We introduce a method for breaking Lorentz reciprocity based upon the non-commutation of frequency conversion and delay. The method requires no magnetic materials or resonant physics, allowing for the design of scalable and broadband non-reciprocal circuits. With this approach, two types of gyrators -universal building blocks for linear, non-reciprocal circuits -are constructed. Using one of these gyrators, we create a circulator with > 15 dB of isolation across the 5 − 9 GHz band. Our designs may be readily extended to any platform with suitable frequency conversion elements, including semiconducting devices for telecommunication or an on-chip superconducting implementation for quantum information processing.Lorentz reciprocity follows from Maxwell's equations, and places strong physical constraints on the operation of electromagnetic devices and networks [1]. In the case where propagating fields, entering through ports as guided modes, are scattered by a closed network, Lorentz reciprocity implies that the scattering between a pair of ports is invariant upon exchange of the source and detector [2,3]. In other words, fields flow backward through the network as easily as they flow forward. When directional scattering is required, such as the ubiquitous case of unidirectional information flow in a communication network, the reciprocity theorem must be broken by violating one of its assumptions.Typical non-reciprocal elements such as microwave circulators and optical isolators rely on ferromagnetic effects, which are odd under time-reversal, to break Lorentz reciprocity. This approach, however, is incompatible with some desirable chip-based technologies. For instance, ferrite circulators cannot be integrated with superconducting qubits and circuits, and Faraday isolators cannot be miniaturized for integration with onchip photonics. A broad experimental effort has therefore emerged to develop alternative non-reciprocal devices, including approaches based on: nonlinear materials [4,5], quantum Hall physics [6][7][8][9], and active modulation [10][11][12][13][14][15][16][17][18][19][20][21][22].Many active circuits realize non-reciprocity with parametric coupling between resonant modes [21,[23][24][25][26][27][28][29][30]. The parametric interaction creates a frequency conversion process, illustrated in Fig. 1a. Time-dependence of a system parameter is the fundamental source of the nonreciprocity: the phase of parametric modulation provides a gauge freedom [31][32][33] and imprints a non-reciprocal phase shift on the frequency-converted signals. However, such approaches have been limited in bandwidth to a small fraction of the operating frequency, constrained by the linewidths of the coupled resonant modes.In this Letter, we propose and demonstrate an alternative method for breaking reciprocity, based upon the noncommutation of frequency conversion and delay. This approach requires no resonant physics, and allows for the design of broadband circuits, in which the bandwidth is comparable to the operating frequency. We...