Four Absorption Channels (I to IV) and Probabilities of Their States $(l,m)$ (Denoted by $aEb$ for $a\times {10}^b$ beneath the States) at the End of Pulses in Fig. 1 in Ref. [17]

Pulse Delay Effects on CD

Probability of ${\mathrm{H}\mathrm{e}}^{+}(S)$ at the End of Pulse for Various Cases, Where $S=1s$, $3p_1$, Excited (Excluding $1s$, $3p_1$), and Ionized

Probability of ${\mathrm{H}\mathrm{e}}^{+}(S)$ (Denoted by $a(-b)$ for $a\times {10}^{-b}$ or by %) from ${\mathrm{H}\mathrm{e}}^{+}(3p_1)$ at the End of Pulse for Cases $A=(10,5.6,120,120)$ and $B=(4.75,5.6,175,$ $175)$, Where $S$ Denotes a State with Quantum Numbers ($l$, $m$) in the Four Absorption Channels Defined in Table 1

Table 1.

Four Absorption Channels (I to IV) and Probabilities of Their States $(l,m)$ (Denoted by $aEb$ for $a\times {10}^b$ beneath the States) at the End of Pulses in Fig. 1 in Ref. [17]

Table 2.

Pulse Delay Effects on CD

Table 3.

Probability of ${\mathrm{H}\mathrm{e}}^{+}(S)$ at the End of Pulse for Various Cases, Where $S=1s$, $3p_1$, Excited (Excluding $1s$, $3p_1$), and Ionized

Table 4.

Probability of ${\mathrm{H}\mathrm{e}}^{+}(S)$ (Denoted by $a(-b)$ for $a\times {10}^{-b}$ or by %) from ${\mathrm{H}\mathrm{e}}^{+}(3p_1)$ at the End of Pulse for Cases $A=(10,5.6,120,120)$ and $B=(4.75,5.6,175,$ $175)$, Where $S$ Denotes a State with Quantum Numbers ($l$, $m$) in the Four Absorption Channels Defined in Table 1