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Journal articles on the topic 'Wigglers'

Author: Grafiati

Published: 3 June 2025

Last updated: 31 July 2025

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1

Scharlemann, E. T. "Wiggle plane focusing in linear wigglers." Journal of Applied Physics 58, no. 6 (1985): 2154–61. http://dx.doi.org/10.1063/1.335980.

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2

Kang, Y., H. Sun, K. Q. Zhang, and C. Feng. "Recent progress of THz source at the SXFEL." Journal of Physics: Conference Series 2687, no. 3 (2024): 032011. http://dx.doi.org/10.1088/1742-6596/2687/3/032011.

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Abstract Coherent, wide-tunable frequency and high intensity terahertz (THz) source is under preparation at the Shanghai Soft X-ray free-electron laser facility (SXFEL). The electron bunches modulated by frequency beating light can generate coherent, wide-tunable, high intensity THz radiation from 0.1 to 30 THz through wigglers. The electromagnetic wiggler with peak magnetic field up to 1.75 T is adopted and the parameters of the wiggler are optimized to ensure the generation of strong field THz radiation. Due to the limitation of layout space of the SXFEL, the length of wiggler is limited wit

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3

Mezentsev, Nikolay, and Erik Wallén. "Superconducting Wigglers." Synchrotron Radiation News 24, no. 3 (2011): 3–9. http://dx.doi.org/10.1080/08940886.2011.583883.

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4

Ispirian, K. A., and M. K. Ispiryan. "Crystalline wigglers." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 247, no. 2 (2006): 377–80. http://dx.doi.org/10.1016/j.nimb.2006.02.011.

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5

Klementiev, Konstantin, Hamed Tarawneh, and Pedro Fernandes Tavares. "Wiggler radiation at a low-emittance storage ring and its usage for X-ray absorption spectroscopy." Journal of Synchrotron Radiation 29, no. 2 (2022): 462–69. http://dx.doi.org/10.1107/s1600577521012844.

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A wiggler is a high-power insertion device that was used in the past to produce a smooth wide-band X-ray spectrum. It is widely believed that on low-emittance synchrotrons this X-ray source loses its spatial and spectral homogeneity and therefore becomes less ideal than a scanning undulator. In this paper, we report on experimental and computational studies of an in-vacuum wiggler installed on the first fourth-generation synchrotron MAX IV. We investigate how several physical parameters affect the wiggler spectrum and propose a combination of a few of them that results in significant spectral

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6

Levichev, Eugene, and Nikolay Vinokurov. "Undulators and Other Insertion Devices." Reviews of Accelerator Science and Technology 03, no. 01 (2010): 203–20. http://dx.doi.org/10.1142/s1793626810000403.

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This article reviews insertion devices (IDs) — wigglers and undulators — both for synchrotron radiation production and for machine parameter control. As there are many types of wigglers and undulators and it is impossible to describe them all in detail, here we particularly emphasize the design, characteristics and tolerances of undulators for free electron lasers and damping wigglers for controlling beam damping parameters. The influence of periodic IDs on beam parameters in cyclic accelerators is described in brief. A profound description of different ID types can be found in [1].

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7

Matsuzawa, Hidenori, Yoshiharu Ishibashi, Masato Ariizumi, and Hiroshi Saegusa. "HighTcbulk superconductor wigglers." Applied Physics Letters 59, no. 2 (1991): 141–42. http://dx.doi.org/10.1063/1.106000.

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8

Nakajima, Hideki, Siriwat Soontaranon, Noppharit Wasanbongngem, et al. "Magnetic field simulation of in-vacuum permanent magnet multipole wiggler." Journal of Physics: Conference Series 3010, no. 1 (2025): 012007. https://doi.org/10.1088/1742-6596/3010/1/012007.

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Abstract We present the magnetic field simulation and design of a high-field permanent magnet-based in-vacuum multipole wiggler for the Siam Photon Source (SPS). SPS utilizes a 1.2-GeV electron storage ring with a double-bend achromat (DBA) lattice, featuring four long straight sections capable of accommodating insertion devices up to 5 m in length. To generate tender and hard X-ray radiation in this low-energy storage ring, an in-vacuum permanent magnet multipole wiggler is designed as a cost-effective alternative to superconducting wigglers, which are expensive to operate and maintain. The m

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9

Khrushchev, S. V., V. K. Lev, N. A. Mezentsev, E. G. Miginsky, V. A. Shkaruba, and V. M. Tsukanov. "Optimization of wigglers side poles." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 603, no. 1-2 (2009): 19–21. http://dx.doi.org/10.1016/j.nima.2008.12.120.

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10

Vetrovec, John. "Performance model for FEL wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 304, no. 1-3 (1991): 759–64. http://dx.doi.org/10.1016/0168-9002(91)90971-r.

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11

Segall, S. B., and J. F. Ostiguy. "Beam spill in long wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 285, no. 1-2 (1989): 355–63. http://dx.doi.org/10.1016/0168-9002(89)90479-8.

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12

Abbasi, E., S. Jafari, and R. Hedayati. "Interaction of a relativistic dense electron beam with a laser wiggler in a vacuum: self-field effects on the electron orbits and free-electron laser gain." Journal of Synchrotron Radiation 23, no. 6 (2016): 1282–95. http://dx.doi.org/10.1107/s1600577516012601.

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Employing laser wigglers and accelerators provides the potential to dramatically cut the size and cost of X-ray light sources. Owing to recent technological developments in the production of high-brilliance electron beams and high-power laser pulses, it is now conceivable to make steps toward the practical realisation of laser-pumped X-ray free-electron lasers (FELs). In this regard, here the head-on collision of a relativistic dense electron beam with a linearly polarized laser pulse as a wiggler is studied, in which the laser wiggler can be realised using a conventional quantum laser. In add

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13

Kim, S. H. "Classical free-electron lasing in an undulating electrostatic field in the axial direction." Journal of Plasma Physics 47, no. 2 (1992): 197–217. http://dx.doi.org/10.1017/s002237780002417x.

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It is shown that the phase of the electromagnetic wave emitted through stimulated emission is intrinsically random. The insensitivity of the phase of the laser field to any disturbance in the laser cavity parameter derives from the fact that stimulated and spontaneous emissions take place concurrently at the same wave vector, the phases of spontaneous emission are mildly bunched, and the central limit theorem can be applied to the phase of the laser field. The two spectral lines observed in the Smith-Purcell free-electron laser experiment show that both classical and quantum-mechanical free-el

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14

Miao Zhang, Qiaogen Zhou, Zhenmei Qian, Jidong Zhang, and Jie Lu. "Development of Two Wigglers at SSRF." IEEE Transactions on Applied Superconductivity 20, no. 3 (2010): 304–7. http://dx.doi.org/10.1109/tasc.2009.2039013.

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15

Geloni, Gianluca, Vitali Kocharyan, and Evgeni Saldin. "Brightness of synchrotron radiation from wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 807 (January 2016): 13–29. http://dx.doi.org/10.1016/j.nima.2015.10.004.

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16

Halbach, K. "Desirable excitation patterns for tapered wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 250, no. 1-2 (1986): 95–99. http://dx.doi.org/10.1016/0168-9002(86)90867-3.

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17

Calvo, Miguel, and Otto Rendon. "Field configurations in Helical magnetic wigglers." Review of Scientific Instruments 61, no. 1 (1990): 124–28. http://dx.doi.org/10.1063/1.1141887.

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18

Vinokurov, N. A. "Multisegment wigglers for short wavelength FEL." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 375, no. 1-3 (1996): 264–68. http://dx.doi.org/10.1016/0168-9002(95)01349-0.

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19

Musardo, M., T. Tanabe, J. Rank, et al. "Three-pole wigglers at NSLS-II." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 1059 (February 2024): 169008. http://dx.doi.org/10.1016/j.nima.2023.169008.

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20

Koda, Shigeru, Yuichi Takabayashi, Tatsuo Kaneyasu, and Yoshitaka Iwasaki. "Investigation of edge radiation intensification effect generated by periodic alignment of three-pole wigglers." Japanese Journal of Applied Physics 61, no. 3 (2022): 036001. http://dx.doi.org/10.35848/1347-4065/ac4a0a.

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Abstract The intensification effect of edge radiation due to the periodic alignment of three-pole wigglers was analytically and numerically investigated. The general equation of the electric field of the radiation from relativistic an electron passing through the alignment was obtained by using a simple model. The model consists of an alternating alignment of straight sections and large gradient orbit sections due to the three-pole wigglers. Based on the radiation equation, various radiation properties such as spatial distribution and spectrum structure were studied. The angular distribution o

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21

Farla, Robert, Shrikant Bhat, Stefan Sonntag, et al. "Extreme conditions research using the large-volume press at the P61B endstation, PETRA III." Journal of Synchrotron Radiation 29, no. 2 (2022): 409–23. http://dx.doi.org/10.1107/s1600577522001047.

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Penetrating, high-energy synchrotron X-rays are in strong demand, particularly for high-pressure research in physics, chemistry and geosciences, and for materials engineering research under less extreme conditions. A new high-energy wiggler beamline P61 has been constructed to meet this need at PETRA III in Hamburg, Germany. The first part of the paper offers an overview of the beamline front-end components and beam characteristics. The second part describes the performance of the instrumentation and the latest developments at the P61B endstation. Particular attention is given to the unprecede

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22

Shatunov, Yu, I. Koop, A. Otboev, and S. Mane. "High Energy Polarized e+e− Beams." International Journal of Modern Physics: Conference Series 40 (January 2016): 1660089. http://dx.doi.org/10.1142/s2010194516600892.

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Recently, the wide discussion about Higgs-factory design again returns to problem of high energy polarized electrons and positrons. It’s good known the radiative beam polarization at LEP-collider. It was obtained after spin resonance suppression at [Formula: see text] pick, but didn’t appear at energies above 70 GeV due to an enhancement of unavoidable depolarization effects. We examine in this paper various ideas for radiative polarization at TLEP/FCC-ee and formulate some estimates for the polarization buildup time and the asymptotic polarization. Using wigglers, a useful degree of polarizat

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23

Joshi, C., T. Katsouleas, J. Dawson, Y. Yan, and J. Slater. "Plasma wave wigglers for free-electron lasers." IEEE Journal of Quantum Electronics 23, no. 9 (1987): 1571–77. http://dx.doi.org/10.1109/jqe.1987.1073557.

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24

Wang, G. M., T. Shaftan, W. X. Cheng, et al. "Emittance and lifetime measurement with damping wigglers." Review of Scientific Instruments 87, no. 3 (2016): 033301. http://dx.doi.org/10.1063/1.4942903.

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25

Stuart, R. A., and G. Kong. "A magnetic circuit model for electromagnet wigglers." Journal of Physics D: Applied Physics 26, no. 2 (1993): 192–98. http://dx.doi.org/10.1088/0022-3727/26/2/004.

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26

Stuart, R. A., and G. Kong. "A magnetic circuit model for electromagnet wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 318, no. 1-3 (1992): 843–46. http://dx.doi.org/10.1016/0168-9002(92)91172-6.

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27

Zhong-xi, Hui. "High-gain FEL with variable parameter wigglers." International Journal of Infrared and Millimeter Waves 10, no. 6 (1989): 651–60. http://dx.doi.org/10.1007/bf01009566.

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28

Ishibashi, Yoshiharu, Masato Ariizumi, Hiroshi Saegusa, Shinzo Mizukami, and Hidenori Matsuzawa. "Jig for high‐Tc superconductor bulk wigglers." Review of Scientific Instruments 62, no. 5 (1991): 1374–75. http://dx.doi.org/10.1063/1.1142505.

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29

Gilfrich, J. V., E. F. Skelton, S. B. Qadri, N. E. Moulton, D. J. Nagel, and J. Z. Hu. "Micro-X-Ray Fluorescence Analysis on a Synchrotron Radiation Wiggler Beam Line." Advances in X-ray Analysis 35, B (1991): 995–1000. http://dx.doi.org/10.1154/s0376030800013227.

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AbstractIt has been well established over recent years that synchrotron radiation possesses some unique features as a source of primary x-rays for x-ray fluorescence analysis. Advantage has been taken of the high intensity emanating from the bending magnets of storage rings to develop x-ray microprobes utilizing apertures or focussing optics, or both, to provide a beam spot at the specimen of the order of micrometers. The use of insertion devices wigglers and undulatora, can further increase the available intensity, especially for the high energy photons. Beam Line X-17C at the National Synchr

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30

Lyutikov, Maxim. "Coherent Emission in Pulsars, Magnetars, and Fast Radio Bursts: Reconnection-driven Free Electron Laser." Astrophysical Journal 922, no. 2 (2021): 166. http://dx.doi.org/10.3847/1538-4357/ac1b32.

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Abstract We develop a model of the generation of coherent radio emission in the Crab pulsar, magnetars, and fast radio bursts (FRBs). Emission is produced by a reconnection-generated beam of particles via a variant of the free electron laser mechanism, operating in a weakly turbulent, guide field-dominated plasma. We first consider nonlinear Thomson scattering in a guide field-dominated regime, and apply it to explain emission bands observed in Crab pulsar and in FRBs. We consider particle motion in a combined field of the electromagnetic wave and the electromagnetic (Alfvénic) wiggler. Charge

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31

Hartzell, K. R. "A free-electron laser amplifier with variable wigglers." Journal of Physics D: Applied Physics 22, no. 8 (1989): 1042–49. http://dx.doi.org/10.1088/0022-3727/22/8/006.

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32

Tran, T., B. Danly, and J. Wurtele. "Free-electron lasers with electromagnetic standing wave wigglers." IEEE Journal of Quantum Electronics 23, no. 9 (1987): 1578–89. http://dx.doi.org/10.1109/jqe.1987.1073537.

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33

Granatstein, V. L., W. W. Destler, and I. D. Mayergoyz. "Small‐period electromagnet wigglers for free‐electron lasers." Applied Physics Letters 47, no. 6 (1985): 643–45. http://dx.doi.org/10.1063/1.96044.

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34

Riyopoulos, Spilios. "Slow wave wigglers for compact free electron lasers." Physics of Plasmas 2, no. 9 (1995): 3524–30. http://dx.doi.org/10.1063/1.871133.

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35

Fedurin, M., G. Kulipanov, N. Mezentsev, and V. Shkaruba. "Superconducting high-field three-pole wigglers at Budker INP." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 448, no. 1-2 (2000): 51–58. http://dx.doi.org/10.1016/s0168-9002(99)00750-0.

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36

Anacker, D. C., W. Hale, and J. L. Erskine. "An algorithm for computer simulation of undulators and wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 284, no. 2-3 (1989): 514–22. http://dx.doi.org/10.1016/0168-9002(89)90323-9.

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37

Ashkenazy, J., and G. Bekefi. "Analysis and measurements of permanent magnet 'bifilar' helical wigglers." IEEE Journal of Quantum Electronics 24, no. 5 (1988): 812–19. http://dx.doi.org/10.1109/3.197.

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38

Karbushev, N. I. "Free electron lasers with static and dynamic plasma wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 358, no. 1-3 (1995): 437–40. http://dx.doi.org/10.1016/0168-9002(94)01263-6.

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39

Warren, R. W., and C. M. Fortgang. "Fabrication of high-field short-period permanent magnet wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 341, no. 1-3 (1994): 444–48. http://dx.doi.org/10.1016/0168-9002(94)90401-4.

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40

Hajima, Ryoichi, and Fumio Matsuura. "Advanced optimization of permanent magnet wigglers using genetic algorithm." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 375, no. 1-3 (1996): ABS19—ABS21. http://dx.doi.org/10.1016/0168-9002(95)01323-7.

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41

Iwasaki, Yoshitaka, Tatsuo Kaneyasu, Yuichi Takabayashi, Harunobu Takeda, and Shigeru Koda. "Operation of two superconducting wigglers at SAGA Light Source." Journal of Physics: Conference Series 3010, no. 1 (2025): 012021. https://doi.org/10.1088/1742-6596/3010/1/012021.

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Abstract The SAGA Light Source (SAGA-LS) is a compact 1.4 GeV synchrotron radiation facility located in Tosu, Japan. The storage ring in this facility consists of a double-bend lattice having a circumference of 75.6 m. Since the SAGA-LS became available to users in 2006, the facility has provided photon beams over a wide spectral range from vacuum ultraviolet to hard X-rays to both industry and academia. A unique feature of the SAGA-LS is the routine operation of two superconducting wigglers (SCWs). These devices were installed in 2010 and 2016 and have increased the upper limit of the availab

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42

Danly, B., G. Bekefi, R. Davidson, R. Temkin, T. Tran, and J. Wurtele. "Principles of gyrotron powered electromagnetic wigglers for free-electron lasers." IEEE Journal of Quantum Electronics 23, no. 1 (1987): 103–16. http://dx.doi.org/10.1109/jqe.1987.1073205.

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43

Vinokurov, Nikolai A., and Evgeny B. Levichev. "Undulators and wigglers for production of radiation and other applications." Uspekhi Fizicheskih Nauk 185, no. 9 (2015): 917–39. http://dx.doi.org/10.3367/ufnr.0185.201509b.0917.

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44

Anwar, F., C. R. Carlos, V. Saraswat, V. S. Mangu, M. S. Arnold, and F. Cavallo. "Nanoscale graphene/Ge wigglers as building blocks for THz sources." AIP Advances 7, no. 11 (2017): 115015. http://dx.doi.org/10.1063/1.4986513.

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45

Batrakov, A., I. Ilyin, G. Karpov, et al. "Control and data acquisition systems for high field superconducting wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 467-468 (July 2001): 202–5. http://dx.doi.org/10.1016/s0168-9002(01)00274-1.

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46

Pissanetzky, S., and P. Tompkins. "3-D magnetic field calculations for wigglers using magnus-3D." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 285, no. 1-2 (1989): 303–6. http://dx.doi.org/10.1016/0168-9002(89)90470-1.

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47

Bobbs, B. L., G. Rakowsky, P. Kennedy, R. A. Cover, and D. Slater. "In search of a meaningful field-error specification for wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 296, no. 1-3 (1990): 574–78. http://dx.doi.org/10.1016/0168-9002(90)91269-h.

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48

Halbach, K. "Some concepts to improve the performance of dc electromagnetic wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 250, no. 1-2 (1986): 115–19. http://dx.doi.org/10.1016/0168-9002(86)90870-3.

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49

Freund, H. P., H. Bluem, and C. L. Chang. "Three-dimensional simulation of free electron lasers with planar wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 272, no. 1-2 (1988): 556–63. http://dx.doi.org/10.1016/0168-9002(88)90283-5.

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50

Wiedemann, Helmut. "An ultra-low emittance mode for PEP using damping wigglers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 266, no. 1-3 (1988): 24–31. http://dx.doi.org/10.1016/0168-9002(88)90354-3.

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