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JWSTs PEARLS: NIRCam imaging and NIRISS spectroscopy of a $z=3.6$ star-forming galaxy lensed into a near-Einstein Ring by a $z=1.258$ massive elliptical galaxy

Nathan J. Adams, Giovanni Ferrami, Lewi Westcott, Thomas Harvey, Vicente Estrada-Carpenter, Christopher J. Conselice, Duncan Austin, J. Stuart B. Wyithe, Caio M. Goolsby, Qiong Li, Vadim Rusakov, Rogier A. Windhorst, Seth H. Cohen, Rolf A. Jansen, Jake Summers, Roselia O'Brein, Anton M. Koekemoer, Simon P. Driver, Brenda Frye, Nimish P. Hathi, Dan Coe, Norman A. Grogin, Madeline A. Marshall, Nor Pirzkal, Russell E. Ryan, Christopher N. A. Willmer, Haojing Yan, Benne W. Holwerda, Patrick S. Kamieneski, Tom Broadhurst, W. Peter Maksym, Payaswini Saikia, Joseph D. Gelfand

TL;DR

This study reports the discovery and initial analysis of a high-redshift strong galaxy-galaxy lens that produces a near-Einstein ring, lensed by a massive elliptical at $z_l=1.258$ with the background source at $z_s=3.6\pm0.1$. By combining JWST/NIRCam imaging, HST data, and NIRISS F200W spectroscopy, the authors perform light deblending, photometric redshift estimation, and lens modelling (lenstronomy) to derive image magnifications, a total lensing mass of $M_{\mathrm{lensing}}=(4.08\pm0.07)\times10^{11}\,M_\odot$, and a DM mass within the Einstein radius of order $\sim2.8\times10^{11}\,M_\odot$. The background source is inferred to be a moderately dusty starburst with $\log_{10}(M_*/M_\odot)=8.17^{+0.18}_{-0.23}$ and $A_V=0.88^{+0.20}_{-0.13}$, while the foreground lens is a massive, passive elliptical with $\log_{10}(M_*/M_\odot)=11.48^{+0.06}_{-0.15}$ and a potential radio AGN. The work demonstrates JWST’s power to probe mass components and IMF variations in massive ellipticals through lensing at high redshift, and outlines future avenues (e.g., deeper spectroscopy and IFU data) to tighten constraints on dark matter content and stellar mass budgets.

Abstract

We present the discovery, and initial lensing analysis, of a high-redshift galaxy-galaxy lensing system within the JWST-PEARLS/HST-TREASUREHUNT North Ecliptic Pole Time Domain Field (designated NEPJ172238.9+655143.1). The lensing geometry shears a $z=3.6\pm0.1$ star-forming galaxy into a near-Einstein ring with a radius of 0\farcs92, consisting of 4 primary images, around a foreground massive elliptical galaxy at $z=1.258\pm0.005$. The system is fortuitously located within the NIRISS F200W footprint of the PEARLS survey, enabling spectroscopic identification of the 8500A TiO band in the foreground galaxy and allowing tight constraints to be placed on the redshift of the background galaxy based on its continuum detection and lack of strong emission lines. We calculate magnification factors of $2.6<μ<8.4$ for the four images and a total lensing mass of $(4.08 \pm 0.07)\times10^{11}M_\odot$. SED fitting of the foreground elliptical galaxy within the Einstein radius reveals a stellar mass of $\sim1.26\times10^{11}M_\odot$, providing a mass/light ratio of 3.24. Employing simple scaling relations and assumptions, an NFW dark matter halo is found to provide the correct remaining mass within $0.12^{+0.21}_{-0.09}$dex. However, if a bottom-heavy IMF for elliptical galaxies is employed, stellar mass estimations increase and can account for the majority of the lensing mass (up to $\sim$83\%), reducing the need for dark matter. This system further demonstrates the new discovery space that the combined wavelength coverage, sensitivity and resolution of JWST now enables.

JWSTs PEARLS: NIRCam imaging and NIRISS spectroscopy of a $z=3.6$ star-forming galaxy lensed into a near-Einstein Ring by a $z=1.258$ massive elliptical galaxy

TL;DR

This study reports the discovery and initial analysis of a high-redshift strong galaxy-galaxy lens that produces a near-Einstein ring, lensed by a massive elliptical at with the background source at . By combining JWST/NIRCam imaging, HST data, and NIRISS F200W spectroscopy, the authors perform light deblending, photometric redshift estimation, and lens modelling (lenstronomy) to derive image magnifications, a total lensing mass of , and a DM mass within the Einstein radius of order . The background source is inferred to be a moderately dusty starburst with and , while the foreground lens is a massive, passive elliptical with and a potential radio AGN. The work demonstrates JWST’s power to probe mass components and IMF variations in massive ellipticals through lensing at high redshift, and outlines future avenues (e.g., deeper spectroscopy and IFU data) to tighten constraints on dark matter content and stellar mass budgets.

Abstract

We present the discovery, and initial lensing analysis, of a high-redshift galaxy-galaxy lensing system within the JWST-PEARLS/HST-TREASUREHUNT North Ecliptic Pole Time Domain Field (designated NEPJ172238.9+655143.1). The lensing geometry shears a star-forming galaxy into a near-Einstein ring with a radius of 0\farcs92, consisting of 4 primary images, around a foreground massive elliptical galaxy at . The system is fortuitously located within the NIRISS F200W footprint of the PEARLS survey, enabling spectroscopic identification of the 8500A TiO band in the foreground galaxy and allowing tight constraints to be placed on the redshift of the background galaxy based on its continuum detection and lack of strong emission lines. We calculate magnification factors of for the four images and a total lensing mass of . SED fitting of the foreground elliptical galaxy within the Einstein radius reveals a stellar mass of , providing a mass/light ratio of 3.24. Employing simple scaling relations and assumptions, an NFW dark matter halo is found to provide the correct remaining mass within dex. However, if a bottom-heavy IMF for elliptical galaxies is employed, stellar mass estimations increase and can account for the majority of the lensing mass (up to 83\%), reducing the need for dark matter. This system further demonstrates the new discovery space that the combined wavelength coverage, sensitivity and resolution of JWST now enables.

Paper Structure

This paper contains 19 sections, 4 equations, 3 figures, 2 tables.

Figures (3)

  • Figure 1: The full F200W NIRCam footprint of the NEP-TDF Field with the object of interested highlighted with a red circle. Accompanying RGB cutouts use the F444W, F200W, F090W filters and show: Top Left a $\sim10\times10$ arcsecond cutout of the region surrounding the target of interest. Top Right a zoom into the core of the elliptical highlighting the ring-like structure which has a radius of 092. Bottom Right A zoom into the residual lensed arcs once a Sérsic profile for the elliptical galaxy is subtracted off and the arcs numbered.
  • Figure 2: The best fitting SED to the extracted photometry of the foreground elliptical galaxy ($<0.9$as, Top) and the demagnified lens source (Second from Bottom). Alongside the SED fits are the NIRISS spectra within the F200W bandpass (approx. 1.75 to 2.25 microns). For the foreground elliptical, we show the forward-modelled NIRISS spectrum using the methodology of Estrada-Carpenter2024 and highlight the broad absorption feature attributed to the 8500Å TiO band. The NIRISS spectrum of the background source has no significant features within the high-throughput region of the F200W bandpass (1.75-2.23 microns, low throughput shaded grey).
  • Figure 3: The results of the lens modelling process with lenstronomy. The top-left panel shows the original input imaging from JWST F150W. The top-centre panel shows the reconstructed model. The top-right panel shows the residual image when the model is subtracted from the data. The centre-left panel shows the source plane. The central panel shows the intrinsic light profile of the elliptical lensing galaxy. The centre-right panel shows the magnification map. The bottom-left panel shows the elliptical model convolved with the PSF. The bottom-centre panel shows the lensed source, with shear, convolved with the PSF. The bottom-right panel again shows the final reconstructed image.