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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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efractory<br />

refractory Material that resists heat, or in geology,<br />

elements or compounds with high melting<br />

or dissociation temperatures that remain in<br />

formations even after heating. See volatile.<br />

region of anomalous seismic intensity A region<br />

where seismic intensity becomes markedly<br />

intense for the magnitude of an earthquake or for<br />

the epicentral distance. For instance, there are<br />

many cases showing that the Pacific coast from<br />

Hokkaido to Kanto districts in Japan is a region<br />

of anomalous seismic intensity for deep earthquakes<br />

beneath the Japan Sea <strong>and</strong> shallow earthquakes<br />

along the Pacific coast. This is thought<br />

to be because seismic waves, including shortperiod<br />

components, reach the region, passing<br />

through the subducted plate with low attenuation.<br />

In a more typical situation, seismic waves<br />

passing through a high attenuation region away<br />

fromthesubductedplatedonotproducesensible<br />

ground motion. Recent research also suggests<br />

that the existence of a low velocity layer overlying<br />

the subducted plate plays an important role<br />

in producing a region of anomalous seismic intensity.<br />

Regolith The fine powdery surface of an atmosphereless<br />

planet (e.g., the moon) which is<br />

produced by radiation <strong>and</strong> micrometeoric impacts<br />

on the surface.<br />

Regulus 1.38 magnitude star of spectral type<br />

B7 at RA10 h 08 m 22.2 s , dec +11 ◦ 58 ′ 02 ′′ .<br />

Reissner–Nordström (RN) metric In general<br />

relativity, the unique, asymptotically flat<br />

metric describing the spherically symmetric<br />

gravitational <strong>and</strong> electric fields of an isolated<br />

massM with electrical charge.<br />

In spherical coordinates (t,r,θ,φ), the line<br />

element takes the form (in geometric units with<br />

speed of light c = 1, <strong>and</strong> Newton’s constant<br />

G= 1)<br />

ds 2 <br />

= − 1 − 2M<br />

© 2001 by CRC Press LLC<br />

394<br />

r<br />

<br />

+ 1 − 2M<br />

r<br />

Q2<br />

+<br />

r2 <br />

dt 2<br />

+ Q2<br />

r 2<br />

−1<br />

dr 2<br />

<br />

2<br />

+r dθ 2 + sin 2 θdφ 2<br />

,<br />

The electric field is described by a potentialφE<br />

=Q/r.<br />

For Q 2 >M 2 the Reissner–Nordström metric<br />

is regular everywhere except for the real<br />

(naked) singularity at r = 0. For Q 2 ≤M 2 ,<br />

theReissner-Nordströmmetricdescribesablack<br />

hole very similar to the Schwarzschild metric;<br />

there is an inner <strong>and</strong> an outer horizon r± =<br />

M± M 2 −Q 2 instead of just one horizon.<br />

Outside the outer horizon r+ (i.e., for r>r+)<br />

the solution has the expected properties of a<br />

mass <strong>and</strong> charged spherical mass (Region I). For<br />

r−

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