Table 2. Predicted carrier mobility.

Carrier type	NL	mx*/m0	my*/m0	E1x	E1y	Cx_2D	Cy_2D	μx_2D	μy_2D
		G–X	G–Y	(eV)		(J m−2)		(103 cm2 V−1 s−1)
e	1	0.17	1.12	2.72±0.02	7.11±0.02	28.94	101.60	1.10–1.14	~0.08
	2	0.18	1.13	5.02±0.02	7.35±0.16	57.48	194.62	~0.60	0.14–0.16
	3	0.16	1.15	5.85±0.09	7.63±0.18	85.86	287.20	0.76–0.80	0.20–0.22
	4	0.16	1.16	5.92±0.18	7.58±0.13	114.66	379.58	0.96–1.08	0.26–0.30
	5	0.15	1.18	5.79±0.22	7.35±0.26	146.58	479.82	1.36–1.58	0.36–0.40
h	1	0.15	6.35	2.50±0.06	0.15±0.03	28.94	101.60	0.64–0.70	10–26
	2	0.15	1.81	2.45±0.05	1.63±0.16	57.48	194.62	2.6–2.8	1.3–2.2
	3	0.15	1.12	2.49±0.12	2.24±0.18	85.86	287.20	4.4–5.2	2.2–3.2
	4	0.14	0.97	3.16±0.12	2.79±0.13	114.66	379.58	4.4–5.2	2.6–3.2
	5	0.14	0.89	3.40±0.25	2.97±0.18	146.58	479.82	4.8–6.4	3.0–4.6

2D, two-dimensional.

Carrier types ‘e’ and ‘h’ denote ‘electron’ and ‘hole’, respectively. N_L represents the number of layers, m_x* and m_y* are carrier effective masses for directions x and y, respectively, E_1x (E_1y) and C_{x_2D} (C_{y_2D}) are the deformation potential and 2D elastic modulus for the x (y) direction. Mobilities μ_{x_2D} and μ_{y_2D} were calculated using equation (1) with the temperature T set to 300 K.