We report on magnetization measurements performed on a single crystal of Bi 2+x Sr 2−x CuO 6+δ with T c ≈ 7 K for H c-axis. The isofield M (T ) curves show a large reversible region, with a pronounced rounding effect as M approaches zero which prevents the determination of T c (H). Deviations from the linear behavior of magnetisation near T c (H) are studied through the asymptotic behavior of −M (T ) ∝ (T − T a ) m , where m is an exponent and T a an apparent temperature transition. Values of m deviates from the expected mean field value, 1/2, suggesting the importance of phase fluctuations. Resulting values of T a , interpreted as the onset of phase correlations, decrease as field increases showing an upward curvature. Values of T c (H) are obtained through a two-dimensional critical scaling analysis obeyed by many M (T ) curves. The resulting phase diagram do not show upward curvature and lies below the T a (H) line. The value of H c2 (0) estimated from the initial slope dH c2 /dT is twice the value suggested by the phase diagram. Amplitude fluctuations above T a (H) are explained in terms of a Ginzburg-Landau approach extended to high reduced temperatures and magnetic fields by the introduction of a total-energy cutoff in the fluctuation spectrum.