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R-matrix calculation of differential cross sections for low-energy electron collisions with ground and electronically excited state O2 molecules

机译:低能量微分截面的R矩阵计算   电子与地面和电子激发态O2分子碰撞

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摘要

Differential cross sections for electron collisions with the O$_2$ moleculein its ground ${X}^{3}\Sigma_g^-$ state, as well as excited ${a}^{1}\Delta_g$and ${b}^{1}\Sigma_g^+$ states are calculated. As previously, the fixed-bondR-matrix method based on state-averaged complete active space SCF orbitals isemployed. In additions to elastic scattering of electron with the O$_2$${X}^{3}\Sigma_g^-$, ${a}^{1}\Delta_g$ and ${b}^{1}\Sigma_g^+$ states, electronimpact excitation from the ${X}^{3}\Sigma_g^-$ state to the ${a}^{1}\Delta_g$and ${b}^{1}\Sigma_g^+$ states as well as '6 eV states' of${c}^{1}\Sigma_u^{-}$, ${A'}^{3}\Delta_u$ and ${A}^{3}\Sigma_u^{+}$ states isstudied. Differential cross sections for excitation to the '6 eV states' havenot been calculated previously. Electron impact excitation to the${b}^{1}\Sigma_g^+$ state from the metastable ${a}^{1}\Delta_g$ state is alsostudied. For electron impact excitation from the O$_2$ ${X}^{3}\Sigma_g^-$state to the ${b}^{1}\Sigma_g^+$ state, our results agree better with theexperimental measurements than previous theoretical calculations. Our crosssections show angular behaviour similar to the experimental ones fortransitions from the ${X}^{3}\Sigma_g^-$ state to the '6 eV states', althoughthe calculated cross sections are up to a factor two larger at large scatteringangles. For the excitation from the ${a}^{1}\Delta_g$ state to the${b}^{1}\Sigma_g^+$ state, our results marginally agree with the experimentaldata except for the forward scattering direction.
机译:电子与基态$ {X} ^ {3} \ Sigma_g ^-$中的O $ _2 $分子以及激发的$ {a} ^ {1} \ Delta_g $和$ {b}发生电子碰撞的微分截面计算^ {1} \ Sigma_g ^ + $状态。如前所述,采用了基于状态平均完整活动空间SCF轨道的固定键R-矩阵方法。除具有O $ _2 $$$ {X} ^ {3} \ Sigma_g ^-$,$ {a} ^ {1} \ Delta_g $和$ {b} ^ {1} \ Sigma_g ^的电子弹性散射外+ $状态,从$ {X} ^ {3} \ Sigma_g ^-$状态到$ {a} ^ {1} \ Delta_g $和$ {b} ^ {1} \ Sigma_g ^ + $状态的电子冲击激发以及$ {c} ^ {1} \ Sigma_u ^ {-} $,$ {A'} ^ {3} \ Delta_u $和$ {A} ^ {3} \ Sigma_u ^ { +} $个州已研究。以前尚未计算出激发到“ 6 eV状态”的微分截面。还研究了从亚稳态$ {a} ^ {1} \ Delta_g $状态到$ {b} ^ {1} \ Sigma_g ^ + $状态的电子冲击激发。对于从O $ _2 $ $ {X} ^ {3} \ Sigma_g ^-$状态到$ {b} ^ {1} \ Sigma_g ^ + $状态的电子冲击激发,我们的结果与实验测量结果相比更加吻合理论计算。我们的横截面显示了类似于从$ {X} ^ {3} \ Sigma_g ^-$状态到'6 eV状态转换的实验行为的角行为,尽管在较大的散射角度下,计算出的横截面最多增大了两倍。对于从$ {a} ^ {1} \ Delta_g $状态到$ {b} ^ {1} \ Sigma_g ^ + $状态的激发,除前向散射方向外,我们的结果与实验数据基本一致。

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