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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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a statement about why the universe is so homogeneous.<br />

As a solution, a period of rapid expansion<br />

(see inflation) has been advocated that<br />

would have stretched the observed universe out<br />

of a horizon volume at early times.<br />

Big Bang nucleosynthesis The production<br />

of deuterium, 3 He <strong>and</strong> 4 He (the latter to about<br />

25% mass fraction) in the first 500 to 1000 sec<br />

of the early universe. These light isotopes, plus<br />

measurable amounts of 7 Li <strong>and</strong> trace amounts of<br />

elements B, Be, are the result of non-equilibrium<br />

nuclear reactions as the universe cooled to about<br />

10 8 K. Heavierisotopeswereproducedinstellar<br />

nucleosynthesis.<br />

big blue bump A feature in the spectral energy<br />

distribution of active galactic nuclei, dominating<br />

the emission shortwards of 4000 Å <strong>and</strong><br />

in the UV. The shape, luminosity, <strong>and</strong> spectral<br />

extension of the big blue bump are as yet uncertain<br />

since the big blue bump lies mostly in<br />

the unobserved far UV, with maximum emission<br />

probably right below the Lyman limit. Only the<br />

low <strong>and</strong> high energy tails of the big blue bump<br />

have actually been observed. The high energy<br />

end of the big blue bump appears to be for several<br />

objects in the soft X-ray domain, where a<br />

sharp rise toward lower energies, the so-called<br />

“soft X-ray excess” is observed. The current<br />

interpretation of the active galactic nuclei spectral<br />

energy distribution, still highly debated, ascribes<br />

this feature to thermal emission from a<br />

hot accretion disk surrounding a supermassive<br />

black hole. See active galactic nuclei, Lyman<br />

limit.<br />

binaries, X-ray X-ray binaries are close binaries<br />

in which one of the objects is either a<br />

black hole or neutron star, <strong>and</strong> the companion is<br />

either a star with a strong wind or a star overfilling<br />

its Roche-lobe. The material transfers from<br />

the companion to the compact object <strong>and</strong> forms<br />

an accretion disk. The gravitational energy releasedasthematerialaccretesontothediskpowers<br />

the X-ray flux. Two classes of X-ray binaries<br />

exist: low-mass (neutron star) <strong>and</strong> high-mass<br />

(black hole) X-ray binaries. Low-mass X-ray<br />

binaries have companion star masses less than<br />

5M⊙, whereas high-mass X-ray binaries have<br />

more massive companions.<br />

© 2001 by CRC Press LLC<br />

binary star<br />

binary black holes Two black holes orbiting<br />

each other, like stars in a binary system. A binary<br />

system of two black holes may radiate away<br />

significant orbital energy by emission of gravitational<br />

radiation, with efficiency that increases<br />

with the eccentricity of the orbit; orbital energy<br />

loss may lead to orbital decay, with the two black<br />

holes spiraling down toward each other <strong>and</strong> ultimately<br />

coalescing to form a single black hole.<br />

Thereisasyetnodefinitiveevidencefromobservations<br />

of the actual occurrence of binary black<br />

holes. Binary black holes have been invoked to<br />

explain peculiar features of kpc-sized radio jets,<br />

of the photometric light curve of the blazar OJ<br />

287, <strong>and</strong> of rarely observed peculiarities in the<br />

spectral line profiles of active galactic nuclei.<br />

Gravitational wave detectors may provide the<br />

first incontrovertible evidence of merging binary<br />

black holes. See black hole, black hole binary.<br />

binary fraction The fraction of stars in a stellar<br />

association which are binary stars. For many<br />

years it was believed that there were no binary<br />

starsamongPopulationIIstars. However, itnow<br />

seems that there may be no difference in the relative<br />

number of binary stars between groups of<br />

stars of the same age, regardless of whether they<br />

are Population I or Population II.<br />

binary pulsar The pulsar PSR 1913+16,<br />

which is in orbit with another neutron star;<br />

both stars have a mass of approximately 1.4<br />

solar masses. Orbital parameters are extracted<br />

from the almost periodic Doppler shifts of the<br />

pulses from the pulsar. The pulse repetition period<br />

is 59 milliseconds, <strong>and</strong> the orbital period<br />

is 2.79 × 10 4 sec. General relativistic effects,<br />

including periastron advance, are verified, <strong>and</strong><br />

they, along with a general relativistic model of<br />

gravitational radiation from the orbiting neutron<br />

stars (period decrease of −2.4 ×10 −12 ), give excellent<br />

agreement with observations.<br />

binary star Two stars gravitationally bound<br />

together. There are numerous types of binaries<br />

including, among others, the following classes:<br />

Algol, RS Canus Venaticorum, W Ursa Majoris<br />

(see contact binary), β Lyrae, cataclysmic variables.<br />

Some binaries show eclipses as one star<br />

passes in front of the other. In such systems,<br />

the amount of light received as a function of

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