slattery_2003 ============= S\. A\. Slattery and D\. N\. Nikogosyan, Opt\. Commun\. 228, 127 \(2003\) `Source record `__ · :doc:`Catalogue ` · :doc:`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 ~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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" } } Table 1\: 'deduced from total absorbance minus optical density, corresponding to the reflection losses' \(spectrophotometer\)\. Napierian base assumed from dragomir\_2002's definition \(a doubt; see the record's notes\)\. slattery\_2003/alpha\_BaF2 ~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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" } } Table 1\: 'deduced from total absorbance minus optical density, corresponding to the reflection losses' \(spectrophotometer\)\. Napierian base assumed from dragomir\_2002's definition \(a doubt; see the record's notes\)\. slattery\_2003/alpha\_CaF2 ~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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" } } Table 1\: 'deduced from total absorbance minus optical density, corresponding to the reflection losses' \(spectrophotometer\)\. Napierian base assumed from dragomir\_2002's definition \(a doubt; see the record's notes\)\. slattery\_2003/band\_gap\_SiO2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "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 :doc:`review register ` for the checks and decisions.