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Influence of atomic densities on propagation property for femtosecond Gaussian pulse in a three-level A-type atomic medium

机译:原子密度对三级A型原子介质飞秒高斯脉冲传播特性的影响

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We investigate effect of atomic densities (N) on propagation and spectral property of large area femtosecond Gaussian pulse (the pulse area is larger than 27π) in a three-level A-type atomic medium by using the numerical solution of the full Maxwell-Bloch equations without the slowly varying envelope and the rotating-wave approximations, and the solution is obtained by PC-FDTD method. It is shown that, variation of value of the atomic density has considerable effect on propagation and spectral property and the effect is closely relative to size of the pulse area. For the pulse with area 4 π, propagate in the dilute medium with smaller atomic density, clear pulse splitting doesn't occur, slight pulse spectrum broadening appears, the strength of the spectral component with higher frequency increases with the distance increasing; when the pulse propagates in the dilute medium with larger atomic density and in the dense medium, the main pulse splits into two sub-pulses, and the spectrum broadening in the dilute medium with larger atomic density is much larger than that in the dense medium. For the pulse with larger area 8π, the case of the pulse propagates in the dilute medium with smaller atomic density is similar to that of the 4π pulse; but when the pulse propagates in the dilute medium with larger atomic density and in the dense medium, the case is considerably different from that for 4π pulse, the main pulse splits into three sub-pulses, and the spectrum broadening in the dilute medium with larger atomic density is much smaller than that in the dense medium.
机译:我们探讨传播和大面积飞秒高斯脉冲的光谱特性原子密度(N)的作用(脉冲面积比27π大)通过使用完整麦克斯韦 - 布洛赫的数值解在三电平A型原子介质没有缓慢变化的外壳和旋转波近似的等式,并通过PC-FDTD方法获得溶液。结果表明,原子密度值的变化对传播和光谱性具有相当大的影响,并且效果紧密相对于脉冲区域的尺寸。对于面积4π的脉冲,在具有较小原子密度的稀释介质中传播,不会出现清晰的脉冲分裂,出现微小的脉冲光谱展会,频率较高的频谱分量的强度随着距离的增加而增加;当脉冲在具有较大原子密度和致密介质中的稀释介质中传播时,主脉冲分成两个子脉冲,并且具有较大原子密度的稀培养基中的光谱扩展远大于致密介质中的稀释介质。对于具有较大区域8π的脉冲,脉冲的情况在稀释介质中传播,具有较小的原子密度类似于4π脉冲的脉冲;但是当脉冲在具有较大原子密度和致密介质中的稀释介质中传播时,壳体与4π脉冲的情况相比不同,主脉冲分成三个子脉冲,并且稀释培养基中的光谱宽度较大原子密度远小于密集介质中的密度。

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