1+1/2 Cell超导加速腔的本征高阶模场分布研究

为实现高平均流强加速, 需要有效地消除超导加速腔中的高阶模场. 为研制有效的高阶模耦合器, 本文对北京大学DC-SC光阴极超导注入器的核心部件—1+1/2 cell超导加速腔中高阶模场进行了分析研究, 用HFSS程序计算给出前31个高阶模场参数, 与实验测量较为符合. HFSS计算与Superfish计算结果比较符合很好, 验证用HFSS计算可靠, 为以后超导腔的升级研究提供有效的手段.     

TESLA式高阶模衰减器的改进与设计研究

为了消除超导加速腔中高阶模场对加速粒子的影响, 在DESY的高阶模耦合器结构的基础上本文提出了改进的耦合器. 用HFSS程序针对1.5cell腔设计优化了高阶模耦合器, 得到高阶模耦合器对几种主要模式的吸收. 研究结果表明, 采用新型结构后, 衰减器对主要有害模的衰减由－40dB提高到－15dB, 使原有高阶模衰减器的性能明显提高. 该高阶模衰减器也适用于国产2cell超导腔的使用.     

9-cell超导腔快速预调谐方法研究

对频率和场平坦度的预调谐是9-cell超导腔耗时最多的后处理工序之一,很快将成为国内相关大科学工程9-cell腔批量生产的瓶颈。首先介绍了9-cell超导腔两种常用的预调谐方法,即DESY方法和Cornell方法的原理,建模分析和比较了两种方法的计算精度和误差来源,给出Cornell方法调谐量计算的修正。然后结合9-cell超导腔预调谐实验研究,给出了快速预调谐方法:DESY的重建算法在低场平时精度较高且收敛迅速,可作为粗调;Cornell微扰算法在高场平时精度较高且测量迅速,可作为微调。结合两种调谐方式,将预调谐分为粗调和微调两步,可有效提升9-cell超导腔预调谐的速度。     

超导加速器CW模式的高阶模初步分析

 超导加速器由于具有极高的Q值,因此表现出较强的腔束相互作用,尤其是在以CW模式运行下,严重时会产生束流崩溃(BBU)效应。德国TESLA式的9-cell超导串腔在束流负载为1 mA,束团重复频率为81.25 MHz情况下,对其高阶模的产生及相应的功率水平进行了分析。结果表明：对于该腔的主要高阶模,谐振偏差值在π/4以上,束流没有发生谐振,高阶模功率在mW量级。     

超导加速器CW模式的高阶模初步分析

超导加速器由于具有极高的Q值,因此表现出较强的腔束相互作用,尤其是在以CW模式运行下,严重时会产生束流崩溃(BBU)效应。德国TESLA式的9-cell超导串腔在束流负载为1 mA,束团重复频率为81.25 MHz情况下,对其高阶模的产生及相应的功率水平进行了分析。结果表明：对于该腔的主要高阶模,谐振偏差值在π/4以上,束流没有发生谐振,高阶模功率在mW量级。     

β=0.45,f=350MHz spoke腔高阶模的研究

质子或者离子在中低能段的加速结构是目前研究的热点, 其中许多实验结果表明spoke腔是连接RFQ加速结构和椭球腔加速结构的最具潜力的桥梁. 但是这种新型结构仍然存在许多问题有待解决, 为此, 北京大学开展了spoke型质子加速腔的研究, 完成了β=0.45, 频率为350MHz spoke腔的设计和铜模型腔的加工. 重点对spoke腔高阶模进行了分析, 模拟计算找出了几种危害模式, 并完成了实验测量, 取得了实验测量与模拟计算相一致的结果.     

直线对撞机用的RF超导多胞加速腔和陷阱模研究

为下世纪直线对撞机设计了一个9胞RF超导加速腔,其加速模的E_pk/E_acc=2.024.胞-胞间耦合系数高达1.95%.高次模通带分布均匀合理,带间无重叠,不存在陷阱模.CSE新形胞结构也保证了加速腔的机械强度.根据目前可实现的铌腔表面处理技术,束载加速梯度达到25—30MeV/m是可能的.     

X波段加速管加高阶模电场分布的测试

介绍了一种用于测试X波段加速管中高阶模电场分布的笼子式微扰体的研制与标定,该微型拢动体通过专门设计加工的固定装置,在尼龙线表面平行沉积溅射数根金属丝膜制成,利用一标准圆柱腔,对笼子式扰动体的扰动因子进行了定标,证实金属丝笼子式拢动体与同外形尺寸的金属圆筒相比,具有高分辨率、高灵敏度的优点,采用笼子式拢动体测试了一根长30cm的X波段加速管中TM110模的纵向电场分布。     

外腔中半导体二极管激光阵列的高阶侧模锁定

理论分析了外腔较短情况下,宽条半导体二极管激光阵列（LDA）高阶侧模相位锁定的可能性,观察了包含主、旁瓣结构的多侧模远场光强分布。从实验记录结果可以看出,在旁瓣中出现了标志锁相的峰、谷结构,而且该结构的调制度明显高于主瓣中的峰、谷结构的调制度,结果表明：在外腔较短情况下,LDA高阶侧模相位锁定的现象是存在的。     

外腔中半导体二极管激光阵列的高阶侧模锁定

 理论分析了外腔较短情况下,宽条半导体二极管激光阵列（LDA）高阶侧模相位锁定的可能性,观察了包含主、旁瓣结构的多侧模远场光强分布。从实验记录结果可以看出,在旁瓣中出现了标志锁相的峰、谷结构,而且该结构的调制度明显高于主瓣中的峰、谷结构的调制度,结果表明：在外腔较短情况下,LDA高阶侧模相位锁定的现象是存在的。     

Study on the RF performance of 2-cell superconducting cavity

The physical design of the 2-cell superconducting cavity is presented. The RF parameters of the cavity and HOMs （high order modes） are reported. In this paper, we put the emphasis on the analysis of the HOMs and interaction between beam and cavity.     

Study on the RF performance of 2-cell superconducting cavity

The physical design of the 2-cell superconducting cavity is presented.The RF parameters of the cavity and HOMs (high order modes) are reported.In this paper,we put the emphasis on the analysis of the HOMs and interaction between beam and cavity.     

Measuring the performance of the coaxial HOM coupler on a 2-cell TESLA-shape copper cavity

Coaxial High Order Mode (HOM) couplers have been fabricated at Peking University and their RF performance has been measured on a test device consisting of a coaxial transmission line and a 2-cellTESLA-shape copper cavity. The test results on the 2-cell TESLA-shape copper cavity with HOM couplers indicate that the coupler can cut off the fundamental mode TM010 and absorb HOMs effectively after a careful adjustment. The optimal angle of the HOM coupler with the beam tube is found. The initial test results of HOM couplers are presented in this paper.     

Measuring the performance of the coaxial HOM coupler on a 2-cell TESLA-shape copper cavity

Coaxial High Order Mode （HOM） couplers have been fabricated at Peking University and their RF performance has been measured on a test device consisting of a coaxial transmission line and a 2-cell TESLA-shape copper cavity. The test results on the 2-cell TESLA-shape copper cavity with HOM couplers indicate that the coupler can cut off the fundamental mode TM010 and absorb HOMs effectively after a careful adjustment. The optimal angle of the HOM coupler with the beam tube is found. The initial test results of HOM couplers are presented in this paper.     

Improvements of performance on sputter-coated niobium films for superconducting cavities by adding a NbN interlayer

A new type of superconducting film is studied at Peking University in order to improve the properties of sputter-coated films for superconducting cavities. NbN film and NbN–Nb film have been prepared by DC diode sputtering technology at certain nitrogen content and temperature. NbN film is prepared between copper and Nb film as a barrier against copper diffusion into Nb. Micro-structure analyses show that the NbN–Nb films grow well on the copper substrate. The T_c of the Cu–NbN–Nb increases to 9.5 K compared to the 9.2 K transition temperature of bulk Nb.     

Free‐electron laser multiplex driven by a superconducting linear accelerator

Free‐electron lasers (FELs) generate femtosecond XUV and X‐ray pulses at peak powers in the gigawatt range. The FEL user facility FLASH at DESY (Hamburg, Germany) is driven by a superconducting linear accelerator with up to 8000 pulses per second. Since 2014, two parallel undulator beamlines, FLASH1 and FLASH2, have been in operation. In addition to the main undulator, the FLASH1 beamline is equipped with an undulator section, sFLASH, dedicated to research and development of fully coherent extreme ultraviolet photon pulses using external seed lasers. In this contribution, the first simultaneous lasing of the three FELs at 13.4 nm, 20 nm and 38.8 nm is presented.     

Charge order driven by Fermi-arc instability and its connection with pseudogap in cuprate superconductors

The recently discovered charge order is a generic feature of cuprate superconductors, however, its microscopic origin remains debated. Within the framework of the fermion-spin theory, the nature of charge order in the pseudogap phase and its evolution with doping are studied by taking into account the electron self-energy (then the pseudogap) effect. It is shown that the antinodal region of the electron Fermi surface is suppressed by the electron self-energy, and then the low-energy electron excitations occupy the disconnected Fermi arcs located around the nodal region. In particular, the charge order state is driven by the Fermi-arc instability, with a characteristic wave vector corresponding to the hot spots of the Fermi arcs rather than the antinodal nesting vector. Moreover, although the Fermi arc increases its length as a function of doping, the charge order wave vector reduces almost linearity with the increase of doping. The theory also indicates that the Fermi arc, charge order and pseudogap in cuprate superconductors are intimately related to each other, and all of them emanates from the electron self-energy due to the interaction between electrons by the exchange of spin excitations.     

Excited state biexcitons in monolayer WSe2 driven by vertically grown graphene nanosheets with high-density electron trapping edges

Interface engineering in atomically thin transition metal dichalcogenides (TMDs) is becoming an important and powerful technique to alter their properties, enabling new optoelectronic applications and quantum devices. Interface engineering in a monolayer WSe₂ sample via introduction of high-density edges of standing structured graphene nanosheets (GNs) is realized. A strong photoluminescence (PL) emission peak from intravalley and intervalley trions at about 750 nm is observed at the room temperature, which indicated the heavily p-type doping of the monolayer WSe₂/thin graphene nanosheet-embedded carbon (TGNEC) film heterostructure. We also successfully triggered the emission of biexcitons (excited state biexciton) in a monolayer WSe₂, via the electron trapping centers of edge quantum wells of a TGNEC film. The PL emission of a monolayer WSe₂/GNEC film is quenched by capturing the photoexcited electrons to reduce the electron-hole recombination rate. This study can be an important benchmark for the extensive understanding of light–matter interaction in TMDs, and their dynamics.     

Pairing symmetry in layered BiS2 compounds driven by electron-electron correlation

We investigate the pairing symmetry of layered BiS2 compomlds by assuming that electron-electron correlation is still important so that the pairing is rather short range. We lind that the extended .s-wave pairing symmetry always wins over d-wave when the pairing is confined between two short range sites up to next nearest neighbors. The pairing strength is peaked around the doping level ：r = 0.5. which is consistent with experimental observation. The extended s-wave pairing symmetry is very robust against spin orbital coupling because it is mainly determined by the structure of Fermi surfaces, Moreover. the extended s-wave pafiring can be distinguished from conventional swave pairing by measuring and comparing superconducting gaps of different Fermi surfaces.     

Magnetic order driven by orbital ordering in the semiconducting KFe1.5Se2

The two-orbital Hubbard model is studied numerically by using the Hartree-Fock approximation in both real space and momentum space, and the ground-state properties of the alkali metal iron selenide semiconducting KFe_1.5Se₂ are investigated. A rhombus-type Fe vacancy order with stripetype antiferromagnetic (AFM) order is found, as was observed in neutron scattering experiments [J. Zhao, et al., Phys. Rev. Lett. 109, 267003 (2012)]. Hopping parameters are obtained by fitting the experimentally observed stripe AFM phase in real space. These hopping parameters are then used to study the ground-state properties of the semiconductor in momentum space. It is found to be a strongly correlated system with a large on-site Coulomb repulsion U, similar to the AFM Mott insulator — the parent compound of copper oxide superconductors. We also find that the electronic occupation numbers and magnetizations in the d_xz and d_yz orbitals become different simultaneously when U>U_c (～3.4 eV), indicating orbital ordering. These results imply that the rotational symmetry between the two orbitals is broken by orbital ordering and thus drives the strong anisotropy of the magnetic coupling that has been observed by experiments and that the stripe-type AFM order in this compound may be caused by orbital ordering together with the observed large anisotropy.