1. CORRECTIONS TO SECTION 4

The version of this manuscript originally published contained a sign error that appears at the re-transformation of the equations into laboratory frame in Section 4. The correctly re-transformed Eq. (8) reads:

(8)$${\rm \omega} ^2 = k^2c^2 + \displaystyle{{1 + u_{\rm e}^1 /c} \over {1 - u_{\rm e}^1 /c}}{\rm \omega} _{{\rm pe}}^2$$

and subsequently Eq. (9) is:

(9)$$k = \pm \displaystyle{{\rm \omega} \over c}\sqrt {1 - \displaystyle{{1 + u_{\rm e}^1 /c} \over {1 - u_{\rm e}^1 /c}}\displaystyle{{{\rm \omega} _{{\rm pe}}^2} \over {{\rm \omega} ^2}}}.$$

The sign error in the original letter also led to a misinterpretation: The Doppler-shifting does not limit the maximum velocity, achieved by the RPA, but it has impact on the admissible lower target thickness. Re-arranging the corrected Eq. (11) for d ₀ yields:

(11)$$\eqalign{d_0{\rm \gg} & \displaystyle{{c{\rm \varkappa} _{\rm e}} \over {\rm \omega}} \left( {\displaystyle{{1 + u_{\rm e}^1 /c} \over {1 - u_{\rm e}^1 /c}}\displaystyle{{{\rm \varkappa} _{\rm e}{\rm \omega} _{{\rm pe},0}^2} \over {{\rm \omega} ^2}} - 1} \right)^{ - 1/2} \cr \approx & \displaystyle{{c\sqrt {{\rm \varkappa} _{\rm e}}} \over {{\rm \omega} _{{\rm pe},0}}}\sqrt {\displaystyle{{1 - u_{\rm e}^1 /c} \over {1 + u_{\rm e}^1 /c}}},}$$

where the last term holds true for ω_pe,0 ≫ ω. Therefore, Eqs (12) and (13) in the original manuscript are obsolete, such as Figure 3. The correct interpretation is given in Figures 1 and 2: Figure 1 shows the lower limit for the initial target width as a function of the compression achieved at the RPA: The target thickness scales with $d \propto {\rm \varkappa} _{\rm e}^{ - 1} $, whereas the penetration depth scales with ${\rm \delta} \propto {\rm \varkappa} _{\rm e}^{ - 1/2} $ and it is: $d/{\rm \delta} \propto {\rm \varkappa} _{\rm e}^{ - 1/2} $.

Fig. 1. Minimum admissible target width from Eq. (3) as a function of the compression ϰ_e, for different initial densities with β = 0.3.

Fig. 2. Minimum admissible target width from Eq. (3) as a function of the longitudinal velocity ${\rm \beta} = u_{\rm e}^1 /c$, for different initial densities with ϰ_e = 3.5.

This effect is countered by the Doppler-shifting, as depicted in Figure 2: With increasing velocity, the laser frequency decreases due to the Doppler-shifting and the limit for the target width decreases. At the RPA, both effects compete and for β ≪ 1, the lower target width is $d_0 \approx (1 + {\rm \beta} ){\rm \varkappa} _{\rm e}^{ - 1/2} $.

Here, the average longitudinal velocity ${\rm \beta} = u_{\rm e}^1 /c$ can be calculated from the prevalent model of a flying mirror (see, e.g. Macchi et al., 2009), whereas the evaluation of the compression ϰ_e requires a more extensive model (see, e.g. Schmidt & Boine-Frankenheim, 2016).