One of the most attractive systems for scalable quantum processing is the trapped atom in the optical cavity, which is easily manipulable with lasers. The qubit-cavity system represents an attractive structure for quantum optics, with possibilities for applications in quantum detecting, quantum computation, and quantum communication. Also, the investigation of the cavity-atom system under temperature is a fundamental concept in quantum optics and quantum information science. Here we continue in this quantum way, investigating different qubit(s)-cavity systems (where we increase the numbers of the qubit inside the optical cavity from one to four). Employing the Dicke model, we calculate the cavity ground state occupation probability ⟨â † ˆ a⟩ and the expectation values ⟨Jz⟩ for each system. We find that these probabilities increase when the coupling 1 strength Cs increases. This leads to reaching the ultra-strong coupling regime, which depends on the numbers of the qubits. To describe the quantum state, we examine the cavity Wigner function WF as a function of the coupling strength Cs. Under the same parameters (e.g., Cs and the dissipation rates), we obtain that the separation of the quantum state in the WFs representation is different from one system to another. Furthermore, since understanding these kinds of systems is very important in order to improve the quantum network system, we study the entropy S of the subsystems (like S of qubit) in each system. Also, we move beyond by studying the effect of the temperature on the Fock-state distribution occupation probability and entropy of the subsystems. Our outcomes present another step to understanding the qubit(s)-cavity interaction to improve the performance of the future quantum networks based on this system.