PMID-sentid Pub_year Sent_text compound_name comp_offset prot_official_name organism prot_offset 30889555-2 2019 Here, the peculiar electric transport behavior of the 2DEG formed at the LGO/STO oxide interface is studied under the application of light pulses of different amplitude, duration, and repetition rate, and by varying the sample temperature from 8 to 300 K. The experimental results evidence a persistent photoconductivity, intimately related to the complex physics of this system. 2deg 54-58 nuclear receptor binding SET domain protein 1 Homo sapiens 77-80 32786931-4 2020 Remarkably, the pure spin polarization of the 2DEG can be created and annihilated by polarizing and depolarizing the ferroelectrics, and can be switched (between pure spin-up and pure spin-down) by flipping the ferroelectric polarization. 2deg 46-50 spindlin 1 Homo sapiens 21-25 32786931-4 2020 Remarkably, the pure spin polarization of the 2DEG can be created and annihilated by polarizing and depolarizing the ferroelectrics, and can be switched (between pure spin-up and pure spin-down) by flipping the ferroelectric polarization. 2deg 46-50 spindlin 1 Homo sapiens 167-171 32786931-4 2020 Remarkably, the pure spin polarization of the 2DEG can be created and annihilated by polarizing and depolarizing the ferroelectrics, and can be switched (between pure spin-up and pure spin-down) by flipping the ferroelectric polarization. 2deg 46-50 spindlin 1 Homo sapiens 167-171 26562134-1 2016 The two-dimensional electron gas (2DEG) formed at the n-type (LaO)(+1)/(TiO2)(0) interface in the polar/nonpolar LaAlO3/SrTiO3 (LAO/STO) heterostructure (HS) has emerged as a prominent research area because of its great potential for nanoelectronic applications. 2deg 34-38 interleukin 4 induced 1 Homo sapiens 62-65 30858519-11 2019 The spin polarization increases with decreasing 2DEG density, suggesting that Coulomb interactions are a key aspect of the symmetry breaking. 2deg 48-52 spindlin 1 Homo sapiens 4-8 30250812-4 2018 The experimental realization of 2DEG at an InGaN/InN heterointerface grown by molecular beam epitaxy is reported here. 2deg 32-36 growth hormone releasing hormone Homo sapiens 49-52 30250812-7 2018 The experimental observations of 2DEG at the InGaN/InN heterointerface have paved the way for fabricating higher-speed transistors based on an InN channel. 2deg 33-37 growth hormone releasing hormone Homo sapiens 51-54 30250812-7 2018 The experimental observations of 2DEG at the InGaN/InN heterointerface have paved the way for fabricating higher-speed transistors based on an InN channel. 2deg 33-37 growth hormone releasing hormone Homo sapiens 143-146 29472630-4 2018 We prove that the resulting spin-flip wave dispersion is the same as in a magnetized 2DEG without spin-orbit coupling, apart from a shift by the spin-helix wave vector. 2deg 85-89 spindlin 1 Homo sapiens 28-32 29472630-4 2018 We prove that the resulting spin-flip wave dispersion is the same as in a magnetized 2DEG without spin-orbit coupling, apart from a shift by the spin-helix wave vector. 2deg 85-89 spindlin 1 Homo sapiens 98-102 29472630-4 2018 We prove that the resulting spin-flip wave dispersion is the same as in a magnetized 2DEG without spin-orbit coupling, apart from a shift by the spin-helix wave vector. 2deg 85-89 spindlin 1 Homo sapiens 98-102 29226675-5 2018 Compared with the bare LAO/STO interface, the 2DEG density at the LAO/STO interface is enhanced or depressed by the PZTdown or PZTup overlayer, respectively. 2deg 46-50 interleukin 4 induced 1 Homo sapiens 23-26 29226675-5 2018 Compared with the bare LAO/STO interface, the 2DEG density at the LAO/STO interface is enhanced or depressed by the PZTdown or PZTup overlayer, respectively. 2deg 46-50 nuclear receptor binding SET domain protein 1 Homo sapiens 27-30 29226675-5 2018 Compared with the bare LAO/STO interface, the 2DEG density at the LAO/STO interface is enhanced or depressed by the PZTdown or PZTup overlayer, respectively. 2deg 46-50 interleukin 4 induced 1 Homo sapiens 66-69 29226675-5 2018 Compared with the bare LAO/STO interface, the 2DEG density at the LAO/STO interface is enhanced or depressed by the PZTdown or PZTup overlayer, respectively. 2deg 46-50 nuclear receptor binding SET domain protein 1 Homo sapiens 70-73 29323182-3 2018 We then studied the electronic characteristics of two-dimensional electron gas (2DEG) produced at the LaO/TiO2 interface in the LaAlO3/BaTiO3 superlattices via spin-polarized density functional theory calculations. 2deg 80-84 interleukin 4 induced 1 Homo sapiens 102-105 29112444-1 2017 The two-dimensional electron gas (2DEG) formed at the interface between SrTiO3 (STO) and LaAlO3 (LAO) insulating layer is supposed to possess strong Rashba spin-orbit coupling. 2deg 34-38 spindlin 1 Homo sapiens 156-160 29112444-2 2017 To date, the inverse Edelstein effect (i.e., spin-to-charge conversion) in the 2DEG layer is reported. 2deg 79-83 spindlin 1 Homo sapiens 45-49 29141404-4 2017 It is demonstrated that the photoinduced inverse spin Hall effect (PISHE) of the top SSs and the 2DEG can be separated based on their opposite signs. 2deg 97-101 spindlin 1 Homo sapiens 49-53 28968124-7 2017 The great tunability of GAO/STO interface by EDLT gating not only shows promise for design of oxide devices with on-demand properties but also sheds new light on the electronic structure of 2DEG at the nonisostructural spinel/perovskite interface. 2deg 190-194 nuclear receptor binding SET domain protein 1 Homo sapiens 24-31 27708415-5 2016 In particular, the Ta-based compounds can form 2DEG with potentially high electron mobility at (TaO2)+/(SrO)0 interface. 2deg 47-51 TAO kinase 2 Homo sapiens 96-100 26959195-1 2016 Since the discovery of two-dimensional electron gas (2DEG) at the oxide interface of LaAlO3/SrTiO3 (LAO/STO), improving carrier mobility has become an important issue for device applications. 2deg 53-57 nuclear receptor binding SET domain protein 1 Homo sapiens 104-107 26959195-3 2016 Moreover, two critical thicknesses for the LSAT/STO (001) interface are found, one at 5 unit cells for appearance of the 2DEG and the other at 12 unit cells for a peak in the carrier mobility. 2deg 121-125 nuclear receptor binding SET domain protein 1 Homo sapiens 48-51 26562134-1 2016 The two-dimensional electron gas (2DEG) formed at the n-type (LaO)(+1)/(TiO2)(0) interface in the polar/nonpolar LaAlO3/SrTiO3 (LAO/STO) heterostructure (HS) has emerged as a prominent research area because of its great potential for nanoelectronic applications. 2deg 34-38 interleukin 4 induced 1 Homo sapiens 128-131 26562134-4 2016 Herein, we studied Nb and Ta-doping effects on the energetics, electronic structure, interfacial charge carrier density, magnetic moment, and the charge confinements of the 2DEG at the n-type (LaO)(+1)/(TiO2)(0) interface of LAO/STO HS using first-principles density functional theory calculations. 2deg 173-177 interleukin 4 induced 1 Homo sapiens 193-196 28191417-3 2016 To create 2DEG at LAO/STO interface, regardless of growing temperature from 25 to 700 C, we found that environment with oxygen deficient during the deposition of LAO overlayer is essentially required. 2deg 10-14 interleukin 4 induced 1 Homo sapiens 18-21 28191417-3 2016 To create 2DEG at LAO/STO interface, regardless of growing temperature from 25 to 700 C, we found that environment with oxygen deficient during the deposition of LAO overlayer is essentially required. 2deg 10-14 interleukin 4 induced 1 Homo sapiens 163-166 28191417-5 2016 2DEG at a-LAO/STO interface is depleted upon ex situ annealing at 300 C under 300 Torr of oxygen pressure, while that in c-LAO/STO interface is still maintained. 2deg 0-4 interleukin 4 induced 1 Homo sapiens 10-13 28191417-6 2016 Our result suggests that the LAO overlayer crystallinity critically affects the thermal-annealing-induced depletion of 2DEG at a-LAO/STO interface rather than the generation of 2DEG. 2deg 119-123 interleukin 4 induced 1 Homo sapiens 29-32 28191417-6 2016 Our result suggests that the LAO overlayer crystallinity critically affects the thermal-annealing-induced depletion of 2DEG at a-LAO/STO interface rather than the generation of 2DEG. 2deg 119-123 interleukin 4 induced 1 Homo sapiens 129-132 28191417-6 2016 Our result suggests that the LAO overlayer crystallinity critically affects the thermal-annealing-induced depletion of 2DEG at a-LAO/STO interface rather than the generation of 2DEG. 2deg 177-181 interleukin 4 induced 1 Homo sapiens 29-32 28191417-7 2016 We clearly provide that amorphous TiOx can efficiently prevent the thermal degradation of 2DEG at the a-LAO/STO interface, which gives a cornerstone for achieving thermal-stable 2DEG at a-LAO/STO interface. 2deg 90-94 interleukin 4 induced 1 Homo sapiens 104-107 28191417-7 2016 We clearly provide that amorphous TiOx can efficiently prevent the thermal degradation of 2DEG at the a-LAO/STO interface, which gives a cornerstone for achieving thermal-stable 2DEG at a-LAO/STO interface. 2deg 90-94 interleukin 4 induced 1 Homo sapiens 188-191 28191417-7 2016 We clearly provide that amorphous TiOx can efficiently prevent the thermal degradation of 2DEG at the a-LAO/STO interface, which gives a cornerstone for achieving thermal-stable 2DEG at a-LAO/STO interface. 2deg 178-182 interleukin 4 induced 1 Homo sapiens 188-191 34553900-3 2021 Herein, a strong photoresponse of the 2DEG in a Pt/LAO/STO heterostructure is achieved by adopting a vertical tunneling configuration. 2deg 38-42 interleukin 4 induced 1 Homo sapiens 51-54 25688656-4 2015 Herein, we investigated the doping effects of LaTiO3(LTO) layers on the electronic properties of 2DEG at n-type (LaO)(+1)/(TiO2)(0) interface in the LAO/STO HS using spin-polarized density functional theory calculations. 2deg 97-101 interleukin 4 induced 1 Homo sapiens 113-116 25688656-4 2015 Herein, we investigated the doping effects of LaTiO3(LTO) layers on the electronic properties of 2DEG at n-type (LaO)(+1)/(TiO2)(0) interface in the LAO/STO HS using spin-polarized density functional theory calculations. 2deg 97-101 interleukin 4 induced 1 Homo sapiens 149-152 22369762-0 2012 Thermionic emission from the 2DEG assisted by image-charge-induced barrier lowering in AlInN/AlN/GaN heterostructures. 2deg 29-33 gigaxonin Homo sapiens 97-100 22369762-3 2012 This model suggests that current transport is controlled by thermionic emission (TE) of the two-dimensional electron gas (2DEG) across the potential barrier at the heterointerface, where the image charges generated by the 2DEG induce a barrier lowering at the Al(1-x)In(x)N/GaN interface, enhancing electron transport. 2deg 122-126 gigaxonin Homo sapiens 274-277 22369762-3 2012 This model suggests that current transport is controlled by thermionic emission (TE) of the two-dimensional electron gas (2DEG) across the potential barrier at the heterointerface, where the image charges generated by the 2DEG induce a barrier lowering at the Al(1-x)In(x)N/GaN interface, enhancing electron transport. 2deg 222-226 gigaxonin Homo sapiens 274-277 20981022-4 2010 Here, we demonstrate room-temperature conductivity switching of 2DEG nanowires formed at atomically sharp LaAlO(3)/SrTiO(3) (LAO/STO) heterointerfaces grown directly on (001) Silicon (Si) substrates. 2deg 64-68 interleukin 4 induced 1 Homo sapiens 125-128 34669088-10 2021 This paper for the first time presents the comprehensive TCAD study of surface donor and analysis of electron concentration in the channel and 2DEG formation at AlGaN-GaN interface. 2deg 143-147 gigaxonin Homo sapiens 167-170 34553900-4 2021 The tunneling of the 2DEG through an ultrathin LAO layer is significantly enhanced by UV light irradiation, showing a maximum photoresponsivity of ~1.11 x 107%. 2deg 21-25 interleukin 4 induced 1 Homo sapiens 47-50 33908251-7 2021 Therefore, the utilization of a 2DEG layer in transferrable AlGaN/GaN heterostructure membranes offers great promises for high performance flexible 2DEG-IPDs for advanced UV detection systems that are critically important in myriad biomedical and environmental applications. 2deg 32-36 gigaxonin Homo sapiens 62-65 33908251-7 2021 Therefore, the utilization of a 2DEG layer in transferrable AlGaN/GaN heterostructure membranes offers great promises for high performance flexible 2DEG-IPDs for advanced UV detection systems that are critically important in myriad biomedical and environmental applications. 2deg 148-152 gigaxonin Homo sapiens 62-65 34029001-3 2021 It is shown that the polar field-assisted VO formation at the LAO/STO surface plays critical roles in the 2DEG formation and concurrent structural transition. 2deg 106-110 interleukin 4 induced 1 Homo sapiens 62-65 34029001-4 2021 Comprehensive scanning transmission electron microscopy analyses, in conjunction with density functional theory calculations, demonstrate that VO forming at the LAO/STO surface above the critical thickness (tc ) cancels the polar field by doping the interface with 2DEG. 2deg 265-269 interleukin 4 induced 1 Homo sapiens 161-164 33883134-2 2021 We show that AFD and FE modes are cooperatively coupled in LAO/STO (111) heterostructures; they coexist below the critical thickness (t c) and disappear simultaneously above t c with the formation of 2DEG. 2deg 200-204 interleukin 4 induced 1 Homo sapiens 59-62 33883134-3 2021 Electron energy-loss spectroscopy and density functional theory (DFT) calculations provide direct evidence of oxygen vacancy (V O) formation at the LAO (111) surface, which acts as the source of 2DEG. 2deg 195-199 interleukin 4 induced 1 Homo sapiens 148-151