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M.Bhushana Reddy et al. Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 11, (Part - 1) November 2015, pp.96-98
www.ijera.com 96 | P a g e
Optical analysis of Cu2+
: CdO - Li2O - B2O3 -TeO2 glass
M.Bhushana Reddy, P.Giridhar, B. Sudhakar Reddy *
Department of Physics, S.V. Degree College, Kadapa-516003, India
ABSTRACT
This article reports on the optical analysis of Cu2+
(0.5 mol %): 59.5B2O3 – 20 TeO2 – 10CdO – 10Li2O glass.
From XRD spectrum , amorphous nature of the glass has been studied. Absorption spectrum of the copper glass
shows a broad absorption band (2
B1g→2
B1g) at 829 nm has been observed. Emission spectrum of Cu2+
(0.5 mol
%): 59.5B2O3 – 20 TeO2 – 10CdO – 10Li2O glass has exhibits a blue emission at 439 nm with an excitation
wavelength 379 nm.
Keywords: absorption, Cu2+
: glass, emission, excitation, XRD
I. INTRODUCTION
In recent years, a great deal of work has been
carried out on tellurium oxide (TeO2) based glasses.
TeO2 based glasses are of great scientific and
technological interest due to their unique properties
such as good chemical durability, high dielectric
constant, electrical conductivity, transmission
capability, high refractive indices and low melting
points [1, 2]. It is well known that a pure TeO2
chemical does not form a glass under usual
quenching rates but it does so when it is mixed with
certain other oxides such as B2O3, Li2O and CdO etc.,
TeO2 based glasses doped with rare earth and
transition metal ions have received significant
attention because they can considerably change
density, optical and thermal properties of these
glasses [3-7]. The applications of tellurite glasses in
industries such as electrical, optical, electronic and
other fields are immense due to their good
semiconducting properties [8]. Transition metal ions
doped glasses are of great importance because of
their applications in various fields. In glasses, copper
can emit bluish green colour and exist as a
monovalent (Cu+
) ion, or as a divalent (Cu2+
) ion. In
the present work, we have studied the CLBT glasses
with Cu2+
as the dopant transition metal ions to
analyze their optical properties systematically.
II. EXPERIMENTAL
2.1 GLASS PREPARATION
The chemicals used were reagent grade of
H3BO3, Li2O, CdO, TeO2, CuO. Transition metal ion
(Cu2+
) doped CLBT glass is prepared by melt
quenching method in the following composition.
20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O - 0.5Cu2+
All the weighed chemicals were finely
powdered. Each batch of (10g) was melted in an
alumina crucibles in an electric furnace at 9500
C, for
an hour. These melts were quenched between two
brass plates to get 2-3 cm diameter optical glasses
with a uniform thickness of 0.2 cm. All the samples
were annealed at 2000
C for an hour to remove the
thermal strains.
Powder X-ray diffraction (XRD) spectrum was
obtained on a Shimadzu XD3A diffractrometer with a
Ni-filter and CuK (=1.542 A0
) radiation with an
applied voltage as 30kV and 20mA anode current,
calibrated with Si at the rate of 20
/min. The optical
absorption spectrum of Cu2+
glass is obtained on a
Varian-Cary Win Spectrophotometer. Both the
excitation and emission spectra of the glass were
obtained on a SPEX Fluorolog-2 Fluorimeter (Model
II) with a datamax software to acquire the data with a
Xe-arc lamp (150W) as the excitation source.
III. RESULTS AND DISCUSSION
The free ion term Cu2+
(3d9
) is 2
D. In octahedral
crystal field, it splits into 2
Eg and 2
T2g with being the
lower level. 2
Eg generally splits due to Jahn - Teller
effect. Therefore, Cu2+
is rarely found in regular
octahedral site. Accordingly, in the present
investigation, Cu2+
is taken to be octahedrally
coordinated by six oxygen atoms and the octahedron
is tetragonally distorted. Therefore in the tetragonally
distorted octahedral environment, the 2
Eg level splits
into 2
A1 and 2
B1 and 2
T2g levels into 2
E and 2
B2, the
ground state being 2
B1[10].
XRD pattern of (0.5 mol %) Cu2+
: CLBT glass is
shown in Fig.1. From this pattern, the glass
amorphous nature has been confirmed. The
absorption spectrum of (0.5 mol %) Cu2+
: CLBT
glass is shown in Fig.2. From this figure an
absorption band centered at 829 nm is observed and
is assigned to the transition 2
B1g→ 2
B2g. The optical
absorption studies confirm the presence of Cu2+
ions
in the 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O :
0.5Cu2+
glass.
The excitation spectrum of (0.5 mol %) Cu2+
:
CLBT glass is shown in Fig.3. with an excitation
band at 379 nm. According to ligand field theory,
oxide based glasses could show charge transfer bands
in the UV region due to the absorption by the oxygen
RESEARCH ARTICLE OPEN ACCESS
M.Bhushana Reddy et al. Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 11, (Part - 1) November 2015, pp.96-98
www.ijera.com 97 | P a g e
ligands around the cations. This band is due to charge
transfer phenomena caused by O2-
with an UV
radiation exposure.
Fig. 4, indicates the emission spectrum of (0.5
mol %) Cu2+
: CLBT glass, which shows two
emission bands at 418 nm and 439 nm respectively
with an excitation wavelength 379 nm. Among these
two, the intense emission band at 439 nm indicates
blue emission.However, according to an earlier report
[9], emission at 439 nm arises due to localized
excitation of isolated Cu2+
ions.
IV. CONCLUSION
It is concluded that, we have developed
transparent, moisture resistant and more stable optical
glass based on the chemical composition of (0.5
mol%) Cu2+
: 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O
.Keeping in view of these encouraging optical
properties, Cu2+
glasses have been selected to
examine its amorphous nature through XRD
spectrum. Absorption spectrum has revealed the
presence of Cu2+
ions, in the glass investigated.
Emission spectrum of Cu2+
(0.5 mol %): 20 TeO2 –
59.5B2O3 – 10CdO – 10Li2O: 0.5Cu2+
glass has
revealed a blue emission at 439 nm with an excitation
wavelength 389 nm. Based on the spectral results, we
suggest that, the Cu2+
glasses have potential
applications to carry on further research work with
several other transition metal ions. Such novel
glasses are considered as potential optical systems. It
is strongly contemplated for further development in
future as laser materials doping with suitable lasing
ions.
V. ACKNOWLEDGEMENTS
This work was financially supported by the
University Grants Commission under Minor
Research Project Scheme No.F. MRP-
6313/15(SERO/UGC) for distinguished teachers
working in Degree Colleges. In this regard one of the
authors (MBR) would like to sincerely thanks the
Joint Secretary (UGC- SERO, Hyderabad, A.P.,
India.) for his kind co-operation and support for this
present work.
REFERENCES
[1.] S. Tanabe, K. Hirao, N. Soga J. Non-Cryst.
Solids 122(1) (1990) 79-82.
[2.] H. Nasu, O. Matsusita, K. Kamiya, H.
Kobayashi, K. Kubodera J. Non-Cryst.
Solids 124 (1990) 275-277.
[3.] K. Kumar, S. B. Rai, D. K. Rai Spectrochim.
Acta A 66 (2007)1052-1057.
[4.] Arshpreet Kaur, Atul Khanna, Carmen
Pesquera, Fernando González, Vasant Sathe
J. Non-Cryst Solids 356 (2010) 864–872.
[5.] L. M. Sharaf El-Deen, M. S. Alsalhi, M. M.
Elkholy, J. Alloy. Compd. 465 (2008) 333-
339.
[6.] El SayedYousef, A. El-Adaway, N. El-
Koshkahany, E. R. Shaaban, J. Phys. Chem.
Solids 67 (2006) 1649-1655.
[7.] J. Ozdanova, H. Jicha, I. Jichy, J. Non-
Cryst. Solids 353 (2007) 2799-2802.
[8.] H. Burger, W. Vogel, V. Kozhukharov
Infrared Phys. 25 (1985) 395-409.
[9.] B. Sudhakar Reddy, S. Buddhudu, Bull.
Mater. Sci. 30 (2007) 481-486.
[10.] R.V.S.S.N Ravikumar, R. Komatsu, K.
Ikeda, A V. Chandrasekhar, L.
Ramamoorthy, B.J. Reddy, Y.P. Reddy, P.S.
Rao Physica B, 334 (2003) 398.
Figures
Fig.1. XRD spectrum of 20 TeO2 – 59.5B2O3 –
10CdO – 10Li2O - 0.5Cu2+
glass
M.Bhushana Reddy et al. Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 11, (Part - 1) November 2015, pp.96-98
www.ijera.com 98 | P a g e
Fig.2.Absorption spectrum of 20 TeO2 – 59.5B2O3
– 10CdO – 10Li2O - 0.5Cu2+
glass
Fig.3.Excitation spectrum of 20 TeO2 – 59.5B2O3 –
10CdO – 10Li2O - 0.5Cu2+
glass
Fig.4.Emission spectrum of 20 TeO2 – 59.5B2O3 –
10CdO – 10Li2O - 0.5Cu2+
glass

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Optical analysis of Cu2+: CdO - Li2O - B2O3 -TeO2 glass

  • 1. M.Bhushana Reddy et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 11, (Part - 1) November 2015, pp.96-98 www.ijera.com 96 | P a g e Optical analysis of Cu2+ : CdO - Li2O - B2O3 -TeO2 glass M.Bhushana Reddy, P.Giridhar, B. Sudhakar Reddy * Department of Physics, S.V. Degree College, Kadapa-516003, India ABSTRACT This article reports on the optical analysis of Cu2+ (0.5 mol %): 59.5B2O3 – 20 TeO2 – 10CdO – 10Li2O glass. From XRD spectrum , amorphous nature of the glass has been studied. Absorption spectrum of the copper glass shows a broad absorption band (2 B1g→2 B1g) at 829 nm has been observed. Emission spectrum of Cu2+ (0.5 mol %): 59.5B2O3 – 20 TeO2 – 10CdO – 10Li2O glass has exhibits a blue emission at 439 nm with an excitation wavelength 379 nm. Keywords: absorption, Cu2+ : glass, emission, excitation, XRD I. INTRODUCTION In recent years, a great deal of work has been carried out on tellurium oxide (TeO2) based glasses. TeO2 based glasses are of great scientific and technological interest due to their unique properties such as good chemical durability, high dielectric constant, electrical conductivity, transmission capability, high refractive indices and low melting points [1, 2]. It is well known that a pure TeO2 chemical does not form a glass under usual quenching rates but it does so when it is mixed with certain other oxides such as B2O3, Li2O and CdO etc., TeO2 based glasses doped with rare earth and transition metal ions have received significant attention because they can considerably change density, optical and thermal properties of these glasses [3-7]. The applications of tellurite glasses in industries such as electrical, optical, electronic and other fields are immense due to their good semiconducting properties [8]. Transition metal ions doped glasses are of great importance because of their applications in various fields. In glasses, copper can emit bluish green colour and exist as a monovalent (Cu+ ) ion, or as a divalent (Cu2+ ) ion. In the present work, we have studied the CLBT glasses with Cu2+ as the dopant transition metal ions to analyze their optical properties systematically. II. EXPERIMENTAL 2.1 GLASS PREPARATION The chemicals used were reagent grade of H3BO3, Li2O, CdO, TeO2, CuO. Transition metal ion (Cu2+ ) doped CLBT glass is prepared by melt quenching method in the following composition. 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O - 0.5Cu2+ All the weighed chemicals were finely powdered. Each batch of (10g) was melted in an alumina crucibles in an electric furnace at 9500 C, for an hour. These melts were quenched between two brass plates to get 2-3 cm diameter optical glasses with a uniform thickness of 0.2 cm. All the samples were annealed at 2000 C for an hour to remove the thermal strains. Powder X-ray diffraction (XRD) spectrum was obtained on a Shimadzu XD3A diffractrometer with a Ni-filter and CuK (=1.542 A0 ) radiation with an applied voltage as 30kV and 20mA anode current, calibrated with Si at the rate of 20 /min. The optical absorption spectrum of Cu2+ glass is obtained on a Varian-Cary Win Spectrophotometer. Both the excitation and emission spectra of the glass were obtained on a SPEX Fluorolog-2 Fluorimeter (Model II) with a datamax software to acquire the data with a Xe-arc lamp (150W) as the excitation source. III. RESULTS AND DISCUSSION The free ion term Cu2+ (3d9 ) is 2 D. In octahedral crystal field, it splits into 2 Eg and 2 T2g with being the lower level. 2 Eg generally splits due to Jahn - Teller effect. Therefore, Cu2+ is rarely found in regular octahedral site. Accordingly, in the present investigation, Cu2+ is taken to be octahedrally coordinated by six oxygen atoms and the octahedron is tetragonally distorted. Therefore in the tetragonally distorted octahedral environment, the 2 Eg level splits into 2 A1 and 2 B1 and 2 T2g levels into 2 E and 2 B2, the ground state being 2 B1[10]. XRD pattern of (0.5 mol %) Cu2+ : CLBT glass is shown in Fig.1. From this pattern, the glass amorphous nature has been confirmed. The absorption spectrum of (0.5 mol %) Cu2+ : CLBT glass is shown in Fig.2. From this figure an absorption band centered at 829 nm is observed and is assigned to the transition 2 B1g→ 2 B2g. The optical absorption studies confirm the presence of Cu2+ ions in the 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O : 0.5Cu2+ glass. The excitation spectrum of (0.5 mol %) Cu2+ : CLBT glass is shown in Fig.3. with an excitation band at 379 nm. According to ligand field theory, oxide based glasses could show charge transfer bands in the UV region due to the absorption by the oxygen RESEARCH ARTICLE OPEN ACCESS
  • 2. M.Bhushana Reddy et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 11, (Part - 1) November 2015, pp.96-98 www.ijera.com 97 | P a g e ligands around the cations. This band is due to charge transfer phenomena caused by O2- with an UV radiation exposure. Fig. 4, indicates the emission spectrum of (0.5 mol %) Cu2+ : CLBT glass, which shows two emission bands at 418 nm and 439 nm respectively with an excitation wavelength 379 nm. Among these two, the intense emission band at 439 nm indicates blue emission.However, according to an earlier report [9], emission at 439 nm arises due to localized excitation of isolated Cu2+ ions. IV. CONCLUSION It is concluded that, we have developed transparent, moisture resistant and more stable optical glass based on the chemical composition of (0.5 mol%) Cu2+ : 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O .Keeping in view of these encouraging optical properties, Cu2+ glasses have been selected to examine its amorphous nature through XRD spectrum. Absorption spectrum has revealed the presence of Cu2+ ions, in the glass investigated. Emission spectrum of Cu2+ (0.5 mol %): 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O: 0.5Cu2+ glass has revealed a blue emission at 439 nm with an excitation wavelength 389 nm. Based on the spectral results, we suggest that, the Cu2+ glasses have potential applications to carry on further research work with several other transition metal ions. Such novel glasses are considered as potential optical systems. It is strongly contemplated for further development in future as laser materials doping with suitable lasing ions. V. ACKNOWLEDGEMENTS This work was financially supported by the University Grants Commission under Minor Research Project Scheme No.F. MRP- 6313/15(SERO/UGC) for distinguished teachers working in Degree Colleges. In this regard one of the authors (MBR) would like to sincerely thanks the Joint Secretary (UGC- SERO, Hyderabad, A.P., India.) for his kind co-operation and support for this present work. REFERENCES [1.] S. Tanabe, K. Hirao, N. Soga J. Non-Cryst. Solids 122(1) (1990) 79-82. [2.] H. Nasu, O. Matsusita, K. Kamiya, H. Kobayashi, K. Kubodera J. Non-Cryst. Solids 124 (1990) 275-277. [3.] K. Kumar, S. B. Rai, D. K. Rai Spectrochim. Acta A 66 (2007)1052-1057. [4.] Arshpreet Kaur, Atul Khanna, Carmen Pesquera, Fernando González, Vasant Sathe J. Non-Cryst Solids 356 (2010) 864–872. [5.] L. M. Sharaf El-Deen, M. S. Alsalhi, M. M. Elkholy, J. Alloy. Compd. 465 (2008) 333- 339. [6.] El SayedYousef, A. El-Adaway, N. El- Koshkahany, E. R. Shaaban, J. Phys. Chem. Solids 67 (2006) 1649-1655. [7.] J. Ozdanova, H. Jicha, I. Jichy, J. Non- Cryst. Solids 353 (2007) 2799-2802. [8.] H. Burger, W. Vogel, V. Kozhukharov Infrared Phys. 25 (1985) 395-409. [9.] B. Sudhakar Reddy, S. Buddhudu, Bull. Mater. Sci. 30 (2007) 481-486. [10.] R.V.S.S.N Ravikumar, R. Komatsu, K. Ikeda, A V. Chandrasekhar, L. Ramamoorthy, B.J. Reddy, Y.P. Reddy, P.S. Rao Physica B, 334 (2003) 398. Figures Fig.1. XRD spectrum of 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O - 0.5Cu2+ glass
  • 3. M.Bhushana Reddy et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 11, (Part - 1) November 2015, pp.96-98 www.ijera.com 98 | P a g e Fig.2.Absorption spectrum of 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O - 0.5Cu2+ glass Fig.3.Excitation spectrum of 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O - 0.5Cu2+ glass Fig.4.Emission spectrum of 20 TeO2 – 59.5B2O3 – 10CdO – 10Li2O - 0.5Cu2+ glass