Growth and Characterization of L-Alanine Doped TGS Crystal

DOI : 10.17577/IJERTV3IS060067

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Growth and Characterization of L-Alanine Doped TGS Crystal

P. R. Deepthi1*, and J. Shanthi2

1Department of Physics, The Oxford College of Engineering, Bangalore, Karnataka, India-560068

2Department Of Physics, Avinashilingam University for Women, Coimbatore, Tamilnadu, India- 641038

Abstract – AbstractTriglycine sulphate (TGS), an important ferroelectric material has been widely used in the fabrication of high sensitivity infrared detectors at room temperature. Single crystals of L-Alanine doped TGS was grown by slow evaporation method at room temperature in this study. The grown crystal was characterized by UV-Vis spectroscopy, FTIR spectroscopy, powder X-ray diffraction studies, and Vickers hardness analysis. L-Alanine doped TGS crystals were found to be highly transparent and full faced. The experimental results evidence the suitability of the grown crystal for optoelectronic applications

.

Keywords: Crystal growth; UV-Vis spectroscopy; FTIR spectroscopy; X-ray diffraction.

  1. INTRODUCTION

    Try Glycine Sulphate crystal is considered as one of the potential material for its wide range of applications namely, UV tunable laser, second harmonic generation, and pyro electric IR sensors due to its high pyro electric coefficient, optical transmission, and reasonably low dielectric constant [1-4]. It is a hydrogen bonded ferroelectric material having a typical second order phase transition at a Curie temperature of 490C [5-7]. Below Curie temperature, ferroelectric and pyro electric materials are polar and possess a spontaneous polarization or electric dipole moment [8-11].

    Despite its complicated chemical and crystallographic form, it is being studied for several years mainly for two reasons: firstly, its excellent pyro electric properties and high figure of merits make it suitable for use in the low- power detector applications where high directivities are required, e.g. in the setup of spectrometers. Secondly, it is one of the very few ferroelectrics known to exhibit a typical order-disorder type of phase transition, offering a spectrum of possibilities for understanding the basic mechanism of group-subgroup type of phase transitions in crystalline solids.

    In Triglycine sulphate, glycine is one of the amino acids. The substitution of another amino acid L Alanine in the place of glycine has been found to improve the crystal properties by way of contributing to effective internal bias in these crystals which, in turn inhibits ferroelectric switching giving permanently poled single domain crystal. This improved the device characteristics and hence Alanine mixed crystals of TGS family has been investigated by many researchers (Fang et al 1983).

    In this paper the effect of doping TGS crystal with the amino acid L-Alanine and results obtained from various characterization studies have been reported. The doped crystal has been named as LATGS.

  2. MATERIALS AND METHODS:

Synthesis and crystal growth: Analar grade reagents Glycine and concentrated sulphuric acid (H2SO4) were dissolved in deionized water in the molar ratio of 3:1, and

the solution was heated at 500C to obtain synthesized TGS salt. Glycine reacts with sulphuric acid as follows.

3(NH2CH2COOH) +H2SO4 (NH2CH2COOH)3.H2SO4

The synthesized salt was again dissolved in double distilled water and then recrystallized by natural evaporation process. This process was repeated two times to improve the purity of the material.

To obtain doped TGS crystal, L-Alanine was added to the saturated mother solution. Highly transparent and full faced crystals were obtained within three weeks. The pure TGS and L-Alanine doped TGS crystals grown are colourless and are shown in figure

1 (a) and 1(b) respectively.

Fig 1(a). Photograph of pure TGS

Fig 1(b). Photograph of L-Alanine doped TGS

TGS may be called glycine-di glyciniumsulphate with chemical formula (NH3+CH2COO-)(NH3+CH2COOH)2 SO42-). Of the three glycine groups contained in the asymmetric unit, two assume a completely planar configuration and the third one assumes a partially planar

configuration. The bond between two planar groups II and III are responsible for ferroelectric transition. Above the Curie temperature, glycine I molecule is split. Reversal of the polarization in the material is largely associated with the rotation of the glycine I group about the crystallographic a axis to change into its mirror image [12].

3 RESULTS AND DISCUSSION:

3.1 UV-Vis spectral analysis

Optical properties of crystalline materials give information regarding the composition, nature and quality of the crystal. The optical transmission spectra of the grown crystal were carried out in the range of 200nm to 800nm covering the entire near-ultraviolet, visible, and near infrared region using SHIMADZU UV-160 Spectrometer to find the transmission range about the suitability of the grown crystal for optical applications. An optically polished single crystal was used for this study. The UV-Vis NIR spectrum of the pure and doped TGS crystal is shown in fig 2 (a) and 2 (b) respectively. The UV cut off for the doped crystal was found to be 218 nm and the low absorption through the entire visible region is one of the most desired properties for the fabrication of optoelectronic devices. The band gap was

hc

3.2. Powder x-ray diffraction

X-ray diffraction technique is a powerful tool to analyze the crystalline nature of the materials. If the material to be investigated is crystalline, well defined peaks will be observed. Powder X-ray diffraction analysis was carried out by using PANalytical X -Ray diffractometer with Cu K radiation. The sample was scanned over the range 20° – 70°. The XRD pattern obtained for the pure TGS and LATGS is shown in fig 3 (a) and 3(b) respectively.

Fig 3 (a). Powder XRD pattern of pure TGS

calculated using the formula Eg = and the optical band gap is found to be 5.69 eV.

Fig 3 (a). Powder XRD pattern of L-Alanine doped TGS

Fig 2 (a) . Optical Transmission spectra of pure TGS

Fig 2 (b) . Optical Transmission spectra of L-Alanine doped TGS

    1. FTIR spectral study

      The Infrared spectral analysis is effectively used to understand the chemical bonding and it provides information about the functional group present in the synthesized compound. The FTIR spectra have been recorded in the range 400 to 4000 cm1. The FTIR spectra of pure TGS and L-Alanine doped TGS is shown in Figure 4(a) and 4 (b) respectively. The observed frequencies and their assignments for L-Alanine doped TGS crystal are listed in Table 1.

      Fig 4 (a) FTIR spectrum of pure TGS

      Fig 4 (b) FTIR spectrum of L-Alanine doped TGS

      Table1. Frequencies and their assignments for L-Alanine doped TGS crystal.

      The variation of load versus Vickers hardness number is shown in Fig 5.

      Fig. 5. The variation of Vickers hardness versus load for L-Alanine doped TGS crystal.

      Meyers index number was calculated from Meyers Law [13]. Meyers index number was found to be 3 which suggest that L-Alanine doped TGS crystal belongs to soft material category [14]. The stiffness constant is calculated using the formula

      Wavenumber

      Assignments

      3159

      (NH +) symmetric stretching

      3

      2924

      CH2 stretching

      2630

      CH2 stretching

      1716

      Overtones and combinations

      1627

      Amie

      1500

      +) anti symmetric bending (NH3

      1423

      NHi bending+ NH3 symmetric bending

      1311

      CO2 symmetric stretching+ CH2 twisting

      1126

      stretching + NC stretching NC2 3

      902

      C-C stretching

      613

      C2 out of plane bending + C2 N torsion

      +C1O out of plane bending

      501

      NH3 oscillation

      C11= (Hv)7/4

      The variation of load versus stiffness constant for L-Alanine doped TGS crystal is shown in Fig 6.

      Fig. 6. The variation of stiffness Constant versus load for L-Alanine doped TGS crystal.

    2. Vickers Micro hardness Studies.

The hardness of a material is related to its bond strength and crystallographic orientation. The important property of any device material is its mechanical strength, represented by its hardness. Vickers micro hardness indentations were made at room temperature with the load ranging from 10 g to 100

g. The indentation time was kept as 6 sec for all the loads. Vickers micro hardness number, Hv, was calculated using the following equation:

Hv = 1.8544P/ d2

Where P is the applied load in Kg, d is the diagonal length of indentation impression in millimeter, and 1.8544 is a constant of a geometrical factor for the diamond pyramid.

4. Conclusion.

Optically good quality single crystals of pure TGS and L- Alanine doped TGS crystals have been grown by slow evaporation method. UV-Vis spectra showed that the grown crystal was optically transparent through 200-800 nm and hence suggests the suitability of this material for optical devices. Powder X-ray diffraction analysis confirms the crystalline nature of grown crystal. The FTIR spectral analysis confirms the presence of functional groups in the crystals. Vickers micro hardness test shows that the grown crystals belong to the category of soft materials.

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