Table 5 Table shows bands, subgroups and eigenvectors of M2B2H4 (M = Sc, Y, V, Nb), where the direction of vibration referred as out-of-plane (OP) or in-plane (IP)
From: High-Tc 2D ambient BCS superconductors in hydrogenated transition-metal borides
Band ν | Subgroup | Eigenvec. | Sc2B2H4 | Band ν | Subgroup | Eigenvec. | Y2B2H4 |
|---|---|---|---|---|---|---|---|
4,5 | E1g | Sc:IP | 20.40 | 4,5 | E1g | Y:IP | 13.23 |
6 | A1g | Sc:OP | 28.17 | 6 | A1g | Y:OP | 18.93 |
7 | B2u | H:OP | 44.26 | 7,8 | E1u | B:IP | 37.49 |
8 | B1g | H:OP | 44.37 | 9 | B2u | H:OP | 40.21 |
9,10 | E1u | B:IP | 44.57 | 10 | B1g | H:OP | 42.47 |
11 | A2u | B:OP | 52.40 | 11 | A2u | B:OP | 46.30 |
12 | B1g | B:OP | 81.51 | 12,13 | E2g | B:IP | 65.96 |
13,14 | E2g | B:IP | 90.36 | 14 | B1g | B:OP | 75.81 |
15 | A2u | H:OP | 103.56 | 15 | A2u | H:OP | 99.14 |
16 | A1g | H:OP | 104.06 | 16 | A1g | H:OP | 99.45 |
17,18 | E1u | H:IP | 138.94 | 17,18 | E1u | H:IP | 137.79 |
19,20 | E1g | H:IP | 139.26 | 19,20 | E1g | H:IP | 138.11 |
21,22 | E2u | H:IP | 159.29 | 21,22 | E2u | H:IP | 159.66 |
23,24 | E2g | H:IP | 159.44 | 23,24 | E2g | H:IP | 159.90 |
Band ν | Subgroup | Eigenvec. | V2B2H4 | Band ν | Subgroup | Eigenvec. | Nb2B2H4 |
4,5 | E1g | V:IP | 23.34 | 4,5 | E1g | Nb:IP | 12.60 |
6 | A1g | V:OP | 27.97 | 6 | A1g | Nb:OP | 21.01 |
7,8 | E1u | H:IP | 30.95 | 7,8 | E1u | H:IP | 32.17 |
9,10 | E1g | H:IP | 48.84 | 9,10 | E1g | H:IP | 61.69 |
11,12 | E1u | B:IP | 64.94 | 11,12 | E1u | H:IP | 66.40 |
13 | A2u | B:OP | 65.94 | 13 | A2u | B:OP | 68.40 |
14 | B1g | B:OP | 71.01 | 14 | B1g | B:OP | 69.61 |
15,16 | E2g | H:IP | 80.18 | 15 | B2u | H:OP | 76.24 |
17,18 | E2u | H:IP | 88.50 | 16 | B1g | H:OP | 90.20 |
19 | B2u | H:OP | 102.44 | 17,18 | E2g | B:IP | 95.48 |
20 | A1g | H:OP | 106.17 | 19,20 | E2g | H:IP | 102.73 |
21 | B1g | H:OP | 107.11 | 21 | A1g | H:OP | 111.72 |
22 | A2u | H:OP | 111.05 | 22 | A2u | H:OP | 117.11 |
23,24 | E2g | B:IP | 122.03 | 23,24 | E2u | H:IP | 121.43 |