Pratyusava Baral

Career Stage
Student (postgraduate)
Poster Abstract

Compact orbiting binaries like the black hole binary system observed in GW150914 carry large amount of orbital angular momentum. The post-ringdown compact object formed after merger of such a binary configuration has only spin angular momentum, and this results in a large orbital angular momentum excess. One significant possibility is that the gravitational waves generated by the system carry away this excess orbital angular momentum. An estimate of this excess is made. Arguing that plane gravitational waves cannot possibly carry any orbital angular momentum, a case is made in this paper for gravitational wave beams carrying orbital angular momentum, akin to optical beams. Restricting to certain specific beam-configurations, we predict that such beams may produce a new type of strain, in addition to the longitudinal strains measured at aLIGO. Current constraints on post-ringdown spins, derived within the plane-wave approximation of gravitational waves, therefore stand to improve.

Plain text summary
The Laser Interferometer Gravitational-Wave Observatory (LIGO)-Virgo collaboration has detected gravitational waves (GWs) from the last few orbits before merger of two compact objects (black holes/neutron stars) of nearly equal mass (∼10 – 100 solar masses). Binary black holes in orbit loose energy thereby coming close to each other and ultimately merge. This process also involves a large amount of orbital angular momentum (OAM) loss. Thus gravitational waves (GWs) not only carry energy but also radiated orbital angular momentum. Had the Earth lost orbital angular momentum at the rate of OAM loss at a typical LIGO-Virgo event; it would collide with the sun in 1 ms !!

For detection of these gravitational events, the plane wave approximation is widely used. Unfortunately, this approximation throws away any information regarding angular momentum. In plane waves, the direction of momentum transfer (direction of Poynting vector) is parallel to the direction of propagation and thus carries no angular momentum. More specifically the total orbital angular momentum is proportional to ʃ(x^i k^j – x^jk^i) d^3x which is zero as d^3x is a rotationally invariant measure while the others are three vector components. Thus in other words, the plane wave approximation throws away information about angular momentum.

This to solve this problem, we need to look for solutions of the linearized vacuum Einstein’s equations which are not plane. To carry angular momentum, a radiation has to have a position dependent polarisation tensor which is equivalent to having a spacetime dependent phase term. Before looking for such solutions one needs to remember that GWs propagate with the speed of light (null) on 4D flat (Minkowskian) spacetime and oscillations are perpendicular to the direction of propagation (transverse). 4D Minkowskian spacetime can be written as a product of a 2D light cone and a 2D flat (Euclidean) surface. The polarization which lies on the Euclidean Surface has to have non-trivial spatial dependence for such a transverse wave to carry angular momentum. Its simple to write down a general solution after this decomposition. We refer to this solution as GW beams. It can be shown that these solutions are analogous to electromagnetic beams used in the field of laser optics.

GWs stretch and contract spacetime thus creating a strain which can be detected by a Michelson-like interferometer. For plane waves strain induced due to a gravitational wave is constant. If we consider a GW beam, strain is not constant or is a function of coordinates. What this means is a circular ring of particles which changes to an ellipse upon the passage of plane waves gets distorted. This distortion from an ellipse shall give a measure of OAM carried by the wave. This in turn shall be helpful in constraining the angular momentum of the source from a new handle thus improving present constraints.

Poster Title
Gravitational waves with orbital angular momentum
Tags
Astrophysics
Theoretical Physics
Url
https://link.springer.com/article/10.1140/epjc/s10052-020-7881-2#citeas