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... Majorana fermions. Ideal probes of these excitations are inelastic neutron scattering experiments. These we report here for a ruthenium-based material, α-RuCl3, continuing a major search (so far concentrated on iridium materials) for realizations of the celebrated Kitaev honeycomb topological QSL. O ...
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... The obtainable spin squeezing improves with the quality of the resonator and the number of atoms. Fig. 4 shows the calculated spin squeezing for a typical atom number (N=2×104) and varying finesse of the resonator. Note that we obtain excellent agreement between the calculation [23] and the experime ...
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... Shouldn’t 2 be right? You don’t need to get the details of atomic dynamics remotely right to understand why the air in the room is uniform, or understand why metals form at low temperature. We then need a general, thermodynamic type argument. Also, phenomenology predictions, low energy symmetry shou ...
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... On the LHS of the barrier, the particle is free. The waveform for free particles is  1 x   AeiK x  Be iK x The part of the wavefunctionA is interpreted as a wave incident on the barrier. B is the wave reflected. The squared-amplitude of intensity of the reflected wave relative to the incident ...
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... lead isotopes. Later experiments made by others, again using lead, were also unable to detect an effect of atomic mass on transition temperature Tc. However with the development of nuclear reactors after World War II, it became possible to make artificial isotopes in sizeable quantities and in turn ...
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... experiment. It then looks at nature on a quantum scale by investigating the behaviour of electrons in the double-slit experiment. This experiment yields results that defy classical thinking. Electrons leave the source as particles and strike the detection screen as particles, producing small localiz ...
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Quantum tunnelling

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