Resolving the phase of a Dirac topological state via interferometric photoemission
The electronic wavefunction is at the heart of physical phenomena, defining the frontiers of quantum materials research. While the amplitude of the electron wavefunction in crystals can be measured with state-of-the-art probes in unprecedented resolution, its phase has remained largely inaccessible, obscuring rich electronic information. Here we develop a quantum-path electron interferometer based on time- and angle-resolved photoemission spectroscopy, that enables the reconstruction of phase information associated with electronic states, as encoded in the photoemission transition amplitudes - with energy and momentum resolution. We demonstrate the scheme by resolving the phase along the Dirac electronic band of a prototypical topological insulator and observe a resonance-associated phase jump as well as a momentum and phase synchronized inversion revealing the helicity of the Dirac cone. We show the interferometer can be optically controlled by the polarization of the absorbed light, allowing a differential measurement of the phase - a crucial component for extracting phase information from an interferogram. This photo-electron-interferometer provides direct experimental access to the phase of electronic transition amplitudes. Its implementation relies on experimentally accessible conditions - such as the presence of a suitable intermediate state and polarization-selective coupling - and can therefore be extended to a wide class of materials.