Upper critical field Hc2 in Bechgaard salts (TMTSF)2PF6

PMC Physics B

Table 1 Summary of results. Here $ρ_{0} (0) = \frac{{\hat{v}}^{2} e H_{c 2} (0)}{2 {(2 π T_{c})}^{2}}$ and $h (0) = \frac{H_{c 2} (0)}{\frac{\partial H_{c 2} (t)}{\partial t} |_{t} = 1}$

	symmetry	C(0)	C(1)	$- \frac{\partial ρ}{\partial t} \|_{t} = 1$	ρ₀(0)	h(0)
$\vec{H} \| \| {\vec{b}}^{'}$	p-wave	-0.031	0	0.2377	0.1583	0.6659
	chiral p-wave	-0.2247	-0.3660	0.3838	0.2734	0.71324
	chiral f'-wave	-0.2247	-0.3660	0.5181	0.3734	0.72073
$\vec{H} \| \| \vec{a}$	p-wave	-0.017	0	0.2377	0.1751	0,7366
	chiral p-wave	-0.066	-0.028	0.2126	0.1396	0,6566
	chiral f-wave	-0.066	-0.035	0.2744	0.1920	0.6997
	chiral f'-wave	-0.1019	-0.05	0.2910	0.2090	0,7182