  Identified-hadron (PID) $p_t$ spectra from 13 TeV $p$-$p$ collisions are
compared with a two-component (soft+hard) model (TCM) that accurately
distinguishes jet-related hadron production (hard component) from nonjet
projectile-nucleon dissociation (soft component). The present $p$-$p$ study is
similar to and is guided by recent TCM studies of PID spectra from 5 TeV $p$-Pb
collisions. The combined analyses serve to establish a well-understood
quantitative description of PID hadron production in small collision systems as
a control experiment. The control can then be contrasted with conventional
interpretations of collision data from more-central A-A collisions as
indicating formation of a quark-gluon plasma (QGP). PID $p_t$ spectra from 13
TeV $p$-$p$ collisions exhibit simple consistency with spectra from 5 TeV
$p$-Pb collisions. Hadron species abundances are consistent with
statistical-model trends predicted prior to commencement of the large hadron
collider program. Differential spectrum structure and various ratio measures
are quantitatively explained by the TCM, including its jet contribution, and
admit no room for claims of hydrodynamic flows in small collision systems.
