戻る
「早戻しボタン」を押すと検索画面に戻ります。 [閉じる]

コーパス検索結果 (１語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します
1  (192)Ir (15 Gy delivered 2 mm away from the radiation source).
2  matrix environment and a tunable narrowband radiation source.
3 se of active interrogation using an external radiation source.
4 onary artery segments by using a synchrotron radiation source.
5 exposed to 10 Gy WBI using Cesium-137 as the radiation source.
6 ies with the help of a tunable synchrotron X-radiation source.
7 ary intervention but were not covered by the radiation source.
8 ter-based intervention and the length of the radiation source.
9 ation of the haversian canals as a potential radiation source.
10 radiation, and at same dose rates using same radiation source.
11 ature diffraction images irrespective of the radiation source.
12 roperties of the crystals rather than to the radiation source.
13 esearch Institute high level cobalt-60 gamma-radiation source.
14 ate for a miniaturized solid-state cyclotron radiation source.
15 sented in the manuscript using four pairs of radiation sources.
16 ving organisms that are regularly exposed to radiation sources.
17 m and is therefore well suited for broadband radiation sources.
18 he development of tunable and multifrequency radiation sources.
19 ned from the same volunteers and ultraviolet radiation sources.
20 is a feature hard to mimic with conventional radiation sources.
21 duced neutron flux of both moving and static radiation sources.
22 act and industrially robust accelerators and radiations sources.
23 ent doses (10, 20, and 50 Gy) from different radiation sources (60)Co or (137)Cs).
24                             At a synchrotron radiation source, a crystal with a tetragonal space grou
25  the first step demonstration towards GW THz radiation source and GV/m THz wakefield accelerator.
26 entional echocardiographer to stand near the radiation source and patient, the primary source of scat
27 latter models were determined using in-house radiation source and the X-ray dose received by Pdx crys
28 red vessel is irradiated, using a variety of radiation sources and delivery systems.
29                      Advances in synchrotron radiation sources and detector technology are pushing th
30 l light-matter interactions to make brighter radiation sources and unleash unprecedented control over
31 ing the X-ray optical problem at synchrotron radiation sources and X-ray free-electron lasers.
32 ures of merit indicate that the data of both radiation sources are of equivalent quality.
33 energies, suggesting that laser plasma based radiation sources are promising for advanced application
34 lopment of compact laser-driven particle and radiation sources, as well as investigations of some lab
35          Here we propose a tunable polarized radiation source based on a helical plasma undulator in
36 of an efficient, megawatt coherent Cherenkov radiation source based on a two-dimensional periodic sur
37 n the ID14B BioCARS (Consortium for Advanced Radiation Sources) beamline at the Advanced Photon Sourc
38 ial as the basis for next generation compact radiation sources because of their extremely high accele
39 or dipole magnet beamline at the synchrotron radiation source BESSY II is about 4.3 nm.
40  facilities worldwide as complementary space radiation sources can help alleviate the shortage of ava
41 sing the latest third-generation synchrotron radiation sources, can be inverted to obtain full three-
42 ich take advantage of the latest synchrotron radiation sources, can be used to obtain quantitative th
43  A solid-state implementation of a cyclotron radiation source consisting of arrays of semicircular ge
44                                   Inadequate radiation source coverage of the injured segment (GM) ha
45  of three exposures on alternating days to a radiation source covering a cumulative UVR exposure rang
46 he ever-increasing brightness of synchrotron radiation sources demands improved X-ray optics to utili
47 LPP) for extreme ultraviolet (EUV) and X-ray radiation sources due to the expected plasma conditions
48                   The impact of all relevant radiation sources during different stages of the operati
49    The high brilliance of modern synchrotron radiation sources facilitates experiments with high-ener
50                          Sadly, conventional radiation sources (gamma or X rays, electrons) used for
51 raction studies carried out at a synchrotron radiation source have allowed the structure solution and
52 , the doors of the world's first synchrotron radiation source have closed.
53 evices; sensors; field emission displays and radiation sources; hydrogen storage media; and nanometer
54 t with simulated free-moving single detector radiation source imaging scenarios.
55 rapeutic NM procedures without shielding the radiation source in the 1980s (HR, 1.32; 95% CI: 1.04, 1
56 arrangement is a novel optical recombination radiation source in which the electrons and holes are in
57 each conducted respective assessments of all radiation sources in the United States and worldwide.
58 use in vacuum experimental chambers of X-ray radiation sources including the newly developed, first-o
59 s show reasonable response under a series of radiation sources, including (241)Am and (57)Co radiatio
60 ions in free electron lasers and synchrotron radiation source injectors.
61  is a well-established method at synchrotron radiation sources, its near-field analog has received le
62 r constitutes a millimetre-sized synchrotron radiation source of X-rays.
63                  Next-generation synchrotron radiation sources, such as X-ray free-electron lasers, e
64 resolved experiments can be conducted at the radiation source that best matches the desired time reso
65 y unexposed buttock skin with an ultraviolet radiation source that complied with European recommendat
66      In outer space, protons are the primary radiation source that poses a range of potential health
67 rt an injectable nanoparticle-based internal radiation source that potentially offers more efficaciou
68                    Furthermore, for ionizing radiation sources that cannot be imaged using these stan
69 ized to predict a new path towards nonlinear radiation sources that combine resonant upconversion wit
70  Importantly, in addition to the synchrotron radiation source, this approach has been demonstrated fo
71 d at the output facet of any electromagnetic radiation source to deflect electromagnetic waves at a d
72 l, compared with the cell size, and when the radiation sources were on the cell surface.
73                          Two electromagnetic radiation sources were used to irradiate the lower back
74 lecular crystals at the CXLS and synchrotron radiation sources, which holds enormous potential for ad
75 iheterodyne techniques using frequency combs-radiation sources whose lines are perfectly evenly-space
76                        We demonstrate that a radiation source with millimeter size and peak brillianc
77 f a tungsten lamp as an inexpensive infrared radiation source, with cooling effected with a solenoid-
78 option allows simultaneously two independent radiation sources, with a full coverage of the EUV (2.5