†WPI Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan.
‡Faculty of Pure and Applied Sciences, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8571, Japan.
ACS Nano. 2015 Mar 24;9(3):2989-3001. doi: 10.1021/nn507159u. Epub 2015 Feb 20.
Modern field-effect transistors or laser diodes take advantages of band-edge structures engineered by large uniaxial strain εzz, available up to an elasticity limit at a rate of band-gap deformation potential azz (= dEg/dεzz). However, contrary to aP values under hydrostatic pressure, there is no quantitative consensus on azz values under uniaxial tensile, compressive, and bending stress. This makes band-edge engineering inefficient. Here we propose SEM-cathodoluminescence nanospectroscopy under in situ nanomanipulation (Nanoprobe-CL). An apex of a c-axis-oriented free-standing ZnO nanorod (NR) is deflected by point-loading of bending stress, where local uniaxial strain (εcc = r/R) and its gradient across a NR (dεcc/dr = R(-1)) are controlled by a NR local curvature (R(-1)). The NR elasticity limit is evaluated sequentially (εcc = 0.04) from SEM observation of a NR bending deformation cycle. An electron beam is focused on several spots crossing a bent NR, and at each spot the local Eg is evaluated from near-band-edge CL emission energy. Uniaxial acc (= dEg/dεcc) is evaluated at regulated surface depth, and the impact of R(-1) on observed acc is investigated. The acc converges with -1.7 eV to the R(-1) = 0 limit, whereas it quenches with increasing R(-1), which is attributed to free-exciton drift under transversal band-gap gradient. Surface-sensitive CL measurements suggest that a discrepancy from bulk acc = -4 eV may originate from strain relaxation at the side surface under uniaxial stress. The nanoprobe-CL technique reveals an Eg(εij) response to specific strain tensor εij (i, j = x, y, z) and strain-gradient effects on a minority carrier population, enabling simulations and strain-dependent measurements of nanodevices with various structures.
现代场效应晶体管或激光二极管利用大的单轴应变 εzz 工程化的能带边缘结构,其在弹性极限内的能带隙变形势 azz(=dEg/dεzz)的速率可达。然而,与静水压力下的 aP 值相反,在单轴拉伸、压缩和弯曲应力下,并没有关于 azz 值的定量共识。这使得能带边缘工程效率低下。在这里,我们提出了原位纳米操纵下的扫描电子显微镜 - 阴极荧光纳米光谱学(Nanoprobe-CL)。在单轴取向的自由-standing ZnO 纳米棒(NR)的尖端通过弯曲应力的点加载进行偏折,其中局部单轴应变(εcc=r/R)及其在 NR 上的梯度(dεcc/dr=R(-1))由 NR 的局部曲率(R(-1))控制。通过 SEM 观察 NR 弯曲变形周期,依次评估 NR 的弹性极限(εcc=0.04)。电子束聚焦在跨越弯曲 NR 的几个点上,并且在每个点处,从近带边缘 CL 发射能量评估局部 Eg。在受调节的表面深度处评估单轴 acc(dEg/dεcc),并研究 R(-1) 对观察到的 acc 的影响。acc 收敛于 -1.7 eV,与 R(-1)=0 极限,而它随着 R(-1)的增加而猝灭,这归因于横向能带隙梯度下的自由激子漂移。表面敏感的 CL 测量表明,与 bulk acc=-4 eV 的差异可能源自单轴应力下的侧表面应变弛豫。纳米探针 CL 技术揭示了 Eg(εij)对特定应变张量 εij(i,j=x,y,z)和应变梯度对少数载流子群体的响应,从而能够模拟和测量具有各种结构的纳米器件的应变依赖性。