2026-09-03 シカゴ大学(UChicago)

Gravitational lensing occurs when the enormous gravity of galaxies bends passing rays of light, which shows up in characteristic half-moon shapes (as in the above image, taken by the Hubble Space Telescope).Image courtesy ESA/Hubble & NASA, S. Jha.
<関連情報>
- https://news.uchicago.edu/story/south-pole-telescope-releases-clearest-map-ever-matter-distant-universe
- https://arxiv.org/abs/2608.31136
SPT-3G D1: 二次推定器によるCMBレンズ再構成と宇宙論
SPT-3G D1: Quadratic-Estimator CMB Lensing Reconstruction and Cosmology
Y. Omori, W. L. K. Wu, Y. Nakato, F. Bianchini, L. Balkenhol, C. Daley, W. Quan, E. Anderes, A. J. Anderson, B. Ansarinejad, M. Archipley, D. R. Barron, P. S. Barry, K. Benabed, A. N. Bender, B. A. Benson, L. E. Bleem, S. Bocquet, F. R. Bouchet, E. Camphuis, M. G. Campitiello, J. E. Carlstrom, J. Carron, C. L. Chang, P. M. Chichura, A. Chokshi, T.-L. Chou, A. Coerver, T. M. Crawford, T. de Haan, K. R. Dibert, M. A. Dobbs, M. Doohan, D. Dutcher, C. Feng, K. R. Ferguson, N. C. Ferree, K. Fichman, A. Foster, S. Galli, A. E. Gambrel, A. K. Gao, F. Ge, F. Guidi, S. Guns, N. W. Halverson, E. Hivon, G. P. Holder, W. L. Holzapfel, J. C. Hood, A. Hryciuk, N. Huang, T. Jhaveri, F. Kéruzoré, A. R. Khalife, L. Knox, K. Kornoelje, C.-L. Kuo, K. Levy, Y. Li, A. E. Lowitz, C. Lu, G. P. Lynch, T. J. Maccarone, A. S. Maniyar, E. S. Martsen, F. Menanteau, M. Millea, J. Montgomery, T. Natoli, A. Ouellette, Z. Pan, P. Paschos, K. A. Phadke, A. W. Pollak, K. Prabhu, M. Rahimi, A. Rahlin, C. L. Reichardt, M. Rouble, J. E. Ruhl, A. C. Silva Oliveira, A. Simpson, J. A. Sobrin, A. A. Stark, J. Stephen, C. Tandoi, C. Trendafilova, J. D. Vieira, A. G. Vieregg, A. Vitrier, Y. Wan, N. Whitehorn, M. R. Young, J. A. Zebrowski
arXiv Submitted on 31 Aug 2026
DOI:https://doi.org/10.48550/arXiv.2608.31136
We present a map of the cosmic microwave background (CMB) lensing potential reconstructed from observations taken during the 2019 and 2020 seasons with the third-generation camera on the South Pole Telescope (SPT), covering the 1500deg2 SPT-3G Main field, referred to as the SPT-3G D1 dataset. From the multi-frequency temperature and polarization data, we reconstruct the CMB lensing field using a quadratic estimator that jointly accounts for the T, E, and B fields and their covariance. The resulting lensing map is dominated by polarization information for L≲600 and provides the highest signal-to-noise measurement per mode reported to date. With nuisance parameters fixed to their best-fit values, we measure a lensing amplitude consistent with unity at 2% precision relative to the ΛCDM model that best fits the combined Planck, ACT DR6, and SPT-3G D1 TT/TE/EE likelihoods (CMBSPA). We further measure the structure-growth parameter σ8Ω0.25m to be 0.6046±0.0096 from the SPT-3G D1 lensing spectrum alone and 0.6020±0.0084 when combined with ACT DR6 and Planck PR4 CMB lensing. By further combining this with CMBSPA and the latest DESI DR2 BAO data, we obtain ∑mν<0.072eV (95% C.L.) when allowing the neutrino mass to vary within ΛCDM. Compared with previous work, the better agreement of our measurement with DESI DR2 BAO yields both this relaxed upper bound and reduced (∼2σ) preferences for nonzero spatial curvature and for deviations of (w0,wa) from the ΛCDM expectation. When we combine CMB lensing with the DES Y3 3×2pt analysis, we obtain S8=0.811±0.011, corresponding to a 1.4% constraint on the late-time clustering amplitude. This precision is competitive with that obtained from the primary CMB within ΛCDM.


