Dapčevć, Aleksandra

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86e6c30b-b178-4256-bdef-e409f4bb0255
  • Dapčevć, Aleksandra (3)
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Author's Bibliography

B-site doping as a strategy for tailoring BiFeO3 properties

Radojković, Aleksandar; Luković Golić, Danijela; Ćirković, Jovana; Dapčevć, Aleksandra; Pajić, Damir; Torić, Filip; Branković, Zorica; Branković, Goran

(Društvo za keramičke materijale Srbije, 2017)

TY  - CONF
AU  - Radojković, Aleksandar
AU  - Luković Golić, Danijela
AU  - Ćirković, Jovana
AU  - Dapčevć, Aleksandra
AU  - Pajić, Damir
AU  - Torić, Filip
AU  - Branković, Zorica
AU  - Branković, Goran
PY  - 2017
UR  - http://rimsi.imsi.bg.ac.rs/handle/123456789/2330
AB  - Ferroelectric, magnetic and structural properties of BiFe1–xNbxO3 (x = 0.002,
0.005 and 0.01) ceramics were investigated in order to study the influence of B-site
doping of multiferroic BiFeO3. It is known that pure BiFeO3 exhibits G-type of
antiferromagnetism below Néel temperature (TN = 370 °C) and spontaneous
polarization along one of the eight pseudo-cubic [111] axes below Curie temperature
(TC = 826–845 °C). However, poor ferroelectric (high electrical conductivity) and
weak ferromagnetism of pure BiFeO3 can be enhanced by doping. In this study,
Nb5+ was introduced to replace Fe3+ (B-site doping) since it could disturb the nearly
antiparallel spin ordering of the adjacent Fe3+ ions responsible for cycloidal (spiral)
spin structure. On the other hand, the pentivalent Nb cations will reduce the amount
of oxygen vacancies and consequently reduce the electrical conductivity. It was
shown that 1 % Nb drastically changed the magnetic properties compared with pure
BiFeO3: while the remnant magnetization at 300 K reaches only 0.0042 emu/g at
applied magnetic fields up to 50 000 Oe, the coercive magnetic field as high as
~7460 Oe classifies BiFe0.99Nb0.01O3 as hard magnetic material. With lower Nb
content the magnetic properties moved up towards the properties of pure BiFeO3.
Relatively inferior ferroelectric properties showed the sample with 0.2 % Nb, since
its hysteresis loops deformed at electrical fields higher than 40 kV/cm. At the
highest applied electrical field (70 kV/cm) only the sample with 1 % Nb showed a
stable ferroelectric response with hysteresis periods up to 1000 ms, with the highest
remnant electrical polarization of 0.5 μC/cm2
and the coercive electrical field of 22.2
kV/cm. Thus, it was shown that by carefully selected dopant it was possible to
improve both magnetic and ferroelectric properties of BiFeO3.
PB  - Društvo za keramičke materijale Srbije
C3  - 4th Conference of The Serbian Society for Ceramic Materials
T1  - B-site doping as a strategy for tailoring BiFeO3 properties
SP  - 95
UR  - https://hdl.handle.net/21.15107/rcub_rimsi_2330
ER  - 
@conference{
author = "Radojković, Aleksandar and Luković Golić, Danijela and Ćirković, Jovana and Dapčevć, Aleksandra and Pajić, Damir and Torić, Filip and Branković, Zorica and Branković, Goran",
year = "2017",
abstract = "Ferroelectric, magnetic and structural properties of BiFe1–xNbxO3 (x = 0.002,
0.005 and 0.01) ceramics were investigated in order to study the influence of B-site
doping of multiferroic BiFeO3. It is known that pure BiFeO3 exhibits G-type of
antiferromagnetism below Néel temperature (TN = 370 °C) and spontaneous
polarization along one of the eight pseudo-cubic [111] axes below Curie temperature
(TC = 826–845 °C). However, poor ferroelectric (high electrical conductivity) and
weak ferromagnetism of pure BiFeO3 can be enhanced by doping. In this study,
Nb5+ was introduced to replace Fe3+ (B-site doping) since it could disturb the nearly
antiparallel spin ordering of the adjacent Fe3+ ions responsible for cycloidal (spiral)
spin structure. On the other hand, the pentivalent Nb cations will reduce the amount
of oxygen vacancies and consequently reduce the electrical conductivity. It was
shown that 1 % Nb drastically changed the magnetic properties compared with pure
BiFeO3: while the remnant magnetization at 300 K reaches only 0.0042 emu/g at
applied magnetic fields up to 50 000 Oe, the coercive magnetic field as high as
~7460 Oe classifies BiFe0.99Nb0.01O3 as hard magnetic material. With lower Nb
content the magnetic properties moved up towards the properties of pure BiFeO3.
Relatively inferior ferroelectric properties showed the sample with 0.2 % Nb, since
its hysteresis loops deformed at electrical fields higher than 40 kV/cm. At the
highest applied electrical field (70 kV/cm) only the sample with 1 % Nb showed a
stable ferroelectric response with hysteresis periods up to 1000 ms, with the highest
remnant electrical polarization of 0.5 μC/cm2
and the coercive electrical field of 22.2
kV/cm. Thus, it was shown that by carefully selected dopant it was possible to
improve both magnetic and ferroelectric properties of BiFeO3.",
publisher = "Društvo za keramičke materijale Srbije",
journal = "4th Conference of The Serbian Society for Ceramic Materials",
title = "B-site doping as a strategy for tailoring BiFeO3 properties",
pages = "95",
url = "https://hdl.handle.net/21.15107/rcub_rimsi_2330"
}
Radojković, A., Luković Golić, D., Ćirković, J., Dapčevć, A., Pajić, D., Torić, F., Branković, Z.,& Branković, G.. (2017). B-site doping as a strategy for tailoring BiFeO3 properties. in 4th Conference of The Serbian Society for Ceramic Materials
Društvo za keramičke materijale Srbije., 95.
https://hdl.handle.net/21.15107/rcub_rimsi_2330
Radojković A, Luković Golić D, Ćirković J, Dapčevć A, Pajić D, Torić F, Branković Z, Branković G. B-site doping as a strategy for tailoring BiFeO3 properties. in 4th Conference of The Serbian Society for Ceramic Materials. 2017;:95.
https://hdl.handle.net/21.15107/rcub_rimsi_2330 .
Radojković, Aleksandar, Luković Golić, Danijela, Ćirković, Jovana, Dapčevć, Aleksandra, Pajić, Damir, Torić, Filip, Branković, Zorica, Branković, Goran, "B-site doping as a strategy for tailoring BiFeO3 properties" in 4th Conference of The Serbian Society for Ceramic Materials (2017):95,
https://hdl.handle.net/21.15107/rcub_rimsi_2330 .

Improved multiferroic properties of Nb doped BiFeO3

Radojković, Aleksandar; Luković Golić, Danijela; Ćirković, Jovana; Pajić, Damir; Torić, Filip; Dapčevć, Aleksandra; Branković, Zorica; Branković, Goran

(2017)

TY  - CONF
AU  - Radojković, Aleksandar
AU  - Luković Golić, Danijela
AU  - Ćirković, Jovana
AU  - Pajić, Damir
AU  - Torić, Filip
AU  - Dapčevć, Aleksandra
AU  - Branković, Zorica
AU  - Branković, Goran
PY  - 2017
UR  - http://rimsi.imsi.bg.ac.rs/handle/123456789/2340
AB  - Pure BiFeO3 (TN = 370 °C and TC = 826–845 °C) exhibits poor ferroelectric (high electrical conductivity) and weak ferromagnetism. In this study, up to 1% Nb5+ was introduced to replace Fe3+ (B-site doping) since it could disturb the nearly antiparallel spin ordering of the adjacent Fe3+ ions responsible for cycloidal (spiral) spin structure. On the other hand, the pentivalent Nb cations will compensate the negatively charged defects and consequently reduce the electrical conductivity.
Unlike pure BiFeO3, the sample with 1% Nb exhibits hard magnetic behaviour due to its high coercive magnetic field of ~7460 Oe (at H = 50 000 Oe). The ferroelectric response for the sample with 0.2 % Nb was unstable above 
40 kV/cm, while at 70 kV/cm only the sample with 1 % Nb showed a regular ferroelectric response with remnant electrical polarization of 0.5 μC/cm2 and coercive electrical field of 22.2 kV/cm. Thus, by doping with Nb, both magnetic and ferroelectric properties of BiFeO3 were improved.
C3  - Solid-State Science & Research Meeting
T1  - Improved multiferroic properties of Nb doped BiFeO3
UR  - https://hdl.handle.net/21.15107/rcub_rimsi_2340
ER  - 
@conference{
author = "Radojković, Aleksandar and Luković Golić, Danijela and Ćirković, Jovana and Pajić, Damir and Torić, Filip and Dapčevć, Aleksandra and Branković, Zorica and Branković, Goran",
year = "2017",
abstract = "Pure BiFeO3 (TN = 370 °C and TC = 826–845 °C) exhibits poor ferroelectric (high electrical conductivity) and weak ferromagnetism. In this study, up to 1% Nb5+ was introduced to replace Fe3+ (B-site doping) since it could disturb the nearly antiparallel spin ordering of the adjacent Fe3+ ions responsible for cycloidal (spiral) spin structure. On the other hand, the pentivalent Nb cations will compensate the negatively charged defects and consequently reduce the electrical conductivity.
Unlike pure BiFeO3, the sample with 1% Nb exhibits hard magnetic behaviour due to its high coercive magnetic field of ~7460 Oe (at H = 50 000 Oe). The ferroelectric response for the sample with 0.2 % Nb was unstable above 
40 kV/cm, while at 70 kV/cm only the sample with 1 % Nb showed a regular ferroelectric response with remnant electrical polarization of 0.5 μC/cm2 and coercive electrical field of 22.2 kV/cm. Thus, by doping with Nb, both magnetic and ferroelectric properties of BiFeO3 were improved.",
journal = "Solid-State Science & Research Meeting",
title = "Improved multiferroic properties of Nb doped BiFeO3",
url = "https://hdl.handle.net/21.15107/rcub_rimsi_2340"
}
Radojković, A., Luković Golić, D., Ćirković, J., Pajić, D., Torić, F., Dapčevć, A., Branković, Z.,& Branković, G.. (2017). Improved multiferroic properties of Nb doped BiFeO3. in Solid-State Science & Research Meeting.
https://hdl.handle.net/21.15107/rcub_rimsi_2340
Radojković A, Luković Golić D, Ćirković J, Pajić D, Torić F, Dapčevć A, Branković Z, Branković G. Improved multiferroic properties of Nb doped BiFeO3. in Solid-State Science & Research Meeting. 2017;.
https://hdl.handle.net/21.15107/rcub_rimsi_2340 .
Radojković, Aleksandar, Luković Golić, Danijela, Ćirković, Jovana, Pajić, Damir, Torić, Filip, Dapčevć, Aleksandra, Branković, Zorica, Branković, Goran, "Improved multiferroic properties of Nb doped BiFeO3" in Solid-State Science & Research Meeting (2017),
https://hdl.handle.net/21.15107/rcub_rimsi_2340 .

Tm(III)-doped d-Bi2O3 for solid - oxide fuel cells

Dapčevć, Aleksandra; Dejan, Poleti; Rogan, Jelena; Radojković, Aleksandar

(Univerzitet u Beogradu, Tehnološko-metalurški fakultet, 2013)

TY  - CONF
AU  - Dapčevć, Aleksandra
AU  - Dejan, Poleti
AU  - Rogan, Jelena
AU  - Radojković, Aleksandar
PY  - 2013
UR  - http://rimsi.imsi.bg.ac.rs/handle/123456789/2890
AB  - The oxide ion conductors have widely been investigated because of their application in many
devices with high economical and ecological interests, such as solid oxide fuel cells (SOFC).
-Bi2O3
 polymorph possesses the highest known O2–
 ion conductivity, which is one to two
orders of magnitude higher than that of stabilized zirconia at corresponding temperatures [1].
At the moment, the application of this high-temperature polymorph as an electrolyte in SOFC
requires temperatures above 730 °C. However, the doping allows -Bi2O3
 stabilization to room
temperature and opens the possibility for construction of SOFC that will operate at
intermediate temperatures (ca. 350 °C) [2].
As it is found that some lanthanides are suitable dopants [3], the possibility to stabilize O2–
 ion
conductors related to the -Bi2O3
 polymorph in the Bi2O3–Tm2O3
 system was investigated. Two
starting mixtures with compositions (Bi1–xTmx
)2O3
 (x = 0.04 and 0.20) were homogenized in an
agate mortar, heat treated at 750 °C for 3 h and then slowly furnace cooled. The samples were
characterized by XRPD, DTA and SEI techniques.
Based on XRPD, the single-phase tetragonal β-Bi2O3
 was identified in the sample with x = 0.04.
Its unit cell parameters, a = 7.742(2) and c = 5.650(2) Å, well-correspond to those of undoped
β-Bi2O3
 [4]. On the other hand, the cubic -Bi2O3
 phase was obtained in the sample with
x = 0.20. Its unit cell parameter was greater than the value reported for Tm-doped -Bi2O3
sample with x = 0.25 [3] (5.5033(9) vs. 5.478 Å). Both values are smaller than reported for
undoped -Bi2O3
 [4]. This means that the unit cell parameter of cubic -Bi2O3
 decreases as
Tm-content increases and it is in accordance with Tm3+ and Bi3+ ionic radii [5].
For the sample with x = 0.04, cyclic DTA curves showed one reversible β-Bi2O3 ↔ -Bi2O3
transition with corresponding temperatures: on heating, 660 °C, and, on cooling, 600 °C.
Surprisingly, no phase transitions were observed in the sample with x = 0.20 which indicates
that the obtained -Bi2O3
 is stable within the whole investigated interval, i.e., from room
temperature to 1000 °C.
Electrochemical impedance of -Bi2O3
 phase was measured in the following temperature
range: 300 – 800 °C. At higher temperatures (600 – 800 °C) the conductivities are similar
(0.11 – 0.32 S cm
–1
), but with lowering temperature they rapidly decrease, and amount, for
example, 2.1·10–5
 S cm–1
at 300 °C. As a consequence, two activation energies are found:
0.45(4) eV (600 – 800 °C), and 1.33(2) eV (300 – 600 °C).
References:
[1] P. Shuk, H.-D. Wiemhöfer, U. Guth, W. Göpel, M. Greenblatt, Solid State Ionics 89 (1996) 179
[2] E. D. Wachsman, K.T. Lee, Science 334 (2011) 935
[3] H. T. Cahen, T. G. M. Van Den Belt, J. H. W. De Wit, G. H. J. Broers, Solid State Ionics 1 (1980) 411
[4] H. A. Harwig, Z. anorg. allg. Chem. 444 (1978) 151
[5] R. D. Shannon, Acta Cryst. A 32 (1976) 751
PB  - Univerzitet u Beogradu, Tehnološko-metalurški fakultet
C3  - 8 th International Conference of the Chemical Societies of the South-East European Countries
T1  - Tm(III)-doped d-Bi2O3 for solid - oxide fuel cells
SP  - 188
UR  - https://hdl.handle.net/21.15107/rcub_rimsi_2890
ER  - 
@conference{
author = "Dapčevć, Aleksandra and Dejan, Poleti and Rogan, Jelena and Radojković, Aleksandar",
year = "2013",
abstract = "The oxide ion conductors have widely been investigated because of their application in many
devices with high economical and ecological interests, such as solid oxide fuel cells (SOFC).
-Bi2O3
 polymorph possesses the highest known O2–
 ion conductivity, which is one to two
orders of magnitude higher than that of stabilized zirconia at corresponding temperatures [1].
At the moment, the application of this high-temperature polymorph as an electrolyte in SOFC
requires temperatures above 730 °C. However, the doping allows -Bi2O3
 stabilization to room
temperature and opens the possibility for construction of SOFC that will operate at
intermediate temperatures (ca. 350 °C) [2].
As it is found that some lanthanides are suitable dopants [3], the possibility to stabilize O2–
 ion
conductors related to the -Bi2O3
 polymorph in the Bi2O3–Tm2O3
 system was investigated. Two
starting mixtures with compositions (Bi1–xTmx
)2O3
 (x = 0.04 and 0.20) were homogenized in an
agate mortar, heat treated at 750 °C for 3 h and then slowly furnace cooled. The samples were
characterized by XRPD, DTA and SEI techniques.
Based on XRPD, the single-phase tetragonal β-Bi2O3
 was identified in the sample with x = 0.04.
Its unit cell parameters, a = 7.742(2) and c = 5.650(2) Å, well-correspond to those of undoped
β-Bi2O3
 [4]. On the other hand, the cubic -Bi2O3
 phase was obtained in the sample with
x = 0.20. Its unit cell parameter was greater than the value reported for Tm-doped -Bi2O3
sample with x = 0.25 [3] (5.5033(9) vs. 5.478 Å). Both values are smaller than reported for
undoped -Bi2O3
 [4]. This means that the unit cell parameter of cubic -Bi2O3
 decreases as
Tm-content increases and it is in accordance with Tm3+ and Bi3+ ionic radii [5].
For the sample with x = 0.04, cyclic DTA curves showed one reversible β-Bi2O3 ↔ -Bi2O3
transition with corresponding temperatures: on heating, 660 °C, and, on cooling, 600 °C.
Surprisingly, no phase transitions were observed in the sample with x = 0.20 which indicates
that the obtained -Bi2O3
 is stable within the whole investigated interval, i.e., from room
temperature to 1000 °C.
Electrochemical impedance of -Bi2O3
 phase was measured in the following temperature
range: 300 – 800 °C. At higher temperatures (600 – 800 °C) the conductivities are similar
(0.11 – 0.32 S cm
–1
), but with lowering temperature they rapidly decrease, and amount, for
example, 2.1·10–5
 S cm–1
at 300 °C. As a consequence, two activation energies are found:
0.45(4) eV (600 – 800 °C), and 1.33(2) eV (300 – 600 °C).
References:
[1] P. Shuk, H.-D. Wiemhöfer, U. Guth, W. Göpel, M. Greenblatt, Solid State Ionics 89 (1996) 179
[2] E. D. Wachsman, K.T. Lee, Science 334 (2011) 935
[3] H. T. Cahen, T. G. M. Van Den Belt, J. H. W. De Wit, G. H. J. Broers, Solid State Ionics 1 (1980) 411
[4] H. A. Harwig, Z. anorg. allg. Chem. 444 (1978) 151
[5] R. D. Shannon, Acta Cryst. A 32 (1976) 751",
publisher = "Univerzitet u Beogradu, Tehnološko-metalurški fakultet",
journal = "8 th International Conference of the Chemical Societies of the South-East European Countries",
title = "Tm(III)-doped d-Bi2O3 for solid - oxide fuel cells",
pages = "188",
url = "https://hdl.handle.net/21.15107/rcub_rimsi_2890"
}
Dapčevć, A., Dejan, P., Rogan, J.,& Radojković, A.. (2013). Tm(III)-doped d-Bi2O3 for solid - oxide fuel cells. in 8 th International Conference of the Chemical Societies of the South-East European Countries
Univerzitet u Beogradu, Tehnološko-metalurški fakultet., 188.
https://hdl.handle.net/21.15107/rcub_rimsi_2890
Dapčevć A, Dejan P, Rogan J, Radojković A. Tm(III)-doped d-Bi2O3 for solid - oxide fuel cells. in 8 th International Conference of the Chemical Societies of the South-East European Countries. 2013;:188.
https://hdl.handle.net/21.15107/rcub_rimsi_2890 .
Dapčevć, Aleksandra, Dejan, Poleti, Rogan, Jelena, Radojković, Aleksandar, "Tm(III)-doped d-Bi2O3 for solid - oxide fuel cells" in 8 th International Conference of the Chemical Societies of the South-East European Countries (2013):188,
https://hdl.handle.net/21.15107/rcub_rimsi_2890 .