Table 1 Thermoelectric properties

From: Phonon transport manipulation in TiSe2 via reversible charge density wave melting

T, [K]

\({\kappa }_{ph}\left[\frac{{\rm{W}}}{{\rm{m}}\cdot {\rm{K}}}\right]\)

\({\kappa }_{el}\left[\frac{{\rm{W}}}{{\rm{m}}\cdot {\rm{K}}}\right]\)

\(\sigma \left[\frac{{\rm{S}}}{{\rm{m}}}\right]\)

\({S}_{el}\left[\frac{{\rm{V}}}{{\rm{K}}}\right]\)

ZT

184.984

8.581

4.039 × 10−1

1.027 × 105

1.232 × 10−4

3.209 × 10−2

184.988

8.609

4.077 × 10−1

1.045 × 105

1.242 × 10−4

3.307 × 10−2

185.126

8.809

4.117 × 10−1

1.050 × 105

1.237 × 10−4

3.226 × 10−2

186.876

1.080 × 101

4.321 × 10−1

1.053 × 105

1.196 × 10−4

2.507 × 10−2

  1. Lattice thermal conductivity (κph), electronic thermal conductivity (κel), diffusive Sebeeck coefficient (Sel), electrical conductivity (σ), and thermoelectric figure of merit (ZT) for 1 × 1 1L-TiSe2 for four different temperatures (T).
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