical study of multilayer formation and response using donor−acceptor, hydrogen-bond building blocks. Chem. Mater. 16, 1848-1854.
- Kurtz SK and Perry TT (1968) A powder technique for the evaluation of non-linear optical materials. J. Appl. Phys. 39, 3798-3813.
- Prasad NV, Prasad G, Bhimasankaram T, Suryanarayana S V and Kumar GS (1996) Dielectric properties of cobalt doped cadmium oxalate crystals. Bull. Mater. Sci. 19, 639-643.
- Prasad PN and Williams DJ (1991) Introduction to non-linear optical effects in molecules and polymers, Wiley, NY. 1003-1008.
- Ramesh Babu R, Vijayan N, Gopalakrishnan R and Ramasamy P (2002) Growth and characterization of benzaldehyde semicarbazone (BSC) single crystals. J. Cryst. Growth. 240, 545-548.
- Vijayan N, Ramesh Babu R, Gopalakrishnan R, Dhanuskodi S and Ramasamy P (2001) Growth and characterization of organic crystals of semicarbazone of acetophenone. J. Cryst. Growth. 233, 863-867.
- Third Order Non-linear Optical Properties of L-arginine Hydrochloride Monohydrate Single Crystals by Z-scan Technique
Abstract Views :551 |
PDF Views:139
Authors
Affiliations
1 Dept. of Physics, Rajalakshmi Institute of Technology, Kunthampakkam-602124, TN, IN
2 Dept. of Physics, Aksheyaa College of Engineering, Puluthivakkam, Kanchipuram 603 314, TN, IN
3 Dept. of Physics, Presidency College, Chennai- 600 005, IN
1 Dept. of Physics, Rajalakshmi Institute of Technology, Kunthampakkam-602124, TN, IN
2 Dept. of Physics, Aksheyaa College of Engineering, Puluthivakkam, Kanchipuram 603 314, TN, IN
3 Dept. of Physics, Presidency College, Chennai- 600 005, IN
Source
Indian Journal of Science and Technology, Vol 3, No 8 (2010), Pagination: 897-899Abstract
L-arginine hydrochloride monohydrate (L-arginine hydrochloride monohydrate) was synthesized by the reaction between hydrochloric acid and the strongly basic amino acid, L-arginine taken in the ratio of 1:1. The crystal structure of the sample was studied by single X-ray diffraction. The UV transmittance spectra of the grown crystals indicate a good transparency between 200 and 1000 nm. The nonlinear refractive index η2 and susceptibility χ(3) have been measured through the Z-scan technique. The results indicate that the compound exhibits reverse saturation absorption and selfdefocusing performance. Non-linear absorption co-efficient is determined as 9.2194 x 10- 4 cm/w. The non-linear refractive index of the L-arginine hydrochloride single crystals were found to be 1.7129 x 10- 7cm 2/w. The real and imaginary pars of non-linear susceptibility χ(3) have been measured at 632.8 nm and found to be 1.1573 x 10-05 esu and 3.1382 x 10-05 esu, respectively.Keywords
Growth from Solution, Single XRD, UV Spectrum, Z-scanReferences
- Fryad Z Henari, Shane MacNamara, Stevenson O, Callagham J, Weldon D and Blau WJ (1993) Low power nonlinear optical response of C60 and C70 fullerene solutions. Adv. Mater. 5, 930-936.
- Gomes MH and De Araujo GB (1992) Infrared non-linearity of commercial Cd(S, Se) glass composites. Opt. Commun. 87, 19-22.
- Kalaiselvi D, Mohan Kumar R and Jayavel R (2008) Single crystal growth and properties of semi-organic nonlinear optical L-arginine hydrochloride monohydrate crystals. Cryst. Res. Technol. 43(8), 851–856.
- Kurtz SK and Perry TT (1968) A powder technique for the evaluation of non-linear optical materials. J. Appl. Phys. 39, 3798-3812.
- Lee W Tutt and Boggess TF(1993) A review of optical limiting mechanisms and devices using organics, fullerenes, semiconductors and other materials. Prog. Quant. Elecr. 17, 299-306.
- Li L, Yuan HJ, Hu GH and Palffy- Muthoray P (1994) A new configurational transition in inhomogeneous nematics. Liq. Cryst. 16, 703-712.
- Meera K, Muralidharan R, Dhanasekaran R, Manyum P and Ramasamy P (2004) Growth of non-linear optical material: Larginine hydrochloride and its characterization. J. Crystal Growth. 263, 510–516.
- Monaco SB, Davis LE, Velso SP, Wang FT, Eimerl D and Zalkin A (1987) Synthesis and characterization of chemical analogs of L-arginine phosphate. J. Crystal Growth. 85, 252- 257.
- Natarajan V, Sivanesan T and Pandi S (2010) Third order nonlinear optical properties of potassium aluminium sulphate single crystals by Z-Scan technique. Indian J.Sci.Technol. 3 (6), 656-658.
- Paparo D, Maddalena P, Abbade G, Santamato E and Jannossy (1994) Wavelength dependence of optical reorientation in dye-doped nematics. Mol. Cryst. Liq. Cryst. 251, 73-84.
- Rangel-Rojo R, Kosa T, Hajito E, Ewen PJS, Owen AE, Kar AK and Whereett BS (1994) Near-infrared optical non-linearities in amorphous chalcogenides. Opt. Commun. 109, 145-150.
- Sivanesan T, Natarajan V and Pandi S (2010) Non-linear optical properties of a-glycine single crystals by Z-Scan technique. Indian J.Sci.Technol. 3 (6), 653-655.
- Tod D Krauss and Wise FW (1994)Femto-second measurement of non-linear absorption and refraction in CdS, ZnSe, and ZnS. Appl. Phys. Lett. 65, 1739-1741.
- Wei TH, Hagan DJ and Sence MJ, Van Stryland EW, Perry JW and Coulter DR (1992) Direct measurements of non-linear absorption and refraction in solutions of phthalocyanines. Appl. Phys. B. 54, 46-51.
- Yin M, Li HP, Tang SH and Ji W (2000) Determination of non-linear absorption and refraction by single Z-scan method. Appl. Phys. B. 70, 587-591.
- Zhang W, Zen H, Du Y, Han Y, Dong F and Xia Y (1993) Large non-linear absorption in C60 thin films. J. Phys. B. 26, L451-L456.
- Zhao W and Palffy-Muhoray P (1993) Z-scan technique using top-hat beams. Appl. Phys. Lett. 63, 1613-1615.