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Graphene-diamond-silicon devices with increased current-carrying capacity: sp2-Carbon-sp3-Carbon-on-Silicon technology

机译:石墨烯 - 金刚硅装置,具有载流量增加:SP 2 -Carbon-SP 3 - 硅技术

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Graphene demonstrated potential for practical applications owing to its excellent electronic and thermal properties. Typical graphene field-effect transistors (FETs) and interconnects built on conventional SiO2/Si substrates reveal the breakdown current density on the order of 108 A/cm2, which is ∼100× larger than the fundamental limit for the metals but still smaller than the maximum achieved in carbon nanotubes. It was discovered by some of us that graphene has excellent thermal conduction properties with the thermal conductivity K exceeding 2000 W/mK at room temperature [1]. Few-layer graphene largely preserves the heat conduction properties [2]. However, the thermally resistive SiO2, with the thermal conductivity in the range from 0.5 to 1.4 W/mK, creates a bottleneck for heat removal. The latter does not allow graphene to demonstrate its true current-carrying potential. We show that by replacing SiO2 with synthetic diamond one can substantially increase the current-carrying capacity of graphene to as high as ∼ 20×108 A/cm2 under ambient conditions. The two-terminal and three-terminal top-gated graphene devices (see Figure 1) were fabricated on synthetic single-crystal diamond (SCD) and ultrananocrystalline diamond (UNCD). To ensure Si integration, the UNCD layers were grown at low temperatures compatible with Si CMOS technology [3]. Our results indicate that graphene's current-induced breakdown is thermally activated. It was found that the current carrying capacity of graphene can be improved not only on SCD but also on an inexpensive UNCD. The latter was attributed to the decreased thermal resistance of UNCD at elevated temperatures (see Figure 2). The obtained results are important for graphene's hetero-integration on Si substrates. The enhanced current-carrying capacity is beneficial for the proposed applications of graphene in interconnects and hi- h-frequency transistors.
机译:由于其优异的电子和热性能,石墨烯显示出实际应用的潜力。典型的石墨烯场效应晶体管(FET)和基于传统SiO2 / Si基板的互连显示,在10 8 a / cm 2 的量级上显示击穿电流密度~100×大于金属的基本极限,但仍然小于碳纳米管中实现的最大值。我们中的一些人发现,石墨烯具有优异的热传导性能,导热性k在室温下超过2000w / mk [1]。几层石墨烯大部分保留了导热性能[2]。然而,具有0.5至1.4W / mK的导热率的热电阻SiO 2产生了用于除去的瓶颈。后者不允许石墨烯展示其真正携带的电流潜力。我们表明,通过用合成金刚石更换SiO 2,可以在环境条件下基本上增加石墨烯的电流承载能力至高达〜20×10 2 。双端子和三端顶门的石墨烯装置(参见图1)在合成单晶金刚石(SCD)和超晶金刚石(UNCOD)上制造。为了确保SI集成,在与SI CMOS技术兼容的低温下生长UNC分层[3]。我们的结果表明,石墨烯的电流诱导的分解是热敏激活的。结果发现石墨烯的当前承载能力不仅可以在SCD上改善,而且可以在廉价的UNC;后者归因于升高温度下的UNC的热阻降低(见图2)。获得的结果对于石墨烯对Si基材的异质集成是重要的。增强的电流承载能力是有益的石墨烯在互连和高频晶体管中的应用。

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