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NASA's Beyond Einstein Program: An Architecture for Implementation (2007)
Space Studies Board (SSB)
Board on Physics and Astronomy (BPA)

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Nasa ’s Beyond Einstein Program: An Architecture for Implementation

TABLE 2.24 Laser Interferometer Space Antenna (LISA): Broader Science Examples

Program

Program Characteristics

Program Significance

Galactic compact binaries

Science question

What is the distribution of binary systems of white dwarfs and neutron stars in our Galaxy?

Could provide a census of compact binary systems not achievable by electromagnetic means, and could survey the systems that are progenitors of high-frequency gravitational-wave sources detectable by ground-based interferometers. Population statistics could improve models of binary stellar evolution.

 

Measurements

Sinusoidal gravitational waveforms

 

 

Quantities determined

Orbital frequencies, sky distribution

 

LISA will also be able to test the nature of the gravitational waves and test specific alternative theories to general relativity. Using massive-black-hole inspiral data, LISA will be able to measure any hypothetical difference in the speeds of gravitational waves and of light with a precision of parts in 1017 and test whether or not the “graviton,” the putative quantum particle of gravity, has a mass.66 Because the LISA spacecraft orbit the Sun, they will be sensitive to different mixtures of the polarization modes in the waves from a sufficiently longlasting source and may be able to test whether the general relativistic prediction of only two transverse quadrupolar modes is correct. These would constitute tests of Einstein’s theory in an entirely new regime.

Because binary black hole inspirals are controlled by a relatively small number of parameters, such as mass, spin, and orbital eccentricity, they are good candidates for standard candles.67 They are good candidates because the frequency and frequency evolution of the waves are determined only by the system’s parameters, while the wave amplitude depends on those same parameters and on the luminosity distance to the source. No complex calibrations are needed. Matched filtering analyses have shown that, for nearly circular inspirals, LISA could measure luminosity distances to a few percent at redshift 2 and to tens of percent at z = 10. At the same time, because of the changing orientation of the LISA array with respect to the source, it can also determine the orientation, with precision of better than a degree for massive inspirals at z = 1. If this angular and distance resolution were enough to link a LISA event with a corresponding electromagnetic event in a host galaxy or quasar and thereby to yield a redshift, LISA would contribute a direct, absolute calibration of the cosmic distance scale (Hubble diagram) that relies only on fundamental physics rather than on the complex chain of largely empirical distance ladders on which researchers rely at present. A 2 percent measurement of distance combined with a redshift at z = 1 would give a 2 percent measurement of the dark energy parameter w. The combination of several such measurements could give a dark energy bound that begins to be competitive with JDEM. The main challenge will be in using LISA’s angular resolution to identify the host galaxy.

Contributions to Other Science

Because of the apparent close connection between galactic center black holes and the structure of their host galaxies, information on the formation and growth of massive black holes over cosmic time will feed into models of galactic formation and evolution. The study of EMRIs using coordinated gravitational-wave and electromagnetic observations will improve the understanding of the stars and gas in the close vicinity of galactic black holes. Within our own Galaxy, LISA will measure the orbits and determine the locations of up to 10,000 close binary systems consisting mainly of white dwarfs; as such systems are the precursors of Type Ia supernovas and millisecond pulsars, such a census will aid in understanding the evolution of such systems (see Table 2.24 for a summary).

66

C.M. Will, 1998, Bounding the mass of the graviton using gravitational-wave observations of inspiralling compact binaries, Phys. Rev. D 57:2061-2068.

67

B.F. Schutz, 1986, Determining the Hubble constant from gravitational wave observations, Nature 323:310-311.

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