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S. S. Abukari

Publications and source records attributed to S. S. Abukari.

At least 19 recordsLinked to original sources

Attractor-Basin-Limited Fidelity in Reproducible Multistate Vortex Memory

Multilevel non-volatile memory technologies face recurring trade-offs among information density, endurance, retention, and switching energy. We investigate an alternative state variable based on the discrete vortex configuration of self-organized vortices in a boundary-driven electron fluid. A dissipative point-vortex model derived from magnetohydrodynamic dynamics yields six reproducible vortex codewords, corresponding to 2.585 bits per cell, whose write fidelity, noise sensitivity, 100-cycle endurance, and effective information capacity are quantified. The ordering of their finite-amplitude basin radii $r_{50}$ differs from that predicted by both fixed-circulation and fully coupled linear-stability spectra. A nonlinear saddle-point construction based on the reduced dynamics likewise does not recover the measured basin ordering. The discrepancy is associated with escape pathways involving coupled position--circulation dynamics that are absent from the fixed-circulation description. These results show that local stability alone does not determine the finite perturbation tolerance of the vortex states considered here. The proposed memory requires active hold power, and passive retention remains to be established experimentally.

cond-mat.mtrl-sci↗

Behaviour of hot electrons under the dc field in chiral carbon nanotubes

Behaviour of hot electrons under the influence of dc field in carbon nanotubes is theoretically considered. The study was done semi-classically by solving Boltzmann transport equation with the presence of the hot electrons source to derive the current densities. Plots of the normalized axial current density versus electric field strength of the chiral CNTs reveal a negative differential conductivity (NDC). Unlike achiral CNTs, the NDC occurs at a low field about $\mathrm{6\ kV/cm}$ for chiral CNT. We further observed that the switch from NDC to PDC occurs at lower dc field in chiral CNTs than achiral counterparts. Hence the suppression of the unwanted domain instability usually associated with NDC and a potential generation of terahertz radiations occurs at low electric field for chiral CNTs.

cond-mat.mes-hall↗

Nonlinear Conductivity in Graphene

We consider the tight-binding approximation for the description of energy bands of graphene, together with the standard Boltzmann's transport equation and constant relaxation time, an expression for the conductivity was obtained. We predicted strong nonlinear effects in graphene which may be useful for high frequency generation.

cond-mat.mes-hall↗

Magnetoplasmon excitations at graphene vortex Hall fluid edge

We investigate magnetoplasmon dynamics localized on the edges of graphene vortex Hall fluid. The vortex matter captures an anomalous term that causes vortex localization near fluid boundary and creates a double boundary layer, $Δ_0\propto (β-1)\ell_B$ with $β$ being filling factor. The term also has qualitative effect on resonant excitations of edge magnetoplasmons. We found that for sharp edges under experimental conditions, graphene Edge Magnetoplasmon (EMP) resonances have similar behavior as in recent experiments. Gradual distinctions arise for smooth edges in the presence of the anomalous term, where a weak EMP peak appear. The second peak becomes well noticed as the smoothness is increased. We identified the resonant mode as an Inter-EMP. It originates from the oscillations of charges in the inner boundary of the double layer. The present observation brings to light the direct cause of Inter-EMP which remained to be detected in graphene experiments.

cond-mat.mes-hall↗

Hot electrons injection in carbon nanotubes under the influence of quasi-static ac-field

Hot electrons injection in carbon nanotubes (CNTs ) where in addition to applied dc field ($\mathbf{E}$), there exist simultaneously a quasi-static ac electric field (i.e. when the frequency $ω$ of ac field is much less than the scattering frequency $v$ ($ω\ll v$ or $ωτ\ll 1$, $v =τ^{-1}$, where $τ$ is relaxation time) is considered. The investigation is done theoritically by solving semiclassical Boltzmann transport equation with and without the presence of the hot electrons source to derive the current densities. Plots of the normalized current density versus dc field ($\mathbf{E}$) applied along the axis of the CNTs in the presence and absence of hot electrons reveal ohmic conductivity initially and finally negative differential conductivity (NDC) provided $ωτ\ll 1$ (i.e. quasi- static case). With strong enough axial injection of the hot electrons , there is a switch from NDC to positive differential conductivity (PDC) about $\mathbf{E} \geq 75 kV/cm$ and $\mathbf{E} \geq 140 kV/cm$ for a zigzag CNT and an armchair CNT respectively. Thus, the most important tough problem for NDC region which is the space charge instabilities can be suppressed due to the switch from the NDC behaviour to the PDC behaviour predicting a potential generation of terahertz radiations whose applications are relevance in current-day technology, industry, and research.

cond-mat.mes-hall↗

High Frequency Conductivity of Hot Electrons in Carbon Nanotubes

High frequency conductivity of hot electrons in an undoped single walled achiral carbon nanotubes (CNTs) under the influence of ac-dc driven fields is considered. We investigated semiclassically by solving the Boltzmann's transport equation with and without the presence of the hot electrons source to derive the current densities. Plots of the normalized current density versus frequency of ac-field reveal an increase in both the minimum and maximum peaks of normalized current density at lower frequencies as a result of a strong enough injection of hot electrons . The applied ac-field plays twofold role of suppressing the space-charge instability in CNT and simultaneously pumping an energy for lower frequency generation and amplification of THz radiations which have enormous promising applications in very different areas of science and technology.

cond-mat.mes-hall↗

Hypersound Absorption of Acoustic Phonons in a degenerate Carbon Nanotube

Hypersound Absorption of acoustic phonons having $ql>>1$ in a degenerate Carbon Nanotube (CNT) with linear energy dispersion near the Fermi level was theoretically studied. The general expression for the absorption coefficient ($Γ$) under a non-quantizing electric field ($E$) with drift velocity ($V_D$)was obtained. At $T = 10K$ and scattering angle $θ> 0$, the dependence of $Γ$ on acoustic wave number ($\vec{q}$), frequency ($ω_q$), and $γ= 1-\frac{V_D}{V_s}$, ($V_s$ being the speed of sound) were analysed numerically at $n = 0, \pm 1, \pm 2$ (where $n$ represent the various harmonics) and presented graphically. In a $3D$ representation, when $γ< 0$, the maximum amplification was attained at $V_D = 1.1V_s$ which occurred at $E = 51.7Vcm^{-1}$. In the second harmonics, ($n =\pm 2$), the absorption obtained was compared to experimental measurement of acoustoelectric current via the Weinreich relation. From the graphs, the observed amplification of acoustic phonons caused by intraband transition shows CNT as a promising hypersound generator (SASER).

cond-mat.mes-hall↗

Stark-cyclotron Resonance in an Array of Carbon Nanotubes

Using the kinetic approach based on the semiclassical Boltzmann transport equation with constant relaxation time, we theoretically studied the Stark-cyclotron resonance in an array of Carbon Nanotubes (CNs). Exact expression for the current density was obtained. We noted that Stark-cyclotron resonance occurs when the Larmor frequency coincides with the Stark frequency. A coincidence of these frequencies produce resonance.

cond-mat.mes-hall↗

Amplification of Acoustic Waves in Graphene Nanoribbon in the Presence of External Electric and Magnetic Field

Amplification of Acoustic Waves in Armchair Graphene Nanoribbon (AGNR) in the presence of an external Electric and Magnetic field was studied using the Boltzmann's kinetic equation. The general expression for the Amplification $(Γ_{\perp}/Γ_0)$ was obtained in the region $ql >> 1$ for the energy dispersion $\varepsilon(\vec{p})$ near the Fermi point. For various parameters of the quantized wave vector ($β$), the analysis of $Γ_{\perp}/Γ_0$ against the sub-bands index $(p_i)$; width of AGNR; and magnetic strength $(Ωτ)$, were numerically analyzed. The results showed a linear relation for $Γ_{\perp}/Γ_0$ with constant electric field $(\vec{E})$ but non-linear for $Γ_{\perp}/Γ_0$ with $q$ or $Ωτ$. Sound Amplification in AGNR is reported with an increase in Acoustic wave number $(\vec{q}) > 1.5\times 10^{7}cm^{-1}$. This can cause SASER in Armchair Graphene Nanoribbon (AGNR).

cond-mat.mes-hall↗

Acoustomagnetoelectric Effect in Graphene Nanoribbon in the Presence of External Electric and Magnetic Field

The Acoustomagnetoelectric Effect (AME) in Graphene Nanoribbon (GNR) was theoretically studied using the Boltzmann kinetic equation. On open circuit, the general formular for Surface Acoustomagnetoelectric field ($\vec{E}_{SAME}$) in GNR with energy dispersion $\varepsilon(p)$ near the Fermi point was calculated. The $E_{SAME}$ was found to depend on the magnetic strength ($η$), $α$ = ${\hbar ω_q}/{E_g}$ and the energy gap ($E_g$). The expression for $\vec{E}_{SAME}$ was analyzed numerically for varying width of GNR, magnetic strength ($η$) and $α$ at different sub-bands indices ($p_i$). It was noted that the dependence of $\vec{E}_{SAME}$ on the width of GNR increased to a saturation point of approximately $15$Vcm$^{-1}$ and remained constant. For $E_{SAME}$ versus $η$, the $E_{SAME}$ increases rapidly to a maximum point and then decayed to a constant minimum value. The graph was modulated either by varying the width of GNR or the sub-band index $p_i$ with an inversion occurring at $p_i = 6$. The dependence of $E_{SAME}$ versus $α$ was analyzed. The $E_{SAME}$ was constant up to a point and sharply increased asymptotically at approximately $α= 1$. A $3$D graph of $\vec{E}_{SAME}$ with $η$ and width is also presented. This study is relevant for investigating the properties of GNR.

cond-mat.mes-hall↗

Laser Stimulated Thermal Conductivity in chiral carbon nanotube

An investigation of laser stimulated thermal conductivity in chiral CNT is presented. The thermal conductivity of a chiral CNT is calculated using a tractable analytical approach. This is done by solving the Boltzmann transport equation with energy dispersion relation obtained in the tight binding approximation. The electron thermal conductivity along the circumferential χ_c and axial χ_z are obtained. The results obtained are numerically analyzed and both χ_c and χ_z are found to oscillate in the presence of laser radiations. We have also noted that the laser source caused a drastic reduction in the both χ_c and χ_z values.

cond-mat.mtrl-sci↗

Appearance of Large Amplitude Current Dynamics as a Result of Bragg Reflection in Carbon Nanotubes

We report on theoretical analysis of large amplitude current dynamics due to Bragg reflections in carbon nanotubes exposed to an external electric field. Using the kinetic equation with constant relaxation time, an analytical expression for the current density is obtained. Our results suggest that Bloch gain exists up to frequencies on the order of the Bloch frequency. We noted that due to the high density of states of conduction electrons in metallic carbon nanotubes and the specific dispersion law inherent in hexagonal crystalline structure result in a uniquely high frequency gain than the corresponding values for semiconducting ones. We suggest that this phenomenon can be used for domainless multiplication of the frequency of an electromagnetic signal at room temperature

cond-mat.mes-hall↗

External electric field effect on electron transport in carbon nanotubes

Electronic transport properties of carbon nanotubes are studied theoretically in the presence of external electric field E(t) by using the Boltzmann's transport with constant relaxation time. An analytical expression for the current densities of the nanotubes are obtained. It is observed that the current density-electric field characteristics of the CNs exhibit total self-induced transparency and absolute negative conductivity

cond-mat.mes-hall↗

Appearance of Negative Differential Conductivity in Graphene Nanoribbons at High-Harmonics

We theoretically study current dynamics of graphene nanoribbons subject to bias dc and ac driven fields. We showed that graphene nanoribbons exhibit negative high-harmonic differential conductivity. Negative differential conductivity appears when bias electric filed is in the neighborhood of applied ac filed amplitude. We also observe both even and odd high-harmonic negative differential conductivity at wave mixing of two commensurate frequencies. The even harmonics are more pronounced than the odd harmonics. A possible use of the present method for generating terahertz frequencies at even harmonics in graphene is suggested.

cond-mat.mtrl-sci↗

Generation and Amplification of Terahertz Radiation in Carbon Nanotubes

We investigate theoretically the feasibility of generation and amplification of terahertz radiation in aligned achiral carbon nanotubes (zigzag and armchair) in comparison with a superlattice in the presence of a constant (dc) and high-frequency (ac) electric fields. The electric current density expression is derived using the semiclassical Boltzmann transport equation with a constant relaxation time with the electric field applied along the nanotube axis. Our analysis on the current density versus electric field characteristics demonstrates negative differential conductivity at high frequency as well as photon assisted peaks. The characteristic peaks are about an order of magnitude styronger in the carbon nanotubes compared to superlattice. These strong phenomena in carbon nanotubes can be used to obtain domainless amplification of terahertz radiation in carbon nanotubes at room temperature.

cond-mat.mes-hall↗

Terahertz Generation and Amplification in Graphene Nanoribbons in Multi-frequency Electric Fields

We study theoretically a multi-frequency response of electrons in confined graphene subject to dc-ac driven fields. We explore the possibility for using graphene nanoribbons (GNRs) to generate and amplify terahertz (THz) radiations in electric field domainless regime. We discover two main important schemes of generation; when the frequencies are commensurate, THz generation is due to wave mixing and when they are non-commensurate, a single strong field suppresses space charge instability and any weak signals can get amplified. The use of graphene as a best substitute for semiconductor nanoelectronic devices is suggested.

cond-mat.mtrl-sci↗

Photon-Assisted Process and High-Harmonic Dynamic Localization in Graphene Nanoribbons

We used a complete tight-binding band structure of graphene nanoribbon to obtain, for the first time, analytical techniques for observing photon assisted transport, and dynamic localization of electrons in the graphene nanoribbons. When the ribbons are subject to a multi-frequency dc-ac field, photon assisted replicas show up at rather strong drive force. The strong dependence of the photon peaks on ac amplitudes allow for high-harmonic dynamic oscillations at these amplitudes. We identified regions of positive differential conductivity where a nanoelectronic graphene device may be operated as a small signal amplifier. Our research has also reveal another quantum mechanical phenomenon, fractional photon assisted transport, when the stark factor $r > 1$.

cond-mat.mtrl-sci↗

General Scattering Mechanism and Transport in Graphene

Using quasi-time dependent semi-classical transport theory in RTA, we obtained coupled current equations in the presence of time varying field and based on general scattering mechanism $τ\propto \mathcal{E}^β$. We find that close to the Dirac point, the characteristic exponent $β= +2$ corresponds to acoustic phonon scattering. $β= +1$ long-range Coulomb scattering mechanism. $β= -1$ is short-range delta potential scattering in which the conductivity is constant of temperature. The $β= 0$ case is ballistic limit. In the low energy dynamics of Dirac electrons in graphene, the effect of the time-dependent electric field is to alter just the electron charge by $e \to e(1 + (Ωτ)^2)$ making electronic conductivity non-linear. The effect of magnetic filed is also considered.

cond-mat.mtrl-sci↗