Manuscript Oai227-A@1 · Oai227-A.tex · section · 7f45f607
Initialization, observables, and convergence
Stage 4: change one hypothesis at a time › Initialization, observables, and convergence · lines 1049–1096
| Proposed change | Mathematical effect | Disposition |
|---|---|---|
| Proposed change | Mathematical effect | Disposition |
| Replace by | The entrance density becomes one from the start. | This removes the quench-selection problem. |
| Keep only stationary convergence | One loses the waiting-time variable and uniform-start selection. | Closer to the stationary companion, not all of 227-01. |
| Drop either named disorder | One no longer compares the two coupling laws. | The universality clause has been weakened. |
| Replace the mean of spin autocorrelations by magnetization autocorrelation | Cross-spin terms are introduced. | A different observable requires its own argument. |
| Average disorder before taking the process law | Random conditional means are replaced by annealed averages. | The claimed non-point limiting law is no longer the same object. |
| Use a mixing-time exponent | Only a distance-to-equilibrium timescale is controlled. | No entrance law or random autocorrelation limit follows. |
| Use a finite time grid only | Between-grid oscillation is uncontrolled without a modulus. | Finite-dimensional information is not automatically functional. |
| Use the finite modulus in Lemma lem:modulus at growing | Its constants grow polynomially with . | It supplies no uniform asymptotic tightness by itself. |