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1  (192)Ir (15 Gy delivered 2 mm away from the radiation source).
2 se of active interrogation using an external radiation source.
3 onary artery segments by using a synchrotron radiation source.
4 exposed to 10 Gy WBI using Cesium-137 as the radiation source.
5 ies with the help of a tunable synchrotron X-radiation source.
6 ary intervention but were not covered by the radiation source.
7 ter-based intervention and the length of the radiation source.
8 ation of the haversian canals as a potential radiation source.
9  matrix environment and a tunable narrowband radiation source.
10 is a feature hard to mimic with conventional radiation sources.
11 he development of tunable and multifrequency radiation sources.
12 ned from the same volunteers and ultraviolet radiation sources.
13                             At a synchrotron radiation source, a crystal with a tetragonal space grou
14 latter models were determined using in-house radiation source and the X-ray dose received by Pdx crys
15 red vessel is irradiated, using a variety of radiation sources and delivery systems.
16                      Advances in synchrotron radiation sources and detector technology are pushing th
17 ing the X-ray optical problem at synchrotron radiation sources and X-ray free-electron lasers.
18 energies, suggesting that laser plasma based radiation sources are promising for advanced application
19 lopment of compact laser-driven particle and radiation sources, as well as investigations of some lab
20          Here we propose a tunable polarized radiation source based on a helical plasma undulator in
21 n the ID14B BioCARS (Consortium for Advanced Radiation Sources) beamline at the Advanced Photon Sourc
22 ial as the basis for next generation compact radiation sources because of their extremely high accele
23 or dipole magnet beamline at the synchrotron radiation source BESSY II is about 4.3 nm.
24  facilities worldwide as complementary space radiation sources can help alleviate the shortage of ava
25 sing the latest third-generation synchrotron radiation sources, can be inverted to obtain full three-
26 ich take advantage of the latest synchrotron radiation sources, can be used to obtain quantitative th
27                                   Inadequate radiation source coverage of the injured segment (GM) ha
28  of three exposures on alternating days to a radiation source covering a cumulative UVR exposure rang
29 he ever-increasing brightness of synchrotron radiation sources demands improved X-ray optics to utili
30                          Sadly, conventional radiation sources (gamma or X rays, electrons) used for
31 raction studies carried out at a synchrotron radiation source have allowed the structure solution and
32 , the doors of the world's first synchrotron radiation source have closed.
33 evices; sensors; field emission displays and radiation sources; hydrogen storage media; and nanometer
34 rapeutic NM procedures without shielding the radiation source in the 1980s (HR, 1.32; 95% CI: 1.04, 1
35 arrangement is a novel optical recombination radiation source in which the electrons and holes are in
36 each conducted respective assessments of all radiation sources in the United States and worldwide.
37 s show reasonable response under a series of radiation sources, including (241)Am and (57)Co radiatio
38 r constitutes a millimetre-sized synchrotron radiation source of X-rays.
39                  Next-generation synchrotron radiation sources, such as X-ray free-electron lasers, e
40 y unexposed buttock skin with an ultraviolet radiation source that complied with European recommendat
41      In outer space, protons are the primary radiation source that poses a range of potential health
42 rt an injectable nanoparticle-based internal radiation source that potentially offers more efficaciou
43                    Furthermore, for ionizing radiation sources that cannot be imaged using these stan
44  Importantly, in addition to the synchrotron radiation source, this approach has been demonstrated fo
45 d at the output facet of any electromagnetic radiation source to deflect electromagnetic waves at a d
46 l, compared with the cell size, and when the radiation sources were on the cell surface.
47                          Two electromagnetic radiation sources were used to irradiate the lower back
48                        We demonstrate that a radiation source with millimeter size and peak brillianc
49 f a tungsten lamp as an inexpensive infrared radiation source, with cooling effected with a solenoid-

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