slattery_2003#

S. A. Slattery and D. N. Nikogosyan, Opt. Commun. 228, 127 (2003)

Source record · Catalogue · Review register

DOI: 10.1016/j.optcom.2003.09.086

Source kind: measurement

Recorded technique: Transmittance against irradiance at 211 nm (2-40 GW/cm2): the fifth harmonic of a Twinkle Nd:glass laser (Light Conversion), made by non-collinear sum-frequency mixing of 1055 and 264 nm pulses in a 0.2 mm BBO crystal, ~100 uJ at 27 Hz, energy stability ~15 %; pulse duration 250 +- 20 fs taken from Dubietis et al. (same laser system); Gaussian beam of 2.2 +- 0.1 mm FWHM (from aperture transmission), focused by a 424 mm CaF2 lens, the sample always well before the focus (no self-focusing or filamentation seen). Energies by Ophir PE10 detectors; the curves are fitted with the theory of their Ref. [6] after correcting the focal shift in the sample (Ref. [1], dragomir_2002). Room temperature. Low-intensity transmittance by an HP8453 spectrophotometer.

Materials in structured entries: BaF2, CaF2, SiO2, SiO2_quartz

Dataset quantities: absorption_coefficient, band_gap, refractive_index, two_photon_absorption_coefficient

Contents: 28 datasets; 0 formulas.

Curation notes#

Tables 1 and 2 (pp. 3-4) are transcribed in full; checked against the images (the wrapped material names of Table 1 and the spanned material and E_g cells of Table 2 are handled in the script). Total uncertainty of beta ‘about 16 %’ (p. 2); the uncertainties are printed per value, level not stated.

Samples (p. 3): ‘two samples of Suprasil fused silica glass (Heraues [sic], Germany), as well as samples of crystalline quartz (cut perpendicular to the optic axis), calcium fluoride and barium fluoride (all from former Soviet Union, unknown manufacturers)’. The quartz is printed ‘(||c)’: light along the optic axis, so its datasets are given axis ‘o’ (an inference). Its length, 1.380 cm, is that of the quartz of dragomir_2002 (1.38 cm), probably the same sample. Table 1’s lengths l (cm): 1.000, 1.005, 1.380, 0.250, 0.815 (kept in the printed column). The beta of fused silica is one value for the two Suprasil samples.

Definition: the paper does not write the propagation equation; it uses the theory and fitting of its Refs. [1] and [6], i.e. dragomir_2002’s dI/dz = -alpha I - beta I^2 with (1 - R) at the entrance face (Eqs. 3-7 there): reflection losses are removed (Table 1’s (1 - R)^2) and alpha is Napierian (exp(-alpha l)). Table 1’s alpha is ‘experimentally determined linear absorption coefficient alpha (at 211 nm, deduced from total absorbance minus optical density, corresponding to the reflection losses, for details see [1])’; the words absorbance and optical density are decadic, and the paper does not say whether the difference was converted to a Napierian coefficient (a doubt; base ‘e’ is recorded as in dragomir_2002).

Table 1’s refractive index is ‘calculated from dispersion relations, given in [12]’ (Nikogosyan’s handbook) and (1 - R)^2 is in per cent. For BaF2 and CaF2, (1 - R)^2 follows from n with R = ((n - 1)/(n + 1))^2 (91.02 and 92.50, reproduced). For the Suprasil samples n = 1.5275 gives 91.48, not the printed 91.23, which needs n = 1.537; Malitson’s formula (malitson_1965, Eq. 1) gives n = 1.5373 at 211 nm. For quartz n = 1.6347 gives 88.73, not 88.57, which needs n = 1.641. The printed n of fused silica and quartz is therefore inconsistent with the paper’s own reflection loss (checked 2026-09-26); those two index datasets are excluded, the others reproduced.

Reproductions (Table 2, ‘Literature data for TPA coefficients together with our results at 211 nm’; ‘only picosecond and femtosecond data are considered’): [17] is kittelmann_1994 (its Gaussian-profile values; the +- is 70 % of the value, Kittelmann’s 50 % absolute plus 20 % relative), [20] taylor_1988 (the +- is 65 %, Taylor’s 50 % + 15 %; CaF2’s 0.8 is 8.3e-12 rounded), [1] dragomir_2002 (fused silica 1.7 +- 0.2 is Dragomir’s Suprasil, the smallest of its six glasses; quartz 1.2 +- 0.2), [18] Schenker et al. 1995 and [19] Gurzadyan and Ispiryan 1992 (not in the library; footnote a: ‘Only relative uncertainty is mentioned in publications’). The band gaps come from [15] weinberg_1979 (fused silica 9.3 eV) and [16] eva_1996 (quartz ~9, BaF2 9.1, CaF2 10 eV), which took them from weinberg_1979 and taylor_1988. The text (p. 4) says ‘for fused silica, crystalline quartz and BaF2 E_g is about 9 eV, and for CaF2 it equals 10 eV’. The paper judges Kittelmann’s 193 nm values for fused silica and BaF2 ‘underestimated’. The abstract’s range ‘26-59 x 10^-11 cm/W’ is this work’s.

Recorded bibliographic identity status: VALIDATED. This concerns identification of the source; it does not establish the scientific correctness of its contents.

Datasets#

slattery_2003/index_SiO2#

{
  "id": "index_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__index_SiO2.csv",
  "table": "tbl_43ed8a53704c",
  "quantity": "refractive_index",
  "abscissa_unit": "nm",
  "use": "excluded",
  "reproduced_from": [
    "D. N. Nikogosyan, Properties of Optical and Laser-related Materials, A Handbook, Wiley, Chichester, 1997"
  ],
  "parameters": {
    "grade": "Suprasil"
  }
}

Table 1: ‘calculated from dispersion relations, given in [12]’. Both samples 1.5275; inconsistent with the paper’s own (1 - R)^2 = 91.23 %, which needs n = 1.537 (Malitson’s formula gives 1.5373 at 211 nm); see the record’s notes.

slattery_2003/index_SiO2_quartz#

{
  "id": "index_SiO2_quartz",
  "material": "SiO2_quartz",
  "file": "SiO2_quartz/slattery_2003__index_SiO2_quartz.csv",
  "table": "tbl_43ed8a53704c",
  "quantity": "refractive_index",
  "abscissa_unit": "nm",
  "use": "excluded",
  "reproduced_from": [
    "D. N. Nikogosyan, Properties of Optical and Laser-related Materials, A Handbook, Wiley, Chichester, 1997"
  ],
  "parameters": {
    "axis": "o"
  }
}

Table 1: ‘calculated from dispersion relations, given in [12]’. Inconsistent with the paper’s own (1 - R)^2 = 88.57 %, which needs n = 1.641; see the record’s notes. Axis ‘o’ inferred from ‘(||c)’.

slattery_2003/index_BaF2#

{
  "id": "index_BaF2",
  "material": "BaF2",
  "file": "BaF2/slattery_2003__index_BaF2.csv",
  "table": "tbl_43ed8a53704c",
  "quantity": "refractive_index",
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "D. N. Nikogosyan, Properties of Optical and Laser-related Materials, A Handbook, Wiley, Chichester, 1997"
  ]
}

Table 1: ‘calculated from dispersion relations, given in [12]’.

slattery_2003/index_CaF2#

{
  "id": "index_CaF2",
  "material": "CaF2",
  "file": "CaF2/slattery_2003__index_CaF2.csv",
  "table": "tbl_43ed8a53704c",
  "quantity": "refractive_index",
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "D. N. Nikogosyan, Properties of Optical and Laser-related Materials, A Handbook, Wiley, Chichester, 1997"
  ]
}

Table 1: ‘calculated from dispersion relations, given in [12]’.

slattery_2003/alpha_SiO2#

{
  "id": "alpha_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__alpha_SiO2.csv",
  "table": "tbl_43ed8a53704c",
  "quantity": "absorption_coefficient",
  "unit": "cm-1",
  "abscissa_unit": "nm",
  "use": "primary",
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "base": "e",
    "form": "bulk",
    "technique": "spectrophotometry",
    "grade": "Suprasil"
  }
}

Table 1: ‘deduced from total absorbance minus optical density, corresponding to the reflection losses’ (spectrophotometer). Napierian base assumed from dragomir_2002’s definition (a doubt; see the record’s notes). Two Suprasil samples.

slattery_2003/alpha_SiO2_quartz#

{
  "id": "alpha_SiO2_quartz",
  "material": "SiO2_quartz",
  "file": "SiO2_quartz/slattery_2003__alpha_SiO2_quartz.csv",
  "table": "tbl_43ed8a53704c",
  "quantity": "absorption_coefficient",
  "unit": "cm-1",
  "abscissa_unit": "nm",
  "use": "primary",
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "base": "e",
    "form": "bulk",
    "technique": "spectrophotometry",
    "axis": "o"
  }
}

slattery_2003/alpha_BaF2#

{
  "id": "alpha_BaF2",
  "material": "BaF2",
  "file": "BaF2/slattery_2003__alpha_BaF2.csv",
  "table": "tbl_43ed8a53704c",
  "quantity": "absorption_coefficient",
  "unit": "cm-1",
  "abscissa_unit": "nm",
  "use": "primary",
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "base": "e",
    "form": "bulk",
    "technique": "spectrophotometry"
  }
}

slattery_2003/alpha_CaF2#

{
  "id": "alpha_CaF2",
  "material": "CaF2",
  "file": "CaF2/slattery_2003__alpha_CaF2.csv",
  "table": "tbl_43ed8a53704c",
  "quantity": "absorption_coefficient",
  "unit": "cm-1",
  "abscissa_unit": "nm",
  "use": "primary",
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "base": "e",
    "form": "bulk",
    "technique": "spectrophotometry"
  }
}

slattery_2003/band_gap_SiO2#

{
  "id": "band_gap_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__band_gap_SiO2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "band_gap",
  "unit": "eV",
  "abscissa": "none",
  "use": "reproduced",
  "reproduced_from": [
    "weinberg_1979"
  ],
  "parameters": {
    "kind": "photoconductivity"
  }
}

Table 2: ‘9.3 [15]’: weinberg_1979’s gap of amorphous SiO2 from the field dependence of photoconductivity.

slattery_2003/band_gap_SiO2_quartz#

{
  "id": "band_gap_SiO2_quartz",
  "material": "SiO2_quartz",
  "file": "SiO2_quartz/slattery_2003__band_gap_SiO2_quartz.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "band_gap",
  "unit": "eV",
  "abscissa": "none",
  "use": "reproduced",
  "reproduced_from": [
    "eva_1996"
  ],
  "parameters": {
    "kind": "not stated"
  }
}

Table 2: ‘≈9 [16]’: eva_1996’s approximate value, which it attributes to weinberg_1979.

slattery_2003/band_gap_BaF2#

{
  "id": "band_gap_BaF2",
  "material": "BaF2",
  "file": "BaF2/slattery_2003__band_gap_BaF2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "band_gap",
  "unit": "eV",
  "abscissa": "none",
  "use": "reproduced",
  "reproduced_from": [
    "eva_1996"
  ],
  "parameters": {
    "kind": "not stated"
  }
}

Table 2: ‘9.1 [16]’: eva_1996’s value, from taylor_1988.

slattery_2003/band_gap_CaF2#

{
  "id": "band_gap_CaF2",
  "material": "CaF2",
  "file": "CaF2/slattery_2003__band_gap_CaF2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "band_gap",
  "unit": "eV",
  "abscissa": "none",
  "use": "reproduced",
  "reproduced_from": [
    "eva_1996"
  ],
  "parameters": {
    "kind": "not stated"
  }
}

Table 2: ‘10 [16]’: eva_1996’s value (10.0), from taylor_1988.

slattery_2003/beta_211_SiO2#

{
  "id": "beta_211_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__beta_211_SiO2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "primary",
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "form": "bulk",
    "technique": "intensity-dependent transmission",
    "pulse_fs": 250,
    "grade": "Suprasil"
  }
}

Table 2, ‘This work’; also in the text (p. 4). One value for the two Suprasil samples.

slattery_2003/beta_211_SiO2_quartz#

{
  "id": "beta_211_SiO2_quartz",
  "material": "SiO2_quartz",
  "file": "SiO2_quartz/slattery_2003__beta_211_SiO2_quartz.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "primary",
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "form": "bulk",
    "technique": "intensity-dependent transmission",
    "pulse_fs": 250,
    "axis": "o"
  }
}

Table 2, ‘This work’; also in the text (p. 4).

slattery_2003/beta_211_BaF2#

{
  "id": "beta_211_BaF2",
  "material": "BaF2",
  "file": "BaF2/slattery_2003__beta_211_BaF2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "primary",
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "form": "bulk",
    "technique": "intensity-dependent transmission",
    "pulse_fs": 250
  }
}

Table 2, ‘This work’; also in the text (p. 4).

slattery_2003/beta_211_CaF2#

{
  "id": "beta_211_CaF2",
  "material": "CaF2",
  "file": "CaF2/slattery_2003__beta_211_CaF2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "primary",
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "form": "bulk",
    "technique": "intensity-dependent transmission",
    "pulse_fs": 250
  }
}

Table 2, ‘This work’; also in the text (p. 4).

slattery_2003/kittelmann_1994_SiO2#

{
  "id": "kittelmann_1994_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__kittelmann_1994_SiO2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "kittelmann_1994"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 800
  }
}

Table 2, [17]: kittelmann_1994’s Gaussian-profile beta at 193 nm; the +- is 70 % of the value.

slattery_2003/kittelmann_1994_BaF2#

{
  "id": "kittelmann_1994_BaF2",
  "material": "BaF2",
  "file": "BaF2/slattery_2003__kittelmann_1994_BaF2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "kittelmann_1994"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 800
  }
}

Table 2, [17]: kittelmann_1994’s Gaussian-profile beta at 193 nm; the +- is 70 % of the value.

slattery_2003/kittelmann_1994_CaF2#

{
  "id": "kittelmann_1994_CaF2",
  "material": "CaF2",
  "file": "CaF2/slattery_2003__kittelmann_1994_CaF2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "kittelmann_1994"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 800
  }
}

Table 2, [17]: kittelmann_1994’s Gaussian-profile beta at 193 nm; the +- is 70 % of the value.

slattery_2003/schenker_1995_SiO2#

{
  "id": "schenker_1995_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__schenker_1995_SiO2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "R. Schenker, L. Eichner, H. Vaidya, S. Vaidya, P. Schermerhorn, D. Fladd, W. G. Oldham, Proc. SPIE 2428 (1995) 458"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  }
}

Table 2, [18], 213 nm, pulse length printed ‘?’; footnote a: only a relative uncertainty in the original. Not in the library; dragomir_2002 Table 1 gives the fused-silica value as a range, 35-52.

slattery_2003/schenker_1995_SiO2_quartz#

{
  "id": "schenker_1995_SiO2_quartz",
  "material": "SiO2_quartz",
  "file": "SiO2_quartz/slattery_2003__schenker_1995_SiO2_quartz.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "R. Schenker, L. Eichner, H. Vaidya, S. Vaidya, P. Schermerhorn, D. Fladd, W. G. Oldham, Proc. SPIE 2428 (1995) 458"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  }
}

Table 2, [18], 213 nm, pulse length printed ‘?’; footnote a: only a relative uncertainty in the original. Not in the library; dragomir_2002 Table 1 gives the fused-silica value as a range, 35-52.

slattery_2003/gurzadyan_1992_SiO2#

{
  "id": "gurzadyan_1992_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__gurzadyan_1992_SiO2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "G. G. Gurzadyan, R. K. Ispiryan, Int. J. Nonl. Opt. Phys. 1 (3) (1992) 533"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 15000000
  }
}

Table 2, [19], 216 nm, 15 ps; footnote a: only a relative uncertainty in the original. Not in the library.

slattery_2003/gurzadyan_1992_SiO2_quartz#

{
  "id": "gurzadyan_1992_SiO2_quartz",
  "material": "SiO2_quartz",
  "file": "SiO2_quartz/slattery_2003__gurzadyan_1992_SiO2_quartz.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "G. G. Gurzadyan, R. K. Ispiryan, Int. J. Nonl. Opt. Phys. 1 (3) (1992) 533"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 15000000
  }
}

Table 2, [19], 216 nm, 15 ps; footnote a: only a relative uncertainty in the original. Not in the library.

slattery_2003/taylor_1988_SiO2#

{
  "id": "taylor_1988_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__taylor_1988_SiO2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "taylor_1988"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 700
  }
}

Table 2, [20]: taylor_1988’s beta at 248 nm; the +- is 65 % of the value.

slattery_2003/taylor_1988_BaF2#

{
  "id": "taylor_1988_BaF2",
  "material": "BaF2",
  "file": "BaF2/slattery_2003__taylor_1988_BaF2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "taylor_1988"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 700
  }
}

Table 2, [20]: taylor_1988’s beta at 248 nm; the +- is 65 % of the value.

slattery_2003/taylor_1988_CaF2#

{
  "id": "taylor_1988_CaF2",
  "material": "CaF2",
  "file": "CaF2/slattery_2003__taylor_1988_CaF2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "taylor_1988"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 700
  }
}

Table 2, [20]: taylor_1988’s beta at 248 nm; the +- is 65 % of the value.

slattery_2003/dragomir_2002_SiO2#

{
  "id": "dragomir_2002_SiO2",
  "material": "SiO2",
  "file": "SiO2/slattery_2003__dragomir_2002_SiO2.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "dragomir_2002"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 220
  }
}

Table 2, [1]: dragomir_2002’s beta at 264 nm (fused silica: its Suprasil value).

slattery_2003/dragomir_2002_SiO2_quartz#

{
  "id": "dragomir_2002_SiO2_quartz",
  "material": "SiO2_quartz",
  "file": "SiO2_quartz/slattery_2003__dragomir_2002_SiO2_quartz.csv",
  "table": "tbl_0a42752ea230",
  "quantity": "two_photon_absorption_coefficient",
  "unit": "cm/W",
  "scale": 1e-11,
  "abscissa_unit": "nm",
  "use": "reproduced",
  "reproduced_from": [
    "dragomir_2002"
  ],
  "uncertainty": {
    "column": true,
    "level": "not stated"
  },
  "parameters": {
    "pulse_fs": 220
  }
}

Table 2, [1]: dragomir_2002’s beta at 264 nm (fused silica: its Suprasil value).

Formulas#

No formulas are recorded.

Corrections#

No dataset errata are recorded in this source record.

Formula corrections, where recorded, appear with their formulas above. Curation notes may also discuss corrections or unresolved interpretation. Consult the review register for the checks and decisions.