<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:creator>Schultze, Volkmar</dc:creator>
  <dc:creator>Schillig, Bastian</dc:creator>
  <dc:creator>IJsselsteijn, Rob</dc:creator>
  <dc:creator>Scholtes, Theo</dc:creator>
  <dc:creator>Woetzel, Stefan</dc:creator>
  <dc:creator>Stolz, Ronny</dc:creator>
  <dc:date>2017-03-10</dc:date>
  <dc:description xmlns:ns0="xml" ns0:lang="en">We present an optically pumped magnetometer working in a new operational mode— the light-shift dispersed Mz (LSD-Mz) mode. It is realized combining various features;  (1) high power off-resonant optical pumping; (2) Mz configuration, where pumping light  and magnetic field of interest are oriented parallel to each other; (3) use of small alkali  metal vapor cells of identical properties in integrated array structures, where two such  cells are pumped by circularly polarized light of opposite helicity; and (4) subtraction of  the Mz signals of these two cells. The LSD-Mz magnetometer’s performance depends  on the inherent and very complex interplay of input parameters. In order to find the  configuration of optimal magnetometer resolution, a sensitivity analysis of the input  parameters by means of Latin Hypercube Sampling was carried out. The resulting  datasets of the multi-dimensional parameter space exploration were assessed by a  subsequent physically reasonable interpretation. Finally, the best shot-noise limited  magnetic field resolution was determined within that parameter space. As the result,  using two 50 mm3 integrated vapor cells a magnetic ﬁeld resolution below 10 fT/√Hz at  Earth’s magnetic ﬁeld strength is possible.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>https://folia.unifr.ch/global/documents/305581</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/305581/files/sch_opm.pdf</dc:identifier>
  <dc:language>eng</dc:language>
  <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.3390/s17030561</dc:relation>
  <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
  <dc:rights>License undefined</dc:rights>
  <dc:source>Sensors. - 2017, vol. 17, no. 3, p. 561</dc:source>
  <dc:subject xmlns:ns1="xml" ns1:lang="en">magnetometer</dc:subject>
  <dc:subject xmlns:ns2="xml" ns2:lang="en">optically pumped magnetometer</dc:subject>
  <dc:subject xmlns:ns3="xml" ns3:lang="en">light shift</dc:subject>
  <dc:subject xmlns:ns4="xml" ns4:lang="en">Mz</dc:subject>
  <dc:subject xmlns:ns5="xml" ns5:lang="en">magnetic-field resolution</dc:subject>
  <dc:subject xmlns:ns6="xml" ns6:lang="en">Latin Hypercube Sampling</dc:subject>
  <dc:subject xmlns:ns7="xml" ns7:lang="en">Downhill simplex</dc:subject>
  <dc:subject>info:eu-repo/classification/udc/53</dc:subject>
  <dc:title xmlns:ns8="xml" ns8:lang="en">An optically pumped magnetometer working in the light-shift dispersed Mz mode</dc:title>
  <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
</oai_dc:dc>
