  Thermal Pulse (LTP) stellar evolution models experience a helium pulse that
occurs following Asymptotic Giant Branch (AGB) departure and causes a rapid
looping evolution in the HR Diagram between the Asymptotic Giant Branch (AGB)
and Planetary Nebula phase (PN). The transient LTP phases only last decades to
centuries while increasing and decreasing in temperature, luminosity, and size
over orders of magnitude. LTP objects have often been described in the context
of their more dramatic counterparts, very late thermal pulses (VLTP). LTP stars
do not evolve as quickly and do not become as hydrogen deficient as VLTP
objects. They do not become conspicuous until after resembling a Planetary
Nebula for thousands of years. We present stellar evolution calculations from
the AGB to the PN phase for models over a range of metallicities from, Z =
0.0015 through Z = 0.03, and for masses 0.90 $M_\odot$, 1.2 $M_\odot$, and 2.0
$M_\odot$. We focus in on our most dense series (1.2 $M_\odot$, Z = 0.015) and
designate a stratification of late thermal pulse types based on at what
temperature they erupt, which may hint at the progenitor mass. We discuss one
type that fits neither a LTP nor VLTP, which may offer an explanation for the
star FG Sge. We present the timescales during which LTP models heat up until
they reach peak helium burning luminosity, during the rapid luminosity decline,
and during the period of cooling and brightening, and we briefly discuss four
LTP candidates.
