Figure F12. Time serial variation of natural gamma ray (NGR) intensity in Hole 1150D with bandpass filtered components and orbital parameters by Laskar (1993). A. Sedimentation rate (L = low sedimentation rate stage, H = high sedimentation rate stage). B. NGR intensity. C. 20-k.y. bandpass filtering of NGR components. D. Precession index (Laskar, 1993). E. 41-k.y. bandpass filtering of NGR components. F. Obliquity (Laskar, 1993). G. 100-k.y. bandpass filtering of NGR components. H. Eccentricity (Laskar, 1993). I. Power spectral density (PSD) of NGR intensity in each L or H interval (E = periodic components in eccentricity band, O = periodic components in obliquity band, P = periodic components in precession band).

Figure F12. Time serial variation of natural gamma ray (NGR) intensity in Hole 1150D with bandpass filtered components and orbital parameters by Laskar (1993). A. Sedimentation rate (L = low sedimentation rate stage, H = high sedimentation rate stage). B. NGR intensity. C. 20-k.y. bandpass filtering of NGR components. D. Precession index (Laskar, 1993). E. 41-k.y. bandpass filtering of NGR components. F. Obliquity (Laskar, 1993). G. 100-k.y. bandpass filtering of NGR components. H. Eccentricity (Laskar, 1993). I. Power spectral density (PSD) of NGR intensity in each L or H interval (E = periodic components in eccentricity band, O = periodic components in obliquity band, P = periodic components in precession band).