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1 lf-absorption effect, typical for low-energy beta particles.
2 f secondary electrons in c-Si by the primary beta-particles.
3 varied significantly in their absorption of beta-particles.
5 ionuclides that emit low-energy electrons or beta particles (169Er, 117mSn, and 33p) were evaluated.
6 tent cytotoxicity of alpha-particles than of beta-particles, (211)At-labeled agents may be ideal for
7 increase the steady-state level of apo B100-beta particles above that of apo B100 particles in contr
9 bution of a radioisotope that emits alpha or beta particles, and show empirically that the null funct
11 the Au-198 isotope; the range of the (198)Au beta-particle (approximately 11 mm in tissue or approxim
12 gations, recent calculations have shown that beta particles, because of their helicity, radiolyse L-
13 tion of whether absorption and scattering of beta-particles by stent struts will cause significant pe
16 models, radionuclide S values (electron and beta particle components only) were subsequently calcula
23 EG) chains linked to DOTA for complexing the beta-particle emitter (177)Lu and to panitumumab for tar
24 notherapy with these bsRICs labeled with the beta-particle emitter (177)Lu or the Auger electron-emit
26 stantial dosimetric advantage over energetic beta-particle emitters (e.g., 32p, 89Sr, 186Re) for irra
27 delivered by Ab LL1, both Auger electron and beta-particle emitters can produce specific and effectiv
28 a large dosimetric advantage over energetic beta-particle emitters for alleviating bone pain, and po
31 kill than other Auger electron emitters and beta-particle emitters, using an anti-CD74 antibody (Ab)
34 as to evaluate the dose-related effects of a beta-particle-emitting radioactive stent in a porcine co
36 Cerenkov luminescence, the light produced by beta-particle-emitting radionuclides such as clinical po
37 ivo bremsstrahlung with the high-energy pure beta-particle-emitting radionuclides used for therapeuti
38 rivascular space of vessels treated with the beta-particle-emitting stent compared with control vesse
39 e of low-dose endovascular irradiation via a beta-particle-emitting stent inhibits neointimal formati
40 estigate whether low-dose irradiation from a beta-particle-emitting stent would inhibit neointimal pr
41 % versus 36.0 +/- 10.7%, P = .02) within the beta-particle-emitting stents compared with the control
45 erwent placement of 35 nonradioactive and 39 beta-particle-emitting stents with activity levels of 23
46 166Ho with beta-emission (half-life, 26.8 h; beta-particle energies, 1.85 MeV [51%] and 1.77 MeV [48%
49 rrow are comparable to the mean range of the beta particles for a wide variety of beta-emitting radio
50 Moreover, autoradiography, which recorded beta particles from (198)Au, enabled visualizing the het
51 ere obtained with only a few hundred emitted beta particles from the (90)Y/(90)Sr source or conversio
53 biologic effectiveness equivalent to that of beta particles) from a low-dose rate 137Cs irradiator.
54 imaging system comprising a microchip and a beta-particle imaging camera permitted routine cell-base
55 mity to the radioisotope convert the emitted beta(-) particles into photons having wavelengths in the
56 erential response to the doses of continuous beta-particle irradiation used in this experimental mode
62 t localizes in skeletal metastases and emits beta particles that may be therapeutically beneficial.
63 d with no therapy, alpha- ((149)Tb-cm09) and beta(-)-particle therapy ((161)Tb-cm09) resulted in a ma
66 dition, the cross-fire effect of high-energy beta(-)-particles within the bone and the marrow may del
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