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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-02-26 20:57:59 -0500 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-02-26 20:57:59 -0500 |
| commit | def56efbc5d788f88cd2021a3fd3f915ec1e22d3 (patch) | |
| tree | c129dc425afd2f14e44042ea71337978c0e7f8ea | |
| parent | 21f3c3601b70742c8d718e782f1a6bd7e96d8b70 (diff) | |
| download | aps_mm_2020-def56efbc5d788f88cd2021a3fd3f915ec1e22d3.tar.gz aps_mm_2020-def56efbc5d788f88cd2021a3fd3f915ec1e22d3.tar.bz2 aps_mm_2020-def56efbc5d788f88cd2021a3fd3f915ec1e22d3.zip | |
clarification on modulus tensor
| -rw-r--r-- | poster_aps_mm_2020.tex | 4 |
1 files changed, 2 insertions, 2 deletions
diff --git a/poster_aps_mm_2020.tex b/poster_aps_mm_2020.tex index d63be44..90e3794 100644 --- a/poster_aps_mm_2020.tex +++ b/poster_aps_mm_2020.tex @@ -109,8 +109,8 @@ \hspace{1em} Resonant ultrasound spectroscopy drives a sample with sound and measures its resonances by looking for spikes in the response. Using the sample geometry - and the location of sufficiently many resonances, the modulus tensor $C$ - can be calculated. + and the location of sufficiently many resonances, the modulus tensor + $C$---which gives the energetic cost of strain---can be calculated. \textbf{ The structure of the modulus tensor and its temperature dependence yield a lot of information about symmetry breaking. |