text stringlengths 0 205 |
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so what you see is only at really low |
temperature |
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temperature |
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temperature |
um is the electronic thermal expansion |
align:start position:0% |
um is the electronic thermal expansion |
align:start position:0% |
um is the electronic thermal expansion |
important in these materials now why is |
align:start position:0% |
important in these materials now why is |
align:start position:0% |
important in these materials now why is |
it so important here anybody know |
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align:start position:0% |
it's actually because the phoneon one is |
align:start position:0% |
it's actually because the phoneon one is |
align:start position:0% |
it's actually because the phoneon one is |
really small remember this is the ratio |
align:start position:0% |
really small remember this is the ratio |
align:start position:0% |
really small remember this is the ratio |
of the two um when you're at really low |
align:start position:0% |
of the two um when you're at really low |
align:start position:0% |
of the two um when you're at really low |
temperature the thermal expansion is |
align:start position:0% |
temperature the thermal expansion is |
align:start position:0% |
temperature the thermal expansion is |
very small in general and the reason is |
align:start position:0% |
very small in general and the reason is |
align:start position:0% |
very small in general and the reason is |
you're essentially harmonic in your |
align:start position:0% |
you're essentially harmonic in your |
align:start position:0% |
you're essentially harmonic in your |
phone on degrees of freedom so you have |
align:start position:0% |
phone on degrees of freedom so you have |
align:start position:0% |
phone on degrees of freedom so you have |
almost no thermal expansion you know if |
align:start position:0% |
almost no thermal expansion you know if |
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almost no thermal expansion you know if |
you have fully harmonic vibrations |
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