We point out that (TMTSF)(2)PF6 compound at P similar or equal to 6 kbar is
possibly a triplet superconductor with the vector order parameter d = (d(x
) not equal 0, d(y), d(z) = 0). It corresponds to an anisotropic spin susce
ptibility in a superconducting state: chi (b'(z)) = chi (0), chi (a(x)) not
equal chi (0), where chi (0) is its value in a metallic phase. (Here, the
spin quantization axis, z, is parallel to the easy axis, b', of an antiferr
omagnetic SDW phase existing at P = 0). It is shown that the suggested orde
r parameter can explain why the upper critical field along b'-axis (I.J. Le
e, M.J. Naughton, G. Danner, and P.M. Chaikin, Phys. Rev. Lett. 78, 3555 (1
997)) exceeds all paramagnetic limiting fields (including that for a non-un
iform superconductivity) whereas the upper critical field along the a-axis
is restricted by the Pauli paramagnetic effects. The triplet order paramete
r is consistent with the earlier results on a destruction of superconductiv
ity by nonmagnetic impurities and the absence of the Hebel-Slichter peak in
the NMR data as well as with the recent Knight shift measurements by S. Br
own et al and by I. J. Lee et al.