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1 3He images were successfully and reproducibly generated
2 3He MR imaging may provide a method for evaluating progr
3 3He NMR spectroscopy has been used to study the equilibr
4 3He NMR was used to determine if the products are a mixt
5 3He/4He ratios for MORBs show both positive and negative
6 3He/4He ratios in many ocean-island basalts (OIBs) that
9 Although the primordial abundances of 2H, 3He, 4He, and 7Li inferred from current observational da
14 independently predicts both the dominant 4He/3He peak found in modern mid-ocean-ridge basalts, as wel
19 not for healthy volunteers (P=.35), although 3He and 129Xe VDPs showed a significant correlation for
24 tions of 3-methyl-2-cyclohexenone to C70 and 3He@C70 have been studied by a combination of HPLC chrom
28 Ventilation defect percentages (VDPs) at 3He and 129Xe imaging were obtained by using semiautomat
38 He/4He ratios are due to low 4He, not excess 3He, and do not imply or require a deep or primordial or
40 ignificant correlation was also observed for 3He and 129Xe ADC (r=0.97, P<.0001); 129Xe ADC was signi
41 t excess "primordial" 3He is responsible for 3He/4He ratios higher than the average for midocean ridg
42 ion coefficients (ADCs) were calculated from 3He (b=1.6 sec/cm2) and 129Xe (b=12 sec/cm2) diffusion-w
44 ence of neutrons from the reaction D + D --> 3He (820 keV) + n (2.45 MeV) within the target is confir
51 mposed on the regional trend are local, high 3He/4He anomalies indicating hidden magmatic activity an
52 eservoir may be the principal source of high 3He/4He in mantle plumes, and may explain why the helium
53 thorium during mantle melting and that high 3He/4He ratios can be preserved in depleted residues of
58 lung periphery, unlike static hyperpolarized 3He MR images on which only the lung periphery is seen.
59 a related but different phenomenon occurs in 3He) may pave the way for a new class of practical rotat
61 R can alternatively reflect high integrated 3He/(U+Th) ratios or low 4He abundances, as expected in
64 re efficient at producing the helium isotope 3He, which they mix into the convective envelope on the
66 ondensation, and the fermion systems (liquid 3He, the electrons in some metals), which display the re
71 less soluble than xenon in these materials, 3He has been used exclusively for imaging air spaces.
73 upper limit for the primordial abundance of 3He relative to hydrogen: 3He/H = (1.1 +/- 0.2) x 10(-5)
74 concile the low observed cosmic abundance of 3He with the predictions of both stellar and Big Bang nu
76 The evidence however favors depletion of 3He and excessive depletion of 4He and, therefore, favor
77 d heavy-fermion behavior in bilayer films of 3He atoms when adsorbed on the surface of graphite prepl
81 bears analogies with the familiar phases of 3He and 4He (the only known zero-temperature liquids), b
88 ind these models is that excess "primordial" 3He is responsible for 3He/4He ratios higher than the av
91 ause IDPs are rich in 3He, seafloor sediment 3He concentrations provide a unique means of probing the
92 fluid-mineral equilibria, phase separation, 3He/heat ratios and fluxes of volatiles from submarine h
93 roscopic quantum systems (such as superfluid 3He and superconducting UGe2), the superconductivity (or
94 This regime has been detected in superfluid 3He, but was hitherto believed to be unobservable, owing
96 was discovered in a weak link of superfluid 3He, which is characterized by a 'p-wave' order paramete
98 129Xe VDP was significantly greater than 3He VDP for patients with COPD (P<.0001) but not for hea
99 e first experimental data demonstrating that 3He gas diffusivity in the acinus of human lung is highl
100 rd theory of stellar evolution predicts that 3He is also produced by solar-type stars, so its abundan
101 Thus, we are able to remove the threat that 3He production in low-mass stars poses to the Big Bang n
106 ) were allowed to reach equilibrium, and the 3He and 129Xe NMR spectra were taken at the same tempera
107 than in local interstellar hydrogen, and the 3He/4He ratio of (1.1 +/- 0.2) x 10(-4) provides a new v
109 l density of all baryons determined from the 3He data is in excellent agreement with the densities ca
110 e remarkably similar event is present in the 3He record 35 Myr ago, but its origin by comet shower or
114 nd trace element ratios demonstrate that the 3He-rich end-member is present in basalts that are deriv
115 um plume is strongest near Hawaii, where the 3He/4He ratio at a depth of about 1100 meters reaches va
118 of uranium and thorium produces 4He, whereas 3He in the Earth's mantle is not produced by radioactive
119 d a similar and significant correlation with 3He VDP (r=-0.84, P<.0001) and 129Xe VDP (r=-0.89, P<.00
120 rameters at the alveolar level obtained with 3He diffusion MRI in healthy human subjects and patients
121 ing was significantly greater than that with 3He MR imaging, suggesting incomplete or delayed filling
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