Chinese Journal of Lasers, Volume. 50, Issue 22, 2211002(2023)

Statistical Structure Gene Modeling of Alkali to Spectroscopic Properties of NdPhosphate Glass

Yuechun Hou1,2, Chen Dai3, and Liyan Zhang1、*
Author Affiliations
  • 1Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3College of Materials Science and Engineering, Hunan University, Changsha 410082, Hunan, China
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    Figures & Tables(13)
    BL,PL,PN glass properties response as a function of the addition of Li2O,Na2O
    IR spectra and residual between the simulated and measured spectra. (a) Measured (black symbols) and curve-fitting derived (green lines) IR spectra of BL, PL2, and PN2 glasses (spectra are shifted vertically for clarity),and individual bands (orange lines) of BL glass; (b) residual (ΔI) between the simulated and measured spectra of BL glass
    IR difference spectrs of PL2 (black line) and PN2 (red dot) to BL glass
    S-P models. (a) σemi; (b) τf; (c) Δλeff; (d) Ω2; (e) Ω4; (f) Ω6 (* denotes BL, ▷ denotes PL1‒4, and ● denotes PN1‒4)
    S-P models. (a) σemi(without PL2); (b) τf(without PN2); (c) Δλeff; (d) Ω2(without PL2); (e) Ω4(without PN2); (f) Ω6 (without PN3)
    C-S models. (* denotes BL, ▷ denotes PL1‒4, ● denotes PN1‒4). (a) Li2O; (b) Na2O
    Illustration of C-S-P model based glass property design for achieving specific composition
    • Table 1. Composition of the glass samples (normalized)

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      Table 1. Composition of the glass samples (normalized)

      No.Mole fraction /%
      Li2ONa2OK2OP2O5MgOAl2O3R2O3Nd2O3
      BL0023.7659.418.914.951.990.99
      PL11.94023.3058.258.744.851.950.97
      PL23.81022.8657.148.574.761.910.95
      PL35.61022.4356.078.414.671.880.93
      PL47.34022.0255.058.264.591.820.92
      PN101.9423.3058.258.744.851.950.97
      PN203.8122.8657.148.574.761.910.95
      PN305.6122.4356.078.414.671.880.93
      PN407.3422.0255.058.264.591.820.92
      PLN2.003.0422.5656.418.464.701.880.94
    • Table 2. Properties of the glass samples

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      Table 2. Properties of the glass samples

      No.σemi /pm2Ω2 /pm2Ω4 /pm2Ω6 /pm2τf /μsΔλeff /nmnd
      BL4.374.685.206.1733724.691.5083
      PL14.264.744.825.8532624.411.5108
      PL24.314.504.935.8433024.391.5107
      PL34.234.544.785.7733424.711.5114
      PL44.344.465.075.8732724.661.5128
      PN14.284.504.775.8333024.561.5088
      PN24.304.504.875.8433624.451.5088
      PN34.454.534.995.9934124.291.5083
      PN44.104.844.555.4635424.201.5088
      PLN4.134.624.845.7333124.491.5119
    • Table 3. Integral area of IR bands derived from IR curve fitting

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      Table 3. Integral area of IR bands derived from IR curve fitting

      No.Integral area
      A1A2A3A4A5A6A7A8A9A10A11A12A13A14A15
      BL21.93.10.92.71.24.36.99.28.512.03.71.17.28.68.8
      PL122.25.20.82.42.04.77.29.07.810.74.31.06.07.49.1
      PL221.06.10.62.32.55.07.39.07.69.65.30.55.77.110.3
      PL323.53.70.93.01.64.77.29.18.211.73.11.26.27.68.5
      PL423.13.60.82.62.25.17.49.07.810.64.20.96.27.58.9
      PN121.94.70.72.42.55.47.89.17.68.95.80.65.56.710.4
      PN221.72.51.02.80.94.17.19.98.812.13.51.27.38.58.4
      PN322.34.20.82.42.25.17.79.37.99.75.21.26.17.18.7
      PN420.47.10.72.32.55.27.69.17.58.65.90.75.66.710.0
      PLN21.45.80.72.42.34.97.49.17.710.44.70.85.77.19.6
    • Table 4. IR band positions identified from this study and band assignments taken from literatures

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      Table 4. IR band positions identified from this study and band assignments taken from literatures

      Ai(structural unit)Bands observed in this work /cm-1Band assignments based on phosphates vibrational spectra taken from literatures
      A1477‒491458‒680 cm-1,bending vibrations of bridging phosphorus:δ(O—P—O);a fundamental frequency of PO43- or harmonics of P=O bending vibrations
      A2569‒582
      A3716‒720684‒830 cm-1,symmetric stretching vibration of P—O—P bridges bonded to a phosphorus atom in P(2) unit:νs(P—O—P)
      A4762‒762
      A5863‒877860‒1002 cm-1,asymmetric stretching vibration of P—O—P bridges:νas(P—O—P)of P(2) unit
      A6900‒919
      A71006‒10161000‒1100 cm-1,symmetric vibration of P—O- groups of chain terminator:νs(P—O-)of chain terminator;asymmetric stretching vibration of PO2- groups:νas(PO2-)of P(2) unit
      A81108‒11181108‒1118 cm-1,stretching vibration of PO2- terminal groups:νs(PO2-
      A91162‒11701148‒1280 cm-1,asymmetric stretching vibration of PO2- groups:νas(PO2-)of P(2) unit
      A101263‒1273
      A111304‒13271250‒1420cm-1,asymmetric stretching vibration of the two nonbridging oxygen atoms bonded to phosphorus atoms:νas(O—P—O)or νas(PO2-);harmonics of ν(P—O)from two bridging oxygen bonds and two non-bridging bonds,(P—O)and(P—O-
      A121376‒1420
      A131485‒1575bonding vibration of P—OH:νas(O—H)
      A141632‒1638
      A151835‒1909
    • Table 5. Analysis of variance of statistical S-P models

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      Table 5. Analysis of variance of statistical S-P models

      ItemσemiτfΔλeffΩ2Ω4Ω6
      Analysis of variance
      Root mean square error0.01962.11090.03270.03560.04170.0292
      Corrected total degree of freedom778777
      F-ratio47.4732.3060.6525.1840.474674.87
      Prob>F<0.0048<0.0084<0.0054<0.0121<0.0061<0.0025
      Parameter estimation
      Intercept(t-ratio)5.94(36.52)459.06(19.01)26.41(40.34)9.78(7.16)6.84(8.93)-28.86(-7.95)
      A1t-ratio)Insignificant-16.57(-10.81)Insignificant-0.13(-4.60)InsignificantInsignificant
      A2t-ratio)-0.11(-11.25)Insignificant-0.12(-7.92)0.07(3.13)-0.12(-6.07)0.20(6.80)
      A3t-ratio)-1.02(-5.13)InsignificantInsignificant1.60(5.84)-2.79(-6.72)Insignificant
      A4t-ratio)-0.27(-4.99)36.94(5.75)0.47(5.81)InsignificantInsignificantInsignificant
      A6t-ratio)Insignificant23.09(3.42)InsignificantInsignificantInsignificantInsignificant
      A7t-ratio)InsignificantInsignificantInsignificantInsignificantInsignificant2.73(9.25)
      A8t-ratio)InsignificantInsignificant-0.41(-8.25)-0.44(-4.65)InsignificantInsignificant
      A12t-ratio)0.36(6.18)InsignificantInsignificantInsignificantInsignificantInsignificant
      A13t-ratio)Insignificant38.02(7.90)InsignificantInsignificant0.34(6.86)Insignificant
      A14t-ratio)InsignificantInsignificantInsignificantInsignificantInsignificant4.34(11.08)
      A15t-ratio)InsignificantInsignificant0.13(5.17)Insignificant-0.14(-2.92)Insignificant
    • Table 6. Model validation results and relative error

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      Table 6. Model validation results and relative error

      ParameterMeasured valuePredicted value

      Relative error /

      %

      σemi /pm24.134.140.24
      τf /μs3313330.60
      Δλeff /nm24.4924.50.04
      Ω2 /pm24.624.620.01
      Ω4 /pm24.844.830.21
      Ω6 /pm25.735.720.17
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    Yuechun Hou, Chen Dai, Liyan Zhang. Statistical Structure Gene Modeling of Alkali to Spectroscopic Properties of NdPhosphate Glass[J]. Chinese Journal of Lasers, 2023, 50(22): 2211002

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    Paper Information

    Category: spectroscopy

    Received: Feb. 15, 2023

    Accepted: Mar. 23, 2023

    Published Online: Nov. 17, 2023

    The Author Email: Zhang Liyan (jndxzly@hotmail.com)

    DOI:10.3788/CJL230530

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