A Smörgåsbord of Skyrmions: index, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16
10a ε1.0961 ± 0.0001
b0.9999
r2.0606
VD(2579.7,4679.9,5081.8)
UD(356.0,371.9,369.9)
83.6%symD2h [R. Battye and P. Sutcliffe, Phys. Rev. C73, 055205 (2006)]
Can be interpreted as symmetric graphene or a collapsed fullerene.
10b ε1.0965 ± 0.0001
b0.9999
r2.0352
VD(2626.9,4698.7,4728.1)
UD(359.4,361.7,361.3)
0.63%symD3d [R. A. Battye and P. M. Sutcliffe, Rev. Math. Phys. 14, 29-86 (2002)]
Standing upright, the solution has four layers of holes. The layers have 3, 6, 6 and 3 holes each. Similar to the 7a-Skyrmion with an extra layer which stretches it out.
10c ε1.0974 ± 0.0001
b0.9999
r2.3929
VD(1740.7,7589.3,7590.5)
UD(373.5,381.7,382.3)
7.74%symD4d
A slice of the infinite twisted chain. Can be thought of as five 2-tori or a 8a-Skyrmion with an additional torus attached.
10d ε1.0995 ± 0.0001
b0.9999
r2.1797
VD(2267.2,5808.4,5888.0)
UD(384.0,363.7,369.7)
1.69%symC1h
The 7a-Skyrmion with a tetrahedron attached to a face.
10e ε1.0999 ± 0.0001
b0.9999
r2.2237
VD(2216.5,6166.9,6183.6)
UD(366.5,379.3,378.6)
0.04%symC1h
The 7a-Skyrmion with the tetrahedron attached to a face, but rotated with respect to the 10d-Skyrmion solution.
10f ε1.1007 ± 0.0001
b0.9999
r2.2713
VD(2348.9,6119.3,6744.6)
UD(392.3,369.8,381.4)
3.89%symC1h
The 8a-Skyrmion chain with a torus attached on a face with a normal perpendicular to the axis joining the two cubes. The Skyrmions are attached with little matching symmetry.
10g ε1.1011 ± 0.0001
b0.9999
r2.1720
VD(2628.0,5185.6,6077.2)
UD(409.7,361.9,364.2)
2.28%symC1h
A cube attached to a 6-Skyrmion. The 6-Skyrmion has approximate D4h symmetry (rather than the D4d symmetry of the 6a-Skyrmion).
10h ε1.1102 ± 0.0001
b0.9999
r1.9784
VD(3721.7,3724.8,3725.2)
UD(402.9,402.9,402.9)
0.08%symTd [M. Gillard, D. Harland, E. Kirk, B. Maybee and M. Speight,Nucl. Phys. B917, 286-316 (2017)]
A tetrahedral arrangement of single Skyrmions, originally seen in the lightly bound model of Skyrmions [M. Gillard, D. Harland, E. Kirk, B. Maybee and M. Speight,Nucl. Phys. B917, 286-316 (2017)].