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Absence of quantum features in sideband asymmetry
by J.D.P. Machado, Ya.M. Blanter
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Submission summary
Authors (as registered SciPost users): | João Machado |
Submission information | |
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Preprint Link: | scipost_201909_00003v1 (pdf) |
Date submitted: | 2019-09-07 02:00 |
Submitted by: | Machado, João |
Submitted to: | SciPost Physics |
Ontological classification | |
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Academic field: | Physics |
Specialties: |
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Approach: | Theoretical |
Abstract
Sideband asymmetry in cavity optomechanics has been explained by particle creation and annihilation processes, which bestow an amplitude proportional to 'n+1' and 'n' excitations to each of the respective sidebands. We discuss the issues with this interpretation and why a proper quantum description of the measurement should not display such imbalance. Considering the case of linearly coupled resonators, we find that the asymmetry arises from the backaction caused by the probe and the cooling lasers.
Current status:
Reports on this Submission
Report #2 by Anonymous (Referee 2) on 2019-12-22 (Invited Report)
- Cite as: Anonymous, Report on arXiv:scipost_201909_00003v1, delivered 2019-12-22, doi: 10.21468/SciPost.Report.1410
Weaknesses
1 - Inappropriate language
2 - Unclear on subtle aspects of calculations, while asserting that other work is unclear/incorrect
3 - Unconvincing conclusions
Report
Sideband asymmetry in optomechanical systems has been observed in a number of experiments. The origin of this sideband asymmetry has been discussed by a number of authors, and is somewhat subtle, being dependent on the method of detection of scattered radiation. It has been attributed to zero-point fluctuations of the mechanical or electromagnetic modes, or due to correlation between backaction noise and the imprecision noise of the detector.
The present paper appears to support the latter interpretation, though in a manner which is rather unconvincing and much less clear than prior work on the subject. Here the asymmetry appears to be attributed to “coincidental” variations in intrinsic system parameters, in a manner which is unlikely to be reproducible across multiple experiments and would be experimentally testable, should anybody be sufficiently motivated.
The spectral densities are defined in an unclear manner, presenting a spurious distinction between the time and frequency domain, where in fact they can be related in a well-defined manner if one is sufficiently careful. This has been done in a number of other places.
While I have not attempted to reproduce the authors’ calculations myself, I am skeptical as to their correctness.
Some specific comments follow:
- The authors claim, using melodramatic and inappropriate language, that the sideband asymmetry has solely been attributed to the mechanical zero-point fluctuations. The authors will find that this is not the case after a quick perusal of the relevant literature; alternative interpretations have been discussed at length.
- The authors assert that Eq (1) is simply asserted to be true, where in fact this expression appears to me to be just an expression proportional to the Fourier transform of the position correlation function of the undamped quantum harmonic oscillator, easily calculated. The full sideband spectrum of an optomechanical system has been calculated in other places, though this is not it.
- The authors undertake some calculations which appear reasonably standard, though I have not followed them through in detail. I expect they are mostly correct, though am suspicious of them in more subtle points where the authors are unclear.
- The crux of this work is their assertion that the calculations in Ref 6 are incorrect. Given this claim, they should directly compare their results with that work and point out the supposed flaw in Ref 6. As it stands, and without having reproduced either calculation in full myself, I find Ref 6 much more clear and convincing.
Report #1 by Anonymous (Referee 1) on 2019-11-4 (Invited Report)
- Cite as: Anonymous, Report on arXiv:scipost_201909_00003v1, delivered 2019-11-04, doi: 10.21468/SciPost.Report.1290
Strengths
Quite generally, I think this manuscript could be a valuable contribution to the field of quantum optomechanics. Indeed, with regards to experiments showing sideband asymmetry, the authors have convinced me that the question of operator ordering has not been given an appropriate level of attention. I found the paper fairly well written, with relevant examples that are placed in the context of prominent experiments. These comparisons are very pointed and will certainly aid in initiating further discussions on this topic.
Weaknesses
As the paper currently stands, I see two minor weaknesses. Both of which could be easily resolved.
First, the details of the calculations in Sec. 3 detract from the overarching message. For example, the list of Fourier components in Sec. 3.1 (Eq. 9-15) does not, in my opinion, provide any additional insight beyond what is said elsewhere. This is also true for Sec. 3.2 (Eq.28-31), which finds a result similar to that obtained in Sec. 3.1 but with a modified susceptibilty. I suspect a more concise version would actually have a stronger impact (with the details moved into the supplemental material).
Second, there is no reference to recent optomechanical experiments that use single photon detection, such as those performed in the laboratories of Oskar Painter and Simon Groblacher. I understand this is an different measurement technique to homodyne and heterodyne, and not necessarily the target of the claims made in this paper. However, that sub-community has borrowed the term "sideband asymmetry" to denote the difference in click rates between the upper and lower sidebands. Furthermore, they reference many of the papers under discussion in this manuscript. I think it would be valuable to broaden the context and directly comment on these experiments.
Report
As a broad field of research, cavity optomechanics has been around for many decades. However, many early experiments where limited to the classical regime since reaching/measuring the quantum level was (and still is) experimentally challenging. As a result, the community identified certain experimental signatures that could be used to distinguish quantum behaviour from classical behaviour. One such signature is the observation of asymmetry in the displacement noise power spectral density.
In the manuscript presented here, the authors present an argument against this convention, claiming that this particular experimental signature (sideband asymmetry) is an artifact of the decision to use a particular operator ordering. Indeed, I agree with the authors claim that, in contrasting quantum from classical behaviour, one needs to carefully consider the form of measurement being performed (in addition to the physical system itself).
If this paper is published it would hopefully initiate further discussions. Those discussions may, or may not, fall in favour of the claims made here; eitherway I think it's conversation worth having.
I recommend its publication in SciPost
Requested changes
As per earlier suggestions;
1-Condense theoretical section.
2-Add discussion on photon counting experiments.
Author: João Machado on 2020-01-09 [id 702]
(in reply to Report 1 on 2019-11-04)
We thank referee 1 for his valuable feedback.
The referee says "First, the details of the calculations in Sec. 3 detract from the overarching message. For example, the list of Fourier components in Sec. 3.1 (Eq. 9-15) does not, in my opinion, provide any additional insight beyond what is said elsewhere. This is also true for Sec. 3.2 (Eq.28-31), which finds a result similar to that obtained in Sec. 3.1 but with a modified susceptibility. I suspect a more concise version would actually have a stronger impact (with the details moved into the supplemental material)."
Our reply: We fully agree with the referee and we have implemented his suggestions. For a description of the new structure of the manuscript, see the list of changes.
The referee says "Second, there is no reference to recent optomechanical experiments that use single photon detection, such as those performed in the laboratories of Oskar Painter and Simon Groblacher. I understand this is an different measurement technique to homodyne and heterodyne, and not necessarily the target of the claims made in this paper. However, that sub-community has borrowed the term "sideband asymmetry" to denote the difference in click rates between the upper and lower sidebands. Furthermore, they reference many of the papers under discussion in this manuscript. I think it would be valuable to broaden the context and directly comment on these experiments."
Our reply: We agree with the referee that the aforementioned single photon detection experiments should be mentioned. However, as the referee is aware, these experiments are not equivalent to the homo-/heterodyne detection considered in our manuscript, and we fear that an extended discussion of single-photon detection is beyond the scope of our manuscript and that it would harm the conciseness and focus we intended to achieve. We have thus briefly discuss them in the manuscript and enlightened the differences. For the additional discussion, see the list of changes.
Author: João Machado on 2020-01-09 [id 701]
(in reply to Report 2 on 2019-12-22)The referee presents unsubstantiated and rather vague criticism of our manuscript, which is largely based on arguments against statements not present in our manuscript and seemingly personal bias. We urge the referee to read the manuscript thoroughly and elaborate a report that reflects higher scientific standards. Particularly, the referee should pay attention to two major issues: the real goal of the manuscript, which is to show that backaction is responsible for sideband asymmetry; and careless attacks on the validity of the present work.
Regarding the latter, the referee states that "While I have not attempted to reproduce the authors’ calculations myself, I am skeptical as to their correctness.", " As it stands, and without having reproduced either calculation in full myself, I find Ref 6 much more clear and convincing." and "The authors undertake some calculations which appear reasonably standard, though I have not followed them through in detail. I expect they are mostly correct, though am suspicious of them in more subtle points where the authors are unclear.".
The referee repeatedly dismisses our findings, and yet is unable to point to any precise instance where the referee believes that we are wrong or unclear. We find that such statements lack any scientific basis and preclude all healthy scientific discussion. Further, the statements made by the referee that the referee has not attempted to reproduce nor follow our work in detail while judging it as unsound, constitutes a poor scientific practice. If the referee has spotted any mistake or flaw in our work, the referee should point what and where exactly the error is, for which we would be considerably grateful. The same holds for the points where the referee believes to be unclear.
Regarding the purpose of the article, this is repeatedly stated throughout the manuscript:
» abstract-'we find that the asymmetry arises from the backaction caused by the probe and the cooling lasers';
» introduction, end of page 2: 'we show that ZPM does not contribute to the asymmetry and that SA naturally arises from the backaction between the cavity and the mechanical oscillator';
» end of subsection 3.1, page 7: 'As backaction already occurs at the classical level, Eq.(23) shows a classical origin for SA.';
» end of subsection 3.2, page 8: '... backaction leads to an asymmetry in the spectrum.";
» conclusion, beginning of page 9: ' we have shown that SA arises from the backaction caused by the laser drive, and that no ZPM contributes to the asymmetry';
» conclusion, end of page 9: 'We stress once more that there are no quantum features in SA. For a linear system, the noise response function is identical in both classical and quantum descriptions, and as Stokes and anti-Stokes processes provide different amplitudes for the sidebands, an asymmetry naturally emerges.'
Nevertheless, the referee insists on contradictory views about our manuscript, none of which has any solid anchoring in our manuscript:
"The crux of this work is their assertion that the calculations in Ref 6 are incorrect." - The purpose of our manuscript was not to assert that Ref.6 was wrong. We believe that Ref.6 contains a mistake, and we mention it once in the body of the manuscript. Nevertheless, the emphasis given by the referee on Ref.6 does not reflect its importance to our present manuscript, nor does Ref. 6 stand out from the other references. We thus find that the insistence of the referee with Ref.6 is not due to any scientific reason.
"Sideband asymmetry ... has been attributed to zero-point fluctuations of the mechanical or electromagnetic modes, or due to correlation between backaction noise and the imprecision noise of the detector.
The present paper appears to support the latter interpretation" - There is no statement present in the paper that supports such interpretation.
Reply to the referee's remaining concerns:
"The spectral densities are defined in an unclear manner, presenting a spurious distinction between the time and frequency domain, where in fact they can be related in a well-defined manner if one is sufficiently careful. This has been done in a number of other places." - There are 2 issues to be addressed here:
»1st: we do not understand what precisely is unclear to the referee. None of the spectral densities present in the article are new, and they have been defined before elsewhere. Further, we always work in the frequency domain, so we do not understand what exactly the referee means with " spurious distinction between the time and frequency domain". We ask the referee to point to specific equations or sentences which the referee believes to be unclear, so that we can provide a proper answer.
»2nd: the referee seems to suggest that defining spectral densities in a quantum context is a matter of meticulosity. This is simply not true, and the issues associated with defining quantum spectral densities are already known from the literature (for a good review on the subject, see J.D. Cresser, Phys. Rep. 94, 47 (1983))
Related to this later issue, the referee states:
"The authors assert that Eq (1) is simply asserted to be true, where in fact this expression appears to me to be just an expression proportional to the Fourier transform of the position correlation function of the undamped quantum harmonic oscillator, easily calculated."
Our reply: The referee seems to have overlooked an entire section (Section 2) discussing the issues with the aforementioned spectral density (pages 3 & 4 of our manuscript). Further, the "easily calculated Fourier transform of the position correlation function of the undamped quantum harmonic oscillator" is not as well-defined as the referee seems to believe (once again, see J.D. Cresser, Phys. Rep. 94, 47 (1983)).
And at last, the referee states:
"The authors claim ... that the sideband asymmetry has solely been attributed to the mechanical zero-point fluctuations."
Our reply: We do not make such claim. Once the referee reads our manuscript carefully, the referee will find that we discuss other interpretations of sideband asymmetry as well:
»'Alternative interpretations and explanations such as interference between different noise channels [6,15] and laser phase noise [16] have been discovered': page 2 of our manuscript
»'The interpretation of SA differs for different operator orders (arising from different detector models' - page 2 of our manuscript
Further, the referee's comments about Ref.6 answered above contradict the referee's own statement.