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        <formatdesc>A 1 meter silica multimode fiber of 600 microemeter core diamter was used to collect the side scattered light from side of hollow core fiber.</formatdesc>
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    <datestamp>2018-01-19 12:50:24</datestamp>
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          <family>Yu</family>
          <given>Fei</given>
        </name>
        <id>F.Yu@bath.ac.uk</id>
        <orcid>0000-0002-1831-859X</orcid>
        <affiliation>University of Bath</affiliation>
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    <title>Dataset for &apos;&apos;Continuous-Wave Mid-Infrared Gas Fiber Lasers&apos;&apos;</title>
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    <note>1. Figure_1_original_absorption_intensity_strength_from_HITRAN.csv contains the orignal downloaded data from HITRAN database. MATLAB code is to convert the absorption intensity to the spectral transmittance per meter in fig.1.

2. Figure_4_b_input_spectra.csv contains the measured EDFA output spectrum for different amplifications in fig.4 (b).

3. Figure_4_c_fiber_attenuation.csv contains the measured hollow core fiber attenuations in fig.4 (c).

4. Figure_5_a_output_power_at_different_pressures_incident_power.csv contains the measured output laser power as a function of incident power at different pressures in fig.5 (a).

5. Figure_5_b_output_power_at_different_pressures_absorbed_power.csv contains the measured output laser power as a function of absorbed power at different pressures in fig.5 (b).

6. Figure_6_a_max_3_microns_power.csv contains the maximum output laser power as a function of the pressure for different fiber lengths in fig.6 (a).

7. Figure_6_b_threshold.csv shows the lasing threshold as a fuction of pressure for different fiber lengths (6m, 15m, 40m) in fig.6 (b).

8. Figure_7_P_P_ratio.csv contains the laser peak intensity via P(9) transition over the one via R(7) transition as a function of incident pump power in fig.7.

9. Figure_7_inset_output_spectrum.csv contains the normalized laser spectrum at 3 micron in fig.7 inset.

10. Figure_8_a_absorbed_spectrum.csv contains the typical measured spectra when pump light is tuned on and off P(9) wavelength in fig.8 (a).

11. Figure_8_b_fiber_side_length.csv contains the pump absorption as a function of position along 15 m fiber for different incident powers at 0.6 mbar pressure in fig.8 (b).

12. Figure_8_c_fiber_side_different_pressures.csv contains the pump absorption as a function of position along 31m fiber at different pressures with full incident power in fig.8 (c).

13. Figure_8_c_inset.csv contains the caculated pump absorption slope efficiency as a function of pressure in fig.8 (c) inset.</note>
    <abstract>The dataset include all necessary data to generate figures 1, 4 (b), 4(c), 5–8 in the associated manuscript, &quot;Continuous-Wave Mid-Infrared Gas Fiber Lasers&quot;. These data measure the properties of the lasers under different conditions, including different gas pressures and fiber lengths.</abstract>
    <date>2018-01-19</date>
    <publisher>University of Bath</publisher>
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        <funder_id>https://doi.org/10.13039/501100000266</funder_id>
        <grant_id>EP/M025381/1</grant_id>
        <project_name>Hollow Antiresonant Fibres for Visible and Ultraviolet Beam Delivery</project_name>
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        <funder_name>Engineering and Physical Sciences Research Council</funder_name>
        <funder_id>https://doi.org/10.13039/501100000266</funder_id>
        <grant_id>EP/I011315/1</grant_id>
        <project_name>New Fibres for New Lasers - Photonic Crystal Fibre Optics for the Delivery of High-Power Light</project_name>
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    <version>1</version>
    <doi>10.15125/BATH-00406</doi>
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