0000000001319873

AUTHOR

Fernando Iikawa

showing 13 related works from this author

Inhomogeneous free-electron distribution in InN nanowires: Photoluminescence excitation experiments

2010

Photoluminescence excitation (PLE) spectra have been measured for a set of self-assembled InN nanowires (NWs) and a high-crystalline quality InN layer grown by molecular-beam epitaxy. The PLE experimental lineshapes have been reproduced by a self-consistent calculation of the absorption in a cylindrical InN NW. The differences in the PLE spectra can be accounted for the inhomogeneous electron distribution within the NWs caused by a bulk donor concentration $({N}_{D}^{+})$ and a two-dimensional density of ionized surface states $({N}_{ss}^{+})$. For NW radii larger than 30 nm, ${N}_{D}^{+}$ and ${N}_{ss}^{+}$ modify the absorption edge and the lineshape, respectively, and can be determined f…

Free electron modelMaterials scienceCondensed matter physics: Physics [G04] [Physical chemical mathematical & earth Sciences]02 engineering and technology021001 nanoscience & nanotechnologyCondensed Matter PhysicsEpitaxy7. Clean energy01 natural sciencesMolecular physicsSpectral lineElectronic Optical and Magnetic Materials: Physique [G04] [Physique chimie mathématiques & sciences de la terre]Absorption edgeIonization0103 physical sciencesPhotoluminescence excitationAbsorption (logic)010306 general physics0210 nano-technologySurface statesPhysical Review B
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Defect spectroscopy of single ZnO microwires

2014

The point defects of single ZnO microwires grown by carbothermal reduction were studied by microphotoluminescence, photoresistance excitation spectra, and resistance as a function of the temperature. We found the deep level defect density profile along the microwire showing that the concentration of defects decreases from the base to the tip of the microwires and this effect correlates with a band gap narrowing. The results show a characteristic deep defect levels inside the gap at 0.88 eV from the top of the VB. The resistance as a function of the temperature shows defect levels next to the bottom of the CB at 110 meV and a mean defect concentration of 4 1018 cm3 . This combination of tech…

Materials sciencePhotoluminescenceDeep levelbusiness.industryBand gapCiencias FísicasWide-bandgap semiconductorNanowireGeneral Physics and Astronomy//purl.org/becyt/ford/1.3 [https]Crystallographic defect//purl.org/becyt/ford/1 [https]NanolithographyMicrowiresZnOOptoelectronicsDefectsSpectroscopybusinessCIENCIAS NATURALES Y EXACTASSpectroscopyFísica de los Materiales Condensados
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Inhomogeneous electron distribution in InN nanowires: Influence on the optical properties

2012

In this work, we study theoretically and experimentally the influence of the surface electron accumulation on the optical properties of InN nanowires. For this purpose, the photoluminescence and photoluminescence excitation spectra have been measured for a set of self-assembled InN NWs grown under different conditions. The photoluminescence excitation experimental lineshapes have been reproduced by a self-consistent calculation of the absorption in a cylindrical InN nanowires. With the self-consistent model we can explore how the optical absorption depends on nanowires radius and doping concentration. Our model solves the Schrodinger equation for a cylindrical nanowire of infinite length, a…

010302 applied physicsElectron densityPhotoluminescenceMaterials scienceCondensed matter physicsNanowirePhysics::Optics02 engineering and technologyElectronCondensed Matter::Mesoscopic Systems and Quantum Hall Effect021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesCondensed Matter::Materials ScienceAbsorption edge0103 physical sciencesPhotoluminescence excitation0210 nano-technologyAbsorption (electromagnetic radiation)Surface statesphysica status solidi c
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Optical properties of InN nanocolumns: Electron accumulation at InN non‐polar surfaces and dependence on the growth conditions

2009

InN nanocolumns grown by plasma-assisted molecular beam epitaxy have been studied by photoluminescence (PL) and photoluminescence excitation (PLE). The PL peak energy was red-shifted with respect to the PLE onset and both energies were higher than the low temperature band-gap reported for InN. PL and PLE experiments for different excitation and detection energies indicated that the PL peaks were homogeneously broadened. This overall phenomenology has been attributed to the effects of an electron accumulation layer present atthe non-polar surfaces of the InN nanocolumns. Variations in the growth conditions modify the edge of the PLE spectra and the PL peak energies evidencing that the densit…

010302 applied physicsFree electron modelElectron densityPhotoluminescenceCondensed matter physicsAbsorption spectroscopyChemistry02 engineering and technologyElectron021001 nanoscience & nanotechnologyCondensed Matter PhysicsEpitaxy01 natural sciencesMolecular physics0103 physical sciencesPhotoluminescence excitation0210 nano-technologyMolecular beam epitaxyphysica status solidi c
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A Luminescent Thermometer Exhibiting Slow Relaxation of the Magnetization: Toward Self-Monitored Building Blocks for Next-Generation Optomagnetic Dev…

2019

The development and integration of Single-Molecule Magnets (SMMs) into molecular electronic devices continue to be an exciting challenge. In such potential devices, heat generation due to the electric current is a critical issue that has to be considered upon device fabrication. To read out accurately the temperature at the submicrometer spatial range, new multifunctional SMMs need to be developed. Herein, we present the first self-calibrated molecular thermometer with SMM properties, which provides an elegant avenue to address these issues. The employment of 2,2′-bipyrimidine and 1,1,1-trifluoroacetylacetonate ligands results in a dinuclear compound, [Dy2(bpm)(tfaa)6], which exhibits slow …

Materials sciencePhotoluminescenceZeeman effect010405 organic chemistrybusiness.industryGeneral Chemical EngineeringRelaxation (NMR)General ChemistryAtmospheric temperature range010402 general chemistry01 natural sciences7. Clean energy0104 chemical sciencesMagnetizationsymbols.namesakeChemistryThermometerMagnetHeat generationsymbolsOptoelectronicssingle-molecule magnetsbusinessQD1-999Research ArticleACS Central Science
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Valence-band splitting energies in wurtzite InP nanowires : Photoluminescence spectroscopy and ab initio calculations

2010

We investigated experimentally and theoretically the valence-band structure of wurtzite InP nanowires. The wurtzite phase, which usually is not stable for III-V phosphide compounds, has been observed in InP nanowires. We present results on the electronic properties of these nanowires using the photoluminescence excitation technique. Spectra from an ensemble of nanowires show three clear absorption edges separated by 44 meV and 143 meV, respectively. The band edges are attributed to excitonic absorptions involving three distinct valence-bands labeled: A, B, and C. Theoretical results based on “ab initio” calculation gives corresponding valence-band energy separations of 50 meV and 200 meV, r…

PhotoluminescenceMaterials scienceNanoestructuresNanowireAb initioPhysics::OpticsCondensed Matter PhysicsCondensed Matter::Mesoscopic Systems and Quantum Hall EffectSpectral lineElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceAb initio quantum chemistry methodsPhotoluminescence excitationAtomic physicsSpectroscopyWurtzite crystal structure
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Spatial carrier distribution in InP/GaAs type II quantum dots and quantum posts

2011

We performed a detailed investigation of the structural and optical properties of multi-layers of InP/GaAs quantum dots, which present a type II interface arrangement. Transmission electronic microscopy analysis has revealed relatively large dots that coalesce forming so-called quantum posts when the GaAs layer between the InP layers is thin. We observed that the structural properties and morphology affect the resulting radiative lifetime of the carriers in our systems. The carrier lifetimes are relatively long, as expected for type II systems, as compared to those observed for single layer InP/GaAs quantum dots. The interface intermixing effect has been pointed out as a limiting factor for…

Materials scienceNanostructureCondensed matter physicsbusiness.industryMechanical EngineeringBioengineeringGeneral ChemistryElectronFermionCarrier lifetimeCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter::Materials ScienceMechanics of MaterialsQuantum dotTransmission electron microscopyOptoelectronicsGeneral Materials ScienceElectrical and Electronic EngineeringWave functionbusinessQuantumNanotechnology
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Optical emission of InAs nanowires

2012

Wurtzite InAs nanowire samples grown by chemical beam epitaxy have been analyzed by photoluminescence spectroscopy. The nanowires exhibit two main optical emission bands at low temperatures. They are attributed to the recombination of carriers in quantum well structures, formed by zincblende-wurtzite alternating layers, and to the donor-acceptor pair. The blue-shift observed in the former emission band when the excitation power is increased is in good agreement with the type-II band alignment between the wurtzite and zincblende sections predicted by previous theoretical works. When increasing the temperature and the excitation power successively, an additional band attributed to the band-to…

PhotoluminescenceMaterials scienceCondensed matter physicsBand gapMechanical EngineeringNanowireBioengineeringGeneral ChemistryChemical beam epitaxyMechanics of MaterialsGeneral Materials ScienceElectrical and Electronic EngineeringSpectroscopyQuantum wellExcitationWurtzite crystal structureNanotechnology
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Polarized and resonant Raman spectroscopy on single InAs nanowires

2011

We report polarized Raman scattering and resonant Raman scattering studies on single InAs nanowires. Polarized Raman experiments show that the highest scattering intensity is obtained when both the incident and analyzed light polarizations are perpendicular to the nanowire axis. InAs wurtzite optical modes are observed. The obtained wurtzite modes are consistent with the selection rules and also with the results of calculations using an extended rigid-ion model. Additional resonant Raman scattering experiments reveal a redshifted E1 transition for InAs nanowires compared to the bulk zinc-blende InAs transition due to the dominance of the wurtzite phase in the nanowires. Ab initio calculatio…

Materials scienceScatteringCondensed Matter::OtherNanotecnologiaNanowireCiència dels materialsCondensed Matter PhysicsCondensed Matter::Mesoscopic Systems and Quantum Hall EffectMolecular physicsElectronic Optical and Magnetic MaterialsEspectroscòpia Ramansymbols.namesakeCondensed Matter::Materials ScienceX-ray Raman scatteringNuclear magnetic resonancesymbolsCoherent anti-Stokes Raman spectroscopyRaman spectroscopyElectronic band structureRaman scatteringWurtzite crystal structure
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Fermi energy dependence of the optical emission in core/shell InAs nanowire homostructures.

2017

InAs nanowires grown by vapor–liquid–solid (VLS) method are investigated by photoluminescence. We observe that the Fermi energy of all samples is reduced by ~20 meV when the size of the Au nanoparticle used for catalysis is increased from 5 to 20 nm. Additional capping with a thin InP shell enhances the optical emission and does not affect the Fermi energy. The unexpected behavior of the Fermi energy is attributed to the differences in the residual donor (likely carbon) incorporation in the axial (low) and lateral (high incorporation) growth in the VLS and vapor–solid (VS) methods, respectively. The different impurity incorporation rate in these two regions leads to a core/shell InAs homost…

PhotoluminescenceMaterials scienceCondensed matter physicsMechanical EngineeringDopingNanowireShell (structure)BioengineeringFermi energy02 engineering and technologyGeneral ChemistryCondensed Matter::Mesoscopic Systems and Quantum Hall Effect021001 nanoscience & nanotechnology01 natural sciencesCore (optical fiber)Condensed Matter::Materials ScienceMechanics of MaterialsImpurityElectric field0103 physical sciencesGeneral Materials ScienceElectrical and Electronic Engineering010306 general physics0210 nano-technologyNanotechnology
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Optical phonon modes of wurtzite InP

2013

Optical vibration modes of InP nanowires in the wurtzite phase were investigated by Raman scattering spectroscopy. The wires were grown along the [0001] axis by the vapor-liquid-solid method. The A1(TO), E2h, and E1(TO) phonon modes of the wurtzite symmetry were identified by using light linearly polarized along different directions in backscattering configuration. Additionally, forbidden longitudinal optical modes have also been observed. Furthermore, by applying an extended 11-parameter rigid-ion model, the complete dispersion relations of InP in the wurtzite phase have been calculated, showing a good agreement with the Raman experimental data.

PhysicsCondensed Matter - Materials ScienceNanoestructuresCondensed Matter - Mesoscale and Nanoscale PhysicsPhysics and Astronomy (miscellaneous)Condensed matter physicsLinear polarizationPhononPhase (waves)NanowireMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesCiència dels materialsCondensed Matter::Mesoscopic Systems and Quantum Hall EffectEspectroscòpia RamanCondensed Matter::Materials Sciencesymbols.namesakeNormal modeDispersion relationMesoscale and Nanoscale Physics (cond-mat.mes-hall)symbolsRaman spectroscopyWurtzite crystal structureApplied Physics Letters
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CCDC 1859276: Experimental Crystal Structure Determination

2019

Related Article: Dylan Errulat, Riccardo Marin, Diogo A. Gálico, Katie L. M. Harriman, Amelie Pialat, Bulat Gabidullin, Fernando Iikawa, Odilon D. D. Couto, Jani O. Moilanen, Eva Hemmer, Fernando A. Sigoli, Muralee Murugesu|2019|ACS Cent.Sci.|5|1187|doi:10.1021/acscentsci.9b00288

Space GroupCrystallographyCrystal System(mu-22'-bipyrimidine)-hexakis(111-trifluoroacetylacetonato)-di-dysprosium(iii)Crystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 1859277: Experimental Crystal Structure Determination

2019

Related Article: Dylan Errulat, Riccardo Marin, Diogo A. Gálico, Katie L. M. Harriman, Amelie Pialat, Bulat Gabidullin, Fernando Iikawa, Odilon D. D. Couto, Jani O. Moilanen, Eva Hemmer, Fernando A. Sigoli, Muralee Murugesu|2019|ACS Cent.Sci.|5|1187|doi:10.1021/acscentsci.9b00288

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameters(mu-22'-bipyrimidine)-hexakis(111-trifluoroacetylacetonato)-di-gadoliniumExperimental 3D Coordinates
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