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Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology.
© 2017, www.IJARIIT.com All Rights Reserved Page | 221
ISSN: 2454-132X
Impact factor: 4.295
(Volume3, Issue6)
Available online at www.ijariit.com
Good Blue Emission of Synthesized Zn2GeO4 Phosphor Doped
with Eu (0.5%)
P. B Lakshmi Prasanna
Department of Physics
VSR & NVR College, Tenali, Andhra Pradesh
psranu@gmail.com
P. Sai Raju
Department of Physics
Government Polytechnic College, Andhra Pradesh
psranu@gmail.con
B. Subba Rao
Department of Physics
VSR & NVR College, Tenali, Andhra Pradesh
bezawadasubbarao1@gmail.com
Dr. K. V. R Murthy
Department of Physics
M. S University of Baroda
drkvrmurth@yahoo.con
Abstract: The present paper discusses an important phosphor material which is Zn2GeO4. The phosphor is prepared by taking
appropriate quantities of ZnO and GeO2 of AR grade. This completes solid state reaction. It is important to note here there is
no evolving of the gases. Therefore this solid state reaction can be called as Green chemistry route. The phosphor Zn2GeO4:
Base and Eu (0.5%) is Excited with 250, 255, 260, 265, 270, 275 nm the PL emission is found around 480nm. For 260nm
excitation, the PL emission intensity of 400nm peak is increased by 75%. It can be stated that the increase PL emission peak
intensity of 480nm peak is due to Eu3+
present in Zn2GeO4. This PL emission intensity may be due to the emission from Eu3+
and or the energy transfer Eu3+
to Ge. One of its promising application is to be used as phosphors in display technology such as
field emission display which is considered to be the next generation flat panel displays.
Keywords: Photoluminescence, X-ray diffraction [XRD], Scanning Electron Microscopy [SEM], Energy Dispersion Spectrum
[EDS], Particle size Analysis, Solid State Reaction technique.
1. INTRODUCTION
Zinc germinate (Zn2GeO4) is a wide band gap semiconducting ternary oxide. In recent years, many efficient sulfide-based
compounds have been investigated as possible candidates. But the luminous efficiency drops dramatically due to easy decomposition
of cathodes under electron bombardment. Oxide-based phosphors are getting more focused these years, due to their good chemical
durability, excellent light output, and an environmental friendliness.
At the present time, only ZnO has the acceptable luminescence performance below 100 V supply voltage. Notably,
experimental results of Zn2GeO4 with native defects indicate its photoluminescence (PL) is about 40% brighter than that of the
commercial ZnO phosphor. Recently various phosphor materials have been actively investigated to improve their luminescent
properties and to meet the development of a different display and luminescence devices.
2. MATERIALS AND EXPERIMENTAL METHODS
The phosphor Zn2GeO4 prepared with different dopants. The received powder after grinding is transferred into Aluminum crucibles,
these crucibles contain mixer covered with lids are transferred into the furnace. This crucibles contained mixer is heated at 12000
C
for 2 hours and allowed to cool to room temperature by switching off the furnace. After 18 hours of cooling the sintered material
which is a ceramic phosphor is collected from the crucible and grinded thoroughly to get the uniform size of phosphor grounded
using motor and pestle for 30 minutes of each phosphor. All the phosphor samples were characterized by X-ray diffraction using
(Synchrotron Beam Indus -II). The Photoluminescence (PL) emission and excitation spectra were measured by
Spectrofluorophotometer (SHIMADZU, RF-5301 PC) using Xenon lamp as excitation source at display research Lab, Department
Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology.
© 2017, www.IJARIIT.com All Rights Reserved Page | 222
of Applied Physics, Faculty of Technology and Engg., M. S. University, Baroda. The emission and excitation slit was kept at 1.5
nm, recorded at room temperature.
3. RESULTS AND DISCUSSIONS
3.1 Photoluminescence Studies of Zn2GeO4: Base and Eu3+
phosphors
200 250 300 350 400 450 500 550 600 650
0
100
200
300
400
500
600
700
PLIntensity
Wavelength (nm)
1. Ex
=250nm
2. Ex
=255nm
3. Ex
=260nm
4. Ex
=265nm
5. Ex
=270nm
6. Ex
=275nm
Fig.6.0 Zn2
GeO4
Base phosphor
480nm
270nm
1
2
3
4
5
6
em
=480nm
Fig.1 PLE and PL spectra of Zn2GeO4 phosphor
Fig 1 is the PL emission and excitation of the Zn2GeO4 phosphor. This the phosphor is Excited with 250, 255, 260, 265, 270, 275
nm the PL emission is found around 480nm. When the PL excitation is recorded monitoring at 480nm and excitation is found at
270nm. From the fig 1, it is observed as the excitation wavelength increases the PL emission Increases linearly up to 265nm and
this decreases marginally. The highest intensity for 265nm excitation of the 480nm peak of Zn2GeO4 is due to resonance energy
transfer from Zn to Ge.
200 250 300 350 400 450 500 550 600 650
0
100
200
300
400
500
600
700
PLIntensity
Wavelenth(nm)
1. Em=480nm
2. Ex=250nm
3. Ex=255nm
4. Ex=260nm
5. Ex=265nm
Fig. 6.1 Zn2
GeO4
:Eu(0.5 mol%)
480nm
2
1
3
4
5
265nm
Fig.2 PLE and PL spectra of Eu (0.5%) doped Zn2GeO4 phosphor
Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology.
© 2017, www.IJARIIT.com All Rights Reserved Page | 223
Fig 2 is the PL emission and excitation spectra of Eu doped Zn2GeO4 phosphor. Fig 2 curve 1 is the excitation spectra when
monitored at 480nm. Curve2, 3, 4, 5 are the PL emissions for different excitations. As the excitation wavelength increases, the PL
emission also increases linearly up to 260nm excitation and reduced marginally for 265nm. The PL emission of Eu doped Zn2GeO4
spreads near UV to 620nm peaking at 480 nm (Blue region).
Table 1: Excitation wavelength and intensity of 480nm emission peak of
Eu doped Zn2GeO4 phosphors
S.No Sample Excitation
Wavelength(nm)
Intensity of 480 nm Emission
Peak
1
Zn2GeO4:
Eu(0.5%)
250 321
2 255 533
3 260 692
4 265 591
Here Table 1 is the excitation wavelength and intensity of 480nm emission peak of Eu doped Zn2GeO4 phosphor. It is found from
the fig. as excitation wavelength increases, the emission intensity of 480nm peak linearly increases upto 260nm excitation for better
understanding.
3.2 XRD Pattern of Zn2GeO4: Base and Eu (0.5%) Phosphors
From the XRD pattern, it can be observed both the phosphors looks mostly in a single phase. The crystallite size is calculated using
Scherrer’s formula d=Kλ/ β cosθ, where ‘K’ is the Scherer’s constant (0.94), ‘λ’ the wavelength of the X-ray (1.54060 Å), ‘β’ the
full-width at half maxima (FWHM), ‘θ’ the Bragg angle of the XRD big peak. Using the Schrieffer’s formula the crystallite size.
Fig.3 XRD pattern of Zn2GeO4 phosphor Fig.4 XRD pattern of Eu (0.5%) doped
Zn2GeO4 phosphor
The calculated crystallite size for the base Zn2GeO4 phosphor is 6.35nm and doping of Eu the crystallite size is around
6.89nm. From overall XRD study, the phosphor under study the addition of dopants to the host material did not change their
crystallite size significantly.
3.3 SEM diagram of Zn2GeO4: Base and Eu (0.5%) Phosphors
Fig 5 is the SEM of Zn2GeO4 phosphor. From the micro graphs, it is found that particles are looks like broken pieces without
any shape.
Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology.
© 2017, www.IJARIIT.com All Rights Reserved Page | 224
Fig.5 SEM image of Zn2GeO4 base phosphor
Fig 6 is the SEM of Eu (0.5%) doped with Zn2GeO4 phosphor. From the micro graphs, it is found that particles are looks
like broken pieces without any shape.
Fig.6 SEM image of Eu (0.5%) doped Zn2GeO4 phosphor
3.3 EDS Spectrum of Zn2GeO4: Base and Eu(0.5%) Phosphors
EDS is recorded in the SEM machine where in SEM micrographs are recorded. Here Fig 7 and Fig 8 are the EDS spectra of the
phosphors mentioned. In EDS spectrums mostly elements of base materials are seen. However, in the few of the EDS spectrums
magnesium is seen which are adjacent elements of the host elements and their contribution to PL is negligible. Therefore, in general,
it is normally concluded that the phosphors under EDS study are pure without any impurities.
Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology.
© 2017, www.IJARIIT.com All Rights Reserved Page | 225
Fig.7 EDS of Zn2GeO4 phosphor
Fig.8 EDS of Eu (0.5%) doped Zn2GeO4 phosphor
6.4: PARTICLE SIZE ANALYSIS
0 50 100 150 200 250 300
0
1
2
3
4
5
Relative%
particle diameter
B
0 50 100 150 200 250
0
1
2
3
4
5
6
Relative%
particle diameter
B
Fig.9 particle size histogram of Fig.10 particle size histogram of
Zn2GeO4 Base phosphor Zn2GeO4: Eu(0.5%) phosphor
Fig.9 and Fig.10 are the particle size histogram of Zn2GeO4 base and Eu(0.5%) doped phosphors. For Zn2GeO4 the specific surface
is 1.125 and for Eu doped, it is 0.816. The specific surface area of the particle reduces gradually as the doping increases.
CONCLUSIONS
 From the fig 1, it is observed as the excitation Wavelength increases the PL emission Increases linearly up to 265nm and
this decreases marginally.
 The PL emission of Zn2GeO4 Base when excited to 250 to 275nm found from 350 to 600nm. The maximum PL
intensity is found for 265 nm excitation and the emission peaking at perfect blue region peaking at 480nm. This is an
interesting observation in Zn2GeO4 phosphors.
 The highest intensity for 265nm excitation of the 480nm peak of Zn2GeO4 Base is due to resonance energy transfer from
Zn to Ge.
 The PL emission of Eu doped Zn2GeO4 spreads near UV to 620nm peaking at 480 nm (Blue region).
 It is found from the fig.2 as excitation wavelength increases, the emission intensity of 480nm peak linearly increases upto
260nm excitation.
 XRD study the calculated crystallite size for the base Zn2GeO4 phosphor is 6.35nm and doping of Eu the crystallite size is
around 6.89nm.
 SEM investigation it is found that particles are looks like broken pieces without any shape.
 EDS study it is normally concluded that the phosphors are pure without any impurities.
 From particle size analysis study the specific surface area of the particle reduces gradually as the doping increases and
comparing the particle size histogram it is suggested high power ball milling to get a uniform size. Hence we are can use
this phosphor on display devices
Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology.
© 2017, www.IJARIIT.com All Rights Reserved Page | 226
REFERENCES
1. Wu X L, Li J-G, Ping D-H, Li J K, Zhu Q, Li X D, Sun X D and Sakka Y 2013 J. Alloys Compd. 559 188.
2. S. Shinoya, W.M. Yen, Phosphor Handbook, Laser and Optical Science and Technology Series, CRC Press, Boca
Raton, 1999.
3. K.V.R. Murthy et al, Journal of Lumin., Vol.124, Issue 2, (2007), Pages 217-220.
4. K V R Murthy, et al, MRB, Vol.41, 10, (2006), 1854-1860.
5. K V R Murthy, et al Philosophical Magazine Letters, Vol.90, No.9, Sept2010, 653–662.
6. Ch. Kishore Babu, K. V. R. Murthy, B. Subba Rao, P. Sujitha, Synthesis and characterization of SrS: Eu, Ga
Phosphor, International Journal on Science Innovations and Discoveries (IJSID)2012,2(3), ISSN: 2249-5347.
7. Yen, W.M et.al, Inorganic Phosphors, CRC Press. Boca Raton, FL (USA),(2004).
8. Maniquiz M C, Jung K Y and Jeong S M 2010, J. Electrochem. Soc. 157 H1135
9. Hipolito M G, Ocampo A C, Fregoso O A, Martinez E, Mendoza J G and Falcony C 2004 Phys. Status Solidi a
201 72
10. Song H W and Wang J W 2006 J. Lumin. 118 220
11. Ratinen H 1972 Phys. Solid State A 12 447
12. Klimczak M, Malinowski M, Sarnecki J and Piramidowicz R 2009 J. Lumin. 129 1869
13. Heyes A L, Seefeldt S and Feist J P 2006 Opt. Laser Technol.38 257
14. Wang H, Yang J, Zhang C M and Lin J 2009 J. Solid State Chem. 182 2716
15. Yang J, Li C, Quan Z, Zhang C, Yang P, Li Y, Yu C and Lin J 2008 J. Phys. Chem. C 112 12777
16. Zhu Q, Li J-G, Li X D and Sun X D 2009 Acta Mater. 57 5975
17. Di W, Wang X, Zhu P and Chen B 2007 J. Solid State Chem.180 467
18. Wu X L, Li J-G, Li J K, Zhu Q, Li X D, Sun X D and Sakka Y 2013 Sci. Technol. Adv. Mater. 14 015006
19. Azuel F 2004 Chem. Rev. 104 139
20. Raukas M, Basun S A, van Schaik W, Yen W M and Happek U 1996 Appl. Phys. Lett. 69 3300 Sci. Technol.
Adv. Mater. 16 (2015) 014902

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Good blue emission of synthesized zn2 geo4 phosphor doped with eu (0.5%)

  • 1. Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology. © 2017, www.IJARIIT.com All Rights Reserved Page | 221 ISSN: 2454-132X Impact factor: 4.295 (Volume3, Issue6) Available online at www.ijariit.com Good Blue Emission of Synthesized Zn2GeO4 Phosphor Doped with Eu (0.5%) P. B Lakshmi Prasanna Department of Physics VSR & NVR College, Tenali, Andhra Pradesh psranu@gmail.com P. Sai Raju Department of Physics Government Polytechnic College, Andhra Pradesh psranu@gmail.con B. Subba Rao Department of Physics VSR & NVR College, Tenali, Andhra Pradesh bezawadasubbarao1@gmail.com Dr. K. V. R Murthy Department of Physics M. S University of Baroda drkvrmurth@yahoo.con Abstract: The present paper discusses an important phosphor material which is Zn2GeO4. The phosphor is prepared by taking appropriate quantities of ZnO and GeO2 of AR grade. This completes solid state reaction. It is important to note here there is no evolving of the gases. Therefore this solid state reaction can be called as Green chemistry route. The phosphor Zn2GeO4: Base and Eu (0.5%) is Excited with 250, 255, 260, 265, 270, 275 nm the PL emission is found around 480nm. For 260nm excitation, the PL emission intensity of 400nm peak is increased by 75%. It can be stated that the increase PL emission peak intensity of 480nm peak is due to Eu3+ present in Zn2GeO4. This PL emission intensity may be due to the emission from Eu3+ and or the energy transfer Eu3+ to Ge. One of its promising application is to be used as phosphors in display technology such as field emission display which is considered to be the next generation flat panel displays. Keywords: Photoluminescence, X-ray diffraction [XRD], Scanning Electron Microscopy [SEM], Energy Dispersion Spectrum [EDS], Particle size Analysis, Solid State Reaction technique. 1. INTRODUCTION Zinc germinate (Zn2GeO4) is a wide band gap semiconducting ternary oxide. In recent years, many efficient sulfide-based compounds have been investigated as possible candidates. But the luminous efficiency drops dramatically due to easy decomposition of cathodes under electron bombardment. Oxide-based phosphors are getting more focused these years, due to their good chemical durability, excellent light output, and an environmental friendliness. At the present time, only ZnO has the acceptable luminescence performance below 100 V supply voltage. Notably, experimental results of Zn2GeO4 with native defects indicate its photoluminescence (PL) is about 40% brighter than that of the commercial ZnO phosphor. Recently various phosphor materials have been actively investigated to improve their luminescent properties and to meet the development of a different display and luminescence devices. 2. MATERIALS AND EXPERIMENTAL METHODS The phosphor Zn2GeO4 prepared with different dopants. The received powder after grinding is transferred into Aluminum crucibles, these crucibles contain mixer covered with lids are transferred into the furnace. This crucibles contained mixer is heated at 12000 C for 2 hours and allowed to cool to room temperature by switching off the furnace. After 18 hours of cooling the sintered material which is a ceramic phosphor is collected from the crucible and grinded thoroughly to get the uniform size of phosphor grounded using motor and pestle for 30 minutes of each phosphor. All the phosphor samples were characterized by X-ray diffraction using (Synchrotron Beam Indus -II). The Photoluminescence (PL) emission and excitation spectra were measured by Spectrofluorophotometer (SHIMADZU, RF-5301 PC) using Xenon lamp as excitation source at display research Lab, Department
  • 2. Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology. © 2017, www.IJARIIT.com All Rights Reserved Page | 222 of Applied Physics, Faculty of Technology and Engg., M. S. University, Baroda. The emission and excitation slit was kept at 1.5 nm, recorded at room temperature. 3. RESULTS AND DISCUSSIONS 3.1 Photoluminescence Studies of Zn2GeO4: Base and Eu3+ phosphors 200 250 300 350 400 450 500 550 600 650 0 100 200 300 400 500 600 700 PLIntensity Wavelength (nm) 1. Ex =250nm 2. Ex =255nm 3. Ex =260nm 4. Ex =265nm 5. Ex =270nm 6. Ex =275nm Fig.6.0 Zn2 GeO4 Base phosphor 480nm 270nm 1 2 3 4 5 6 em =480nm Fig.1 PLE and PL spectra of Zn2GeO4 phosphor Fig 1 is the PL emission and excitation of the Zn2GeO4 phosphor. This the phosphor is Excited with 250, 255, 260, 265, 270, 275 nm the PL emission is found around 480nm. When the PL excitation is recorded monitoring at 480nm and excitation is found at 270nm. From the fig 1, it is observed as the excitation wavelength increases the PL emission Increases linearly up to 265nm and this decreases marginally. The highest intensity for 265nm excitation of the 480nm peak of Zn2GeO4 is due to resonance energy transfer from Zn to Ge. 200 250 300 350 400 450 500 550 600 650 0 100 200 300 400 500 600 700 PLIntensity Wavelenth(nm) 1. Em=480nm 2. Ex=250nm 3. Ex=255nm 4. Ex=260nm 5. Ex=265nm Fig. 6.1 Zn2 GeO4 :Eu(0.5 mol%) 480nm 2 1 3 4 5 265nm Fig.2 PLE and PL spectra of Eu (0.5%) doped Zn2GeO4 phosphor
  • 3. Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology. © 2017, www.IJARIIT.com All Rights Reserved Page | 223 Fig 2 is the PL emission and excitation spectra of Eu doped Zn2GeO4 phosphor. Fig 2 curve 1 is the excitation spectra when monitored at 480nm. Curve2, 3, 4, 5 are the PL emissions for different excitations. As the excitation wavelength increases, the PL emission also increases linearly up to 260nm excitation and reduced marginally for 265nm. The PL emission of Eu doped Zn2GeO4 spreads near UV to 620nm peaking at 480 nm (Blue region). Table 1: Excitation wavelength and intensity of 480nm emission peak of Eu doped Zn2GeO4 phosphors S.No Sample Excitation Wavelength(nm) Intensity of 480 nm Emission Peak 1 Zn2GeO4: Eu(0.5%) 250 321 2 255 533 3 260 692 4 265 591 Here Table 1 is the excitation wavelength and intensity of 480nm emission peak of Eu doped Zn2GeO4 phosphor. It is found from the fig. as excitation wavelength increases, the emission intensity of 480nm peak linearly increases upto 260nm excitation for better understanding. 3.2 XRD Pattern of Zn2GeO4: Base and Eu (0.5%) Phosphors From the XRD pattern, it can be observed both the phosphors looks mostly in a single phase. The crystallite size is calculated using Scherrer’s formula d=Kλ/ β cosθ, where ‘K’ is the Scherer’s constant (0.94), ‘λ’ the wavelength of the X-ray (1.54060 Å), ‘β’ the full-width at half maxima (FWHM), ‘θ’ the Bragg angle of the XRD big peak. Using the Schrieffer’s formula the crystallite size. Fig.3 XRD pattern of Zn2GeO4 phosphor Fig.4 XRD pattern of Eu (0.5%) doped Zn2GeO4 phosphor The calculated crystallite size for the base Zn2GeO4 phosphor is 6.35nm and doping of Eu the crystallite size is around 6.89nm. From overall XRD study, the phosphor under study the addition of dopants to the host material did not change their crystallite size significantly. 3.3 SEM diagram of Zn2GeO4: Base and Eu (0.5%) Phosphors Fig 5 is the SEM of Zn2GeO4 phosphor. From the micro graphs, it is found that particles are looks like broken pieces without any shape.
  • 4. Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology. © 2017, www.IJARIIT.com All Rights Reserved Page | 224 Fig.5 SEM image of Zn2GeO4 base phosphor Fig 6 is the SEM of Eu (0.5%) doped with Zn2GeO4 phosphor. From the micro graphs, it is found that particles are looks like broken pieces without any shape. Fig.6 SEM image of Eu (0.5%) doped Zn2GeO4 phosphor 3.3 EDS Spectrum of Zn2GeO4: Base and Eu(0.5%) Phosphors EDS is recorded in the SEM machine where in SEM micrographs are recorded. Here Fig 7 and Fig 8 are the EDS spectra of the phosphors mentioned. In EDS spectrums mostly elements of base materials are seen. However, in the few of the EDS spectrums magnesium is seen which are adjacent elements of the host elements and their contribution to PL is negligible. Therefore, in general, it is normally concluded that the phosphors under EDS study are pure without any impurities.
  • 5. Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology. © 2017, www.IJARIIT.com All Rights Reserved Page | 225 Fig.7 EDS of Zn2GeO4 phosphor Fig.8 EDS of Eu (0.5%) doped Zn2GeO4 phosphor 6.4: PARTICLE SIZE ANALYSIS 0 50 100 150 200 250 300 0 1 2 3 4 5 Relative% particle diameter B 0 50 100 150 200 250 0 1 2 3 4 5 6 Relative% particle diameter B Fig.9 particle size histogram of Fig.10 particle size histogram of Zn2GeO4 Base phosphor Zn2GeO4: Eu(0.5%) phosphor Fig.9 and Fig.10 are the particle size histogram of Zn2GeO4 base and Eu(0.5%) doped phosphors. For Zn2GeO4 the specific surface is 1.125 and for Eu doped, it is 0.816. The specific surface area of the particle reduces gradually as the doping increases. CONCLUSIONS  From the fig 1, it is observed as the excitation Wavelength increases the PL emission Increases linearly up to 265nm and this decreases marginally.  The PL emission of Zn2GeO4 Base when excited to 250 to 275nm found from 350 to 600nm. The maximum PL intensity is found for 265 nm excitation and the emission peaking at perfect blue region peaking at 480nm. This is an interesting observation in Zn2GeO4 phosphors.  The highest intensity for 265nm excitation of the 480nm peak of Zn2GeO4 Base is due to resonance energy transfer from Zn to Ge.  The PL emission of Eu doped Zn2GeO4 spreads near UV to 620nm peaking at 480 nm (Blue region).  It is found from the fig.2 as excitation wavelength increases, the emission intensity of 480nm peak linearly increases upto 260nm excitation.  XRD study the calculated crystallite size for the base Zn2GeO4 phosphor is 6.35nm and doping of Eu the crystallite size is around 6.89nm.  SEM investigation it is found that particles are looks like broken pieces without any shape.  EDS study it is normally concluded that the phosphors are pure without any impurities.  From particle size analysis study the specific surface area of the particle reduces gradually as the doping increases and comparing the particle size histogram it is suggested high power ball milling to get a uniform size. Hence we are can use this phosphor on display devices
  • 6. Prasanna P. B Lakshmi et al, International Journal of Advance Research, Ideas and Innovations in Technology. © 2017, www.IJARIIT.com All Rights Reserved Page | 226 REFERENCES 1. Wu X L, Li J-G, Ping D-H, Li J K, Zhu Q, Li X D, Sun X D and Sakka Y 2013 J. Alloys Compd. 559 188. 2. S. Shinoya, W.M. Yen, Phosphor Handbook, Laser and Optical Science and Technology Series, CRC Press, Boca Raton, 1999. 3. K.V.R. Murthy et al, Journal of Lumin., Vol.124, Issue 2, (2007), Pages 217-220. 4. K V R Murthy, et al, MRB, Vol.41, 10, (2006), 1854-1860. 5. K V R Murthy, et al Philosophical Magazine Letters, Vol.90, No.9, Sept2010, 653–662. 6. Ch. Kishore Babu, K. V. R. Murthy, B. Subba Rao, P. Sujitha, Synthesis and characterization of SrS: Eu, Ga Phosphor, International Journal on Science Innovations and Discoveries (IJSID)2012,2(3), ISSN: 2249-5347. 7. Yen, W.M et.al, Inorganic Phosphors, CRC Press. Boca Raton, FL (USA),(2004). 8. Maniquiz M C, Jung K Y and Jeong S M 2010, J. Electrochem. Soc. 157 H1135 9. Hipolito M G, Ocampo A C, Fregoso O A, Martinez E, Mendoza J G and Falcony C 2004 Phys. Status Solidi a 201 72 10. Song H W and Wang J W 2006 J. Lumin. 118 220 11. Ratinen H 1972 Phys. Solid State A 12 447 12. Klimczak M, Malinowski M, Sarnecki J and Piramidowicz R 2009 J. Lumin. 129 1869 13. Heyes A L, Seefeldt S and Feist J P 2006 Opt. Laser Technol.38 257 14. Wang H, Yang J, Zhang C M and Lin J 2009 J. Solid State Chem. 182 2716 15. Yang J, Li C, Quan Z, Zhang C, Yang P, Li Y, Yu C and Lin J 2008 J. Phys. Chem. C 112 12777 16. Zhu Q, Li J-G, Li X D and Sun X D 2009 Acta Mater. 57 5975 17. Di W, Wang X, Zhu P and Chen B 2007 J. Solid State Chem.180 467 18. Wu X L, Li J-G, Li J K, Zhu Q, Li X D, Sun X D and Sakka Y 2013 Sci. Technol. Adv. Mater. 14 015006 19. Azuel F 2004 Chem. Rev. 104 139 20. Raukas M, Basun S A, van Schaik W, Yen W M and Happek U 1996 Appl. Phys. Lett. 69 3300 Sci. Technol. Adv. Mater. 16 (2015) 014902