Electronic spectra of C 6 H are measured in the 18 950´21 100 cm´1 domain using cavity ring-down spectroscopy of a supersonically expanding hydrocarbon plasma. In total, 19 (sub)bands of C 6 H are presented, all probing the vibrational manifold of the B 2 Π electronically excited state. The assignments are guided by electronic spectra available from matrix isolation work, isotopic substitution experiments (yielding also spectra for 13 C 6 H and C 6 D), predictions from ab initio calculations as well as rotational fitting and vibrational contour simulations using the available ground state parameters as obtained from microwave experiments. Besides the 0 0 0 origin band, three non-degenerate stretching vibrations along the linear backbone of the C 6 H molecule are assigned: the ν 6 mode associated with the C-C bond vibration and the ν 4 and ν 3 modes associated with C"C triple bonds. For the two lowest ν 11 and ν 10 bending modes, a Renner-Teller analysis is performed identifying the µ 2 Σ(ν 11 ) and both µ 2 Σ(ν 10 ) and κ 2 Σ(ν 10 ) components. In addition, two higher lying bending modes are observed, which are tentatively assigned as µ 2 Σ(ν 9 ) and µ 2 Σ(ν 8 ) levels. In the excitation region below the first non-degenerate vibration (ν 6 ), some 2 Π´2Π transitions are observed that are assigned as even combination modes of low-lying bending vibrations. The same holds for a 2 Π´2Π transition found above the ν 6 level. From these spectroscopic data and the vibronic analysis a comprehensive energy level diagram for the B 2 Π state of C 6 H is derived and presented.