  The double-scaled infinite temperature limit of the SYK model has been
conjectured by Rahman and Susskind (RS) [1, 2, 3, 4], and independently by
Verlinde [5] to be dual to a certain low dimensional de Sitter space. In a
recent discussion of this conjecture Narovlansky and Verlinde (NV) [6] came to
conclusions which radically differ from those of RS. In particular these
conclusions disagree by factors which diverge as $N \to \infty$. Among these is
a mismatch between the scaling of boundary entropy and bulk horizon area. In
this note, we point out differences in two key assumptions made by RS and NV
which lead to these mismatches, and explain why we think the RS assumptions are
correct. When the NV assumptions, which we believe are unwarranted, are
replaced by those of RS, the conclusions match both RS and the standard
relation between entropy and area.
  In the process of discussing these, we will shed some light on: the various
notions of temperature that appear in the duality; the relationship between
Hamiltonian energy and bulk mass; and the location of bulk conical defect
states in the spectrum of DSSYK$_{\infty}$.
