(Based on Wong et al. 2019 and Kochanek 2020)
Wei Zhu (祝伟)
2020-04-30
DS
DL
DLS
β
α
α^
r⊥
Source
Image
Lens
β=θ−α=θ−DSDLSα^
α^=c2r⊥4GM(<r⊥);r⊥=DLθ
θ
Lensing geometry alone does not provide a distance scale (L=VT).
DS
DL
DLS
β
α
α^
r⊥
Source
Image
Lens
DΔt≡(1+zL)DLSDLDS
∇θψ(θ)=α
∇θ2ψ(θ)=2κ(θ)
Δt∝H0−1(1−⟨κ⟩)
θ
Without information about the lens density distribution (κ), time delay itself does not measure H0.
If uncertainty is dominated by kinematics, σ(H0)=σ(κ)≈σ(σ⋆2)=2σ(σ⋆).
DS
DL
DLS
β
α
α^
r⊥
Source
Image
Lens
θ
For each pair of images
θ1
θ2
Lensing data alone
Lensing data & kinematics (10% uncertainty)
No less than ~10% uncertainty on H0. Adding more lenses does not reduce the uncertainty.