A Universal 1 → 2 Cloner is proposed using cavity QED. This is a deterministic proposal that takes far less steps than previous models, and makes use of dispersive C-NOT gates.It is not possible to produce an exact copy of a quantum state. This dramatic result was embodied in the paper by Wooters andŻurek, and is usually referred to as the No Cloning Theorem [1]. This theorem is an unexpected quantum effect due to the linear superpositions of quantum states, as opposed to classical physics, where the copying process presents no difficulties, and represents the most significant difference between the classical and the quantum information. Thus, an operation like |ψ a |0 b |Q x → |ψ a |ψ b |Q x , is impossible, where |ψ a corresponds to the arbitrary qubit to copy, |0 b is the blank state to be copied on and |Q x , |Q x are the initial and final states of the cloner (the subscripts a, b, x indicate the different spaces for the input qubit, the blank qubit and the cloner respectively).In 1996, Buzek and Hillery suggested that non-perfect copies were possible and proposed the Universal Quantum Cloning Machine (UQCM) [2], that produced two imperfect copies from, say, an original qubit, the quality of which was independent of the input state.The quality of the copying process is measured through the fidelity, that corresponds to the overlap between the quantum state of the copy and the state of an ideal output |ψ ideal (the state of the input qubit). The fidelity is defined as | ψ ideal |ρ copy | ψ ideal |, and can take values between 0 and 1 (1 for a perfect copy). Both copies produced with the 1 → 2 UQCM are identical and have a fidelity of 5/6 for any input state. Later on, in 1998, it was shown that it is the maximum fidelity of a quantum cloning process [3,4].It is possible to generalize the UQCM allowing the existence of a greater number of inputs and outputs. In [4] and [5] the authors show how to implement a cloner that takes N identical input qubits and produces M output copies (with M > N).