...
首页> 外文期刊>Laser physics letters >Polarization rotation of photon echo at J = 0 <->1 transition in magnetic field
【24h】

Polarization rotation of photon echo at J = 0 <->1 transition in magnetic field

机译:磁场中J = 0 <-> 1跃迁时光子回波的极化旋转

获取原文
获取原文并翻译 | 示例

摘要

Detailed experimental analysis of photon echo polarization in a longitudinal magnetic field is performed for the first time at the simplest quantum transition J = 1<-> J = 0 for which the non-Faraday rotation of photon echo polarization plane was predicted. The echo was generated at the intercombination transition (6s6p){sup}3Pi →(6s{sup}2){sup}1So of 174{sup left}Yb by two resonant laser pulses of linear (parallel or mutually orthogonal) polarization, and the angled echo optical scheme was applied for the detection. At the magnetic field strength B ≤5 G the photon echo has polarization very close to linear one; its polarization plane rotates around magnetic field vector, and photon echo polarization components and integral echo power oscillate versus B from its maximum value to zero, in agreement with theory. At a stronger magnetic field B ~ 40 G photon echo power oscillations disappear, no preferable orientation of polarization vector is observed; the fluctuations of exciting radiation spectrum are supposed to be responsible for this "non-polarized" echo. Photon echo power in dependence on azimuthal angle at high magnetic field B ≈ 40 G. Solid line represents cubic parametric interpolation of B-spline type.
机译:首次在最简单的量子跃迁J = 1-J = 0上对纵向磁场中的光子回波极化进行了详细的实验分析,为此,我们预测了光子回波极化平面的非法拉第旋转。回声是在174 {sup left} Yb的互变跃迁(6s6p){sup} 3Pi→(6s {sup} 2){sup} 1So处通过线性(平行或相互正交)偏振的两个共振激光脉冲产生的,并且角度回波光学方案用于检测。在磁场强度B≤5G时,光子回波的极化非常接近线性极化。它的极化平面围绕磁场矢量旋转,并且光子回波极化分量和积分回波功率相对于B从最大值振荡到零,这与理论一致。在强磁场B〜40 G处,光子的回波功率振荡消失,没有观察到极化矢量的最佳取向。激发辐射光谱的波动被认为是造成这种“非极化”回波的原因。在高磁场B≈40 G时,光子回波功率取决于方位角。实线表示B样条曲线类型的三次参数插值。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

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