A Smörgåsbord of Skyrmions: index, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16
11a ε1.0957 ± 0.0001
b0.9999
r2.3915
VD(2475.2,8018.3,8021.6)
UD(421.5,402.7,405.6)
33.4%symC1h
The 7a-Skyrmion with the cube attached to a face. The reflection plane of the cube and icosahedron match.
11b ε1.0964 ± 0.0001
b0.9999
r2.4314
VD(2455.5,8353.5,8354.9)
UD(434.6,401.2,398.6)
0.03%sym
The 7a-Skyrmion with the cube attached to a face. The icosahedral Skyrmion has a C2 symmetry around a vector which lies in one of the cubes' reflection planes. This is not a reflection plane of the icosahedron and so the overall configuration has no symmetry.
11c ε1.0982 ± 0.0001
b0.9999
r2.1759
VD(3352.7,5365.9,6560.8)
UD(429.6,402.5,394.5)
26.2%symC1h [R. Battye and P. Sutcliffe, Phys. Rev. C73, 055205 (2006)]
Symmetric graphene.
11d ε1.0983 ± 0.0001
b0.9999
r2.1458
VD(3401.5,5273.4,6183.1)
UD(415.1,394.3,401.1)
6.97%symC2v
Symmetric graphene.
11e ε1.0985 ± 0.0001
b0.9999
r2.2329
VD(2883.4,6180.5,7088.6)
UD(418.9,401.4,405.4)
11.5%symC1h
Symmetric graphene.
11f ε1.0986 ± 0.0001
b0.9999
r2.1983
VD(3111.6,5700.8,6819.4)
UD(422.9,402.9,398.6)
0.03%sym
Asymmetric graphene.
11g ε1.0986 ± 0.0001
b0.9999
r2.5802
VD(1940.5,9895.1,9957.5)
UD(407.6,418.0,425.9)
0.14%symC1h
A natural extension of the 9d solution. The 8a-Skyrmion chain with the tetrahedron attached at the end of the chain.
11h ε1.0987 ± 0.0001
b0.9999
r2.1298
VD(4214.7,4223.2,6206.1)
UD(413.6,398.6,398.9)
0.10%symD3h [R. M. Battye and P. M. Sutcliffe, Phys. Rev. Lett. 86, 3989-3992 (2001)]
Highly symmetric graphene.
11i ε1.0987 ± 0.0001
b0.9999
r2.3737
VD(2796.1,7312.3,8181.3)
UD(403.5,422.1,426.7)
7.38%symC2v
Two cubes joined by the tetrahedron with each cube attached to adjacent faces of the tetrahedron.
11j ε1.0987 ± 0.0001
b0.9999
r2.1839
VD(3209.4,5517.8,6696.0)
UD(424.9,395.4,401.5)
0.03%sym
Asymmetric graphene.
11k ε1.0991 ± 0.0001
b0.9999
r2.4889
VD(2342.8,8684.2,9163.4)
UD(428.6,407.4,415.7)
0.48%symC1h
The 8b-Skyrmion chain sharing a corner with the cube.
11l ε1.0998 ± 0.0001
b0.9999
r2.1463
VD(3824.3,4650.2,6298.6)
UD(398.0,418.5,421.4)
2.85%symC1h
Out-of-phase graphene with a single Skyrmion attached on the side. Note that there is no stable out-of-phase graphene solution with B=10, the 1-Skyrmion stabilizes the configuration.
11m ε1.1007 ± 0.0001
b0.9999
r2.4012
VD(2320.3,8053.7,8431.8)
UD(436.8,404.3,407.9)
0.48%symC2h
Two cubes joined by a 3-torus to become a chain.
11n ε1.1010 ± 0.0001
b0.9999
r2.3902
VD(2362.6,7947.5,8339.6)
UD(402.0,421.0,424.0)
0.34%sym
Two cubes joined by a 3-torus to become a chain, but with one cube rotated by 45° relative to the other.
11o ε1.1018 ± 0.0001
b0.9999
r2.4591
VD(2438.4,8375.3,8961.7)
UD(433.8,404.2,416.8)
0.03%sym
A weakly bound cluster of the 6a-Skyrmion and the 5a-Skyrmion. Almost has one reflection symmetry in the plane of the paper.
11p ε1.1078 ± 0.0001
b0.9999
r2.0730
VD(3914.4,4403.9,5404.1)
UD(412.1,436.3,434.5)
0.03%symC2v
Six (out of twelve) faces of a the dodecahedral 7a-Skyrmion form a shell with three single Skyrmions partially tucked inside.