Unfortunately the first answer by benrg is not correct: "$\log m$ qubits" in that sentence does not have to do with "asymptotic complexity" and the reason why floor and ceiling functions are left out is not because of them being equivalent asymptotically (even though they are equivalent asymptotically, it's not the reason why they left those symbols out here).
What is being described is an algorithm, and in step 4 of the algorithm, exactly $\log_2 m$ qubits are needed, not "$\mathcal{O}(\log_2 m)$ qubits" which means $\le C\log_2 m$ qubits for a positive constant $C$ and for sufficiently large $m$.
You can see later in the paper that the "first $\log_2 m$ qubits" are treated one way, and the "last $\log_2 m$ qubits" are treated another way:
"Furthermore, from Eqs.32, we can see that the first logm
qubits are plain (i.e., the maximally mixed state), while the
last logm qubits are obscure due to the secret 𝑟."
They also describe what happens to the "second $\log_2 m$ qubits" elsewhere.
It's just describing a specific number of qubits on which you're doing, for example, a measurement. This indicates that $m$ ought to be a power of 2 in the algorithm. You can read the algorithm in more detail and try it in full for small values of $m$ to get a feel for why that might be.
At the end of the paper they talk about the algorithm needing $\mathcal{O}(\log_2 m)$ qubits, but that's the total number of qubits required, which includes the "first" $\log_2 m$ qubits, the "second" $\log_2 m$ qubits, and the "last" $\log_2 m$ to which they referred. The authors did not forget a "big Oh" when they were talking about what to do to the "first" $\log_2 m$ qubits.