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            <gco:CharacterString>Cite this dataset as: Brandes, J., Miller, W., Powers, L., Stubbins, A. (2024) Chromophoric Dissolved Organic Matter Napierian Absorption Coefficients for Open Ocean Blue Water Samples from the North Atlantic Subtropical Gyre from R/V Atlantic Explorer AE1707, AE1829, AE1820, AE1905 at Bermuda Atlantic Time Series Stations (BATS) f. Biological and Chemical Oceanography Data Management Office (BCO-DMO). (Version 1) Version Date 2024-05-14 [if applicable, indicate subset used]. doi:10.26008/1912/bco-dmo.927300.1 [access date]</gco:CharacterString>
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        <gco:CharacterString>Chromophoric dissolved organic matter (CDOM) Napierian absorption coefficients for open ocean blue water samples from the North Atlantic subtropical gyre Dataset Description:  Methods and Sampling: &amp;lt;p&amp;gt;&amp;lt;strong&amp;gt;Water sampling details&amp;lt;/strong&amp;gt;&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;Water samples were gravity filtered from Niskin bottles through 0.2 μm Whatman Polycap 36 AS nylon membrane cartridge filters, directly into combusted borosilicate glass bottles. Filtered sample waters were stored in the dark at 4°C until measurements. Sample waters were left in the dark at room temperature (~20°C) so they were back to room temperature before absorbance measurements.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;These seawater samples were collected for photochemical degradation experiments, and water samples at the various BATS stations had similar optical properties, for example, similar absorbance at 325 nm. Therefore, which stations we collected samples from were largely determined by the cruise schedule, scientific tasks performed by the core BATS crew, and weather, i.e., where CTDs can be cast that allowed us ample time to directly filter water from the Niskin bottles.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;We also wanted to compare the photoproduction of dissolved inorganic carbon (DIC) between seawater at the surface and at depth, as the deep water may have different photodegradation history and different dissolved organic carbon composition, and thus have different DIC photoproduction rates and efficiencies. Therefore, we collected water samples from the surface (1 m) and at depth (3000 m).&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;&amp;lt;strong&amp;gt;Measurement details&amp;lt;/strong&amp;gt;&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;Absorbance (&amp;lt;em&amp;gt;A&amp;lt;/em&amp;gt;(λ)) of the water samples were measured at 250–800 nm at 1.0 nm intervals, in triplicate. May 13&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt;, 2017 samples were measured in 10-cm-pathlength quartz spectrophotometric cuvettes with an Agilent 8453 UV-visible spectrophotometer with ChemStation software; July 17&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt;, 2018 samples were measured in a World Precision Instruments UltraPath capillary cell set at 50 cm pathlength using a Maya Pro 2000 spectrophotometer with SpectraSuite software, and the rest of the samples were measured in the same UltraPath capillary cell set at 200 cm pathlength using the same Maya spectrophotometer.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;Milli-Q water was similarly measured to use as blanks. The absorbance spectra of the sample water were first corrected by subtracting the absorbance spectra of blanks (Milli-Q water) from the absorbance spectra of the sample water; the absorbance spectra of the sample water were further corrected for potential offsets and instrument drift by subtracting the average absorbance at 690–710 nm. The corrected absorbance spectra (&amp;lt;em&amp;gt;A&amp;lt;/em&amp;gt;(λ)&amp;lt;sub&amp;gt;corr&amp;lt;/sub&amp;gt;) of the sample water generated from these corrections were converted to Napierian absorption coefficients (&amp;lt;em&amp;gt;a&amp;lt;/em&amp;gt;&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt;(λ); m&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;; represented in this dataset as CDOM_absorption_a_g), using the following equation: &amp;lt;em&amp;gt;a&amp;lt;/em&amp;gt;&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt;(λ)= &amp;lt;em&amp;gt;A&amp;lt;/em&amp;gt;(λ)&amp;lt;sub&amp;gt;corr&amp;lt;/sub&amp;gt; ln10/&amp;lt;em&amp;gt;L&amp;lt;/em&amp;gt;, where &amp;lt;em&amp;gt;L&amp;lt;/em&amp;gt; (m) is the pathlength.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;The May 13&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt;, 2017 samples were measured in 10-cm-pathlength cuvettes with the Agilent spectrophotometer because these samples were T0 samples of a photoirradiation experiments, the water was photoirradiated in these 10-cm-pathlength cuvettes, and the absorbance were also measured in these cuvettes, which only works on the Agilent spectrophotometer, which has a 10-cm-pathlength cuvette holder.&amp;lt;/p&amp;gt;</gco:CharacterString>
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        <gmx:Anchor xlink:href="http://lod.bco-dmo.org/id/award/744568.rdf" xlink:title="OCE-1635618" xlink:actuate="onRequest">Funding provided by NSF Division of Ocean Sciences (NSF OCE) Award Number: OCE-1635618 Award URL: https://www.nsf.gov/awardsearch/show-award?AWD_ID=1635618</gmx:Anchor>
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Photoproduction describes chemical reactions which use the energy of sunlight to change the molecular structure of one product to another. This process has been shown to play an important role in the coastal ocean changing dissolved organic carbon (DOC) to dissolved inorganic carbon (DIC); however, minimal information is available on the extent to which this process takes place in the open ocean. The main obstacle to obtaining DIC production data for open ocean waters is the inability to measure the small DIC production rates against the large background of seawater DIC. Currently the most common method for high precision measurement of DIC production has unacceptable detection limits to resolve this difference. Researchers from the University of Georgia have developed MoDIE (Moderate DI13C Isotope Enrichment), a novel means of determining low levels of DIC produced in the open ocean with high precision. As part of this project, they plan to refine their MoDIE method and obtain measurements of DIC photoproduction in open ocean waters (i.e, South Atlantic Bight, North Atlantic Ocean and North Pacific Ocean subtropical gyres). Results from this work will provide improved estimates of DIC photoproduction in the open ocean which in turn will improve existing models of carbon cycling.&lt;/p&gt;
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	Name: BATS_station
	Units: unitless
	Description: &lt;p&gt;Name of the Bermuda Atlantic Time-series Study (BATS) station where the sample was obtained.&lt;/p&gt; 
http://lod.bco-dmo.org/id/dataset-parameter/934040.rdf
	Name: BATS_station_Latitude
	Units: decimal degrees
	Description: &lt;p&gt;Latitude of the BATS station where the sample was obtained in decimal degrees; a positive value indicates a Northern coordinate.&lt;/p&gt; 
http://lod.bco-dmo.org/id/dataset-parameter/934041.rdf
	Name: BATS_station_Longitude
	Units: decimal degrees
	Description: &lt;p&gt;Longitude of the BATS station where the sample was obtained in decimal degrees; a negative value indicates a Western coordinate.&lt;/p&gt; 
http://lod.bco-dmo.org/id/dataset-parameter/934042.rdf
	Name: Sample_date
	Units: unitless
	Description: &lt;p&gt;Date sample was collected.&lt;/p&gt; 
http://lod.bco-dmo.org/id/dataset-parameter/934043.rdf
	Name: Sample_depth_m
	Units: meters (m)
	Description: &lt;p&gt;Depth from which the sample was taken.&lt;/p&gt; 
http://lod.bco-dmo.org/id/dataset-parameter/934044.rdf
	Name: lambda
	Units: nanometer (nm)
	Description: &lt;p&gt;Wavelength at which the absorbance was measured.&lt;/p&gt; 
http://lod.bco-dmo.org/id/dataset-parameter/934045.rdf
	Name: CDOM_absorption_a_g
	Units: meters^(-1)
	Description: &lt;p&gt;Chromophoric dissolved organic matter (CDOM) Naperian absorption coefficients (ag)&lt;/p&gt; 
http://lod.bco-dmo.org/id/dataset-parameter/934046.rdf
	Name: Sample_no
	Units: unitless
	Description: &lt;p&gt;Sample from the same location, depth and date was collected into different bottles, and for some of the samples, each bottle was measured for absorbance separately, in which case, sample numbers were given to the subsamples from each bottle. For example, 3 means this is a third bottle of the same sample taken from the same location, depth and date.&lt;/p&gt; 
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        <gco:CharacterString>Monday - Friday 8:00am - 5:00pm</gco:CharacterString>
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		    <gco:CharacterString>For questions regarding this resource, please contact BCO-DMO via the email address provided.</gco:CharacterString>
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                <gco:CharacterString>&amp;lt;p&amp;gt;&amp;lt;strong&amp;gt;Water sampling details&amp;lt;/strong&amp;gt;&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;Water samples were gravity filtered from Niskin bottles through 0.2 μm Whatman Polycap 36 AS nylon membrane cartridge filters, directly into combusted borosilicate glass bottles. Filtered sample waters were stored in the dark at 4°C until measurements. Sample waters were left in the dark at room temperature (~20°C) so they were back to room temperature before absorbance measurements.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;These seawater samples were collected for photochemical degradation experiments, and water samples at the various BATS stations had similar optical properties, for example, similar absorbance at 325 nm. Therefore, which stations we collected samples from were largely determined by the cruise schedule, scientific tasks performed by the core BATS crew, and weather, i.e., where CTDs can be cast that allowed us ample time to directly filter water from the Niskin bottles.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;We also wanted to compare the photoproduction of dissolved inorganic carbon (DIC) between seawater at the surface and at depth, as the deep water may have different photodegradation history and different dissolved organic carbon composition, and thus have different DIC photoproduction rates and efficiencies. Therefore, we collected water samples from the surface (1 m) and at depth (3000 m).&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;&amp;lt;strong&amp;gt;Measurement details&amp;lt;/strong&amp;gt;&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;Absorbance (&amp;lt;em&amp;gt;A&amp;lt;/em&amp;gt;(λ)) of the water samples were measured at 250–800 nm at 1.0 nm intervals, in triplicate. May 13&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt;, 2017 samples were measured in 10-cm-pathlength quartz spectrophotometric cuvettes with an Agilent 8453 UV-visible spectrophotometer with ChemStation software; July 17&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt;, 2018 samples were measured in a World Precision Instruments UltraPath capillary cell set at 50 cm pathlength using a Maya Pro 2000 spectrophotometer with SpectraSuite software, and the rest of the samples were measured in the same UltraPath capillary cell set at 200 cm pathlength using the same Maya spectrophotometer.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;Milli-Q water was similarly measured to use as blanks. The absorbance spectra of the sample water were first corrected by subtracting the absorbance spectra of blanks (Milli-Q water) from the absorbance spectra of the sample water; the absorbance spectra of the sample water were further corrected for potential offsets and instrument drift by subtracting the average absorbance at 690–710 nm. The corrected absorbance spectra (&amp;lt;em&amp;gt;A&amp;lt;/em&amp;gt;(λ)&amp;lt;sub&amp;gt;corr&amp;lt;/sub&amp;gt;) of the sample water generated from these corrections were converted to Napierian absorption coefficients (&amp;lt;em&amp;gt;a&amp;lt;/em&amp;gt;&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt;(λ); m&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;; represented in this dataset as CDOM_absorption_a_g), using the following equation: &amp;lt;em&amp;gt;a&amp;lt;/em&amp;gt;&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt;(λ)= &amp;lt;em&amp;gt;A&amp;lt;/em&amp;gt;(λ)&amp;lt;sub&amp;gt;corr&amp;lt;/sub&amp;gt; ln10/&amp;lt;em&amp;gt;L&amp;lt;/em&amp;gt;, where &amp;lt;em&amp;gt;L&amp;lt;/em&amp;gt; (m) is the pathlength.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;The May 13&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt;, 2017 samples were measured in 10-cm-pathlength cuvettes with the Agilent spectrophotometer because these samples were T0 samples of a photoirradiation experiments, the water was photoirradiated in these 10-cm-pathlength cuvettes, and the absorbance were also measured in these cuvettes, which only works on the Agilent spectrophotometer, which has a 10-cm-pathlength cuvette holder.&amp;lt;/p&amp;gt;</gco:CharacterString>
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                        <gco:CharacterString>Specified by the Principal Investigator(s)</gco:CharacterString>
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                      <gmd:date gco:nilReason="unknown"/>
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              <gmd:description>
                <gco:CharacterString>&amp;lt;p&amp;gt;&amp;lt;strong&amp;gt;Data Corrections and Conversions&amp;lt;/strong&amp;gt;&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;The average absorbance spectra of blanks were subtracted from the absorbance spectra of the sample water.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;Absorbance spectra were further corrected for potential offsets and instrument drift by subtracting the average absorbance at 690–710 nm.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;&amp;lt;em&amp;gt;A&amp;lt;/em&amp;gt;(λ) was converted to Napierian absorption coefficients (&amp;lt;em&amp;gt;a&amp;lt;/em&amp;gt;&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt;(λ); m&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;), using the following equation:&amp;amp;nbsp;&amp;lt;em&amp;gt;a&amp;lt;/em&amp;gt;&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt;(λ)=&amp;amp;nbsp;&amp;lt;em&amp;gt;A&amp;lt;/em&amp;gt;(λ) ln10/&amp;lt;em&amp;gt;L&amp;lt;/em&amp;gt;, where&amp;amp;nbsp;&amp;lt;em&amp;gt;L&amp;lt;/em&amp;gt;&amp;amp;nbsp;(m) is the pathlength.&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;&amp;lt;strong&amp;gt;Data Processing Software&amp;lt;/strong&amp;gt;&amp;lt;/p&amp;gt;

&amp;lt;ul&amp;gt;
&amp;lt;li&amp;gt;Importing and correcting absorbance measurements (A(λ))&amp;lt;/li&amp;gt;
&amp;lt;li&amp;gt;Converting A(λ) to Napierian absorption coefficients (ag(λ))&amp;lt;/li&amp;gt;
&amp;lt;li&amp;gt;R-3.3.3, R-3.4.4, R-3.5.3, R-3.6.2, R-3.6.3, R-4.2.1&amp;lt;/li&amp;gt;
&amp;lt;li&amp;gt;Package ‘stringr’:
&amp;lt;ul&amp;gt;
&amp;lt;li&amp;gt;Wickham H (2023). _stringr: Simple, Consistent Wrappers for Common String Operations_. R package version 1.5.1, &amp;amp;lt;https://CRAN.R-project.org/package=stringr&amp;amp;gt;.&amp;lt;/li&amp;gt;
&amp;lt;/ul&amp;gt;
&amp;lt;/li&amp;gt;
&amp;lt;/ul&amp;gt;

&amp;lt;p&amp;gt;&amp;amp;nbsp;&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;&amp;amp;nbsp;&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;&amp;amp;nbsp;&amp;lt;/p&amp;gt;

&amp;lt;p&amp;gt;&amp;amp;nbsp;&amp;lt;/p&amp;gt;</gco:CharacterString>
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                        <gco:CharacterString>Specified by the Principal Investigator(s)</gco:CharacterString>
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                  <gco:CharacterString>- Latitude and longitude values were joined to the dataset for BATS station sites</gco:CharacterString>
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                          <gco:CharacterString>Specified by BCO-DMO Data Managers</gco:CharacterString>
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				    <gco:CharacterString>Unavailable</gco:CharacterString>
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				    <gco:CharacterString>508-289-2009</gco:CharacterString>
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				    <gco:CharacterString>WHOI MS#36</gco:CharacterString>
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				    <gco:CharacterString>Woods Hole</gco:CharacterString>
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				    <gco:CharacterString>02543</gco:CharacterString>
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                <gmx:Anchor xlink:href="http://lod.bco-dmo.org/id/instrument/707.rdf" xlink:title="Spectrophotometer" xlink:actuate="onRequest">Agilent 8453 UV-visible spectrophotometer</gmx:Anchor>
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