Dear John, We are relieved to finally resubmit our manuscript ApJL #21952 in slightly modified form with this response. We have addressed these final comments and sincerely hope that our manuscript can be accepted in its current form. Best wishes, Michael Meyer *****************Response to the Referee************************************* We thank the referee for her/his most recent comments. Our responses follow below. In addition to addressing these comments, we have removed the phrase "...broadly consistent with models of terrestrial planet formation and the inferred evolution of our solar system" from the abstract given the complications in comparison our results to currently available models. In addition, we have added one sentence to the last paragraph in section 4: "These results can be compared to the observed frequency of gas giant planets of at least 6.6 \% within 5 AU (and 12 \% when extrapolated out to 20 AU \citet{Marcy05}; see also \citet{Lafreniere07}) and the suggestion that extant Spitzer data are consistent with most stars having debris disks comparable to our solar system \citet{Bryden06}." REFEREE: The weakness in the argument is primarily in the fact that the Kenyon & Bromley terrestrial planet formation models which are being invoked to justify the excess being detectable for a factor ~3 in age actually produce detectable 24micron excesses for much longer than a factor of 3 in age. The reply about the model results only being pertinent to 10 and 20micron excesses is not valid. While 10 and 20micron evolution was plotted in Kenyon & Bromley (2004), Fig. 4 of Kenyon & Bromley (2005) shows the 24micron evolution in which detectable emission is seen for a factor of >100 in age for a range in radii of x2. The long duration of detectable excess is due in part to the scaling of sigma as a^-1.5, but mostly because emission in the Kenyon & Bromley models is not just detected at the "era of maximum dust production", but for a long period afterwards as the small bodies are depleted. RESPONSE: We have attempted to clarify in the text that our estimate for the duration of 24 micron excess emission does not follow solely from the detailed models of Kenyon and Bromley, but more generally from consideration of the evolution of planetesimal swarm. Though we do acknowledge that our basic scaling does assume that we are detecting dust near the era of maximum dust production. Because the models of Kenyon and Bromley predict maximum excesses x5 larger than observed, it is difficult to scale their predicted duration of the 24 micron excess phase. We believe this may be due to the fact that their published models are tracing hotter dust at smaller radii. We have verified with the authors that the results in Figure 4 of Kenyon and Bromley (2005) are comparable to those shown in Figure 3 of Kenyon and Bromley (2004) for disks that range from 0.68-1.32 AU with excess emission indicated at different wavelengths. The model that shows 24 micron excess in Fig 4 (KB05) likely also shows excess at shorter wavelengths at early times due to dust generated by planetesimals at the smaller radii (< 1 AU). As a result the duration of 24 micron excess shown in Fig 4 (KB05) is longer than expected if the models only considered planetesimal belts outside of 1 AU. Such models are not currently available. Because our sources lack excess emission at 8 microns, we conclude that they lack dust producing planetesimals inside of 1 AU. We now state this explicitly in the second paragraph of section 4, and reference Silverstone et al. (2006) in support of this claim. We have also added a footnote explaining the discrepency in timescales: "While the published Kenyon and Bromley models predict excess emission much longer than a factor of $\times$ 3--6, we note that those models also predict hot dust at smaller radii covering a wider range of radii than our observations imply." A fuller discussion of these points awaits more detailed analysis of the dust temperatures as described in paragraph 4 of section 4. REFEREE: I don't think this should prevent the paper being published, since the Kenyon & Bromley models include many assumptions and may not provide an accurate picture of the dust production during terrestrial planet formation. However, this does invalidate the current argument, the wording of which would have to be changed for this to be acceptable. I think the problem is in the sentence "This simple calculation...", since the authors have made a further assumption which needs to be mentioned, which is that 24micron emission is only detectable at the epoch of maximum dust production at each radius. Also, whatever the "simple calculation" is, it does not suggest that the "emission we observe SHOULD not persist" rather that it "MIGHT not persist". And there should be a caveat recognising that 24micron emission actually persists on timescales longer than x3 in age in the Kenyon & Bromley (2005) models. In this form the argument would be still be very weak, but would be sufficient to justify the "Perhaps many stars..." and "Nevertheless, one might consider..." elements of the rest of the argument which leads to summing the excess fractions over all ages. RESPONSE: We have changed "SHOULD" to "MIGHT" as the referee suggests and explicitly mention the discrepency in timescales to which the referee alludes (see response above). We have also included an interpretation that would be robust if the dust production phase lasts up to a factor of x10 in age: "Averaging the results over factors of ten in age results in excess fractions of 18 \% (3--30 Myr) and 12 \% (30--300 Myr) implying that at least 30 \% of sun--like stars exhibit evidence for terrestrial planet formation, provided that the epoch of 24 $\mu$m excess emission lasts $< \times 10$ in age." REFEREE: The same paragraph also equates the "era of maximum dust production" with the transition from orderly to runaway growth. However, in the Kenyon & Bromley models, this era is associated with the growth of planetesimals to 2000km in size, which is not the same thing. RESPONSE: We thank the referee for pointing out the confusion in our description of the Kenyon and Bromley results. Following Kenyon and Bromley (2004, section 3, paragraph 6; see also Kenyon and Bromley 2006, section 3.5 paragraph 2) We now state in paragraph 2 of section 4 that: "Sometime after gas disk dissipation, orderly growth proceeds to runaway growth, transitioning to chaotic growth. Maximum dust production is thought to occur between the latter two phases when the largest planetesimals reach $\sim$ 2000 km at a given radius \citep{Kenyon04,Kenyon06}."