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| The H2 Double-Slit Experiment: Where Quantum and Classical Physics Meet |
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For the first time, an international research team carried out a double-slit experiment in H2, the smallest and simplest molecule. Thomas Young's original experiment in 1803 passed light through two slits cut in a solid thin plate. In the groundbreaking experiment performed at ALS Beamlines 4.0 and 11.0.1, the researchers used electrons instead of light and the nuclei of the hydrogen molecule as the slits. The experiment revealed that only one "observing" electron suffices to induce the emergence of classical properties such as loss of coherence.
Double photoionization of H2. Left: Circularly polarized light comes from the top. All angular distributions are in the plane perpendicular to the photon propagation vector: Φe–mol is the angle of the fast electron's trajectory to the molecular axis; Φe–e is the angle between both electron trajectories. Center: Photoionization by circularly polarized light launches a coherent spherical photoelectron wave at each nucleus of the molecule; the light propagates into the plane. Right: Measured electron angular distribution Φe–mol of the faster electron (E1) from double photoionization of H2 by circularly polarized light. The orientation of the molecule is horizontal. Light propagates into the plane of the figure, the molecule is fixed ±10° within the plane shown, Eϒ = 240 eV, and the energy of the slow electron E2 = 0 to 5 eV, resulting in E1 = 185 to 190 eV.
Present-day single photoionization experiments demonstrate double-slit self-interference for a single particle fully isolated from the classical environment. But if quantum particles were put in contact with the classical world in a controlled manner, at what scale would quantum interference begin to diminish and particles start to behave classically? The team decided to study the double photoionization (complete fragmentation) of H2, creating two repelling protons acting as a double slit, a fast interfering electron, and a second electron behaving as an active or inactive observer. Experiments were performed at two different photon energies: Eϒ = 240 and 160 eV, leaving about 190 and 110 eV to be shared between the two electrons, respectively. At these high photon energies, double photoionization of H2 led in most cases to one fast and one slow electron. The fast electron's energies were 185 to 190 eV; the slow electron’s were 5 eV or less (corresponding to an inactive observer). The interference pattern of the fast electron was conditioned by the presence and velocity of the other: the greater the difference in their speeds, the less their interaction and the more visible the interference patterns. Both electrons were isolated from their surroundings, and quantum coherence prevailed, revealed by the fast electron's wavelike interference pattern at the two protons. However, at high photon-energy levels, the fast electron absorbed almost all the energy of the incident single photon, leaving the system too rapidly for interaction with the slow electron. Yet the slow electron was also ejected from the molecule through the mysterious process of electron–electron correlation. This "secret entanglement" allows two electrons to remain connected even though far apart. The researchers now had what they needed to build their classical/quantum interface.
They choose ionization events where the slow electron had a bit more energy (5–25 eV) allowing it act as the classical environment (an active observer). The quantum system of the fast electron now interacted with the slow electron and began to decohere, its interference pattern disappearing. However, the overall coherence was still hidden in the two electrons' entanglement. The dielectron's wavelength was short enough to still interfere (the sum energy of the two electrons was high enough), and there was no environment to disturb the interference as the two electrons were now combined into one quasiparticle. Thus, interference between the entangled electrons could be reconstructed by graphing their correlated momenta from the angles at which they were ejected. Two waveforms appeared in the graph, either of which could be projected to show an interference pattern. Because the two waveforms were out of phase with each other, when viewed simultaneously, the interference vanished. If the two-electron system is split into its subsystems and one is thought of as the environment of the other, it becomes evident that classical properties such as loss of coherence can emerge even when only four particles are involved. Yet because the two electrons' subsystems are entangled in a tractable way, their quantum coherence can be reconstructed. In solid-state–based quantum computing devices, such electron–electron interaction represents a key challenge as decoherence and loss of information occur on the tiny scale of a single hydrogen molecule. The good news, however, is that, in theory, the information is not completely lost.
Research conducted by D. Akoury, Th. Weber (University Frankfurt, Germany, and Berkeley Lab, U.S.); K. Kreidi, t. Jahnke, A. Staudte, M. Schöffler, N. Neumann, J. Titze, L. Ph. H. Schmidt, A. Czasch, O. Jagutzki, R. A. Costa Fraga, R. E. Grisenti, H. Schmidt-Böcking, R. Dörner (University Frankfurt, Germany); T. Osipov, H. Adaniya, M. H. Prior, A. Belkacem, (Berkeley Lab, CA, U.S.); R. Díez Muiño (Centro de Física de Materiales and Donostia International Physics Center, San Sebastian, Spain); N. A. Cherepkov, S. K. Semenov (State University of Aerospace Instrumentation, St. Petersburg, Russia); P. Ranitovic, C. L. Cocke (Kansas State University, U.S.); J. C. Thompson, A. L. Landers (Auburn University, U.S.) Research funding: Deutsche Forschungsgemeinschaft and by the U. S. Department of Energy, Office of Basic Energy Sciences (BES). Operation of the ALS is supported by BES. |
