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Dive into the research topics where I. Vurgaftman is active.

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Featured researches published by I. Vurgaftman.


Journal of Applied Physics | 2001

Band parameters for III–V compound semiconductors and their alloys

I. Vurgaftman; Jerry R. Meyer; L. R. Ram-Mohan

We present a comprehensive, up-to-date compilation of band parameters for the technologically important III–V zinc blende and wurtzite compound semiconductors: GaAs, GaSb, GaP, GaN, AlAs, AlSb, AlP, AlN, InAs, InSb, InP, and InN, along with their ternary and quaternary alloys. Based on a review of the existing literature, complete and consistent parameter sets are given for all materials. Emphasizing the quantities required for band structure calculations, we tabulate the direct and indirect energy gaps, spin-orbit, and crystal-field splittings, alloy bowing parameters, effective masses for electrons, heavy, light, and split-off holes, Luttinger parameters, interband momentum matrix elements, and deformation potentials, including temperature and alloy-composition dependences where available. Heterostructure band offsets are also given, on an absolute scale that allows any material to be aligned relative to any other.


Journal of Applied Physics | 2003

Band parameters for nitrogen-containing semiconductors

I. Vurgaftman; J. R. Meyer

We present a comprehensive and up-to-date compilation of band parameters for all of the nitrogen-containing III–V semiconductors that have been investigated to date. The two main classes are: (1) “conventional” nitrides (wurtzite and zinc-blende GaN, InN, and AlN, along with their alloys) and (2) “dilute” nitrides (zinc-blende ternaries and quaternaries in which a relatively small fraction of N is added to a host III–V material, e.g., GaAsN and GaInAsN). As in our more general review of III–V semiconductor band parameters [I. Vurgaftman et al., J. Appl. Phys. 89, 5815 (2001)], complete and consistent parameter sets are recommended on the basis of a thorough and critical review of the existing literature. We tabulate the direct and indirect energy gaps, spin-orbit and crystal-field splittings, alloy bowing parameters, electron and hole effective masses, deformation potentials, elastic constants, piezoelectric and spontaneous polarization coefficients, as well as heterostructure band offsets. Temperature an...


Applied Physics Letters | 2006

Graded band gap for dark-current suppression in long- wave infrared W-structured type-II superlattice photodiodes

I. Vurgaftman; E. H. Aifer; C. L. Canedy; Joseph G. Tischler; J. R. Meyer; J. H. Warner; E. M. Jackson; G. Hildebrandt; G. J. Sullivan

A new W-structured type-II superlattice photodiode design, with graded band gap in the depletion region, is shown to strongly suppress dark currents due to tunneling and generation-recombination processes. The long-wave infrared (LWIR) devices display 19%–29% quantum efficiency and substantially reduced dark currents. The median dynamic impedance-area product of 216Ωcm2 for 33 devices with 10.5μm cutoff at 78K is comparable to that for state-of-the-art HgCdTe-based photodiodes. The sidewall resistivity of ≈70kΩcm for untreated mesas is also considerably higher than previous reports for passivated or unpassivated type-II LWIR photodiodes, apparently indicating self-passivation by the graded band gap.


Nanophotonics | 2015

Low-loss, infrared and terahertz nanophotonics using surface phonon polaritons

Joshua D. Caldwell; Lucas Lindsay; Vincenzo Giannini; I. Vurgaftman; Thomas L. Reinecke; Stefan A. Maier; Orest J. Glembocki

Abstract The excitation of surface-phonon-polariton (SPhP) modes in polar dielectric crystals and the associated new developments in the field of SPhPs are reviewed. The emphasis of this work is on providing an understanding of the general phenomenon, including the origin of the Reststrahlen band, the role that optical phonons in polar dielectric lattices play in supporting sub-diffraction-limited modes and how the relatively long optical phonon lifetimes can lead to the low optical losses observed within these materials. Based on this overview, the achievements attained to date and the potential technological advantages of these materials are discussed for localized modes in nanostructures, propagating modes on surfaces and in waveguides and novel metamaterial designs, with the goal of realizing low-loss nanophotonics and metamaterials in the mid-infrared to terahertz spectral ranges.


Applied Physics Letters | 2000

Continuous-wave operation of λ=3.25 μm broadened-waveguide W quantum-well diode lasers up to T=195 K

W. W. Bewley; H. Lee; I. Vurgaftman; Ray Menna; C. L. Felix; Ramon U. Martinelli; D. W. Stokes; Dmitri Z. Garbuzov; J. R. Meyer; M. Maiorov; John C. Connolly; Alan R. Sugg; G. H. Olsen

Mid-infrared (λ=3.25 μm) broadened-waveguide diode lasers with active regions consisting of 5 type-II “W” quantum wells operated in continuous-wave (cw) mode up to 195 K. At 78 K, the threshold current density was 63 A/cm2, and up to 140 mW of cw output power was generated. A second structure with ten quantum wells operated up to 310 K in pulsed mode.


Applied Physics Letters | 1998

Near-room-temperature mid-infrared interband cascade laser

Linda J. Olafsen; E. H. Aifer; I. Vurgaftman; W. W. Bewley; C. L. Felix; Jerry R. Meyer; D. Zhang; C.-H. Lin; S. S. Pei

A 25-stage interband cascade laser with a W active region and a third hole quantum well for the suppression of leakage current has exhibited lasing in pulsed mode up to 286 K. A peak output power of 160 mW/facet and a slope efficiency of 197 mW/A per facet (1.1 photons per injected electron) were measured at 196 K. Above 200 K, the characteristic temperature was higher (T0=53 K) and the threshold current densities lower than for a previously reported W interband cascade laser without the third hole quantum well.


Applied Physics Letters | 2008

Interband cascade laser emitting at λ=3.75μm in continuous wave above room temperature

Mijin Kim; C. L. Canedy; W. W. Bewley; C. S. Kim; J. R. Lindle; J. Abell; I. Vurgaftman; J. R. Meyer

We report a five-stage interband cascade laser that operates at λ=3.75μm in cw mode up to a maximum temperature of 319K. With gold electroplating, epitaxial-side-up mounting, and one facet coated for high reflectivity, a 3mm×9.2μm ridge emits over 10mW of cw power at 300K.


Applied Physics Letters | 1998

Auger coefficients in type-II InAs/Ga1−xInxSb quantum wells

J. R. Meyer; C. L. Felix; W. W. Bewley; I. Vurgaftman; E. H. Aifer; Linda J. Olafsen; J. R. Lindle; C. A. Hoffman; M. J. Yang; Brian R. Bennett; B. V. Shanabrook; H. Lee; C.-H. Lin; S. S. Pei; R. H. Miles

Two different approaches, a photoconductive response technique and a correlation of lasing thresholds with theoretical threshold carrier concentrations have been used to determine Auger lifetimes in InAs/GaInSb quantum wells. For energy gaps corresponding to 3.1–4.8 μm, the room-temperature Auger coefficients for seven different samples are found to be nearly an order-of-magnitude lower than typical type-I results for the same wavelength. The data imply that at this temperature, the Auger rate is relatively insensitive to details of the band structure.


Journal of Physics D | 2015

Interband cascade lasers

I. Vurgaftman; Jerry R. Meyer; Chadwick Lawrence Canedy; W. W. Bewley; James R. Lindle; Chul Soo Kim; Mijin Kim

Recent advances in midwave infrared interband cascade lasers (ICLs) include novel distributed feedback configurations, vertical-cavity surface-emitting lasers, light-emitting devices, frequency combs, dual-comb spectroscopy, and ICLs incorporated into photonic integrated circuits on silicon and III-V platforms.


Journal of Applied Physics | 1998

Improved quantitative mobility spectrum analysis for Hall characterization

I. Vurgaftman; J. R. Meyer; C. A. Hoffman; D.A. Redfern; Jarek Antoszewski; Lorenzo Faraone; J.R. Lindemuth

We present an improved quantitative mobility spectrum analysis (i-QMSA) procedure for determining free electron and hole densities and mobilities from magnetic-field-dependent Hall and resistivity measurements on bulk or layered semiconductor samples. The i-QMSA technique is based on a fundamentally new approach, which optimizes the fit to the conductivity tensor components and their slopes by making those adjustments in the mobility spectra that result in the greatest error reduction. Empirical procedures for manipulating the mobility spectra are also introduced, with the dual purpose of reducing the error of the fit and simplifying the shape of the spectra to minimize the presence of unphysical artifacts. A fully automated computer implementation of the improved QMSA is applied to representative synthetic and real data sets involving various semiconductor material systems. These results show that, as compared with previous approaches, the presented algorithm maximizes the information that may be extract...

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W. W. Bewley

United States Naval Research Laboratory

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Jerry R. Meyer

United States Naval Research Laboratory

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J. R. Meyer

United States Naval Research Laboratory

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C. L. Canedy

United States Naval Research Laboratory

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Mijin Kim

United States Naval Research Laboratory

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C. S. Kim

United States Naval Research Laboratory

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C. L. Felix

United States Naval Research Laboratory

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J. R. Lindle

United States Naval Research Laboratory

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E. H. Aifer

United States Naval Research Laboratory

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Charles D. Merritt

United States Naval Research Laboratory

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