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Journal articles on the topic 'Synchrotron radiation'

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Published: 4 June 2021
Last updated: 12 June 2025

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1

MIYAHARA, Tsuneaki. "Synchrotron Radiation. II. Synchrotron Radiation. 2. Optics for Synchrotron Radiation." RADIOISOTOPES 47, no. 1 (1998): 79–84. http://dx.doi.org/10.3769/radioisotopes.47.79.

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2

UJIHIRA, Yusuke. "Synchrotron Radiation. I. Synchrotron Radiation - Approach." RADIOISOTOPES 47, no. 1 (1998): 56–65. http://dx.doi.org/10.3769/radioisotopes.47.56.

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3

HIRANO, Tatsumi. "Synchrotron Radiation. III. Measurement by Synchrotron Radiation. 10. Computed Tomography Using Synchrotron Radiation." RADIOISOTOPES 47, no. 5 (1998): 446–51. http://dx.doi.org/10.3769/radioisotopes.47.446.

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4

TANAKA, Hitoshi. "Synchrotron Radiation. II. Synchrotron Radiation. 1. Accelerators Operated as a Synchrotron Radiation Source." RADIOISOTOPES 47, no. 1 (1998): 66–78. http://dx.doi.org/10.3769/radioisotopes.47.66.

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5

Pérez, Serge, and Daniele de Sanctis. "Glycoscience@Synchrotron: Synchrotron radiation applied to structural glycoscience." Beilstein Journal of Organic Chemistry 13 (June 14, 2017): 1145–67. http://dx.doi.org/10.3762/bjoc.13.114.

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Synchrotron radiation is the most versatile way to explore biological materials in different states: monocrystalline, polycrystalline, solution, colloids and multiscale architectures. Steady improvements in instrumentation have made synchrotrons the most flexible intense X-ray source. The wide range of applications of synchrotron radiation is commensurate with the structural diversity and complexity of the molecules and macromolecules that form the collection of substrates investigated by glycoscience. The present review illustrates how synchrotron-based experiments have contributed to our understanding in the field of structural glycobiology. Structural characterization of protein–carbohydrate interactions of the families of most glycan-interacting proteins (including glycosyl transferases and hydrolases, lectins, antibodies and GAG-binding proteins) are presented. Examples concerned with glycolipids and colloids are also covered as well as some dealing with the structures and multiscale architectures of polysaccharides. Insights into the kinetics of catalytic events observed in the crystalline state are also presented as well as some aspects of structure determination of protein in solution.
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6

Henderson, Richard, and Mejd Alsari. "Radiation Sources in Structural Biology." Scientific Video Protocols 1, no. 1 (2020): 1–3. http://dx.doi.org/10.32386/scivpro.000023.

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What is radiation damage? Are electrons more suitable than X-rays in structural biology? Richard Henderson talks about synchrotron radiation and how cryo-EM laboratories are being established at synchrotrons as national research facilities.
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7

NAKAGAWA, Atsushi. "Synchrotron Radiation." Journal of Synthetic Organic Chemistry, Japan 54, no. 5 (1996): 384–94. http://dx.doi.org/10.5059/yukigoseikyokaishi.54.384.

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8

Ternov, I. M. "Synchrotron radiation." Uspekhi Fizicheskih Nauk 165, no. 4 (1995): 429. http://dx.doi.org/10.3367/ufnr.0165.199504c.0429.

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9

HARA, MASAHIRO. "Synchrotron radiation." Review of Laser Engineering 21, no. 1 (1993): 126–32. http://dx.doi.org/10.2184/lsj.21.126.

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10

Winick, Herman. "Synchrotron Radiation." Scientific American 257, no. 5 (1987): 88–99. http://dx.doi.org/10.1038/scientificamerican1187-88.

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11

Hofmann, A. "Synchrotron Radiation." Reviews of Accelerator Science and Technology 01, no. 01 (2008): 121–41. http://dx.doi.org/10.1142/s1793626808000071.

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The physics of synchrotron radiation, undulator radiation, and free electron lasers is reviewed with an emphasis on the underlying physical principles and the experimental observables, such as the radiation spectrum, angular distribution, and radiation polarization.
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12

NISHINO, Takashi. "Synchrotron Radiation." Kobunshi 55, no. 4 (2006): 285–89. http://dx.doi.org/10.1295/kobunshi.55.285.

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13

Ternov, I. M. "Synchrotron radiation." Physics-Uspekhi 38, no. 4 (1995): 409–34. http://dx.doi.org/10.1070/pu1995v038n04abeh000082.

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14

Kapadia, Phiroze. "Synchrotron Radiation." Optics & Laser Technology 36, no. 6 (2004): 516. http://dx.doi.org/10.1016/j.optlastec.2004.02.010.

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15

ISHII, Takehiko. "Synchrotron Radiation Spectroscopy I. Properties of Synchrotron Radiation." Journal of the Spectroscopical Society of Japan 35, no. 1 (1986): 82–95. http://dx.doi.org/10.5111/bunkou.35.82.

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16

OHTA, Toshiaki. "Synchrotron Radiation. III. Measurement by Synchrotron Radiation. 2. XAFS." RADIOISOTOPES 47, no. 3 (1998): 233–39. http://dx.doi.org/10.3769/radioisotopes.47.233.

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17

Chen Jie, 陈杰, 叶恺容 Ye Kairong, and 冷用斌 Leng Yongbin. "Development of Shanghai Synchrotron Radiation Facility synchrotron radiation interferometer." High Power Laser and Particle Beams 23, no. 1 (2011): 179–84. http://dx.doi.org/10.3788/hplpb20112301.0179.

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18

Bagrov, Vladislav, Anna Kasatkina, and Alexey Pecheritsyn. "Effective Angle of Synchrotron Radiation." Symmetry 12, no. 7 (2020): 1095. http://dx.doi.org/10.3390/sym12071095.

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An exact analytical expression for the effective angle is determined for an arbitrary energy value of a radiating particle. An effective angle of instantaneous power is defined for synchrotron radiation in the framework of classical electrodynamics. This definition explicitly contains the most symmetric distribution of half the total of the instantaneous power of synchrotron radiation. Two exact analytical expressions for the effective angle are considered for the arbitrary energy values of a radiating particle, and the second expression brings to light the exact asymptotics of the effective angle in the ultrarelativistic limit.
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19

IIDA, Atsuo. "Synchrotron Radiation. III. Measurement by Synchrotron Radiation. 6. Synchrotron X-Ray Fluorescence Spectrometry." RADIOISOTOPES 47, no. 4 (1998): 336–43. http://dx.doi.org/10.3769/radioisotopes.47.336.

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20

Hirosawa, Ichiro. "Synchrotron Radiation as Analytical Tools for Industrial Materials ～Synchrotron Radiation and Synchrotron Facilities～." Materia Japan 58, no. 7 (2019): 391–94. http://dx.doi.org/10.2320/materia.58.391.

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21

Fernandez-Palomo, Cristian, Zacharenia Nikitaki, Valentin Djonov, Alexandros G. Georgakilas, and Olga A. Martin. "Non-Targeted Effects of Synchrotron Radiation: Lessons from Experiments at the Australian and European Synchrotrons." Applied Sciences 12, no. 4 (2022): 2079. http://dx.doi.org/10.3390/app12042079.

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Studies have been conducted at synchrotron facilities in Europe and Australia to explore a variety of applications of synchrotron X-rays in medicine and biology. We discuss the major technical aspects of the synchrotron irradiation setups, paying specific attention to the Australian Synchrotron (AS) and the European Synchrotron Radiation Facility (ESRF) as those best configured for a wide range of biomedical research involving animals and future cancer patients. Due to ultra-high dose rates, treatment doses can be delivered within milliseconds, abiding by FLASH radiotherapy principles. In addition, a homogeneous radiation field can be spatially fractionated into a geometric pattern called microbeam radiotherapy (MRT); a coplanar array of thin beams of microscopic dimensions. Both are clinically promising radiotherapy modalities because they trigger a cascade of biological effects that improve tumor control, while increasing normal tissue tolerance compared to conventional radiation. Synchrotrons can deliver high doses to a very small volume with low beam divergence, thus facilitating the study of non-targeted effects of these novel radiation modalities in both in-vitro and in-vivo models. Non-targeted radiation effects studied at the AS and ESRF include monitoring cell–cell communication after partial irradiation of a cell population (radiation-induced bystander effect, RIBE), the response of tissues outside the irradiated field (radiation-induced abscopal effect, RIAE), and the influence of irradiated animals on non-irradiated ones in close proximity (inter-animal RIBE). Here we provide a summary of these experiments and perspectives on their implications for non-targeted effects in biomedical fields.
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22

Nelson, Robert W., and Ira Wasserman. "Synchrotron radiation with radiation reaction." Astrophysical Journal 371 (April 1991): 265. http://dx.doi.org/10.1086/169889.

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23

Peter, William, and Anthony L. Peratt. "Thermalization of synchrotron radiation from field-aligned currents." Laser and Particle Beams 6, no. 3 (1988): 493–501. http://dx.doi.org/10.1017/s0263034600005413.

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Three-dimensional plasma simulations of interacting galactic-dimensioned current filaments show bursts of synchroton radiation of energy density 1·2 ×10−13 erg/cm3 which can be compared with the measured cosmic microwave background energy density of 1·5 × 10−13 erg/cm3. However, the synchrotron emission observed in the simulations is not blackbody. In this paper, we analyze the absorption of the synchrotron emission by the current filaments themselves (i.e., self-absorption) in order to investigate the thermalization of the emitted radiation. It is found that a large number of current filaments (>1031) are needed to make the radiation spectrum blackbody up to the observed measured frequency of 100 GHz. The radiation spectrum and the required number of current filaments is a strong function of the axial magnetic field in the filaments.
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24

Viani, Giuseppe, and Giorgio Margaritondo. "Synchrotron Radiation Facilities." Science 255, no. 5052 (1992): 1626. http://dx.doi.org/10.1126/science.255.5052.1626.b.

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25

Hirshfield, J. L. "Synchrotron-radiation laser." Physical Review Letters 68, no. 6 (1992): 792–95. http://dx.doi.org/10.1103/physrevlett.68.792.

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26

Aginian, M. A., S. G. Arutunian, E. G. Lazareva, and A. V. Margaryan. "SUPERLUMINAL SYNCHROTRON RADIATION." Resource-Efficient Technologies, no. 4 (December 26, 2018): 19–25. http://dx.doi.org/10.18799/24056537/2018/4/216.

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To avoid complex computations based on wide Fourier expansions, the electromagnetic field of synchrotron radiation (SR) was analyzed using Lienard–Wiechert potentials in this work. The retardation equation was solved for ultrarelativistic movement of rotating charge at distances up to the trajectory radius. The radiation field was determined to be constricted into a narrow extended region with transverse sizes approximately the radius of trajectory divided by the particle Lorentz factor (characteristic SR length) cubed in the plane of trajectory and the distance between the observation and radiation emission point divided by the Lorentz factor in the vertical direction. The Lienard–Wiechert field of rotating charge was visualized using a parametric form to derive electric force lines rather than solving a retardation equation. The electromagnetic field of a charging point rotating at superluminal speeds was also investigated. This field, dubbed a superluminal synchrotron radiation (SSR) field by analogy with the case of a circulating relativistic charge, was also presented using a system of electric force lines. It is shown that SSR can arise in accelerators from “spot” of SR runs faster than light by outer wall of circular accelerator vacuum chamber. Furthermore, the mentioned characteristic lengths of SR in orbit plane and in vertical direction are less than the interparticle distances in real bunches in ultrarelativistic accelerators. It is indicating that this phenomenon should be taken into account when calculating bunch fields and involved at least into the beam dynamic consideration.
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27

McDonald;, K. T. "Synchrotron-Cerenkov Radiation." Science 303, no. 5656 (2004): 310c—311. http://dx.doi.org/10.1126/science.303.5656.310c.

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28

Wille, K. "Synchrotron radiation sources." Reports on Progress in Physics 54, no. 8 (1991): 1005–67. http://dx.doi.org/10.1088/0034-4885/54/8/001.

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29

Lieu, R. "Synchrotron radiation reaction." Journal of Physics A: Mathematical and General 20, no. 9 (1987): 2405–13. http://dx.doi.org/10.1088/0305-4470/20/9/027.

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30

Tomaschitz, Roman. "Tachyonic synchrotron radiation." Physica A: Statistical Mechanics and its Applications 335, no. 3-4 (2004): 577–610. http://dx.doi.org/10.1016/j.physa.2003.11.016.

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31

Helliwell, John R. "Synchrotron radiation facilities." Nature Structural Biology 5, no. 8 (1998): 614–17. http://dx.doi.org/10.1038/1307.

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32

WILSON, ELIZABETH K. "SYNCHROTRON RADIATION SHINES." Chemical & Engineering News 79, no. 3 (2001): 44. http://dx.doi.org/10.1021/cen-v079n003.p044.

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33

VIANI, G., and G. MARGARITONDO. "Synchrotron Radiation Facilities." Science 255, no. 5052 (1992): 1626. http://dx.doi.org/10.1126/science.255.5052.1626-a.

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34

Marks, N. "Synchrotron radiation sources." Radiation Physics and Chemistry 45, no. 3 (1995): 315–31. http://dx.doi.org/10.1016/0969-806x(95)92798-4.

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35

Kapitza, S. P. "Induced synchrotron radiation." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 261, no. 1-2 (1987): 43. http://dx.doi.org/10.1016/0168-9002(87)90559-6.

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36

ATODA, Nobufumi. "Synchrotron radiation lithography." Hyomen Kagaku 7, no. 1 (1986): 83–90. http://dx.doi.org/10.1380/jsssj.7.83.

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37

YAMADA, Tadatoshi, and Masatomi IWAMOTO. "Synchrotron Radiation Source." Journal of the Society of Mechanical Engineers 92, no. 848 (1989): 622–24. http://dx.doi.org/10.1299/jsmemag.92.848_622.

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38

Afanasiev, G. N., V. G. Kartavenko, and Yu P. Stepanovsky. "On synchrotron radiation." Journal of Physics D: Applied Physics 33, no. 15 (2000): 1803–16. http://dx.doi.org/10.1088/0022-3727/33/15/309.

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39

Aginian, M. A., S. G. Arutunian, E. G. Lazareva, and A. V. Margaryan. "SUPERLUMINAL SYNCHROTRON RADIATION." Resource-Efficient Technologies, no. 4 (December 26, 2018): 19–27. http://dx.doi.org/10.18799/24056529/2018/4/216.

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To avoid complex computations based on wide Fourier expansions, the electromagnetic field of synchrotron radiation (SR) was analyzed using Lienard–Wiechert potentials in this work. The retardation equation was solved for ultrarelativistic movement of rotating charge at distances up to the trajectory radius. The radiation field was determined to be constricted into a narrow extended region with transverse sizes approximately the radius of trajectory divided by the particle Lorentz factor (characteristic SR length) cubed in the plane of trajectory and the distance between the observation and radiation emission point divided by the Lorentz factor in the vertical direction. The Lienard–Wiechert field of rotating charge was visualized using a parametric form to derive electric force lines rather than solving a retardation equation. The electromagnetic field of a charging point rotating at superluminal speeds was also investigated. This field, dubbed a superluminal synchrotron radiation (SSR) field by analogy with the case of a circulating relativistic charge, was also presented using a system of electric force lines. It is shown that SSR can arise in accelerators from “spot” of SR runs faster than light by outer wall of circular accelerator vacuum chamber. Furthermore, the mentioned characteristic lengths of SR in orbit plane and in vertical direction are less than the interparticle distances in real bunches in ultrarelativistic accelerators. It is indicating that this phenomenon should be taken into account when calculating bunch fields and involved at least into the beam dynamic consideration.
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40

SAKAI, Nobuhiko. "Synchrotron Radiation. III. Measurement by Synchrotron Radiation. 8. Compton Scattering." RADIOISOTOPES 47, no. 4 (1998): 353–62. http://dx.doi.org/10.3769/radioisotopes.47.353.

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41

SATOW, Yoshinori. "Synchrotron Radiation. VI. Analyses of Biological Samples Using Synchrotron Radiation." RADIOISOTOPES 48, no. 6 (1999): 421–28. http://dx.doi.org/10.3769/radioisotopes.48.421.

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42

Kvick, Å. "Synchrotron Radiation and Instrumentation at the European Synchrotron Radiation Facility." Acta Physica Polonica A 82, no. 1 (1992): 7–12. http://dx.doi.org/10.12693/aphyspola.82.7.

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43

OHTSUKA, Sadanori, and Yasuro SUGISHITA. "Synchrotron Radiation. VI. Analyses of Biological Samples Using Synchrotron Radiation. 5. Cardiovascular Imaging by Using Synchrotron Radiation." RADIOISOTOPES 47, no. 12 (1998): 976–81. http://dx.doi.org/10.3769/radioisotopes.47.12_976.

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44

MATSUBAYASHI, Nobuyuki. "Synchrotron Radiation. IV. Study on Physical Property by Synchrotron Radiation. 3. Study on Catalysts by Synchrotron Radiation." RADIOISOTOPES 47, no. 7 (1998): 590–96. http://dx.doi.org/10.3769/radioisotopes.47.590.

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45

KUBOZONO, Yoshihiro. "Synchrotron Radiation. IV. Study on Physical Property by Synchrotron Radiation. 4. Study of Fullerenes by Synchrotron Radiation." RADIOISOTOPES 47, no. 8 (1998): 634–41. http://dx.doi.org/10.3769/radioisotopes.47.634.

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46

KAWASAKI, Koichi. "Synchrotron Radiation. IV. Study on Physical Property by Synchrotron Radiation. 7. Dynamic Observation Using by Synchrotron Radiation." RADIOISOTOPES 47, no. 8 (1998): 656–62. http://dx.doi.org/10.3769/radioisotopes.47.656.

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47

TAKAKURA, Kaoru. "Synchrotron Radiation. VI. Analyses of Biological Samples Using Synchrotron Radiation. 3. Research on Radiation Damage to DNA Using Synchrotron Radiation." RADIOISOTOPES 47, no. 11 (1998): 872–82. http://dx.doi.org/10.3769/radioisotopes.47.11_872.

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48

Ebrahim, Ali, Tadeo Moreno-Chicano, Martin V. Appleby, et al. "Dose-resolved serial synchrotron and XFEL structures of radiation-sensitive metalloproteins." IUCrJ 6, no. 4 (2019): 543–51. http://dx.doi.org/10.1107/s2052252519003956.

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An approach is demonstrated to obtain, in a sample- and time-efficient manner, multiple dose-resolved crystal structures from room-temperature protein microcrystals using identical fixed-target supports at both synchrotrons and X-ray free-electron lasers (XFELs). This approach allows direct comparison of dose-resolved serial synchrotron and damage-free XFEL serial femtosecond crystallography structures of radiation-sensitive proteins. Specifically, serial synchrotron structures of a heme peroxidase enzyme reveal that X-ray induced changes occur at far lower doses than those at which diffraction quality is compromised (the Garman limit), consistent with previous studies on the reduction of heme proteins by low X-ray doses. In these structures, a functionally relevant bond length is shown to vary rapidly as a function of absorbed dose, with all room-temperature synchrotron structures exhibiting linear deformation of the active site compared with the XFEL structure. It is demonstrated that extrapolation of dose-dependent synchrotron structures to zero dose can closely approximate the damage-free XFEL structure. This approach is widely applicable to any protein where the crystal structure is altered by the synchrotron X-ray beam and provides a solution to the urgent requirement to determine intact structures of such proteins in a high-throughput and accessible manner.
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49

Eichhorn, Klaus D. "Single-crystal X-ray diffractometry using synchrotron radiation." European Journal of Mineralogy 9, no. 4 (1997): 673–92. http://dx.doi.org/10.1127/ejm/9/4/0673.

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50

BABA, Yuji. "Synchrotron Radiation. III. Measurement by Synchrotron Radiation. 3. Auger Electron Spectrometry." RADIOISOTOPES 47, no. 3 (1998): 240–47. http://dx.doi.org/10.3769/radioisotopes.47.240.

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