Table 1. Relaxation times and their relative errors obtained by ESS and QENS.
τ_INPUT/μeV | τ_ESS/μeV | τ_QENS/μeV | Δτ/τ ESS % | Δτ/τ QENS % |
---|---|---|---|---|
5 | 4,918 | 5,250 | −1,637 | 4,990 |
6 | 6,492 | 6,102 | 8,200 | 1,708 |
8 | 8,585 | 8,522 | 7,306 | 6,522 |
10 | 10,136 | 10,404 | 1,355 | 4,038 |
12 | 11,240 | 12,874 | −6,338 | 7,284 |
<Δτ/τ>/% | 4,967 | 4,908 |
ESS adopts a model-free approach aimed to extract the abscissa of inflection points, whereas QENS needs an a priori model that here was the same one used as input in the simulations, something that is not possible in real experiments where any model can be proposed a priori. The error on the relative error is 1.2%, so ESS and QENS have the same ability but QENS was given all the advantages, which is not usually realistic in practice.