Table 1 Structural refinements

From: Charge-density-wave quantum critical point under pressure in 2H-TaSe2

 

Hexagonal

Hexagonal

HexagonalCDW

Hexagonal

Hexagonal

Pressure (GPa)

0.3

0.3

0.3

15.3

15.5

Temperature (K)

150

40

40

40

80

Space group

\(P{6}_{3}/{mmc}\)

\(a({{\text{\AA}}})\)

3.42621(9)

3.42441(9)

10.27599(14)

3.2961(2)

3.29460(15)

\(b({{\text{\AA}}})\)

3.42621(9)

3.42441(9)

10.27599(14)

3.2961(2)

3.29460(15)

\(c({{\text{\AA}}})\)

12.579(7)

12.574 (7)

12.569(3)

11.383(14)

11.362(9)

\({V}^{3}\left({{\text\AA} }^{3}\right)\)

127.88(7)

127.70(7)

1149.4(3)

107.10(14)

106.81(9)

\(\alpha\)(°)

90

\(\beta\)(°)

90

\(\gamma\)(°)

120

\({R}_{{{\mathrm{int}}}}\) (%)

1.9

3.1

2.3

2.4

5.2

\({R}_{1}\)/wR2 (%)

1.36/1.55

1.44/1.54

2.17/2.63

1.84/1.88

3.78/4.77

  1. Overview of the unit cell, space group, lattice parameters (a, b, and c), angles (α, β, and γ), and R factors for a representative set of pressure–temperature values. Bold denotes a refinement taking into account the CDW 3 × 3 supercell at low pressure. The other refinements were done disregarding the superlattice peaks. The detailed pressure dependence of the z parameter (Se place) for the refinements of the high-temperature unit cell is displayed in Fig. 4d. All x,y,z parameters (Se places) for the supercell, crystallographic information files (CIF) for the refinements shown here and a more detailed table for all measured data sets can be found in the KITopen data repository46.