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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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esponding chromospheric network defined by<br />

bright emission in Ca K spectroheliograms.<br />

Neupert effect Statement that the temporal<br />

derivative of the observed soft X-ray emission<br />

during a solar flare reproduces the observed time<br />

development of the hard X-ray emission. This<br />

is found in many flares <strong>and</strong> indicates that a single<br />

energization process is responsible for the<br />

production of both the non-thermal <strong>and</strong> thermal<br />

radiation.<br />

neutral equilibrium In mechanics, a configuration<br />

in which the system experiences no net<br />

force (equilibrium), <strong>and</strong> if the system is moved<br />

slightly from this state, no forces arise, so a<br />

nearby configuration is also an equilibrium. The<br />

paradigm is a ball on a smooth horizontal surface.<br />

See stable equilibrium, unstable equilibrium.<br />

neutral point In electromagnetism, a point<br />

in a magnetic configuration in which the field<br />

intensity B drops to zero, <strong>and</strong> where therefore<br />

the direction of the magnetic field is undefined.<br />

Exp<strong>and</strong>ing the field B around an isolated neutral<br />

point gives B = B0 + r ·∇B0 in the immediate<br />

neighborhood of the point, with subscript zero<br />

marking values at the point. Since B0 = 0, the<br />

constant dyadic ∇B0 determines the character<br />

of the field. In an “x-type neutral point,” ∇B0<br />

has three real characteristic roots <strong>and</strong> three field<br />

lines cross at the point, giving a configuration<br />

like the letter “x” but usually an intricate smallscale<br />

geometry. In an “o-type neutral point”<br />

∇B0 has just one real root <strong>and</strong> the point is the<br />

limiting point of nested closed field lines.<br />

Neutral lines of x-type <strong>and</strong> o-type form<br />

in two-dimensional geometries (extending unchanged<br />

in the third dimension), where the number<br />

of real roots is 2 or 0. The nearby field lines<br />

either form an x-shaped pattern outlined by the<br />

eigenvectors of ∇B0, or form nested o-shaped<br />

loops.<br />

Neutral points are of great interest in space<br />

plasma physics because theory associates them<br />

with magnetic reconnection. The polar cusps<br />

of the Earth magnetosphere are also evolved (xtype)<br />

neutral points.<br />

In atmospheric physics, the points where the<br />

degree of polarization of sky diffuse radiation<br />

© 2001 by CRC Press LLC<br />

neutrino annihilation<br />

equals zero. Due to aerosol scattering, multiple<br />

scattering <strong>and</strong> reflecting from surfaces, polarization<br />

of sky light is not consistent with the<br />

ideal status; there will be some abnormal neutral<br />

points. According to Rayleigh scattering theory,<br />

under ideal conditions the solar point (the direction<br />

of solar incident ray) <strong>and</strong> anti-solar point<br />

are neutral points. In the real atmosphere, in<br />

general, there are three neutral points: Arago<br />

neutral point, which locates about 15 ◦ to 25 ◦<br />

above the anti-solar point; Babinet neutral point,<br />

which locates about 12 ◦ to 25 ◦ above the sun;<br />

<strong>and</strong> Brewster neutral point, which locates about<br />

15 ◦ to 25 ◦ below the sun. All these angles <strong>and</strong><br />

positions may change due to the variations of the<br />

position of sun, the atmospheric turbidity <strong>and</strong><br />

the reflective properties of the Earth surface.<br />

neutral stability In meteorology, the stratification<br />

status when the lapse rate of air temperature<br />

(γ ) equals its adiabatic lapse rate (γd).<br />

neutrino A stable elementary particle which<br />

carries zero electric charge, angular momentum<br />

of 1 2 ¯h, little or no mass, but finite momentum<br />

<strong>and</strong> energy. Invented by Pauli in the<br />

1930s to make energy, momentum, <strong>and</strong> angular<br />

momentum conservation hold in weak nuclear<br />

decays, the electron neutrino was identified in<br />

the laboratory by Cowan <strong>and</strong> Reines in 1953.<br />

Two additional types, called the µ <strong>and</strong> τ neutrinos<br />

(for the other particles co-produced with<br />

them), have been found since. Each has an antiparticle,<br />

leading to a total of six types. In astrophysics,<br />

electron neutrinos are produced in<br />

stellar nuclear reactions, including the protonproton<br />

chain <strong>and</strong> CNO cycle. All three types<br />

are produced by Type II Supernovae, <strong>and</strong> there<br />

should be a thermal sea of all types left from<br />

the early universe, corresponding to the cosmic<br />

microwave background radiation. Solar neutrinos<br />

<strong>and</strong> those from one supernova, 1987A, have<br />

been observed in laboratory detectors.<br />

neutrino annihilation In core-collapse supernovae<br />

<strong>and</strong> gamma-ray burst models, the<br />

number density of neutrinos <strong>and</strong> anti-neutrinos<br />

can become large, <strong>and</strong> the rate of their annihilation<br />

<strong>and</strong> production of electron/positron pairs<br />

<strong>and</strong> photons can be an important part of the<br />

explosion energy. However, the annihilation<br />

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