We present a method to experimentally realize large-scale permutation-symmetric Hamiltonians for continuous-time quantum protocols such as quantum walk and adiabatic quantum computation. In particular, the method can be used to perform an encoded continuous-time quantum search on a hypercube graph with 2 n vertices encoded into 2n qubits. We provide details for a realistically achievable implementation in Rydberg atomic systems. Although the method is perturbative, the realization is always achieved at second order in perturbation theory, regardless of the size of the mapped system. This highly efficient mapping provides a natural set of problems which are tractable both numerically and analytically, thereby providing a powerful tool for benchmarking quantum hardware and experimentally investigating the physics of continuous-time quantum protocols.Quantum computing based on continuous time evolution rather than discrete gate operations offers a promising route for practical near-term quantum computing. This approach has a wide variety of natural applications including in finance [1-3], aerospace [4], machine learning [5][6][7], theoretical computer science [8], mathematics [9,10], decoding of communications [11] and computational biology [12]. Moreover, experimental quantum annealing has proven highly successful recently [13][14][15][16][17].While continuous-time quantum computing shows great promise, there are few known methods to experimentally implement test problems that can be used to prove the performance of hardware. For quantum computing based on discrete gates, solving unstructured search by Grover's algorithm [18] provides a quadratic speedup over any classical algorithm-the best possible speedup as proven by Bennett et al. [19]. There are continuous-time variants of quantum search algorithms which can obtain the same optimal speedup for both adiabatic quantum computation [20,21] and continuoustime quantum walk [22]. It has recently been shown that these are the two extremes of a continuum of protocols that all achieve the optimal quantum speedup [23].Continuous-time search algorithms are not easy to experimentally implement when encoded into qubits. In contrast, Grover's original algorithm can be efficiently decomposed into quantum gates [24]. A naive decomposition of the continuous-time search problem yields exponentially many terms coupling all possible subsets of qubits. To date, the largest qubit-encoded continuous-time quantum walks have been performed on two qubits [25,26]; neither implemented a search algorithm. Larger encoded discrete-time quantum walks and quantum searches have been experimentally realized [27,28], and alternative encodings have been explored in [29,30].Because of the difficulty of implementing qubitencoded continuous-time quantum search algorithms, this has been considered a toy problem: useful as a theoretical tool, but not practical experimentally. The search Hamiltonian can always be represented in a permutation symmetric basis, by transforming the marked state to either t...