What is a gravity wave detector measuring?

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Discussion Overview

The discussion revolves around the functioning of gravity wave detectors and the challenges of decoupling the detector's response from the gravitational waves it is intended to measure. Participants explore conceptual analogies and the mechanics of detection, focusing on the implications of common mode rejection and the orientation of detectors relative to wavefronts.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about how a gravity wave detector can be decoupled from the gravitational waves it measures, using an analogy involving a ticking clock and an observer.
  • Another participant suggests that the distance to the clock changes, leading to observable oscillations in time differences, and mentions the use of interferometry for measurement.
  • A different participant argues that a detector must be coupled to what it measures, questioning the premise of decoupling.
  • One participant proposes an analogy involving a laser on a pond and a photon detector, highlighting the challenge of common mode rejection when both the laser and detector are affected by the same wavefront.
  • Another participant suggests that the detector should not focus on whether the laser was moved, but rather on the movement of the detector and nearby objects, proposing a setup with multiple floats to detect relative changes.
  • A later reply indicates understanding of the concept of non-synchronous movement among detectors as a means to detect gravitational waves.

Areas of Agreement / Disagreement

Participants express differing views on the feasibility of decoupling a detector from gravitational waves, with some questioning the premise while others explore analogies to clarify the concept. The discussion remains unresolved regarding the specifics of how detection can be achieved without common mode effects.

Contextual Notes

Participants rely on analogies that may not fully capture the complexities of gravity wave detection. The discussion includes assumptions about the behavior of waves and detectors that are not fully explored or defined.

Grinkle
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I am having trouble understanding how a gravity wave detector can be de-coupled from the wave it is intended to measure.

For the sake of conceptual discussion, if I am eyeballing a ticking clock some distance away and a wavefront hits the clock and say 10 or so waves pass through the clock before the wavefront reaches me, and my eyeball is the detector, what kind of behavior am I on the lookout for from the clock? Since the wavefront reaches my eyeball at the same time as information from the clock that was affected by that same wavefront, (I think so anyway) can I de-couple the wavefront effects on my eyeball from what I am hoping to measure about the clock?
 
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The distance to the clock changes, you could see this as oscillations in the observed time difference between your clock nearby and the distant clock. Those differences are too small for actual clocks, so interferometry is used.
Ideally, waves come in orthogonal to the baseline(s) of the experiment for maximal length changes.
 
Grinkle said:
am having trouble understanding how a gravity wave detector can be de-coupled from the wave it is intended to measure.

A detector that is decoupled from whatever it is trying to measure won't detect anything. In order for any detector to work, it has to be coupled in some way to what it is trying to detect. So I think you might need to reformulate your question.
 
PeterDonis said:
you might need to reformulate your question.

Agreed. I'll attempt an analogy.

If I think of a laser floating on a pond surface and a photon detector floating some distance away watching the laser, then my problem is exampled like so -

The pond waves (gravity waves in my analogy) travel at the same speed as the laser photons so when the laser photons reach the detector, the detector is lifted by the same wavefront that lifted the laser, so the detector can't tell the laser was moved by the wave because it was also moved by exactly the same wavefront in exactly the same manner when its detecting the laser's photons. I am seeing common mode rejection, I think, anytime I try to figure out how gravity wave detection might work.

I don't see how the photon detector can be placed out of the way of the gravity-wave wavefront.

What am I missing? Is there some gravity wave that is planar rather than traveling spherically in all three space dimensions so a detector can be "out of the way" of the wave? Or maybe the wave is asymmetric and this asymmetry leaves some non-common signal?
 
Grinkle said:
The pond waves (gravity waves in my analogy) travel at the same speed as the laser photons so when the laser photons reach the detector, the detector is lifted by the same wavefront that lifted the laser

This just means you are detecting the waves the wrong way; you're trying to use a detector that's oriented along the wave direction, instead of perpendicular to it. See below.

Grinkle said:
the detector can't tell the laser was moved by the wave

The detector shouldn't be trying to tell whether the laser was moved by the wave. It should be trying to tell whether the detector itself, and objects near it, were moved by the wave.

Try it this way: we have a bunch of floats that each have a laser and a detector mounted on them. As the wave passes by, the floats move up and down. But if we've been smart about how we place them, they won't all move in sync, so each one will be able to detect changes in the distance and direction of the others, relative to it. These changes will be evidence of the passage of the wave.
 
PeterDonis said:
they won't all move in sync

I get it.

Thanks!
 

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