In the presence of rfdriven current, Equation (11.2) generalizes such that
(12.27) 
(12.28) 
In the presence of rf current drive, Equation (11.68) generalizes to give
(12.29) 
(12.30) 
(12.32) 

We can think of the dimensionless parameter as a sort of rf current drive efficiency. If then the destabilizing bootstrap term (i.e., the third term) on the righthand side of the modified generalized Rutherford equation, (12.31), can be completely suppressed (assuming that ) by driving a current density at the rational surface that matches the missing bootstrap current density (i.e., ). In this case, the rf current drive is 100% efficient at stabilizing the neoclassical tearing mode. On the other hand, if then the destabilizing bootstrap term in the generalized Rutherford equation can only be completely eliminated by driving a current density at the rational surface that is twice the missing bootstrap current density (i.e., ). In this case, the rf current drive is only 50% efficient.

Suppose that the normalized rfdriven current density profile is such that
(12.33) 
It is easily demonstrated that
(12.34) 
(12.35) 
(12.36)  
(12.37) 

Figures 12.4 and 12.5 illustrate how the current drive efficiency parameter, , varies with the current drive profile width parameter, , and the duty cycle parameter, , in cases where these is no misalignment between the current drive profile and the rational surface (i.e., ). It can be seen that attains a maximum value of about when and [28]. Thus, the optimal fullwidthhalfmaximum of the current drive profile is about 83% of the width of the magnetic island chain. It can also be seen that optimal modulation of the driven current increases the maximum achievable current drive efficiency by about 50%, while reducing the required rf power by 40% [28].
Figure 12.6 illustrates what happens when the current drive profile is misaligned with the rational surface (i.e., when the peak driven current density does not lie on the rational surface). It can be seen that misalignment decreases the current drive efficiency. Indeed, if the misalignment becomes too great then the efficiency becomes negative (indicating that the current drive destabilizes, rather than stabilizes, the neoclassical tearing mode) [28]. When , the maximum tolerable misalignment is about , which corresponds to a misalignment in minor radius of about 63% of the island width [28].
The broad conclusion that can be drawn from Figures 12.4–12.5 is that the maximum current drive efficiency is achieved when the driven current profile matches the profile of the missing bootstrap current (i.e., when it is centered on the rational surface, is of radial extent of about an island width, and is slightly concentrated at the island Opoints).

Consider a neoclassical tearing mode for which the righthand side of the generalized Rutherford equation case is specified in Figure 12.3. Suppose that the magnetic island chain has achieved its final steadystate width, . Let us apply an rf current drive profile whose width and misalignment parameters are and , respectively. The applied current drive causes the island chain to shrink in width. Assuming that the current drive profile remains constant, the effective width and misalignment parameters when the normalized island width has shrunk to the value are
(12.38)  
(12.39) 
Figure 12.7 shows how the righthand side of the generalized Rutherford equation specified in Figure 12.3 is modified by an rf current drive profile with optimal width, (i.e., a fullwidthhalfmaximum of 9.2% of the plasma minor radius), optimal alignment, , and optimal duty cycle, . It can be seen that the neoclassical tearing mode is completely stabilized [i.e., for all ] once the peak amplitude of the driven current density exceeds 75% of the equilibrium bootstrap current density at the rational surface (i.e., ). Of course, as soon as the island width has shrunk to value less than the seed island width shown in Figure 12.3 (i.e., ), the rf power can be switched off, and the neoclassical tearing mode will not return (unless it is triggered again by a transient resonant magnetic perturbation).

Figure 12.8 shows how the righthand side of the generalized Rutherford equation specified in Figure 12.3 is modified by an unmodulated (i.e., ) rf current drive profile with optimal width, , and optimal alignment, . It can be seen that the neoclassical tearing mode is completely stabilized once peak amplitude of the driven current density exceeds 291% of the equilibrium bootstrap current density at the rational surface (i.e., ). The large increase in the requisite driven current density, relative to the modulated case shown in Figure 12.7, comes about because unmodulated current drive becomes very inefficient at stabilizing a neoclassical tearing mode once the island width shrinks to such an extent that it is much less than the current drive profile width. In other words, as for unmodulated current drive, whereas remains finite as for modulated current drive [21,31]. To be more specific, for the case of unmodulated current drive, the stabilizing effect of the current driven at the island Opoints is partially cancelled by the destabilizing effect of the current driven at the island Xpoints [29]. This cancellation becomes almost exact when the island width is much less than the current drive profile width [21]. Of course, there is no such cancellation in the case of modulated current drive because no current is driven at the Xpoints.

Figure 12.9 shows how the righthand side of the generalized Rutherford equation specified in Figure 12.3 is modified by an rf current drive profile with optimal width, , nonoptimal alignment, , and optimal duty cycle, . It can be seen that the misalignment of the current drive profile causes the critical peak current density required to stabilize the neoclassical tearing mode to rise to 261% of the equilibrium bootstrap current density at the rational surface.
The broad conclusion that can be drawn from Figures 12.7–12.9 is that a neoclassical tearing mode can be stabilized by properly aligned, modulated, current drive in which the driven current density profile has a similar width to the magnetic island chain, and a similar peak magnitude to the equilibrium bootstrap current density at the rational surface.
Finally, successful stabilization of neoclassical tearing modes via electron cyclotron wave current drive has been achieved in many tokamak experiments, including ASDEX Upgrade [39], DIIID [22], and JT60U [25].