The shape of Fermi contour high-temperature superconductors (HTS) has the i
mportant feature. Namely, the components of hole pair reduced effective mas
s are of opposite sign at the most part of the Fermi contour. As a result,
it is possible a rise of a hole pairing dire to direct Coulomb interaction.
This conception is used to explain the essential distinction between the t
emperature of a pseudogap arising and the temperature of the superconductor
transition in the case of underdoped HTS compounds.