There is a debate as to the identity of the fluctuations which constitute the relatively high-frequency plasma turbulence observed in the solar wind. One school holds that these modes are kinetic Alfvén waves, whereas another opinion is that they are whistler modes. Here linear kinetic theory for electromagnetic fluctuations in homogeneous, collisionless, magnetized plasmas is used to compute two dimensionless transport ratios, the electron compressibility C_e and the magnetic compressibility C _$\parallel$ for these two modes. The former is a measure of the amplitude of density fluctuations, and the latter indicates the relative energy in magnetic fluctuations in the component parallel to the background magnetic field B_o. For β_e $\ll$ 1, [C _$\parallel$ ]_Alfven $\ll$ [C _$\parallel$ ]_whistler, and the latter quantity is of order 0.5 at whistler propagation strongly oblique to B_o. Such values of C _$\parallel$ are sometimes measured at relatively high frequencies and β_e $\ll$ 1 in the solar wind; thus, it is concluded that such observations correspond to whistler mode turbulence. But other solar wind observations indicate that kinetic Alfvén fluctuations also contribute to relatively high-frequency solar wind turbulence.