In a cycle you usually deal with powers $\dot L $ and $\dot Q$ both being given in $W$ (Watt)
What you want from a cycle is to obtain a power source $\dot L$.
In order to obtain it, you have to degrade some heat power from an hot source to a colder source. The power you can obtain from a thermodynamic cycle, applying power balance, is:
$$\dot L=\dot Q_h -\dot Q_c$$ where h stands for hot and c for cold
The efficiency is defined as the power you can obtain divided for the thermal flux input: $$\eta = \frac{\dot L}{\dot Q_h}$$
Replacing $\dot L$ from the first equation you get $$\eta=1-\frac{\dot Q_c}{\dot Q_h}$$
So, considering a reversible process, for which the thermal energy can be written as $Q=T\delta s$ you get the maximum efficiency (Carnot efficiency): $$\eta _{rev} =1-\frac{T_c}{T_h}$$
In the end you're right, in order to keep the same efficiency you have to keep the same temperature, but what's important is that you have to give a thermal flux to obtain a work flux.