首页> 外文OA文献 >Excitation of H$_{2}^{+}$ with one-cycle laser pulses: Shaped post-laser-field electronic oscillations, generation of higher- and lower-order harmonics
【2h】

Excitation of H$_{2}^{+}$ with one-cycle laser pulses: Shaped post-laser-field electronic oscillations, generation of higher- and lower-order harmonics

机译:用单周期激光脉冲激发H $ _ {2} ^ {+} $:成形   后激光场电子振荡,产生更高和更高   低次谐波

代理获取
本网站仅为用户提供外文OA文献查询和代理获取服务,本网站没有原文。下单后我们将采用程序或人工为您竭诚获取高质量的原文,但由于OA文献来源多样且变更频繁,仍可能出现获取不到、文献不完整或与标题不符等情况,如果获取不到我们将提供退款服务。请知悉。

摘要

Non Born-Oppenheimer quantum dynamics of H$_{2}^{+}$ excited by shapedone-cycle laser pulses linearly polarized along the molecular axis have beenstudied by the numerical solution of the time-dependent Schr\"odinger equationwithin a %three-body three-dimensional model, including the internuclearseparation, $R$, and the electron coordinates $z$ and $\rho$. Laser carrierfrequencies corresponding to the wavelengths $\lambda_{l}=25$~nm through$\lambda_{l}=400$~nm were used and the amplitudes of the pulses were chosensuch that the energy of H$_{2}^{+}$ was close to its dissociation threshold atthe end of any laser pulse applied. It is shown that there exists acharacteristic oscillation frequency $\omega_{\rm osc} \simeq 0.2265$~au(corresponding to the period of $\tau_{\rm osc} \simeq 0.671$~fs and thewavelength of $\lambda_{\rm osc} \simeq 200$~nm) that manifests itself as a"carrier" frequency of temporally shaped oscillations of the time-dependentexpectation values $\langle z \rangle$ and $\langle \partial V/\partial z\rangle$ that emerge at the ends of the laser pulses and exist on a timescaleof at least 50~fs. Time-dependent expectation values $\langle \rho \rangle$ and$\langle \partial V/\partial \rho \rangle$ of the optically-passive degree offreedom, $\rho$, demonstrate post-laser-field oscillations at two basicfrequencies $\omega^{\rho}_{1} \approx \omega_{\rm osc}$ and $\omega^{\rho}_{2}\approx 2\omega_{\rm osc}$. Power spectra associated with the electronic motionshow higher- and lower-order harmonics with respect to the driving field.
机译:由时间依赖性的薛定od方程在3%以内的三点研究了由沿分子轴线性极化的整形周期激光脉冲激发的H $ _ {2} ^ {+} $的非伯恩-奥本海默量子动力学体三维模型,包括核间距,$ R $和电子坐标$ z $和$ \ rho $。对应于波长$ \ lambda_ {l} = 25 $〜nm到$ \ lambda_ {使用l} = 400 $〜nm,并选择脉冲幅度,使得在施加任何激光脉冲结束时,H $ _ {2} ^ {+} $的能量接近其解离阈值。存在特征振荡频率$ \ omega _ {\ rm osc} \ simeq 0.2265 $〜au(对应于$ \ tau _ {\ rm osc} \ simeq 0.671 $〜fs的周期和$ \ lambda _ {\ rm osc}的波长\ simeq 200 $〜nm)表现为时间相关期望值$ \ langle z \ rangle $和$ \ langle \ partial V / \ partial z \ rangle $出现在激光脉冲的末端,并且存在的时间尺度至少为50〜fs。随时间变化的期望值$ \ langle \ rho \ rangle $和$ \ langle \ partial V / \ partial \ rho \ rangle $的光学无源自由度$ \ rho $证明了两个激光场后的振荡基本频率$ \ omega ^ {\ rho} _ {1} \ approx \ omega _ {\ rm osc} $和$ \ omega ^ {\ rho} _ {2} \ approx 2 \ omega _ {\ rm osc} $。与电子运动相关的功率谱显示出相对于驱动场的高次谐波和低次谐波。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
代理获取

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号