Crossover between thermal and quantum noise in the externally-pumped Josephson-junction parametric amplifiers is theoretically followed. Two different approaches are used for the analysis : i. Josephson junction is replaced with its RSJ model with the equilibrium source of fluctuations; ii. microscopic theory of the tunnel junctions is used, which takes into account not only thermal and quantum but also shot noise. Because of inconvenience of the noise temperature T
Nfor the amplifier sensitivity characterization in the quantum limit, we express our results in terms of the figure Θ
Nwhich is essentially the amplifier output noise energy, reduced to its input (in the classical limit,

). For the nondegenerate amplifier, the minimum value of Θ
N. equals hω/2 and is due to quantum noise (zero-point oscillations) in the idle-frequency resonator of the amplifier. For the degenerate amplifier, sensitive to only one quadrature component of the input signal, Θ
Ncan be made much less than the above "quantum limit" even at operation temperatures much higher than

, if the Josephson junction characteristic frequency ω
cis high enough,

. Our analysis of the experimental situatlon shows that the values

can be achieved using two-dimensional arrays of a large number (

) single-tunnel-junction interferometers with low inductances, inductively coupled to a microwave cavity.