Nonlinear Memory Effect

Gravitational memory effects, also known as gravitational-wave memory effects are predicted persistent changes in the relative position of pairs of masses in space due to the passing of a gravitational wave. Detection of gravitational memory effects has been suggested as a way of validating general relativity.

In 2014 Andrew Strominger and Alexander Zhiboedov showed that the formula related to the memory effect is the Fourier transform in time of Weinberg's soft graviton theorem.

Linear and non linear effect

There are two kinds of predicted gravitational memory effects: one based on a linear approximation of Einstein's equations, first proposed in 1974 by the Soviet scientists Yakov Zeldovich and A. G. Polnarev, developed also by Vladimir Braginsky and L. P. Grishchuk, and a non-linear phenomenon known as the non-linear memory effect, which was first proposed in the 1990s by Demetrios Christodoulou.

The non-linear memory effect could be exploited to determine the inclination, with respect to us observers, of the plane on which the two objects that merged and generated the gravitational waves were moving, making the calculation of their distance more precise, since the amplitude of the received wave (what is experimentally measured) depends on the distance of the source and the aforementioned inclination with respect to us.

Gravitational spin memory

In 2016, a new type of memory effect, induced by gravitational waves incident on rays of light moving along circular trajectories perpendicular to the waves, was proposed by Sabrina Gonzalez Pasterski, Strominger and Zhiboedov. This is caused by the angular momentum of the waves themselves and therefore termed gravitational spin memory. As in the previous case, this memory also turns out to be a Fourier transform in time, but, in this case, of the graviton theorem expanded to the subleading term.

Detection

The effect should, in theory, be detectable by recording changes in the distance between pairs of free-falling objects in spacetime before and after the passage of gravitational waves. The proposed LISA detector is expected to detect the memory effect easily. In contrast, detection with the existing LIGO is complicated by two factors. First, LIGO detection targets a higher frequency range than is desirable for detection of memory effects. Secondly, LIGO is not in free-fall, and its parts will drift back to their equilibrium position following the passage of the gravitational waves. However, as thousands of events from LIGO and similar earth-based detectors are recorded and statistically analyzed over the course of several years, the cumulative data may be sufficient to confirm the existence of the gravitational memory effect. A recent proposal aims to detect gravitational waves by monitoring the cumulative memory that accrues over cosmological distances, observable as coherent astrometric deflections.

See also

* Pasterski–Strominger–Zhiboedov triangle

References

External links

Gravitational-wave memory: an overview
by Marc Favata

The gravitational memory effect: what it is and why Stephen and I did not discover it
by Gary Gibbons
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Astronomy
General relativity
Effects of gravity