to Ref. fix

src/hops_tweak.tex

@@ -375,7 +375,7 @@ Some basic experimentation has shown, that the cutoff parameter has to
 be tuned and is not universally valid which is in accord with the
 findings of~\cite{RichardDiss}.
 
-Similarly to~\cite{Shi2009Feb}, a dynamic truncation scheme could also
+Similarly to \refcite{Shi2009Feb}, a dynamic truncation scheme could also
 be implemented.
 
 \section{Some Mathematical Details}

src/thermo.tex

@@ -804,7 +804,7 @@ baths, that a definition of heat involving any nonzero fraction of the
 interaction energy will lead to the internal energy (as defined by the
 first law) not being an exact differential.
 
-In contrast to~\cite{Strasberg2021Aug}, no interpretation in terms of
+In contrast to \refcite{Strasberg2021Aug}, no interpretation in terms of
 thermodynamical quantities is required for \cref{eq:secondlaw_cyclic}
 to be useful.  Assume that the interaction Hamiltonian in
 \cref{eq:katoineqsys} attains the same value periodically, so that
@@ -857,7 +857,7 @@ with periodically modulated system and coupling
   a_k^†) + ∑_k ω_k a_k^\dag a_k,
 \end{equation}
 where \(λ,Δ\geq 0\) and \(f\in \{x, y, z\}\). The form of the system
-Hamiltonian has been chosen similar to~\cite{Mukherjee2020Jan} where
+Hamiltonian has been chosen similar to \refcite{Mukherjee2020Jan} where
 Floquet theory was used, and it was shown that the relevant quantities
 are scaling with \(λ\). For \(λ=0\) the system Hamiltonian is positive
 semi-definite with the energies zero and one.  The modulation of the