Hydrodynamical fluctuations of the electron gas comprise low-frequency
and long-range stochastic excitations over a steady state of the syst
em. In this work we develop the theory of hydrodynamic fluctuations in
the nonequilibrium electron gas which can be described by its electro
n temperature. For this case the characteristic spatial-time parameter
s are the electric charge decay time tau(M), the electron temperature
relaxation time tau(T), and two corresponding diffusion lengths L(M) a
nd L(T), respectively. The spectral densities of the fluctuations are
found and investigated for arbitrary relationships between the fluctua
tion frequency omega and times tau(M) and tau(T), for wave vectors q a
nd lengths L(M), L(T). In the first case, we established the effect of
the crossover correlation of the electron density delta n(r,t) and te
mperature delta T(r,t) fluctuations. The cross correlation depends on
omega and changes its sign, which indicates the existence of the frequ
ency range of correlation and anticorrelation of delta n (r,r) and del
ta T(r,t). In the general case, spectral densities of the fluctuations
have non-lorentz form, which also holds with thermal equilibrium, At
the equilibrium the cross-correlation effect leads to only redistribut
ion of the fluctuation intensity over the frequency region. Under none
quilibrium conditions the cross correlation also changes the integral
intensities of the fluctuations and is directly related to additional
kinetic correlation of the hot electrons caused by electron-electron i
nteraction. The results are applied to the calculation of light scatte
ring by electron plasma fluctuations. The cross-correlation effect giv
es the essential contribution to the doss section of the light scatter
ing. It is shown that the additional kinetic correlation of hot electr
ons can be directly measured by means of the light-scattering experime
nt.