2007
DOI: 10.1063/1.2823606
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Device physics and guiding principles for the design of double-gate tunneling field effect transistor with silicon-germanium source heterojunction

Abstract: Physical-gap-channel graphene field effect transistor with high on/off current ratio for digital logic applications Appl. Phys. Lett. 101, 143102 (2012) Short channel mobility analysis of SiGe nanowire p-type field effect transistors: Origins of the strain induced performance improvement Appl. Phys. Lett. 101, 143502 (2012) Terahetz detection by heterostructed InAs/InSb nanowire based field effect transistors Development of high-performance fully depleted silicon-on-insulator based extended-gate field-effect t… Show more

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Cited by 97 publications
(54 citation statements)
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“…The tunnel FET has been given much attention in this regard as an alternative device architecture exhibiting a subthreshold swing (SS) below the conventional limits of MOSFET i.e. 60mV/dec, a low leakage current, suppressed Short Channel Effects (SCE) [1,2] and CMOS compatible process flow [3]. Numerous device designs and optimization techniques (both experimental and simulation based) such as strain engineering, heterojunction architectures, usage of low bandgap materials, tunnel source MOSFET [4][5][6][7][8][9], have been proposed in recent years in order to improve upon the shortcomings of TFET (a low ON current being the major bottleneck).…”
Section: Introductionmentioning
confidence: 99%
“…The tunnel FET has been given much attention in this regard as an alternative device architecture exhibiting a subthreshold swing (SS) below the conventional limits of MOSFET i.e. 60mV/dec, a low leakage current, suppressed Short Channel Effects (SCE) [1,2] and CMOS compatible process flow [3]. Numerous device designs and optimization techniques (both experimental and simulation based) such as strain engineering, heterojunction architectures, usage of low bandgap materials, tunnel source MOSFET [4][5][6][7][8][9], have been proposed in recent years in order to improve upon the shortcomings of TFET (a low ON current being the major bottleneck).…”
Section: Introductionmentioning
confidence: 99%
“…With the BTBT mechanism, TFET suggests a breakthrough of SS < 60 mV/decade at 300 K. Despite the steep switching feature, the TFET performance (e.g., I ON $ 1:7 µA/µm at V DD of 1 V [9]) is not sufficient even for low-power applications. To improve the performance, hetero-junction TFETs with narrow band-gap materials (such as Ge or III-V materials) in the source region are proposed [5,6,7]. However, another disadvantage of TFETs still remained unsolved: the asymmetry of the TFET device structure requires more area in the layout when the devices are connected.…”
Section: Nominal Device Designmentioning
confidence: 99%
“…Because reducing V DD has become a critical issue for manageable power density, the tunnel field effect transistor (TFET) is proposed, providing scaling of V DD down to 0.5 V or even below due to the subthreshold slope (SS) less than 60 mV/decade. However, the various types of TFETs suggested so far [1,2,3,4,5,6,7] are not symmetric, resulting in an area penalty in layout. In a previous work [8], a novel symmetric tunnel field-effect transistor (S-TFET) was proposed as an alternative device structure for low-power applications.…”
Section: Introductionmentioning
confidence: 99%
“…A heterojunction design, in which Ge is used only in the source region, is necessary to maintain low off-state leakage current (I OFF ) (5,6). The structure illustrated in Figure 1 was fabricated using a moderately doped poly-Ge source refill process to achieve the highest TFET I ON /I OFF reported to date for low-voltage (0.5 V) operation (7).…”
Section: Planar Ge-source Tfet Design Optimizationmentioning
confidence: 99%