Pulsed coherent excitation of a two-level atom strongly coupled to a resonant cavity mode will create a superposition of two coherent states of opposite amplitudes in the field. By choosing proper parameters of interaction time and pulse shape the field after the pulse will be almost disentangled from the atom and can be efficiently outcoupled through cavity decay. The fidelity of the generation approaches unity if the atom-field coupling strength is much larger than the atomic and cavity decay rates. This implies a strong difference between even and odd output photon number counts. Alternatively, the coherence of the two generated field components can be proven by phase-dependent annihilation of the generated nonclassical superposition state by a second pulse. . Recently, it has been noted that such states could also be used in quantum-information processing for encoding qubits in the relative phase of the two classical amplitude [3]. In principle they allow quantum teleportation and linear quantum gates in a straightforward manner [4]. Although nondeterministic sources could be used for these applications it would clearly be more desirable if a controlled deterministic source was available in the optical domain.Nonlinear optical setups, such as, e.g., a subthreshold optical parametric oscillator or electrically induced transparency type interactions in atomic media, have been suggested as possible sources of such states [5]. Alternatively, traveling-wave coherent-superposition states might be generated by sending a three-level atom in a superposition state of the two lower levels through a high-Q cavity, which couples only one of the levels with a third upper state [6]. The desired quantum state is then generated by sending a light pulse through the cavity followed by postselection on the outcome of a subsequent proper projective measurement on the atom. In this way, the microscopic quantum superposition of the atom is transformed to a macroscopic superposition of the light field being transmitted or reflected from the cavity. Although this scheme works well in principle it is slow and hard to implement in practice.Here we propose a significantly simpler version of a cavity QED scheme using just a two-level atom resonantly coupled to a single mode of a high-Q cavity mode with a coupling strength g exceeding the natural linewidth ␥ of the atomic transition and the cavity decay rate (Fig. 1). All that is needed is to apply a coherent driving pulse of proper strength and duration to the atom from the side. The induced Rabi flopping of the atom together with coherent scattering of the pulse light into the cavity mode then generate the desired field state. Interestingly, it is possible to tailor the interaction time in such a way that the atom gets disentangled from the field after the pulse so that no projective measurement on the atom is required. This is a central difference from previous suggestions of using a far-detuned pulse. Such a pulse creates a similar field, but as it induces no atomic transitions it le...