We　propose　a　dissipation-engineering　method　for　generation　and　stabilization　of　a　Bell　state　for　two　superconducting　qubits　in　coupled　circuit　quantum　electrodynamics　architecture.　In　the　scheme,　the　large　dispersive　qubit-resonator　interaction　and　resonant　photon　hopping　between　resonators　jointly　induce　asymmetric　energy　gaps　in　the　dressed　state　subspaces　for　the　qubits　and　the　collective　resonator　photon　modes.　The　target　steady　state　is　reached　and　protected　by　applying　each　qubit　with　two　microwave　drives,　that　perturbatively　induce　the　specific　dressed　state　transition,　while　simultaneously　by　employing　the　decay　of　the　collective　photon　modes.　Numerical　simulation　verifies　that　high-fidelity　and　long-lived　two-qubit　Bell　state　can　be　obtained　(based　on　the　recently　available　experimental　parameters)　and　is　robust　against　the　potential　fluctuation　of　the　system　parameters.