We report a thorough characterization of the glassy dynamics of benzophenone by broadband dielectric spectroscopy. We detect a well pronounced β relaxation peak developing into an excess wing with increasing temperature. A previous analysis of results from Optical-Kerr-effect measurements on this material within the mode coupling theory revealed a highfrequency Cole-Cole peak. We address the question if this phenomenon also may explain the Johari-Goldstein β relaxation, a so far unexplained spectral feature inherent to glass-forming matter, mainly observed in dielectric spectra. Our results demonstrate that according to the present status of theory, both spectral features seem not to be directly related.PACS numbers: 64.70. Pf, 77.22.Gm Aside of the α relaxation, characterizing the slowing down dynamics during the glass transition, glassy matter reveals a rich variety of further, so far only poorly understood dynamic processes [1,2,3]. Among the most prominent ones is the socalled Johari-Goldstein (JG) β relaxation [4]. In spectra of the imaginary part of the susceptibility χ" (the "loss") it shows up as second peak at a frequency beyond the α relaxation. It is inherent to the glassy state of matter but its microscopic origin still is controversially discussed. Even if superimposed by a dominating α relaxation, it still may show up in the loss as a socalled excess wing [5]. This long known feature [2,3,6,7] only recently was discovered to be due to a second relaxation peak [8].The most prominent theory of the glass transition is the mode coupling theory (MCT) [9]. It predicts a so-called fast β relaxation, showing up in the GHz -THz range, which was experimentally verified in numerous investigations [10]. It is envisioned by the rattling motion of a particle in the cage formed by the surrounding particles. It should be noted that this fast β process usually is presumed not to be identical with the JG β relaxation, sometimes also termed "slow β process". In the basic versions of MCT, a combination of two asymptotic power laws is predicted to describe the data in the regime of the fast process, with both exponents determined by a system parameter λ. They form a shallow minimum in the frequency-dependent loss, followed by the so-called microscopic peak located in the THz range [ Fig. 1(a)]. Some consensus seems to develop in the glass community that MCT is the correct description for high temperatures, T > T c . The critical temperature T c can be regarded as idealized glass-transition temperature often roughly located at 1.2 T g with T g the experimental glass temperature. The original MCT only revealed three characteristic spectral features, the α relaxation, the minimum, and the microscopic peak. The high-frequency flank of the α relaxation peak directly crosses over into the low-frequency wing of the minimum, the so-called von-Schweidler law ν -b [ Fig. 1(a)]. At high temperatures this is in accord with experimental observations. However, excess wing or JG β peak developing at lower temperatures seemed not t...