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

 
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