Reply to “Comment on two-mode stability islands around AdS”
In a recent Comment Bizoń and Rostworowski (2014), Bizoń and Rostworowski present a few criticisms of our recent Letter Balasubramanian et al. (2014). In particular, they present three arguments: (1) that their own evolutions of the two-mode initial data we had studied collapse to a black hole around a time whereas we found no collapse for times up to roughly , (2) that our two-timescale framework (TTF) “cannot be even used to infer stability,” and (3) that our “claims about stability islands” may not be correct.
We have studied evolutions of this initial data with resolutions higher than we had originally. As displayed in Fig. 1, we do find that higher resolutions display higher concentrations of energy, but we nevertheless have still not observed collapse to a black hole. We note that our code demonstrates convergence to a unique solution even at the late times in question (i.e., around ). We also emphasize that we have demonstrated that the solution to which our numerical results converge is in fact a solution of the scalar anti–de Sitter (AdS) system we seek to solve. This latter property (consistency) is demonstrated with tests that the constraint residuals and mass loss converge to zero (see our Supplementary Material). And so, while it is possible that the continuum solution does in fact collapse around (and indeed, the work of Deppe (2015) does see collapse in a code for which both convergence and consistency are verified), we cannot confirm this (in time for the publication of Bizoń and Rostworowski (2014)) and hence their claim (1).
However even if collapse does take place at a time , the main claims of our paper still stand. We could not know if collapse occurred after the time which we ran our code, and so collapse for some time soon after was always a possibility. And so if instead collapse occurs at , there is no change to our claims. Within that time one still finds both direct and inverse cascades which is now confirmed by the Comment.
Another important point is that, were we to decrease the initial amplitude , we would certainly observe any possible collapse pushed to times later than .
Regarding their claims (2) and (3), there seems to be some misunderstanding of what we tried to communicate in our Letter. Determining whether some scalar perturbation of AdS with arbitrarily small amplitude collapses to a black hole is not possible with numerical evolutions which require some finite , finite resolution, and finite evolution time .
More particularly regarding their claim (2), we agree that the TTF cannot be used to infer stability beyond times . Indeed, we stressed that we have carried our TTF analysis to so that one can only trust predictions within times scaling as . However, for shorter times, we disagree with the claims of the Comment that our truncation to “does not suffice to capture the dynamics of the turbulent cascade” for 2-mode initial data. As is clear from Fig. 4 of Balasubramanian et al. (2014), the vast majority of the energy remains in the lowest modes of the system during evolution, and the dynamics of these modes (in particular, the recurrence times) are very well-captured by the TTF evolution with . We have clearly stated the limitations of our mode-truncation in the Supplementary Material; in particular, we explained that this leads to the discrepancy with the full numerical GR curve in Fig. 3 of Balasubramanian et al. (2014) because the high- modes are highly peaked about the origin (despite carrying very small amounts of energy). We note that the TTF has been verified in Ref. Craps et al. (2015) and even the authors of the Comment have now used the method Bizoń et al. (2015).
With regard to claim (3), we did not use the phrase “two-mode stability islands” in our Letter. In later work Buchel et al. (2015) we referred to “stability islands,” but in that case we were referring to quasi-periodic solutions.
Their Comment provides independent confirmation of our main claims: (i) the presence of both direct and inverse energy cascades (a fact that was missed in the original perturbative analysis), and (ii) the validity of the TTF.
Acknowledgments: This work was supported by the NSF under grant PHY-1308621 (LIU), NASA under grant NNX13AH01G, NSERC through a Discovery Grant (to A.B. and L.L.) and CIFAR (to L.L.). Research at Perimeter Institute is supported through Industry Canada and by the Province of Ontario through the Ministry of Research & Innovation.
- Bizoń and Rostworowski (2014) P. Bizoń and A. Rostworowski, (2014), at the time of submission, the arXiv submission and the version intended for publication were similar, but not identical., arXiv:1410.2631 [gr-qc] .
- Balasubramanian et al. (2014) V. Balasubramanian, A. Buchel, S. R. Green, L. Lehner, and S. L. Liebling, Phys. Rev. Lett. 113, 071601 (2014), arXiv:1403.6471 [hep-th] .
- Deppe (2015) N. Deppe, Personal communication (2015).
- Craps et al. (2015) B. Craps, O. Evnin, and J. Vanhoof, JHEP 1501, 108 (2015), arXiv:1412.3249 [gr-qc] .
- Bizoń et al. (2015) P. Bizoń, M. Maliborski, and A. Rostworowski, (2015), arXiv:1506.03519 [gr-qc] .
- Buchel et al. (2015) A. Buchel, S. R. Green, L. Lehner, and S. L. Liebling, Phys.Rev. D91, 064026 (2015), arXiv:1412.4761 [gr-qc] .