2023PASP..135a4502K


Query : 2023PASP..135a4502K

2023PASP..135a4502K - Publ. Astron. Soc. Pac., 135, part no 1, 4502 (2023/January-0)

The Near Infrared Imager and Slitless Spectrograph for JWST. V. Kernel Phase Imaging and Data Analysis.

KAMMERER J., COOPER R.A., VANDAL T., THATTE D., MARTINACHE F., SIVARAMAKRISHNAN A., CHAUSHEV A., STOLKER T., LLOYD J.P., ALBERT L., DOYON R., SALLUM S., PERRIN M.D., PUEYO L., MERAND A., GALLENNE A., GREENBAUM A., SANCHEZ-BERMUDEZ J., BLAKELY D., JOHNSTONE D., VOLK K., MARTEL A., GOUDFROOIJ P., MEYER M.R., WILLOTT C.J., DE FURIO M., DANG L., RADICA M. and NOIROT G.

Abstract (from CDS):

Kernel phase imaging (KPI) enables the direct detection of substellar companions and circumstellar dust close to and below the classical (Rayleigh) diffraction limit. The high-Strehl full pupil images provided by the James Webb Space Telescope (JWST) are ideal for application of the KPI technique. We present a kernel phase analysis of JWST NIRISS full pupil images taken during the instrument commissioning and compare the performance to closely related NIRISS aperture masking interferometry (AMI) observations. For this purpose, we develop and make publicly available the custom Kpi3Pipeline data reduction pipeline enabling the extraction of kernel phase observables from JWST images. The extracted observables are saved into a new and versatile kernel phase FITS file data exchange format. Furthermore, we present our new and publicly available fouriever toolkit which can be used to search for companions and derive detection limits from KPI, AMI, and long-baseline interferometry observations while accounting for correlated uncertainties in the model fitting process. Among the four KPI targets that were observed during NIRISS instrument commissioning, we discover a low-contrast (∼1:5) close-in (∼1 λ/D) companion candidate around CPD-66 562 and a new high-contrast (∼1:170) detection separated by ∼1.5 λ/D from 2MASS J062802.01-663738.0. The 5σ companion detection limits around the other two targets reach ∼6.5 mag at ∼200 mas and ∼7 mag at ∼400 mas. Comparing these limits to those obtained from the NIRISS AMI commissioning observations, we find that KPI and AMI perform similar in the same amount of observing time. Due to its 5.6 times higher throughput if compared to AMI, KPI is beneficial for observing faint targets and superior to AMI at separations ≳325 mas. At very small separations (≲100 mas) and between ∼250 and 325 mas, AMI slightly outperforms KPI which suffers from increased photon noise from the core and the first Airy ring of the point-spread function.

Abstract Copyright: © 2023. The Author(s). Published by IOP Publishing Ltd on behalf of the Astronomical Society of the Pacific (ASP). All rights reserved

Journal keyword(s): High angular resolution - Interferometry - Direct imaging - Astronomy data reduction

Simbad objects: 13

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Number of rows : 13
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 Ross 28 ** 04 12 58.8326322803 +52 36 42.021350887   15.0   13.203   M4.0V 54 0
2 V* T Tau TT* 04 21 59.4319873992 +19 32 06.432393336   11.22 10.12 9.80   K0IV/Ve 1404 1
3 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 4425 0
4 V* AB Dor C LM* 05 28 44.83 -65 26 54.9           M8: 67 0
5 V* AB Dor TT* 05 28 44.8712165880 -65 26 55.199147208 8.259 7.856 6.999 6.496 5.993 K0V 1023 0
6 HD 36805 * 05 29 06.4770554328 -66 41 13.201208412   9.36 8.09     K2III 23 0
7 HD 37093 * 05 31 08.2590174816 -65 07 42.083399712   10.70 9.25     K5(III) 13 0
8 TYC 8906-1660-1 * 06 27 00.5443408200 -66 21 59.052159720   12.24 10.64     ~ 3 0
9 UCAC4 117-011267 * 06 28 02.0014566936 -66 37 38.095571100   11.979   10.708   ~ 4 0
10 CPD-67 607 * 06 29 31.9252018176 -67 13 13.004316048   11.784 10.732     ~ 6 0
11 CPD-66 562 * 06 31 36.6171205438 -66 21 47.605754007   11.344 10.511     ~ 8 0
12 * 26 Cir cC* 14 52 35.2587595008 -63 48 35.356730796   6.66 5.96   4.993 F8II 141 0
13 * alf Oph ** 17 34 56.06945 +12 33 36.1346 2.32 2.22 2.07 1.93 1.85 A5IVnn 479 0

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