首页> 外文OA文献 >High-field Overhauser DNP in silicon below the metal-insulator transition
【2h】

High-field Overhauser DNP in silicon below the metal-insulator transition

机译:在金属绝缘体下面的硅中的高场Overhauser DNp   过渡

代理获取
本网站仅为用户提供外文OA文献查询和代理获取服务,本网站没有原文。下单后我们将采用程序或人工为您竭诚获取高质量的原文,但由于OA文献来源多样且变更频繁,仍可能出现获取不到、文献不完整或与标题不符等情况,如果获取不到我们将提供退款服务。请知悉。

摘要

Single crystal silicon is an excellent system in which to explore dynamicnuclear polarization (DNP), as it exhibits a continuum of properties frommetallic to insulating as a function of doping concentration and temperature.At low doping concentrations DNP has been observed to occur via the solideffect, while at very high doping concentrations an Overhauser mechanism isresponsible. Here we report the hyperpolarization of 29Si in n-doped siliconcrystals, with doping concentrations in the range of 1-3 x 10^17 /cc. In thisregime exchange interactions between donors become extremely important. Thesign of the enhancement in our experiments and its frequency dependence suggestthat the 29Si spins are directly polarized by donor electrons via an Overhausermechanism within exchange-coupled donor clusters. The exchange interactionbetween donors only needs to be larger than the silicon hyperfine interaction(typically much smaller than the donor hyperfine coupling) to enable thisOverhauser mechanism. Nuclear polarization enhancement is observed for a rangeof donor clusters in which the exchange energy is comparable to the donorhyperfine interaction. The DNP dynamics are characterized by a singleexponential time constant that depends on the microwave power, indicating thatthe Overhauser mechanism is the rate-limiting step. Since only about 2 % of thesilicon nuclei are located within one Bohr radius of the donor electron,nuclear spin diffusion is important in transferring the polarization to all thespins. However, the spin-diffusion time is much shorter than the Overhausertime due to the relatively weak silicon hyperfine coupling strength. In a 2.35T magnetic field at 1.1 K, we observed a DNP enhancement of $244 +/- 84resulting in a silicon polarization of $10.4 +/- 3.4 % following two hours ofmicrowave irradiation.
机译:单晶硅是探索动态核极化(DNP)的极佳系统,因为它表现出从金属到绝缘的连续性随掺杂浓度和温度的变化。在低掺杂浓度下,已观察到DNP是通过固体效应发生的,在非常高的掺杂浓度下,Overhauser机制是负责任的。在这里,我们报道了n掺杂硅晶体中29Si的超极化现象,其掺杂浓度范围为1-3 x 10 ^ 17 / cc。在这种制度下,捐助者之间的交流互动变得极为重要。在我们的实验中增强的迹象及其频率依赖性表明,29Si自旋通过交换耦合的供体簇内的Overhauser机制被供体电子直接极化。施主之间的交换相互作用仅需大于硅超精细相互作用(通常比施主超精细偶合小得多)即可实现该Overhauser机理。观察到一系列供体簇的核极化增强,其中交换能量可与供体超精细相互作用相媲美。 DNP动力学的特征在于取决于微波功率的单指数时间常数,这表明Overhauser机制是速率限制步骤。由于仅约2%的硅原子核位于施主电子的一个玻尔半径内,因此核自旋扩散对于将极化转移到所有自旋中很重要。但是,由于相对较弱的硅超精细耦合强度,自旋扩散时间比Overhausertime短得多。在1.1 K的2.35T磁场中,我们观察到DNP增强$ 244 +/- 84,导致在微波辐射两个小时后硅极化达到$ 10.4 +/- 3.4%。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
代理获取

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号