METHODSCretaceous cores from Site 260 (16°8.67'S, 110°17.92'E); Site 261 (12°56.83'S, 117°53.56'E); and Site 263 (23°19.43'S, 110°57.81'E) were sampled for paleomagnetic measurements. Except for the upper cores from Site 260, which were sampled by pressing the 5.8-cc rectangular sample boxes into the split core face, all samples were cut on a diamond saw. The cores consist of cylindrical pieces of undeformed claystone and siltstone from a few centimeters to tens of centimeters in length. Drilling caused the pieces to rotate horizontally by an unknown amount. Rather than a uniform sampling interval, several adjacent samples from the same piece were often taken to minimize breakup of core material, expedite sampling, and enable comparison of declination data from samples known to have undergone no horizontal rotation relative to each other. Table 1 shows the directions of remanent magnetization and intensities of the samples after 50-oe ac demagnetization. Samples were measured at 5 Hz on a Schonstedt magnetometer. An asterisk in Column 1 indicates that the Schonstedt magnetometer and ac demagnetization apparatus at Massachusetts Institute of Technology were used (see Green and Brecher [this volume] for detailed discussion of these measurements). All other samples were measured using the Schonstedt magnetometer and ac demagnetization apparatus at the University of California at Santa Barbara. Sample Interval in Table 1 is the distance in centimeters from the top of the 2-cm-wide sample to the top of the section. Inclinations (Incl) are given with respect to the present horizontal, positive downward, assuming vertical drill holes; negative inclinations indicate normal polarities for these southern hemisphere cores. Declinations (Decl) are relative only to the split face of the core.
RELIABILITY OF MEASUREMENTSMM and A are measures of the consistency of replicate measurements on a single sample (Doell and Cox, 1965). Values of MM greater than about 30% or of A greater than about 5° indicate that the intensity or direction of magnetization, respectively, are probably unreliable, generally because the sample intensity is near the noise level of the magnetometer or because of instability of sample magnetization. Table 2 shows results of ac demagnetization series on four samples. Little change in direction of magnetization upon demagnetization is apparent, indicating that postdepositional viscous components of magnetization are small. Cumulative intensity changes for these samples (Figure 1) show that a majority of the magnetization resides in domains of high coercive force.Fifty oersted was chosen as the minimum demagnetizing field needed to remove viscous components. Histograms of 50-oe inclinations are generally considerably steeper than the geocentric axial dipole inclinations for the present latitudes of the sites. If a significant viscous component is present in these 50-oe measurements,lower average inclinations and higher average intensities should result for normally polarized samples than for reversely magne...