Table B.1
Near-IR continuum (stellar) radii determinations.
IRAS | ![]() |
![]() |
Comm. | ![]() |
![]() |
Comm. | Adopted | code | Previous Rhl |
name | (kpc) | (kpc) | code | (kpc) | (kpc) | code | (kpc) | (kpc)(ref) | |
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) |
|
|||||||||
01159 N | 0.81 ± 0.32 | 1.30 ± 0.44 | 1,7 | ... | ... | 1.0 ± 0.4 | 1100 | ||
01159 S | 2.39 ± 0.72 | 2.09 ± 0.47 | 1 | ... | ... | 2.2 ± 0.6 | 1100 | ||
01341 N | 2.56 ± 0.50 | 2.20 ± 0.56 | 1.55 ± 0.65 | 0.95 ± 0.15 | c | 2.2 ± 0.6 | 1110 | ||
01341 S | 1.50 ± 0.60 | 0.93 ± 0.26 | 4 | ... | ... | 1.5 ± 0.6 | 1000 | ||
04315 | 1.15 ± 0.35 | 0.94 ± 0.14 | 4 | 0.55 ± 0.30 | 0.36 ± 0.12 | c | 1.2 ± 0.4 | 1000 | 0.06 (b) |
05189 | ... | (0.67) | 6 | (0.10) | (0.25) | h | (0.18) | 0000 | |
06035 | ... | 4.71 ± 1.35 | ... | ... | 4.7 ± 1.4 | 0100 | |||
06076 N | 3.00 ± 1.40 | 2.21 ± 0.37 | 1 | 3.23 ± 0.06 | ... | d | 3.2 ± 0.6 | 1110 | |
06076 S | 3.40 ± 1.20 | 1.73 ± 0.45 | 1 | 3.11 ± 0.06 | ... | d | 3.1 ± 0.6 | 1010 | |
06206 | (3.60) | (4.56) | 5 | ... | 2.41 ± 0.60 | 2.4 ± 0.6 | 0001 | ||
06259 N | 1.09 ± 0.20 | 1.45 ± 0.58 | 1 | 1.15 ± 0.05 | 1.02 ± 0.02 | 1.0 ± 0.2 | 1011 | ||
06259 C | 1.67 ± 0.12 | 1.73 ± 0.35 | 1 | 2.91 ± 0.07 | 1.16 ± 0.04 | f | 2.6 ± 0.7 | 1010 | |
06259 S | 2.60 ± 0.50 | 1.74 ± 0.58 | 4 | ... | 1.14 ± 0.04 | e | 2.6 ± 0.7 | 1000 | |
06295 | ... | 3.03 ± 0.62 | 3 | ... | ... | 3.0 ± 0.6 | 0100 | ||
06592 | 1.53 ± 0.60 | 1.17 ± 0.26 | ... | ... | 1.2 ± 0.4 | 1100 | |||
07027 N | ... | (0.79) | 6 | ... | (0.2 ) | h | (0.2) | 0000 | |
07027 S | 1.61 ± 0.70 | 1.54 ± 0.69 | 1.75 ± 0.06 | 0.96 ± 0.02 | 1.5 ± 0.5 | 1111 | |||
07160 | 3.64 ± 0.35 | 2.32 ± 0.35 | 4 | ... | 0.82 ± 0.03 | a,e | 3.6 ± 0.5 | 1000 | |
08355 | 0.91 ± 0.25 | 1.21 ± 0.34 | 2.09 ± 0.38 | 0.91 ± 0.18 | f | 1.3 ± 0.8 | 1110 | ||
08424 N | 2.50 ± 1.10 | 0.81 ± 0.07 | 1,4 | ... | ... | 2.5 ± 0.5 | 1000 | ||
08424 S | 2.20 ± 0.80 | 1.02 ± 0.10 | 1 | ... | ... | 2.2 ± 0.4 | 1000 | ||
08520 E | 2.87 ± 0.98 | ... | 2.36 ± 0.34 | 2.17 ± 0.25 | g | 2.4 ± 0.6 | 1010 | ||
08520 W | 4.00 ± 0.30 | ... | 4 | 5.95 ± 0.22 | 2.64 ± 0.30 | g | 5.3 ± 1.4 | 1010 | |
09022 | 1.96 ± 0.45 | 1.95 ± 0.40 | 3.25 ± 0.85 | 2.40 ± 0.40 | d | 2.2 ± 0.6 | 1111 | ||
09437 N | 6.10 ± 1.10 | 3.46 ± 0.71 | 4 | ... | ... | 6.1 ± 1.3 | 1000 | ||
09437 S | 3.09 ± 0.21 | 2.33 ± 0.39 | 4 | ... | ... | 3.1 ± 0.5 | 1000 | ||
10015 | 3.56 ± 0.45 | 2.75 ± 0.48 | 1.18 ± 0.18 | 1.36 ± 0.10 | a | 3.2 ± 0.6 | 1100 | ||
10038 | 2.12 ± 0.70 | 1.96 ± 0.61 | ... | ... | 2.0 ± 0.6 | 1100 | |||
10257 | 2.66 ± 0.86 | 1.76 ± 0.27 | 1.55 ± 0.04 | 1.33 ± 0.01 | a,d | 1.8 ± 0.6 | 1100 | ||
10409 | 2.92 ± 0.22 | 2.25 ± 0.19 | ... | ... | 2.5 ± 0.5 | 1100 | |||
10567 | 2.88 ± 1.50 | 3.20 ± 0.40 | 2 | ... | ... | 3.2 ± 0.9 | 1100 | ||
11254 | 3.14 ± 0.86 | 2.40 ± 0.57 | 2 | ... | ... | 2.6 ± 0.7 | 1100 | ||
11506 | 1.22 ± 0.20 | 0.94 ± 0.17 | 0.67 ± 0.02 | 0.61 ± 0.02 | c | 1.1 ± 0.2 | 1100 | ||
12042 N | 1.22 ± 0.20 | 1.18 ± 0.29 | 1 | ... | ... | 1.2 ± 0.2 | 1100 | ||
12042 S | 2.32 ± 0.32 | 1.47 ± 0.26 | 4 | ... | ... | 2.3 ± 0.5 | 1000 | ||
12115 | 2.97 ± 0.57 | 2.14 ± 0.36 | ... | ... | 2.4 ± 0.6 | 1100 | |||
12116 | 1.17 ± 0.35 | 1.34 ± 0.25 | 1 | 1.94 ± 0.88 | 1.12 ± 0.11 | b,f | 1.3 ± 0.5 | 1110 | |
12596 | 2.17 ± 0.97 | 1 | ... | 3.13 ± 0.45 | c | 2.7 ± 1.0 | 0101 | ||
13001 | 3.71 ± 1.00 | 2.89 ± 1.10 | 4 | 5.79 ± 0.15 | 3.33 ± 0.09 | d | 5.7 ± 1.5 | 1010 | |
13229 | 3.41 ± 0.85 | 2.39 ± 0.84 | 4 | 1.08 ± 0.09 | 0.87 ± 0.04 | a | 3.4 ± 1.2 | 1000 | |
14544 E | 4.76 ± 0.56 | 2.63 ± 0.48 | 4 | 2.66 ± 0.19 | 1.24 ± 0.06 | c | 4.8 ± 1.2 | 1000 | |
14544 W | 3.04 ± 1.43 | 2.25 ± 0.51 | 2 | 1.55 ± 0.16 | 1.09 ± 0.12 | a | 2.3 ± 1.0 | 1100 | |
17138 | 1.78 ± 0.15 | 1.46 ± 0.25 | 1.44 ± 0.13 | 1.06 ± 1.14 | a | 1.7 ± 0.2 | 1100 | ||
18093 N | 1.75 ± 0.32 | 1.64 ± 0.35 | 1 | 1.57 ± 0.18 | 1.13 ± 0.08 | a | 1.8 ± 0.5 | 1000 | |
18093 C | (1.04) | 5 | 0.39 ± 0.21 | 0.26 ± 0.14 | c,g | >0.3± 0.2 | 0011 | ||
18093 S | 2.07 ± 0.53 | 1.46 ± 0.30 | 4 | 1.89 ± 0.27 | 1.32 ± 0.09 | c | 2.1 ± 0.7 | 1000 | |
21130 | 4.95 ± 0.48 | 4.56 ± 1.21 | ... | ... | 4.9 ± 0.8 | 1100 | |||
21453 | 3.68 ± 0.51 | 2.97 ± 0.82 | 2.59 ± 0.29 | 1.34 ± 0.08 | a | 3.5 ± 0.7 | 1100 | ||
22132 | 5.13 ± 0.66 | 3.12 ± 1.15 | 2,4 | ... | 1.11 ± 0.04 | a,e | 5.1 ± 0.7 | 1000 | |
22491 | 3.70 ± 1.00 | 3.42 ± 2.80 | 2 | ... | 3.00 ± 2.40 | b | 3.6 ± 1.5 | 1101 | 8.29 (a) |
23128 | ... | 1.91 ± 0.22 | ... | 1.60 ± 0.22 | 1.8 ± 0.3 | 0101 |
Notes. Columns: (1) Identification. (2) Half-light radius from the 2MASS K-band image using GALFIT. (3) Half-light radius from the 2MASS K-band image using the A/2 method (see text). (4) Comments associated with the 2MASS images determinations, according to the following code: 1- large uncertainties when applying the A/2 method due to galaxy decomposition; 2- uncertainty due to background value, field stars, and/or complex structure; 3- GALFIT could not obtain a reliable fit; 4- disc with b/a < 0.4, leading to discrepancies between the two methods; 5- unreliable estimates due to background and/or complex structure; 6- point-like source dominating the (unreliable) radius determination; 7- FWHM of the bulge component close to the value for the PSF, making the radii estimates uncertain. (5) Half-light radius from the HST H-band image using GALFIT. (6) Half-light radius from the HST H-band image using the A/2 method. (7) Comments associated with the HST determinations, according to the following code: a- severely limited by FoV; b- very uncertain results due to bad background definition; c- limited by FoV; d- HST image obtained with WFC3 or NIC3 (instead of NIC2); e- bad GALFIT fit; f- rich structure in the HST image; g- uncertainties when applying the A/2 method due to galaxy decomposition; h- point-like source dominating the (unreliable) radius determination. (8) Adopted values. (9) Code indication if the individual values in columns 2, 3, 5, and 6 were used in the adopted value (0 = not used, 1 = used). (10) Previous determinations with the following code: (a) Scoville et al. (2000), model fitting (de Vaucoulers or exponential) to F160W images; (b) Hinz & Rieke (2006).
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.