adair_1987
==========

R\. Adair, L\. L\. Chase, and S\. A\. Payne, "Nonlinear refractive\-index measurements of glasses using three\-wave frequency mixing", J\. Opt\. Soc\. Am\. B 4, 875\-881 \(1987\)

`Source record <https://github.com/LupoLab/optmat/blob/main/src/optmat/data/sources/adair_1987.toml>`__ · :doc:`Catalogue </the-data/sources>` · :doc:`Review register </register>`

DOI: `10\.1364/josab\.4\.000875 <https://doi.org/10.1364/josab.4.000875>`__

**Source kind:** measurement

**Recorded technique:** Nearly degenerate three\-wave mixing \(NDTWM\) at 1\.06 um \(Sec\. 3, pp\. 877\-878\)\: omega\_1 = the 1\.064\-um fundamental of a Q\-switched Nd\:YAG laser \(attenuated to \<= 5 mJ, spatially filtered; its pulse duration is not stated\), omega\_2 = 1\.071 um from the second harmonic\-pumped R6G dye laser \(0\.567 um\) Stokes\-shifted twice in H2 at 3e4 Torr, 0\.1 mJ, 3\-ns pulse; Delta = omega\_1 \- omega\_2 ~ 60 cm^\-1\. Both beams vertically polarized \(parallel linear polarizations\), combined, focused with 100\-cm lenses to a 400\-um spot, zero\-degree phase matching; the 2 omega\_1 \- omega\_2 signal of the sample and of a 1\-cm CS2 reference cell detected through a double monochromator by S\-1 photomultipliers and boxcars, the sample signal normalised shot by shot to the reference \(200 shots, then 50 background shots, five times; only shots within half a standard deviation of the mean reference used\)\. n2 of an unknown from its signal relative to a standard by Eqs\. \(6a\)\-\(6b\), \[chi1111\]\_u = \[chi1111\]\_s \(I\_u/I\_s\)^\(1/2\) \(n\_u/n\_s\)^2 \(l\_s/l\_u\) C^2, and Eq\. \(3\), n2\(LP\) = \(12 pi/n0\) chi1111\. The relative values were put on an absolute scale by 'equating our average value of n2 for those samples to theirs' for the seven glasses measured by time\-resolved interferometry by Weber et al\. \(Ref\. 13\) \(pp\. 878\-879\)\. Bulk samples several mm thick, of moderate optical quality\. Room temperature \(not stated\)\.

**Materials in structured entries:** BK7, C\-2828, E\-115, E\-131, E\-132, E\-133, ED\-2, ED\-3, ED\-8, FR\-5, Hoya\-5037, Hoya\-5038, K\-1172, K\-1261, Kigre\-3151, L\-109, L\-65, LG\-650, LHG\-5, LHG\-6, P\-108, Q\-246, Q\-88, S\-7606, SF\-6, SiO2, fluorozirconate\-9028

**Dataset quantities:** nonlinear\_index\_field

**Contents:** 63 datasets; 1 formula.

Curation notes
--------------

Journal pages 875\-881 = pdf pages 1\-7 \(journal page = 874 \+ pdf page\)\. Identity checked against the first page \(title, authors, J\. Opt\. Soc\. Am\. B 4, 875\)\. Table 2 \(p\. 879\) is the only data table; Table 1 \(p\. 878\) lists the compositions \(mol %\) and makers, which the material registry entries quote\.

DEFINITIONS \(Gaussian esu, quoted\)\. p\. 875\: 'The nonlinear refractive index is defined by n = n0 \+ n2 \<E^2\>, where n0 is the linear refractive index and E is the optical electric field\.' Eq\. \(1\)\: P\_crit = c lambda^2/\(32 pi^2 n2\)\. Eq\. \(2\)\: P1^\(3\)\(r, omega\_a\) = 3 chi1111^\(3\)\(\-omega\_a; omega\_1, omega\_1, \-omega\_2\) E\(omega\_1\)^2 E\(omega\_2\)\* for parallel polarizations in an isotropic material \(Bloembergen's convention\)\. Eq\. \(3\)\: n2\(LP\) = \(12 pi/n0\) chi1111^\(3\)\(\-omega; omega, omega, \-omega\), 'where LP stands for linearly polarized'\. No circular\-polarization value is given\. The n2 of Table 2 are for linear polarization \(esu; the paper converts nothing to cm2/W\)\.

PART \(p\. 876\)\. Eq\. \(4\)\: n2 = n2\(electronic\) \+ n2\(nuclear\) \+ n2\(electrostrictive\) \+ n2\(thermal\)\. 'Using R = 200 um and V = 5 x 10^5 cm/sec, we find that R/V = 40 nsec\. Our effective measurement time is of the order of the reciprocal of the frequency difference Delta^\-1 ~ 5 x 10^\-13 sec\. Because of this extremely large difference in time scale, we ignore the latter two effects\. We consider only the electronic and nuclear contributions\.' With Hellwarth's curves for fused quartz, Re\(A \+ B\) = 5\.9e\-15 cm^3/erg at Delta = 0 and 6\.0e\-15 at 60 cm^\-1 \(Im 0\.0 and 0\.5e\-15\)\: 'the nuclear contribution changes little from Delta = 0 to Delta = 60 cm^\-1'; 'the nuclear contribution, on the average, accounts for only 25% of the total n2' \(Refs\. 24\-26\) \(p\. 877\)\. Hence part = electronic\_vibrational for the measured values \(Raman included, electrostriction and thermal not\), as for adair\_1989\.

ACCURACY \(p\. 879\)\: 'We believe that our experimental method provides results that are accurate to within 15%\.' Level not stated; recorded as relative 0\.15\. The absolute scale is Weber et al\.'s\: any error of their seven TRI values is carried \(the reproduced datasets weber\_1978\_\*\)\. FINDING \(computed 2026\-09\-27\)\: the printed calibrated values of the seven standards average 1\.356e\-13 esu against 1\.286e\-13 for Weber et al\.'s \(the mean of the ratios is 1\.064\), so the stated equal\-average calibration is not reproduced by the printed numbers \(5 % high\); the paper gives no other detail\. The sample\-length dependence \(Eq\. 5, I\_a proportional to l^2\) was checked with CS2 cells of several lengths \(Fig\. 2\)\.

TABLE 2 \(tbl\_cd009634988d, image checked\: every cell agrees\)\. Columns\: 'n2 meas\. a' \(this work\: datasets n2\_\*, primary\), 'n2 meas\.' with footnote c \(Ref\. 13, Weber, Milam and Smith 1978\: datasets weber\_1978\_\*, reproduced\) or d \(Ref\. 7, Moran, She and Carman 1975\: datasets moran\_1975\_\*, reproduced\), and 'n2 calc\. b' \(Ref\. 31, Stokowski, Saroyan and Weber 1981, LLNL report M\-95\: datasets calc\_\*, reproduced\)\. The literature values are weber\_1978 Table 1 converted to esu with its n\_D by its Eq\. \(18\) \(computed 2026\-09\-27\: LHG\-5 1\.158, LHG\-6 1\.009, Q\-88 1\.140, FR\-5 2\.092, ED\-2 1\.414, fused silica 0\.950, BK\-7 1\.241, all equal to the printed cells to the printed digits; ED\-2 is Weber's reference\-a value 3\.77, not his reference\-d 4\.05\)\. The two Moran values \(C2828 2\.077, SF\-6 9\.129\) are the same conversion of Weber's asterisked entries, i\.e\. Moran's CS2\-relative values scaled by Weber et al\. to ED\-2 = 4\.05e\-20 m2/W\. 'The glasses are grouped by types' \(Table 1 footnote a\)\: the Type column labels each group once\. Glass\-name discrepancies between the tables \(images checked\)\: Table 1 'K\-133' against Table 2 'E\-133' \(registered as E\-133\: the other Owens\-Illinois glasses of the group are E\-115, E\-131, E\-132; the NBS glasses are K\-1172, K\-1261\), Table 1 'SF6' against Table 2 'SF\-6'\. Table 1's BK\-7 composition sums to 102\.9 % with '4 Nd2O3' \(see the dataset notes\)\.

FORMULA\. Eq\. \(10a\) \(Boling et al\., Ref\. 28\) with K = 68 and the constant 1\.52 \(Boling et al\. and adair\_1989 print 1\.517\)\: recorded as bgo\_10a\. The paper uses Ref\. 31's calculated values rather than computing its own\. Eq\. \(12\)\: n2 = \(L^4 pi/2n\) N gamma with L = \(n^2 \+ 2\)/3, and Eq\. \(13\), n^2 \- 1 = 4 pi L N alpha \(p\. 880\); Eq\. \(11\), gamma = Q alpha^2\. Eq\. \(14\), alpha = s e^2/m\(omega\_0^2 \- omega^2\)\.

TEXT VALUES\. The fluorophosphates 'have the lowest n2 values of 0\.6 to 0\.8 x 10^\-13 esu' and E\-115 'the largest n2 value of 0\.80' \(p\. 880\); fused silica 0\.85 and ED\-8 1\.69 \(p\. 880\)\: all repeat Table 2\. The lowest VUV bands of fused quartz at 10\.3 and 11\.3 eV \(Philipp; p\. 880\), quoted, not recorded\.

FIGURES \(not digitised\)\. Fig\. 1 \(p\. 877\)\: the apparatus\. Fig\. 2 \(p\. 878\)\: square root of the TWM signal against CS2 cell length \(linear\)\. Fig\. 3 \(p\. 879\)\: calculated against measured n2 of the Table 2 glasses \(SF\-6 and the tellurites divided by 15\)\.

REPRODUCTIONS OF THIS PAPER\. adair\_1989 cites it \(Ref\. 19\) for the method only\. ensley\_2019 reproduces its BK\-7 value \(Ensley's reference m\); refractiveindex\.info's BK7 'Adair' n2 page is from this paper \(adair\_1989 notes\)\.

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

Datasets
--------

adair\_1987/n2\_E\-115
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_E-115",
     "material": "E-115",
     "file": "E-115/adair_1987__n2_E-115.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Owens-Illinois"
     }
   }

Table 2 \(p\. 879\), row 'E\-115' \(fluorophosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_E\-115
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_E-115",
     "material": "E-115",
     "file": "E-115/adair_1987__calc_E-115.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'E\-115', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_E\-131
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_E-131",
     "material": "E-131",
     "file": "E-131/adair_1987__n2_E-131.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Owens-Illinois"
     }
   }

Table 2 \(p\. 879\), row 'E\-131' \(fluorophosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_E\-131
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_E-131",
     "material": "E-131",
     "file": "E-131/adair_1987__calc_E-131.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'E\-131', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_E\-132
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_E-132",
     "material": "E-132",
     "file": "E-132/adair_1987__n2_E-132.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Owens-Illinois"
     }
   }

Table 2 \(p\. 879\), row 'E\-132' \(fluorophosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_E\-132
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_E-132",
     "material": "E-132",
     "file": "E-132/adair_1987__calc_E-132.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'E\-132', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_E\-133
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_E-133",
     "material": "E-133",
     "file": "E-133/adair_1987__n2_E-133.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Owens-Illinois"
     }
   }

Table 2 \(p\. 879\), row 'E\-133' \(fluorophosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\. Table 1 prints this glass as 'K\-133' \(Owens\-Illinois\); Table 2 prints 'E\-133'\.

adair\_1987/calc\_E\-133
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_E-133",
     "material": "E-133",
     "file": "E-133/adair_1987__calc_E-133.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'E\-133', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_K\-1172
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_K-1172",
     "material": "K-1172",
     "file": "K-1172/adair_1987__n2_K-1172.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "NBS"
     }
   }

Table 2 \(p\. 879\), row 'K\-1172' \(fluorophosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_K\-1172
~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_K-1172",
     "material": "K-1172",
     "file": "K-1172/adair_1987__calc_K-1172.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'K\-1172', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_LHG\-5
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_LHG-5",
     "material": "LHG-5",
     "file": "LHG-5/adair_1987__n2_LHG-5.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Hoya"
     }
   }

Table 2 \(p\. 879\), row 'LHG\-5' \(phosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/weber\_1978\_LHG\-5
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "weber_1978_LHG-5",
     "material": "LHG-5",
     "file": "LHG-5/adair_1987__weber_1978_LHG-5.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "time-resolved interferometry (TRI)",
       "polarization": "linear"
     }
   }

Table 2 \(p\. 879\), row 'LHG\-5', column 'n2 meas\.', footnote c \(Ref\. 13, Weber, Milam and Smith 1978\)\: Weber et al\.'s time\-resolved interferometry at 1064 nm \(100\-1000 ps\), their gamma converted to esu with their n\_D \(weber\_1978 Table 1 by their Eq\. 18 reproduces this cell to the printed digits; source notes\)\. One of the seven calibration standards of this paper\.

adair\_1987/calc\_LHG\-5
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_LHG-5",
     "material": "LHG-5",
     "file": "LHG-5/adair_1987__calc_LHG-5.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'LHG\-5', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_LHG\-6
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_LHG-6",
     "material": "LHG-6",
     "file": "LHG-6/adair_1987__n2_LHG-6.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Hoya"
     }
   }

Table 2 \(p\. 879\), row 'LHG\-6' \(phosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/weber\_1978\_LHG\-6
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "weber_1978_LHG-6",
     "material": "LHG-6",
     "file": "LHG-6/adair_1987__weber_1978_LHG-6.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "time-resolved interferometry (TRI)",
       "polarization": "linear"
     }
   }

Table 2 \(p\. 879\), row 'LHG\-6', column 'n2 meas\.', footnote c \(Ref\. 13, Weber, Milam and Smith 1978\)\: Weber et al\.'s time\-resolved interferometry at 1064 nm \(100\-1000 ps\), their gamma converted to esu with their n\_D \(weber\_1978 Table 1 by their Eq\. 18 reproduces this cell to the printed digits; source notes\)\. One of the seven calibration standards of this paper\.

adair\_1987/calc\_LHG\-6
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_LHG-6",
     "material": "LHG-6",
     "file": "LHG-6/adair_1987__calc_LHG-6.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'LHG\-6', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_Q\-88
~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_Q-88",
     "material": "Q-88",
     "file": "Q-88/adair_1987__n2_Q-88.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Kigre"
     }
   }

Table 2 \(p\. 879\), row 'Q\-88' \(phosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/weber\_1978\_Q\-88
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "weber_1978_Q-88",
     "material": "Q-88",
     "file": "Q-88/adair_1987__weber_1978_Q-88.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "time-resolved interferometry (TRI)",
       "polarization": "linear"
     }
   }

Table 2 \(p\. 879\), row 'Q\-88', column 'n2 meas\.', footnote c \(Ref\. 13, Weber, Milam and Smith 1978\)\: Weber et al\.'s time\-resolved interferometry at 1064 nm \(100\-1000 ps\), their gamma converted to esu with their n\_D \(weber\_1978 Table 1 by their Eq\. 18 reproduces this cell to the printed digits; source notes\)\. One of the seven calibration standards of this paper\.

adair\_1987/calc\_Q\-88
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_Q-88",
     "material": "Q-88",
     "file": "Q-88/adair_1987__calc_Q-88.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'Q\-88', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_P\-108
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_P-108",
     "material": "P-108",
     "file": "P-108/adair_1987__n2_P-108.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Kigre"
     }
   }

Table 2 \(p\. 879\), row 'P\-108' \(phosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_P\-108
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_P-108",
     "material": "P-108",
     "file": "P-108/adair_1987__calc_P-108.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'P\-108', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_Hoya\-5037
~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_Hoya-5037",
     "material": "Hoya-5037",
     "file": "Hoya-5037/adair_1987__n2_Hoya-5037.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Hoya"
     }
   }

Table 2 \(p\. 879\), row '5037' \(phosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_Hoya\-5037
~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_Hoya-5037",
     "material": "Hoya-5037",
     "file": "Hoya-5037/adair_1987__calc_Hoya-5037.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row '5037', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_Hoya\-5038
~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_Hoya-5038",
     "material": "Hoya-5038",
     "file": "Hoya-5038/adair_1987__n2_Hoya-5038.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Hoya"
     }
   }

Table 2 \(p\. 879\), row '5038' \(phosphate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_Hoya\-5038
~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_Hoya-5038",
     "material": "Hoya-5038",
     "file": "Hoya-5038/adair_1987__calc_Hoya-5038.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row '5038', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_FR\-5
~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_FR-5",
     "material": "FR-5",
     "file": "FR-5/adair_1987__n2_FR-5.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Hoya"
     }
   }

Table 2 \(p\. 879\), row 'FR\-5' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/weber\_1978\_FR\-5
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "weber_1978_FR-5",
     "material": "FR-5",
     "file": "FR-5/adair_1987__weber_1978_FR-5.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "time-resolved interferometry (TRI)",
       "polarization": "linear"
     }
   }

Table 2 \(p\. 879\), row 'FR\-5', column 'n2 meas\.', footnote c \(Ref\. 13, Weber, Milam and Smith 1978\)\: Weber et al\.'s time\-resolved interferometry at 1064 nm \(100\-1000 ps\), their gamma converted to esu with their n\_D \(weber\_1978 Table 1 by their Eq\. 18 reproduces this cell to the printed digits; source notes\)\. One of the seven calibration standards of this paper\.

adair\_1987/calc\_FR\-5
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_FR-5",
     "material": "FR-5",
     "file": "FR-5/adair_1987__calc_FR-5.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'FR\-5', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_ED\-2
~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_ED-2",
     "material": "ED-2",
     "file": "ED-2/adair_1987__n2_ED-2.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Owens-Illinois"
     }
   }

Table 2 \(p\. 879\), row 'ED\-2' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/weber\_1978\_ED\-2
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "weber_1978_ED-2",
     "material": "ED-2",
     "file": "ED-2/adair_1987__weber_1978_ED-2.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "time-resolved interferometry (TRI)",
       "polarization": "linear"
     }
   }

Table 2 \(p\. 879\), row 'ED\-2', column 'n2 meas\.', footnote c \(Ref\. 13, Weber, Milam and Smith 1978\)\: Weber et al\.'s time\-resolved interferometry at 1064 nm \(100\-1000 ps\), their gamma converted to esu with their n\_D \(weber\_1978 Table 1 by their Eq\. 18 reproduces this cell to the printed digits; source notes\)\. One of the seven calibration standards of this paper\.

adair\_1987/calc\_ED\-2
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_ED-2",
     "material": "ED-2",
     "file": "ED-2/adair_1987__calc_ED-2.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'ED\-2', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_SiO2
~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_SiO2",
     "material": "SiO2",
     "file": "SiO2/adair_1987__n2_SiO2.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Dynasil 4001"
     }
   }

Table 2 \(p\. 879\), row 'Fused silica' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\. 100 SiO2 \(Dynasil 4001\), Table 1\.

adair\_1987/weber\_1978\_SiO2
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "weber_1978_SiO2",
     "material": "SiO2",
     "file": "SiO2/adair_1987__weber_1978_SiO2.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "time-resolved interferometry (TRI)",
       "polarization": "linear"
     }
   }

Table 2 \(p\. 879\), row 'Fused silica', column 'n2 meas\.', footnote c \(Ref\. 13, Weber, Milam and Smith 1978\)\: Weber et al\.'s time\-resolved interferometry at 1064 nm \(100\-1000 ps\), their gamma converted to esu with their n\_D \(weber\_1978 Table 1 by their Eq\. 18 reproduces this cell to the printed digits; source notes\)\. One of the seven calibration standards of this paper\.

adair\_1987/calc\_SiO2
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_SiO2",
     "material": "SiO2",
     "file": "SiO2/adair_1987__calc_SiO2.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'Fused silica', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_C\-2828
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_C-2828",
     "material": "C-2828",
     "file": "C-2828/adair_1987__n2_C-2828.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "American Optical"
     }
   }

Table 2 \(p\. 879\), row 'C2828' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/moran\_1975\_C\-2828
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "moran_1975_C-2828",
     "material": "C-2828",
     "file": "C-2828/adair_1987__moran_1975_C-2828.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "M. J. Moran, C.-Y. She, and R. L. Carman, IEEE J. Quantum Electron. QE-11, 259-263 (1975)",
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "unknown",
       "coefficient": "self",
       "technique": "relative time-resolved interferometry against CS2 (Moran et al.)"
     }
   }

Table 2 \(p\. 879\), row 'C2828', column 'n2 meas\.', footnote d \(Ref\. 7, Moran, She and Carman 1975\)\. The number equals weber\_1978 Table 1's value for this glass \(Moran et al\.'s measurement relative to ED\-2, scaled by Weber et al\. to ED\-2 = 4\.05e\-20 m2/W, their asterisk\) converted to esu with Weber's n\_D \(source notes\)\: the scaled number, not Moran's own\.

adair\_1987/calc\_C\-2828
~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_C-2828",
     "material": "C-2828",
     "file": "C-2828/adair_1987__calc_C-2828.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'C2828', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_ED\-8
~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_ED-8",
     "material": "ED-8",
     "file": "ED-8/adair_1987__n2_ED-8.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Owens-Illinois"
     }
   }

Table 2 \(p\. 879\), row 'ED\-8' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_ED\-8
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_ED-8",
     "material": "ED-8",
     "file": "ED-8/adair_1987__calc_ED-8.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'ED\-8', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_S\-7606
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_S-7606",
     "material": "S-7606",
     "file": "S-7606/adair_1987__n2_S-7606.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Schott"
     }
   }

Table 2 \(p\. 879\), row 'S\-7606' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_S\-7606
~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_S-7606",
     "material": "S-7606",
     "file": "S-7606/adair_1987__calc_S-7606.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'S\-7606', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_LG\-650
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_LG-650",
     "material": "LG-650",
     "file": "LG-650/adair_1987__n2_LG-650.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Schott"
     }
   }

Table 2 \(p\. 879\), row 'LG\-650' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_LG\-650
~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_LG-650",
     "material": "LG-650",
     "file": "LG-650/adair_1987__calc_LG-650.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'LG\-650', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_ED\-3
~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_ED-3",
     "material": "ED-3",
     "file": "ED-3/adair_1987__n2_ED-3.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Owens-Illinois"
     }
   }

Table 2 \(p\. 879\), row 'ED\-3' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_ED\-3
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_ED-3",
     "material": "ED-3",
     "file": "ED-3/adair_1987__calc_ED-3.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'ED\-3', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_Q\-246
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_Q-246",
     "material": "Q-246",
     "file": "Q-246/adair_1987__n2_Q-246.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Kigre"
     }
   }

Table 2 \(p\. 879\), row 'Q\-246' \(silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_Q\-246
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_Q-246",
     "material": "Q-246",
     "file": "Q-246/adair_1987__calc_Q-246.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'Q\-246', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_BK7
~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_BK7",
     "material": "BK7",
     "file": "BK7/adair_1987__n2_BK7.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Schott"
     }
   }

Table 2 \(p\. 879\), row 'BK\-7' \(borosilicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\. Table 1 gives the composition 69\.6 SiO2, 9\.9 B2O3, 8\.4 Na2O, 8\.4 K2O, 0\.07 CaO, 2\.5 BaO, 0\.04 Al2O3, 4 Nd2O3 \(Schott\) mol %, which sums to 102\.9 \(with 0\.4 Nd2O3, 99\.3\)\: an Nd\-doped BK\-7 or a misprint; the sample is recorded as BK7 \(Schott BK 7\), as the paper names it and calibrates it against Weber et al\.'s BK\-7\.

adair\_1987/weber\_1978\_BK7
~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "weber_1978_BK7",
     "material": "BK7",
     "file": "BK7/adair_1987__weber_1978_BK7.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "time-resolved interferometry (TRI)",
       "polarization": "linear"
     }
   }

Table 2 \(p\. 879\), row 'BK\-7', column 'n2 meas\.', footnote c \(Ref\. 13, Weber, Milam and Smith 1978\)\: Weber et al\.'s time\-resolved interferometry at 1064 nm \(100\-1000 ps\), their gamma converted to esu with their n\_D \(weber\_1978 Table 1 by their Eq\. 18 reproduces this cell to the printed digits; source notes\)\. One of the seven calibration standards of this paper\.

adair\_1987/calc\_BK7
~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_BK7",
     "material": "BK7",
     "file": "BK7/adair_1987__calc_BK7.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'BK\-7', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_L\-109
~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_L-109",
     "material": "L-109",
     "file": "L-109/adair_1987__n2_L-109.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Kigre"
     }
   }

Table 2 \(p\. 879\), row 'L\-109' \(borate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_L\-109
~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_L-109",
     "material": "L-109",
     "file": "L-109/adair_1987__calc_L-109.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'L\-109', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_L\-65
~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_L-65",
     "material": "L-65",
     "file": "L-65/adair_1987__n2_L-65.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "NBS"
     }
   }

Table 2 \(p\. 879\), row 'L\-65' \(aluminate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_L\-65
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_L-65",
     "material": "L-65",
     "file": "L-65/adair_1987__calc_L-65.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'L\-65', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_fluorozirconate\-9028
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_fluorozirconate-9028",
     "material": "fluorozirconate-9028",
     "file": "fluorozirconate-9028/adair_1987__n2_fluorozirconate-9028.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Univ. Remes"
     }
   }

Table 2 \(p\. 879\), row '9028' \(fluorozirconate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\.

adair\_1987/calc\_fluorozirconate\-9028
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_fluorozirconate-9028",
     "material": "fluorozirconate-9028",
     "file": "fluorozirconate-9028/adair_1987__calc_fluorozirconate-9028.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row '9028', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_K\-1261
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_K-1261",
     "material": "K-1261",
     "file": "K-1261/adair_1987__n2_K-1261.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "NBS"
     }
   }

Table 2 \(p\. 879\), row 'K\-1261' \(tellurite\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\. Fig\. 3 plots the tellurites divided by 15\.

adair\_1987/calc\_K\-1261
~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_K-1261",
     "material": "K-1261",
     "file": "K-1261/adair_1987__calc_K-1261.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'K\-1261', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_Kigre\-3151
~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_Kigre-3151",
     "material": "Kigre-3151",
     "file": "Kigre-3151/adair_1987__n2_Kigre-3151.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Kigre"
     }
   }

Table 2 \(p\. 879\), row '3151' \(tellurite\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\. Fig\. 3 plots the tellurites divided by 15\.

adair\_1987/calc\_Kigre\-3151
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_Kigre-3151",
     "material": "Kigre-3151",
     "file": "Kigre-3151/adair_1987__calc_Kigre-3151.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row '3151', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

adair\_1987/n2\_SF\-6
~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "n2_SF-6",
     "material": "SF-6",
     "file": "SF-6/adair_1987__n2_SF-6.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "primary",
     "uncertainty": {
       "relative": 0.15,
       "level": "not stated"
     },
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic_vibrational",
       "coefficient": "self",
       "technique": "nearly degenerate three-wave mixing (NDTWM), 1.064 and 1.071 um, Delta ~ 60 cm^-1, relative to CS2",
       "polarization": "linear",
       "form": "bulk",
       "grade": "Schott"
     }
   }

Table 2 \(p\. 879\), row 'SF\-6' \(lead silicate\), column 'n2 meas\. a' \(this work\), 10^\-13 esu\. NDTWM at 1\.064/1\.071 um, relative to CS2 and scaled to Weber et al\. 1978's TRI values of seven glasses \(source notes\)\. 57\.6 SiO2, 2 K2O, 40\.4 PbO \(Schott\), Table 1 \(printed 'SF6' there, 'SF\-6' in Table 2\)\. Fig\. 3 plots it divided by 15\.

adair\_1987/moran\_1975\_SF\-6
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "moran_1975_SF-6",
     "material": "SF-6",
     "file": "SF-6/adair_1987__moran_1975_SF-6.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "M. J. Moran, C.-Y. She, and R. L. Carman, IEEE J. Quantum Electron. QE-11, 259-263 (1975)",
       "weber_1978"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "unknown",
       "coefficient": "self",
       "technique": "relative time-resolved interferometry against CS2 (Moran et al.)"
     }
   }

Table 2 \(p\. 879\), row 'SF\-6', column 'n2 meas\.', footnote d \(Ref\. 7, Moran, She and Carman 1975\)\. The number equals weber\_1978 Table 1's value for this glass \(Moran et al\.'s measurement relative to ED\-2, scaled by Weber et al\. to ED\-2 = 4\.05e\-20 m2/W, their asterisk\) converted to esu with Weber's n\_D \(source notes\)\: the scaled number, not Moran's own\.

adair\_1987/calc\_SF\-6
~~~~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "calc_SF-6",
     "material": "SF-6",
     "file": "SF-6/adair_1987__calc_SF-6.csv",
     "table": "tbl_cd009634988d",
     "quantity": "nonlinear_index_field",
     "unit": "esu",
     "scale": 1e-13,
     "abscissa_unit": "um",
     "use": "reproduced",
     "reproduced_from": [
       "S. E. Stokowski, R. A. Saroyan, and M. J. Weber, Nd-doped laser glass: spectroscopic and physical properties, Lawrence Livermore National Laboratory report M-95 (1981)"
     ],
     "parameters": {
       "definition": "<E^2>, 'E is the optical electric field' (p. 875)",
       "part": "electronic",
       "coefficient": "self"
     }
   }

Table 2 \(p\. 879\), row 'SF\-6', column 'n2 calc\. b' \(footnote b, Ref\. 31\)\: the Boling\-Glass\-Owyoung Eq\. \(10a\) value, 'The calculated n2 values and the linear refractive\-index measurements were obtained from Ref\. 31' \(p\. 878\)\. A long\-wavelength estimate of the electronic n2 \(formula bgo\_10a\), not a measurement; wavelength not stated\.

Formulas
--------

adair\_1987/bgo\_10a
~~~~~~~~~~~~~~~~~~~~

.. code-block:: text

   {
     "id": "bgo_10a",
     "equation": "Eqs. (10a)-(10b), p. 877",
     "printed": "n_2 (10^{-13} esu) = 68 (n_d - 1)(n_d^2 + 2)^2 / ( \\nu_d [1.52 + (n_d^2 + 2)(n_d + 1) \\nu_d / (6 n_d)]^{1/2} ), \\nu_d = (n_d - 1)/(n_F - n_C)",
     "variable": "n_d: the index at 5876 A; nu_d the Abbe number with lambda_F = 4861 A and lambda_C = 6563 A; n2 in 10^-13 esu (n = n0 + n2 <E^2>)",
     "range": "glasses and fluoride crystals with one dominant polarizable constituent (p. 880: SF-6 and the tellurites violate it)",
     "coefficients": {
       "K": "68",
       "constant": "1.52"
     },
     "check": "Not reproducible from this paper, which prints neither n_d nor nu_d (Table 2's calculated column is Ref. 31's). With boling_1978's fused silica n_d = 1.458 and nu_d = 70 it gives 0.833 (Table 2: 0.83); with milam_1976's BK 7 (1.517, 64) 1.153 against Table 2's BK-7 1.18, and with ED-2 (1.567, 54) 1.729 against 1.60, so Ref. 31's n_d and nu_d differ from Milam's (computed 2026-09-27)."
   }

The Boling\-Glass\-Owyoung Abbe\-number formula \(boling\_1978 Eq\. 38, whose constant is 1\.517; adair\_1989 Eq\. 6\)\. The derivation assumes one polarizable constituent and gamma = Q alpha^2, 'There is no rigorous justification for this assumption' \(p\. 877\)\.

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 </register>` for the checks and decisions.