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

  1. The visualization of these eigenvectors is shown in Fig. 6.