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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
7                                 The low 238U/3He component may be in the associated depleted refracto
8 ances of the light elements and isotopes 2H, 3He, 4He and 7Li.
9    Although the primordial abundances of 2H, 3He, 4He, and 7Li inferred from current observational da
10             Dynamic hyperpolarized helium 3 (3He) magnetic resonance (MR) imaging of the human airway
11                    Two-dimensional helium-3 (3He) provides a simple model for the experimental invest
12 o reservoirs of B-phase superfluid helium-3 (3He-B) were made over a wide range of temperatures.
13                                  Apatite 4He/3He thermochronometry tightly constrains the timing and
14 independently predicts both the dominant 4He/3He peak found in modern mid-ocean-ridge basalts, as wel
15 lts, as well as estimates of the initial 4He/3He ratio of the Earth.
16         Here I show that the spectrum of 4He/3He ratios in ocean island basalts appears to preserve t
17                        This indicates that a 3He-recharged depleted mantle (HRDM) reservoir may be th
18 pact structure contain trapped helium with a 3He/4He ratio of 5.5 x 10(-4) to 5.9 x 10(-4).
19 not for healthy volunteers (P=.35), although 3He and 129Xe VDPs showed a significant correlation for
20 s-adduct, 3, from macrocyclic malonate 1 and 3He@C60 was proven by 3He NMR.
21                  We used 5704 14C, 10Be, and 3He ages that span the interval from 10,000 to 50,000 ye
22 ography and FAB-MS, as well as IR and 1H and 3He NMR spectroscopies.
23 at 76% and 4He at 24% by mass through 2H and 3He at parts in 105 down to 7Li at parts in 1010.
24 tions of 3-methyl-2-cyclohexenone to C70 and 3He@C70 have been studied by a combination of HPLC chrom
25 y greater (P=.01) than that for FEV1/FVC and 3He VDP (r=-0.84, P<.0001).
26                        Together, the D/H and 3He/4He ratios are consistent with conversion in the sun
27        Consequently the 40Ar/36Ar ratios and 3He/36Ar ratios (1.45) determined are minimum estimates
28     Ventilation defect percentages (VDPs) at 3He and 129Xe imaging were obtained by using semiautomat
29                 A strong correlation between 3He/4He and 87Sr/86Sr, 143Nd/144Nd and trace element rat
30 ocyclic malonate 1 and 3He@C60 was proven by 3He NMR.
31            We obtained a relatively constant 3He flux over the past 30,000 years.
32                         Solutions containing 3He@C60, 129Xe@C60, and varying amounts of 9,10-dimethyl
33 e sun of protosolar deuterium to present-day 3He.
34 e in the flux of interplanetary dust-derived 3He.
35 claim that all low-mass stars should destroy 3He.
36  most solar-mass stars do not produce enough 3He to enrich the interstellar medium significantly.
37                                       Excess 3He is also present on the same isopycnal between 15°
38 He/4He ratios are due to low 4He, not excess 3He, and do not imply or require a deep or primordial or
39                        This finding excludes 3He as a pacemaker of late Pleistocene glacial cycles.
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
43                       Laser-polarized gases (3He and 129Xe) are currently being used in magnetic reso
44 ence of neutrons from the reaction D + D --&gt; 3He (820 keV) + n (2.45 MeV) within the target is confir
45                                         High 3He/4He gases are viewed as products of ancient gas exso
46                                         High 3He/4He ratios are due to low 4He, not excess 3He, and d
47                                         High 3He/4He ratios at many ocean islands, along with lower a
48                                         High 3He/4He ratios found in ocean island basalts are the mai
49                           Consequently, high 3He/4He ratios in OIBs are conventionally viewed as evid
50                   A depleted source for high 3He/4He ocean island basalts would resolve the apparent
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
54                                     The high 3He/4He ratio of volcanic rocks thought to be derived fr
55                                  The highest 3He/4He basalts from Hawaii and Iceland plot on the obse
56 rdial abundance of 3He relative to hydrogen: 3He/H = (1.1 +/- 0.2) x 10(-5).
57                       VDPs at hyperpolarized 3He and 129Xe imaging were compared with a two-tailed Wi
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
60                     Because IDPs are rich in 3He, seafloor sediment 3He concentrations provide a uniq
61  R can alternatively reflect high integrated 3He/(U+Th) ratios or low 4He abundances, as expected in
62  focused on generating a method to introduce 3He into the vascular system.
63 lity that destroys all of the helium isotope 3He produced during the star's lifetime.
64 re efficient at producing the helium isotope 3He, which they mix into the convective envelope on the
65 lower mantle, rich in the primordial isotope 3He.
66 ondensation, and the fermion systems (liquid 3He, the electrons in some metals), which display the re
67                            A shallow and low 3He source explains the spatial variability and the temp
68  source) with low 3He concentrations and low 3He/4He ratios.
69 depleted upper mantle (MORB source) with low 3He concentrations and low 3He/4He ratios.
70 in Island, Canada, have the highest magmatic 3He/4He ratios yet recorded.
71  less soluble than xenon in these materials, 3He has been used exclusively for imaging air spaces.
72                                      Minimum 3He/4He ratios in surface fluids from the northern Basin
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
75 hat some stars produce prodigious amounts of 3He.
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
78  gradient-echo images (resonant frequency of 3He) were obtained to depict lung ventilation.
79 ars poses to the Big Bang nucleosynthesis of 3He.
80                              Observations of 3He in planetary nebulae, however, indicate that some st
81  bears analogies with the familiar phases of 3He and 4He (the only known zero-temperature liquids), b
82      However, considering that the signal of 3He is more than 10 times greater than that of 129Xe for
83 solubility issue by producing suspensions of 3He microbubbles.
84                             The technique of 3He NMR was used to confirm the selective formation of s
85                                   The use of 3He NMR was especially powerful in determining the regio
86 ascular images obtained with laser-polarized 3He.
87            After inhalation of the polarized 3He gas, single breath-hold, gradient-echo images (reson
88 ind these models is that excess "primordial" 3He is responsible for 3He/4He ratios higher than the av
89                                    The ratio 3He/4He (R) plays a central role in models of mantle evo
90                             At finer scales, 3He/4He variations along mid-ocean ridges have been rela
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
95 ce experiment involving a liquid: superfluid 3He.
96  was discovered in a weak link of superfluid 3He, which is characterized by a 'p-wave' order paramete
97                          Rather, it supports 3He as a constant flux parameter in paleoclimatic studie
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
102                                          The 3He abundance in star-forming (H II) regions agrees with
103                                          The 3He bilayer system can be driven toward a quantum critic
104                                          The 3He/4He ratio exceeds the accepted solar wind value by 2
105                                          The 3He/4He ratios in the Sudbury fullerenes are similar to
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
108 e pattern with periodicity determined by the 3He quantum of circulation.
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
111 , with time, generate inhomogeneities in the 3He/4He ratio.
112 ontrol parameter is the total density of the 3He film.
113                               Results of the 3He NMR experiments conducted on the product mixture imp
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
116           Ventilation and diffusion-weighted 3He MR images were obtained in healthy subjects: 11 smok
117        Through the use of diffusion-weighted 3He MR imaging, Fain et al in this issue of Radiology de
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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