We report efficient direct optoelectronic generation of sub-ps-THz pulses on 50 ⍀ coaxial transmission lines with a 330 m diameter solid copper outer tube filled with Teflon containing the 80 m diameter inner conductor. The transmitted pulses after propagating as much as 105 mm were measured at the end of the line with an optoelectronic antenna having sub-ps-time resolution. We observed low-loss, single transverse electromagnetic mode propagation with very little group velocity dispersion. Recently, efficient broadband coupling of freely propagating pulses of THz electromagnetic radiation into circular and rectangular metal waveguides has been demonstrated. 1,2 Single-mode coupling and propagation were achieved for these waveguides, and thereby demonstrated much larger bandwidths with 1/10 the loss of lithographically defined coplanar transmission lines. 3 Although these waveguides are quite useful for narrow band or THz time-domain spectroscopy (THz-TDs) applications, they all have very high group velocity dispersion (GVD), which make them incapable of sub-ps-pulse propagation.The excessive broadening of sub ps THz pulses by these waveguides is caused by the extreme GVD near the cutoff frequencies. [1][2][3] This excessive pulse broadening would not occur for the transverse electromagnetic (TEM) modes of a two-wire transmission line, a coaxial transmission line, or a metal parallel-plate waveguide (PPWG), that do not have a cutoff frequency. The group and phase velocities of these TEM modes are determined solely by the surrounding dielectric. Unfortunately, quasioptic coupling techniques are not effective for the complex field patterns of the TEM modes of the two wire or the coaxial transmission lines. However, efficient coupling is possible for the simple field pattern of the TEM mode of the metal PPWG and has been recently reported. 4 In a more recent demonstration, 0.22 ps THz input pulses to a flexible Cu PPWG were observed to broaden only to 0.39 ps after propagating 250 mm. 5 The minimal broadening of the output pulses was due to the absorption of the higher frequency components of the pulse by the waveguide due to the finite conductivity of Cu. Consequently, a THz interconnect capable of propagating sub-ps-pulses with minimal loss and little distortion has been realized. 3 Here, in the continuing search for the ideal THz interconnect, we report the first optoelectronic generation of subps-THz pulses launched directly into commercial sub-mmdiameter coaxial transmission lines and the optoelectronic measurement of the propagated pulses. These THz pulses were then used to characterize the frequency response of the coaxial lines by THz-TDS from 0.05 to 1 THz, the broadest bandwidth and highest frequency characterization of coaxial transmission lines to date.For completeness we note the earlier work on the transfer of shorter than 5 ps pulses to and between coplanar and coaxial devices, 6 and the optoelectronic characterization of a microwave probe up to 400 GHz. 7 Also, the related and unusual observations of...