# number_of_header_lines: 69 # comment: # comment: ************ USE OF GML DATA **************** # comment: # comment: These data are made freely available to the public and the # comment: scientific community in the belief that their wide dissemination # comment: will lead to greater understanding and new scientific insights. # comment: The availability of these data does not constitute publication # comment: of the data. NOAA relies on the ethics and integrity of the user to # comment: ensure that GML receives fair credit for their work. If the data # comment: are obtained for potential use in a publication or presentation, # comment: GML should be informed at the outset of the nature of this work. # comment: If the GML data are essential to the work, or if an important # comment: result or conclusion depends on the GML data, co-authorship # comment: may be appropriate. This should be discussed at an early stage in # comment: the work. Manuscripts using the GML data should be sent to GML # comment: for review before they are submitted for publication so we can # comment: ensure that the quality and limitations of the data are accurately # comment: represented. # comment: Please see accompanying README file, if available, for citation text. # comment: # comment: Every effort is made to produce the most accurate and precise # comment: measurements possible. However, we reserve the right to make # comment: corrections to the data based on recalibration of standard gases # comment: or for other reasons deemed scientifically justified. # comment: # comment: We are not responsible for results and conclusions based on use # comment: of these data without regard to this warning. # comment: # contact_parameter: H2 CCGG (Individual Flasks) # contact_name: Gabrielle Petron # contact_telephone: (720) 295-0145 # contact_email: Gabrielle.Petron@noaa.gov # comment: # comment: ************ COLLABORATORS *************** # comment: # comment: NOAA thanks the following collaborators without # comment: whom these measurements would not be possible. # comment: # collaborator_name: National Central University, Taiwan [NCU] # comment: # comment: ************ RECIPROCITY AGREEMENT *************** # comment: # comment: Use of these data implies an agreement to reciprocate. # comment: Laboratories making similar measurements agree to make their # comment: own data available to the general public and to the scientific # comment: community in an equally complete and easily accessible form. # comment: Modelers are encouraged to make available to the community, # comment: upon request, their own tools used in the interpretation # comment: of the GML data, namely well documented model code, transport # comment: fields, modeled mole fractions, and additional information # comment: necessary for other scientists to repeat the work and to run # comment: modified versions. Model availability includes collaborative # comment: support for new users of the models. # comment: # comment: ************ DATA DESCRIPTION *************** # comment: # description_site-code: dsi # description_project-abbr: ccg_surface # description_strategy-abbr: flask # description_analysis-constraints: flag:..% # description_creation-time: 2023-07-05 12:59:04 # comment: # comment: ************ DATA DOCUMENTATION *************** # comment: # comment: Please refer to the species-specific README file in the # comment: appropriate directory folder at https://gml.noaa.gov/aftp/data/trace_gases/. # comment: # data_fields: site year month value DSI 2010 3 557.63 DSI 2010 4 563.97 DSI 2010 5 565.36 DSI 2010 6 554.10 DSI 2010 7 544.13 DSI 2010 8 545.10 DSI 2010 9 544.94 DSI 2010 10 545.47 DSI 2010 11 547.77 DSI 2010 12 546.87 DSI 2011 1 554.53 DSI 2011 2 565.54 DSI 2011 3 567.93 DSI 2011 4 567.05 DSI 2011 5 564.17 DSI 2011 6 555.30 DSI 2011 7 553.45 DSI 2011 8 556.35 DSI 2011 9 545.18 DSI 2011 10 540.88 DSI 2011 11 550.96 DSI 2011 12 553.41 DSI 2012 1 548.46 DSI 2012 2 548.53 DSI 2012 4 559.63 DSI 2012 5 560.71 DSI 2012 6 554.59 DSI 2012 7 554.37 DSI 2012 8 558.07 DSI 2012 9 551.16 DSI 2012 10 544.23 DSI 2012 11 551.31 DSI 2012 12 558.31 DSI 2013 1 551.60 DSI 2013 2 547.44 DSI 2013 3 558.70 DSI 2013 4 570.38 DSI 2013 5 571.93 DSI 2013 6 568.04 DSI 2013 7 560.92 DSI 2013 8 552.32 DSI 2013 9 542.37 DSI 2013 10 535.56 DSI 2013 11 543.62 DSI 2013 12 555.21 DSI 2014 1 551.12 DSI 2014 2 549.28 DSI 2014 3 559.85 DSI 2014 4 569.94 DSI 2014 5 570.16 DSI 2014 6 562.61 DSI 2014 7 557.85 DSI 2014 8 558.96 DSI 2014 9 556.04 DSI 2014 10 543.28 DSI 2014 11 538.34 DSI 2014 12 551.72 DSI 2015 1 569.91 DSI 2015 2 570.06 DSI 2015 3 561.10 DSI 2015 4 561.15 DSI 2015 5 564.91 DSI 2015 6 557.70 DSI 2015 7 550.63 DSI 2015 8 551.49 DSI 2015 9 548.55 DSI 2015 10 540.09 DSI 2015 11 544.88 DSI 2015 12 562.90 DSI 2016 1 570.54 DSI 2016 2 559.45 DSI 2016 3 557.11 DSI 2016 4 570.85 DSI 2016 5 576.57 DSI 2016 6 566.74 DSI 2016 7 559.66 DSI 2016 8 562.94 DSI 2016 11 553.07 DSI 2016 12 552.06 DSI 2017 1 549.79 DSI 2017 2 552.27 DSI 2017 3 560.08 DSI 2017 4 566.34 DSI 2017 5 566.29 DSI 2017 6 559.97 DSI 2017 7 557.28 DSI 2017 8 562.70 DSI 2017 9 559.97 DSI 2017 10 543.17 DSI 2017 11 537.19 DSI 2017 12 549.13 DSI 2018 1 559.40 DSI 2018 2 560.59 DSI 2018 3 565.61 DSI 2018 4 575.38 DSI 2018 5 575.07 DSI 2018 6 564.18 DSI 2018 7 561.61 DSI 2018 8 562.56 DSI 2018 9 552.74 DSI 2018 10 549.14 DSI 2018 11 556.40 DSI 2018 12 558.70 DSI 2019 1 557.22 DSI 2019 2 558.99 DSI 2019 3 564.14 DSI 2019 4 569.14 DSI 2019 5 568.28 DSI 2019 6 563.29 DSI 2019 7 561.03 DSI 2019 8 561.48 DSI 2019 9 559.47 DSI 2019 10 552.90 DSI 2019 11 545.19 DSI 2019 12 543.23 DSI 2020 1 550.29 DSI 2020 2 561.79 DSI 2020 3 568.30 DSI 2020 4 571.42 DSI 2020 5 572.97 DSI 2020 6 568.03 DSI 2020 7 563.46 DSI 2020 8 562.66 DSI 2020 9 554.35 DSI 2020 10 543.24 DSI 2020 11 545.66 DSI 2020 12 555.70 DSI 2021 1 565.51 DSI 2021 2 568.03 DSI 2021 3 563.96 DSI 2021 4 564.22 DSI 2021 5 570.37 DSI 2021 6 570.34 DSI 2021 7 566.22 DSI 2021 8 566.31 DSI 2021 9 564.06 DSI 2021 10 554.61 DSI 2021 11 550.04 DSI 2021 12 559.71