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1.
当用微波场作用到V型三能级原子的两个激发态能级时,系统跃迁路径之间发生交叉耦合导致了量子相干效应.通过调节微波场的强度,可实现对原子吸收和色散性质的改变,并呈现零吸收高折射率现象.此外,微波场诱导的量子相干也可实现相对相位对探测光增益的控制.  相似文献   

2.
当用微波场作用到V型三能级原子的两个激发态能级时,系统跃迁路径之间发生交叉耦合导致了量子相干效应.通过调节微波场的强度,可实现对原子吸收和色散性质的改变,并呈现零吸收高折射率现象.此外,微波场诱导的量子相干也可实现相对相位对探测光增益的控制.  相似文献   

3.
三能级Λ-型原子系统被非相干辐射场泵浦,系统处于稳态时产生无反转激光,本文分析无反转激光及增益的起源。  相似文献   

4.
张志颖  付申成  苟立丹  姚治海 《物理学报》2013,62(10):104206-104206
为了获得位相敏感的无粒子数反转探测增益, 研究了一个三能级闭合环路子系统控制的四能级原子系统.在三光子共振情况下, 获得了大的稳态无反转探测增益. 由于量子干涉效应, 探测增益对三能级闭合环路子系统的相对位相是敏感的. 三能级闭合环路子系统中的场强也是影响探测场增益特性的重要参数. 关键词: 量子干涉 位相敏感效应 无反转增益  相似文献   

5.
杨丽君  马腾  孙克家  冯晓敏 《物理学报》2015,64(6):64205-064205
研究了外加微波场作用下三能级原子系统的无粒子数反转放大特性. 通过求解系统的密度矩阵方程得到其探测吸收谱. 结果表明, 介质对探测场的吸收呈现多峰结构, 并且在强微波驱动场的作用下, 特定范围内出现了明显的负吸收(即光放大). 进一步定量分析各能级粒子数布居随作用场强度的变化, 揭示出该三能级原子系统呈现无粒子数反转光放大的规律. 最后, 采用缀饰态理论对探测吸收特性做出了准确的解释.  相似文献   

6.
在旋波、慢变振幅近似下,求解考虑了驱动场相位扩散后的系统密度矩阵运动方程,并给出了这个三能级梯型系统稳态线性解析解.利用得到的稳态线性解析解分析驱动场相位扩散是如何影响该系统输出无反转激光的.对稳态线性解析解数值计算的结果显示:由于驱动场相位扩散会导致无反转激光增益减小;即使由于驱动场相位扩散引起的线宽足够大,在该系统中仍能够获得无反转激光;线宽往往是破坏无反转激光产生和折射率的提高;因驱动场相位扩散导致无反转激光增益的减小,并不是总能够通过增大驱动场的Rabi频率得到补偿.  相似文献   

7.
研究发现在具有真空诱导相干性的开放和封闭ladder 型原子系统中,探测场和驱动场之间相对位相对吸收性质有重要的调制作用,同时非相干泵浦对位相相关的吸收性质有显著的影响.在这两种系统中,通过调节非相干泵浦,可以实现从吸收到增益和从粒子数反转激光到无粒子数反转激光的转化,并可获得最大的无反转激光增益.但是,当非相干泵浦不存在时,对相对位相的任意值,在封闭系统中只出现吸收而不能得到无反转激光增益;然而在开放系统中,对于适当的相对位相值甚至可以产生比有非相干泵浦时更大的无反转激光增益.  相似文献   

8.
研究了在具有自发辐射诱导相干性的Doppler展宽的封闭Λ型三能级系统中探测场和驱动场之间的相对位相对探测场无反转增益的控制作用. 研究结果表明: 1) 不管探测场和驱动场是同向传播还是反向传播, 驱动场是失谐还是共振,无反转增益总是随相对位相的改变而作周期性变化,周期为2π. 2) 驱动场共振时,无反转增益极大值随Doppler展宽值的增大而单调减小,且反向传播时比同向传播时减小的速度更快;驱动场失谐时,无反转增益的极大值随Doppler展宽值的增大不再单调地减小或增大. 在以上两种情况下,均可以通过调 关键词: 自发辐射诱导相干 相位控制 Doppler展宽 无反转增益  相似文献   

9.
研究了在具有自发辐射诱导相干性的Doppler展宽的封闭Λ型三能级系统中探测场和驱动场之间的相对位相对探测场无反转增益的控制作用. 研究结果表明: 1) 不管探测场和驱动场是同向传播还是反向传播, 驱动场是失谐还是共振,无反转增益总是随相对位相的改变而作周期性变化,周期为2π. 2) 驱动场共振时,无反转增益极大值随Doppler展宽值的增大而单调减小,且反向传播时比同向传播时减小的速度更快;驱动场失谐时,无反转增益的极大值随Doppler展宽值的增大不再单调地减小或增大. 在以上两种情况下,均可以通过调  相似文献   

10.
王丽  李根全  肖绍武  郑长波 《物理学报》2010,59(12):8512-8517
在以三个电偶极跃迁构成简并N型四能级系统中,利用密度矩阵方程计算了介质对探测场的吸收,研究了激光场拉比相位对吸收的影响.结果表明:介质对探测场的吸收和放大取决于控制场和信号场的拉比相位,且吸收和放大随控制场、信号场的拉比相位改变而作周期性变化,周期为2π;而探测场的拉比相位变化对吸收没有影响.同时,控制场、信号场拉比相位对吸收的影响是相同的,而且拉比相位主要影响原子相干,对原子布居影响不大.  相似文献   

11.
We theoretically investigate the features of two-photon absorption in a coherently driven four-level atomic system with closed-loop configuration. It is found that two-photon absorption can be completely suppressed just by properly adjusting the relative phase of four coherent low-intensity driving fields and the atomic system becomes trans- parent against two-photon absorption. From a physical point of view, we explicitly explain these results in terms of quantum interference induced by two different two-photon excitation channels.  相似文献   

12.
A four-level system is proposed to produce large index of refraction accompanied by vanishing absorption in the Er^{3+}-doped yttrium aluminium garnet (YAG) crystal. It is found that the high index of refraction with zero absorption can be provided by adjusting the incoherent pumping, the coherent field, as well as the concentration of Er^{3+} ions in the crystal. Furthermore, the value of the incoherent pump to achieve the high index of refraction with zero absorption is greatly changed with increasing the concentration of Er^{3+} ions in the crystal. This indicates that the effect of concentration on the high index of refraction with zero absorption cannot be neglected.  相似文献   

13.
We have investigated optical dimensional phenomena which are manifested as the thickness dependences of the indices of refraction n and absorption k and of the magnitude of the quasiBrewster angle of thin layers of gold. In the range of thicknesses 20 < d > 180 , all these phenomena have an oscillating character. Based on the earlier published experimental data on the energy coefficients of transmission T and reflection R of thin layers of atomic semiconductors (Se, Te, Ge, and Si), new calculations of the thickness dependences of n and k have been carried out without the simplifying assumptions which lead to incorrect results. The errors in determining the optical constants of thin layers from photometric data have been analyzed in detail. The causes of the earlier errors in works devoted to this kind of investigation have been established.  相似文献   

14.
周骏  贾振红 《光子学报》2003,32(11):1332-1335
用单光束扫描法测量了在532nm处一种新型非晶态分子材料5,5′Bis(dimesitylboryl)2,2′bithiophene的非线性折射率和吸收系数样品非线性透射特性的分析表明,在靠近线性吸收区的532nm处有饱和吸收存在由三能级饱和模型和Zscan法确定了饱和强度、非线性折射率的实部和虚部研究结果表明:这种新型非晶态分子材料具有非常好的光子学应用前景.  相似文献   

15.
光场的线宽对无粒子数反转光放大增益的影响   总被引:2,自引:2,他引:0  
针对拉曼驱动场下的四能级理论模型,讨论了实现无吸收、高折射率的条件,并分析了探测场及相干激发场的线宽对介质的折射率及增益的影响。计算结果表明,改变相干激发场 场强,或改变相干场的频率与原子能级间的失谐均可获得介质的无吸收,高折射率。激发扬线宽破坏了原子的相干性,使使介质的增闪下降并改变了折射率的大小,探测场的线宽使介质的探测增益谱及折射率谱的分辨率下降。  相似文献   

16.
The probe absorption-dispersion spectra of a radio-frequency (RF)-driven five-level atom embedded in a photonic crystal are investigated by considering the isotropic double-band photonic-band-gap (PBG) reservoir. In the model used, the two transitions are, respectively, coupled by the upper and lower bandsin such a PBG material, thus leading to some curious phenomena. Numerical simulations are performed for the optical spectra. It is found that when one transition frequency is inside the band gap and the other is outside the gap, there emerge three peaks in the absorption spectra. However, for the case that two transition frequencies lie inside or outside the band gap, the spectra display four absorption profiles. Especially, there appear two sharp peaksin the spectra when both transition frequencies exist inside the band gap. The influences of the intensity and frequency of the RF-driven field on the absorptive and dispersive response are analyzed under different band-edge positions. It is found that a transparency window appears in the absorption spectra and is accompanied by a very steep variation of the dispersion profile by adjusting system parameters. These results show that the absorption-dispersion properties of the system depend strongly on the RF-induced quantum interference and the density of states (DOS) of the PBG reservoir.  相似文献   

17.
研究了梯形四能级冷原子系统的非线性光学行为,在一微波场耦合两上简并能级时双暗态共振将会出现。在合适的参数条件下,系统将表现出正常色散与反常色散之间的转变。改变耦合场和微波场的大小能够调控慢光和超光速间的转变。  相似文献   

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