S Velayutham1, M Selvapandiyan1. 1. Department of Physics, Periyar University PG Extension Centre, Dharmapuri, 636-701, Tamil Nadu, India.
Abstract
Tri Ethyl Ammonium Picrate (TEAP) and Yttrium (Y2+) ions doped single crystals were grown by slow evaporation technique at room temperature. The estimated band gap of the pure TEAP, 0.10 mol % and 0.15 mol % of Y2+ ions doped TEAP are 3.76 eV, 3.82 eV and 3.86 eV. Crystallite size of the grown materials was calculated from powder XRD as 1.456 nm for TEAP, 3.2028 nm for 0.10 mol % of Y2+ ions doped TEAP and 6.934 nm for 0.15 mol % of Y2+ ions doped TEAP single crystals. Y-O stretching mode was assigned by FTIR spectral peak at 549 cm-1. The PL excitation wavelength of the grown materials is 350 nm. The EDAX analysis confirmed by the Carbon, Nitrogen, Oxygen and Yttrium were presented in grown crystals.
Tri Ethyl Ammonium Picrate (TEAP) and Yttrium (Y2+) ions doped single crystals were grown by slow evaporation technique at room temperature. The estimated band gap of the pure TEAP, 0.10 mol % and 0.15 mol % of Y2+ ions doped TEAP are 3.76 eV, 3.82 eV and 3.86 eV. Crystallite size of the grown materials was calculated from powder XRD as 1.456 nm for TEAP, 3.2028 nm for 0.10 mol % of Y2+ ions doped TEAP and 6.934 nm for 0.15 mol % of Y2+ ions doped TEAP single crystals. Y-O stretching mode was assigned by FTIR spectral peak at 549 cm-1. The PL excitation wavelength of the grown materials is 350 nm. The EDAX analysis confirmed by the Carbon, Nitrogen, Oxygen and Yttrium were presented in grown crystals.
Nonlinear optical materials have been synthesized and grown by many researchers for the past four decades due to their versatile properties such as low laser damage threshold, high third order nonlinear optical susceptibility, and high chemical flexibility [1, 2]. Due to unique properties, the multifunctional NLO material attracts the number of fields of applications like Optical signal processing, Optical switching, Lasers, Sensors, Environment monitors and Optical communications, Optical memory, Optical modulating, Optical storage technology and Optical limiting [3, 4, 5, 6, 7, 8, 9, 10]. Organic nonlinear optical materials are high quality in nature due to π-electron delocalization which means that the valance free electron is interacting with neighbouring electron and enhances the properties of the materials [11]. The phenolic group might favour the formation of hydrogen-bonding interactions to increase the molecular hyperpolarizability and NLO effects [12]. Nonlinear optical response of Tri Ethyl Ammonium Picrate single crystal is 1.5 times as larger than that of KDP [13]. A number of works such as 3-Methyl anilium picrate [14], 1, 3 –Dimethyl urea dimethyl ammonium picrate [15] have been already reported. Based on the literature survey and the knowledge of the authors, no researcher has analysed Tri Ethyl Ammonium Picrate (TEAP) and Y2+ ions doped TEAP and characterised by PL, EDAX, FTIR, and UV –visible technique. In this present investigation, Tri Ethyl Ammonium Picrate, 0.10 mol % and 0.15 mol % of Y2+ ions doped single crystals were grown. The properties of grown crystal were analysed by Powder XRD, UV –visible, FT-IR, PL, and EDAX. The obtained results of grown materials were reported in this article.
Experimental
Single crystals of TEAP were grown by slow evaporation method [16] at room temperature from the calculated amount of AR of grade Tri Ethyl Amine and Picric Acid. Initially 6.97 ml of Tri Ethyl Amine and 22.9 g of picric acids was dissolved in equal mixture of deionised water (50 ml) and ethanol (50 ml) in the molar ratio of 1:1. The mixed solution was stirred continuously for 6 h at 60 °C for getting homogeneous saturated solution. The saturated solution was filtered with the help of Whattman Filter paper (125 mm dia) and kept unperturbed place for evaporation. At the end of 40th day the transparent yellow coloured TEAP crystals with size of 8 × 7 × 5 mm3 was harvested. Again TEAP solution was prepared as per above procedure in two different beakers and then slowly added 0.10 and 0.15 mol % of Yttrium Oxide and stirred continuously about an hour to get completely saturated homogeneous solution. Then clear solution was filtered and kept for evaporation in unperturbed place. The 0.10 and 0.15 mol % of Y2+ ions doped TEAP crystals were obtained at the end of 30th day with the sizes about 5 × 1 × 1 mm3 and 13 × 1 × 1 mm3. The As grown TEAP, 0.10 mol % of Y2+ doped TEAP and 0.15 mol % of Y2+ doped TEAP were shown Fig. 1 (a, b & c). The grown crystals were subjected to various characterization studies such as Powder X-ray diffraction, FTIR, UV –visible, Photoluminescence and EDAX, and their detailed results are discussed in this article.
Fig. 1
As grown: (a) TEAP (b) 0.10 mol % of Y2+ doped TEAP and (c) 0.15 mol % of Y2+ doped TEAP.
As grown: (a) TEAP (b) 0.10 mol % of Y2+ doped TEAP and (c) 0.15 mol % of Y2+ doped TEAP.
Results and discussion
Powder X-ray diffraction studies
Powder X-ray diffraction studies have been carried out to confirm the crystallinity of the grown crystals by using The X-Pert PRO family of multipurpose PAN analytical X-ray diffractometer with the wavelength of CuKα radiation (λ = 1.54 Å). The Powder XRD pattern of pure TEAP and Y2+ ions doped TEAP is shown Fig. 2. All the prominent peaks are indexed with JCPDS card No 51–2120. Calculated lattice parameters of the grown crystals are a = 6.985 Å, b = 22.03 Å, c = 20.810 Å and α = β = γ = 90°. Lattice parameters confirm that the grown crystals belong to the system of Orthorhombic [17]. The doped crystals angles were slightly shifted and intensity of peaks varied due to concentrations of Y2+ ions in Tri Ethyl Ammonium Picrate, but not altered the crystal system of grown materials. High crystalline nature of the materials was confirmed by the well defined sharp peaks. The estimated average crystallite size and Lattice strain of the materials are 1.456 nm, 3.2038 nm, 6.934 nm and 0.12522, 0.06658, 0.03048 for pure TEAP, 0.10 mol % and 0.15 mol % of Y2+ ions doped TEAP single crystals. The estimated average crystallite size is high for 0.15 mol % of Y2+ ions concentrated materials which shows that the materials have higher quality structural nature than that of pure TEAP. Under the assumption and Debye Sheerer formula, the crystallite sizes of the grown materials were calculated. An estimated Average Crystallite size and lattice strain of the grown crystals have presented in the
Table 1.
Fig. 2
Powder XRD Pattern of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ +TEAP.
Table 1
An Average Crystallite size and lattice strain of the grown crystals.
S. No.
Crystals
2θ (degree)
Crystallite Size (nm)
Lattice Strain
Average Crystallite Size (nm)
Average Lattice Strain
1
Pure TEAP
17.02
1.44
0.1702
1.456
0.12522
22.77
1.45
0.1300
23.63
1.45
0.1217
25.42
1.46
0.1129
31.17
1.48
0.0913
2
0.10 mol % of Y2+ions doped TEAP
11.57
3.13
0.1146
3.2038
0.06658
17.02
3.15
0.0776
22.17
3.18
0.0593
25.02
3.19
0.0523
43.47
3.36
0.0291
3
0.15 mol % of Y2+ions doped TEAP
10.72
6.81
0.0570
6.934
0.03048
18.97
6.87
0.0320
25.17
6.94
0.0239
28.47
6.99
0.0211
32.32
7.06
0.0184
Powder XRD Pattern of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ +TEAP.An Average Crystallite size and lattice strain of the grown crystals.
FTIR studies
Fourier transform infrared spectral studies of the grown Tri Ethyl Ammonium Picrate, 0.10 mol % and 0.15 mol % of Y2+ ions doped Tri Ethyl Ammonium Picrate single crystals was analysed by using Perkin Elmer spectrometer (version 10.4.00) in the range of 4000 cm−1 – 400 cm−1. The analysed and recorded spectra of the grown crystals are depicted in Fig. 3. The peaks are found at 3433, 3091, 1632, 1559 and 1436 cm−1 due to the presence of N–H stretching, C–H stretching, CO stretching, N–H bending and CC stretching vibration. The CH2 bending, C–O stretching, and C–O–C asymmetric stretching of the molecule was assigned by the peaks 720, 1078 and 1274 cm−1 [[18], [19]]. The peak at 549 cm−1 could be attributed to Y–O stretching mode. In the case of doped materials, the spectral peaks were slightly shifted due to the incorporation of Y2+ ions in pure TEAP. The vibrational frequencies and Assignments of the pure and doped materials have been given in the Table 2.
Fig. 3
FT-IR spectra of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ +TEAP.
Table 2
Vibrational frequency and assignment of TEAP and doped TEAP.
Assignment
Vibration frequencies (cm−1)
0.15 mol % Y2++TEAP
0.10 mol % Y2++TEAP
TEAP
N–H Stretching
3417
3417
3433
C–H Stretching
-
3034
3091
CO Stretching
1641
1632
1632
N–H bending
1559
1559
1559
CC Stretching
1485
1494
1436
C–O–C Asymmetric Stretching
1274
1266
1274
C–O Stretching
1078
1070
1078
CH2 bending
720
712
712
Y–O Stretching
549
516
525
FT-IR spectra of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ +TEAP.Vibrational frequency and assignment of TEAP and doped TEAP.
UV – visible studies
UV –Visible studies of Tri Ethyl Ammonium Picrate (TEAP), 0.10 mol % and 0.15 mol % of Y2+ ions doped TEAP was carried out using Thermo fisher Evolution 220 UV –Visible Spectrophotometer in the range of 190 nm–1100 nm at Alagappa University, Karaikudi as shown in Figs. 4 and 5. From the absorption spectra cut off wavelength of the materials was observed as 309.16 nm for TEAP, 307.49 nm for 0.10 mol % of Y2+ ions doped TEAP and 306.30 nm for 0.15 mol % of Y2+ ions doped TEAP respectively. The transmittance of TEAP, 0.10 mol % Y2+ ions and 0.15 mol % Y2+ ions doped TEAP crystals are 74.70 %, 83.47 % and 87.52 % in entire visible and near IR regions. This results show that the transmittance of the 0.15 mol % of Y2+ ions doped materials have greater value than that of TEAP and 0.10 mol % Y2+ ions doped materials. This increase of transmittance of the material is due to the higher concentrations of Y2+ ions in TEAP. By using the absorption data, the graph was plotted between hν and (αhν)2 to find the forbidden energy gap of the grown materials and as shown in Fig. 6. The obtained forbidden energy band gap of the grown materials from Tauc's plot graphs are 3.76 eV, 3.82 eV and 3.87 eV for TEAP, 0.10 mol % and 0.15 mol % of Y2+ ions doped TEAP crystals. UV –Visible studies results reveal that the 0.15 mol % of Y2+ ions doped material is a well suitable candidate for optoelectronic device applications [20, 21].
Fig. 4
UV –Vis Absorbance spectra of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ +TEAP.
Fig. 5
UV –Vis Transmittance spectra of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ + TEAP.
Fig. 6
hν vs (αhν) 2.
UV –Vis Absorbance spectra of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ +TEAP.UV –Vis Transmittance spectra of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ + TEAP.hν vs (αhν) 2.
Photoluminescence studies
The Photoluminescence studies of the grown materials were carried out by using Varian Cary Eclipsc Photoluminescence spectrometer (Oxford low temperature LN277K setup) in the wavelength range between 350 nm and 600 nm. PL spectra of Tri Ethyl Ammonium Picrate (TEAP), 0.10 mol % of Y2+ ions doped TEAP and 0.15 mol of % Y2+ ions doped TEAP crystals is shown in Fig. 7. The Photoluminescence spectra exhibited a broad band from 400 nm to 475 nm with lower intensities due to the benzene ring in TEAP crystals. The excitation wavelength of the grown materials is 350 nm and the sharp emission peaks was observed at 488 nm with few additional peaks were found at 507 nm (2.45 eV), 521 nm (2.38 eV) and 552nm (2.25 eV). The sharp peak at 488 nm shows that the materials have blue emission on excitation wavelength at 350 nm. Additional peaks were observed at 507 nm, 521 nm and 552 nm are also shows that the materials have blue and green emission. Both Intensities and Wavelength of all the doped material was shifted due to the addition of Yttrium in TEAP. From the PL spectra, the sharp emission peak suggests that the grown materials are well suitable candidate to use in Photonic applications.
Fig. 7
Photoluminescence spectra of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ +TEAP.
Photoluminescence spectra of TEAP, 0.10 mol % Y2+ +TEAP and 0.15 mol % Y2+ +TEAP.
EDAX analysis
Energy dispersive X-ray analysis (EDAX) is an important tool to obtain the chemical composition of the grown single crystals. Tri Ethyl Ammonium Picrate (TEAP), 0.10 mol % of Y2+ ions doped TEAP, 0.15 mol % of Y2+ ion doped TEAP single crystals was subjected to Energy dispersive X-ray analysis by using EDS BRUKER NANO GMBH D-12489 (Germany) with accelerating voltage 0–30 kV. As per the Molecular formula of TEAP (C12H18N4O7) and dopants (Y2O3), Carbon, Nitrogen, Oxygen and Yttrium elements were presented in grown materials. The EDAX spectrum of pure TEAP, 0.10 mol % and 0.15 mol % of Y2+ doped TEAP are exhibited in Figs. 8, 9, and 10. The atomic Wt % and Wt % of the elements of the materials are tabulated in Table 3.
Fig. 8
EDAX spectrum of TEAP.
Fig. 9
EDAX spectrum of 0.10 mol% Y2+ +TEAP.
Fig. 10
EDAX spectrum of 0.15 mol % Y2+ +TEAP.
Table 3
Percentage of elements in TEAP and doped TEAP.
S. No.
Elements
TEAP
0.10 mol % of Y2+ TEAP
0.15 mol % of Y2+ TEAP
At wt%
Wt %
At wt%
Wt %
At wt%
Wt %
1
C
43.90
38.02
56.71
50.69
42.17
32.56
2
N
36.94
42.63
25.85
30.78
37.42
38.50
3
O
19.16
19.35
17.39
18.13
18.22
16.40
4
Y
0.06
0.40
2.19
12.54
EDAX spectrum of TEAP.EDAX spectrum of 0.10 mol% Y2+ +TEAP.EDAX spectrum of 0.15 mol % Y2+ +TEAP.Percentage of elements in TEAP and doped TEAP.
Conclusion
The single crystals of TEAP and Y2+ ions doped TEAP crystals were grown by slow evaporation method at room temperature. The calculated lattice parameters are a = 6.985 Å, b = 22.03 Å, c = 20.810 Å and α = β = γ = 90° which confirms that the grown materials belong to crystal system of Orthorhombic. The FTIR spectral peak at 549 cm−1 could be attributed to Y–O stretching mode. EDAX spectra revealed the presence of elements Carbon, Nitrogen, Oxygen and Yttrium in the grown materials. The PL emission peak was observed at 488 nm. Based on the analysis report, 0.15 mol % of Y2+ ions doped TEAP single crystal is well suitable candidate to use in optoelectronic device applications.
Declarations
Author contribution statement
Shanmugam Velayutham: Conceived and designed the experiments; Performed the experiments; Analyzed and interpreted the data; Contributed reagents, materials, analysis tools or data.Selvapandiyan Marimuthu: Conceived and designed the experiments; Analyzed and interpreted the data; Contributed reagents, materials, analysis tools or data; Wrote the paper.
Funding statement
This research did not receive any specific grant from funding agencies in the public, commercial, or not-for-profit sectors.
Competing interest statement
The authors declare no conflict of interest.
Additional information
No additional information is available for this paper.
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