“…Therefore, the main operation regime for the heavily doped devices (JL) is usually bulk (V TH < V GS < V FB ), due to the large V FB -V TH difference, and for slightly or highly doped devices (AM) is accumulation (V GS > V FB ). Operation in the bulk regime has the advantage of less degradation of carrier mobility due to the perpendicular field (conduction at the middle part of the channel) [10] but suffering from a non-straight forward analytical model in this region [11].…”
Section: Conduction Mechanism In Accumulation-mode and Junctionless Rmentioning
confidence: 99%
“…3 can be seen as a degenerate double-gate architecture and therefore, an estimation of the accumulation current can be obtained from [11]. Indeed, noting that in the linear accumulation regime (V DS < V GS -V FB ), the log terms can be discarded in the charge vs. potential and retaining only the highest order term in Eqs.…”
Section: Analytical Model In the Strong Accumulation Regimementioning
confidence: 99%
“…Indeed, noting that in the linear accumulation regime (V DS < V GS -V FB ), the log terms can be discarded in the charge vs. potential and retaining only the highest order term in Eqs. (16), (22), and (24) in [11] (an assumption valid only in strong accumulation), we obtain (using source as a reference):…”
Section: Analytical Model In the Strong Accumulation Regimementioning
confidence: 99%
“…Since the accumulation-mode and junctionless transistors work in a simple MOSFET-like manner only above the flat-band voltage but not above the threshold voltage [11], direct extraction of the flat-band voltage as a key MOSFET parameter from the characterization data seem to be pretty necessary. At the first glance, the V FB value is expected to be extracted using the intersect of the two quasi-straight lines above the threshold voltage corresponding to the bulk and accumulation regimes in the transfer characteristic [25] or using I D / ffiffiffiffiffiffi g m p in the strong accumulation regime as an approximation [21,22].…”
a b s t r a c tIn this work we report dense arrays of accumulation-mode gate-all-around Si nanowire nMOSFETs with sub-5 nm cross-sections in a highly doped regime. The integration of local stressor technologies (both local oxidation and metal-gate strain) to achieve P2.5 GPa uniaxial tensile stress in the Si nanowire is reported. The deeply scaled Si nanowire including such uniaxial tensile stress shows a low-field electron mobility of 332 cm 2 /V s at room temperature, 32% higher than bulk mobility at the equivalent high channel doping. The conduction mechanism as well as high temperature performance was studied based on the electrical characteristics from room temperature up to %400 K and a V TH drift of À1.72 mV/K and an ionized impurity scattering-based mobility reduction were observed.
“…Therefore, the main operation regime for the heavily doped devices (JL) is usually bulk (V TH < V GS < V FB ), due to the large V FB -V TH difference, and for slightly or highly doped devices (AM) is accumulation (V GS > V FB ). Operation in the bulk regime has the advantage of less degradation of carrier mobility due to the perpendicular field (conduction at the middle part of the channel) [10] but suffering from a non-straight forward analytical model in this region [11].…”
Section: Conduction Mechanism In Accumulation-mode and Junctionless Rmentioning
confidence: 99%
“…3 can be seen as a degenerate double-gate architecture and therefore, an estimation of the accumulation current can be obtained from [11]. Indeed, noting that in the linear accumulation regime (V DS < V GS -V FB ), the log terms can be discarded in the charge vs. potential and retaining only the highest order term in Eqs.…”
Section: Analytical Model In the Strong Accumulation Regimementioning
confidence: 99%
“…Indeed, noting that in the linear accumulation regime (V DS < V GS -V FB ), the log terms can be discarded in the charge vs. potential and retaining only the highest order term in Eqs. (16), (22), and (24) in [11] (an assumption valid only in strong accumulation), we obtain (using source as a reference):…”
Section: Analytical Model In the Strong Accumulation Regimementioning
confidence: 99%
“…Since the accumulation-mode and junctionless transistors work in a simple MOSFET-like manner only above the flat-band voltage but not above the threshold voltage [11], direct extraction of the flat-band voltage as a key MOSFET parameter from the characterization data seem to be pretty necessary. At the first glance, the V FB value is expected to be extracted using the intersect of the two quasi-straight lines above the threshold voltage corresponding to the bulk and accumulation regimes in the transfer characteristic [25] or using I D / ffiffiffiffiffiffi g m p in the strong accumulation regime as an approximation [21,22].…”
a b s t r a c tIn this work we report dense arrays of accumulation-mode gate-all-around Si nanowire nMOSFETs with sub-5 nm cross-sections in a highly doped regime. The integration of local stressor technologies (both local oxidation and metal-gate strain) to achieve P2.5 GPa uniaxial tensile stress in the Si nanowire is reported. The deeply scaled Si nanowire including such uniaxial tensile stress shows a low-field electron mobility of 332 cm 2 /V s at room temperature, 32% higher than bulk mobility at the equivalent high channel doping. The conduction mechanism as well as high temperature performance was studied based on the electrical characteristics from room temperature up to %400 K and a V TH drift of À1.72 mV/K and an ionized impurity scattering-based mobility reduction were observed.
“…The theoretical foundations of JL FETs with double-gate [3], analysis of turned on characteristics of JL nanowire FET at different drain voltages and the potential under various operating conditions [4], discrete doping-induced variability in junctionless nanowire MOSFETs using dissipative quantum transport simulations [5], the impact of random dopant fluctuation for several JL FinFET [6], et al can be searched. Furthermore, some modeling results such as theoretical model of the JL silicon-on-insulator (SOI) FET [7] and a charge-based model of DG MOSFETs [8] have been reported. Some groups studied the OFF-state behavior of JLTs, and showed the effect of BTBT on JLT operating in volume depletion in OFF state [2].…”
Abstract-The effect of band-to-band tunneling (BTBT) leads to an obvious increase of the leakage current of junctionless (JL) transistors in the OFF state. In this paper, we propose an effective method to decline the influence of BTBT with the example of ntype double gate (DG) JL metal-oxide-semiconductor field-effect transistors (MOSFETs). The leakage current is restrained by changing the geometrical shape and the physical dimension of the gate of the device. The optimal design of the JL MOSFET is indicated for reducing the effect of BTBT through simulation and analysis.
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