Molecule | Lattice I | T_{m} (°C) | d_{I} (nm) | Lattice II | d_{II} (nm) | Μ |

1 | Triclinic crystal | 138 | — | Disordered | — | — |

2a | Lamellae | 145 | 4.50 | A15 | 13.2* | 38/50§ |

2b | Lamellae | 144 | 4.60 | A15 | 14.2* | 46/61§ |

2c | Lamellae | 146 | 4.67 | A15 | 14.6* | 49/65§ |

2d | Lamellae | 126 | 4.50 | bcc | 8.2* | 44§ |

3a | Lamellae | 177 | 5.40 | Double gyroid | 6.35 | — |

3b | Lamellae | 172 | 5.90 | Lamellae | 6.40† | — |

3c | Lamellae | 180 | 6.00 | Lamellae | 7.30† | — |

4a | Disordered | — | — | Cylinder | 6.22‡ | 6.7# |

4b | Disordered | — | — | Cylinder | 6.28‡ | 6.6# |

4c | Disordered | — | — | Cylinder | 6.70‡ | 7.4# |

*Dimensions of the A15 or bcc unit cells.

†Lamellar periodicities in supramolecular lattice II.

‡The corresponding principal (01) spacing between the cylinders in the honeycomb-like hexagonal lattices.

§Calculated numbers of giant tetrahedra in two types of spheres in the A15 lattice (the size ratios of two types of spheres in **2b** and **2c** are assumed to be 1.1, the same as in **2a**) or in each sphere in the bcc lattice.

#Average number of giant tetrahedra within 1-nm-thick cross section of the cylinders in the honeycomb-like hexagonal supramolecular lattices.