Pis’ma v ZhETF, vol. 111, iss. 10, pp. 707 - 708
© 2020
May 25
Reply to Comment on “Amplitude of waves in the Kelvin-wave cascade”
(Pis’ma v ZhETF 111, 462 (2020))
V. B. Eltsov+1), V. S. L’vov
+Department of Applied Physics, Aalto University, POB 15100, FI-00076 AALTO, Finland
Department of Chemical Physics and Biological Physics, Weizmann Institute of Science, 7610001 Rehovot, Israel
Submitted 14 April 2020
Resubmitted 16 April 2020
Accepted 16 April 2020
This is a Reply to Sonin’s Comment [arXiv preprint arXiv:2003.09912, 2020] on Eltsov and L’vov [Pis’ma
v ZhETF 111, 462 (2020)] in which we provide relation of the energy flux carried by the cascade to the
amplitude of the excited Kelvin waves, important for analysis of future experiments.
DOI: 10.31857/S1234567820100110
In his Comment, Sonin used our paper [1] as an ex-
tude of Kelvin waves. We stress that the target of the ini-
cuse to return to a rather old dispute on the theoretical
tial experiments would be to discriminate between dissi-
models of the Kelvin-wave cascade. This dispute was ini-
pation originating from the Kelvin-wave cascade versus
tiated by the controversy between the Kozik-Svistunov
other dissipation mechanisms like acoustic or tunneling
[2] and the L’vov-Nazarenko [3, 4] energy spectra of the
two-level system damping. Here we hope that our order-
cascade. The discussion also included other contribu-
of-magnitude estimation of the expected amplitudes will
tions [5, 6], in particular from the author of the Com-
be useful as well as pointing out two important parame-
ment, whose arguments were criticized in [7, 8]. Numer-
ters, the energy flux and the starting wave vector of the
ical simulation efforts intended to resolve the contro-
cascade kmin, which preferably should be controlled in
versy were built up as well. The authors of the latest
the experiment independently. The focus of the initial
published numerical works known to us [9, 10] claim
experiments will probably not be on verifying particu-
that their results support the L’vov-Nazarenko spec-
lar models of the cascade. In fact, we agree with the
trum [4], including the numerical prefactor. Remarkably,
author of the Comment that in an experiment which
these calculations were performed using different numer-
probes only the longest energy-containing length scales,
ical approaches (Gross-Pitaevskii formalism in [9] and
the discrimination between different cascade models is
vortex-filament method in [10]). We should say from the
unlikely.
outset that our paper has nothing to contribute to this
We think therefore that our paper [1] should not
extended discussion and its focus is on a different topic.
serve as a reason for reanimating the old debate. Of
Independently of the details of the theoretical mod-
course, we do not have in mind to preclude others
els, the generally accepted picture of quantum turbu-
from continuing discussions, preferably finding new ar-
lence includes the Kelvin-wave cascade as an essential
guments. One interesting development for proponents
component in the low-temperature limit. There is, how-
of other theoretical models of the cascade would be to
ever, no experimental evidence so far for the existence
make alternative predictions for observables in single-
of such cascade. The relevant difficulties are mentioned
vortex dynamics and to suggest possible experimental
both in our paper and in the Comment. With recent
realizations where the difference between cascade mod-
progress in experimental techniques we hope that stud-
els becomes potentially resolvable.
ies of the dynamics of nearly straight vortices, not hin-
dered by the hydrodynamic energy cascade and recon-
1. V. B. Eltsov and V. S. L’vov, Pis’ma v ZhETF 111, 462
nections, will become possible in near future. The pur-
(2020).
pose of our paper is to facilitate interpretation of the
2. E. Kozik and B. Svistunov, Phys. Rev. Lett. 92, 035301
results of such potential experiments by providing a par-
(2004).
ticular relation between the energy flux and the ampli-
3. J. Laurie, V. S. L’vov, S. Nazarenko, and O. Rudenko,
Phys. Rev. B 81, 104526 (2010).
4. V. S. L’vov and S. Nazarenko, Pis’ma v ZhETF 91, 464
1)e-mail: vladimir.eltsov@aalto.fi
(2010).
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9
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V. B. Eltsov, V. S. L’vov
5. W. F. Vinen, J. Phys.: Condens. Matter 17, S3231
8. V. V. Lebedev, V. S. L’vov, and S. V. Nazarenko, J. Low
(2005).
Temp. Phys. 161, 606 (2010).
6. E. B. Sonin, Phys. Rev. B 85, 104516 (2012).
9. G. Krstulovic, Phys. Rev. E 86, 055301 (2012).
7. V. V. Lebedev and V. S. L’vov, J. Low Temp. Phys. 161,
10. A. W. Baggaley and J. Laurie, Phys. Rev. B 89, 014504
548 (2010).
(2014).
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2020