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  assessment of biological sources of NADPH's high energy electrons.
2             Frozen RNAs were irradiated with high energy electrons.
3 lectric wakefield accelerators as sources of high-energy electrons.
4 nergy protons and an outer zone dominated by high-energy electrons.
5 plasmids were exposed in the frozen state to high-energy electrons.
6  reverse transcriptase, were irradiated with high-energy electrons.
7 ucts of the K92 gene cluster were exposed to high-energy electrons.
8 rozen rabbit immunoglobulin G was exposed to high-energy electrons.
9 pton up-scattering of synchrotron photons by high-energy electrons.
10                     Hard X-rays, produced by high-energy electrons accelerated in the flare(5), requi
11                 In principle, the relatively high energy electron and hole generated by SB-CS within
12  various situations in astrophysics in which high-energy electrons and intense circularly polarized l
13 parated inner zone is composed of commingled high-energy electrons and very energetic positive ions (
14 s also a major source of both NADH and NADPH high-energy electrons, and this role is augmented under
15          These results suggest that relevant high-energy electrons are accelerated by quasi-periodic
16 iation was observed for many organ pairs for high-energy electrons (as would be emitted by nuclides s
17  Purified HL was exposed to various doses of high energy electrons at -135 degrees C; lipase activity
18         Here, we use a picosecond pulse of a high energy electron beam to generate electrons in liqui
19 oying, Hg was evaporated due to the use of a high-energy electron beam and the process was imaged in
20                                              High-energy electron beam and X-ray processing of foods
21  The effects of vacuum packaging followed by high-energy electron beam irradiation on the shelf-life
22 lly and through numerical simulations that a high-energy electron beam is produced simultaneously wit
23 r-diameter pores by using a tightly focused, high-energy electron beam to sputter atoms in 10-nm-thic
24 iently to the pre-compressed fuel core via a high-energy electron beam.
25 mers and terpolymers or via irradiation with high-energy electron-beam or gamma-ray radiations.
26                                              High energy electron beams consisting of a long train of
27  small excitation volume that interacts with high-energy electron beams.
28 r wakefield accelerators (LWFAs) can produce high-energy electron bunches in short distances.
29  structural transition probed via Reflection High Energy Electron Diffraction (RHEED) for the first t
30 film was characterized by in situ reflection high energy electron diffraction and multiple X-ray diag
31 d SrO unit cells aided by in situ reflection high energy electron diffraction monitoring.
32 as revealed by x-ray diffraction, reflection high energy electron diffraction, and transmission elect
33 rystals investigated with in situ reflection high-energy electron diffraction (RHEED) and ex situ ato
34 ion of two in-situ techniques-(a) Reflection high-energy electron diffraction (RHEED) for heteroepita
35          A combination of in-situ reflection high-energy electron diffraction recorded during the gro
36 to the single-cycle nature of the field, the high-energy electron emission is predicted to be confine
37 e cell-killing potential of the short-range, high-energy electrons emitted during the neutron capture
38   A Varian Clinac iX is used to simulate the high-energy electrons emitted from (90)Sr, and a high ef
39 er network (MCN) that converts sunlight into high-energy electrons for CO(2) reduction to CH(3)OH.
40  They play an essential role in accelerating high-energy electrons forming the hazardous radiation be
41  can be understood in detail by tunneling of high-energy electrons from the gate contact to the nanow
42 is was attributed to the transfer of excited high-energy electrons from ZnO to CuSe.
43 ed surface plasmons create a non-equilibrium high-energy electron gas in nanostructures that can be i
44  in the nanocrystals yields fluorescence and high energy electrons giving rise to structural damage t
45                       Radiotherapy with very high energy electrons has been investigated for a couple
46 role of radicals generated via radiolysis by high-energy electrons in modifying galvanic reactions.
47  electron microscopy is the damage caused by high-energy electrons interacting with any sample.
48 p-Bi 6p bonding, accelerating the filling of high-energy electrons into the pai* orbital of N(2), lea
49  species must originate from collisions with high-energy electrons, ions or particles from a hot plas
50 noscale particles leads to the production of high-energy electrons, ions, neutral atoms, neutrons and
51                                 By employing high-energy electron-loss signals (of several hundred eV
52                                By scattering high-energy electrons off a proton we are able to resolv
53 inately fast neutrons generated by impinging high-energy electrons onto a tantalum convertor are mode
54 used primarily on alkali metal ionization or high-energy electrons or photons.
55 e chorus is instrumental in the formation of high-energy electrons outside the plasmasphere, whereas
56 uded in the design of the next generation of high-energy electron-positron colliders.
57 rements confirmed the existence of Jupiter's high-energy electron-radiation belts, with evidence for
58 nstrating that a substantial fraction of the high-energy electrons responsible for the polarized phot
59 amples were irradiated with various doses of high energy electrons; samples were subsequently thawed,
60                                  Here we use high-energy electron scattering measurements that isolat
61                                          Our high-energy electron-scattering measurements using (12)C
62 sent work reveals the potential of BDDL as a high-energy electron source for use with co-catalysts in
63 gnificant cross irradiation was observed for high-energy electrons, such as those from (90)Y or (188)
64   This important wave is known to remove the high-energy electrons that are trapped along the Earth's
65                           Unfortunately, the high-energy electrons that carry this important informat
66 --also known as the Van Allen belts--contain high-energy electrons trapped on magnetic field lines.
67 Energy Electron (VHEE, 50-300 MeV) and Ultra-High Energy Electron (UHEE, > 300 MeV) beams can accurat
68                                         Very High Energy Electron (VHEE) beams are a promising altern
69                                         Very high energy electron (VHEE) beams are an exciting prospe
70 penetrating dose delivery using focused very high energy electron (VHEE) beams using quadrupole magne
71 el to measure DNA damage in response to Very High Energy Electron (VHEE) irradiation at conventional
72                                 Focused Very-High Energy Electron (VHEE, 50-300 MeV) and Ultra-High E
73                                         Very high energy electrons (VHEE) are a potential candidate f
74 asmid DNA irradiations carried out with Very High Energy Electrons (VHEE) over 100-200 MeV at the CLE
75  available for the effect of FLASH with Very High Energy Electrons (VHEE).
76                               Moreover, Very High Energy Electrons (VHEEs) provide more favourable do
77                The increased inertia of very high-energy electrons (VHEEs) due to relativistic effect