cleanup data folder

This commit is contained in:
Benoît Sierro
2023-07-27 11:11:13 +02:00
parent ee1683b107
commit 3d9b4f57f3
16 changed files with 65993 additions and 452 deletions

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@@ -1,3 +1,4 @@
THz,gain
0,0
0.01, 1.4653e-3
0.0234, 1.4682e-3
1 0 THz 0 gain
1 THz gain
2 0 0 0 0
3 0.01 0.01 1.4653e-3 1.4653e-3
4 0.0234 0.0234 1.4682e-3 1.4682e-3

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@@ -6,4 +6,4 @@ echo "starting ray head node"
ray start --head --node-ip-address=$1 --port=6379 --redis-password=$2 --num-cpus=$SLURM_CPUS_PER_TASK --dashboard-host=127.0.0.1
sleep infinity
sleep infinity

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@@ -2,4 +2,4 @@
head /proc/cpuinfo
echo "starting ray worker node"
ray start --address $1 --redis-password=$2 --num-cpus=$SLURM_CPUS_PER_TASK
sleep infinity
sleep infinity

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@@ -1,10 +1,10 @@
# source of the Sellmeir coefficients
Air, Nitrogen, Helium, Neon, Argon, Krypton, Xenon : A. Börzsönyi et al. "Dispersion measurement of inert gases and gas mixtures at 800 nm" (2008)
Silica : I. H. Malitson. Interspecimen comparison of the refractive index of fused silica (1965)
In sellmeierRefractiveIndex : see refractiveindex.info
Van der Waals constants from https://en.wikipedia.org/wiki/Van_der_Waals_constants_(data_page)
# `materials.json`
Contains material property like Sellmeir coefficients, nonlinear refractive index and Van der Waals constants.
Sources are embeded in the document and are completed as such:
Van der Waals constants : https://en.wikipedia.org/wiki/Van_der_Waals_constants_(data_page)
Chi3 : Wahlstrand 2012
# `raman_response.csv`
Raman impulse response recovered from measured gain spectrum. This is used then `raman_type` is set to `"measured"`.

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@@ -1,29 +0,0 @@
DTf.
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mainy 0
window 0 23 1920 1177
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texts \z , , , \z
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params 7 1 1 2 3 1 4
dump show 1028.0 185.0
point 109.5 1241.0 124.35055146851568 1235.0450758962884 124.35055146851568 1235.0450758962884 2 0 -16724992
point 3101.0 1234.0 3101.000000000001 1234.0 3101.000000000001 1234.0 0 0 -3407872
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@@ -0,0 +1,447 @@
{
"air":
{
"a": 0.1358,
"atomic_mass": 4.809e-26,
"atomic_number": 7.14,
"b": 3.64e-5,
"kerr":
{
"P0": 101325,
"T0": 293.15,
"n2": 4e-23,
"source": "Pigeon, J. J., Tochitsky, S. Y., Welch, E. C., & Joshi, C. (2016). Measurements of the nonlinear refractive index of air, N 2, and O 2 at 10 μm using four-wave mixing. Optics letters, 41(17), 3924-3927."
},
"sellmeier":
{
"B":
[
57921050000,
1679170000
],
"C":
[
2.380185e+14,
5.7362e+13
],
"P0": 101325,
"T0": 288.15,
"kind": 2
}
},
"argon":
{
"a": 0.1355,
"atomic_mass": 6.6338e-26,
"atomic_number": 18,
"b": 3.201e-5,
"ionization_energy": 2.5249661793774e-18,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 9.7e-24,
"source": "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
},
"sellmeier":
{
"B":
[
2501410000,
500283000,
52234300000
],
"C":
[
9.1012e+13,
8.7892e+13,
2.1402e+14
],
"P0": 101325,
"T0": 273.15,
"kind": 2,
"source": "A. Bideau-Mehu, Y. Guern, R. Abjean, A. Johannin-Gilles. Measurement of refractive indices of neon, argon, krypton and xenon in the 253.7-140.4 nm wavelength range. Dispersion relations and estimated oscillator strengths of the resonance lines. J. Quant. Spectrosc. Rad. Transfer 25, 395-402 (1981)"
}
},
"argon_alt":
{
"a": 0.1355,
"b": 3.201e-5,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 9.7e-24,
"source": "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
},
"sellmeier":
{
"B":
[
0.0002033229,
0.0003445831
],
"C":
[
2.0612e-16,
8.066e-15
],
"P0": 101325,
"T0": 273.15,
"kind": 1,
"source": "A. Börzsönyi, Z. Heiner, M. P. Kalashnikov, A. P. Kovács, and K. Osvay, Dispersion measurement of inert gases and gas mixtures at 800 nm, Appl. Opt. 47, 4856-4863 (2008)"
}
},
"argon_alt2":
{
"a": 0.1355,
"b": 3.201e-5,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 9.7e-24,
"source": "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
},
"sellmeier":
{
"B":
[
0.030182943
],
"C":
[
1.44e+14
],
"P0": 101325,
"T0": 273.15,
"const": 6.7867e-5,
"kind": 2,
"source": "E. R. Peck and D. J. Fisher. Dispersion of argon, J. Opt. Soc. Am. 54, 1362-1364 (1964)"
}
},
"d-zlaf52la":
{
"sellmeier":
{
"B":
[
-8487502830,
3.1753525,
3.71301651e-14,
-1.09609062e-27,
2.4418582e-40,
-8.94583294e-54
],
"C": [],
"kind": 3,
"reference":
[
"CDGM Zemax catalog 2017-09 (obtained from http://www.cdgmgd.com)"
]
}
},
"e7":
{
"sellmeier":
{
"B":
[
0,
7.2e-15,
3e-28
],
"C": [],
"kind": 3,
"reference":
[
"J. Li, C. H. Wen, S. Gauza, R. Lu and S. T. Wu. Refractive indices of liquid crystals for display applications, J. Disp. Technol. 1, 51-61, 2005"
]
}
},
"helium":
{
"a": 0.00346,
"atomic_mass": 6.646477e-27,
"atomic_number": 2,
"b": 2.38e-5,
"ionization_energy": 3.9393356074281e-18,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 3.1e-25,
"source": "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
},
"sellmeier":
{
"B":
[
2.16463842e-5,
2.10561127e-7,
4.7509272e-5
],
"C":
[
-6.80769781e-16,
5.13251289e-15,
3.18621354e-15
],
"P0": 101325,
"T0": 273.15,
"kind": 1,
"source": "A. Ermolov, K. F. Mak, M. H. Frosz, J. C. Travers, P. St. J. Russell, Supercontinuum generation in the vacuum ultraviolet through dispersive-wave and soliton-plasma interaction in a noble-gas-filled hollow-core photonic crystal fiber, Phys. Rev. A 92, 033821 (2015)"
}
},
"helium_alt":
{
"a": 0.00346,
"b": 2.38e-5,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 3.1e-25
},
"sellmeier":
{
"B":
[
14755297000
],
"C":
[
4.262974e+14
],
"P0": 101325,
"T0": 273.15,
"kind": 2,
"source": " C. Cuthbertson and M. Cuthbertson. The refraction and dispersion of neon and helium. Proc. R. Soc. London A 135, 40-47 (1936)"
}
},
"hydrogen":
{
"a": 0.02453,
"atomic_mass": 1.674e-27,
"b": 2.651e-5,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 6.36e-24,
"source": "Shelton, D. P., & Rice, J. E. (1994). Measurements and calculations of the hyperpolarizabilities of atoms and small molecules in the gas phase. Chemical Reviews, 94(1), 3-29"
},
"sellmeier":
{
"B":
[
0.0148956,
0.0049037
],
"C":
[
1.807e-10,
9.2e-11
],
"P0": 101325,
"T0": 273.15,
"kind": 2,
"source": "E. R. Peck and S. Hung. Refractivity and dispersion of hydrogen in the visible and near infrared, J. Opt. Soc. Am. 67, 1550-1554 (1977)"
}
},
"krypton":
{
"a": 0.2349,
"atomic_mass": 1.3915e-25,
"atomic_number": 36,
"b": 3.978e-5,
"ionization_energy": 2.2429831039374e-18,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 2.2e-23,
"source": "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
},
"sellmeier":
{
"B":
[
2536370000,
2736490000,
62080200000
],
"C":
[
6.54742e+13,
7.3698e+13,
1.8108e+14
],
"P0": 101325,
"T0": 273.15,
"kind": 2
}
},
"nbk7":
{
"sellmeier":
{
"B":
[
1.03961212,
0.231792344,
1.01046945
],
"C":
[
6.00069867e-15,
2.00179144e-14,
1.03560653e-10
],
"kind": 1,
"reference":
[
"SCHOTT Zemax catalog 2017-01-20b (obtained from http://www.schott.com)"
]
}
},
"neon":
{
"a": 0.02135,
"atomic_mass": 3.35092e-26,
"atomic_number": 10,
"b": 1.709e-5,
"ionization_energy": 3.45501365359425e-18,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 8.7e-25,
"source": "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
},
"sellmeier":
{
"B":
[
1281450000,
22048600000
],
"C":
[
1.84661e+14,
3.7684e+14
],
"P0": 101325,
"T0": 273.15,
"kind": 2
}
},
"nitrogen":
{
"a": 0.137,
"atomic_mass": 2.3259e-26,
"atomic_number": 7,
"b": 1.709e-5,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 2.2e-23,
"source": "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
},
"sellmeier":
{
"B":
[
32431570000
],
"C":
[
1.44e+14
],
"P0": 101325,
"T0": 273.15,
"const": 6.8552e-5,
"kind": 2
}
},
"silica":
{
"sellmeier":
{
"B":
[
0.6961663,
0.4079426,
0.8974794
],
"C":
[
4.67914826e-15,
1.35120631e-14,
9.79340025e-11
],
"kind": 1,
"reference":
[
"I. H. Malitson. Interspecimen comparison of the refractive index of fused silica, J. Opt. Soc. Am. 55, 1205-1208 (1965)",
"C. Z. Tan. Determination of refractive index of silica glass for infrared wavelengths by IR spectroscopy, J. Non-Cryst. Solids 223, 158-163 (1998)"
]
}
},
"vacuum":
{
"a": 0,
"atomic_mass": 0,
"atomic_number": 1,
"b": 0,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 0,
"source": "none"
},
"sellmeier":
{
"B": [],
"C": [],
"P0": 101325,
"T0": 273.15,
"kind": 1
}
},
"xenon":
{
"a": 0.425,
"atomic_mass": 2.18017e-25,
"atomic_number": 54,
"b": 5.105e-5,
"ionization_energy": 1.94342415157935e-18,
"kerr":
{
"P0": 30400,
"T0": 273.15,
"n2": 5.8e-23,
"source": "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
},
"sellmeier":
{
"B":
[
3228690000,
3553930000,
60676400000
],
"C":
[
4.6301e+13,
5.9578e+13,
1.1274e+14
],
"P0": 101325,
"T0": 273.15,
"kind": 2
}
}
}

View File

@@ -1,274 +0,0 @@
[silica.sellmeier]
B = [0.6961663, 0.4079426, 0.8974794]
C = [4.67914826e-15, 1.35120631e-14, 9.79340025e-11]
kind = 1
reference = [
"I. H. Malitson. Interspecimen comparison of the refractive index of fused silica, J. Opt. Soc. Am. 55, 1205-1208 (1965)",
"C. Z. Tan. Determination of refractive index of silica glass for infrared wavelengths by IR spectroscopy, J. Non-Cryst. Solids 223, 158-163 (1998)",
]
[nbk7.sellmeier]
B = [1.03961212, 0.231792344, 1.01046945]
C = [6.00069867e-15, 2.00179144e-14, 1.03560653e-10]
kind = 1
reference = [
"SCHOTT Zemax catalog 2017-01-20b (obtained from http://www.schott.com)",
]
[e7.sellmeier]
B = [0.0, 7.2e-15, 3e-28]
C = []
kind = 3
reference = [
"J. Li, C. H. Wen, S. Gauza, R. Lu and S. T. Wu. Refractive indices of liquid crystals for display applications, J. Disp. Technol. 1, 51-61, 2005",
]
[d-zlaf52la.sellmeier]
B = [
-8.48750283e9,
3.1753525,
3.71301651e-14,
-1.09609062e-27,
2.4418582e-40,
-8.94583294e-54,
]
C = []
kind = 3
reference = ["CDGM Zemax catalog 2017-09 (obtained from http://www.cdgmgd.com)"]
# -----
# GASES
# -----
[air]
a = 0.1358
atomic_mass = 4.809e-26
atomic_number = 7.14 # 78% N2 and 21 O2
b = 3.64e-5
[air.sellmeier]
B = [57921050000.0, 1679170000.0]
C = [238018500000000.0, 57362000000000.0]
P0 = 101325
T0 = 288.15
kind = 2
[air.kerr]
P0 = 101325
T0 = 293.15
n2 = 4.0e-23
source = "Pigeon, J. J., Tochitsky, S. Y., Welch, E. C., & Joshi, C. (2016). Measurements of the nonlinear refractive index of air, N 2, and O 2 at 10 μm using four-wave mixing. Optics letters, 41(17), 3924-3927."
[nitrogen]
a = 0.137
atomic_mass = 2.3259e-26
atomic_number = 7
b = 1.709e-5
[nitrogen.sellmeier]
B = [32431570000.0]
C = [144000000000000.0]
P0 = 101325
T0 = 273.15
const = 6.8552e-5
kind = 2
[nitrogen.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 2.2e-23
source = "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
[helium]
a = 0.00346
atomic_mass = 6.646477e-27
atomic_number = 2
b = 2.38e-5
ionization_energy = 3.9393356074281e-18
[helium.sellmeier]
B = [2.16463842e-5, 2.10561127e-7, 4.7509272e-5]
C = [-6.80769781e-16, 5.13251289e-15, 3.18621354e-15]
P0 = 101325
T0 = 273.15
kind = 1
source = "A. Ermolov, K. F. Mak, M. H. Frosz, J. C. Travers, P. St. J. Russell, Supercontinuum generation in the vacuum ultraviolet through dispersive-wave and soliton-plasma interaction in a noble-gas-filled hollow-core photonic crystal fiber, Phys. Rev. A 92, 033821 (2015)"
[helium.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 3.1e-25
source = "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
[helium_alt]
a = 0.00346
b = 2.38e-5
[helium_alt.sellmeier]
B = [14755297000.0]
C = [426297400000000.0]
P0 = 101325
T0 = 273.15
kind = 2
source = " C. Cuthbertson and M. Cuthbertson. The refraction and dispersion of neon and helium. Proc. R. Soc. London A 135, 40-47 (1936)"
[helium_alt.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 3.1e-25
[hydrogen]
a = 0.02453
atomic_mass = 1.674e-27
b = 2.651e-5
[hydrogen.sellmeier]
B = [0.0148956, 0.0049037]
C = [1.807e-10, 9.2e-11]
P0 = 101325
T0 = 273.15
kind = 2
source = "E. R. Peck and S. Hung. Refractivity and dispersion of hydrogen in the visible and near infrared, J. Opt. Soc. Am. 67, 1550-1554 (1977)"
[hydrogen.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 6.36e-24
source = "Shelton, D. P., & Rice, J. E. (1994). Measurements and calculations of the hyperpolarizabilities of atoms and small molecules in the gas phase. Chemical Reviews, 94(1), 3-29"
[neon]
a = 0.02135
atomic_mass = 3.35092e-26
atomic_number = 10
b = 1.709e-5
ionization_energy = 3.45501365359425e-18
[neon.sellmeier]
B = [1281450000.0, 22048600000.0]
C = [184661000000000.0, 376840000000000.0]
P0 = 101325
T0 = 273.15
kind = 2
[neon.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 8.7e-25
source = "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
[argon]
a = 0.1355
atomic_mass = 6.6338e-26
atomic_number = 18
b = 3.201e-5
ionization_energy = 2.5249661793774e-18
[argon.sellmeier]
B = [2501410000.0, 500283000.0, 52234300000.0]
C = [91012000000000.0, 87892000000000.0, 214020000000000.0]
P0 = 101325
T0 = 273.15
kind = 2
source = "A. Bideau-Mehu, Y. Guern, R. Abjean, A. Johannin-Gilles. Measurement of refractive indices of neon, argon, krypton and xenon in the 253.7-140.4 nm wavelength range. Dispersion relations and estimated oscillator strengths of the resonance lines. J. Quant. Spectrosc. Rad. Transfer 25, 395-402 (1981)"
[argon.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 9.7e-24
source = "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
[argon_alt]
a = 0.1355
b = 3.201e-5
[argon_alt.sellmeier]
B = [0.0002033229, 0.0003445831]
C = [2.0612e-16, 8.066e-15]
P0 = 101325
T0 = 273.15
kind = 1
source = "A. Börzsönyi, Z. Heiner, M. P. Kalashnikov, A. P. Kovács, and K. Osvay, Dispersion measurement of inert gases and gas mixtures at 800 nm, Appl. Opt. 47, 4856-4863 (2008)"
[argon_alt.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 9.7e-24
source = "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
[argon_alt2]
a = 0.1355
b = 3.201e-5
[argon_alt2.sellmeier]
B = [0.030182943]
C = [144000000000000.0]
P0 = 101325
T0 = 273.15
const = 6.7867e-5
kind = 2
source = "E. R. Peck and D. J. Fisher. Dispersion of argon, J. Opt. Soc. Am. 54, 1362-1364 (1964)"
[argon_alt2.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 9.7e-24
source = "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
[krypton]
a = 0.2349
atomic_mass = 1.3915e-25
atomic_number = 36
b = 3.978e-5
ionization_energy = 2.2429831039374e-18
[krypton.sellmeier]
B = [2536370000.0, 2736490000.0, 62080200000.0]
C = [65474200000000.0, 73698000000000.0, 181080000000000.0]
P0 = 101325
T0 = 273.15
kind = 2
[krypton.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 2.2e-23
source = "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
[xenon]
a = 0.425
atomic_mass = 2.18017e-25
atomic_number = 54
b = 5.105e-5
ionization_energy = 1.94342415157935e-18
[xenon.sellmeier]
B = [3228690000.0, 3553930000.0, 60676400000.0]
C = [46301000000000.0, 59578000000000.0, 112740000000000.0]
P0 = 101325
T0 = 273.15
kind = 2
[xenon.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 5.8e-23
source = "Wahlstrand, J. K., Cheng, Y. H., & Milchberg, H. M. (2012). High field optical nonlinearity and the Kramers-Kronig relations. Physical review letters, 109(11), 113904."
[vacuum]
a = 0
atomic_mass = 0
atomic_number = 1
b = 0
[vacuum.sellmeier]
B = []
C = []
P0 = 101325
T0 = 273.15
kind = 1
[vacuum.kerr]
P0 = 30400.0
T0 = 273.15
n2 = 0
source = "none"

View File

@@ -1,69 +0,0 @@
{
"silica" : {
"B" : [0.696166300, 0.407942600, 0.897479400],
"C" : [4.67914826e-15, 1.35120631e-14, 97.9340025e-12],
"kind": 1
},
"air" : {
"B" : [0.05792105e12, 0.00167917e12],
"C" : [238.0185e12, 57.362e12],
"kind": 2,
"P0": 101325,
"T0": 288.15
},
"nitrogen" : {
"B" : [3.243157e10],
"C" : [144e12],
"a" : 0.137,
"b" : 0.01709e-3,
"const": 6.8552e-5,
"kind": 2,
"P0": 101325,
"T0": 273.15
},
"helium" : {
"B" : [0.014755297e12],
"C" : [426.2974e12],
"a" : 0.00346,
"b" : 0.0238e-3,
"kind": 2,
"P0": 101325,
"T0": 273.15
},
"neon" : {
"B" : [0.00128145e12, 0.0220486e12],
"C" : [184.661e12, 376.84e12],
"a" : 0.02135,
"b" : 0.01709e-3,
"kind": 2,
"P0": 101325,
"T0": 273.15
},
"argon" : {
"B" : [2.50141e9, 5.00283e8, 5.22343e10],
"C" : [91.012e12, 87.892e12, 214.02e12],
"a" : 0.1355,
"b" : 0.03201e-3,
"kind": 2,
"P0": 101325,
"T0": 273.15
},
"krypton" : {
"B" : [0.00253637e12, 0.00273649e12, 0.0620802e12],
"C" : [65.4742e12, 73.698e12, 181.08e12],
"a" : 0.2349,
"b" : 0.03978e-3,
"kind": 2,
"P0": 101325,
"T0": 273.15
},
"xenon" : {
"B" : [0.00322869e12, 0.00355393e12, 0.0606764e12],
"C" : [46.301e12, 59.578e12, 112.74e12],
"a" : 0.425,
"b" : 0.05105e-3,
"kind": 2,
"P0": 101325,
"T0": 273.15
}
}

View File

@@ -1,34 +0,0 @@
{
"silica" : {
"B" : [0.696166300, 0.407942600, 0.897479400],
"C" : [4.67914826e-15, 1.35120631e-14, 97.9340025e-12]
},
"air" : {
"B" : [14926.44e-8, 41807.57e-8],
"C" : [19.36e-18, 7.434e-15]
},
"nitrogen" : {
"B" : [39209.95e-8, 18806.48e-8],
"C" : [1146.24e-18, 13.476e-15]
},
"helium" : {
"B" : [4977.77e-8, 1856.94e-8],
"C" : [28.54e-18, 7.760e-15]
},
"neon" : {
"B" : [9154.48e-8, 4018.63e-8],
"C" : [656.97e-18, 5.728e-15]
},
"argon" : {
"B" : [20332.29e-8, 34458.31e-8],
"C" : [206.12e-18, 8.066e-15]
},
"krypton" : {
"B" : [26102.88e-8, 56946.82e-8],
"C" : [2.01e-18, 10.043e-15]
},
"xenon" : {
"B" : [103701.61e-8, 31228.61e-8],
"C" : [12.75e-15, 0.561e-15]
}
}

View File

@@ -1,8 +0,0 @@
{
"sellmeier": {
"B": [0.6961663, 0.4079426, 0.8974794],
"C": [4.67914826e-15, 1.35120631e-14, 9.79340025e-11],
"kind": 1
}
}

View File

@@ -1,29 +0,0 @@
[silica.sellmeier]
B = [0.6961663, 0.4079426, 0.8974794]
C = [4.67914826e-15, 1.35120631e-14, 9.79340025e-11]
kind = 1
reference = [
"I. H. Malitson. Interspecimen comparison of the refractive index of fused silica, J. Opt. Soc. Am. 55, 1205-1208 (1965)",
"C. Z. Tan. Determination of refractive index of silica glass for infrared wavelengths by IR spectroscopy, J. Non-Cryst. Solids 223, 158-163 (1998)",
]
[nbk7.sellmeier]
B = [1.03961212, 0.231792344, 1.01046945]
C = [6.00069867e-15, 2.00179144e-14, 1.03560653e-10]
kind = 1
reference = [
"SCHOTT Zemax catalog 2017-01-20b (obtained from http://www.schott.com)",
]
[d-zlaf52la.sellmeier]
B = [
-8.48750283e9,
3.1753525,
3.71301651e-14,
-1.09609062e-27,
2.4418582e-40,
-8.94583294e-54,
]
C = []
kind = 3
reference = ["CDGM Zemax catalog 2017-09 (obtained from http://www.cdgmgd.com)"]