Optimal SIE and ε − γ lens parameters for the Q2237+0305 system, derived by the ferret sophisticated genetic algorithm which is a component of the Qubist Global Optimization Toolbox.
. | SIE . | SIE . | ε − γ . | ε − γ . | NSIE + γ . |
---|---|---|---|---|---|
. | . | first order . | . | first order . | . |
|$\chi ^{2}_{r}$| | 1.5466 | 12.204 | 18.165 | – | 0.7319 |
f | |$0.6649_{-0.0094}^{+0.0100}$| | |$0.6479_{-0.0097}^{+0.0097}$| | – | – | |$0.6634_{-0.0096}^{+0.0110}$| |
ϖ | |$1.9720_{-0.0029}^{+0.0028}$| | |$1.9686_{-0.0024}^{+0.0024}$| | – | – | |$2.0111_{-0.0023}^{+0.0023}$| |
ε | – | – | |$0.6653_{-0.0094}^{+0.0100}$| | 1.5949 | – |
γ | – | – | |$0.1047_{-0.0094}^{+0.0100}$| | -0.0292 | |$0.0138_{-0.00012}^{+0.00012}$| |
ω | – | – | |$2.7437_{-0.0094}^{+0.0100}$| | 1.1729 | |$2.7107_{-0.0010}^{+0.0010}$| |
θS | |$0.0652_{-0.0021}^{+0.0021}$| | |$0.0669_{-0.0035}^{+0.0035}$| | |$0.0595_{-0.0094}^{+0.0100}$| | -0.0166 | |$0.0632_{-0.0011}^{+0.0012}$| |
θ | |$6.1261_{-0.0146}^{+0.0150}$| | |$6.0629_{-0.0408}^{+0.0408}$| | |$6.0589_{-0.0094}^{+0.0100}$| | 6.0524 | |$6.1236_{-0.0118}^{+0.0119}$| |
θE | |$0.8974_{-0.0023}^{+0.0023}$| | |$0.9024_{-0.0021}^{+0.0021}$| | |$0.8812_{-0.0094}^{+0.0100}$| | 0.8865 | |$0.9396_{-0.0019}^{+0.0019}$| |
ρc | – | – | – | – | |$0.0332_{-0.0013}^{+0.0013}$| |
ΔxA | 0.0031 | 0.0163 | 0.0064 | – | 0.0028 |
ΔxB | 0.0087 | 0.0097 | 0.0082 | – | 0.0020 |
ΔxC | 0.0082 | 0.0006 | 0.0210 | – | 0.0030 |
ΔxD | 0.0036 | 0.0268 | 0.0335 | – | 0.0027 |
. | SIE . | SIE . | ε − γ . | ε − γ . | NSIE + γ . |
---|---|---|---|---|---|
. | . | first order . | . | first order . | . |
|$\chi ^{2}_{r}$| | 1.5466 | 12.204 | 18.165 | – | 0.7319 |
f | |$0.6649_{-0.0094}^{+0.0100}$| | |$0.6479_{-0.0097}^{+0.0097}$| | – | – | |$0.6634_{-0.0096}^{+0.0110}$| |
ϖ | |$1.9720_{-0.0029}^{+0.0028}$| | |$1.9686_{-0.0024}^{+0.0024}$| | – | – | |$2.0111_{-0.0023}^{+0.0023}$| |
ε | – | – | |$0.6653_{-0.0094}^{+0.0100}$| | 1.5949 | – |
γ | – | – | |$0.1047_{-0.0094}^{+0.0100}$| | -0.0292 | |$0.0138_{-0.00012}^{+0.00012}$| |
ω | – | – | |$2.7437_{-0.0094}^{+0.0100}$| | 1.1729 | |$2.7107_{-0.0010}^{+0.0010}$| |
θS | |$0.0652_{-0.0021}^{+0.0021}$| | |$0.0669_{-0.0035}^{+0.0035}$| | |$0.0595_{-0.0094}^{+0.0100}$| | -0.0166 | |$0.0632_{-0.0011}^{+0.0012}$| |
θ | |$6.1261_{-0.0146}^{+0.0150}$| | |$6.0629_{-0.0408}^{+0.0408}$| | |$6.0589_{-0.0094}^{+0.0100}$| | 6.0524 | |$6.1236_{-0.0118}^{+0.0119}$| |
θE | |$0.8974_{-0.0023}^{+0.0023}$| | |$0.9024_{-0.0021}^{+0.0021}$| | |$0.8812_{-0.0094}^{+0.0100}$| | 0.8865 | |$0.9396_{-0.0019}^{+0.0019}$| |
ρc | – | – | – | – | |$0.0332_{-0.0013}^{+0.0013}$| |
ΔxA | 0.0031 | 0.0163 | 0.0064 | – | 0.0028 |
ΔxB | 0.0087 | 0.0097 | 0.0082 | – | 0.0020 |
ΔxC | 0.0082 | 0.0006 | 0.0210 | – | 0.0030 |
ΔxD | 0.0036 | 0.0268 | 0.0335 | – | 0.0027 |
Notes. The parameters ε represents the slope of the power-law mass distribution, γ the magnitude of the external shear, ω the orientation of the external shear and ρc the size of the core radius in arcsec. The lower and upper limits correspond to the range of the lens parameters used by the genetic algorithm routine. The distances between the lensed images and the modelled images are represented by Δx.
Optimal SIE and ε − γ lens parameters for the Q2237+0305 system, derived by the ferret sophisticated genetic algorithm which is a component of the Qubist Global Optimization Toolbox.
. | SIE . | SIE . | ε − γ . | ε − γ . | NSIE + γ . |
---|---|---|---|---|---|
. | . | first order . | . | first order . | . |
|$\chi ^{2}_{r}$| | 1.5466 | 12.204 | 18.165 | – | 0.7319 |
f | |$0.6649_{-0.0094}^{+0.0100}$| | |$0.6479_{-0.0097}^{+0.0097}$| | – | – | |$0.6634_{-0.0096}^{+0.0110}$| |
ϖ | |$1.9720_{-0.0029}^{+0.0028}$| | |$1.9686_{-0.0024}^{+0.0024}$| | – | – | |$2.0111_{-0.0023}^{+0.0023}$| |
ε | – | – | |$0.6653_{-0.0094}^{+0.0100}$| | 1.5949 | – |
γ | – | – | |$0.1047_{-0.0094}^{+0.0100}$| | -0.0292 | |$0.0138_{-0.00012}^{+0.00012}$| |
ω | – | – | |$2.7437_{-0.0094}^{+0.0100}$| | 1.1729 | |$2.7107_{-0.0010}^{+0.0010}$| |
θS | |$0.0652_{-0.0021}^{+0.0021}$| | |$0.0669_{-0.0035}^{+0.0035}$| | |$0.0595_{-0.0094}^{+0.0100}$| | -0.0166 | |$0.0632_{-0.0011}^{+0.0012}$| |
θ | |$6.1261_{-0.0146}^{+0.0150}$| | |$6.0629_{-0.0408}^{+0.0408}$| | |$6.0589_{-0.0094}^{+0.0100}$| | 6.0524 | |$6.1236_{-0.0118}^{+0.0119}$| |
θE | |$0.8974_{-0.0023}^{+0.0023}$| | |$0.9024_{-0.0021}^{+0.0021}$| | |$0.8812_{-0.0094}^{+0.0100}$| | 0.8865 | |$0.9396_{-0.0019}^{+0.0019}$| |
ρc | – | – | – | – | |$0.0332_{-0.0013}^{+0.0013}$| |
ΔxA | 0.0031 | 0.0163 | 0.0064 | – | 0.0028 |
ΔxB | 0.0087 | 0.0097 | 0.0082 | – | 0.0020 |
ΔxC | 0.0082 | 0.0006 | 0.0210 | – | 0.0030 |
ΔxD | 0.0036 | 0.0268 | 0.0335 | – | 0.0027 |
. | SIE . | SIE . | ε − γ . | ε − γ . | NSIE + γ . |
---|---|---|---|---|---|
. | . | first order . | . | first order . | . |
|$\chi ^{2}_{r}$| | 1.5466 | 12.204 | 18.165 | – | 0.7319 |
f | |$0.6649_{-0.0094}^{+0.0100}$| | |$0.6479_{-0.0097}^{+0.0097}$| | – | – | |$0.6634_{-0.0096}^{+0.0110}$| |
ϖ | |$1.9720_{-0.0029}^{+0.0028}$| | |$1.9686_{-0.0024}^{+0.0024}$| | – | – | |$2.0111_{-0.0023}^{+0.0023}$| |
ε | – | – | |$0.6653_{-0.0094}^{+0.0100}$| | 1.5949 | – |
γ | – | – | |$0.1047_{-0.0094}^{+0.0100}$| | -0.0292 | |$0.0138_{-0.00012}^{+0.00012}$| |
ω | – | – | |$2.7437_{-0.0094}^{+0.0100}$| | 1.1729 | |$2.7107_{-0.0010}^{+0.0010}$| |
θS | |$0.0652_{-0.0021}^{+0.0021}$| | |$0.0669_{-0.0035}^{+0.0035}$| | |$0.0595_{-0.0094}^{+0.0100}$| | -0.0166 | |$0.0632_{-0.0011}^{+0.0012}$| |
θ | |$6.1261_{-0.0146}^{+0.0150}$| | |$6.0629_{-0.0408}^{+0.0408}$| | |$6.0589_{-0.0094}^{+0.0100}$| | 6.0524 | |$6.1236_{-0.0118}^{+0.0119}$| |
θE | |$0.8974_{-0.0023}^{+0.0023}$| | |$0.9024_{-0.0021}^{+0.0021}$| | |$0.8812_{-0.0094}^{+0.0100}$| | 0.8865 | |$0.9396_{-0.0019}^{+0.0019}$| |
ρc | – | – | – | – | |$0.0332_{-0.0013}^{+0.0013}$| |
ΔxA | 0.0031 | 0.0163 | 0.0064 | – | 0.0028 |
ΔxB | 0.0087 | 0.0097 | 0.0082 | – | 0.0020 |
ΔxC | 0.0082 | 0.0006 | 0.0210 | – | 0.0030 |
ΔxD | 0.0036 | 0.0268 | 0.0335 | – | 0.0027 |
Notes. The parameters ε represents the slope of the power-law mass distribution, γ the magnitude of the external shear, ω the orientation of the external shear and ρc the size of the core radius in arcsec. The lower and upper limits correspond to the range of the lens parameters used by the genetic algorithm routine. The distances between the lensed images and the modelled images are represented by Δx.
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