![](data:image/png;base64,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)
(vi) Complex Volumes and Cusp Shapes
Solutions to I
u
1
√
−1(vol +
√
−1CS) Cusp shape
u = −0.153909 + 1.134970I
a = 0.417347 + 1.214000I
b = 1.49588 − 1.44581I
1.12873 + 4.25478I 0
u = −0.153909 − 1.134970I
a = 0.417347 − 1.214000I
b = 1.49588 + 1.44581I
1.12873 − 4.25478I 0
u = −0.178162 + 1.177710I
a = −0.495039 − 1.310920I
b = −1.68518 + 1.60196I
2.58467 − 1.25382I 0
u = −0.178162 − 1.177710I
a = −0.495039 + 1.310920I
b = −1.68518 − 1.60196I
2.58467 + 1.25382I 0
u = 0.692151 + 0.390660I
a = −2.83083 + 0.45729I
b = −2.42917 + 0.16265I
−1.15801 + 12.77270I 5.19545 − 9.98793I
u = 0.692151 − 0.390660I
a = −2.83083 − 0.45729I
b = −2.42917 − 0.16265I
−1.15801 − 12.77270I 5.19545 + 9.98793I
u = −0.655533 + 0.444833I
a = −0.568758 + 0.309874I
b = −0.165875 + 0.683566I
−4.78712 − 0.77055I 4.27518 − 2.02219I
u = −0.655533 − 0.444833I
a = −0.568758 − 0.309874I
b = −0.165875 − 0.683566I
−4.78712 + 0.77055I 4.27518 + 2.02219I
u = −0.622505 + 0.481239I
a = 0.245787 − 0.637722I
b = −0.380467 − 0.619541I
−4.93263 − 3.45869I 3.45815 + 8.17533I
u = −0.622505 − 0.481239I
a = 0.245787 + 0.637722I
b = −0.380467 + 0.619541I
−4.93263 + 3.45869I 3.45815 − 8.17533I
5