Parameter dependencies of the separatrix density in low triangularity L-mode and H-mode JET-ILW plasmas

The midplane electron separatrix density, n(e,sep), in JET-ILW L-mode and H-mode low triangularity deuterium fuelled plasmas exhibits a strong explicit dependence on the averaged outer divertor target electron temperature, n(e,sep) similar to T-e,ot(-1/2). This dependence is reproduced by analytic reversed two point model (rev-2PM), and arises from parallel pressure balance, as well as the ratio of the power and momentum volumetric loss factors, (1 - f(cooling))/(1- f(mom-loss)). Quantifying the influence of the (1 - f(cooling)) and (1 -f(mom-loss)) loss factors on ne,sep has been enabled by measurement estimates of these quantities from L-mode density (fueling) ramps in the outer horizontal, VH(C), and vertical target, VV, divertor configurations. Rev-2PM n(e,sep )estimates from the extended H-mode and more limited L-mode datasets are recovered to within +/- 25% of the measurements, with a scaling factor applied to account for use of (T-e,T-ot), an averaged quantity, rather than flux tube resolved target values. Both the (1 - f(cooling)) and (1 - f(mom-loss)) trends and recovery of n(e,sep) using the rev-2PM formatting are reproduced in EDGE2D-EIRENE L-mode-like and H-mode-like density scan simulations. The general lack of a divertor configuration effect in the JET-ILW n(e,sep) trends can be attributed to a significant influence of main chamber recycling, which has been shown in the EDGE2D-EIRENE results to moderate ne,sep with respect to changes in divertor neutral leakage imposed by changes in the divertor configuration. The unified n(e,sep) vs (T-e,T-ot) trends can, however, be broken if large modifications to the divertor geometry (e.g. complete removal of the outer divertor baffle structure) are introduced in the model. The more pronounced high-field side high density region formation in the VH(C) configuration with reduced clearance to the separatrix does not appear to have a significant influence on the outer midplane separatrix and pedestal parameters when mapped to (T-e,T-ot), although conditions at the inner midplane could not be assessed.