FIG. 11.
(Top) τp,He−I* as a function of heating power measured from the decay of a perturbative helium puff using the 468.6 nm line. The solid lines indicate a power function fit for each configuration. (Middle) τp,He−II* as a function of heating power measured from the decay of a perturbative helium puff using the 667.8 nm line. The solid lines indicate a power function fit for each configuration. (Bottom) τp,H* as a function of heating power measured from the decay of the interferometer line-averaged density. The values of τp,H* are negative because the plasma density is rising rather than falling. The solid lines indicate a power function fit for each configuration.

(Top) τp,HeI* as a function of heating power measured from the decay of a perturbative helium puff using the 468.6 nm line. The solid lines indicate a power function fit for each configuration. (Middle) τp,HeII* as a function of heating power measured from the decay of a perturbative helium puff using the 667.8 nm line. The solid lines indicate a power function fit for each configuration. (Bottom) τp,H* as a function of heating power measured from the decay of the interferometer line-averaged density. The values of τp,H* are negative because the plasma density is rising rather than falling. The solid lines indicate a power function fit for each configuration.

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