<?xml version='1.0' encoding='utf-8'?>
<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:contributor>B. Moskowitz</dc:contributor>
  <dc:contributor>J. Rosenbaum</dc:contributor>
  <dc:contributor>Catherie Kissel</dc:contributor>
  <dc:creator>M. Jackson</dc:creator>
  <dc:date>1998</dc:date>
  <dc:description>AC susceptibility measurements as a function of field amplitude Hac and of frequency show a strong field dependence for a set of synthetic titanomagnetites (Fe3-xTixO4) and for certain basalts from the SOH-1 Hawaiian drill hole and from Iceland. In-phase susceptibility is constant below fields of about 10-100 A/m, and then increases by as much as a factor of two as Hsc is increased to 2000 A/m. Both the initial field-independent susceptibilities and field-dependence of susceptibility are systematically related to composition: initial susceptibility is 3 SI for a single-crystal sphere of TMO (x = 0) and decreases with increasing titanium content; field-dependence is nearly zero for TM0 and increases systematically to a maximum near TM60 (x = 0.6). This field dependence can in some cases be mistaken for frequency dependence, and leaf to incorrect interpretations of magnetic grain size and composition when titanomagnetite is present.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1016/S0012-821X(98)00032-6</dc:identifier>
  <dc:language>en</dc:language>
  <dc:title>Field-dependence of AC susceptibility in titanomagnetites</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>