Quoting from linked chapter, there are two points worth addressing
A combination of radio frequency (RF) and static (DC) voltages are
applied to opposite rod pairs to achieve mass separation. The voltages
$\left(V_{\mathrm{dc}}+V_{\mathrm{ac}} \cos (\omega t)\right)$ and
$-\left(V_{\mathrm{dc}}+V_{\mathrm{ac}} \cos (\omega t)\right)$, where
$\omega$ is the frequency of $V_{\mathrm{ac}}$, result in a
two-dimensional quadrupole field of the form $$ \varphi(x,
y)=\left(V_{\mathrm{dc}}+V_{\mathrm{ac}} \cos (\omega
t)\right)\left(x^2-y^2\right) / R_0^2 $$ where $R_0(0.5 \mathrm{~cm})$
is the distance from the $z$ (symmetry) axis to the nearest rod
surface, and $x$ and $y$ are the axes crossing both the $z$ axis and
nearest point of the adjacent rods. Three fixed frequencies were used
over the 2-535 Da mass range of QMS: 3.013 MHz for the mass range 1.5
to 19.5 Da, 1.438 MHz for the range 19.5 to 150.5
Da , and 0.853 for the range 150.5 to 535.5 Da.
The frequencies authors refer to is the frequency ($\omega$) of the radiofrequency alternating voltage in MHz. With given frequency, ions with a range of $m/z$ will be able to pass through the quadrupole with a stable trajectory.
Now coming to your main query, what is meant by range of masses. The authors referring to a certain mass scan mode. This is explained in the next paragraph.
Mass Scan Modes: The SAM flight software is designed to allow the QMS
detectors to sample during any 0.017 sec integration period (IP) any
unit or fractional $\mathrm{m} / \mathrm{z}$ value within the 1.5 to
535.5 Da mass range of the instrument with a resolution of 0.1 Da. 0.003 seconds of deadtime elapse before counts are summed in a
different $m / z$ value. In addition, the RF/DC rod voltages can be
independently and precisely set to transmit a selected range (band) of
$m / z$ values in a single IP.