Table 1
NIR interferometric detections of hot exozodiacal dust, together with associated outer debris belt locations.
Object | Sp. type | Band | Excess | FOVa | Instrument | Refs. | Outer belt distanceb | Refs. | ||
[%] | [AU] | [AU] | ||||||||
|
||||||||||
Vega | A0V | H | 1.23 | ± | 0.53 | 6 | IOTA/IONIC | D11 | 10–14, 80 | D00, S13 |
Vega | A0V | K | 1.26 | ± | 0.27 | 3 | CHARA/FLUOR | A06, A13 | 10–14, 80 | D00, S13 |
Vega | A0V | K |
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4 | PTI | C01 | 10–14, 80 | D00, S13 | ||
ζ Aql | A0V | K | 1.69 | ± | 0.27 | 10 | CHARA/FLUOR | A08, A13 | no detectable outer belt | A08, P09 |
β Leo | A3V | K | 0.94 | ± | 0.26 | 4 | CHARA/FLUOR | Ak09, A13 | 19 | C06 |
λ Gem | A3V | K | 0.74 | ± | 0.17 | 12 | CHARA/FLUOR | A13 | no detectable outer belt | M09, G13 |
Fomalhaut | A4V | K | 0.88 | ± | 0.12 | 6 | VLTI/VINCI | Ab09 | 2, 8–11, 133 | K05, L13, S13 |
β Picc | A6V | H | 1.37 | ± | 0.16 | 4 | VLTI/PIONIER | D12 | 10–40d | L94, P97 |
β Picc | A6V | K | 0.76 | ± | 0.49 | 1.3 | VLTI/VINCI | D04, D12 | 10–40d | L94, P97 |
α Aql | A7V | K | 3.07 | ± | 0.24 | 2 | CHARA/FLUOR | A13 | no detectable outer belt | A13 |
α Cep | A7IV | K | 0.87 | ± | 0.18 | 6 | CHARA/FLUOR | A13 | no detectable outer belt | C05 |
η Lepe | F1V | K | 0.89 | ± | 0.21 | 6 | CHARA/FLUOR | A13 | 1–16, 18 | L09, E13 |
110 Here | F6V | K | 0.94 | ± | 0.25 | 8 | CHARA/FLUOR | A13 | 70–500 | M13 |
10 Taue | F9V | K | 1.21 | ± | 0.11 | 6 | CHARA/FLUOR | A13 | >5.8 | T08 |
ξ Booe | G8V | K | 0.74 | ± | 0.20 | 3 | CHARA/FLUOR | A13 | no detectable outer belt | A13 |
τ Cet | G8V | K | 0.98 | ± | 0.18 | 1.5 | CHARA/FLUOR | D07, A13 | 10–55 | G04 |
κ CrBe | K1IV | K | 1.18 | ± | 0.20 | 12 | CHARA/FLUOR | A13 | 20, 41 | B13 |
Notes.
For the outer belt distance (r0 in our models) we list literature estimates of the radial distance to (the inner edge of) “cold” and “warm” outer belts, derived from SED fitting and/or resolved imaging.
The NIR excess of β Pic contains a significant contribution from stellar light scattered by the outer belt (Defrère et al. 2012).
The debris disk around β Pic is seen edge-on, making it hard to determine the parent belt location. The values given mark the radial range in which the particle density is derived to decrease.
For η Lep, 110 Her, 10 Tau, ξ Boo, and κ CrB, the possibility that the observed NIR excess is due to a low-mass companion within the field-of-view cannot be excluded (Absil et al. 2013).
Reference. (A06) Absil et al. (2006); (A08) Absil et al. (2008); (Ab09) Absil et al. (2009); (Ak09) Akeson et al. (2009); (A13) Absil et al. (2013); (B13) Bonsor et al. (2013); (C01) Ciardi et al. (2001); (C05) Chen et al. (2005); (C06) Chen et al. (2006); (D00) Dent et al. (2000); (D04) di Folco et al. (2004); (D07) di Folco et al. (2007); (D11) Defrère et al. (2011); (D12) Defrère et al. (2012); (E13) Eiroa et al. (2013); (G04) Greaves et al. (2004); (G13) Gáspár et al. (2013); (K05) Kalas et al. (2005); (L94) Lagage & Pantin (1994); (L09) Lawler et al. (2009); (L13) Lebreton et al. (2013); (M09) Morales et al. (2009); (M13) Marshall et al. (2013); (P97) Pantin et al. (1997); (P09) Plavchan et al. (2009); (S13) Su et al. (2013); (T08) Trilling et al. (2008).
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