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![Top: strain calculated at peak of the second harmonic in the (111) reflection of the LNO, using the strain components given in Table 1, in the cases of single and multiple domain configurations. Middle: difference between single and multiple domains, as a function of wavelength, for the same material and conditions as the top figure. Bottom: difference between single and multiple domains, for four different rods, representing rods with different cross-sections, for the same material and conditions as the top figure. The label “multiple domains” refers to the case corresponding to the top figure, with the addition of a second rod as the domain. The labels “single domain”, “multiple domains for rod 2” and “multiple domains for rod 4” correspond to the three cases where the domains of a single rod are extended to include a second rod, all at the same material properties and conditions as the top figure. \[fig:diff-dlogf\]](Fig-diff-dlogf.pdf){width=”9cm”}

Discussion
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As mentioned in the introduction, Mössbauer spectroscopy is not generally adopted in the evaluation of critical straining of materials, owing to the fact that it is a *nonspectroscopic* method. Our work shows that one may find a suitable compromise by using the second harmonic of an acoustic pulse to measure the strain gradient when a Mössbauer-like spectroscopy can be applied. The second harmonic will oscillate at twice the frequency of the fundamental acoustic pulse, so that both components of strain can be easily measured and that the strain gradient can be identified. The use of a Mössbauer-like spectroscopy also means that the combination of experimental with theoretical results is no longer needed, as it was for the original Mössbauer experiments.

A systematic error evaluation shows that strain measurements based on both the fundamental and the second harmonic can be performed with a precision of about 0.05%. The results, that are comparable to the very low sensitivity of the original Mössbauer
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