We propose far-infrared photodetectors with the graphene nanoribbon (GNR) array as the photosensitive element and the black phosphorus (bP) base layer (BL). The operation of these GNR infrared photodetectors (GNR-IPs) is associated with the interband photogeneration of the electron–hole pairs in the GNR array followed by the tunneling injection of either electrons or holes into a wide gap bP BL. The GNR-IP operating principle is akin to that of the unitraveling-carrier photodiodes based on the standard semiconductors. Due to a narrow energy gap in the GNRs, the proposed GNR-IPs can operate in the far-, mid-, and near-infrared spectral ranges. The cut-off photon energy, which is specified by the GNR energy gap (i.e., is dictated by the GNR width), can be in the far-infrared range, being smaller that the energy gap of the bP BL of ΔG ≃ 300 meV. Using the developed device models of the GNR-IPs and the GNR-IP terahertz photomixers, we evaluate their characteristics and predict their potential performance. The speed of the GNR-IP response is determined by rather short times: the photocarrier try-to-escape time and the photocarrier transit time across the BL. Therefore, the GNR-IPs could operate as terahertz photomixers. The excitation of the plasma oscillations in the GNR array might result in a strong resonant photomixing.
We analyze the pumping of the graphene-based laser heterostructures by infrared radiation using the numerical model. To enable the injection of sufficiently cooled carriers into the graphene layer (GL) leading to the interband population inversion, we propose to use the graded-gap black-PxAs1 − x absorption-cooling layers. Our calculations are based on the thermodiffusion-drift carrier transport model. We demonstrate that the proposed optical pumping method can provide an efficient injection of the cool electron–hole plasma into the GL and the interband population inversion in the GL. Since the energy gap in b-As layer can be smaller than the energy of optical phonons in the GL, the injected electron–hole plasma can be additionally cooled down to the temperatures lower than the lattice temperature. This promotes a stronger population inversion that is beneficial for realization of the GL-based optically pumped terahertz and far-infrared laser, plasmon emitters, and the superluminescent downconverters. We also compare the efficiency of optical pumping through the graded-gap and uniform absorbing-cooling layers.
We propose a novel technology for fabricating plasmonic photoconductive antennas (PCAs) based on superlattice (SL) with increased height of the plasmonic gratings up to 100 nm. We passivate the surface of the SL by Si3N4, etch there windows and deposit Ti/Au antenna metallization. The plasmonic gratings are formed by electron-beam lithography with Ti/Au metallization followed by lift-off. Then an Al2O3 anti-reflection coating layer for reduction of the Fresnel reflection losses is used on the top of the plasmonic gratings, which also serves for maintaining its mechanical stability and providing the excitation of guided modes at the resonant wavelengths of the subwavelength slab waveguide formed by the metal gratings. Current-voltage measurements under femtosecond laser illumination reveal strong increase of the transient photocurrent generated by the fabricated plasmonic PCA which is 15 times higher than for conventional one (i.e. without the plasmonic gratings). The obtained terahertz (THz) power spectra demonstrate 100-times increase of the THz power in the plasmonic PCA. The results might be of interest to the needs of THz spectroscopy and imaging systems, in particular, operating with low-power lasers.
This paper reviews recent advances in the terahertz (THz) graphene-based 2D-heterostructure lasers and amplifiers. The linear gapless graphene energy spectrum enables population inversion under optical and electrical pumping giving rise to the negative dynamic conductivity in a wide THz frequency range. We first theoretically discovered these phenomena and recently reported on the experimental observation of the amplified spontaneous THz emission and single-mode THz lasing at 100K in the current-injection pumped graphene-channel field-effect transistors (GFETs) with a distributedfeedback dual-gate structure. We also observed the light amplification of stimulated emission of THz radiation driven by graphene-plasmon instability in the asymmetric dual-grating gate (ADGG) GFETs by using a THz time-domain spectroscopy technique. Integrating the graphene surface plasmon polariton (SPP) oscillator into a current-injection graphene THz laser transistor is the most promising approach towards room-temperature intense THz lasing.
This paper reviews recent advancement on the research toward graphene-based terahertz (THz) lasers. Optical and/or injection pumping of graphene can enable negative-dynamic conductivity in the THz spectral range, which may lead to new types of THz lasers. A forward-biased graphene structure with a lateral p-i-n junction was implemented in a distributed-feedback (DFB) dual-gate graphene-channel FET and observed a single mode emission at 5.2 THz at 100K. The observed spectral linewidth fairly agrees with the modal gain analysis based on DFB-Fabry-Perrot hybrid-cavitymode modeling. Although the results obtained are still preliminary level, the observed emission could be interpreted as THz lasing in population-inverted graphene by carrier-injection.
The gated GaAs structures like the field-effect transistor with the array of the Sn nanothreads was fabricated via delta-doping of vicinal GaAs surface by Sn atoms with a subsequent regrowth. That results in the formation of the chains of Sn atoms at the terrace edges. Two device models were developed. The quantum model accounts for the quantization of the electron energy spectrum in the self-consistent two-dimensional electric potential, herewith the electron density distribution in nanothread arrays for different gate voltages is calculated. The classical model ignores the quantization and electrons are distributed in space according to 3D density of states and Fermi-Dirac statistics. It turned out that qualitatively both models demonstrate similar behavior, nevertheless, the classical one is in better quantitative agreement with experimental data. Plausibly, the quantization could be ignored because Sn atoms are randomly placed along the thread axis. The terahertz hot-electron bolometers (HEBs) could be based on the structure under consideration.
This paper reviews recent advances in the research of graphene-based van der Waals heterostructures for emission and detection of terahertz radiation. A gated double-graphene-layer (DGL) nanocapacitor is the core shell under consideration, in which a thin tunnel barrier layer is sandwiched by outer graphene layers at both sides. The DGL can support symmetric optical and anti-symmetric acoustic coupled plasmon modes in the GLs. The latter mode can modulate the band-offset between the GL, giving rise to modulation of the inter-GL-layer resonant tunneling. This can dramatically enhance the THz gain or responsivity via plasmon-assisted inter-GL resonant tunneling.
This paper reviews recent advances in the double-graphene-layer (DGL) active plasmonic heterostructures for the terahertz (THz) device applications. The DGL consists of a core shell in which a thin tunnel barrier layer is sandwiched by the two GLs being independently connected with the side contacts and outer gate stack layers at both sides. The DGL core shell works as a nano-capacitor, exhibiting inter-GL resonant tunneling (RT) when the band offset between the two GLs is aligned. The RT produces a strong nonlinearity with a negative differential conductance in the DGL current-voltage characteristics. The excitation of the graphene plasmons by the THz radiation resonantly modulates the tunneling currentvoltage characteristics. When the band offset is aligned to the THz photon energy, the DGL structure can mediate photonassisted RT, resulting in resonant emission or detection of the THz radiation. The cooperative double-resonant excitation with structure-sensitive graphene plasmons gives rise to various functionalities such as rectification (detection), photomixing, higher harmonic generation, and self-oscillation, in the THz device implementations.
This paper reviews recent advances in the research and development toward the graphene-based terahertz (THz) lasers. Mass-less Dirac Fermions of electrons and holes in gapless and linear symmetric band structures in graphene enable a gain in a wide THz frequency range under optical or electrical pumping. The excitation of the surface plasmon polaritons in the population-inverted graphene dramatically enhances the THz gain. Photon-emission-assisted resonant tunneling in a double-graphene-layered nano-capacitor structure also strongly enhances the THz gain. Novel graphene-based heterostructures using these physical mechanisms for the current-injection driven THz lasing are discussed. Their superior gain-spectral properties are analyzed and the laser cavity structures for the graphene THz laser implementation are discussed.
This paper reviews recent advances in graphene plasmonic heterostructures for new types of terahertz lasers. We
theoretically discovered and experimentally manifested that the excitation of surface plasmons in population-inverted
graphene by the terahertz photons results in propagating surface plasmon polaritons with a giant gain in a wide terahertz
range. Furthermore, double graphene layer heterostructures consisting of a tunnel barrier insulator sandwiched with a
pair of gated graphene monolayers are introduced. Photoemission-assisted quantum-mechanical resonant tunneling can
be electrically tuned to meet a desired photon energy for lasing, resulting in enormous enhancement of the terahertz gain.
Current injection structures are also addressed.
Among different carbon materials (diamond, graphite, fullerene, carbon nanotubes), graphene and more complex graphene-based structures attracted a considerable attention. The gapless energy spectrum of graphene implies that graphene can absorb and emit photons with rather low energies corresponding to terahertz (THz) and infrared (IR) ranges of the electromagnetic spectrum. In this presentation, the discussion is focused on the double-graphene-layer (double-GL) structures. In these structures, GLs are separated by a barrier layer (Boron Nitride, Silicon Carbide, and so on). Applying voltage between GLs, one can realize the situation when one GL is filled with electrons while the other is filled with holes. The variation of the applied voltage leads to the variations of the Fermi energies and, hence, to the change of the interband and intraband absorption of electromagnetic radiation and to the variation of the tunneling current. The plasma oscillations in double-GL structures exhibit interesting features. This is mainly because each GL serves as the gate for the other GL. The spectrum of the plasma oscillations in the double-GL structures falls into the terahertz range (THz) of frequencies and can be effectively controlled by the bias voltage. In this paper, we discuss the effects of the excitation of the plasma oscillations by incoming THz radiation and by optical radiation of two lasers with close frequencies as well as negative differential conductivity of the N-type and Z-type. These effects can be used in resonant THz detectors and THz photomixers. The models of devices based on double-GL structures as well as their characteristics are discussed.
This paper reviews recent advances in terahertz-wave generation in graphene toward the creation of new types of graphene terahertz lasers. Fundamental basis of the optoelectronic properties of graphene is first introduced. Second, nonequilibrium carrier relaxation/recombination dynamics and resultant negative terahertz conductivity in optically or electrically pumped graphene are described. Third, recent theoretical advances toward the creation of current-injection graphene terahertz lasers are described. Fourth, unique terahertz dynamics of the two-dimensional plasmons in graphene are discussed. Finally, the advantages of graphene materials and devices for terahertz-wave generation are summarized.
We report on the effect of population inversion associated with the electron and hole injection in graphene pi-
n structures at the temperatures 200K-300K. It is assumed that the recombination and energy relaxation of
electrons and holes is associated primarily with the interband and intraband processes assisted by optical phonons.
The dependences of the electron-hole and optical phonon effective temperatures on the applied voltage, the
current-voltage characteristics, and the frequency-dependent dynamic conductivity are obtained. In particular,
at low and moderate voltages the injection can lead to a pronounced cooling of the electron-hole plasma in the
device i-section to the temperatures below the lattice temperature. At higher voltages, the current and electronhole
and phonon temperature dependences on voltage exhibit the S-shape. At a certain values of the applied
voltage the frequency-dependent dynamic conductivity can be negative in the terahertz range of frequencies. The
electron-hole plasma cooling substantially reinforces the effect of negative dynamic conductivity and promotes
the realization of terahertz lasing. It is demonstrated that the heating of optical phonon system hinders the
realization of negative dynamic conductivity and terahertz lasing at the room temperatures.
We study nonequilibrium carriers (electrons and holes) in an intrinsic graphene at low temperatures under farand
mid-infrared optical pumping in a wide range of its power densities. The energy distributions of carriers
are calculated using a quasiclassic kinetic equation which accounts for the energy relaxation due to acoustic
phonons and the radiative generation-recombination processes associated with thermal radiation and the carrier
photoexcitation by incident radiation. It is found that the nonequilibrium distributions are determined by an
interplay between weak energy relaxation on acoustic phonons and generation-recombination processes as well as
by the effect of pumping saturation. Due to the effect of pumping saturation, the carrier distribution functions
can exhibit plateaus whose width increases with increasing pumping power density. The graphene steady-state
conductivity as a function of the pumping power density exhibits a pronounced nonlinearity with a sub-linear
region at fairly low power densities. As shown, at certain pumping power density the population inversion as
well as the dynamic negative conductivity can take place in terahertz and far-infrared frequencies, suggesting the
possibility of utilization of graphene under optical pumping for optoelectronic applications, in particular, lasing
at such frequencies.
We study plasma effects in a micromachined high-electron mobility transistor (HEMT) with the microcantilever
(MC) serving as the gate using the developed model. The model accounts for mechanical motion of the MC and
spatio-temporal variations (plasma effects) of the two-dimensional electron gas (2DEG) system in the transistor
channel. The MC mechanical motion is described in the point-mass approximation. The hydrodynamic electron
transport model is used to describe distributed electron plasma phenomena in the 2DEG system. Using the
developed model, we calculated the response function characterizing the amplitude microcantilever oscillations
and the output electric signal as functions of the signal frequency and the bias voltage for the devices with
different parameters. We find the voltage dependences of the frequency of the mechanical resonance and its
damping. In particular, it is demonstrated that the amplitudes of the mechanical oscillations and output electric
signal exhibit pronounced maxima at the bias voltages close to the voltage of the 2DEG channel depletion
followed by a steep drop with further increase in the bias voltage. We also consider a concept of a resonant
detector of modulated terahertz radiation based on a micromachined HEMT. This device can exhibit both the
plasma (in terahertz range) and mechanical (in megahertz or gigahertz range) resonances.
KEYWORDS: Plasma, Terahertz radiation, Heterojunctions, Monte Carlo methods, Instrument modeling, Electron transport, Metals, Particles, Field effect transistors, Absorption
We study theoretically a heterostructure device with the structure akin to a high-electron mobility transistor which can be
used to generate electro-magnetic radiation in the terahertz range of frequencies. The gated electron channel is supplied
with a lateral Schottky contact serving as the source. The operation of the device is associated with photomixing of
optical signals in high-electric-field depletion region of the Schottky junction. The electrons and holes photogenerated in
the Schottky junction depletion region and propagating across it induce the ac current in the quasi-neutral electron channel
which, in turn, excites the plasma oscillations in this channel. Fast electron transport in the Schottky junction depletion
region and resonant properties of the electron channel provide an enhanced response of the photomixer to optical signals
at the plasma frequencies.
We develop device models of a terahertz (THz) photomixer based on
a high-electron mobility transistor (HEMT) structure utilizing
the excitation of electron plasma oscillations in the HEMT channel by the electrons and holes photogenerated by optical signals.
We use hydrodynamic equations both for electrons in the channel and
for photoelectrons and photoholes in the absorption layer, or hydrodynamic equations for electrons in the channel combined with
a kinetic description of the photogenerated carriers, and the Poisson equation for the self-consistent electric field. The models are used for an analytical as well as numerical (based on an ensemble Monte Carlo particle technique) analysis of the HEMT-photomixer operation in the THz frequency range.
We review recent studies of physical phenomena in quantum well infrared photodetectors (QWIPs), and some other QW and QD infrared devices and discuss their features. We show that the optimization of QWIPs, improvement of QDIPs, and creation of novel QWIP- and QDIP-based devices still requires an in-depth understanding of underlying physical effects.
As predicted theoretically, quantum dot infrared photodetectors (QDIPs) can substantially surpass quantum well infrared photodetectors (QWIPs). Recently, a number of research groups reported fabrication and extensive experimental investigation of various InAs/GaAs, InGaAs/GaAs, and InGaAs/InGaP QDIPs. However, most of the fabricated QDIPs have worse performance than QWIPs. To answer the questions why QDIPs are still inferior to QWIPs and how to improve them, we analyze the QDIP operation using the developed device model of QDIPs with realistic parameters. The model takes into account the main physical factors determining the operation of QDIPs. We calculate the dark current and the responsivity of QDIPs as functions of their structural parameters, the applied voltage, and temperature. The calculated characteristics are in agreement with those of realistic QDIPs studied experimentally. The revealed relations between the QDIP operation characteristics and structural parameters explain the main features of QDIPs observed in experiments. We estimate the QDIP detectivity and find the conditions for its maximum value. We compare the QDIP characteristics with those of QWIPs.
In this paper a two-dimensional ensemble Monte Carlo particle method is used to simulate the metal-semiconductor-metal (MSM) photodetector response in the terahertz range of signal frequencies. We consider planar MSM photodetectors consisting of a GaAs absorbing layer with a system of Schottky contacts made 'back-to-back' on the above layer. The model takes into account the features of the carrier energy spectra, mechanisms of their scattering and a self-consistent electric field. The intrinsic transient response triggered by an ultra-short light pulse is calculated. The MSM frequency response is calculated using the Fourier transform of the obtained temporal dependences. It is shown that due to velocity overshoot effect exhibited by the photoelectrons, the MSM photodetector reveals rather high response to terahertz signals even if the contact spacing is relatively large. The frequency response of the MSM photodetectors utilizing the photoelectron velocity overshoot effect is compared with that of the MSM photodetectors with ultra-short carrier lifetime.
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