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c, apart from degeneracies, define the breaking segment.
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The value of 334 GPa mentioned in the Introduction was for an area at 4 K.
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The reader, who would like to use the presented scheme, is cautioned that for very low strains the transition state is found in a larger unit cell: going to lower strains, the breaking bond will at a certain point increase more (it can go to infinity) than the all other bonds will shrink, since they have to have positive strain. This implies that there is a minimal length L*, below which no transition state exists.
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An additional correction to the dynamical matrix has been applied since residual interchain interactions led to a spurious imaginary rotation mode in the spectra. The calculated force constants are adjusted in such a way that only the energy of this specific mode was shifted to zero at Γ.
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