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1                                              AFM force-spectroscopy results showed that the adhesion
2                                              AFM images can clearly differentiate R from its complex
3                                              AFM images further show polyplexes on the nucleoplasmic
4                                              AFM images show NPCs clogged only with sub-50nm polyplex
5                                              AFM imaging of the MIP film surface indicated changes in
6                                              AFM observations demonstrated that these ZnPcs form diff
7                                              AFM probes with an attached N-cadherin-coated microbead
8                                              AFM pulling on glypican-1 and heparan sulfate for 10 min
9                                              AFM studies of the assembled aggregates revealed that th
10                                              AFM studies with solid-supported mixed monolayers contai
11                                              AFM utilizing VWF-coated 2-mum beads confirmed the weak
12                                              AFM volume analysis indicates that PARP1 binds to DNA at
13                                              AFM, using tips functionalized with immunologically rele
14                                              AFM-based nanomechanical maps revealed significant heter
15                                              AFM-IR applications that will be discussed include those
16                                              AFM-IR thus can provide the spatial resolution of AFM in
17                                              AFM-IR works by using the tip of an AFM probe to locally
18  measurements underlies the definition of 11 AFMs across core and belt regions of human auditory cort
19       From August through December 2014, 120 AFM cases were reported from 34 states.
20                                 In addition, AFM measurements showed a similar decrease, by up to 70%
21                                 In addition, AFM tips functionalized with Dectin-1 revealed that the
22                   Classically one expects an AFM tip interacting with a cell surface to be repelled d
23          AFM-IR works by using the tip of an AFM probe to locally detect thermal expansion in a sampl
24 e detection is unrelated to the radius of an AFM tip and, in fact, a matter of the switched area.
25 ervoir fluids affects the interactions of an AFM tip with a calcite surface, as surrogates for nanoma
26 n techniques we integrated a microbead on an AFM cantilever thus realizing a system to efficiently po
27                         Crystallographic and AFM data were used to build a structural model of a memb
28 -spin coupling drives the concurrent IMT and AFM-to-FM transition, which fosters the near room-T magn
29 ic or chemical interactions between ions and AFM tip.
30 sent a combination of optical microscopy and AFM-IR imaging to characterize OM heterogeneity in an ar
31 res (>100 degrees C), RHEED oscillations and AFM data indicate a transition to a step-flow growth mod
32 anostructures, as revealed by DSC, SAXS, and AFM, were generated.
33 e nanocomposite films as revealed by SEM and AFM images.
34 odified electrodes was studied by FE-SEM and AFM.
35       Scanning electron microscopy (SEM) and AFM imaging of C. albicans confirmed the polymorphic beh
36 anoBioAnalytical platform, combining SPR and AFM, is a suitable method for a sensitive, reproducible,
37 L structures were directly imaged by TEM and AFM, and doped with 4'-(4-benzoate)-(2,2',2''-terpyridin
38  thin film, accompanying an antiferromagnet (AFM) to ferromagnet (FM) phase transition.
39 magnetic (FM) metal to an antiferromagnetic (AFM) insulator at [Formula: see text]21 GPa whose AFM sp
40 metal (Pt) and a bi-axial antiferromagnetic (AFM) dielectric (NiO) can be a source of a coherent THz
41 ipulation of magnetism in antiferromagnetic (AFM) based nanojunctions by purely electric field means
42 portunity of manipulating antiferromagnetic (AFM) states should offer another route for creating a br
43 rmal induced resonance (PTIR), also known as AFM-IR, is a scanning probe technique that provides samp
44   Results in this model of EV-D68-associated AFM provide a rational basis for selecting empirical the
45      The results indicate that the MIP based AFM nanosensor has high sensitivity for the CPX molecule
46                                         Both AFM and Raman analysis confirmed the layer-by-layer fabr
47 th surface glycans were quantified with both AFM and QCM techniques that revealed the presence of var
48                          Pectins analysed by AFM are visualized as individual chains, branched or unb
49 anically labile protein yet characterized by AFM.
50 2.30+/-0.5mgm(-2) of IgGNS1, as confirmed by AFM topography and phase images along with QCM-D.
51 nd NaCl and nonanoic acid (NA) determined by AFM using area (2D) equivalent diameters, similar to con
52 imes higher mean stiffness (as determined by AFM) and 6-13-fold higher ratios of protein over polysac
53 ructure of interfacial water was observed by AFM force spectroscopy.
54 olding intermediate previously undetected by AFM and then measuring the stabilization of calmodulin b
55 face formed during the ORR was visualized by AFM and high-resolution SEM, which also showed approxima
56 he static conformation of VWF, visualized by AFM imaging, we estimate that in VWF multimers approxima
57 from Aspergillus aculeatus and visualized by AFM.
58 , suggesting it still keeps the small canted AFM state.
59                              Antibody-coated AFM probes exhibited strong surface binding to RFPEC mon
60 le streptavidin-biotin linkage to PEG-coated AFM tips enhanced data quality and throughput.
61                             Here, we combine AFM with an electrostatic force microscopy (EFM) method
62  Such efficient SMFS studies on a commercial AFM enable the rapid characterization of macromolecular
63 ity over 100 s when measured on a commercial AFM.
64                       On a modern commercial AFM, these applications and others are now limited by th
65 or modifications of many existing commercial AFMs, making the technique readily available.
66                                      Control AFM experiments on other lipids and at different tempera
67 lls and hydrogels directly from conventional AFM F-Z experiments, thereby creating a common platform
68 of N; (2) demonstration that deltaN/N for CP-AFM junctions is remarkably small (</=2%) and that the l
69 conducting probe atomic force microscopy (CP-AFM) in which an Au-coated tip contacts a self-assembled
70 conducting probe atomic force microscopy (CP-AFM) junctions with 50 nm(2) areas.
71                                      Current AFM setups perform high-throughput probing of living cel
72 well-defined elastic modulus using different AFMs revealed that the uncertainties in the determinatio
73 ans can pave the way toward ultra-low energy AFM-based MeRAM devices.
74 force spectra, facilitated by robot-enhanced AFM, can help reveal the existence of weak stabilizing i
75 mulations and by comparison with the existed AFM techniques on living cells and hydrogels.
76  large out-of-plane (in-plane) MA in the FM (AFM) phase, its magnetization is more rigid to external
77                            In conclusion, FM-AFM enables the physiological and quantitative investiga
78 uency-modulation atomic force microscopy (FM-AFM) and tested it on MDCK polarized monolayers.
79 ct measurement of dynamic contact angles for AFM tips and can also be taken as a general approach for
80 rm the chemical identification inferred from AFM/STM.
81 e spin alignment of interfacial Mn ions from AFM to FM exchange-coupled, while the injection of minor
82  a controllable metamagnetic transition from AFM to FM ordering would open the door to a plethora of
83 m 30 mK to 300 K suggest strongly frustrated AFM interactions on the scale of J/kb approximately 30 K
84 iate magnetic phases between the AFM-b and G-AFM states, which is in contrasted to manganites where a
85  Mott insulating G-type antiferromagnetic (G-AFM) state was found in Ca3(Ru(1-x)Ti(x))2O7 at about x
86                               The AFM-b-to-G-AFM transition in Ca3(Ru(1-x)Ti(x))2O7 happens through a
87 driven Pt layer and polarized along the hard AFM anisotropy axis excites a non-uniform in time preces
88                                           HS-AFM avoids amplification artifacts present in PCR or in
89                                           HS-AFM movies provide unprecedented real-space and real-tim
90 novel high-speed atomic force microscopy (HS-AFM) method to detect and characterize particulate and p
91 esent high-speed atomic force microscopy (HS-AFM) observations of membrane-reconstituted GltPh at wor
92  used high-speed atomic force microscopy (HS-AFM) to directly image enzymatic phospholipid degradatio
93                                       Our HS-AFM set-up is adapted for such biological applications t
94                                      This HS-AFM "nanomapping" technique can be complementary to both
95 osphate to WEOM-adsorbed iron (oxy)hydroxide AFM tips suggesting that the molecular mass of aromatic
96 oom-temperature antiferromagnetic insulator (AFM-I) and the perovskite SrCoO3 that is a ferromagnetic
97                                   Time-lapse AFM imaging, in solution, show that over time, oligomers
98 cies absorb IR photons from a tunable laser, AFM-IR can study particles smaller than the optical diff
99 scopy (AFM) tips are of much concern in many AFM-related measurement, fabrication, and manipulation a
100 ors is presented by magnetic conducting (mc-)AFM measurements, in which chiral and achiral Zn-porphyr
101             A phase transition from metallic AFM-b antiferromagnetic state to Mott insulating G-type
102 ltiple-probes in an atomic force microscope (AFM) or a scanning electron microscope (SEM), optical tw
103          We applied atomic force microscope (AFM) to demonstrate directly that on-surface aggregation
104                  An atomic force microscope (AFM) was employed to further examine the mechano-respons
105                  An Atomic force microscope (AFM) was used to confirm the hybridization.
106 ents, including the atomic force microscope (AFM)(1-4) and optical and magnetic tweezers(5-8), have h
107  nonpolar tip of an atomic force microscope (AFM).
108 oscopic (UV-vis, FTIR, XPS) and microscopic (AFM, SEM, and TEM) techniques.
109                    Atomic Force Microscopic (AFM) and Transmission Electron Microscopic (TEM) images
110 force - scanning electrochemical microscopy (AFM-SECM) imaging of topography and redox species diffus
111 g, HybriD, etc.) of atomic force microscopy (AFM) allow imaging of compositional contrast of (bio)mat
112        In addition, atomic force microscopy (AFM) analysis of WT and TSP2 KO ECM did not reveal diffe
113 icroscopy (SEM) and atomic force microscopy (AFM) analysis, respectively.
114  stiffness, we used atomic force microscopy (AFM) and developed a novel "bed of nails"-like approach
115                     Atomic force microscopy (AFM) and electrochemical techniques including cyclic vol
116                     Atomic force microscopy (AFM) and force spectroscopy have the intrinsic capabilit
117 n microscopy (TEM), atomic force microscopy (AFM) and Fourier transform infrared spectroscopy (FT-IR)
118 was investigated by atomic force microscopy (AFM) and Fourier transform infrared spectroscopy (FTIR)
119                     Atomic force microscopy (AFM) and high resolution transmission electron microscop
120 pectroscopy (FTIR), atomic force microscopy (AFM) and high-resolution scanning transmission electron
121 ms was monitored by atomic force microscopy (AFM) and optical coherence tomography (OCT) during three
122 n microscopy (SEM), atomic force microscopy (AFM) and scanning electrochemical microscopy (SECM).
123                     Atomic force microscopy (AFM) and scanning electron microscopy (SEM) confirmed th
124       Here, we used atomic force microscopy (AFM) and single molecule fluorescence microscopy to exam
125 ace was analyzed by atomic force microscopy (AFM) and the NS1 detection was followed by quartz crysta
126 e reference methods atomic force microscopy (AFM) and thioflavin T (ThT) assay.
127                     Atomic force microscopy (AFM) and transmission electron microscopy (TEM) confirme
128  Here we present an atomic force microscopy (AFM) approach for measuring energy landscapes that incre
129 d non-contact based atomic force microscopy (AFM) approaches have been extensively utilized to explor
130 ntermittent-contact atomic force microscopy (AFM) can detect the Hall effect in conducting domain wal
131     High resolution atomic force microscopy (AFM) confirmed the efficiency of electrode functionaliza
132 icroscopy (SEM) and atomic force microscopy (AFM) feature a uniform and open-networked array of aggre
133                     Atomic force microscopy (AFM) force-distance measurements are used to investigate
134 The analysis of the Atomic Force Microscopy (AFM) images showed two different nanostructures indicati
135               Using atomic force microscopy (AFM) imaging, we show good agreement between the number
136                 The atomic force microscopy (AFM) indentation method combined with the brush model ca
137                     Atomic force microscopy (AFM) measurements in aqueous solutions containing NaCl,
138 ss test method, and atomic force microscopy (AFM) measurements.
139  most commonly used Atomic Force Microscopy (AFM) mode to measure the local, nanoscale elastic proper
140 nation of different atomic force microscopy (AFM) modes to present the first images of three coexisti
141                     Atomic force microscopy (AFM) on wild-type BM in vivo reveals an anterior-posteri
142 croscopy (TEM), and atomic force microscopy (AFM) show that ADH-41 wholly suppresses the aggregation
143 ces by employing an atomic force microscopy (AFM) single-cell force spectroscopy (SCFS) technique.
144 -scale radius of an atomic force microscopy (AFM) tip yields a very low signal-to-noise ratio.
145 tting properties of atomic force microscopy (AFM) tips are of much concern in many AFM-related measur
146         We utilized atomic force microscopy (AFM) to apply force selectively to components of the EGL
147     We then utilize atomic force microscopy (AFM) to demonstrate that the redox state of the [4Fe4S]
148 ce (FD) curve based atomic force microscopy (AFM) to detect a target DNA bound to small (1.4-1.9 mum
149 adhesion assays and atomic force microscopy (AFM) to identify the ligands involved and to quantify th
150         Here we use Atomic Force Microscopy (AFM) to monitor the structural evolution of individual v
151 t combine SECM with atomic force microscopy (AFM) to perform measurements at the nanoscale.
152 ty (XR) and in situ atomic force microscopy (AFM) to probe the calcite (104) - water interface in the
153 ) method coupled to atomic force microscopy (AFM) to quantify and qualify platelet-derived microparti
154        Here, we use atomic force microscopy (AFM) to show that ordered, extensive macromolecular arra
155       Here, we used atomic force microscopy (AFM) to show that the stiffness of the axon plasma membr
156 ft assay (EMSA) and atomic force microscopy (AFM) to show that Ver preferentially binds single-strand
157 ere we used in situ atomic force microscopy (AFM) to study the interactions of ammonium phosphate sol
158             We used atomic force microscopy (AFM) to study their mechanical properties in solution an
159         By applying atomic force microscopy (AFM) to the nuclear envelope and the nuclear pore comple
160 f wet cell walls by atomic force microscopy (AFM) with a stretching device and endoglucanase treatmen
161 h method can be the atomic force microscopy (AFM) working in the force spectroscopy mode combined wit
162 optical microscopy, atomic-force microscopy (AFM), and scanning electron microscopy (SEM).
163 obing measurements, atomic force microscopy (AFM), and scanning transmission electron microscopy (STE
164 n microscopy (SEM), atomic force microscopy (AFM), and synchrotron radiation-X-ray photoelectron spec
165 ium Ion Microscopy, Atomic Force Microscopy (AFM), and Time of Flight-Secondary Ion Mass Spectrometry
166             We used atomic force microscopy (AFM), complemented with electron microscopy, to characte
167             We used atomic force microscopy (AFM), scanning and transmission electron microscopy (SEM
168 nd characterized by atomic force microscopy (AFM), scanning electron microscopy (SEM) and X-ray diffr
169 ray analysis (EDX), atomic force microscopy (AFM), scanning electron microscopy (SEM), UV-Vis spectro
170                     Atomic force microscopy (AFM), surface plasmon resonance (SPR), and molecular sim
171 eric aerosols using atomic force microscopy (AFM), which gives information on both the particle heigh
172 n microscopy (SEM), atomic force microscopy (AFM), X-ray diffraction (XRD), Fourier transform infrare
173 nical rheometry and atomic force microscopy (AFM)-based indentation as reference-standards.
174 , we have performed atomic force microscopy (AFM)-based single-molecule force measurements on dimers,
175                     Atomic force microscopy (AFM)-based single-molecule force spectroscopy (SMFS) is
176                     Atomic force microscopy (AFM)-based single-molecule force spectroscopy (SMFS) is
177 led high-throughput atomic force microscopy (AFM)-based single-molecule force spectroscopy (SMFS) mea
178 een investigated by Atomic Force Microscopy (AFM).
179 troscopy (EIS), and atomic force microscopy (AFM).
180 ng living cells, by atomic force microscopy (AFM).
181 (RHEED) and ex situ atomic force microscopy (AFM).
182 y (EDX) mapping and atomic force microscopy (AFM).
183 tometry (RT-DC) and Atomic Force Microscopy (AFM).
184 croscopy (SEM), and atomic force microscopy (AFM).
185  in live cells with atomic force microscopy (AFM).
186 ron microscopy, and atomic force microscopy (AFM).
187 ovel application of atomic force microscopy (AFM).
188 resonance (TR) mode atomic force microscopy (AFM).
189 icroscopy (TEM) and atomic force microscopy (AFM).
190 d and quantified by atomic force microscopy (AFM).
191 gy was confirmed by Atomic Force Microscopy (AFM).
192 e is explored using atomic force microscopy (AFM).
193 ce microscopy/scanning tunneling microscopy (AFM/STM) experiment can both distinguish neutral O2 mole
194 in piezoresponse force microscopy as a model AFM mode.
195                 In conclusion, PMMA-modified AFM probes have shown to be a reliable technique to char
196 an ultrahigh-resolution frequency modulation-AFM for measuring the effect of two biological osmolytes
197 DSF) are consistent with our single molecule AFM experiments.
198                                    Moreover, AFM measurements demonstrated the modulation of the self
199                                      In most AFM-based measurements, a concurrent electrostatic effec
200 -MS, ion-mobility mass spectrometry (IM-MS), AFM, and TEM.
201 copy, operated in molecule touching mode (Mt/AFM-SECM), and of dense nanodot arrays, for designing an
202       We show that the high resolution of Mt/AFM-SECM enables the electrochemical interrogation of se
203              Overall, we demonstrate that Mt/AFM-SECM enables high throughput reading of dense nanoar
204  (EV-D68)-associated acute flaccid myelitis (AFM) is a devastating neurological disease for which the
205 , pediatric cases of acute flaccid myelitis (AFM) occurred in the United States, coincident with a na
206              The standardized nanomechanical AFM procedure (SNAP) ensures the precise adjustment of t
207                                    Nanoscale AFM results confirm the alteration of crystallographic c
208 s of non-contact Atomic Force Microscopy (nc-AFM) techniques are discussed, as well as the capability
209 ng properties of silicon and silicon nitride AFM tips are investigated through dynamic contact angle
210  step to achieve fully-automated analysis of AFM-generated data.
211                           The application of AFM technologies to study purified HIV-1 cores represent
212 l broadly benefit biological applications of AFM.
213       The subdiffraction limit capability of AFM-IR has the potential to advance understanding of par
214 s study, we present the first combination of AFM with scanning electrochemical microscopy (SECM) in P
215  investigated using force-distance curves of AFM on nanobubbles.
216                          Geometric models of AFM tips were constructed using scanning electronic micr
217 otothermal IR spectroscopy, the potential of AFM-IR is shown for a diverse set of single-component pa
218 R thus can provide the spatial resolution of AFM in combination with the chemical analysis and compos
219             The extreme force sensitivity of AFM provides the ability to elucidate small differences
220                       Combining strengths of AFM (ambient pressure, height, morphology, and phase mea
221 the development and underlying technology of AFM-IR, including recent advances, and then surveys a wi
222 ve the impact of the electrostatic effect on AFM-based measurements.
223 epidemiologic, and radiologic information on AFM cases to the Centers for Disease Control and Prevent
224      The conclusions can be applied to other AFM-based measurements that are subject to a strong elec
225 e-scale objects immobilized while performing AFM.
226 FM, due to the presence of a weak easy-plane AFM anisotropy.
227                    To illustrate this point, AFM was used to follow the adsorption of the membrane-pe
228 higher unfolding velocities than in previous AFM studies.
229  topographical data under force control (QNM-AFM-SECM).
230 velopments necessary for stable and reliable AFM- and STM-based TERS experiments, together with the s
231                  Montages of high-resolution AFM images of the newly deposited wall surface showed th
232 ophysical evidence from TEM, cryo-TEM, SAXS, AFM, and STEM measurements on the 3FD-IL nanosheets supp
233                     XRD, contact angle, SEM, AFM and SECM studies revealed that the surface of the me
234 hniques (e.g., fluorescence microscopy, SEM, AFM), and show that the PFBs continue to be mobile on th
235                                Specifically, AFM-based SMFS data quality is degraded by a commercial
236 py-based single-molecule force spectroscopy (AFM-SMFS), the tetravalency of these systems impedes the
237 orce microscopy-based infrared spectroscopy (AFM-IR) is a rapidly emerging technique that provides ch
238 force microscopy with infrared spectroscopy (AFM-IR) to detect trace organic and inorganic species an
239 orce microscopy-based infrared spectroscopy (AFM-IR) to measure the chemical and mechanical heterogen
240 e (CRISPR-Cas9 nanoparticles) for high-speed AFM-based physical mapping of DNA and (2) the first succ
241 ptics to image DNA molecules with high-speed AFM.
242               Here we exploit a combined STM/AFM technique to demonstrate the on-surface formation of
243  tunnelling and atomic force microscope (STM/AFM) was used to dehydrogenate precursor molecules.
244 ytical techniques including FESEM, EDS, TEM, AFM, FTIR, Raman, Fluorescence and Absorption Spectrosco
245          The operation of a room-temperature AFM THz-frequency oscillator is similar to that of a cry
246                             We conclude that AFM pulling can be used to activate EGL-mediated NO prod
247 Through this comparison it is concluded that AFM force measurements are sensitive to the position of
248                                          The AFM analysis of the biochip surface allowed metrological
249                                          The AFM results are complemented by fluorescence recovery af
250                                          The AFM-b-to-G-AFM transition in Ca3(Ru(1-x)Ti(x))2O7 happen
251                                          The AFM-based nanomechanical compression measurements demons
252 inct linear or nonlinear behavior across the AFM to FM metamagnetic transition depending on the Fe- o
253 ntains overall electroneutrality between the AFM tip and sample, while at smaller distances other for
254  concurrent electrostatic effect between the AFM tip/cantilever and sample surface can occur.
255 to a strong electrostatic effect between the AFM tip/cantilever and sample surface, regardless of con
256  no intermediate magnetic phases between the AFM-b and G-AFM states, which is in contrasted to mangan
257                            By converting the AFM phase into the FM phase, the stray field, and hence
258 al of the AFM cantilever after detaching the AFM probe from the sample surface (this signal is curren
259 o the electronic phase transition, i.e., the AFM-to-FM transition occurs before the insulator-to-meta
260 AFM spin configuration is different from the AFM state near the FM ground state.
261            The THz-frequency signal from the AFM with the amplitude exceeding 1 V/cm is picked up by
262 ffect of this removal is clearly seen in the AFM force-separation curves associated with the pericell
263 cession of magnetizations sublattices in the AFM, due to the presence of a weak easy-plane AFM anisot
264 ased on an analysis of ringing signal of the AFM cantilever after detaching the AFM probe from the sa
265 indings demonstrate that manipulation of the AFM Neel-order magnetization direction via purely E-fiel
266 (SNAP) ensures the precise adjustment of the AFM optical lever system, a prerequisite for all kinds o
267                         The frequency of the AFM oscillations varies in the range of 0.1-2.0 THz with
268 el for brushes larger than the height of the AFM probe, which seems to be the case for fibroblast cel
269                        By calibration of the AFM signal, an upper estimate of approximately 1 x 10(16
270            The dynamic contact angles of the AFM tips were calculated from the capillary force measur
271                          We predict that the AFM Fe-terminated phase undergoes an E-field magnetizati
272 n we applied a Gaussian mixture model to the AFM data, we observed a distinct force range for recepto
273 rt (when the corrugations are exposed to the AFM probe).
274 tion that reviews the physics underlying the AFM-IR measurement and detection mechanisms.
275 We presented antigenic stimulation using the AFM cantilever while simultaneously imaging with optical
276  emulated the forces of the T cell using the AFM cantilever, even these actin-inhibited T cells becam
277 ight that is in excellent agreement with the AFM data.
278 le assay gave corresponding results with the AFM imaging.
279  nN) to the N-cadherin-coated-beads with the AFM induced a localized mechanical response from the VSM
280 tion of bacteria adhering to glass and their AFM force-distance curves and include the following obse
281  single and double layers as judged by their AFM heights of hAFM approximately 1.2 +/- 0.5 and 2.2 +/
282            Future research can now use these AFMs to investigate specific stages of auditory processi
283 elements is investigated via high throughput AFM single-molecule force spectroscopy.
284 ants were tested in a second high-throughput AFM SMFS experiment revealing that in one case a single
285                     For experiments, tipless AFM cantilevers were functionalized with PMMA microspher
286                                 According to AFM images, a PGworks solution triggered H9e hydrogel fi
287 nterface magnetization from C-type to A-type AFM state.
288                                Here, we used AFM imaging and NMR, fluorescence, and mass spectrometry
289                                        Using AFM force-clamp experiments, we show that formin control
290                                        Using AFM-based single-cell force spectroscopy, we investigate
291                                        Using AFM-SMFS, the mechanical properties of the interaction b
292 nge of applications and investigations using AFM-IR.
293 termined to be 100 nm and 88 +/- 15 nm using AFM and EIS, respectively.
294 s study establishes the methodology of using AFM to accurately quantify the water uptake of individua
295  on endothelial cytoskeletal structure using AFM, SEM, and immunofluorescence.
296                    We measured stiffness via AFM nanoindentation with a spherical indenter and found
297 -molecule properties on the surface, whereas AFM measurements resolved its planar, threefold symmetri
298 insulator at [Formula: see text]21 GPa whose AFM spin configuration is different from the AFM state n
299 tions of particles can be distinguished with AFM, an individual particle method, whereas HTDMA sees t
300 equivalent diameter for quantifying GFs with AFM agreed well with those determined by substrate-free
301                            It was shown with AFM imaging that the inhibition of fibril formation was

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