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Table 7

Results of two-temperature Gaussian fits.

Name R in b Near-IR Gaussian Mid-IR Gaussian c Minor/major


(pc) T(K) HWHM (Rin) f 0 T(K) HWHM (Rin) f 0

NGC 4151 0.033 1389  ±  68 1.06  ±  0.02 0.36  ±  0.10 282  ±  6 51.1  ±  1.2 0.12  ±  0.01 12.9
NGC 3783 0.061 1220  ±  108 (fixed to 1) 0.57  ±  0.28 242  ±  9 32.4  ±  0.6 0.77  ±  0.14 8.1
NGC 3783a 0.061 1220  ±  108 (fixed to 1) 0.57  ±  0.28 242  ±  9 39.5  ±  1.0 1.12  ±  0.21 4.1 0.46  ±  0.02
ESO323 0.10 1539  ±  175 (fixed to 1) 0.29  ±  0.14 320  ±  18 12.3  ±  0.4 0.71  ±  0.15 1.7
H0557-385 0.12 1241  ±  54 (fixed to 1) 0.97  ±  0.26 307  ±  15 18.2  ±  1.2 1.06  ±  0.26 1.4
IRAS09149 0.47 1204  ±  103 (fixed to 1) 0.63  ±  0.32 290  ±  39 7.4  ±  0.5 1.67  ±  0.89 0.65
IRAS13349 0.49 1314  ±  57 1.57  ±  0.06 0.37  ±  0.10 366  ±  26 9.6  ±  0.7 1.9  ±  0.6 0.98

Notes. 

(a)

An elliptical Gaussian is fit for the mid-IR component, assuming the major axis at 136°. The quoted mid-IR HWHM is along this major axis.

(b)

See Table 1 for Rin (≡ RτK fit) in mas.

(c)

Reduced χ2 values for visibility fits.

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