Heat capacity measurements on the recently discovered geometrically frustrated β-pyrochlore superconductor RbOs2O6 (Tc = 6.4 K) yield a Sommerfeld coefficient of 44 mJ/mol f.u. /K 2 . This is about 4 times larger than the one found in band structure calculations. In order to specify the enhancement due to electron-electron interactions, we have measured the electron-phonon enhancement. By a suitable analysis, an electron-phonon coupling constant λep = 1 ± 0.1 is derived from the specific heat jump at Tc. This leaves a significant additional λ add = 2.1 ± 0.3 for enhancement due to other mechanisms, possibly related to the triangular lattice. To arrive at these results, an appropriate analysis method for bulk thermodynamic data based on the condensation energy was applied.Key words: RbOs2O6, superconductivity, correlation, DOS enhancement, thermodynamic properties PACS: 74.25. Bt; 71.27.+a; Long standing interest in the pyrochlores stems from their inherent geometrical frustration due to the metal ions forming a network of corner-sharing tetrahedra. Thus, metallic pyrochlores constitute ideal systems to study to what degree itinerant electrons are affected by a lattice which is known to cause geometrical frustration for interactions among localized magnetic moments. For similar reasons, the superconductivity recently found in RbOs2O6 has been of considerable interest. RbOs2O6 is one of only four pyrochlore superconductors known to date. These are the α-pyrochlore Cd2Re2O7 and the β-pyrochlores AOs2O6, where A = Cs, Rb, or K. [1,2,3] RbOs2O6 is a conventional s-wave superconductor with a critical temperature Tc = 6.4 K. [4,5,6,7] In this short paper, we provide evidence for an additional electronic mass enhancement beyond the contribution from the coupling to phonons. Specific heat measurements on RbOs2O6 show that the residual Sommerfeld coefficient in the superconducting state γr and the normal-state coefficient γ vary among the various samples measured. The variation is consistent with the presence of a second metallic component, and subsequent x-ray diffraction analysis has confirmed the presence of OsO2 in the samples. We have therefore developed a suitable quantitative method to analyze thermodynamic data when dealing with a superconducting sample containing a metallic second phase. Since the analysis is based on the condensation energy of the superconductor of interest, we call it condensation energy analysis (CEA). It involves integrating the heat capacity to obtain the condensation energy which is a reliable measure of the superconducting fraction. From the systematic variation of the thermodynamic parameters on the superconducting fraction it is possible to extract the properties of the pure sample. [7] According to the CEA, the superconducting electronic specific heat Ces is extracted from the measurement by Ces(T ) = η −1 m ∆Cp + γ1T . Here, ηm is the superconducting mass fraction, ∆Cp = C0 T − C12 T is the difference in heat capacity between the superconducting and normal state, and γ1 is the ...