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1 low field anomaly does not contribute to the magnetic susceptibility.
2  phase directly relates to local bulk tissue magnetic susceptibility.
3 lies near 150 K in both resistivity and d.c. magnetic susceptibility.
4 ption spectroscopy, and variable-temperature magnetic susceptibility.
5 ercent total organic matter, grain size, and magnetic susceptibility.
6 en evolution, DSC, optical spectroscopy, and magnetic susceptibility.
7 ment with previous studies on the hemoglobin magnetic susceptibility.
8 and trace metal chemistry, bulk density, and magnetic susceptibility.
9 cyclic voltammetry, and variable-temperature magnetic susceptibility.
10 heme tissue iron, deoxyhemoglobin, and their magnetic susceptibilities.
11 was found that dendrite structure shows good magnetic susceptibility (180.2 emu/g).
12 ts, which behave differently as shown by the magnetic susceptibility analysis, while the Fe(II) (LS,
13 celles) that have positive anisotropy of the magnetic susceptibility and align with their normals par
14 ctivity in compressed lithium is observed by magnetic susceptibility and electrical resistivity measu
15                     In particular, Evans NMR magnetic susceptibility and EPR measurements indicate th
16                         Variable-temperature magnetic susceptibility and EPR spectroscopy measurement
17 contained in the frequency dependence of the magnetic susceptibility and in its high frequency or adi
18 erized by solid state X-ray crystallography, magnetic susceptibility and LIII-edge XANES spectroscopy
19 ue to the dramatically enhanced out-of-phase magnetic susceptibility and magnetically tailored AC/DC
20                               Fits to the DC magnetic susceptibility and magnetization data for 1 sho
21                                           Dc magnetic susceptibility and magnetization measurements r
22 g process, which is represented by dynamical magnetic susceptibility and maximized at phase transitio
23                                              Magnetic susceptibility and Mossbauer spectroscopy revea
24 y shifts originating from local variation in magnetic susceptibility and other sources have greatly i
25  volume differences, and both its Pauli-like magnetic susceptibility and resistivity are an order of
26                                              Magnetic susceptibility and resistivity measurements are
27  by complementary electrical resistivity, ac magnetic susceptibility and single-crystal neutron diffr
28 pendicular magnetic field depending on their magnetic susceptibility and size and on the flow rate.
29 gnetization with a tangential loss in the ac-magnetic susceptibility and the Mydosh parameter (phi =
30                    At lower temperatures, ac magnetic susceptibility and variable field heat capacity
31 licate columns using sequential extractions, magnetic susceptibility and X-ray absorption spectroscop
32 t parameters (radius, length, Young modulus, magnetic susceptibility) and, using these values, we fou
33 n examined using magnetic criteria, NICS and magnetic susceptibility, and by structural criteria, HOM
34  the many tissue parameters, such as T1, T2, magnetic susceptibility, and chemical shift, that contri
35 absorption near-edge structure spectroscopy, magnetic susceptibility, and complete active space self-
36 lvated framework is supported by structural, magnetic susceptibility, and computational studies.
37                              Mossbauer, EPR, magnetic susceptibility, and DFT studies of the unusual
38 examined with X-ray and neutron diffraction, magnetic susceptibility, and electrical resistivity meas
39 cence efficiency, electron mobility, doping, magnetic susceptibility, and electrocatalytic performanc
40  sample temperature gradient and anisotropic magnetic susceptibility, and present a refined high-reso
41 ich is confirmed by the zero resistivity, AC magnetic susceptibility, and specific heat measurements.
42 ted-state lifetime, electron spin resonance, magnetic susceptibility, and structural data all suggest
43 y, magnetic circular dichroism spectroscopy, magnetic susceptibility, and transmission electron micro
44 py, elemental analysis, variable-temperature magnetic susceptibility, and UV-visible-NIR spectroscopy
45 rast agents reveals unexpected trends in the magnetic susceptibility anisotropy that cannot be explai
46 fferent external alignment media and also by magnetic susceptibility anisotropy.
47                        Temperature-dependent magnetic susceptibilities are reported for all complexes
48  of sigma(RT) = 0.03 S/cm and the Pauli-like magnetic susceptibility are best described by the resona
49 es such as X-ray absorption spectroscopy and magnetic susceptibility are complicated by contributions
50                               While 1/T2 and magnetic susceptibility are not equivalent measures of t
51 ie-Weiss law observed in the low-temperature magnetic susceptibility, are consistent with the presenc
52 on spin relaxivity, magnetic anisotropy, and magnetic susceptibilities argues for a low-spin, (d(xy))
53 The alpha-phase shows a broad maximum in the magnetic susceptibility around 8 K that, coupled with a
54 tense signal on FLAIR images can result from magnetic susceptibility artifacts, CSF/vascular pulsatio
55 t is undersampled in neuroimaging because of magnetic susceptibility artifacts.
56                  In addition, probing the ac magnetic susceptibility as a function of both temperatur
57                        Temperature dependent magnetic susceptibility as well as field dependent magne
58 ransition is a rather abrupt decrease in the magnetic susceptibility at 210 K followed by a steady de
59  We report a paramagnetic singularity in the magnetic susceptibility at low magnetic fields that pers
60    Both clusters exhibit high solution-phase magnetic susceptibility at room temperature, suggesting
61 FM correlation with a characteristic peak in magnetic susceptibility at T'(N).
62 fy microcirculation in breast neoplasms with magnetic susceptibility-based contrast material-enhanced
63 erivatives through template destruction, and magnetic susceptibility behaviors.
64  signal phase does not depend on tissue bulk magnetic susceptibility but tissue magnetic architecture
65  deposits produces moderately high values of magnetic susceptibility, but magnetite is absent in near
66 strate a virtually universal HN form for the magnetic susceptibility chi (omega, T), a general KWW fo
67 olenoid to avoid line broadening from volume magnetic susceptibility (chi v) mismatches at both ends
68                                              Magnetic susceptibility (chi) data for Y(3)MnAu(5) were
69  produce a significant temperature-dependent magnetic susceptibility, chi(T), in both alpha-Pu and de
70 nstead contain paramagnetic salts with molar magnetic susceptibilities (chim) approximately approxima
71 ramagnetism characteristic of a metal with a magnetic susceptibility, chip approximately 4.5x10(-4) e
72                        Orientation-dependent magnetic susceptibility (chiT) and magnetization (M(H))
73 dichroism, transmission electron microscopy, magnetic susceptibility, cobalt K-shell X-ray absorption
74 ctra, combined with quantitative analysis of magnetic susceptibilities, confirmed that the manganese
75 echo planar imaging combined with a bolus of magnetic susceptibility contrast agent; and (b) diffusio
76 ') component of the alternating current (ac) magnetic susceptibility data and by the appearance of hy
77               Thus, the variable-temperature magnetic susceptibility data are well described by a Hei
78     Variable temperature direct current (dc) magnetic susceptibility data collected in the 1.8-300 K
79                                Mossbauer and magnetic susceptibility data demonstrate that this mater
80                                  Solid-state magnetic susceptibility data establish the complexes hav
81                                          The magnetic susceptibility data exhibit a negative Curie te
82                    The temperature-dependent magnetic susceptibility data for 2 reveals that an excit
83                                 A fit to the magnetic susceptibility data for 2, gives J = -113 cm(-1
84                         Variable-temperature magnetic susceptibility data for crystalline 1 and 2 est
85 lecular structures and temperature-dependent magnetic susceptibility data for several new metal compl
86                         Variable-temperature magnetic susceptibility data have established 1 to posse
87                                          The magnetic susceptibility data in the temperature range 4-
88                                              Magnetic susceptibility data indicate that there is net
89                         Variable-temperature magnetic susceptibility data indicates a well-isolated S
90                         Variable-temperature magnetic susceptibility data indicates that the exchange
91  1/T2 (with repetition time of 700 msec) and magnetic susceptibility data led to a slight increase in
92                    In this case, fitting the magnetic susceptibility data requires use of two couplin
93                                              Magnetic susceptibility data reveal a well-isolated S =
94          Solution-phase variable-temperature magnetic susceptibility data reveal weak ferromagnetic s
95                 At very low temperatures, ac magnetic susceptibility data show the magnetic relaxatio
96 rature dependence of the resistivity and the magnetic susceptibility data suggest Ce(3+/4+) valence f
97 ange [D] = 0.44-0.72 cm(-1), and fits to the magnetic susceptibility data yield exchange coupling con
98                          Structural details, magnetic susceptibility data, and Mossbauer spectra demo
99  and Mossbauer spectroscopies, together with magnetic susceptibility data, confirm the strong binding
100 facilitated accurate interpretation of their magnetic susceptibility data.
101 ge term was required for the best fit of the magnetic susceptibility data.
102 g, indicating some paramagnetism verified by magnetic susceptibility data.
103 les in temperature-dependent resistivity and magnetic susceptibility data.
104 frequency shift (fL) and quantitative volume magnetic susceptibility (Deltachi).
105                                     Solution magnetic susceptibility demonstrates that [Cp' '(2)Zr](2
106 arisons of microhemorrhage number, size, and magnetic susceptibility derived from quantitative suscep
107  a field mapping pulse sequence yielding the magnetic susceptibility difference between blood in the
108 t, resulting in low temperature anomalies in magnetic susceptibility, electrical resistivity, and hea
109 of information from UV-vis-NIR spectroscopy, magnetic susceptibility, electrochemistry, resonance Ram
110 y absorption spectroscopy, a chemical assay, magnetic susceptibility, electron paramagnetic resonance
111 V-vis spectroscopy, EPR, cyclic voltammetry, magnetic susceptibility, electrospray mass spectrometry
112 rum at 77 K, but it can be observed by using magnetic susceptibility, EPR at approximately 8 K, and m
113                   Using variable-temperature magnetic susceptibility, EPR hyperfine coupling constant
114 rido species that on the basis of Mossbauer, magnetic susceptibility, EPR, and X-ray absorption in co
115                               Calculation of magnetic susceptibility exaltation using the CSGT (conti
116 Deltar(m), Julg A, HOMA) and magnetic (NICS, magnetic susceptibility exaltation) criteria of aromatic
117 ow an excellent linear relationship with the magnetic susceptibility exaltation, Lambda, for neutral,
118 dependent chemical shifts (NICS(1)(zz)), and magnetic susceptibility exaltation, Lambda, supported th
119 cleus-independent chemical shifts, NICS, and magnetic susceptibility exaltation, Lambda.
120 eus independent chemical shifts, and through magnetic susceptibility exaltation.
121 d shifting in 4 are highly aromatic based on magnetic susceptibility exaltations.
122   The X-ray crystallographic structures, the magnetic susceptibilities from 2 to 300 K, and a theoret
123                  In addition, the densities, magnetic susceptibilities, glass transition temperatures
124 us and inhomogeneous magnetic fields and the magnetic susceptibility gradient across the wave front.
125  (137)Cs), Hg, and main sediment parameters (magnetic susceptibility, grain size, dry bulk density, m
126 d syndrome had increased (more paramagnetic) magnetic susceptibilities in the basal ganglia.
127 ompare the paramagnetic contribution to cell magnetic susceptibility in erythrocytes differing in the
128      Here we address this issue by measuring magnetic susceptibility in the two most studied spin-ice
129 issue magnetic architecture--distribution of magnetic susceptibility inclusions (lipids, proteins, ir
130                                              Magnetic susceptibility increases with temperature above
131 erties of these nanocrystals were studied by magnetic susceptibility, magnetic circular dichroism (MC
132 tructure from X-ray and neutron diffraction, magnetic susceptibility, magnetization, and electrical r
133 ompound to be a p-type semiconductor while a magnetic susceptibility measurement shows technetium dic
134  X-ray crystallography, variable-temperature magnetic susceptibility measurement, cyclic voltammetry,
135 ition above 80 K as inferred by the dc SQUID magnetic susceptibility measurement.
136  transition near 100 K was observed in their magnetic susceptibility measurement.
137                                              Magnetic susceptibility measurements (SQUID) confirm the
138  variable-temperature Raman spectroscopy and magnetic susceptibility measurements a thermally accessi
139                         Variable temperature magnetic susceptibility measurements agree very well wit
140 t study and comparison of the performance of magnetic susceptibility measurements and a newly propose
141 powder and single crystal X-ray diffraction, magnetic susceptibility measurements and density functio
142 identify with X-ray absorption spectroscopy, magnetic susceptibility measurements and density functio
143               Variable temperature dc and ac magnetic susceptibility measurements and field-dependent
144                        Temperature-dependent magnetic susceptibility measurements and Mossbauer data
145  state of the diradicals has been studied by magnetic susceptibility measurements and theoretical cal
146     IR, UV-vis/NIR, and variable-temperature magnetic susceptibility measurements are also reported.
147                                           As magnetic susceptibility measurements are easily acquired
148 erized by X-ray powder diffraction, TEM, and magnetic susceptibility measurements as a function of te
149                                 In all cases magnetic susceptibility measurements confirm the presenc
150                                              Magnetic susceptibility measurements confirmed the singl
151                                           Dc magnetic susceptibility measurements demonstrate the pre
152                      Variable-temperature dc magnetic susceptibility measurements demonstrate the pre
153 tron microscopy, Mossbauer spectroscopy, and magnetic susceptibility measurements demonstrated that i
154                                              Magnetic susceptibility measurements for 1 were fitted t
155                                      EPR and magnetic susceptibility measurements for 5 indicate that
156 opy, electronic absorption spectroscopy, and magnetic susceptibility measurements have been performed
157 ssbauer spectroscopic characterizations, and magnetic susceptibility measurements have been used for
158     Variable-temperature alternating current magnetic susceptibility measurements imply that both 1 a
159                          Direct current (DC) magnetic susceptibility measurements in the temperature
160                                              Magnetic susceptibility measurements indicate approximat
161                                           Ac magnetic susceptibility measurements indicate field-depe
162                                           Ac magnetic susceptibility measurements indicate the absenc
163                                              Magnetic susceptibility measurements of all samples sugg
164                                              Magnetic susceptibility measurements of Na4ZnU6F30 yield
165                               Significantly, magnetic susceptibility measurements of these complexes
166          Variable-temperature direct current magnetic susceptibility measurements on 2 indicate a par
167                         Variable-temperature magnetic susceptibility measurements on alpha-1b indicat
168                                Transport and magnetic susceptibility measurements on Li17Ag3Sn6 indic
169 etrahedral arrangement; this is evidenced by magnetic susceptibility measurements on the La(21)Fe(8)S
170                                Results of ac magnetic susceptibility measurements performed on the tr
171                            For [U@Bi12](3-), magnetic susceptibility measurements rationalize an unpr
172                                           Dc magnetic susceptibility measurements reveal a spontaneou
173                                              Magnetic susceptibility measurements reveal Eu(2+) groun
174 SiMe3)3)2](-), for which alternating current magnetic susceptibility measurements reveal slow magneti
175                        Solid state dc and ac magnetic susceptibility measurements reveal that each Mn
176                                           Dc magnetic susceptibility measurements reveal the presence
177 )H NMR spectroscopy, VT crystallography, and magnetic susceptibility measurements revealed that ((Ar)
178                        Solid-state dc and ac magnetic susceptibility measurements revealed that [Mn(3
179                  As expected, the results of magnetic susceptibility measurements show no evidence fo
180                                 Both EPR and magnetic susceptibility measurements show no measurable
181  nitroxide CH3 contacts, but polycrystalline magnetic susceptibility measurements show quite small an
182                                              Magnetic susceptibility measurements show that 10 is a d
183 d high temperatures and variable-temperature magnetic susceptibility measurements show that a low-spi
184                 X-ray powder diffraction and magnetic susceptibility measurements show that Ag(pyz)(2
185                                              Magnetic susceptibility measurements show that all the c
186                                              Magnetic susceptibility measurements show that the radic
187            Consistent with these results, AC magnetic susceptibility measurements show the molecule t
188                         Variable-temperature magnetic susceptibility measurements were performed on b
189 litting parameters, and variable-temperature magnetic susceptibility measurements were used to evalua
190 agnetic relaxation barrier (determined by ac magnetic susceptibility measurements) between a negligib
191 nsuperimposed) PLY rings, and the structure, magnetic susceptibility measurements, and band structure
192  has been monitored by optical spectroscopy, magnetic susceptibility measurements, and single crystal
193 emperature crystallography, resistivity, and magnetic susceptibility measurements, and these results
194                                       The ac magnetic susceptibility measurements, collected in a sma
195 omenon is supported by temperature-dependent magnetic susceptibility measurements, differential scann
196 resolution synchrotron X-ray diffraction and magnetic susceptibility measurements, that cooling the r
197               Using muon spin relaxation and magnetic susceptibility measurements, we demonstrate her
198 ance spectroscopies and variable-temperature magnetic susceptibility measurements, we found that holo
199 ough comparisons with non-radical-bridged ac magnetic susceptibility measurements, we show that the m
200 havior of the iron site was characterized by magnetic susceptibility measurements, which indicate a v
201 d by single crystal X-ray diffraction and ac magnetic susceptibility measurements.
202 tively, and are confirmed by resistivity and magnetic susceptibility measurements.
203 pectroscopy, NMR, X-ray crystallography, and magnetic susceptibility measurements.
204 ition, a spin glass behavior is indicated by magnetic susceptibility measurements.
205  X-ray analysis, Mossbauer spectroscopy, and magnetic susceptibility measurements.
206 y, and variable-temperature conductivity and magnetic susceptibility measurements.
207 p'3Ln, have been characterized via dc and ac magnetic susceptibility measurements.
208 scopy, single crystal X-ray diffraction, and magnetic susceptibility measurements.
209 es, electron spin resonance data, and static magnetic-susceptibility measurements.
210                                          The magnetic susceptibility method probes the magnetic respo
211                                              Magnetic susceptibility, Mossbauer, and neutron diffract
212                                              Magnetic susceptibility (MS) has been proposed as an ine
213  are those with positive anisotropy of their magnetic susceptibility, namely Eu3+, Er3+, Tm3+, and Yb
214 pectra and solid-state temperature-dependent magnetic susceptibilities of 1 and 2, in addition to X-r
215 les were 2.0 and 4.5 microm in diameter with magnetic susceptibilities of 1.12 x 10(-4) and 1.6 x 10(
216 res above Tc, the model matches the measured magnetic susceptibilities of crystalline EuO, Gd, Co and
217 d to hemozoin, calculated based on the known magnetic susceptibilities of hemoglobin heme and hemozoi
218                                          The magnetic susceptibilities of hexanuclear gadolinium clus
219 -temperature EPR spectra of 1(1+) and 1(2+), magnetic susceptibility of 1(1+) and 1(2+), Mossbauer sp
220                        The solid-state molar magnetic susceptibility of 3 obeys the Curie-Weiss law w
221    The ionothermal synthesis, structure, and magnetic susceptibility of a novel inorganic-organic hyb
222 notube, and is thought to play a role in the magnetic susceptibility of CNTs and the magnetoresistanc
223                             The experimental magnetic susceptibility of F4BImNN confirms the expectat
224                          The resistivity and magnetic susceptibility of the compound have also been i
225 nd (ii) using weaker magnets or reducing the magnetic susceptibility of the medium destabilizes the m
226    There is a strong correlation between the magnetic susceptibility of the salt solution, its concen
227 e heart was measured ex vivo (n=27), and the magnetic susceptibility of the tissue was estimated thro
228                                    The large magnetic susceptibility of this material leads to an unu
229 xample, by sensitizing the MRI signal to the magnetic susceptibility of tissue, it is starting to bec
230 ccording to their magnetic properties (e.g., magnetic susceptibilities or magnetophoretic mobilities)
231 nd 5,600 y ago, as inferred from sedimentary magnetic susceptibility, oxygen isotopes, and diatom and
232  parts per billion per day +/- 0.14 for mean magnetic susceptibility (P = .016).
233 cterized by experimental (X-ray diffraction, magnetic susceptibility, pulsed-field magnetization, hea
234 centration also was strongly correlated with magnetic susceptibility (r=0.90, P <.001, epsilonRMS=0.1
235 6) mm3 s/kg, corresponding to the net volume magnetic susceptibility (relative to water) of Deltachi
236                Mossbauer spectroscopy and ac magnetic susceptibility reveal that this complex behaves
237                                              Magnetic susceptibility revealed a spin-glass transition
238 gnetic circular dichroism, X-ray absorption, magnetic susceptibility, scanning electron microscopy, a
239                              Analysis of the magnetic susceptibility shows that it is dominated by a
240       Our high precision measurements of the magnetic susceptibility, specific heat, and electrical r
241 the qugate requirements, as revealed through magnetic susceptibility, specific heat, and EPR.
242                         Variable-temperature magnetic susceptibility studies are consistent with stro
243  biofilm inside opaque porous media with low magnetic susceptibilities such as borosilicate or soda l
244 demonstrated that with two-armed probes, the magnetic susceptibility tensor can be predicted with suf
245            This makes the orientation of the magnetic susceptibility tensor differ significantly betw
246                   The axial component of the magnetic susceptibility tensor has been determined indep
247 er, it was found that the orientation of the magnetic susceptibility tensor is pH dependent (pK(a) ap
248                      It also has a different magnetic susceptibility tensor, so by using both tags, t
249  that the anisotropy of the room temperature magnetic susceptibility tensor, which in turn affects th
250         The best results are obtained if the magnetic susceptibility tensors of the tags are known, b
251 ramagnetism characteristic of a metal with a magnetic susceptibility that implies a density of states
252 r composed of material having an anisotropic magnetic susceptibility that is described by a tensor wi
253 Fitting the frequency-dependent out-of-phase magnetic susceptibility to the Arrhenius equation yields
254 trum, as well as the strict adherence of the magnetic susceptibility to the Curie law in the range 30
255 animal model study demonstrate that 1/T2 and magnetic susceptibility values can be used for estimatio
256                   The strongest predictor of magnetic susceptibility was age.
257  and a very large magnetic anisotropy in the magnetic susceptibility was observed.
258                                          The magnetic susceptibility was studied by SQUID measurement
259 f this new Co species at 1958 cm(-1) and its magnetic susceptibility were consistent with Co(I) compo
260 ontrast is attributed to local variations in magnetic susceptibility, which, at least in part, appear
261 idence for a graduated increase of live cell magnetic susceptibility with developing blood-stage para
262 ld theory yields the Curie-Weiss law for the magnetic susceptibility: X(T) infinity 1/(T - Weiss cons
263                           Analysis of the ac magnetic susceptibility yields an effective spin reversa

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