Markéta Jarošová
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Markéta Jarošová has a total of 166 co-authors. Here are the top co-authors by number of shared publications:
- Mariana Klementová
Department of Material Analysis, FZU—Institute of Physics of the Czech Academy of Sciences, Na Slovance 2, 18200 Prague, Czech Republic
4 shared publications - Michal Dušek
Institute of Physics of the Czech Academy of Sciences , Na Slovance 2
3 shared publications - Alexander Kromka
Institute of Physics of the Czech Academy of Sciences Prague Czech Republic
2 shared publications - Farzaneh Mahmoudi
Department of Chemistry, University of Miami, Coral Gables, FL 33146, USA
2 shared publications - Hanna Sopha
Center of Materials and Nanotechnologies, Faculty of Chemical Technology, University of Pardubice, Nam. Cs. Legii 565, 53002 Pardubice, Czech Republic
2 shared publications Jan Drahokoupil
2 shared publications
Latest Publications
- Open Access
- 11 March 2026
- Published by Elsevier in Ceramics International
- Vol. 52 (12) , 20693-20701
Dielectric, magnetic and lattice dynamics properties of double perovskite (Ca0.5Mn1.5)MnWO6
- 11 March 2026
- Published by Elsevier in Ceramics International
- Vol. 52 (12) , 20693-20701
Open AccessDielectric, magnetic and lattice dynamics properties of double perovskite (Ca0.5Mn1.5)MnWO6
- Open Access
- 2 September 2025
- Published by Mineralogical Society in Mineralogical Magazine
- Vol. 90 (1) , 164-175
Extending the mineralogy of U 6+ (IV): Uranyl phosphate sheet of novel topology in the crystal structure of ranunculite
Ranunculite is a rare supergene hydrated aluminium uranyl phosphate reliably reported only from the type locality – the Kobokobo pegmatite in the Sud-Kivu province, Democratic Republic of Congo; its structure has remained unknown until now. Based on 3D electron diffraction data, ranunculite is monoclinic, with a C -centred unit cell: a = 11.1812(7) Å, b = 17.9281(5) Å, c = 17.91548(16) Å, β = 98.350(4)°, and V = 3553.2(2) Å 3 ( Z = 4). The structure ( C 2/ c ) was refined kinematically to R 1 = 0.4114 for 1697 unique observed reflections. The structure of ranunculite is based upon infinite uranyl-phosphate sheets of novel topology. The two-dimensional representation of the structural unit consists of hexagons (occupied by U 6+ ), pentagons (occupied by U 6+ ), squares (occupied by Al 3+ ) and triangles (occupied by P 5+ ). Those sheets are stacked perpendicular to c ; the interplanar distance is ~9.5 Å. They result from the clusters of edge-sharing uranyl hexagonal and pentagonal bipyramids linked by Al-octahedra and PO 4 tetrahedra. The decoration of the sheets is unique but somewhat resembles the arrangement (of U-clusters, squares and triangles) observed in bijvoetite and lepersonnite topologies; the ring symbol is 6 1 5 1 4 2 3 2 . In the interlayer, there are two Al 3+ -hosting sites (one [6]- and [5]-coordinated; the pyramidal one is only partially occupied), as well as isolated H 2 O groups. There is an extensive network of hydrogen bonds; adjacent sheets are either held by hydrogen bonds only or by tetramers of Al-polyhedra when occupied (through shared O19). This arrangement most probably causes a poor crystallinity of ranunculite (which gives rise to stacking faults observed in the powder diffraction data).
- 2 September 2025
- Published by Mineralogical Society in Mineralogical Magazine
- Vol. 90 (1) , 164-175
Open AccessExtending the mineralogy of U 6+ (IV): Uranyl phosphate sheet of novel topology in the crystal structure of ranunculite
Ranunculite is a rare supergene hydrated aluminium uranyl phosphate reliably reported only from the type locality – the Kobokobo pegmatite in the Sud-Kivu province, Democratic Republic of Congo; its structure has remained unknown until now. Based on 3D electron diffraction data, ranunculite is monoclinic, with a C -centred unit cell: a = 11.1812(7) Å, b = 17.9281(5) Å, c = 17.91548(16) Å, β = 98.350(4)°, and V = 3553.2(2) Å 3 ( Z = 4). The structure ( C 2/ c ) was refined kinematically to R 1 = 0.4114 for 1697 unique observed reflections. The structure of ranunculite is based upon infinite uranyl-phosphate sheets of novel topology. The two-dimensional representation of the structural unit consists of hexagons (occupied by U 6+ ), pentagons (occupied by U 6+ ), squares (occupied by Al 3+ ) and triangles (occupied by P 5+ ). Those sheets are stacked perpendicular to c ; the interplanar distance is ~9.5 Å. They result from the clusters of edge-sharing uranyl hexagonal and pentagonal bipyramids linked by Al-octahedra and PO 4 tetrahedra. The decoration of the sheets is unique but somewhat resembles the arrangement (of U-clusters, squares and triangles) observed in bijvoetite and lepersonnite topologies; the ring symbol is 6 1 5 1 4 2 3 2 . In the interlayer, there are two Al 3+ -hosting sites (one [6]- and [5]-coordinated; the pyramidal one is only partially occupied), as well as isolated H 2 O groups. There is an extensive network of hydrogen bonds; adjacent sheets are either held by hydrogen bonds only or by tetramers of Al-polyhedra when occupied (through shared O19). This arrangement most probably causes a poor crystallinity of ranunculite (which gives rise to stacking faults observed in the powder diffraction data).
- 3 June 2025
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 9 (6)
Single-crystalline CrSb(0001) thin films grown by dc magnetron co-sputtering
- 3 June 2025
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 9 (6)
Single-crystalline CrSb(0001) thin films grown by dc magnetron co-sputtering
- Open Access
- 16 April 2024
- Published by Elsevier in Journal of Materials Research and Technology
- Vol. 30, 4248-4260
The role of the preparation route on microstructure and mechanical properties of AlCoCrFeNi high entropy alloy
- 16 April 2024
- Published by Elsevier in Journal of Materials Research and Technology
- Vol. 30, 4248-4260
Open AccessThe role of the preparation route on microstructure and mechanical properties of AlCoCrFeNi high entropy alloy
- Open Access
- 20 October 2023
- Published by Elsevier in Journal of Molecular Liquids
- Vol. 391
Effect of temperature on memory effect in nematic phase of liquid crystal and their composites with aerosil and geothite nanoparticles
- 20 October 2023
- Published by Elsevier in Journal of Molecular Liquids
- Vol. 391
Open AccessEffect of temperature on memory effect in nematic phase of liquid crystal and their composites with aerosil and geothite nanoparticles
- Open Access
- 18 July 2022
- Published by MDPI AG in Nanomaterials
- Vol. 12 (14) , 2463
Role of Magnetic Nanoparticles Size and Concentration on Structural Changes and Corresponding Magneto-Optical Behavior of Nematic Liquid Crystals
The effect of magnetic nanoparticles size and concentration on nematic liquid crystal (NLC) behavior in a magnetic field was investigated. The magneto-optical investigation using measurements of the light transmission through the liquid crystal was used to study the structural changes induced by an applied weak magnetic field. Magnetic nanoparticles Fe3O4 of spherical shape with different size and volume concentration were added to NLC 4-cyano-40 -hexylbiphenyl (6CB) during its isotropic phase. In contrast to undoped liquid crystals, the distinctive different light transmission responses induced by a magnetic field in studied NLC samples were observed suggesting both structural changes and the orientational coupling between magnetic moments of nanoparticles and the director of the NLC. Experimental measurements were conducted, including investigation under linearly increasing and/or jumped magnetic field, respectively, as well as the investigation of time influence on structural changes to study their stability and switching time. The analysis of observed light transmission characteristics confirmed the role of concentration and size of magnetic nanoparticles on the resultant behavior of investigated NLC compounds. The obtained results showed the lowering of the threshold magnetic field with an increase in the volume concentration of nanoparticles and on the important role of nanoparticles size on stability and switching properties. Obtained results are discussed within the context of previous ones.
- 18 July 2022
- Published by MDPI AG in Nanomaterials
- Vol. 12 (14) , 2463
Open AccessRole of Magnetic Nanoparticles Size and Concentration on Structural Changes and Corresponding Magneto-Optical Behavior of Nematic Liquid Crystals
The effect of magnetic nanoparticles size and concentration on nematic liquid crystal (NLC) behavior in a magnetic field was investigated. The magneto-optical investigation using measurements of the light transmission through the liquid crystal was used to study the structural changes induced by an applied weak magnetic field. Magnetic nanoparticles Fe3O4 of spherical shape with different size and volume concentration were added to NLC 4-cyano-40 -hexylbiphenyl (6CB) during its isotropic phase. In contrast to undoped liquid crystals, the distinctive different light transmission responses induced by a magnetic field in studied NLC samples were observed suggesting both structural changes and the orientational coupling between magnetic moments of nanoparticles and the director of the NLC. Experimental measurements were conducted, including investigation under linearly increasing and/or jumped magnetic field, respectively, as well as the investigation of time influence on structural changes to study their stability and switching time. The analysis of observed light transmission characteristics confirmed the role of concentration and size of magnetic nanoparticles on the resultant behavior of investigated NLC compounds. The obtained results showed the lowering of the threshold magnetic field with an increase in the volume concentration of nanoparticles and on the important role of nanoparticles size on stability and switching properties. Obtained results are discussed within the context of previous ones.
- Open Access
Texture of the Freshwater Shells from the Unionidae Family Collected in the Czech Republic Investigated by X-ray and Neutron Diffraction
Bivalve shells exhibit extreme mechanical resistance despite using a minimal amount of material. The shells thus represent an inspiration and a source of information for environmental, geological, and engineering sciences. In this study, two species of freshwater shells from the Unionidae family, collected in the Czech Luznice River, were investigated with respect to their crystallographic preferred orientation by means of X-ray and neutron diffraction. The observed texture was found to be of a strongly uniaxial type, with the strength increasing along the shell growth direction. The c-axis of aragonite does not change during growth and its alignment remains perpendicular to the outer surface of the shell
Open AccessTexture of the Freshwater Shells from the Unionidae Family Collected in the Czech Republic Investigated by X-ray and Neutron Diffraction
Bivalve shells exhibit extreme mechanical resistance despite using a minimal amount of material. The shells thus represent an inspiration and a source of information for environmental, geological, and engineering sciences. In this study, two species of freshwater shells from the Unionidae family, collected in the Czech Luznice River, were investigated with respect to their crystallographic preferred orientation by means of X-ray and neutron diffraction. The observed texture was found to be of a strongly uniaxial type, with the strength increasing along the shell growth direction. The c-axis of aragonite does not change during growth and its alignment remains perpendicular to the outer surface of the shell
- 1 March 2021
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 5 (3) , 035401
Anomalous Nernst effect in the ceramic and thin film samples of perovskiteWe report the anomalous Nernst effect (ANE) in large-grain ceramics, nanogranular ceramics, and nanogranular thin films of , measured over the temperature range 5–300 K. The study is complemented with thermopower, resistivity, and magnetic measurements. The temperature-dependent ANE below the Curie temperature (240–250 K) is analyzed with the help of longitudinal resistivity and Seebeck using a previously proposed formula derived by a combination of Onsager reciprocity, the Mott formula, and the relation between transverse and longitudinal resistivity, . We observe a characteristic exponent n ∼ 0.4 in agreement with the universal scaling for the bad-metal-type conduction regime. The nanogranular samples are characterized by higher resistivity, lower saturated magnetization, and a higher coercive field compared to large-grain ceramics. On the other hand, the magnitude of the ANE is independent of grain size. This observation likely insinuates that the characteristic length scale characterizing the ANE in is below the grain size of nanogranular samples ∼40 nm. Therefore, the ANE associated with the bad-metal regime is independent of barriers associated with grain surface, which are responsible for activated resistivity and lowered magnetization due to a magnetically “dead” layer. The observation that the advantage of the higher coercive field of nanogranular samples is not deteriorated by a lower ANE is important for possible applications in zero magnetic field.- 1 March 2021
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 5 (3) , 035401
Anomalous Nernst effect in the ceramic and thin film samples of perovskiteWe report the anomalous Nernst effect (ANE) in large-grain ceramics, nanogranular ceramics, and nanogranular thin films of , measured over the temperature range 5–300 K. The study is complemented with thermopower, resistivity, and magnetic measurements. The temperature-dependent ANE below the Curie temperature (240–250 K) is analyzed with the help of longitudinal resistivity and Seebeck using a previously proposed formula derived by a combination of Onsager reciprocity, the Mott formula, and the relation between transverse and longitudinal resistivity, . We observe a characteristic exponent n ∼ 0.4 in agreement with the universal scaling for the bad-metal-type conduction regime. The nanogranular samples are characterized by higher resistivity, lower saturated magnetization, and a higher coercive field compared to large-grain ceramics. On the other hand, the magnitude of the ANE is independent of grain size. This observation likely insinuates that the characteristic length scale characterizing the ANE in is below the grain size of nanogranular samples ∼40 nm. Therefore, the ANE associated with the bad-metal regime is independent of barriers associated with grain surface, which are responsible for activated resistivity and lowered magnetization due to a magnetically “dead” layer. The observation that the advantage of the higher coercive field of nanogranular samples is not deteriorated by a lower ANE is important for possible applications in zero magnetic field.- 1 March 2020
- Published by Elsevier in Polyhedron
- Vol. 179
Li-ion battery studies on nickel oxide nanoparticles prepared by facile route calcination
- 1 March 2020
- Published by Elsevier in Polyhedron
- Vol. 179
Li-ion battery studies on nickel oxide nanoparticles prepared by facile route calcination
- 1 November 2019
- Published by Elsevier in Journal of Alloys and Compounds
- Vol. 811
Thermoelectric properties and stability of Tl-doped SnS
- 1 November 2019
- Published by Elsevier in Journal of Alloys and Compounds
- Vol. 811
Thermoelectric properties and stability of Tl-doped SnS