A method for reducing chaotic dynamics in four-dimensional symplectic maps is presented. The method is to reduce certain chaos measures related to the invariants of the tangent map of fixed points. This method is applied to circular accelerators, where chaotic dynamics determines the dynamic aperture, the region of long-time stable orbits. A factor of 3 -4 increase in the phase-space volume of confined trajectories is obtained. [S0031-9007(98)07495-X] 41.85.Ja, 47.20.Ky We present a systematic method for reducing chaos in Hamiltonian systems of 2 1 2 degrees of freedom. Our method is to vary the system parameters so that the invariants of the tangent map at fixed points take on the values they would have at integrability. Our method, applied to accelerators, increased the phase-space volume of stable trajectories by nearly a factor of 4. As these methods are applicable to general 2.5 degrees-of-freedom Hamiltonian systems, they may improve a wide variety of similar systems, such as free-electron lasers and magnetic fusion devices, where chaos limits performance.An accelerator lattice is an example of a Hamiltonian system that is inherently nonlinear [1] and higher dimensional. Courant and Snyder [2] showed that for the linear motion in a lattice of magnetic quadrupoles of alternating polarity there can be confining invariants. For stability with error fields or natural nonlinearities, the tunes (the ratio of the transverse oscillation frequency to the frequency of circulation around the ring) must be far from low-order rationals [3]. For a range of energies to be confined, the chromaticity, or variation of tune with energy, must be reduced so that the tune remains far from low-order rationals over a range of energies. This is accomplished with sextupoles, nonlinear elements. Hence, though alternating gradient focusing is based on a linear concept, for its practical implementation the motion is nonlinear.Unfortunately, nonlinearity can cause the motion to be chaotic, so that particles wander through phase space until they hit the physical aperture, becoming lost. Since the relative strength of nonlinearities decreases as one moves towards the central design orbit, there is a nearby region, the dynamic aperture, of phase space filled with stable, well confined trajectories. Proton storage rings [4] must have sufficient dynamic aperture to operate. Larger dynamic aperture facilitates capture into an electron storage ring [5]. Hence, increasing dynamic aperture is important for both proton and electron rings.Tracking studies are used to assess and improve accelerators. Trajectories are followed for long times (e.g., 10 6 turns) in a computational model to determine the dynamic aperture [6]. These studies are aided by methods for early determination of chaos. Such methods include evalu-ation of Lyapunov exponents [7], numerical calculation of resonance amplitudes [8], and use of normal form computations [9].In this Letter we outline a systematic method for chaos reduction and, hence, dynamic aperture increase. Our...