Rogan, Jelena

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  • Rogan, Jelena (2)
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Author's Bibliography

Synthesis, Structure, Morphology and Properties of Biphasic ZnO–ZnMn2O4

Radovanovic, Lidija; Vulic, Predrag; Radovanovic, Zeljko; Balanč, Bojana; Simović, Bojana; zekovic, ivana; Dramićanin, Miroslav; Rogan, Jelena; Zekovic, Ivana

(Serbian Academy of Sciences and Arts, Belgrade, 2018)

TY  - CONF
AU  - Radovanovic, Lidija
AU  - Vulic, Predrag
AU  - Radovanovic, Zeljko
AU  - Balanč, Bojana
AU  - Simović, Bojana
AU  - zekovic, ivana
AU  - Dramićanin, Miroslav
AU  - Rogan, Jelena
AU  - Zekovic, Ivana
PY  - 2018
UR  - http://rimsi.imsi.bg.ac.rs/handle/123456789/2090
AB  - Transition metal oxides are important materials that have found many applications,
as capacitors, sensors or in energy storage [1]. Synthesis of these compounds
has been realized by various methods, such as hydro(solvo)thermal synthesis,
precipitation, microwave synthesis or sol-gel synthesis [2]. Recently, the thermolysis
of coordination compounds as precursors has been considered as a new approach in
obtaining functional nanosized materials. [3]. In this way, by selecting the proper
precursor, it is possible to control the phase composition, morphology and particle
size of a resulting material [3].
The biphasic powder composed of ZnO (zincite) and ZnMn2O4 (hetaerolite), (I) has been
obtained by thermolysis of bimetallic complex [MnZn2(dipya)3(tpht)3(H2O)4]·2H2O
(dipya = 2,2’-dipyridylamine, tpht = dianion of 1,4-benzenedicarboxylic acid) at
450 °C during 1 h in air atmosphere. Scanning Electron Microscopy (SEM) was
used to investigate the morphology of I (Figure 1). It can be observed that the
morphology consists of deformed spherical grains of ZnO with an average diameter
of 67 nm and elliptical grains of hetaerolite whose average diameter and length
were 156 and 290 nm, respectively. The X-ray powder diffraction (XRPD) was
applied to investigate the structure of I. In Figure 2 two-phase Rietveld refinement

Electron Microscopy of Nanostructures ELMINA 2018, August 27-29, 2018

172
pattern of I is presented (ZnO to ZnMn2O4 phase-ratio of 62:38 wt. %). The main
crystallographic data and Rietveld refinement parameters for ZnO phase are:
hexagonal, space group P63mc, a = 3.2574(1), c = 5.2175(2) Å, V = 47.945(3) Å3
; for
ZnMn2O4 phase are: tetragonal, space group I41/amd, a = 5.7299(3), c = 9.3000(8) Å,
V = 305.34(3) Å3

; Rwp = 4.80 %, Rp = 3.82 %, Rexp = 3.80 % and χ2

= 1.5960. UV-
Vis-NIR absorption spectrum was measured in order to investigate the direct band

gap (Eg) of I. Due to the existence of two phases in I, two different Eg values of
2.4 and 3.3 eV for ZnMn2O4 and ZnO phase, respectively, were determined using
Kubelka-Munk function. The mean size, polydispersity index (PDI) and zeta
potential of spherical grains were measured using Zetasizer Nano Series, Nano ZS.
The mean size was 418.6±53.1 nm while PDI value was found to be 0.354±0.099.
Relatively high values of PDI and low apostate value of zeta potential (–6.55 mV)
are indications of incipient instability of colloidal dispersion of I, probably due to the
formation of agglomerates [4, 5]. Photoluminescence measurements were carried
out at room temperature on Fluorolog-3 Model FL3-221 spectrofluorimeter system
upon excitation at 350 nm, in order to study the optical properties of I. This analysis
revealed one band centred at 422 nm in the blue region of the visible part of the
spectrum, which can possibly be associated with defects in the crystal structure of
the ZnO phase [6].
References:
[1] C Yuan et al, Angewandte Chemie International Edition 53 (2014), 1488.
[2] CNR Rao and B Raveau in “Transition Metal Oxides: Structure, Properties, and
Synthesis of Ceramic Oxides” 2nd edition (WILEY-VCH, New York).
[3] MY Masoomi and A Morsali, Coordination Chemistry Reviews 256 (2012),
2921.
[4] R Greenwood and K Kendall, Journal of the European Ceramic Society 19
(1999), 479.
[5] M Staiger et al, Journal of Dispersion Science and Technology 23 (2002), 619.
[6] H Zeng et al, Advanced Functional Materials 20 (2010), 561.
[7] The authors acknowledge funding from the Ministry of Education, Science and
Technological Development of the Republic of Serbia, Grant Number III45007.
PB  - Serbian Academy of Sciences and Arts, Belgrade
C3  - First International Conference of electron microscopy of nanostructures (ELMINA 2018)
T1  - Synthesis, Structure, Morphology and Properties of Biphasic ZnO–ZnMn2O4
EP  - 173
SP  - 171
UR  - https://hdl.handle.net/21.15107/rcub_rimsi_2090
ER  - 
@conference{
author = "Radovanovic, Lidija and Vulic, Predrag and Radovanovic, Zeljko and Balanč, Bojana and Simović, Bojana and zekovic, ivana and Dramićanin, Miroslav and Rogan, Jelena and Zekovic, Ivana",
year = "2018",
abstract = "Transition metal oxides are important materials that have found many applications,
as capacitors, sensors or in energy storage [1]. Synthesis of these compounds
has been realized by various methods, such as hydro(solvo)thermal synthesis,
precipitation, microwave synthesis or sol-gel synthesis [2]. Recently, the thermolysis
of coordination compounds as precursors has been considered as a new approach in
obtaining functional nanosized materials. [3]. In this way, by selecting the proper
precursor, it is possible to control the phase composition, morphology and particle
size of a resulting material [3].
The biphasic powder composed of ZnO (zincite) and ZnMn2O4 (hetaerolite), (I) has been
obtained by thermolysis of bimetallic complex [MnZn2(dipya)3(tpht)3(H2O)4]·2H2O
(dipya = 2,2’-dipyridylamine, tpht = dianion of 1,4-benzenedicarboxylic acid) at
450 °C during 1 h in air atmosphere. Scanning Electron Microscopy (SEM) was
used to investigate the morphology of I (Figure 1). It can be observed that the
morphology consists of deformed spherical grains of ZnO with an average diameter
of 67 nm and elliptical grains of hetaerolite whose average diameter and length
were 156 and 290 nm, respectively. The X-ray powder diffraction (XRPD) was
applied to investigate the structure of I. In Figure 2 two-phase Rietveld refinement

Electron Microscopy of Nanostructures ELMINA 2018, August 27-29, 2018

172
pattern of I is presented (ZnO to ZnMn2O4 phase-ratio of 62:38 wt. %). The main
crystallographic data and Rietveld refinement parameters for ZnO phase are:
hexagonal, space group P63mc, a = 3.2574(1), c = 5.2175(2) Å, V = 47.945(3) Å3
; for
ZnMn2O4 phase are: tetragonal, space group I41/amd, a = 5.7299(3), c = 9.3000(8) Å,
V = 305.34(3) Å3

; Rwp = 4.80 %, Rp = 3.82 %, Rexp = 3.80 % and χ2

= 1.5960. UV-
Vis-NIR absorption spectrum was measured in order to investigate the direct band

gap (Eg) of I. Due to the existence of two phases in I, two different Eg values of
2.4 and 3.3 eV for ZnMn2O4 and ZnO phase, respectively, were determined using
Kubelka-Munk function. The mean size, polydispersity index (PDI) and zeta
potential of spherical grains were measured using Zetasizer Nano Series, Nano ZS.
The mean size was 418.6±53.1 nm while PDI value was found to be 0.354±0.099.
Relatively high values of PDI and low apostate value of zeta potential (–6.55 mV)
are indications of incipient instability of colloidal dispersion of I, probably due to the
formation of agglomerates [4, 5]. Photoluminescence measurements were carried
out at room temperature on Fluorolog-3 Model FL3-221 spectrofluorimeter system
upon excitation at 350 nm, in order to study the optical properties of I. This analysis
revealed one band centred at 422 nm in the blue region of the visible part of the
spectrum, which can possibly be associated with defects in the crystal structure of
the ZnO phase [6].
References:
[1] C Yuan et al, Angewandte Chemie International Edition 53 (2014), 1488.
[2] CNR Rao and B Raveau in “Transition Metal Oxides: Structure, Properties, and
Synthesis of Ceramic Oxides” 2nd edition (WILEY-VCH, New York).
[3] MY Masoomi and A Morsali, Coordination Chemistry Reviews 256 (2012),
2921.
[4] R Greenwood and K Kendall, Journal of the European Ceramic Society 19
(1999), 479.
[5] M Staiger et al, Journal of Dispersion Science and Technology 23 (2002), 619.
[6] H Zeng et al, Advanced Functional Materials 20 (2010), 561.
[7] The authors acknowledge funding from the Ministry of Education, Science and
Technological Development of the Republic of Serbia, Grant Number III45007.",
publisher = "Serbian Academy of Sciences and Arts, Belgrade",
journal = "First International Conference of electron microscopy of nanostructures (ELMINA 2018)",
title = "Synthesis, Structure, Morphology and Properties of Biphasic ZnO–ZnMn2O4",
pages = "173-171",
url = "https://hdl.handle.net/21.15107/rcub_rimsi_2090"
}
Radovanovic, L., Vulic, P., Radovanovic, Z., Balanč, B., Simović, B., zekovic, i., Dramićanin, M., Rogan, J.,& Zekovic, I.. (2018). Synthesis, Structure, Morphology and Properties of Biphasic ZnO–ZnMn2O4. in First International Conference of electron microscopy of nanostructures (ELMINA 2018)
Serbian Academy of Sciences and Arts, Belgrade., 171-173.
https://hdl.handle.net/21.15107/rcub_rimsi_2090
Radovanovic L, Vulic P, Radovanovic Z, Balanč B, Simović B, zekovic I, Dramićanin M, Rogan J, Zekovic I. Synthesis, Structure, Morphology and Properties of Biphasic ZnO–ZnMn2O4. in First International Conference of electron microscopy of nanostructures (ELMINA 2018). 2018;:171-173.
https://hdl.handle.net/21.15107/rcub_rimsi_2090 .
Radovanovic, Lidija, Vulic, Predrag, Radovanovic, Zeljko, Balanč, Bojana, Simović, Bojana, zekovic, ivana, Dramićanin, Miroslav, Rogan, Jelena, Zekovic, Ivana, "Synthesis, Structure, Morphology and Properties of Biphasic ZnO–ZnMn2O4" in First International Conference of electron microscopy of nanostructures (ELMINA 2018) (2018):171-173,
https://hdl.handle.net/21.15107/rcub_rimsi_2090 .

HIGHLY CONDUCTIVE LANTHANOIDE STABILIZED δ-Bi2O3 PHASES

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

(Društvo za keramičke materijale Srbije, 2015)

TY  - CONF
AU  - Dapčevć, Aleksandra
AU  - Dejan, Poleti
AU  - Rogan, Jelena
AU  - Radojković, Aleksandar
AU  - Branković, Goran
PY  - 2015
UR  - http://rimsi.imsi.bg.ac.rs/handle/123456789/2831
AB  - Due to the increasing demands for new highly efficient and environmentally
friendly energy conversion technologies, the oxide ion conductors applicable in
solid oxide fuel cells (SOFCs) have widely been investigated. The aim is to find a
suitable electrolyte with the ionic conductivity high enough at intermediate
temperatures in order to reduce the operating temperature of SOFCs. The high
temperature δ-Bi2O3 phase has been proposed as a good candidate for electrolyte in
SOFCs because it is the fastest known ionic conductor.
In this study, the possibility to stabilize O
2–
ion conductors related to the -Bi2O3
polymorph in Bi2O3–Tm2O3 and Bi2O3–Lu2O3 systems was investigated. Six starting
mixtures with the following compositions (Bi1–xTmx)2O3, x = 0.11, 0.14 and 0.20,
and (Bi1–yLuy)2O3, y = 0.15, 0.20 and 0.25, were dry homogenized in an agate
mortar, heat treated at 750 °C for 3 h and then slowly furnace cooled. The samples
were characterized by XRD, TEM/SAED, SEM, DTA and SEI techniques.
Based on XRD and TEM/SAED, the targeted cubic δ-Bi2O3 single-phase
samples (space group
Fm3m
) were successfully obtained within all six systems. The
unit cell parameter of both Tm- and Lu-doped -Bi2O3 decreases as dopant content
increases. By comparing Tm- and Lu-doped δ-Bi2O3 phases mutually, an expected
increase of the unit cell parameters with larger ionic radii of dopant was found
[ri(Tm3+) = 0.88 Å, and ri(Lu3+) = 0.86 Å in the octahedral environment1
].
Electrochemical impedance of -Bi2O3 phases was measured between 300 and
800 °C. At temperatures 550 – 800 °C the conductivities are of the same order of
magnitude (0.1 – 0.4 S cm
–1
), but with lowering temperature they rapidly decrease
resulting in two activation energies. This is due to the changes in conductivity
mechanism which will be discussed.According to the cyclic DTA curves, no phase
transitions were observed in the following samples: (Bi0.8Tm0.2)2O3, (Bi0.8Lu0.2)2O3
and (Bi0.75Lu0.25)2O3, indicating that these -Bi2O3 phases are stable within the
whole investigated interval, i.e., from room temperature to 985 °C. This means that
the application of these electrolyte materials could result not only in the significant
enhancement of IT-SOFC electrochemical performance, but also in their good
structural stability over long time service in a wide temperature range.
1. R. D. Shannon, Acta Cryst. A, 32 (1976) 751
PB  - Društvo za keramičke materijale Srbije
C3  - 3rd Conference of the Serbian Society for Ceramic Materials
T1  - HIGHLY CONDUCTIVE LANTHANOIDE STABILIZED δ-Bi2O3 PHASES
SP  - 63
UR  - https://hdl.handle.net/21.15107/rcub_rimsi_2831
ER  - 
@conference{
author = "Dapčevć, Aleksandra and Dejan, Poleti and Rogan, Jelena and Radojković, Aleksandar and Branković, Goran",
year = "2015",
abstract = "Due to the increasing demands for new highly efficient and environmentally
friendly energy conversion technologies, the oxide ion conductors applicable in
solid oxide fuel cells (SOFCs) have widely been investigated. The aim is to find a
suitable electrolyte with the ionic conductivity high enough at intermediate
temperatures in order to reduce the operating temperature of SOFCs. The high
temperature δ-Bi2O3 phase has been proposed as a good candidate for electrolyte in
SOFCs because it is the fastest known ionic conductor.
In this study, the possibility to stabilize O
2–
ion conductors related to the -Bi2O3
polymorph in Bi2O3–Tm2O3 and Bi2O3–Lu2O3 systems was investigated. Six starting
mixtures with the following compositions (Bi1–xTmx)2O3, x = 0.11, 0.14 and 0.20,
and (Bi1–yLuy)2O3, y = 0.15, 0.20 and 0.25, were dry homogenized in an agate
mortar, heat treated at 750 °C for 3 h and then slowly furnace cooled. The samples
were characterized by XRD, TEM/SAED, SEM, DTA and SEI techniques.
Based on XRD and TEM/SAED, the targeted cubic δ-Bi2O3 single-phase
samples (space group
Fm3m
) were successfully obtained within all six systems. The
unit cell parameter of both Tm- and Lu-doped -Bi2O3 decreases as dopant content
increases. By comparing Tm- and Lu-doped δ-Bi2O3 phases mutually, an expected
increase of the unit cell parameters with larger ionic radii of dopant was found
[ri(Tm3+) = 0.88 Å, and ri(Lu3+) = 0.86 Å in the octahedral environment1
].
Electrochemical impedance of -Bi2O3 phases was measured between 300 and
800 °C. At temperatures 550 – 800 °C the conductivities are of the same order of
magnitude (0.1 – 0.4 S cm
–1
), but with lowering temperature they rapidly decrease
resulting in two activation energies. This is due to the changes in conductivity
mechanism which will be discussed.According to the cyclic DTA curves, no phase
transitions were observed in the following samples: (Bi0.8Tm0.2)2O3, (Bi0.8Lu0.2)2O3
and (Bi0.75Lu0.25)2O3, indicating that these -Bi2O3 phases are stable within the
whole investigated interval, i.e., from room temperature to 985 °C. This means that
the application of these electrolyte materials could result not only in the significant
enhancement of IT-SOFC electrochemical performance, but also in their good
structural stability over long time service in a wide temperature range.
1. R. D. Shannon, Acta Cryst. A, 32 (1976) 751",
publisher = "Društvo za keramičke materijale Srbije",
journal = "3rd Conference of the Serbian Society for Ceramic Materials",
title = "HIGHLY CONDUCTIVE LANTHANOIDE STABILIZED δ-Bi2O3 PHASES",
pages = "63",
url = "https://hdl.handle.net/21.15107/rcub_rimsi_2831"
}
Dapčevć, A., Dejan, P., Rogan, J., Radojković, A.,& Branković, G.. (2015). HIGHLY CONDUCTIVE LANTHANOIDE STABILIZED δ-Bi2O3 PHASES. in 3rd Conference of the Serbian Society for Ceramic Materials
Društvo za keramičke materijale Srbije., 63.
https://hdl.handle.net/21.15107/rcub_rimsi_2831
Dapčevć A, Dejan P, Rogan J, Radojković A, Branković G. HIGHLY CONDUCTIVE LANTHANOIDE STABILIZED δ-Bi2O3 PHASES. in 3rd Conference of the Serbian Society for Ceramic Materials. 2015;:63.
https://hdl.handle.net/21.15107/rcub_rimsi_2831 .
Dapčevć, Aleksandra, Dejan, Poleti, Rogan, Jelena, Radojković, Aleksandar, Branković, Goran, "HIGHLY CONDUCTIVE LANTHANOIDE STABILIZED δ-Bi2O3 PHASES" in 3rd Conference of the Serbian Society for Ceramic Materials (2015):63,
https://hdl.handle.net/21.15107/rcub_rimsi_2831 .