for optimal photon storage times. A second device (II) fabricated with a transmon qubit at each end of the resonator [see Fig. 1(c)] was used for all further experiments. This device has
the energy and angular dependence of the cross sections for the production of various particles by two-photon annihilation processes in e+e¡ and e¡e¡ colliding beams. For beam energy E of
well isolated for optimal photon storage times. A second device (II) fabricated with a transmon qubit at each end of the resonator (see Fig. 1c) was used for all further experiments. This
We report a series of p-functionalized phenylbenzoxazoles that offer remarkable energy storage, exceeding 300 J gā1, for the first time among intermolecular cycloaddition-based molecular
energy storage and on-demand energy delivery.26,27 The lowest lying absorption band of FvRu 2 is centered close to 400 nm and tails into the visible region of the solar spectrum, whereas the
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