From 85def34700545cef8b945718320a0c80a841bd52 Mon Sep 17 00:00:00 2001 From: Federico Grimaldi Date: Wed, 28 Aug 2024 13:23:41 +0200 Subject: [PATCH 1/4] test push --- sandy/core/endf6.py | 1 + sandy/pfns.py | 3 +++ 2 files changed, 4 insertions(+) diff --git a/sandy/core/endf6.py b/sandy/core/endf6.py index c04f39e0..60167dc1 100644 --- a/sandy/core/endf6.py +++ b/sandy/core/endf6.py @@ -2582,6 +2582,7 @@ def apply_perturbations_xs(self, smps, processes=1, pendf=None, njoy_kws={}, **k data["pnu"] = smps[31].iterate_xs_samples() if 33 in smps: data["pxs"] = smps[33].iterate_xs_samples() + # this I'd like to change if processes == 1: outs = {} diff --git a/sandy/pfns.py b/sandy/pfns.py index 5b85195b..721cb343 100644 --- a/sandy/pfns.py +++ b/sandy/pfns.py @@ -527,3 +527,6 @@ def from_endf6(cls, endf6): if not data: raise sandy.Error("no tabulated energy distribution was found") return cls(data) + + def to_endf6(self): + pass From 0f7c18eec873d0b86b186031390cbf6030c825c2 Mon Sep 17 00:00:00 2001 From: Federico Grimaldi Date: Wed, 28 Aug 2024 13:25:26 +0200 Subject: [PATCH 2/4] No PFNS changes --- sandy/pfns.py | 3 --- 1 file changed, 3 deletions(-) diff --git a/sandy/pfns.py b/sandy/pfns.py index 721cb343..5b85195b 100644 --- a/sandy/pfns.py +++ b/sandy/pfns.py @@ -527,6 +527,3 @@ def from_endf6(cls, endf6): if not data: raise sandy.Error("no tabulated energy distribution was found") return cls(data) - - def to_endf6(self): - pass From ac4d3dbef0ca9a0ded8a6c267c088abb317a3ac1 Mon Sep 17 00:00:00 2001 From: Federico Grimaldi Date: Thu, 29 Aug 2024 16:26:57 +0200 Subject: [PATCH 3/4] get perturbations MF 35 --- sandy/core/endf6.py | 15 +- sandy/njoy_outputs/input | 11 + sandy/njoy_outputs/tape20 | 673 ++++++++++++++++++++++++++++++++++++++ 3 files changed, 698 insertions(+), 1 deletion(-) create mode 100644 sandy/njoy_outputs/input create mode 100644 sandy/njoy_outputs/tape20 diff --git a/sandy/core/endf6.py b/sandy/core/endf6.py index a904a271..99cd3cc6 100644 --- a/sandy/core/endf6.py +++ b/sandy/core/endf6.py @@ -2279,12 +2279,19 @@ def get_perturbations_xs(self, nsmp, njoy_kws={}, smp_kws={}, **kwargs,): >>> assert len(smps) == 1 >>> assert isinstance(smps[33], sandy.Samples) >>> assert (smps[33].data.index.get_level_values("MT") == 102).all() + + Test get perturbations from MF 35 + >>> njoy_kws = dict(err=1, errorr_kws=dict(mt=18)) + >>> tape = sandy.get_endf6_file("jeff_33", "xs", 922350) + >>> smps = tape.get_perturbations(nsmp=2, njoy_kws=njoy_kws) + >>> assert len(smps) == 3 + >>> assert isinstance(smps[35], sandy.Samples) + >>> assert (smps[35].data.index.get_level_values("MT") == 18).all() """ smp = {} # -- produce ERRORR files with covariance data njoy_kws["mubar"] = False - njoy_kws["chi"] = False outs = self.get_errorr(**njoy_kws) filename = "PERT_{}_MF{}.xlsx" filenamecov = "COV_{}_MF{}.tape" @@ -2301,6 +2308,12 @@ def get_perturbations_xs(self, nsmp, njoy_kws={}, smp_kws={}, **kwargs,): xls = filename.format(self.get_id(), 33) smp[33] = outs["errorr33"].get_cov().sampling(nsmp, to_excel=xls, seed=smp_kws.get("seed33"), **smp_kws) + # -- Extract samples from MF35 covariance data + if "errorr35" in outs: + outs["errorr35"].to_file(filenamecov.format(self.get_id(), 35)) + xls = filename.format(self.get_id(), 35) + smp[35] = outs["errorr35"].get_cov().sampling(nsmp, to_excel=xls, seed=smp_kws.get("seed35"), **smp_kws) + return smp def get_perturbations_rdd(self, nsmp, smp_hl_kws={}, smp_de_kws={}, smp_br_kws={}, fill_zeros=0.05, **kwargs,): diff --git a/sandy/njoy_outputs/input b/sandy/njoy_outputs/input new file mode 100644 index 00000000..2251f8eb --- /dev/null +++ b/sandy/njoy_outputs/input @@ -0,0 +1,11 @@ +moder +20 -21 / +reconr +-21 -22 / +'sandy runs njoy'/ +125 0 0 / +1.0 0. / +0/ +moder +-22 30 / +stop \ No newline at end of file diff --git a/sandy/njoy_outputs/tape20 b/sandy/njoy_outputs/tape20 new file mode 100644 index 00000000..8caf910b --- /dev/null +++ b/sandy/njoy_outputs/tape20 @@ -0,0 +1,673 @@ + 1 0 0 0 + 1.001000+3 9.991673-1 0 0 2 5 125 1451 1 + 0.000000+0 0.000000+0 0 0 0 6 125 1451 2 + 1.000000+0 2.000000+7 3 0 10 3 125 1451 3 + 0.000000+0 0.000000+0 0 0 87 10 125 1451 4 + 1-H - 1 LANL EVAL-OCT05 G.M.Hale 125 1451 5 + DIST-DEC17 REV3-DEC17 20171231 125 1451 6 +---JEFF-3.3 MATERIAL 125 125 1451 7 +-----INCIDENT NEUTRON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 + 125 1451 10 + **************************************************************** 125 1451 11 +The new R-matrix analysis of the N-N system on which the ENDF/B- 125 1451 12 +VII evaluation for 1H is based differs from the previous one use 125 1451 13 +for ENDF/B-VI in several respects. Firstly, the n-p capture 125 1451 14 +reaction (MT=102), and its inverse, deuteron photo- 125 1451 15 +disintegration, were a part of the analysis, rather than added 125 1451 16 +later as before. The analysis used a new method for including 125 1451 17 +photon channels in R-matrix theory [1], which gave a better 125 1451 18 +description of the E1 transitions, in particular. The data for 125 1451 19 +these reactions are mostly integrated and differential cross 125 1451 20 +sections, but some information about polarizations was also 125 1451 21 +included. The thermal capture cross section was taken to be 125 1451 22 +332.0 mb, as was the recommendation from preliminary data 125 1451 23 +testing. Good agreement was obtained with recent cross-section 125 1451 24 +measurements [2,3] by astrophysical groups in the 20-550 keV 125 1451 25 +range, as well as with earlier measurements that had been done 125 1451 26 +mostly as photo-disintegration experiments at energies below 14 125 1451 27 +MeV. 125 1451 28 +The new analysis includes several additional measurements of the 125 1451 29 +total cross section (MT=1). The evaluated cross section 125 1451 30 +deviates at most by about -0.5% around 10 MeV from that of 125 1451 31 +ENDF/B-VI. The estimated uncertainty of the MT=1 cross section 125 1451 32 +is given at 2 MeV steps in the following table: 125 1451 33 + En Uncert. (%) 125 1451 34 + 0 0.20 125 1451 35 + 2 0.22 125 1451 36 + 4 0.30 125 1451 37 + 6 0.36 125 1451 38 + 8 0.44 125 1451 39 + 10 0.50 125 1451 40 + 12 0.49 125 1451 41 + 14 0.46 125 1451 42 + 16 0.40 125 1451 43 + 18 0.35 125 1451 44 + 20 0.30 125 1451 45 + 125 1451 46 +For n-p scattering (MT=2), new information was included about the 125 1451 47 +low-energy cross sections (MF=3) and about the angular 125 1451 48 +distributions (MF=4). A new measurement of the angular 125 1451 49 +distribution at 10 MeV [4], plus corrections to earlier data at 125 1451 50 +14 MeV, moved the back-angle asymmetry in the 10-14 MeV range to 125 1451 51 +values that lie between those obtained for ENDF/B-V and ENDF/B- 125 1451 52 +VI. The addition of the latest value of the thermal coherent 125 1451 53 +scattering length [5] had the interesting effect of reducing the 125 1451 54 +"zero-energy" scattering cross section somewhat to agree 125 1451 55 +perfectly with an earlier measurement by Houk [6], and disagree 125 1451 56 +with the later, more precise, value of Dilg [7]. The 125 1451 57 +covariances for MT=2 will be added later, but the uncertainties 125 1451 58 +on the integrated cross section should be similar to those 125 1451 59 +listed above for the total cross section. 125 1451 60 + 125 1451 61 +REFERENCES 125 1451 62 + 125 1451 63 +[1] G. M. Hale and A. S. Johnson, Proc. 17th Int. IUPAP Conf. on 125 1451 64 + Few-Body Problems in Physics, 5-10 June 2003, Durham NC, W. 125 1451 65 + Gloeckle and W. Tornow, eds., Elsevier B.V., pp. S120-S122 125 1451 66 + (2004). 125 1451 67 +[2] T. S. Suzuki et al., Astrophys. Lett. 449, L59 (1995). 125 1451 68 +[3] Y. Nagai et al., Phys. Rev. C 56, 3173 (1997). 125 1451 69 +[4] N. Boukharouba et al., Phys. Rev. C 65, 014004 (2002). 125 1451 70 +[5] K. Schoen et al., Phys. Rev. C 67, 044005 (2003). 125 1451 71 +[6] T. L. Houk, Phys. Rev. C 3, 1886 (1971). 125 1451 72 +[7] W. Dilg, Phys. Rev. C 11, 103 (1975). 125 1451 73 + **************************************************************** 125 1451 74 + 125 1451 75 +Covariances were adopted from COMMARA-2.0 library in July 2011. 125 1451 76 +These covariances were obtained at LANL by full scale R-matrix 125 1451 77 +analysis of more than 5000 experimental data (chi-square/degree 125 1451 78 +of freedom of 0.83). [1] The major channel in this case is elastic 125 1451 79 +scattering, often labeled also as ''n-p'' scattering. Elastic 125 1451 80 +scattering serves as neutron cross section standard from 1 keV to 125 1451 81 +20 MeV, with cross sections well determined. Uncertainties for 125 1451 82 +elastic scattering rise from values well below 1%, reach maximum 125 1451 83 +at about 8 MeV, then gradually decrease with increasing energy. 125 1451 84 +In addition to elastic scattering, covariances are supplied for 125 1451 85 +radiative capture. 125 1451 86 + 125 1451 87 +REFERENCES 125 1451 88 +[1] G. M. Hale, "Covariances from light-element R-matrix 125 1451 89 +analyses," Nuclear Data Sheets, 109, 2812 (2008). 125 1451 90 + **************************************************************** 125 1451 91 + 1 451 101 5 125 1451 92 + 2 151 4 0 125 1451 93 + 3 1 35 4 125 1451 94 + 3 2 35 4 125 1451 95 + 3 102 35 5 125 1451 96 + 4 2 196 4 125 1451 97 + 6 102 201 4 125 1451 98 + 33 1 5 5 125 1451 99 + 33 2 21 5 125 1451 100 + 33 102 21 5 125 1451 101 + 125 1 099999 + 125 0 0 0 + 1.001000+3 9.991673-1 0 0 1 0 125 2151 1 + 1.001000+3 1.000000+0 0 0 1 0 125 2151 2 + 1.000000-5 1.000000+5 0 0 0 0 125 2151 3 + 5.000000-1 1.276553+0 0 0 0 0 125 2151 4 + 125 2 099999 + 125 0 0 0 + 1.001000+3 9.991673-1 0 0 0 0 125 3 1 1 + 0.000000+0 0.000000+0 0 0 2 96 125 3 1 2 + 30 5 96 2 125 3 1 3 + 1.000000-5 3.713628+1 2.000000-5 3.224498+1 5.000000-5 2.790478+1 125 3 1 4 + 1.000000-4 2.571732+1 2.000000-4 2.417056+1 5.000000-4 2.279806+1 125 3 1 5 + 1.000000-3 2.210633+1 2.000000-3 2.161720+1 5.000000-3 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3.120757-2 12533102 18 + 4.583375-2 3.902245-2 3.376506-2 2.962370-2 2.626567-2 3.328758-2 12533102 19 + 2.886709-2 2.539081-2 2.257507-2 2.510044-2 2.214385-2 1.975366-2 12533102 20 + 1.960192-2 1.755105-2 1.577899-2 12533102 21 + 12533 099999 + 125 0 0 0 + 0 0 0 0 + -1 0 0 0 \ No newline at end of file From ccc052a00fcda661869e8d9547245f4aa8772093 Mon Sep 17 00:00:00 2001 From: Federico Grimaldi Date: Thu, 29 Aug 2024 16:45:25 +0200 Subject: [PATCH 4/4] remove njoy_outputs/ --- sandy/njoy_outputs/input | 11 - sandy/njoy_outputs/tape20 | 673 -------------------------------------- 2 files changed, 684 deletions(-) delete mode 100644 sandy/njoy_outputs/input delete mode 100644 sandy/njoy_outputs/tape20 diff --git a/sandy/njoy_outputs/input b/sandy/njoy_outputs/input deleted file mode 100644 index 2251f8eb..00000000 --- a/sandy/njoy_outputs/input +++ /dev/null @@ -1,11 +0,0 @@ -moder -20 -21 / -reconr --21 -22 / -'sandy runs njoy'/ -125 0 0 / -1.0 0. / -0/ -moder --22 30 / -stop \ No newline at end of file diff --git a/sandy/njoy_outputs/tape20 b/sandy/njoy_outputs/tape20 deleted file mode 100644 index 8caf910b..00000000 --- a/sandy/njoy_outputs/tape20 +++ /dev/null @@ -1,673 +0,0 @@ - 1 0 0 0 - 1.001000+3 9.991673-1 0 0 2 5 125 1451 1 - 0.000000+0 0.000000+0 0 0 0 6 125 1451 2 - 1.000000+0 2.000000+7 3 0 10 3 125 1451 3 - 0.000000+0 0.000000+0 0 0 87 10 125 1451 4 - 1-H - 1 LANL EVAL-OCT05 G.M.Hale 125 1451 5 - DIST-DEC17 REV3-DEC17 20171231 125 1451 6 ----JEFF-3.3 MATERIAL 125 125 1451 7 ------INCIDENT NEUTRON DATA 125 1451 8 -------ENDF-6 FORMAT 125 1451 9 - 125 1451 10 - **************************************************************** 125 1451 11 -The new R-matrix analysis of the N-N system on which the ENDF/B- 125 1451 12 -VII evaluation for 1H is based differs from the previous one use 125 1451 13 -for ENDF/B-VI in several respects. Firstly, the n-p capture 125 1451 14 -reaction (MT=102), and its inverse, deuteron photo- 125 1451 15 -disintegration, were a part of the analysis, rather than added 125 1451 16 -later as before. The analysis used a new method for including 125 1451 17 -photon channels in R-matrix theory [1], which gave a better 125 1451 18 -description of the E1 transitions, in particular. The data for 125 1451 19 -these reactions are mostly integrated and differential cross 125 1451 20 -sections, but some information about polarizations was also 125 1451 21 -included. The thermal capture cross section was taken to be 125 1451 22 -332.0 mb, as was the recommendation from preliminary data 125 1451 23 -testing. Good agreement was obtained with recent cross-section 125 1451 24 -measurements [2,3] by astrophysical groups in the 20-550 keV 125 1451 25 -range, as well as with earlier measurements that had been done 125 1451 26 -mostly as photo-disintegration experiments at energies below 14 125 1451 27 -MeV. 125 1451 28 -The new analysis includes several additional measurements of the 125 1451 29 -total cross section (MT=1). The evaluated cross section 125 1451 30 -deviates at most by about -0.5% around 10 MeV from that of 125 1451 31 -ENDF/B-VI. The estimated uncertainty of the MT=1 cross section 125 1451 32 -is given at 2 MeV steps in the following table: 125 1451 33 - En Uncert. (%) 125 1451 34 - 0 0.20 125 1451 35 - 2 0.22 125 1451 36 - 4 0.30 125 1451 37 - 6 0.36 125 1451 38 - 8 0.44 125 1451 39 - 10 0.50 125 1451 40 - 12 0.49 125 1451 41 - 14 0.46 125 1451 42 - 16 0.40 125 1451 43 - 18 0.35 125 1451 44 - 20 0.30 125 1451 45 - 125 1451 46 -For n-p scattering (MT=2), new information was included about the 125 1451 47 -low-energy cross sections (MF=3) and about the angular 125 1451 48 -distributions (MF=4). A new measurement of the angular 125 1451 49 -distribution at 10 MeV [4], plus corrections to earlier data at 125 1451 50 -14 MeV, moved the back-angle asymmetry in the 10-14 MeV range to 125 1451 51 -values that lie between those obtained for ENDF/B-V and ENDF/B- 125 1451 52 -VI. The addition of the latest value of the thermal coherent 125 1451 53 -scattering length [5] had the interesting effect of reducing the 125 1451 54 -"zero-energy" scattering cross section somewhat to agree 125 1451 55 -perfectly with an earlier measurement by Houk [6], and disagree 125 1451 56 -with the later, more precise, value of Dilg [7]. The 125 1451 57 -covariances for MT=2 will be added later, but the uncertainties 125 1451 58 -on the integrated cross section should be similar to those 125 1451 59 -listed above for the total cross section. 125 1451 60 - 125 1451 61 -REFERENCES 125 1451 62 - 125 1451 63 -[1] G. M. Hale and A. S. Johnson, Proc. 17th Int. IUPAP Conf. on 125 1451 64 - Few-Body Problems in Physics, 5-10 June 2003, Durham NC, W. 125 1451 65 - Gloeckle and W. Tornow, eds., Elsevier B.V., pp. S120-S122 125 1451 66 - (2004). 125 1451 67 -[2] T. S. Suzuki et al., Astrophys. Lett. 449, L59 (1995). 125 1451 68 -[3] Y. Nagai et al., Phys. Rev. C 56, 3173 (1997). 125 1451 69 -[4] N. Boukharouba et al., Phys. Rev. C 65, 014004 (2002). 125 1451 70 -[5] K. Schoen et al., Phys. Rev. C 67, 044005 (2003). 125 1451 71 -[6] T. L. Houk, Phys. Rev. C 3, 1886 (1971). 125 1451 72 -[7] W. Dilg, Phys. Rev. C 11, 103 (1975). 125 1451 73 - **************************************************************** 125 1451 74 - 125 1451 75 -Covariances were adopted from COMMARA-2.0 library in July 2011. 125 1451 76 -These covariances were obtained at LANL by full scale R-matrix 125 1451 77 -analysis of more than 5000 experimental data (chi-square/degree 125 1451 78 -of freedom of 0.83). [1] The major channel in this case is elastic 125 1451 79 -scattering, often labeled also as ''n-p'' scattering. Elastic 125 1451 80 -scattering serves as neutron cross section standard from 1 keV to 125 1451 81 -20 MeV, with cross sections well determined. Uncertainties for 125 1451 82 -elastic scattering rise from values well below 1%, reach maximum 125 1451 83 -at about 8 MeV, then gradually decrease with increasing energy. 125 1451 84 -In addition to elastic scattering, covariances are supplied for 125 1451 85 -radiative capture. 125 1451 86 - 125 1451 87 -REFERENCES 125 1451 88 -[1] G. M. Hale, "Covariances from light-element R-matrix 125 1451 89 -analyses," Nuclear Data Sheets, 109, 2812 (2008). 125 1451 90 - **************************************************************** 125 1451 91 - 1 451 101 5 125 1451 92 - 2 151 4 0 125 1451 93 - 3 1 35 4 125 1451 94 - 3 2 35 4 125 1451 95 - 3 102 35 5 125 1451 96 - 4 2 196 4 125 1451 97 - 6 102 201 4 125 1451 98 - 33 1 5 5 125 1451 99 - 33 2 21 5 125 1451 100 - 33 102 21 5 125 1451 101 - 125 1 099999 - 125 0 0 0 - 1.001000+3 9.991673-1 0 0 1 0 125 2151 1 - 1.001000+3 1.000000+0 0 0 1 0 125 2151 2 - 1.000000-5 1.000000+5 0 0 0 0 125 2151 3 - 5.000000-1 1.276553+0 0 0 0 0 125 2151 4 - 125 2 099999 - 125 0 0 0 - 1.001000+3 9.991673-1 0 0 0 0 125 3 1 1 - 0.000000+0 0.000000+0 0 0 2 96 125 3 1 2 - 30 5 96 2 125 3 1 3 - 1.000000-5 3.713628+1 2.000000-5 3.224498+1 5.000000-5 2.790478+1 125 3 1 4 - 1.000000-4 2.571732+1 2.000000-4 2.417056+1 5.000000-4 2.279806+1 125 3 1 5 - 1.000000-3 2.210633+1 2.000000-3 2.161720+1 5.000000-3 2.118318+1 125 3 1 6 - 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5.500000+6 1.513553+0 6.000000+6 1.418157+0 6.500000+6 1.333709+0 125 3 2 26 - 7.000000+6 1.258367+0 7.500000+6 1.190697+0 8.000000+6 1.129564+0 125 3 2 27 - 8.500000+6 1.074052+0 9.000000+6 1.023415+0 9.500000+6 9.770347-1 125 3 2 28 - 1.000000+7 9.343974-1 1.050000+7 8.950685-1 1.100000+7 8.586796-1 125 3 2 29 - 1.150000+7 8.249154-1 1.200000+7 7.935044-1 1.250000+7 7.642113-1 125 3 2 30 - 1.300000+7 7.368313-1 1.350000+7 7.111848-1 1.400000+7 6.871141-1 125 3 2 31 - 1.450000+7 6.644799-1 1.500000+7 6.431586-1 1.550000+7 6.230401-1 125 3 2 32 - 1.600000+7 6.040262-1 1.650000+7 5.860290-1 1.700000+7 5.689692-1 125 3 2 33 - 1.750000+7 5.527757-1 1.800000+7 5.373840-1 1.850000+7 5.227359-1 125 3 2 34 - 1.900000+7 5.087783-1 1.950000+7 4.954630-1 2.000000+7 4.827462-1 125 3 2 35 - 125 3 099999 - 1.001000+3 9.991673-1 0 0 0 0 125 3102 1 - 2.224631+6 2.224631+6 0 0 2 96 125 3102 2 - 30 5 96 2 125 3102 3 - 1.000000-5 1.669994+1 2.000000-5 1.180864+1 5.000000-5 7.468441+0 125 3102 4 - 1.000000-4 5.280985+0 2.000000-4 3.734221+0 5.000000-4 2.361728+0 125 3102 5 - 1.000000-3 1.669994+0 2.000000-3 1.180864+0 5.000000-3 7.468441-1 125 3102 6 - 1.000000-2 5.280985-1 2.530000-2 3.320126-1 5.000000-2 2.361728-1 125 3102 7 - 1.000000-1 1.669993-1 2.000000-1 1.180863-1 5.000000-1 7.468415-2 125 3102 8 - 1.000000+0 5.280948-2 2.000000+0 3.734168-2 5.000000+0 2.361645-2 125 3102 9 - 1.000000+1 1.669877-2 2.000000+1 1.180698-2 5.000000+1 7.465816-3 125 3102 10 - 1.000000+2 5.277275-3 2.000000+2 3.728978-3 5.000000+2 2.353460-3 125 3102 11 - 1.000000+3 1.658348-3 2.000000+3 1.164526-3 4.000000+3 8.122556-4 125 3102 12 - 6.000000+3 6.543522-4 8.000000+3 5.592552-4 1.000000+4 4.937688-4 125 3102 13 - 1.500000+4 3.906824-4 2.000000+4 3.283054-4 4.000000+4 2.082663-4 125 3102 14 - 6.000000+4 1.550608-4 8.000000+4 1.241126-4 1.000000+5 1.037740-4 125 3102 15 - 1.500000+5 7.450778-5 2.000000+5 5.927795-5 3.000000+5 4.460357-5 125 3102 16 - 4.000000+5 3.827476-5 5.000000+5 3.529043-5 6.000000+5 3.389904-5 125 3102 17 - 7.000000+5 3.334204-5 8.000000+5 3.324413-5 9.000000+5 3.340211-5 125 3102 18 - 1.000000+6 3.369898-5 1.200000+6 3.445546-5 1.400000+6 3.521705-5 125 3102 19 - 1.600000+6 3.587303-5 1.800000+6 3.638957-5 2.000000+6 3.676631-5 125 3102 20 - 2.200000+6 3.701693-5 2.400000+6 3.715993-5 2.600000+6 3.721435-5 125 3102 21 - 2.800000+6 3.719773-5 3.000000+6 3.712539-5 3.200000+6 3.701023-5 125 3102 22 - 3.400000+6 3.686289-5 3.600000+6 3.669203-5 3.800000+6 3.650457-5 125 3102 23 - 4.000000+6 3.630600-5 4.200000+6 3.610063-5 4.400000+6 3.589183-5 125 3102 24 - 4.600000+6 3.568218-5 4.800000+6 3.547364-5 5.000000+6 3.526769-5 125 3102 25 - 5.500000+6 3.477049-5 6.000000+6 3.430506-5 6.500000+6 3.387418-5 125 3102 26 - 7.000000+6 3.347699-5 7.500000+6 3.311084-5 8.000000+6 3.277233-5 125 3102 27 - 8.500000+6 3.245788-5 9.000000+6 3.216400-5 9.500000+6 3.188749-5 125 3102 28 - 1.000000+7 3.162545-5 1.050000+7 3.137531-5 1.100000+7 3.113485-5 125 3102 29 - 1.150000+7 3.090214-5 1.200000+7 3.067552-5 1.250000+7 3.045360-5 125 3102 30 - 1.300000+7 3.023518-5 1.350000+7 3.001928-5 1.400000+7 2.980507-5 125 3102 31 - 1.450000+7 2.959190-5 1.500000+7 2.937920-5 1.550000+7 2.916656-5 125 3102 32 - 1.600000+7 2.895363-5 1.650000+7 2.874018-5 1.700000+7 2.852603-5 125 3102 33 - 1.750000+7 2.831107-5 1.800000+7 2.809523-5 1.850000+7 2.787851-5 125 3102 34 - 1.900000+7 2.766095-5 1.950000+7 2.744259-5 2.000000+7 2.722354-5 125 3102 35 - 125 3 099999 - 125 0 0 0 - 1.001000+3 9.991673-1 0 1 0 0 125 4 2 1 - 0.000000+0 9.991673-1 0 2 0 0 125 4 2 2 - 0.000000+0 0.000000+0 0 0 1 96 125 4 2 3 - 96 2 125 4 2 4 - 0.000000+0 1.000000-5 0 0 6 0 125 4 2 5 --1.60266-14 5.54677-17 2.13338-17 2.27560-17-7.75773-18-2.23184-17 125 4 2 6 - 0.000000+0 2.000000-5 0 0 6 0 125 4 2 7 --3.19039-14 4.35208-17 9.75257-18 2.08597-17-1.39639-17-4.06982-17 125 4 2 8 - 0.000000+0 5.000000-5 0 0 6 0 125 4 2 9 --7.99013-14 4.90676-17 3.04768-17 1.42225-17 6.20618-18-3.54468-17 125 4 2 10 - 0.000000+0 1.000000-4 0 0 6 0 125 4 2 11 --1.59704-13 4.30942-17 1.21907-17 8.53350-18-1.86185-17-2.75698-17 125 4 2 12 - 0.000000+0 2.000000-4 0 0 6 0 125 4 2 13 --3.19498-13 2.00537-17-7.31443-18 8.53350-18-1.08608-17-3.01955-17 125 4 2 14 - 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