IBM Research Division, Almaden Research Center, 650 Harry Road, San Jose, CA 95120, USA. Department of Physics, University of Basel, Klingelbergstrasse 82, CH-4056 Basel, Switzerland.
IBM Research Division, Almaden Research Center, 650 Harry Road, San Jose, CA 95120, USA.
Science. 2015 Oct 23;350(6259):417-20. doi: 10.1126/science.aac8703.
We combined the high-energy resolution of conventional spin resonance (here ~10 nano-electron volts) with scanning tunneling microscopy to measure electron paramagnetic resonance of individual iron (Fe) atoms placed on a magnesium oxide film. We drove the spin resonance with an oscillating electric field (20 to 30 gigahertz) between tip and sample. The readout of the Fe atom's quantum state was performed by spin-polarized detection of the atomic-scale tunneling magnetoresistance. We determine an energy relaxation time of T1 ≈ 100 microseconds and a phase-coherence time of T2 ≈ 210 nanoseconds. The spin resonance signals of different Fe atoms differ by much more than their resonance linewidth; in a traditional ensemble measurement, this difference would appear as inhomogeneous broadening.
我们将传统自旋共振(这里约为 10 纳电子伏特)的高能量分辨率与扫描隧道显微镜相结合,测量了置于氧化镁薄膜上的单个铁(Fe)原子的电子顺磁共振。我们在针尖和样品之间用振荡电场(20 到 30 千兆赫)驱动自旋共振。通过原子尺度隧道磁电阻的自旋极化检测来读出 Fe 原子的量子态。我们确定了能量弛豫时间 T1≈100 微秒和相位相干时间 T2≈210 纳秒。不同 Fe 原子的自旋共振信号的差异远远大于它们的共振线宽;在传统的集合测量中,这种差异将表现为非均匀展宽。