Fluctuation effects in underdoped cuprates under high fields are examined by trying to fit theoretical results to resistivity and Nernst data in vortex states. The superconducting (SC) fluctuation in underdoped cuprates includes not only the ordinary thermal contribution but also a large amount of quantum dynamical contributions. Together with this, the presence of a SC pseudogap region T0 − Tc0 increasing with underdoping is found to be the origin of the Nernst coefficient becoming anomalously smaller and the in-plane coherence length apparently increasing with underdoping.It has been well understood that the field-induced fanshaped broadenings of curves of resistivity and thermodynamic quantities, typically seen in optimally (hole-)doped high T c0 cuprate superconductors (HTS), are thermal superconducting (SC) fluctuation phenomena mainly in the vortex liquid region of the normal phase below the zero field (H = 0) transition point T c0 [1]. In applied magnetic fields of tesla range perpendicular to the SC planes, the in-plane resistivity and other physical quantities in these materials show familiar behaviors [2, 3] correlated with one another. For instance, the onset temperature of fluctuation effects suggested from resistive data is almost the same as the corresponding one of thermodynamic and thermomagnetic data. This familiar correlation is typically seen in much lower fields than H c2 (0), where the fluctuation is purely thermal [2], and the quantum fluctuation contribution is negligible.In contrast, the resistivity in other HTSs with lower T c0 often behaves in an uncorrelated manner with thermodynamic quantities. Typically, as the applied field is higher, resistivity data in electron-doped HTSs and some of over (hole-)doped materials show not the fan-shaped [1] but a flat curve [4,5] following the in-plane normal resistivity ρ n (T ) = (σ n (T )) −1 curve until a vortexglass (VG) transition field, lying much below [5,6] an effective H c2 (T ) determined thermodynamically, is approached from above. In over (hole)-doped materials with high σ n -value (≃ 10 2 (R q s) −1 [4]), such an absence of correlation is not surprising because the fluctuation conductivity σ f is negligible compared with σ n in the total conductivity σ = σ n + σ f over a wide temperature range, where R q = 6.45(kΩ) is resistance quantum, and s ≃ 10(A) is a typical size of the spacing between SC layers. However, the corresponding uncorrelated behavior seen in the electron-doped materials [5] with σ n of the same order as in the optimally doped YBCO [3] is intrinsic, and its origin needs to be attributed to a fluctuation property. Similar behaviors have been also found in overdoped La 2−x Sr x CuO 4 (LSCOx) [7] and κ-(ET) 2 organic superconductors [8,9]. As argued elsewhere [10] by fitting to data [9], the main origin is expected to consist in the quantum dynamical nature, enhanced with increasing the field, of the SC fluctuation. In general, σ f defined in a Ginzburg-Landau (GL) theory decreases [11]