negative and the condition $a_3 \gg |a_1|$ with $a_2$ non-resonant is satisified approximately. The rate into deep dimers scales in this region approximately as $a_1^2/a_3$ consistent with the prediction by D’Incao and Esry. Two interference minima have been observed at $610$ G and $695$ G [@Lompe:2010] while our results show two minima at $600$ G and $715$ G. Above $700$ G, the data are larger than our results by more than a factor 10. Using the alternative parameters $\Lambda=329~a_0^{-1}$ and $\eta_*=0.34$ obtained in Ref. [@Lompe:2010], we again find a better agreement with the data. With these parameters the second minimum in the rate into the shallow dimer disappears beyond 730 G. Hence, the partial rate decreases monotonically and vanishes near 730 G. For smaller $\eta_*$, the position of the minimum in the total rate is around 730 G. As $\eta_*$ increases, the position remains almost the same and the depth of the minimum becomes shallower. The minimum is not visible when $\eta_*=0.34$ because the rate into deep dimers is much larger than the rate into the shallow dimer. Therefore, with these parameters that were fit to data for $\beta_1$ the position of the second minimum in the data for $\beta_3$ 