Supersymmetries in quantum mechanics offer a way to obtain degeneracies in the excitation spectrum which do not originate from selection rules. The mechanism behind the degeneracies is the same as the one that leads to the miraculous cancellations of divergences in supersymmetric field theories found in the high energy physics context. There is up to now no realistic proposal of nonintegrable systems that show level degeneracies due to a supersymmetric structure. Here, we propose an implementation of a quantum-mechanical supersymmetry in a Cooper-pair box shunted by a Josephson junction rhombus which is effectively π-periodic in the superconducting phase difference. For a characteristic ratio between the strength of the 2π-and the π-periodic junction, we find a two-fold degeneracy of all the energy levels all the way from the weak junction/charge qubit limit to the strong junction/transmon regime. We provide explicit experimental values for the parameters of the system and show that tuning in and out of the supersymmetric point is easily achieved by varying an external gate voltage. We furthermore discuss a microwave experiment to detect the supersymmetry and conclude that it can indeed be implemented with currently existing Josephson junction technology.PACS numbers: 03.67. Ac, 11.30.Pb, 85.25.Cp, 42.50.Pq The macroscopic quantum mechanics of superconducting circuits has allowed the experimental simulation of many complex quantum phenomena such as phase transitions, 1 quantum spins, 2 or dynamics in open systems.3 Theoretically, the quantum simulation of intricate subjects such as Hawking radiation 4 and lattice gauge theories 5-7 has been proposed. In the plethora of phenomena that can be simulated with the help of superconducting circuits, 8,9 degeneracies due to quantummechanical supersymmetries have notably been absent. Typically, degeneracies in the spectrum arise when the Hamiltonian commutes with all group elements of a nonAbelian symmetry which translates into selection rules demanding vanishing off-diagonal and equal diagonal matrix elements of the Hamiltonian within the same irreducible representation.10 The degeneracy of the states thus always follows from the dimension of the representation. Supersymmetry on the other hand does not simply forbid different states to couple but it makes sure that in each order of perturbation theory there is always a pair of terms canceling each other.
11,12It is intriguing that the degeneracies of supersymmetric quantum mechanics occur by the same mechanism 11 that leads to a miraculous cancellation of divergences in supersymmetric field theories and makes supersymmetries an important tool of particle physics.13 In trivial cases like the free particle 14 or the Jaynes-Cummings model, 15 however, the supersymmetric structure is irrelevant since the spectrum is exactly solvable. In order to deepen the connection to the ideas in the high-energy context, it is thus of vital importance to propose a non-integrable system where the level degeneracy can be solely understo...