plasky / OzHF

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Section 2: Design Concept #3

Open plasky opened 4 years ago

plasky commented 4 years ago

Add issues about Section 2 here

Nangush commented 4 years ago

Update Figure 2

ddobie commented 4 years ago
jade-powell commented 4 years ago
plasky commented 4 years ago

Comments from David McClelland

G.L. Mansell, et al “Observation of Squeezed Light in the 2 µm Region”, Phys.Rev.Lett.120, 203603 (2018). M.J. Yap, et al , “Squeezed vacuum control at 2µm”, Optics Letters 44, 5386-5389 (2019).

(In fact when any papers talks about 10dB of squeezing for GW detectors, they should cite M.S. Stefszky, et al “Balanced homodyne detection of optical quantum states at audio-band frequencies and below”, Class.Quant. Grav.29, 145015 (14 pages) (2012).

A-Graham commented 4 years ago
plasky commented 4 years ago
* [ ]  Clarify figure 2b, or caption as appropriate. It should use the _characteristic strain_ of A+,CE, and ET. Design sensitivity typically refers to strain sensitivity of a detector.

@Nangush: can you please clarify what you mean here? The way I understand it, "design sensitivity" refers to the sensitivity of the instrument when it reaches it's final design specifications. You can represent this using the ASD, PSD, noise amplitude, or any other metric that represents a sensitivity curve. In the top panel of figure 2, we use the amplitude spectral density in units of 1/sqrt(Hz), and in the bottom panel we use the dimensionless noise amplitude, which is just \sqrt(f) times the ASD. This is mentioned explicitly in the caption, and I believe the axis labels are also correct. Sorry if I'm missing something, but can you please clarify?

Nangush commented 4 years ago
* [ ]  Clarify figure 2b, or caption as appropriate. It should use the _characteristic strain_ of A+,CE, and ET. Design sensitivity typically refers to strain sensitivity of a detector.

@Nangush: can you please clarify what you mean here? The way I understand it, "design sensitivity" refers to the sensitivity of the instrument when it reaches it's final design specifications. You can represent this using the ASD, PSD, noise amplitude, or any other metric that represents a sensitivity curve. In the top panel of figure 2, we use the amplitude spectral density in units of 1/sqrt(Hz), and in the bottom panel we use the dimensionless noise amplitude, which is just \sqrt(f) times the ASD. This is mentioned explicitly in the caption, and I believe the axis labels are also correct. Sorry if I'm missing something, but can you please clarify?

@plasky Conventionally GW instrumentalists will refer to the strain sensitivity as the design sensitivity of the detector. Calling the characteristic strain the design sensitivity will be confusing to instrumentalists, and conflict with its conventional usage in the literature. You risk instrumentalists misunderstanding that you are comparing the strain sensitivity of A+, CE, and ET with the characteristic strain of OzHF. I feel like this is important because the paper discusses, and compares proposed detectors.

plasky commented 4 years ago

You risk instrumentalists misunderstanding that you are comparing the strain sensitivity of A+, CE, and ET with the characteristic strain of OzHF.

The bottom panel is not doing what you suggest. It's comparing the noise amplitude (ie characteristic strain) of all four detectors (A+, CE, ET, OzHF). i.e., it's an apples and apples comparison in that plot.

plasky commented 4 years ago
* Probably should see if there is a better ref for CE than the Reitze arXiv.  Will get back to you.

Changed to this paper. I think it's the right one to cite, but people should feel free to say otherwise!

PaulEasterMonash commented 4 years ago

Design concept suggestions:

Secondly, high circulating laser-power is required to improve the high-frequency sensitivity. This introduces opto-mechanical instabilities whose control strategies can easily increase the noise in the low-frequency band.

Nangush commented 4 years ago