Study of the circular dichroism of He⁺ ion

Four Absorption Channels (I to IV) and Probabilities of Their States $ (l,m) $ (Denoted by $ a{E}b $ 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 $ {{\rm He}^ + }(S) $ at the End of Pulse for Various Cases, Where $ S = 1s $, $ 3{p_1} $, Excited (Excluding $ 1s $, $ 3{p_1} $), and Ionized

Probability of $ {{\rm He}^ + }(S) $ (Denoted by $ a( - b) $ for $ a \times {10^{ - b}} $ or by %) from $ {{\rm He}^ + }(3{p_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 $ a{E}b $ 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 $ {{\rm He}^ + }(S) $ at the End of Pulse for Various Cases, Where $ S = 1s $, $ 3{p_1} $, Excited (Excluding $ 1s $, $ 3{p_1} $), and Ionized

Table 4.

Probability of $ {{\rm He}^ + }(S) $ (Denoted by $ a( - b) $ for $ a \times {10^{ - b}} $ or by %) from $ {{\rm He}^ + }(3{p_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