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            <gco:CharacterString>Cite this dataset as: Veatch, J., Klinck, J. M., Oliver, M., Kohut, J., Statscewich, H. (2024) Relative Particle Density (RPD) calculations using High Frequency Radar (HFR) observed surface currents around Palmer Deep Canyon from January to March of 2020. Biological and Chemical Oceanography Data Management Office (BCO-DMO). (Version 1) Version Date 2024-01-08 [if applicable, indicate subset used]. doi:10.26008/1912/bco-dmo.917926.1 [access date]</gco:CharacterString>
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        <gco:CharacterString>Methods and Sampling: &amp;lt;p&amp;gt;&amp;lt;span style=&amp;quot;font-family:arial&amp;quot;&amp;gt;Methods for these LCS results can be found in Veatch, et al. (2024, in revision)&amp;lt;/span&amp;gt;.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;Relative Particle Density provides the normalized density of drifters within each gridded bin of the study system. Relative Particle Density calculations begin with tracking virtual particles through a velocity field that are released over a regular grid. RPD is calculated by summing the number of drifters in each grid box, and normalizing by the median number of drifters in all grid boxes. In the following analysis, new particles were released in a regular grid across the 80 % coverage of the HFR footprint every three hours. Particles were not counted until they had been advected in the velocity field for 6 hours (when the autocorrelation of the HFR velocities cross the e-fold), and were no longer counted when they were advected out of the HFR domain, or after they became three days old. Given the average residence time of 2 days (Kohut et al., 2018), the three-day threshold was chosen to coordinate with the time phytoplankton will spend in the surface layer of our study domain. This methodology follows that used by (Oliver et al. 2019). RPD reports the normalized number of drifters present in each gridded bin at each timestamp. Two dimensional RPD assumes that no particles are lost from the surface layer due to vertical velocity, meaning that the integrated surface divergence in the x-y plane is assumed to be zero. Therefore, RPD will map the instantaneous concentration of surface associated particles across the entire domain given the evolving surface current fields provided by the HFR.&amp;lt;/p&amp;gt;</gco:CharacterString>
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        <gmx:Anchor xlink:href="http://lod.bco-dmo.org/id/award/850843.rdf" xlink:title="OPP-1745009" xlink:actuate="onRequest">Funding provided by NSF Office of Polar Programs (formerly NSF PLR) (NSF OPP) Award Number: OPP-1745009 Award URL: https://www.nsf.gov/awardsearch/show-award?AWD_ID=1745009</gmx:Anchor>
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        <gmx:Anchor xlink:href="http://lod.bco-dmo.org/id/award/850848.rdf" xlink:title="OPP-1744884" xlink:actuate="onRequest">Funding provided by NSF Office of Polar Programs (formerly NSF PLR) (NSF OPP) Award Number: OPP-1744884 Award URL: https://www.nsf.gov/awardsearch/show-award?AWD_ID=1744884</gmx:Anchor>
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        <gmx:Anchor xlink:href="http://lod.bco-dmo.org/id/award/850852.rdf" xlink:title="OPP-1745011" xlink:actuate="onRequest">Funding provided by NSF Office of Polar Programs (formerly NSF PLR) (NSF OPP) Award Number: OPP-1745011 Award URL: https://www.nsf.gov/awardsearch/show-award?AWD_ID=1745011</gmx:Anchor>
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&amp;lt;p&amp;gt;Relative Particle Density provides the normalized density of drifters within each gridded bin of the study system. Relative Particle Density calculations begin with tracking virtual particles through a velocity field that are released over a regular grid. RPD is calculated by summing the number of drifters in each grid box, and normalizing by the median number of drifters in all grid boxes. In the following analysis, new particles were released in a regular grid across the 80 % coverage of the HFR footprint every three hours. Particles were not counted until they had been advected in the velocity field for 6 hours (when the autocorrelation of the HFR velocities cross the e-fold), and were no longer counted when they were advected out of the HFR domain, or after they became three days old. Given the average residence time of 2 days (Kohut et al., 2018), the three-day threshold was chosen to coordinate with the time phytoplankton will spend in the surface layer of our study domain. This methodology follows that used by (Oliver et al. 2019). RPD reports the normalized number of drifters present in each gridded bin at each timestamp. Two dimensional RPD assumes that no particles are lost from the surface layer due to vertical velocity, meaning that the integrated surface divergence in the x-y plane is assumed to be zero. Therefore, RPD will map the instantaneous concentration of surface associated particles across the entire domain given the evolving surface current fields provided by the HFR.&amp;lt;/p&amp;gt;</gco:CharacterString>
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* Curatorial note: See supplemental file SWARM_LCS-related_to_bcodmo_917926_917914_v1.zip which contains a release corresponding to commit (10931d9).&amp;lt;/p&amp;gt;</gco:CharacterString>
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 https://github.com/BCODMO/SWARM_LCS/releases/tag/related_to_bcodmo_917926_917914_v1.  No changes to the code were made.  Zip file of this release attache as a supplemental file.</gco:CharacterString>
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