Lan Fanli, Chen Hongyan, Lin Hanxuan, Bai Yu, Yu Yang, Miao Tian, Zhu Yinyan, Ward T Z, Gai Zheng, Wang Wenbin, Yin Lifeng, Plummer E W, Shen Jian
State Key Laboratory of Surface Physics and Department of Physics, Fudan University, 200433 Shanghai, China.
Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831.
Proc Natl Acad Sci U S A. 2019 Mar 5;116(10):4141-4146. doi: 10.1073/pnas.1819641116. Epub 2019 Feb 20.
Characterization of the onset of a phase transition is often challenging due to the fluctuations of the correlation length scales of the order parameters. This is especially true for second-order structural-phase transition due to minute changes involved in the relevant lattice constants. A classic example is the cubic-to-tetragonal second-order phase transition in SrTiO (STO), which is so subtle that it is still unresolved. Here, we demonstrate an approach to resolve this issue by epitaxially grown rhombohedral LaSrMnO (LSMO) thin films on the cubic STO (100) substrate. The shear strain induced nanotwinning waves in the LSMO film are extremely sensitive to the cubic-to-tetragonal structural-phase transitions of the STO substrate. Upon cooling from room temperature, the development of the nanotwinning waves is spatially inhomogeneous. Untwinned, atomically flat domains, ranging in size from 100 to 300 nm, start to appear randomly in the twinned phase between 265 and 175 K. At ∼139 K, the untwinned, atomically flat domains start to grow rapidly into micrometer scale and finally become dominant at ∼108 K. These results indicate that the low-temperature tetragonal precursor phase of STO has already nucleated at 265 K, significantly higher than the critical temperature of STO (∼105 K). Our work paves a pathway to visualize the onset stages of structural-phase transitions that are too subtle to be observed using direct-imaging methods.
由于序参量相关长度尺度的涨落,表征相变的起始通常具有挑战性。对于二阶结构相变而言尤其如此,因为相关晶格常数的变化非常微小。一个经典的例子是SrTiO(STO)中从立方相到四方相的二阶相变,其非常微妙以至于仍未得到解决。在这里,我们展示了一种通过在立方STO(100)衬底上外延生长菱面体LaSrMnO(LSMO)薄膜来解决这个问题的方法。LSMO薄膜中由剪切应变诱导的纳米孪晶波对STO衬底从立方相到四方相的结构相变极其敏感。从室温冷却时,纳米孪晶波的发展在空间上是不均匀的。尺寸从100到300纳米不等的未孪晶、原子级平整的畴在265到175 K之间的孪晶相中开始随机出现。在约139 K时,未孪晶、原子级平整的畴开始迅速生长到微米尺度,并最终在约108 K时占主导地位。这些结果表明,STO的低温四方前驱相在265 K时就已经形核,远高于STO的临界温度(约105 K)。我们的工作为可视化结构相变的起始阶段铺平了道路,这些阶段过于微妙,无法用直接成像方法观察到。