合肥储存环注入状态下的高频系统研究

 对高频系统的束流负载效应和Robinson不稳定性条件进行了详细分析；通过对 失谐角、视在失谐角与储存环注入流强限的研究发现，对于合肥光源这样的中能储存环，由于注入状态的电子束能量较低，同步辐射相角接近90°，因此，只要给高频腔馈入一定的功率，再把腔调到一定的失谐角，就可以在环中注到较高的流强，达到二期工程的设计目标。     

双束流负载效应

分析研究了双束流储存环上的束流负载效应.束团纵向尾场的作用分别为:能量损失、同步频移和耦合束不稳定性,这里只研究前两个方面.以来团连续分布的束团串情形和均匀分布情形为例,给出了同步相移、频移与高次模参数及高频腔分布的关系.研究结果有助于优化高频腔的工作模式(通过调节调谐杆的位置来改变高次模的频率)和环上束团的分布,以减小束流负载效应.当高频腔关于对撞点对称分布时,正负电子的束流负载效应相同,可以用补偿单束流负载效应的方法来补偿正负电子束团的相位.     

直线加速器驻波腔中的瞬态束流负载效应

在高能加速器中, 随着单个束团和束团串中电荷量的提高, 当粒子束穿过加速腔的时候, 感应出的瞬态束流负载电压也越来越高. 但是, 在通常分析束流负载的时候, 往往对稳态束流负载研究的比较多, 而对瞬态束流负载的研究要相对少一些. 本文首先对束流负载的瞬态特性和束团穿过加速腔时高频源所看到谐振腔谐振频率的变化方式进行了分析, 然后又对两种情况下谐振腔的最优失谐条件进行了讨论, 并给出了相应的解析公式. 在第1种情况下, 当粒子束穿过加速腔的时候, 谐振腔的自然谐振频率能够及时地得到调节, 从而使高频源的电流与谐振腔的腔压同相, 以提高高频源的效率; 在第2种情况下, 当粒子束穿过加速腔的时候, 谐振腔的自然谐振频率保持不变, 不能被调节. 最后, 还对BEPCⅡ现有预注入器的预聚束腔、BEPCⅡ未来预注入器的两个次谐波聚束腔中的瞬态束流负载效应进行了分析.     

非均匀束团在储存环高频腔中产生的高次模功率

通过分析束流频谱与高频腔高次模的相互作用,提出了计算单束流和双束流储存环中非均匀束团产生的高频腔高次模功率的方法,推导出了这两种情况下的一般通用公式,并对所得到的解析结果进行了比较和讨论.     

合肥储存环高频系统的调整

讨论了合肥光源高频系统参数对束流流强的影响.在合肥储存环闭轨校正实验中,发现束流轨道有较大的变化,为此对高频系统的频率、腔温等参数进行了必要的调整.此项工作对二期工程高频系统改造也具有指导意义.     

BEPCⅡ零模束流反馈系统研制

 为了抑制BEPCⅡ多束团(93团)、大流强（910 mA）时的纵向振荡（零模）,引入了BEPCⅡ零模束流反馈系统。该系统首次应用于BEPCⅡ储存环上,它包括了束流信号采集、滤波、下变频、鉴相、移相等几个部分。使用该系统后,束流的纵向边带被抑制度大于10 dB,这表明,系统能够抑制束流的纵向振荡。     

台肥储存环高频系统的调整

讨论了合肥光源高频系统参数对束流流强的影响。在合肥储存环闭轨校正实验中，发现束流轨道有较大的变化，为此对高频系统的频率、腔温等参数进行了必要的调整。此项工作对二期工程高频系统改造也具有指导意义。     

储存环高频剔除系统

 介绍了用于电子储存环部分填充和非均匀填充的一种实验装置,它利用储存环中电子运动所具有的横向自由振荡和束团脉冲的时间结构这一特性,采用外加激励的方法使其产生共振,从而使得储存环中部分束团中的电子丢失,形成储存环的部分填充和非均匀填充。还扼要介绍了用高频剔除系统在储存环上实现不同填充方式时的束流积累结果。     

合肥光源慢加速过程中高频系统的调节

 合肥光源是一台专用同步辐射光源，它在低能注入积累束流，然后同步地把束流加速到高能并在储存环中稳定运行。在加速过程中，粒子的同步辐射能量损失迅速增加，束流负载效应发生变化，需要相应地调节高频系统参数保持束流稳定。讨论了合肥光源加速过程中高频系统可能的两种高频系统调节方式以及高能情况下高频系统的最佳运行状态。     

双束流激发的纵向尾场与纵向不稳定性的研究

 用解析的方法研究了同向和反向运动束流激发的纵向尾场,并且给出了线性近似下束团沿环不均匀分布情形下的双束流纵向多束团不稳定性的计算公式,得出了双束流不稳定性与高频腔(或其它类腔结构)在环上位置及模的对称性有关的结论。     

Coherent interaction of ion and electron beams in systems with electron cooling

A hydrodynamic approximation is used to study the behavior of dipole modes of the transverse oscillations of an ion beam in a storage ring with an electron cooling section. It is shown that in addition to the finite interaction time of the beams, instability may be caused by a specific interaction effect between the ion and electron beams in the magnetic field which leads to redistribution of energy between the various modes of the ion beam oscillations. In this case, the condition that the determinant of the transfer matrix for the cooling section does not exceed unity no longer guarantees the stability of the transverse coherent oscillations of the ion beam and all the eigenvalues of the complete matrix of the ion motion including the storage ring must be analyzed. Calculations of the stability of ion beam dipole oscillations are presented for the parameters of CELSIUS.     

Dielectronic recombination at low energy range with Boron-like Ar13+at the CSRm

In order to extend the dielectronic recombination (DR) experiments from the main cooler storage ring CSRm with intermediate charge state ions to the experimental cooler storage ring CSRe with highly charged ions and even radioactive ions, a test electron-ion recombination experiment of B-like Ar¹³⁺ ions was performed with a section of the new electron beam energy detuning system, which will be installed at the CSRe. We present the measured and also the calculated DR spectra for the ∆n = 0 resonances from 0 to 3 eV. The experimental results agree very well with the previous DR experimental data from CRYRING, and the energy resolution reached 30 meV full width at half maximum. This test experiment demonstrates that the reliability and stability of the newly developed electron beam energy detuning system are satisfactory for the upcoming DR experiments at the CSRe. However, we found large discrepancies between the experimental result and the calculation in both resonance positions and the intensities of the recombination spectrum below 0.7 eV, which indicate that precise calculation of the DR spectrum of multielectron ions is still a challenge.     

Oscillation dependence of two-wave mixing gain for unidirectional ring resonator in photorefractive materials

Dependence of the coupling strength of two-wave mixing gain in photorefractive materials for the single unidirectional ring resonator on oscillation conditions has been analyzed in the strong nonlinear regime. In this regime, difference between the frequency of the pump beam and oscillating beam is proportional to the cavity-length detuning, which can be explained in terms of the photorefractive phase-shift. This phase-shift results due to slightly non-degenerate two-wave mixing that compensates for cavity detuning and satisfies the round-trip phase condition for the steady-state oscillation. The presence of such a phase-shift allows the possibility of the nonreciprocal steady-state energy transfer between the pump and oscillating beams. If the gain due to the beam coupling is large enough to overcome the cavity losses then the signal beam is amplified in the presence of material absorption. Such amplification is responsible for the oscillations. For the single unidirectional ring resonator, the effects of cavity-length detuning, energy coupling coefficient, crystal thickness of the material, reflectivity of the cavity mirrors and material's absorption coefficient on the frequency and intensity of oscillations have also been studied in detail. It has been found that for the smaller value of absorption coefficient (α) of the photorefractive crystal, the unidirectional ring resonator can oscillate at almost any cavity-length detuning (ΔΓ) whereas for the larger value of α oscillation occurs only when the cavity-length detuning is limited to small region (around ΔΓ=0). But reverse of the case is found for energy coupling coefficient (γ₀).     

反馈调谐CO2激光器的静态与动态行为

建立了反馈调谐CO_2激光器的物理数学模型.稳态分析结果表明,只有当反馈系数大于某一临界值之后,才能出现激光器泵浦速率与激光输出之间的光学双稳性.线性稳定性分析的结果表明,系统失稳的必要条件是失谐量的Debye弛豫速率(反馈系统的带宽)必须超过布居反转的衰减速率.只有当激光泵浦落在某一范围内时,才出现不稳性.数值分析的结果证明了系统输出倍的周期分岔混沌行为.线性稳定性分析预言的Hopf分岔频率与数值分析的结果符合得很好.     

上海光源储存环横向反馈系统模拟计算

在同步辐射光源中, 阻抗壁不稳定性是一个很严重的问题. 要保证储存环在高流强下正常运行, 就需要安装一套横向反馈系统. 为了了解在横向反馈作用下束流的动力学性质,建立了一套横向反馈模拟计算程序. 并用该程序模拟计算了上海光源储存环横向反馈系统在闭轨误差(COD)、束流位置探测器读数误差以及梳状滤波等条件改变下的反馈效果.     

电子储存环中离子俘获不稳定性的强-强模型模拟

 电子储存环中,由于被束流势阱俘获的离子会引起束流不稳定性。研究这种不稳定性的产生机制和抑制方法对提高机器的性能有重要理论和现实意义。介绍了用强-强模型对合肥光源（HLS）电子储存环中离子俘获不稳定性产生机制进行的模拟研究。模拟结果可用于理解在合肥光源（HLS）储存环上观察到的离子俘获现象。     

The role of birefringence in modulation instability fiber ring resonators

We considered a high birefringence fiber ring cavity, which can be represented by a system of two incoherently coupled nonlinear Schrödinger equations with periodic boundary conditions. The stability of the system against time domain periodic perturbations could be strongly conditioned by fiber birefringence. We apply both a perturbative approach and a mean field approximation, in order to highlight the dependence of modulation instability on birefringence and ring detuning. We extend the study of the dynamical properties of the system by means of a phase matching interpretation and a selection of numerical solutions of the governing equations.     

合肥电子储存环束流不稳定性的抑制

 合肥光源二期工程改造的电子储存环调试过程中,发现多束团存储和运行时存在耦合束团不稳定性,严重地限制了注入的最高流强,并且影响了光源运行的质量。通过过正地增大正色品以及在储存环上插入八极磁铁,基本上抑制了横向的耦合束团不稳定性,保证了稳定注入束流300 mA的技术指标。     

合肥光源储存环束流截面测量系统改造和软件升级

 存储环束流截面及发射度是同步辐射加速器重要的基本参数。从束流截面大小的变化和束斑位置的移动规律，可以进行环上的束流不稳定性的研究。介绍了合肥光源，储存环束流截面测量系统局部改造和它的软件升级并且着重介绍西欧核子中心(CERN)的软件框架ROOT在数据处理和显示方面的应用。