基于冷里德堡原子电磁感应透明的微波电场测量

在磁光阱中利用冷原子温度低,多普勒展宽小的优势获得了窄线宽的里德堡电磁感应透明(EIT)谱峰,结合Autler-Townes分裂效应(EIT-AT分裂)分别测量了多个频率的微波电场强度.结果显示,EIT-AT分裂间距与微波电场强度呈很好的线性关系,EIT-AT分裂方法可测量的微波电场强度线性区的下限可达222μV/cm,这个下限比传统热原子蒸汽池中EIT-AT分裂线性区的下限5 mV/cm提高了大约22倍,这对极弱微波电场的绝对校准非常有帮助.我们进一步利用EIT共振处探测光透过率的变化测量微波电场强度,对应的最小测量值可以小于1μV/cm,相应的灵敏度可达到1μV·cm^-1.Hz^-1/2.这些结果展示了冷原子样品在微波电场测量及其绝对校准方面的优势.     

Theoretical Analysis of Ionic Autoionization Spectra of Lanthanum in the Energy Region of 90650—915—00cm^—1

Eigenquantum defects μα and transformation matrix Uiα of La are calculated from the first principles byrelativistic multichannel theory, and dipole matrix elements Dα are obtained by fitting the experimental spectra.With these parameters, ionic autoionization spectra of lanthanum via an intermediatestate (Xe)5d6d^-1 P1 of La . in the energy region of 90650-91500 cm^-1 are calculated within the framework of multichannel auantum defecttheory. Our calculated spectra are in general agreement with the experimental data.     

Importance of Relativistic Effects for Intermediate-Z Elements： Photoionization Process of Excited Na

Using a modified R-matrix code, the fine-structure-resolved partial photoionization cross sections of excited Na （Z = 11） are calculated within the Breit-Pauli approximation. Our calculated energy levels of Na＋ and Na are in good agreement with the experimental values within 1% and the branching ratios of the J-resolved partial cross sections are consistent with the recent measurements within the experimental uncertainties. The agreements are impossible to be obtained without adequately taking into account the relativistic effects and the electron correlations together. Therefore, even for the intermediate-Z elements （e.g. Na with Z = 11）, the relativistic effects （mainly the spin-orbit interactions） should not be neglected.     

微分散射截面测量中气压效应的修正

介绍了微分散射截面测量过程中的气压效应 ,通过深入分析得出了二次散射系数E(θ)与零度角的强度A0 成正比 ,随散射角θ的增加而增加以及它的值可正可负 .通过与实验的对比 ,证实了前两条结论 ,并指出可把该结论用于指导实验. The pressure effect for the measurement of differential cross section is introduced and analysed in detail. Three conclusions are obtained: the double scattered coefficient E(θ) is proportional to the strength A 0 of the excitations measured at 0°; E(θ) increases with the increasing of scattered angle; the values of E(θ) can be positive or negative. The front two conclusions are tested by experiment, and it is pointed that they are helpful to the measurement of differential cross section.     

An all-optical phase detector by amplitude modulation of the local field in a Rydberg atom-based mixer

Recently, a Rydberg atom-based mixer was developed to measure the phase of a radio frequency (RF) field. The phase of the signal RF (SIG RF) field is down-converted directly to the phase of a beat signal created by the presence of a local RF (LO RF) field. In this study, we propose that the Rydberg atom-based mixer can be converted to an all-optical phase detector by amplitude modulation (AM) of the LO RF field; that is, the phase of the SIG RF field is related to both the amplitude and phase of the beat signal. When the AM frequency of the LO RF field is the same as the frequency of the beat signal, the beat signal will further interfere with the AM of the LO RF field inside the atom, and then the amplitude of the beat signal is related to the phase of the SIG RF field. The amplitude of the beat signal and the phase of the SIG RF field show a linear relationship within the range of 0 to π/2 when the phase of the AM is set with a difference π/4 from the phase of the LO RF field. The minimum phase resolution can be as small as 0.6° by optimizing the experimental conditions according to a simple theoretical model. This study will expand and contribute to the development of RF measurement devices based on Rydberg atoms.     

Decay pathways of superexcited states of nitrous oxide

The ionization and ionic dissociation of the superexcited state of N20 are studied by using electron energy loss spectroscopy and positive ion time-of-flight mass spectroscopy at different momentum transfers; that is, 0 and 0.23 a.u. （atomic unit） . The transitions at 13.8 eV and 14.0 eV are reassigned as 3pπ（000） and 3pσ（000） converging to A^2∑＋, respectively. The competition between the main decay pathways of superexcited states at different momentum transfers is revealed. It is found that 3dσ converging to C^2∑＋ mainly decays into N2O^＋ while 4dσ can decay into both N2^O＋ and NO^＋.     

M带高能光子对发射谱诊断辐射场温度的影响

在稳态近似下通过求解速率方程分别计算了有无M带高能光子存在下,不同温度密度下Cl等离子体的离化度分布以及发射谱,研究了高能光子对等离子体发射谱的影响。研究发现:腔内混有的少量M带高能光子几乎不影响等离子体中重要的离化度分布,但是会激发或者电离各种离子的内壳层电子,从而对发射谱产生重要的影响。因此有M带高能光子存在时,用发射谱诊断等离子体温度时需要同时考虑温度、密度和M带高能光子对发射谱的影响。     

神光III主机上球腔辐射场实验的三维数值模拟与分析

2015年在神光Ⅲ激光装置上开展了两孔球腔物理实验.利用三维隐式蒙特卡罗数值模拟程序模拟两孔球腔中的辐射输运问题,研究辐射场分布及其动态演化过程.数值模拟结果大多数与实验结果符合较好,但局部位置存在明显差异.分析了产生差异的可能原因,提出解决措施及未来发展方向.综合数值模拟结果及其与实验结果的对比可知,三维隐式蒙特卡罗数值模拟程序具备较好的黑腔三维辐射输运数值模拟能力.     

氢分子电子态b1Пu及其振动态的微分截面和振子强度

在电子入射能量300 eV条件下,测量了氮分子在不同散射角下的12—14 eV能区的能量损失谱,散射角范围为2.75°—10.25°。得到了电子态b¹∏_u振动能级v’=1—4的散射微分截面和广义振子强度,并通过外推k~2至零的方法得到了b¹∏_u及其振动能级v’=1—4的散射微分截面和广义振子强度,并通过外推K~2主零的方法得到了b¹∏_u及其振动能级v’=1—4的光学振子强度。所得结果与已发的实验数据和理论结果作了比较     

A Novel Observation of ＂a Sharp Absorption Line＂ Using Much More Broad Laser Lights： Quantum Interference in the Autoionization Spectra of Sc

The most accurate measturements in physical sciences will be precision spectroscopic experiments which are based on the usage of most narrow lines in cooperation with interference phenomena. We present a novel experimental observation of ＂a sharp absorption resonance line＂ with much more broad laser lights. The mechanism of such a novel phenomenon will be elucidated and its implications will be discussed.