arXiv subjects

F. Sam

Publications and source records attributed to F. Sam.

3 recordsLinked to original sources

arXiv2015

Acoustoelectric Effect in degenerate Carbon Nanotube

Acoustoelectric Effect $AE$ in degenerate Carbon Nanotube ($CNT$) was theoretically studied for hypersound in the regime $ql >> 1$. The dependence of acoustoelectric current $j^{ac}$ on the acoustic wave number $\vec{q}$ and frequency $\omega_q$ at $T = 10K$ and scattering angle ($\theta > 0$) was evaluated at various harmonics $n =\pm 1, 2, ...$ (where $n$ is an integer). In the first harmonics ($n = \pm 1$), the non-linear dependence of $j^{ac}$ on $\omega_q$ and $\vec{q}$ were obtained. For $n = \pm 2$, the numerically evaluated $j^{ac}$ qualitatively agreed with an experimentally obtained result.

cond-mat.mes-hall↗

arXiv2015

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 ($\Gamma$) under a non-quantizing electric field ($E$) with drift velocity ($V_D$)was obtained. At $T = 10K$ and scattering angle $\theta > 0$, the dependence of $\Gamma$ on acoustic wave number ($\vec{q}$), frequency ($\omega_q$), and $\gamma = 1-\frac{V_D}{V_s}$, ($V_s$ 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 $\gamma < 0$, 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↗

arXiv2014

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 $(\Gamma_{\perp}/\Gamma_0)$ 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 ($\beta$), the analysis of $\Gamma_{\perp}/\Gamma_0$ against the sub-bands index $(p_i)$; width of AGNR; and magnetic strength $(\Omega\tau)$, were numerically analyzed. The results showed a linear relation for $\Gamma_{\perp}/\Gamma_0$ with constant electric field $(\vec{E})$ but non-linear for $\Gamma_{\perp}/\Gamma_0$ with $q$ or $\Omega\tau$. 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↗