The rotational spectra of cyanoacetylene dimer, HC≡CC≡N HC≡CC≡N, were recorded using Balle-Flygare type Fourier transform microwave (FTMW) spectrometers. The low J transitions were measured down to 1.3 GHz at very high resolution, FWHM ~1 kHz. The spectral hyperfine structure due to the 14 N nuclear quadrupole coupling interactions is wellresolved below 4 GHz using a low frequency spectrometer at the University of Arizona. The experimental spectroscopic constants were fitted as: B 0 = 339.2923310(79) MHz, D J = 32.152(82) Hz, H =-0.00147(20) Hz, eqQ (14 N 1) =-3.9902(14) MHz, and eqQ (14 N 2) =-4.1712(13) MHz. The vibrationally averaged dimer configuration is HC≡CC≡N HC≡CC≡N. Using a simple linear model, the vibrational ground state and the equilibrium hydrogen bond lengths are determined to be: r 0 (N H) = 2.2489(3) Å and r e (N H) = 2.2315 Å. The equilibrium centerof-mass distance between the two HCCCN subunits is com r = 7.0366 Å. Using the rigid procession model, the vibrational ground state center-of-mass distance and the pivot angles which HCCCN subunits make with the a-axis of HC≡CC≡N HC≡CC≡N are. .m c r = 7.0603 Å, 1 = 13.0, and 2 = 8.7, respectively. The calculated hydrogen bond energy of HC≡CC≡N HC≡CC≡N is 1466 cm-1 using the MP2/aug-cc-PVTZ method in present work.