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Laser-triggered proton acceleration from hydrogenated low-density targets 来自氢化低密度目标的激光触发质子加速
Pub Date : 2017-06-19 DOI: 10.1103/PHYSREVACCELBEAMS.20.061301
A. V. Brantov, E. Obraztsova, A. Chuvilin, E. Obraztsova, a.V. Yu Bychenkov
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引用次数: 6
Influence of the injected beam parameters on the capture efficiency of an electron cyclotron resonance based charge breeder 注入光束参数对电子回旋共振电荷增殖器捕获效率的影响
Pub Date : 2017-06-13 DOI: 10.1103/PHYSREVACCELBEAMS.20.063401
A. Galatà, D. Mascali, G. Torrisi, L. Neri, L. Celona, J. Angot
Electron cyclotron resonance ion sources based charge breeders (ECR-CB) are fundamental devices for Isotope Separation On Line (ISOL) facilities aiming at postaccelerating radioactive ion beams (RIBs). Presently, low intensity RIBs do not allow a conventional tuning of the ECR-CB: as a consequence, it has to be set with a stable 1+ pilot beam first, switching then to the radioactive one without changing any parameter; this procedure is usually called “blind tuning.” Besides having different masses, pilot and radioactive beams can also differ in terms of the rms transverse emittance erms and/or longitudinal energy spread ΔE, so the choice of a given pilot beam can determine the overall performances of the final breeding stage. This paper shows a numerical study of how the capture efficiency of the PHOENIX charge breeder is affected by the aforementioned beam paramaters: the analysis reveals the two-step nature of the process, highlighting the role of the injection optics and the plasma capture capability in the overall performances of this device. The simulations predict highest efficiency for erms<5π  mm mrad and ΔE<5  eV in a optimum energy range between 2 and 6 eV, thus giving important information on the possibility of blindly tuning an ECR-CB. No isotopical effects were observed, while it clearly came out the necessity to improve the 1+ beam characteristics with a rf beam cooler prior to the injection into an ECR-CB.
基于电子回旋共振离子源的电荷增殖器(ECR-CB)是针对后加速放射性离子束(RIBs)的同位素在线分离(ISOL)设施的基础装置。目前,低强度肋不允许对ECR-CB进行常规调谐:因此,它必须首先设置稳定的1+导束,然后切换到放射性束,而不改变任何参数;这个过程通常被称为“盲调”。除了质量不同外,导束和放射性光束在横向发射率和/或纵向能量扩散ΔE方面也会有所不同,因此选择一个给定的导束可以决定最终育种阶段的整体性能。本文对PHOENIX电荷增殖器的捕获效率如何受到上述光束参数的影响进行了数值研究:分析揭示了该过程的两步性质,突出了注入光学和等离子体捕获能力在该装置整体性能中的作用。模拟预测了在2到6 eV之间的最佳能量范围内,erms<5π mm mrad和ΔE<5 eV时的最高效率,从而提供了关于盲目调谐ECR-CB的可能性的重要信息。虽然没有观察到同位素效应,但显然有必要在注入ECR-CB之前使用射频束冷却器来改善1+束的特性。
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引用次数: 3
Transverse coupled-bunch instability thresholds in the presence of a harmonic-cavity-flattened rf potential 谐波腔扁平射频电位存在下的横向耦合束不稳定阈值
Pub Date : 2016-12-16 DOI: 10.1103/PHYSREVACCELBEAMS.19.124401
F. Cullinan, R. Nagaoka, G. Skripka, P. Tavares
A small vacuum chamber aperture is a present trend in the design of future synchrotron light sources. This leads to a large resistive-wall impedance that can drive coupled-bunch instabilities. Another trend is the use of passively driven cavities at a harmonic of the main radio frequency to lengthen the electron bunches in order to increase the Touschek lifetime and reduce emittance blowup due to intrabeam scattering. In some cases, the harmonic cavities may be tuned to fulfill the flat potential condition. With this condition met, it has been predicted in simulation that the threshold current for coupled-bunch resistive-wall instabilities is much higher than with no bunch lengthening at all. In this paper, the features of a bunch in the flat potential that would contribute toward this stabilization are identified and discussed. The threshold currents for these instabilities are estimated for the MAX IV 3 GeV storage ring at different values of chromaticity using macroparticle simulations in the time domain and, within the limits of the existing theory, frequency domain calculations. By comparing the results from these two methods and analyzing the spectra of the dominant head-tail modes, the impact of each of the distinguishing features of a bunch in the flat potential can be explained and quantified in terms of the change in threshold current. It is found that, above a certain chromaticity, the threshold current is determined by the radial structure of the zeroth-order head-tail mode. This happens at a lower chromaticity if the bunch length is longer. (Less)
小孔径真空室是未来同步加速器光源设计的趋势。这导致了一个大的电阻壁阻抗,可以驱动耦合束不稳定性。另一个趋势是在主无线电频率的谐波处使用被动驱动腔来延长电子束,以增加图谢克寿命并减少由于束内散射引起的发射率爆炸。在某些情况下,谐波腔可以调谐以满足平电位条件。在满足这一条件的情况下,在模拟中预测耦合束电阻壁不稳定性的阈值电流要远远高于没有束加长的情况。在本文中,识别和讨论了有助于这种稳定的平坦电位束的特征。在不同色度值下,利用时域宏粒子模拟和现有理论范围内的频域计算,对MAX IV 3gev存储环的这些不稳定性阈值电流进行了估计。通过比较这两种方法的结果和分析优势正反模式的光谱,可以用阈值电流的变化来解释和量化平坦电位中束的每个特征的影响。发现在一定色度以上,阈值电流由零阶正反模式的径向结构决定。如果束的长度较长,这种情况就会在较低的色度下发生。(少)
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引用次数: 11
Extreme regimes of femtosecond photoemission from a copper cathode in a dc electron gun 直流电子枪中铜阴极飞秒光发射的极端状态
Pub Date : 2016-10-26 DOI: 10.1103/PHYSREVACCELBEAMS.19.103403
P. Pasmans, Van Vugt, van Jp Lieshout, G. Brussaard, O. J. Luiten
The femtosecond photoemission yield from a copper cathode and the emittance of the created electron beams has been studied in a 12 MeV/m, 100 keV dc electron gun over a wide range of laser fluence, from the linear photoemission regime until the onset of image charge limitations and cathode damaging. The measured photoemission curves can be described well with available theory which includes the Schottky effect, second-order photoemission, and image charge limitation. The second-order photoemission can be explained by thermally assisted one-photon photoemission (1PPE) and by above-threshold two-photon photoemission (2PPE). Measurements with a fresh cathode suggest that the 2PPE process is dominant. The beam emittance has been measured for the entire range of initial surface charge densities as well. The emittance measurements of space-charge dominated beams can be described well by an envelope equation with generalized perveance. The dc gun produces 0.1 pC bunches with 25 nm rms normalized emittance, corresponding to a normalized brightness usually associated with rf photoguns. In this experimental study the limits of femtosecond photoemission from a copper cathode have been explored and analyzed in great detail, resulting in improved understanding of the underlying mechanisms.
在12 MeV/m, 100 keV的直流电子枪中,研究了从线性光电发射到成像电荷限制和阴极损伤的飞秒光电发射产率和产生的电子束的发射度。现有的理论包括肖特基效应、二阶光发射和像电荷限制,可以很好地描述所测得的光发射曲线。二阶光发射可以用热辅助单光子光发射(1PPE)和阈值以上双光子光发射(2PPE)来解释。使用新阴极的测量表明,2PPE过程占主导地位。在整个初始表面电荷密度范围内测量了光束发射度。空间电荷主导光束的发射度测量可以用具有广义性能的包络方程很好地描述。直流枪产生0.1个pC束,rms归一化发射度为25 nm,对应于通常与射频光电枪相关的归一化亮度。在本实验研究中,对铜阴极飞秒光发射的限制进行了非常详细的探索和分析,从而提高了对潜在机制的理解。
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引用次数: 11
TMCI threshold with space charge and different wake fields 空间电荷和不同尾流场的TMCI阈值
Pub Date : 2016-08-22 DOI: 10.1103/PhysRevSTAB.20.034401
V. Balbekov
Transverse mode coupling instability of a bunch with space charge and wake field is considered within the frameworks of the boxcar model. Eigenfunctions of the bunch without wake are used as a basis for the solution of the equations with the wake field included. A dispersion equation for constant wake is presented in the form of an infinite continued fraction and also as the recursive relation with an arbitrary number of the basis functions. Realistic wake fields are considered as well including resistive wall, square, and oscillating wakes. It is shown that the TMCI threshold of the negative wake grows up in absolute value when the SC tune shift increases. Threshold of positive wake goes down at the increasing SC tune shift. The explanation is developed by an analysis of the bunch spectrum.
在箱车模型的框架内考虑了带空间电荷和尾流场的束的横向模耦合不稳定性。利用无尾流束的本征函数作为求解含尾流场方程的基础。以无限连分数的形式给出了恒定尾迹的色散方程,并给出了与任意数量的基函数的递推关系。实际的尾流场包括阻力壁尾流、方形尾流和振荡尾流。结果表明,负尾流的TMCI阈值绝对值随着SC调移的增大而增大。正尾流阈值随着SC调移的增大而减小。这种解释是通过对束谱的分析得到的。
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引用次数: 0
Focusing effects in laser-electron Thomson scattering 激光电子汤姆逊散射中的聚焦效应
Pub Date : 2016-06-18 DOI: 10.1103/PhysRevAccelBeams.19.094701
C. Harvey, M. Marklund, A. Holkundkar
We study the effects of laser pulse focusing on the spectral properties of Thomson scattered radiation. Modeling the laser as a paraxial beam we find that, in all but the most extreme cases of focusing, the temporal envelope has a much bigger effect on the spectrum than the focusing itself. For the case of ultrashort pulses, where the paraxial model is no longer valid, we adopt a subcycle vector beam description of the field. It is found that the emission harmonics are blue shifted and broaden out in frequency space as the pulse becomes shorter. Additionally the carrier envelope phase becomes important, resulting in an angular asymmetry in the spectrum. We then use the same model to study the effects of focusing beyond the limit where the paraxial expansion is valid. It is found that fields focussed to subwavelength spot sizes produce spectra that are qualitatively similar to those from subcycle pulses due to the shortening of the pulse with focusing. Finally, we study high-intensity fields and find that, in general, the focusing makes negligible difference to the spectra in the regime of radiation reaction.
研究了激光脉冲聚焦对汤姆逊散射辐射光谱特性的影响。将激光建模为近轴光束,我们发现,除了最极端的聚焦情况外,时间包络线对光谱的影响要比聚焦本身大得多。对于超短脉冲,当近轴模型不再有效时,我们采用子周期矢量光束描述场。发现随着脉冲变短,发射谐波在频率空间中发生蓝移和变宽。此外,载波包络相位变得重要,导致频谱中的角度不对称。然后,我们使用相同的模型来研究超过极限的聚焦效应,其中近轴扩展是有效的。发现聚焦到亚波长光斑大小的场产生的光谱与亚周期脉冲的光谱在质量上相似,这是由于聚焦缩短了脉冲。最后,我们研究了高强度场,发现在一般情况下,聚焦对辐射反应谱的影响可以忽略不计。
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引用次数: 23
Studies of Beam Induced Electron Cloud Resonances in Dipole Magnetic Fields 偶极磁场中束流诱导电子云共振的研究
Pub Date : 2016-03-15 DOI: 10.1103/PhysRevAccelBeams.19.074401
J. Calvey, W. Hartung, J. Makita, M. Venturini
The buildup of low energy electrons in an accelerator, known as electron cloud, can be severely detrimental to machine performance. Under certain beam conditions, the beam can become resonant with the cloud dynamics, accelerating the buildup of electrons. This paper will examine two such effects: multipacting resonances, in which the cloud development time is resonant with the bunch spacing, and cyclotron resonances, in which the cyclotron period of electrons in a magnetic field is a multiple of bunch spacing. Both resonances have been studied directly in dipole fields using retarding field analyzers installed in the Cornell Electron Storage Ring (CESR). These measurements are supported by both analytical models and computer simulations.
加速器中低能电子的积聚,被称为电子云,会严重损害机器的性能。在一定的光束条件下,光束可以与云动力学发生共振,加速电子的积累。本文将研究两种这样的效应:多冲击共振,其中云的发展时间与束间距共振;回旋共振,其中电子在磁场中的回旋周期是束间距的倍数。用安装在康奈尔电子存储环(CESR)上的延迟场分析仪在偶极子场中直接研究了这两种共振。这些测量结果得到了分析模型和计算机模拟的支持。
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引用次数: 2
Linearization of the longitudinal phase space without higher harmonic field 无高谐场时纵向相空间的线性化
Pub Date : 2015-12-30 DOI: 10.1103/PHYSREVSTAB.18.120102
B. Zeitler, K. Floettmann, F. Grüner
Alternative technique for linearizing the longitudinal phase space of an electron bunch formed via photoemission in an rf gun.
线性化电子束纵向相空间的另一种技术。电子束是在射频枪中通过光发射形成的。
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引用次数: 34
New supersonic gas jet target for low energy nuclear reaction studies 用于低能核反应研究的新型超音速气体射流靶
Pub Date : 2015-12-29 DOI: 10.1103/PHYSREVSTAB.18.123502
F. Favela, L. Acosta, E. Andrade, V. Araujo, A. Huerta, Ó. D. Lucio, G. Murillo, M. E. Ortiz, R. Policroniades, P. S. Rita, A. Varela, E. Chávez
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引用次数: 7
Dipole fringe field thin map for compact synchrotrons 紧凑型同步加速器的偶极子条纹场薄图
Pub Date : 2015-12-29 DOI: 10.1103/PHYSREVSTAB.18.122401
K. Hwang, S. Y. Lee
The fringe field of dipole magnets can be mportant in charged-particle beam dynamics [1,2]. For example, the edge angle effect on the vertical focusing has been parametrized by the fringe field integral introduced [1] and measured [3]. The nonlinear beam dynamics of the fringe field has also been included up to a sextupolelike potential in Ref. [2]. The fringe field effect is particularly important for compact accelerators that have a small bending radius. Applications of compact storage rings include the Inverse Compton Light Source (see, e.g., [4]), proton therapy synchrotrons, etc. The fringe field of dipole magnets typically extends to the range of the vertical magnet gap. The range of the fringe field is usually minimized to avoid magnetic field coupling due to limited available space in compact storage rings. As the range of the fringe field is reduced, parts of the fringe field effects may be minimized and others amplified. In particular, higher-order nonlinearity can become important. Often overlooked, an important feature of the dipole fringe field effect is the closed orbit deviation from the design orbit. This change of the closed orbit arises from the fact that the fringe field introduces continuously varying curvature, while the design orbit is defined by constant curvature starting from the hard edge dipole boundary. Although this fact is naive and simple, its effect can be large for compact storage rings and thus should not be disregarded. If not considered, it can cause significant misalignment errors for all other accelerator elements. As the fringe field extent decreases, the closed orbit deviation will also decrease. However, higher-order nonlinearity would increase. It is important to understand how these effects rely on the fringe field extent. Recently, the fringe field effects on nonlinear dynamics for compact rings and large emittance beams have been considered in Refs. [5,6]. The numerical method was used to extract the Taylor map or Lie map out of the 3D field data [7,8]. However, there is still a demand for an analytic expression of the fringe field map, particularly when the 3D field data are not available at the design stage. Because of its complex nonlinear effects, it is often hard to uncover the underlying physics based on simulation results alone. In addition, a good understanding of the dipole fringe field map can benefit not only storage ring design but also dipole magnet design. Theoretical studies on the influence of dipole fringe fields have been carried out by many researchers from the early 1960s through the early 1970s [9–14]. Although some earlier studies derived mapping equations up to third order of phase space variables, they often led to complicated expressions with too many integration parameters. This paper is intended to provide a simpler physics picture of fringe field effects. The Lie algebraic method is useful to study the fringe field effect [15]; e.g., the Methodical Accelerator Design ver.10
偶极磁体的条纹场在带电粒子束动力学中很重要[1,2]。例如,边缘角对垂直聚焦的影响已经通过引入的条纹场积分参数化[1]并测量[3]。在文献[2]中,条纹场的非线性光束动力学也包括到六极势。对于弯曲半径小的紧凑型加速器,条纹场效应尤为重要。紧凑存储环的应用包括逆康普顿光源(参见,例如[4]),质子治疗同步加速器等。偶极磁体的条纹场通常延伸到垂直磁隙的范围内。由于紧凑存储环的可用空间有限,条纹场的范围通常被最小化以避免磁场耦合。随着条纹场范围的减小,部分条纹场效应可能被最小化,而另一些则可能被放大。特别是,高阶非线性会变得很重要。偶极子条纹场效应的一个经常被忽视的重要特征是闭合轨道偏离设计轨道。闭合轨道的这种变化是由于边缘场引入了连续变化的曲率,而设计轨道是由从硬边偶极子边界开始的恒定曲率定义的。虽然这个事实是天真和简单的,它的影响可能是巨大的紧凑的存储环,因此不应忽视。如果不加以考虑,它可能会导致所有其他加速器元素出现严重的不对齐错误。随着条纹场范围的减小,闭合轨道偏差也会减小。然而,高阶非线性会增加。重要的是要了解这些影响是如何依赖于边缘场的范围。近年来,文献中研究了条纹场对致密环和大发射度光束非线性动力学的影响。(5、6)。采用数值方法从三维野外数据中提取Taylor map或Lie map[7,8]。但是,对于边缘场图的解析表达式仍然有一定的需求,特别是在设计阶段无法获得三维现场数据的情况下。由于其复杂的非线性效应,通常很难仅根据模拟结果揭示其潜在的物理特性。此外,对偶极子条纹场图的理解不仅有助于存储环的设计,也有助于偶极子磁体的设计。从20世纪60年代初到70年代初,许多研究者对偶极子条纹场的影响进行了理论研究[9-14]。虽然早期的一些研究推导出了三阶相空间变量的映射方程,但往往导致积分参数过多的复杂表达式。本文的目的是提供一个更简单的条纹场效应的物理图像。李代数方法是研究条纹场效应的有效方法[15];例如,第10版《有条不紊的加速器设计》多态跟踪码(MADX PTC)模块通过硬边缘近似实现了二阶条纹场效应[2]。然而,推导是在极面平行框架上进行的,忽略了闭合轨道偏差。本文利用李映射方法研究了偶极子软条纹场相对于设计轨道的有效薄映射,该薄映射可达Magnus级数的下一阶和正则变量的四阶。我们还从Lie map中计算出映射方程,将其与仿真和早期研究[1]进行比较。我们将本文组织如下。在第二节中,我们建立了一个一般的边缘场模型。第三节给出相应的哈密顿量。第四节回顾了构建有效薄映射的李代数方法。第五节给出了推导出的解析图。第六节对理论与仿真结果进行了比较。第七节讨论了条纹场诱导的闭合轨道效应。第八节讨论了八极势的物理性质。第9节简要介绍了非线性失谐效应kilean20@gmail.com
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引用次数: 8
期刊
Physical Review Special Topics-accelerators and Beams
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