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arXiv 2608.27566astro-ph.COastro-ph.GA

TDCOSMO. XXVII:基于JWST的WFI2033、HE0435和PG1115的透镜模型与H₀测量

TDCOSMO. XXVII. JWST-based Lens Models and H$_0$ Measurement of WFI2033, HE0435, and PG1115

D. M. Williams, T. Treu, D. P. Johnson, P. Mozumdar, S. Knabel, S. Birrer, C. D. Fassnacht, A. Galan, A. J. Shajib, K. C. Wong, M. Cappellari, F. Courbin, T. Mo… 展开作者

D. M. Williams, T. Treu, D. P. Johnson, P. Mozumdar, S. Knabel, S. Birrer, C. D. Fassnacht, A. Galan, A. J. Shajib, K. C. Wong, M. Cappellari, F. Courbin, T. Morishita, V. Motta, D. Sluse, M. Stiavelli

AI总结:

本研究基于JWST数据构建三个类星体的透镜模型,结合STARRED技术等推断H₀,结果与HST研究一致且离散度降低,后续将利用16个JWST目标提升H₀测量精度

AI中文摘要:

时延宇宙学为哈勃-勒梅特常数H₀提供了一条无需距离阶梯的直接途径。我们基于JWST-NIRCam/F115W成像,为三个四重成像类星体构建了宇宙学级透镜模型,分别是WFI2033-4723、HE0435-1223、PG1115+080。我们采用STARRED建模技术(该技术在我们此前对WFI2033-4723的分析中已引入),以高保真度重构JWST-NIRCam点扩散函数。我们将基于NIRCam的透镜模型、改进的外部汇聚度估计值、已发表的时延数据,以及JWST NIRSpec提供的孔径积分恒星速度弥散相结合,来推断H₀。对HE0435-1223和PG1115+080的分析采用盲法进行,而对WFI2033-4723的分析未采用盲法,因为我们是基于此前已发表的模型开展工作。为与此前基于HST的研究进行对比,我们将分析限定在无内部质量简并的情况(λ_int=1)。我们量化了改进后的成像、单孔径运动学数据以及环境测量对中心值和不确定性的影响。在平坦ΛCDM模型下,假设对Ω_m采用均匀先验,我们得到PG1115+080的H₀为71.8⁺⁹.²₋₇.⁰ λ_int km s⁻¹ Mpc⁻¹,HE0435-1223的H₀为74.2⁺⁴.²₋₄.² λ_int km s⁻¹ Mpc⁻¹,WFI2033-4723的H₀为73.4⁺³.⁴₋₄.⁴ λ_int km s⁻¹ Mpc⁻¹。将这三个透镜的结果合并后,得到H₀为73.5⁺².⁷₋₂.⁸ λ_int km s⁻¹ Mpc⁻¹,与基于HST的结果(73.6⁺².⁶₋₂.⁶ λ_int km s⁻¹ Mpc⁻¹)一致,但三个系统之间的离散度有所降低。这些模型将以分层方式纳入TDCOSMO-2026里程碑论文,其中λ_int为自由参数。最后,我们概述了即将到来的16个JWST NIRCam目标将如何进一步缩小不确定性,使H₀的精度达到百分位水平。

英文摘要:

Time-delay cosmography offers a one-step, distance-ladder-independent route to the Hubble-Lemaitre constant, H_0. We present new cosmography-grade lens models of three quadruply imaged quasars based on JWST-NIRCam/F115W imaging (WFI2033-4723, HE0435-1223, PG1115+080). We use the STARRED modeling technique, introduced in our previous analysis of WFI2033-4723, to reconstruct the complex JWST-NIRCam Point Spread Function at high fidelity. We combine NIRCam-based lens models with improved external convergence estimates, published time delays, and aperture-integrated stellar velocity dispersions from JWST NIRSpec to infer H_0. The analysis was carried out blindly for HE0435-1223 and PG1115+080, while it was not blind for WFI2033-4723, as we build upon the previous published model. For comparison with previous HST-based work, we limit our analysis to the case of no internal mass-sheet degeneracy ($λ_{\rm int}=1$). We quantify the impact of improved imaging, single-aperture kinematics, and environment measurements on central values and uncertainties. Within flat $Λ$CDM, assuming a uniform prior on $Ω_{\rm m}$, we find H_0 = 71.8$_{-7.0}^{+9.2}$ $λ_{\rm int}$ km s$^{-1}$ Mpc$^{-1}$ for PG1115+080, 74.2$_{-4.2}^{+4.2}$ $λ_{\rm int}$ km s$^{-1}$ Mpc$^{-1}$ for HE0435-1223, and 73.4$_{-4.4}^{+3.4}$ $λ_{\rm int}$ km s$^{-1}$ Mpc$^{-1}$ for WFI2033-4723. Combining the three lenses yields H_0 = 73.5$_{-2.8}^{+2.7}$ $λ_{\rm int}$ km s$^{-1}$ Mpc$^{-1}$, consistent with HST-based results (73.6$_{-2.6}^{+2.6}$ $λ_{\rm int}$ km s$^{-1}$ Mpc$^{-1}$), but with reduced scatter between the three systems. These models will be incorporated in the TDCOSMO-2026 milestone paper with free $λ_{\rm int}$ in a hierarchical fashion. We close by outlining how 16 forthcoming JWST NIRCam targets will further tighten uncertainties toward percent-level precision on H_0.

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