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Magnetic monopoles have provided a rich field of study, leading to a wide area of research in particle physics, solid state physics, ultra-cold gases, superconductors, cosmology, and gauge theory. So far, no true magnetic monopoles were found experimentally. Using the Aharonov-Bohm effect, one of the central results of quantum physics, shows however, that an effective monopole field can be produced. Understanding the effects of such a monopole field on its surroundings is crucial to its observation and provides a better grasp of fundamental physical theory. We realize the diffraction of fast electrons at a magnetic monopole field generated by a nanoscopic magnetized ferromagnetic needle. Previous studies have been limited to theoretical semiclassical optical calculations of the motion of electrons in such a monopole field. Solid state systems like the recently studied spin ice provide a constrained system to study similar fields, but make it impossible to separate the monopole from the material. Free space diffraction helps to understand the dynamics of the electron-monopole system without the complexity of a solid state system. The use of a simple object such as a magnetized needle will allow various areas of physics to use the general dynamical effects of monopole fields without requiring a monopole particle or specific solids which have internal monopole-like properties. The experiment performed here shows that even without a true magnetic monopole particle, the theoretical background on monopoles serves as a basis for experiments and can be applied to efficiently create electron vortices. Various predictions about angular momentum and general field effects can readily be studied using the available equipment. This realization provides insights for the scientific community on how to detect magnetic monopoles in high energy collisions, cosmological processes, or novel materials.
A new static and azimuthally symmetric magnetic monopolelike object, which looks like a Dirac monopole when seen from far away but smoothly changes to a dipole near the monopole position and vanishes at the origin, is discussed. This monopolelike obj
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