Daria Belotcerkovtceva
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
Research Subjects
Daria Belotcerkovtceva has a total of 48 co-authors. Here are the top co-authors by number of shared publications:
- Mutta Venkata Kamalakar
Uppsala University
5 shared publications - Alexey I. Berdyugin
National University of Singapore
2 shared publications - Chin Shen Ong
Uppsala University
2 shared publications - Danny Thonig
Uppsala University
2 shared publications - Henry Nameirakpam
Department of Physics and Astronomy, Uppsala University, Box 516, Uppsala SE-751 20, Sweden
2 shared publications Iakov Reznikov
National University of Singapore
2 shared publications
Latest Publications
- 22 October 2026
- Published by American Chemical Society (ACS) in ACS Nano
- Vol. 20 (43) , 28964-28972
Displacement-Field-Induced Ionization of Defect States in High-Quality hBN
Encapsulation of two-dimensional (2D) materials with hexagonal boron nitride (hBN) is widely used to fabricate ultraclean van der Waals (vdW) heterostructures for optoelectronic and quantum transport studies. These devices are often operated under strong out-of-plane displacement fields that tune the electronic properties of the active 2D material, while the surrounding hBN is typically assumed to remain electronically inert. This assumption, however, neglects defect states that are present even in high-quality hBN crystals. Here, we probe their response to the applied displacement field using monolayer graphene encapsulated between hBN crystals as a sensitive charge sensor. Increasing the displacement field induces notable charge transfer between graphene and hBN, producing additional electron doping of ≈10–20 × 109 cm–2 even at the moderate displacement field (∼0.5 V nm–1), while simultaneously increasing carrier-density inhomogeneity of the graphene layer. Both effects are consistent with ionization of defect states within the hBN bandgap, with the bulk density ∼1–7 × 10–5 nm–3 varying across different hBN crystals. Our results show that displacement-field-induced defect ionization in hBN can modify the electronic response of vdW heterostructures, with direct implications for device design and interpretation of experiments.
- 22 October 2026
- Published by American Chemical Society (ACS) in ACS Nano
- Vol. 20 (43) , 28964-28972
Displacement-Field-Induced Ionization of Defect States in High-Quality hBN
Encapsulation of two-dimensional (2D) materials with hexagonal boron nitride (hBN) is widely used to fabricate ultraclean van der Waals (vdW) heterostructures for optoelectronic and quantum transport studies. These devices are often operated under strong out-of-plane displacement fields that tune the electronic properties of the active 2D material, while the surrounding hBN is typically assumed to remain electronically inert. This assumption, however, neglects defect states that are present even in high-quality hBN crystals. Here, we probe their response to the applied displacement field using monolayer graphene encapsulated between hBN crystals as a sensitive charge sensor. Increasing the displacement field induces notable charge transfer between graphene and hBN, producing additional electron doping of ≈10–20 × 109 cm–2 even at the moderate displacement field (∼0.5 V nm–1), while simultaneously increasing carrier-density inhomogeneity of the graphene layer. Both effects are consistent with ionization of defect states within the hBN bandgap, with the bulk density ∼1–7 × 10–5 nm–3 varying across different hBN crystals. Our results show that displacement-field-induced defect ionization in hBN can modify the electronic response of vdW heterostructures, with direct implications for device design and interpretation of experiments.
- 1 July 2026
- Published by Springer Nature in Nature Materials
- Vol. 25 (11) , 2019-2027
Quantum tunnelling and leakage current across two-dimensional materials
Leakage current is a physical phenomenon that critically affects the operation and reliability of mainstream electronic devices and heterostructures for diverse applications. Two-dimensional materials are being integrated into the structure of ultrascaled electronic devices, but the leakage current across them is still not well understood. Here we analyse the leakage current across hexagonal boron nitride (hBN), molybdenum disulfide and tungsten disulfide of different thicknesses, and compare it with industrial-quality SiO2/n++Si samples. The samples are analysed at the nanoscale and at the device level, and the experimental data are complemented with computational modelling assisted by technology computer-aided design and density functional theory. First, we demonstrate that the surface roughness of the bottom electrode dramatically alters the leakage current when an electric field is applied. Second, we show that in multilayer two-dimensional materials, the energy bandgap and density of atomic defects are key factors that determine the leakage current; however, in monolayer two-dimensional materials, the leakage current is mainly determined by sample thickness, understood as the electrode-to-electrode distance. Consequently, leakage current across monolayer hBN is higher than that across monolayer molybdenum disulfide and tungsten disulfide despite hBN having a bandgap nearly three times larger, due to its approximately 50% lower thickness. Third, we establish an equivalence (in terms of leakage current) between hBN and SiO2 films of different thicknesses, which can be used to predict the performance and reliability of two-dimensional-material-based nano-electronic devices, such as transistors and memristors.
- 1 July 2026
- Published by Springer Nature in Nature Materials
- Vol. 25 (11) , 2019-2027
Quantum tunnelling and leakage current across two-dimensional materials
Leakage current is a physical phenomenon that critically affects the operation and reliability of mainstream electronic devices and heterostructures for diverse applications. Two-dimensional materials are being integrated into the structure of ultrascaled electronic devices, but the leakage current across them is still not well understood. Here we analyse the leakage current across hexagonal boron nitride (hBN), molybdenum disulfide and tungsten disulfide of different thicknesses, and compare it with industrial-quality SiO2/n++Si samples. The samples are analysed at the nanoscale and at the device level, and the experimental data are complemented with computational modelling assisted by technology computer-aided design and density functional theory. First, we demonstrate that the surface roughness of the bottom electrode dramatically alters the leakage current when an electric field is applied. Second, we show that in multilayer two-dimensional materials, the energy bandgap and density of atomic defects are key factors that determine the leakage current; however, in monolayer two-dimensional materials, the leakage current is mainly determined by sample thickness, understood as the electrode-to-electrode distance. Consequently, leakage current across monolayer hBN is higher than that across monolayer molybdenum disulfide and tungsten disulfide despite hBN having a bandgap nearly three times larger, due to its approximately 50% lower thickness. Third, we establish an equivalence (in terms of leakage current) between hBN and SiO2 films of different thicknesses, which can be used to predict the performance and reliability of two-dimensional-material-based nano-electronic devices, such as transistors and memristors.
- 27 December 2023
- Published by Royal Society of Chemistry (RSC) in Nanoscale Horizons
- Vol. 9 (3) , 456-464
High current treated-passivated graphene (CTPG) towards stable nanoelectronic and spintronic circuits
High current-treated AlOx passivated-graphene (CTPG) with enhanced carrier mobility offers promise for stability and scalability in graphene nanoelectronic and spintronic devices.
- 27 December 2023
- Published by Royal Society of Chemistry (RSC) in Nanoscale Horizons
- Vol. 9 (3) , 456-464
High current treated-passivated graphene (CTPG) towards stable nanoelectronic and spintronic circuits
High current-treated AlOx passivated-graphene (CTPG) with enhanced carrier mobility offers promise for stability and scalability in graphene nanoelectronic and spintronic devices.
- Open Access
- 13 November 2023
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 5 (4) , 043147
Resistive switching in graphene: A theoretical case study on the alumina-graphene interface
Neuromorphic computing mimics the brain's architecture to create energy-efficient devices. Reconfigurable synapses are crucial for neuromorphic computing, which can be achieved through memory-resistive (memristive) switching. Graphene-based memristors have shown nonvolatile multibit resistive switching with desirable endurance. Through first-principles calculations, we study the structural and electronic properties of graphene in contact with an ultra-thin alumina overlayer and demonstrate how one can use charge doping to exert direct control over its interfacial covalency, reversibly switching between states of conductivity and resistivity in the graphene layer. We further show that this proposed mechanism can be stabilized through the -type doping of graphene, e.g., by naturally occurring defects, the passivation of dangling bonds or defect engineering.- 13 November 2023
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 5 (4) , 043147
Open AccessResistive switching in graphene: A theoretical case study on the alumina-graphene interface
Neuromorphic computing mimics the brain's architecture to create energy-efficient devices. Reconfigurable synapses are crucial for neuromorphic computing, which can be achieved through memory-resistive (memristive) switching. Graphene-based memristors have shown nonvolatile multibit resistive switching with desirable endurance. Through first-principles calculations, we study the structural and electronic properties of graphene in contact with an ultra-thin alumina overlayer and demonstrate how one can use charge doping to exert direct control over its interfacial covalency, reversibly switching between states of conductivity and resistivity in the graphene layer. We further show that this proposed mechanism can be stabilized through the -type doping of graphene, e.g., by naturally occurring defects, the passivation of dangling bonds or defect engineering. - Open Access
sp$^{2}$/sp$^{3}$ bonding controlling mechanism at the $α$-Al$_{2}$O$_{3}|$graphene interface
First-principles calculations reported here illuminate the effects of the interfacial properties of $\alpha$-Al$_{2}$O$_{3}$ and graphene, with emphasis on the structural and electronic properties. Various contact interfaces and different $\alpha$-Al$_{2}$O$_{3}$ surface terminations are considered with on and slightly-off stoichiometric aluminium oxide. We show that depending on whether aluminium or oxygen is in contact with graphene, an $sp^{3}$ structural deformation and spontaneous spin-polarization may occur next to the interface contact. Interestingly, some cases cause a $p$-type doping in the graphene band structure, depending on the initial $\alpha$-Al$_{2}$O$_{3}$ geometry placed on graphene. The importance of leaving the surface dangling bonds of alumina saturated or not is also highlighted, and we show that it might be a control mechanism for opening a gap in graphene by the influence of the $sp^{3}$ bond between oxygen and carbon atoms at the interface. We discuss the potential of utilizing this sensitivity for practical applications.Open Accesssp$^{2}$/sp$^{3}$ bonding controlling mechanism at the $α$-Al$_{2}$O$_{3}|$graphene interface
First-principles calculations reported here illuminate the effects of the interfacial properties of $\alpha$-Al$_{2}$O$_{3}$ and graphene, with emphasis on the structural and electronic properties. Various contact interfaces and different $\alpha$-Al$_{2}$O$_{3}$ surface terminations are considered with on and slightly-off stoichiometric aluminium oxide. We show that depending on whether aluminium or oxygen is in contact with graphene, an $sp^{3}$ structural deformation and spontaneous spin-polarization may occur next to the interface contact. Interestingly, some cases cause a $p$-type doping in the graphene band structure, depending on the initial $\alpha$-Al$_{2}$O$_{3}$ geometry placed on graphene. The importance of leaving the surface dangling bonds of alumina saturated or not is also highlighted, and we show that it might be a control mechanism for opening a gap in graphene by the influence of the $sp^{3}$ bond between oxygen and carbon atoms at the interface. We discuss the potential of utilizing this sensitivity for practical applications. - Open Access
- 25 August 2021
- Published by Royal Society of Chemistry (RSC) in Nanoscale Advances
- Vol. 3 (19) , 5656-5662
Highly-efficient growth of cobalt nanostructures using focused ion beam induced deposition under cryogenic conditions: application to electrical contacts on graphene, magnetism and hard masking
Emergent technologies are required in the field of nanoelectronics for improved contacts and interconnects at nano and micro-scale. In this work, we report a highly-efficient nanolithography process for the growth of cobalt nanostructures requiring an ultra-low charge dose (15 μC cm−2, unprecedented in single-step charge-based nanopatterning). This resist-free process consists in the condensation of a ∼28 nm-thick Co2(CO)8 layer on a substrate held at −100 °C, its irradiation with a Ga+ focused ion beam, and substrate heating up to room temperature. The resulting cobalt-based deposits exhibit sub-100 nm lateral resolution, display metallic behaviour (room-temperature resistivity of 200 μΩ cm), present ferromagnetic properties (magnetization at room temperature of 400 emu cm−3) and can be grown in large areas. To put these results in perspective, similar properties can be achieved by room-temperature focused ion beam induced deposition and the same precursor only if a 2 × 103 times higher charge dose is used. We demonstrate the application of such an ultra-fast growth process to directly create electrical contacts onto graphene ribbons, opening the route for a broad application of this technology to any 2D material. In addition, the application of these cryo-deposits for hard masking is demonstrated, confirming its structural functionality.
- 25 August 2021
- Published by Royal Society of Chemistry (RSC) in Nanoscale Advances
- Vol. 3 (19) , 5656-5662
Open AccessHighly-efficient growth of cobalt nanostructures using focused ion beam induced deposition under cryogenic conditions: application to electrical contacts on graphene, magnetism and hard masking
Emergent technologies are required in the field of nanoelectronics for improved contacts and interconnects at nano and micro-scale. In this work, we report a highly-efficient nanolithography process for the growth of cobalt nanostructures requiring an ultra-low charge dose (15 μC cm−2, unprecedented in single-step charge-based nanopatterning). This resist-free process consists in the condensation of a ∼28 nm-thick Co2(CO)8 layer on a substrate held at −100 °C, its irradiation with a Ga+ focused ion beam, and substrate heating up to room temperature. The resulting cobalt-based deposits exhibit sub-100 nm lateral resolution, display metallic behaviour (room-temperature resistivity of 200 μΩ cm), present ferromagnetic properties (magnetization at room temperature of 400 emu cm−3) and can be grown in large areas. To put these results in perspective, similar properties can be achieved by room-temperature focused ion beam induced deposition and the same precursor only if a 2 × 103 times higher charge dose is used. We demonstrate the application of such an ultra-fast growth process to directly create electrical contacts onto graphene ribbons, opening the route for a broad application of this technology to any 2D material. In addition, the application of these cryo-deposits for hard masking is demonstrated, confirming its structural functionality.