GD200fnr
Under investigation
Binary lens models with parallax
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Model X1 χ2=41144.
s=1.01676±0.0123355 q=0.0444828±0.00753492 u0=-0.260275±0.0141388 α=6.07078±0.0264128 ρ*=0.0557772±0.0161644 tE=100.638±2.16931 t0=9419.14±0.891539 πE,N=-0.281681±0.00768875 πE,E=0.311156±0.0124521 |
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Model X2 χ2=59035.6
s=0.914204±0.0316061 q=0.436298±0.0687325 u0=0.150448±0.00849091 α=5.72224±0.0294089 ρ*=0.0684043±0.00604068 tE=203.477±12.0495 t0=9418.02±0.616872 πE,N=-0.195204±0.0121139 πE,E=0.0291209±0.00870076 |
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Model X3 χ2=67371.
s=0.7271±0.0293439 q=2.44126±0.505678 u0=-0.208792±0.00782361 α=3.00647±0.0134731 ρ*=0.02058±0.00281938 tE=637.136±59.7691 t0=9355.13±0.661839 πE,N=0.069196±0.00193844 πE,E=-0.041429±0.00473355 |
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Model X4 χ2=67522.3
s=0.901423±0.031322 q=0.38412±0.0469387 u0=0.151239±0.00736306 α=5.69826±0.0307342 ρ*=0.073212±0.00737489 tE=207.31±9.95187 t0=9421.81±0.373455 πE,N=-0.19923±0.00958648 πE,E=0.0193441±0.00715509 |
Binary lens models with parallax and orbital motion
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Model O1 χ2=36589.
s=1.03549±0.00146588 q=0.0415906±0.000848704 u0=0.068934±0.00264022 α=3.80246±0.0047864 ρ*=0.0202415±0.000744902 tE=221.854±1.06727 t0=9399.95±0.176161 πE,N=-0.0549331±0.00171826 πE,E=0.0957852±0.000645597 (ds/dt)/s=0.000674364±0.0000178863 dα/dt=-0.000545637±0.0000221464 w3=0.00106988±0.0000972251 |
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Model O2 χ2=38334.6
s=1.01192±0.00236938 q=0.0416307±0.000728301 u0=-0.259688±0.00211814 α=6.08535±0.00435008 ρ*=0.0564783±0.00225098 tE=101.678±0.302566 t0=9418.71±0.130062 πE,N=-0.270629±0.00149942 πE,E=0.307926±0.00191867 (ds/dt)/s=-0.000109594±0.0000108233 dα/dt=-0.0000247955± -6
5.0667 10 w3= -7
1. 10±0.299252 |
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