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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 space that is isotropic with respect to all of its<br />

points is also homogeneous, but the converse is<br />

not true. See isotropy, Killing vector.<br />

homologous flares Solar flares that occur<br />

repetitively in the same active region, with essentially<br />

the same position <strong>and</strong> with a common<br />

pattern of development.<br />

homologous temperature (T/Tm) The temperature<br />

(T ), normalized by the “melting temperature”,<br />

Tm.<br />

homothety A one-parameter family of maps<br />

of space-times with the property<br />

Lξgik =σgik .<br />

Here ξ is the generator <strong>and</strong> gik the metric. L<br />

denotes the Lie derivative along the vector ξ.<br />

Homothety isaspecialone-parameterconformal<br />

group when σ is a constant.<br />

homotopy group Mathematical structure<br />

that allows classification of topological defects<br />

formed during phase transitions. Denoting M<br />

as the vacuum manifold, one can define the zeroth<br />

homotopy group π0 as a counter of its disjoint<br />

parts if it is disconnected. For a connected<br />

manifold, it reduces to the identity element.<br />

Inequivalent paths on a plane with a hole. The closed<br />

curves in full line, not encircling the hole, are all equiv-<br />

alent, <strong>and</strong> so are those in dashed line that wind once<br />

around the hole. However, because of the hole, it is<br />

not possible to smoothly transform full line curves into<br />

dashed lines. The first homotopy group of the plane<br />

with a hole is Z, the group of integers, because the<br />

curves can wind an integer a number of times around<br />

the hole, in one way or another (hence there is a pos-<br />

itive or negative sign associated to each curve).<br />

© 2001 by CRC Press LLC<br />

horizontal branch star<br />

The first, or fundamental, homotopy group<br />

π1 counts the inequivalent closed paths on M:<br />

for a plane with a hole for instance, all paths<br />

encircling the hole are said to be equivalent dependingonthenumberoftimestheypassaround<br />

it (see figure). As they can also wind clockwise<br />

or counter-clockwise inequivalently one has, for<br />

a plane with one hole, π1 ∼ Z, the group of integers.<br />

Similarly, one can define the nth homotopy<br />

groupπn of M by means of the inequivalentndimensional<br />

closed hypersurfaces that exist on<br />

M.<br />

The topological defect classification stems<br />

from these homotopy groups: when π0(M) is<br />

non-trivial, then domain walls must form, while<br />

strings, monopoles, <strong>and</strong> textures will exist, respectively,<br />

if π1(M), π2(M), <strong>and</strong> π3(M) are<br />

non-trivial. See cosmic phase transition, cosmic<br />

topological defect, spontaneous symmetry<br />

breaking.<br />

hopper dredge A dredge that includes a hopper<br />

or bin for storage of sediment that will later<br />

be pumped out. Used to remove s<strong>and</strong> from channel<br />

entrances <strong>and</strong> harbors.<br />

horizon On the Earth, or other planet, the distance<br />

at which a line from the viewpoint above<br />

the surface tangentially touches the surface of<br />

the planet. Hence, the maximum distance that<br />

can be seen from that viewpoint. The distance to<br />

the horizon depends on the height of the viewpoint;<br />

for 2 m above sea level the distance on<br />

Earth is approximately 5 km. In general relativity<br />

one defines an event horizon, which bounds<br />

partsofaspacetimewhichcanneverbeobserved<br />

from outside the horizon; <strong>and</strong> particle horizon,<br />

which delimits the boundary visible up to a particular<br />

time at a particular location in space. See<br />

apparenthorizon, blackholehorizon, eventhorizon,<br />

particle horizon.<br />

horizontal branch star A star of low mass<br />

( < ∼ 1.5 solar masses) <strong>and</strong> low heavy-element<br />

content (0.2%) in the evolutionary phase where<br />

the two main sources of energy are helium burning<br />

in the core <strong>and</strong> CNO-cycle hydrogen burning<br />

in a thin shell. The star is about 30 times as<br />

bright as it was on the main sequence, <strong>and</strong> the<br />

phase lasts about 3% as long. The name comes<br />

227

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