论文标题
$ \ text {n} _2^+$ air lasing的控制
Control of $\text{N}_2^+$ Air Lasing
论文作者
论文摘要
近红外激光器会生成$ \ text {b}^{\ text {2}}σ_ {\ text {u}}^{\ text {\ text {+text {+}} $ and $ \ text {x}^}^}^}^{x}^{\ text {\ text {2} {\ text {\ text {\ text {2} {\ text {\ text {2} {\ text {\ text {2} {\ text {\ text {2} σ_ {\ text {g}}^{\ text {+}} $ natrogen分子阳离子的状态部分是通过耦合$ \ text {x}^{x}^{\ text {2}}} = _ {\ text {\ text { $ \ text {a}^{\ text {2}}π_ {\ text {u}} $状态在v-system中。传统时间解析的泵探针测量取决于泵脉冲的离子化耦合,以初始化$ \ text {a}^{\ text {2}}π_ {\ text {\ text {u}}} $状态中的动态。在这里,我们表明弱的第二激发脉冲降低了歧义,因为它仅作用于离子化的离子上。附加控制脉冲可以通过将总体转移到$ \ text {a}^{\ text {2}}π_ {\ text {u}} $状态来增加增益,从而以两种不同的方式修改了激光发射。 $ \ text {x}^{\ text {2}}σ_ {\ text {g}}^{\ text {+text {+text {+text {+text {+text {a} {a} {a}^{\ text {2}}π_ {\ trestriation formations在我们的实验中处于基态的数据包,但是控制脉冲可以通过泵脉冲逆转冲动的对准,以删除$ \ text {b}^{\ text {\ text {2}}σ_{\ text {\ text {u}}}^{\ text {u}}^{\ text {\ text {+text {+}} $状态中的旋转波数据包。
A near-infrared laser generates gain on transitions between the $\text{B}^{\text{2}} Σ_{\text{u}}^{\text{+}}$ and $\text{X}^{\text{2}} Σ_{\text{g}}^{\text{+}}$ states of the nitrogen molecular cation in part by coupling the $\text{X}^{\text{2}} Σ_{\text{g}}^{\text{+}}$ and $\text{A}^{\text{2}} Π_{\text{u}}$ states in the V-system. Traditional time resolved pump-probe measurements rely on post-ionization coupling by the pump pulse to initialize dynamics in the $\text{A}^{\text{2}} Π_{\text{u}}$ state. Here we show that a weak second excitation pulse reduces ambiguity because it acts only on the ion independent of ionization. The additional control pulse can increase gain by moving population to the $\text{A}^{\text{2}} Π_{\text{u}}$ state, which modifies the lasing emission in two distinct ways. The presence of fast decoherence on $\text{X}^{\text{2}} Σ_{\text{g}}^{\text{+}}$ to $\text{A}^{\text{2}} Π_{\text{u}}$ transitions may prevent the formation of a coherent rotational wave packet in the ground state in our experiment, but the control pulse can reverse impulsive alignment by the pump pulse to remove rotational wave packets in the $\text{B}^{\text{2}} Σ_{\text{u}}^{\text{+}}$ state.