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Figure 2
The deformation of the basis v1 = (1, 0), v2 = (−t, 2) for t ∈ [0, 1] defines a continuous loop of lattices. The basis v1, v2 is reduced for [t\in[0,{{1} \over {2}})] but after [t = {{1} \over {2}}] switches to a non-equivalent (up to rigid motion) reduced basis v1, v0 = (t − 1, −2).

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ISSN: 2053-2733
Volume 79| Part 1| January 2023| Pages 1-13
https://doi.org/10.1107/S2053273322010075
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