//************* REACTOR Location ***********
// Originally created by Rehan Deen
// Modified by Satoko Asahi (5-16-2014) asahis@owl.phy.queensu.ca
// Modified by Jeff Lidgard (3-Aug-2015) jeffrey.lidgard@physics.ox.ac.uk
// Modified by Nuno Barros (16-Oct-2016) nfbarros@hep.upenn.edu
// Modified by Nuno Barros (30-Oct-2016) nfbarros@hep.upenn.edu
// Modified by Stefan Nae (22-Feb-2019) stefan@lip.pt
// Modified by Stefan Nae (07-Aug-2019) stefan@lip.pt
// Modified by Stefan Nae (16-Aug-2019) stefan@lip.pt
// Modified by Logan Lebanowski (2019/09/18) - update isotope models [DocDB 6081]
//
// Power in MW, PRIS data
// Coordinates: - for West and South
// Straight line distance in km
// More details on DocDB-2460
//
//********************************************


//================ REACTOR LISTS ================

{
type: "REACTOR_LIST",
version: 1,
index: "ALL",
run_range: [0, 0],
pass: 0,
comment: "All reactors in this file.",
timestamp: "",
active_reactors: [""], // IMPORTANT: The quotes are necessary to know the type if the array
}

{
type: "REACTOR_LIST",
version: 1,
index: "macro",
run_range: [0, 0],
pass: 0,
comment: "Custom entry to be customized using the macro.",
timestamp: "",
active_reactors: [""], // IMPORTANT: The quotes are necessary to know the type if the array
}

{
type: "REACTOR_LIST",
version: 1,
index: "3CAD",
run_range: [0, 0],
pass: 0,
comment: "Closest Canadian reactors",
timestamp: "",
active_reactors: ["BRUCE", "DARLINGTON", "PICKERING"],
}

{
type: "REACTOR_LIST",
version: 1,
index: "testing",
run_range: [0, 0],
pass: 0,
comment: "Testing list of reactors to be simulated",
timestamp: "",
active_reactors: ["BRUCE", "DAYA BAY", "LINGAO", "ALMARAZ"],
}


//================ REACTOR ISOTOPE INFO ================

{
type: "REACTOR_ISOTOPE_INFO",
version: 1,
index: "235U",
run_range: [0, 0],
pass: 0,
comment: "",
timestamp: "",

// Number of neutrinos per fission above 1.8 MeV [PRD 70 (2004) 053011] - out-of-date but unused
n_nu_fission: 1.92,
n_nu_fission_err: 0.037,

// Energy release per fission [Ma et al. PRC 88 014605]
e_per_fission: 202.36,    // MeV
e_per_fission_err: 0.26,  // MeV

spec_type: "polynomial",
// polynomial coefficients to construct the spectrum
//poly_coeff: [3.217, -3.111, 1.395, -0.3690, 0.04445, -0.002053],  // [Mueller et al. PRC 83 054615]
// DEFAULT
poly_coeff: [4.367, -4.577, 2.100, -0.5294, 0.06186, -0.002777],  // [Huber PRC 84 024617]
// these are used only when spec_type is set to "shape"
spec_e: [],
spec_flux: [],
}

{
type: "REACTOR_ISOTOPE_INFO",
version: 1,
index: "238U",
run_range: [0, 0],
pass: 0,
comment: "",
timestamp: "",

// Number of neutrinos per fission above 1.8 MeV [PRD 70 (2004) 053011] - out-of-date but unused
n_nu_fission: 2.38,
n_nu_fission_err: 0.048,

// Energy release per fission [Ma et al. PRC 88 014605]
e_per_fission: 205.99,    // MeV
e_per_fission_err: 0.52,  // MeV

spec_type: "polynomial",
// DEFAULT
poly_coeff: [0.4833, 0.1927, -0.1283, -0.006762, 0.002233, -0.0001536],  // [Mueller et al. PRC 83 054615]
spec_e: [],
spec_flux: [],
}

{
type: "REACTOR_ISOTOPE_INFO",
version: 1,
index: "239Pu",
run_range: [0, 0],
pass: 0,
comment: "",
timestamp: "",

// Number of neutrinos per fission above 1.8 MeV [PRD 70 (2004) 053011] - out-of-date but unused
n_nu_fission: 1.45,
n_nu_fission_err: 0.031,

// Energy release per fission [Ma et al. PRC 88 014605]
e_per_fission: 211.12,    // MeV
e_per_fission_err: 0.34,  // MeV

spec_type: "polynomial",
//poly_coeff: [6.413, -7.432, 3.535, -0.8820, 0.1025, -0.004550],  // [Mueller et al. PRC 83 054615]
// DEFAULT
poly_coeff: [4.757, -5.392, 2.563, -0.6596, 0.07820, -0.003536],  // [Huber PRC 84 024617]
spec_e: [],
spec_flux: [],
}

{
type: "REACTOR_ISOTOPE_INFO",
version: 1,
index: "241Pu",
run_range: [0, 0],
pass: 0,
comment: "",
timestamp: "",

// Number of neutrinos per fission above 1.8 MeV [PRD 70 (2004) 053011] - out-of-date but unused
n_nu_fission: 1.83,
n_nu_fission_err: 0.035,

// Energy release per fission [Ma et al. PRC 88 014605]
e_per_fission: 214.26,    // MeV
e_per_fission_err: 0.33,  // MeV

spec_type: "polynomial",
//poly_coeff: [3.251, -3.204, 1.428, -0.3675, 0.04254, -0.001896],  // [Mueller et al. PRC 83 054615]
// DEFAULT
poly_coeff: [2.990, -2.882, 1.278, -0.3343, 0.03905, -0.001754],  // [Huber PRC 84 024617]
spec_e: [],
spec_flux: [],
}


//================ REACTOR SPECTRUM INFORMATION ================
// The reactor spectra entries can be provided in terms of
// 1. Isotope list and compositions for which the total spectrum will be inferred from the isotope data in REACTOR_ISOTOPE_INFO.
// 2. A precomputed spectrum. In this case, the energy per neutrino must be provided.

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "PHWR",
run_range: [0, 0],
pass: 0,
comment: " Emission Spectra of U235, U238, Pu239, Pu241 from Phys. Rev.C 83, 054615, 2011. NOTE: this is valid only for E_nu > 1.8 MeV (above IBD threshold).",
timestamp: "",
emin: 1.8,
emax: 11.8,
spectrum_type: "parameterized",

// These entries are ignored unless spectrum_type is "shape"

spec_e: [0],
spec_flux: [0],
flux_norm: 0,
param_isotope: ["235U", "238U", "239Pu", "241Pu"],
param_composition: [0.52, 0.05, 0.42, 0.01], // from AECL private communication (2013)
}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "BWR",
run_range: [0, 0],
pass: 0,
comment: "Neutrino spectrum per fission for BWR for 1 MeV production. Scaling factor is 1\/109.818. Normalizes for \/fission\/MeV. [S.Asahi, 3-8-2016]. Mass fractions 0.56, 0.078, 0.295, 0.057, respectively, from KamLAND [Phys. Rev. Lett., 90:021802, Jan 2003] in PWRBWR and thus PWRBWR emit 1. anti-neutrino (with E in [1.8,9.1] MeV) per 109.818 MeV produced",
timestamp: "",
emin: 1.8,
emax: 9,
spectrum_type: "parameterized",
spec_e: [],
spec_flux: [],
flux_norm: 0,
param_isotope: ["235U", "238U", "239Pu", "241Pu"],
param_composition: [0.568, 0.078, 0.297, 0.057],
}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "PWR",
run_range: [0, 0],
pass: 0,
comment: "Essentially identical to BWR (see e.g., [Phys.Rev. D100 (2019) no.5, 052004]: 0.564, 0.076, 0.304, 0.056)",
timestamp: "",
emin: 1.8,
emax: 9,
spectrum_type: "parameterized",
spec_e: [],
spec_flux: [],
flux_norm: 0,
param_isotope: ["235U", "238U", "239Pu", "241Pu"],
param_composition: [0.568, 0.078, 0.297, 0.057],
}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "PWRInit",
run_range: [0, 0],
pass: 0,
comment: "identical to PWR & BWR (for the time being)",
timestamp: "",
emin: 1.8,
emax: 9,
spectrum_type: "parameterized",
spec_e: [],
spec_flux: [],
flux_norm: 0,
param_isotope: ["235U", "238U", "239Pu", "241Pu"],
param_composition: [0.568, 0.078, 0.297, 0.057],
}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "Param_Huber",
run_range: [0, 0],
pass: 0,
comment: "Taken from Huber et al. PRD 70 053011. This serves just as an example on how to use the parameterized spectra.",
timestamp: "",
emin: 1.8,
emax: 9.1,
spectrum_type: "parameterized",
spec_e: [0],
spec_flux: [0],
flux_norm: 0,
param_isotope: ["235U", "238U", "239Pu", "241Pu"],
param_composition: [0.56, 0.08, 0.3, 0.06],
}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "DayaBayComp",
run_range: [0, 0],
pass: 0,
comment: "Daya Bay Paper arXiv:1607.05378 [hep-ph] (19 July 2016).",
timestamp: "",
emin: 1.8,
emax: 12,
spectrum_type: "shape",
// Neutrino spectrum in paper is weighted by the IBD cross-section, here i divided it.
// They prupose we could use it directely, and this is clearly less exact, serves for now to test shapes (integral here gives 1.7632)


spec_e: [1.9625, 2.25, 2.5, 2.75, 3, 3.25, 3.5, 3.75, 4, 4.25, 4.5, 4.75, 5, 5.25, 5.5, 5.75, 6, 6.25, 6.5, 6.75, 7, 7.25, 7.5, 7.75, 8, 10.0625],
spec_flux: [1.24055, 1.0352, 0.853597, 0.707877, 0.574308, 0.476808, 0.385253, 0.311711, 0.249809, 0.196407, 0.151059, 0.115864, 0.0924527, 0.074467, 0.058144, 0.0451798, 0.0338736, 0.0245644, 0.0179723, 0.01301, 0.00885488, 0.0056222, 0.00359866, 0.00231873, 0.00132232, 5.39287e-05],
// (anti-nu/Mev)/fission
// average energy per fission is 205.99 (this gives 1.76/205.99 = 116.83 antinu/MeV release at reactor (to be comparable

flux_norm: 205.99,

// Since the type is shape, these options are ignored - are kept here just for reference, from the same paper

param_isotope: ["235U", "238U", "239Pu", "241Pu"],
param_composition: [0.561, 0.076, 0.307, 0.056],

// energies/fission: 202.36,205.99,211.12,214.26
// w/ uncertainty :  0.26, 0.52, 0.34, 0.33

}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "dummy",
run_range: [0, 0],
pass: 0,
comment: "THis spectrum has an unknown normalization and therefore should probably not be used. Serves as an example of how to use the type \"shape\".",
timestamp: "",
emin: 1.85,
emax: 8.15,
spectrum_type: "shape",
spec_e: [1.85, 2.15, 2.45, 2.75, 3.05, 3.35, 3.65, 3.95, 4.25, 4.55, 4.85, 5.15, 5.45, 5.75, 6.05, 6.35, 6.65, 6.95, 7.25, 7.55, 7.85, 8.15],
spec_flux: [49.8, 39.66, 31.43, 24.79, 19.45, 15.19, 11.8, 9.12, 7.01, 5.35, 4.06, 3.06, 2.28, 1.67, 1.21, 0.85, 0.58, 0.38, 0.23, 0.13, 0.06, 0.03],
flux_norm: 1,
param_isotope: [],
param_composition: [],
}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "DayaBayMeas",
run_range: [0, 0],
pass: 0,
comment: "Daya Bay Paper arXiv:1607.05378 [hep-ph] (19 July 2016).",
timestamp: "",
emin: 1.8,
emax: 12,
spectrum_type: "shape",

// Neutrino spectrum in paper is weighted by the IBD cross-section, here i divided it.
// They prupose we could use it directely, and this is clearly less exact, serves for now to test shapes (integral here gives 1.7632)

spec_e: [1.9625, 2.25, 2.5, 2.75, 3, 3.25, 3.5, 3.75, 4, 4.25, 4.5, 4.75, 5, 5.25, 5.5, 5.75, 6, 6.25, 6.5, 6.75, 7, 7.25, 7.5, 7.75, 8, 10.0625],
spec_flux: [1.24055, 1.0352, 0.853597, 0.707877, 0.574308, 0.476808, 0.385253, 0.311711, 0.249809, 0.196407, 0.151059, 0.115864, 0.0924527, 0.074467, 0.058144, 0.0451798, 0.0338736, 0.0245644, 0.0179723, 0.01301, 0.00885488, 0.0056222, 0.00359866, 0.00231873, 0.00132232, 5.39287e-05],
// (anti-nu/Mev)/fission
// average energy per fission is 205.99 (this gives 1.76/205.99 = 116.83 antinu/MeV release at reactor (to be comparable with Satoko's norms)

flux_norm: 205.99,
// Since the type is shape, these options are ignored - are kept here just for reference, from the same paper

param_isotope: ["235U", "238U", "239Pu", "241Pu"],
param_composition: [0.561, 0.076, 0.307, 0.056],
// energies/fission: 202.36,205.99,211.12,214.26
// w/ uncertainty :  0.26, 0.52, 0.34, 0.33
}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "PHWR_Satoko",
run_range: [0, 0],
pass: 0,
comment: " Emission Spectra of U235, U238, Pu239, Pu241 from Phys. Rev.C 83, 054615, 2011. NOTE: this is valid only for E_nu > 1.8 MeV (above IBD threshold). Neutrino spectrum per fission for CANDU for 1 MeV production., normalized for \/fission\/MeV. Mass fractions 0.52, 0.05, 0.42, 0.01, respectively from AECL in PHWR (CANDU). Average energy release\/fission is 205.653 MeV and average number of anti neutrinos (with E in [1.8,9.1] MeV) is 1.80479. Thus PHWR\/CANDU emit 1 anti-neutrino (with E in [1.8,9.1] MeV) per 113.95 MeV produced",
timestamp: "",
emin: 1.8,
emax: 9,
spectrum_type: "shape",
spec_e: [1.90286, 2.10857, 2.31429, 2.52, 2.72571, 2.93143, 3.13714, 3.34286, 3.54857, 3.75429, 3.96, 4.16571, 4.37143, 4.57714, 4.78286, 4.98857, 5.19429, 5.4, 5.60571, 5.81143, 6.01714, 6.22286, 6.42857, 6.63429, 6.84, 7.04571, 7.25143, 7.45714, 7.66286, 7.86857, 8.07429, 8.28, 8.48571, 8.69143, 8.89714, 9.10286],
spec_flux: [0.743248, 0.633057, 0.545363, 0.472005, 0.408358, 0.35186, 0.30118, 0.255694, 0.215136, 0.179374, 0.148268, 0.121598, 0.099051, 0.0802325, 0.0646986, 0.0519906, 0.0416644, 0.033311, 0.026569, 0.021129, 0.0167332, 0.0131714, 0.0102762, 0.00791703, 0.00599419, 0.00443367, 0.00318126, 0.00219659, 0.001447, 0.000901705, 0.000527747, 0.000288981, 0.000148371, 7.22756e-05, 3.423e-05, 0],
flux_norm: 113.95,
param_isotope: [],
param_composition: [],
}

{
type: "REACTOR_SPECTRUM",
version: 1,
index: "PWRBWR_Satoko",
run_range: [0, 0],
pass: 0,
comment: "Neutrino spectrum per fission for PWR\/BWR for 1 MeV production. Mass fractions 0.568, 0.078, 0.297, 0.057, respectively, from KamLAND (2003). Average energy release \/ fission is 205.213, average number of anti-neutrinos (w\/ E in [1.8,9.] MeV) is 1.871. So, 109.807 MeV released per antineutrino emmitted in IBD range",
timestamp: "",
emin: 1.8,
emax: 9,
spectrum_type: "shape",
spec_e: [1.90286, 2.10857, 2.31429, 2.52, 2.72571, 2.93143, 3.13714, 3.34286, 3.54857, 3.75429, 3.96, 4.16571, 4.37143, 4.57714, 4.78286, 4.98857, 5.19429, 5.4, 5.60571, 5.81143, 6.01714, 6.22286, 6.42857, 6.63429, 6.84, 7.04571, 7.25143, 7.45714, 7.66286, 7.86857, 8.07429, 8.28, 8.48571, 8.69143, 8.89714, 9.10286],
spec_flux: [0.72615, 0.62378, 0.540617, 0.469957, 0.407983, 0.352586, 0.302678, 0.257754, 0.2176, 0.182101, 0.151124, 0.124459, 0.10181, 0.0828051, 0.0670255, 0.0540385, 0.0434221, 0.0347852, 0.0277793, 0.0221028, 0.0175023, 0.0137688, 0.0107338, 0.0082644, 0.00625727, 0.0046341, 0.00333593, 0.00231765, 0.00154229, 0.000975868, 0.000583656, 0.00032908, 0.000175456, 8.95153e-05, 4.46835e-05, 0],
flux_norm: 109.683,
param_isotope: [],
param_composition: [],
}


//================ INDIVIDUAL REACTOR CORE LOCATIONS ================

{
type: "REACTOR",
version: 1,
index: "ALMARAZ",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [39.8074, 39.8074],
longitude: [-5.69769, -5.69669],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "ANGRA",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [-23.008, -23.0065],
longitude: [-44.4567, -44.4578],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "ANO",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [35.3103, 35.3103],
longitude: [-93.2296, -93.2286],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "ARMENIAN",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 1,
latitude: [40.1813],
longitude: [44.1472],
altitude: [0],
}

{
type: "REACTOR",
version: 1,
index: "ASCO",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [41.2016, 41.2016],
longitude: [0.57136, 0.57236],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "ATUCHA",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [-33.9669, -33.96752],
longitude: [-59.2086, -59.20512],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BALAKOVO",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 4,
latitude: [52.0915, 52.0921, 52.0927, 52.0932],
longitude: [47.9519, 47.9536, 47.9558, 47.9579],
altitude: [0, 0, 0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BEAVER VALLEY",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [40.6238, 40.6238],
longitude: [-80.4319, -80.4309],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BELLEVILLE",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [47.5105, 47.51],
longitude: [2.87116, 2.87123],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BELOYARSK",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [56.8415, 56.8415],
longitude: [61.3188, 61.3188],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BEZNAU",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [47.552, 47.552],
longitude: [8.22946, 8.23046],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BILIBINO",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 4,
latitude: [68.0586, 68.0586, 68.0586, 68.0586],
longitude: [166.492, 166.493, 166.494, 166.495],
altitude: [0, 0, 0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BLAYAIS",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 4,
latitude: [45.2562, 45.2561, 45.2561, 45.2561],
longitude: [-0.69129, -0.69077, -0.69033, -0.68988],
altitude: [0, 0, 0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BOHUNICE",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [48.4921, 48.4916],
longitude: [17.6869, 17.6869],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BORSSELE",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 1,
latitude: [51.4311],
longitude: [3.71867],
altitude: [0],
}

{
type: "REACTOR",
version: 1,
index: "BRAIDWOOD",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [41.247, 41.247],
longitude: [-88.2296, -88.2288],
altitude: [0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BROKDORF",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 1,
latitude: [53.85],
longitude: [9.34455],
altitude: [0],
}

{
type: "REACTOR",
version: 1,
index: "BROWNS FERRY",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 3,
latitude: [34.7038, 34.7033, 34.7028],
longitude: [-87.119, -87.119, -87.119],
altitude: [0, 0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BRUCE",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 8,
latitude: [44.3411, 44.3411, 44.3411, 44.3416, 44.3198, 44.3193, 44.3188, 44.3183],
longitude: [-81.5716, -81.5716, -81.5716, -81.5716, -81.588, -81.588, -81.588, -81.588],
altitude: [0, 0, 0, 0, 0, 0, 0, 0],
}

{
type: "REACTOR",
version: 1,
index: "BRUNSWICK",
run_range: [0,0],
pass: 0,
comment: "",
timestamp: "",
no_cores: 2,
latitude: [33.9579, 33.9574],
longitude: [-78.0071, -78.0071],
altitude: [0, 0],
}

{
type: "REACTOR",
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