0000000000004860

AUTHOR

Raffaella Lo Nigro

showing 7 related works from this author

Metal/Semiconductor Barrier Properties of Non-Recessed Ti/Al/Ti and Ta/Al/Ta Ohmic Contacts on AlGaN/GaN Heterostructures

2019

This paper compares the metal/semiconductor barrier height properties of non-recessed Ti/Al/Ti and Ta/Al/Ta contacts on AlGaN/GaN heterostructures. Both contacts exhibited a rectifying behavior after deposition and after annealing at temperatures up to 550 &deg

Control and OptimizationMaterials scienceAnnealing (metallurgy)Analytical chemistryEnergy Engineering and Power Technology02 engineering and technologylcsh:Technology01 natural sciencesCondensed Matter::Materials ScienceAlGaN/GaNTa/Al/TaTi/Al/Ti0103 physical sciencesElectrical and Electronic EngineeringEngineering (miscellaneous)Ohmic contact010302 applied physicslcsh:TBarrier heightRenewable Energy Sustainability and the Environmentbusiness.industryContact resistanceohmic contactsHeterojunctionConductive atomic force microscopyCondensed Matter::Mesoscopic Systems and Quantum Hall Effect021001 nanoscience & nanotechnologyMicrostructureOhmic contactSemiconductor0210 nano-technologybusinessEnergy (miscellaneous)HillockEnergies
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Direct atomic layer deposition of ultrathin aluminium oxide on monolayer $MoS_2$ exfoliated on gold: the role of the substrate

2021

In this paper we demonstrated the thermal Atomic Layer Deposition (ALD) growth at 250 {\deg}C of highly homogeneous and ultra-thin ($\approx$ 3.6 nm) $Al_2O_3$ films with excellent insulating properties directly onto a monolayer (1L) $MoS_2$ membrane exfoliated on gold. Differently than in the case of 1L $MoS_2$ supported by a common insulating substrate ($Al_2O_3/Si$), a better nucleation process of the high-k film was observed on the 1L $MoS_2/Au$ system since the ALD early stages. Atomic force microscopy analyses showed a $\approx 50\%$ $Al_2O_3$ surface coverage just after 10 ALD cycles, its increasing up to $>90\%$ (after 40 cycles), and an uniform $\approx$ 3.6 nm film, after 80 cycle…

Condensed Matter - Materials Scienceatomic force microscopyPhotoluminescenceMaterials scienceAtomic force microscopyMechanical EngineeringSubstrate (chemistry)Materials Science (cond-mat.mtrl-sci)FOS: Physical sciencesPhysics - Applied PhysicsConductive atomic force microscopyApplied Physics (physics.app-ph)conductive atomic force microscopyAtomic layer depositionsymbols.namesakeChemical engineeringMechanics of Materialsatomic layer depositionRaman spectroscopyMonolayersymbolsphotoluminescenceMoS2Raman spectroscopyAluminum oxide
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Graphene‐SiO2 Interaction from Composites to Doping

2019

An overview of the interaction between monolayer graphene and SiO2 dielectric substrate is reported focusing on the effect this latter has on doping and strain induced by thermal treatments in controlled atmosphere. The disentanglement of strain and doping is highlighted and the comparison with another dielectric substrate of Al2O3 evidences the critical role that the substrate has in the electronic properties of graphene. The reported results pave the way for microelectronic devices based on graphene on dielectrics and for Fermi level tuning in composites of graphene and nanoparticles.

Materials scienceStrain (chemistry)GraphenegrapheneDopingdopingSurfaces and InterfacesCondensed Matter PhysicsSurfaces Coatings and FilmsElectronic Optical and Magnetic Materialslaw.inventionstrainsilicalawgraphene dopingMaterials ChemistryElectrical and Electronic EngineeringComposite material
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Seed‐Layer‐Free Atomic Layer Deposition of Highly Uniform Al 2 O 3 Thin Films onto Monolayer Epitaxial Graphene on Silicon Carbide

2019

Atomic layer deposition (ALD) is the method of choice to obtain uniform insulating films on graphene for device applications. Owing to the lack of out-of-plane bonds in the sp(2) lattice of graphene, nucleation of ALD layers is typically promoted by functionalization treatments or predeposition of a seed layer, which, in turn, can adversely affect graphene electrical properties. Hence, ALD of dielectrics on graphene without prefunctionalization and seed layers would be highly desirable. In this work, uniform Al2O3 films are obtained by seed-layer-free thermal ALD at 250 degrees C on highly homogeneous monolayer (1L) epitaxial graphene (EG) (amp;gt;98% 1L coverage) grown on on-axis 4H-SiC(00…

SiCMaterials sciencePhysics::Opticslaw.inventionchemistry.chemical_compoundAtomic layer depositionlawLattice (order)MonolayerPhysics::Atomic and Molecular ClustersSilicon carbidePhysics::Chemical PhysicsThin filmCondensed Matter::Quantum Gasesatomic force microscopybusiness.industryAtomic force microscopyGrapheneMechanical EngineeringCondensed Matter Physicsepitaxial graphenechemistryMechanics of Materialsatomic layer depositionOptoelectronicsatomic force microscopy; atomic layer deposition; epitaxial graphene; SiCEpitaxial graphenebusinessDen kondenserade materiens fysikAdvanced Materials Interfaces
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Temperature and time dependent electron trapping in Al2O3 thin films onto AlGaN/GaN heterostructures

2022

In this article, the charge trapping phenomena in Al2O3 thin films grown by atomic layer deposition (ALD) on AlGaN/GaN heterostructures have been studied by time-dependent capacitance–voltage (C-V) measurements as a function of temperature. In particular, monitoring the transient of the capacitance enabled us to estimate the maximum depth of the insulating layer interested by the negative charge trapping effect under our bias stress conditions and to determine a charge traps density in the bulk Al2O3 in the order of 3 × 1019 cm−3. A temperature dependent C-V analysis up to 150 °C demonstrated the presence of two competitive mechanisms that rule the electron capture and emission in the Al2O3…

Capacitance transient measurementsCharge trappingAl2O3General Physics and AstronomyGallium nitrideSurfaces and InterfacesGeneral ChemistryCondensed Matter PhysicsPlasma enhanced atomic layer depositionSurfaces Coatings and FilmsApplied Surface Science
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Influence of oxide substrates on monolayer graphene doping process by thermal treatments in oxygen

2019

Abstract The structural and the electronic properties of monolayer graphene made by chemical vapor deposition and transferred on various oxide substrates ( SiO 2 , Al 2 O 3 , and HfO 2 ) are investigated by Raman Spectroscopy and Atomic Force Microscopy in order to highlight the influence of the substrate on the features of p-doping obtained by O 2 thermal treatments. By varing the treatment temperature up to 400 °C, the distribution of the reaction sites of the substrates is evaluated. Their total concentration and the consequent highest doping available is determined and it is shown that this latter is linked to the water affinity of the substrate. Finally, by varing the exposure time to …

inorganic chemicalsMaterials scienceDiffusionOxide02 engineering and technologyChemical vapor depositiondoping010402 general chemistry01 natural sciencesGraphene Thermal doping Substrate effectslaw.inventionsymbols.namesakechemistry.chemical_compoundAdsorptionlawGeneral Materials ScienceGrapheneDopinggraphenetechnology industry and agricultureSubstrate (chemistry)General Chemistry021001 nanoscience & nanotechnology0104 chemical sciencesChemical engineeringchemistrysymbols0210 nano-technologyRaman spectroscopyhigh-k dielectrics
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Modification of the sheet resistance under Ti/Al/Ni/Au Ohmic contacts on AlGaN/GaN heterostructures

2018

This paper reports on the modification of the sheet resistance under Ti/Al/Ni/Au Ohmic contacts on AlGaN/GaN heterostructures, studied by means of Transmission Line Model (TLM) structures, morphological and structural analyses, as well as computer simulations. In particular, the contacts exhibited an Ohmic behaviour after annealing at 800 degrees C, with a specific contact resistance rho(c) = (2.4 +/- 0.2) x 10(-5) Omega cm(2), which was associated to morphological and structural changes of both the metal layer and the interface. Interestingly, TLM analyses gave a value of the sheet resistance under the contact (R-SK = 26.1 +/- 5.0 Omega/rectangle) significantly lower than that measured out…

Materials scienceAnnealing (metallurgy)Algan gan02 engineering and technology01 natural sciencesMetal0103 physical sciencesAlGaN/GaN heterostructuresGeneral Materials ScienceComposite materialOhmic contactSheet resistanceOhmic contacts010302 applied physicsbusiness.industryMechanical EngineeringContact resistanceTransmission Line ModelHeterojunction021001 nanoscience & nanotechnologyCondensed Matter PhysicsSemiconductorMechanics of Materialsvisual_artvisual_art.visual_art_mediumTi/Al/Ni/Au0210 nano-technologybusiness
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