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1 clear NMR, mass spectrometry, and Rutherford backscattering.
2 was identified as a major contributor to the backscattering.
3 asurements of corneal sublayer thickness and backscattering.
4 nse spin currents that are protected against backscattering.
5  into two categories: forward scattering and backscattering.
6 lectromagnetic duality symmetry exhibit zero backscattering.
7 gnetic fields based on strong suppression of backscattering.
8 he protection of surface Dirac fermions from backscattering.
9 tes that are topologically protected against backscattering.
10 states that are topologically protected from backscattering.
11 ing structures, it does not rely on multiple backscattering.
12 rized surface states that are protected from backscattering.
13 ropic nature of structures instead of strong backscattering.
14 analogy, we observe the suppression of 2k(F) backscattering, a characteristic of Dirac particles.
15  reflection symmetry, significantly reducing backscattering and ensuring robust one-way wave propagat
16 ering, which is thought to protect them from backscattering and localization.
17 xhibits parity asymmetry, can remove elastic backscattering and provides robustness against disorder.
18  laser scanning confocal microscopy, both in backscattering and transmission geometries.
19 tinuclear NMR, mass spectrometry, Rutherford backscattering, and density functional theory (DFT) simu
20 gher and temperatures above 14 K, and phonon backscattering, as manifested in the classical size effe
21  chemical systems show clear evidence for Cu backscattering at approximately 2.5 A.
22 cated Hg coordination by O atoms only and Fe backscattering atoms that is consistent with inner-spher
23 tion of Hg by Cl ligands, multiple Hg and Cl backscattering atoms, and concentration of Hg as small p
24 elative insensitivity to the geometry of the backscattering atoms.
25 lectronic band structure and-by studying the backscattering between counter-propagating edge states-t
26 onic crystal ring and linking it to coherent backscattering between counter-propagating WGMs.
27  that, despite strong atomic scale disorder, backscattering between states of opposite momentum and o
28 n the inverted phase that are protected from backscattering by an emergent spin symmetry that remains
29 t the one-dimensional (1D) edge, along which backscattering by nonmagnetic impurities is strictly pro
30 ntration is well correlated with the optical backscattering by particles suspended in seawater.
31 st with ambient light, which is explained by backscattering calculations for the complex fibrous mate
32 tems lacking enough rotational symmetry, the backscattering can be almost-entirely suppressed for a g
33 le-in-cell simulations that stimulated Raman backscattering can generate and amplify twisted lasers t
34                                     Coherent backscattering (CBS) arises from complex interactions of
35 lation, in conjunction with retrieval of the backscattering coefficient from remote-sensing reflectan
36 e simultaneous measurement of its integrated backscattering coefficient related to the cell size and
37                   The spectrum of the single backscattering component is further analyzed to provide
38 sing light in between scattering layers in a backscattering configuration and show that the light int
39 tering behavior, consistent with significant backscattering contributions from grain boundaries.
40 raction imaging, we find unexpectedly strong backscattering contributions from low-Z atoms.
41 ization of photonic integrated circuits, and backscattering control in telecom systems.
42           Such states that propagate without backscattering could find important applications in comm
43                     These parameters are the backscattering cross-sections and the lidar ratio for bl
44 llary dual-bicell (DCDB) microinterferometic backscattering detection (MIBD) system was developed.
45 bstrate, followed by solvent evaporation and backscattering detection.
46 structures obtained via colocalized electron backscattering diffraction (EBSD).
47  light scattering peak is the highest in the backscattering direction.
48 antitatively demonstrates the suppression of backscattering due to the non-trivial topology of the st
49 g non-local transport signals and suppressed backscattering due to the opposite spin polarizations of
50 metry breaking, and that the increase of the backscattering due to the progressive breaking of one of
51 c and aperiodic nanomeshes, and quantify the backscattering effect by comparing variable-pitch nanome
52 nabled by the RF (Radio Frequency) microwave backscattering effect where the biopotentials are modula
53 omagnetic waves around sharp corners without backscattering effects.
54 conventional SEM and FIB-SEM analyses was on backscattering efficiency, in some cases varying several
55 sualized using secondary-electron images and backscattering electron diffraction patterns.
56 yzed by microcomputed tomography followed by backscattering electron microscopy and histology.
57  (such as pig) cannot be imaged using purely backscattering electron wave packets without molecular a
58 ation of the free carrier response by strong backscattering expected from these heavily disordered pe
59 action (Michael addition) was monitored with backscattering fiber optics under strongly attenuated la
60  domain reflectometry methods that rely upon backscattering for spatially resolved detection.
61 a combination of optical gradient forces and backscattering forces, eliminating the need for electron
62 o, which provides perfect unidirectional and backscattering-free edge propagation that is immune to a
63                            These passive and backscattering-free edge waves have the potential to ena
64                           Unidirectional and backscattering-free propagation of sound waves is of fun
65 simulation of the experimental data involves backscattering from a histidine group with Cu-N of 1.92
66 small shear rates (0.001 s(-1)) can increase backscattering from blooms of large phytoplankton by mor
67 tors with non-isotropic scattering caused by backscattering from boundaries and line defects.
68 es it possible to distinguish between single backscattering from epithelial-cell nuclei and multiply
69               The new Ca EXAFS clearly shows backscattering from Mn at 3.4 A, a distance that agrees
70 igh nuclear density, and the relatively weak backscattering from nuclei imposes a fundamental limit o
71                                The increased backscattering from the base of the OS is explained by a
72 crobubble contrast agents to increase signal backscattering from the blood.
73 AFS spectrum was successfully interpreted by backscattering from two His residues (Fe-N at 1.99 A), a
74                                    Using the backscattering geometry at large photon momentum transfe
75 E focus is far from ideal, especially in the backscattering geometry, which is more practical in many
76 ieved in unstained tissues by using a simple backscattering geometry.
77 ng one of the two symmetries on the emerging backscattering has not yet been systematically studied.
78 se materials are characterized by Rutherford backscattering, high-resolution electron microscopy, and
79 ing processes when postprocessing integrated backscattering (IB) coefficients of backscattered signal
80 irm inverted band structures and demonstrate backscattering-immune elastic wave transmissions through
81 al nature of this system, we further observe backscattering-immune propagation of a nontrivial surfac
82 e only observe backward features, due to low backscattering in muscle.
83                             Stimulated Raman backscattering in plasma is potentially an efficient met
84 c states are topologically protected against backscattering in the absence of valley-mixing scatterin
85 ependent pattern of polarization-maintaining backscattering in the corneal stroma secondary to CXL.
86 , consistent with our calculation of reduced backscattering in this 1D system, and suggests that tran
87 rotection mechanism that strongly suppresses backscattering in zero magnetic field.
88 uantum matter exhibit unique protection from backscattering induced by disorders, making them ideal c
89 re of bismuth and in particular, demonstrate backscattering inside a helical topological edge state i
90          We show that DSL depth and acoustic backscattering intensity (a measure of biomass) can be m
91 el (I2, describing the angular change of the backscattering intensity in the model), which presented
92 extent of lipid collections, which had a low backscattering intensity, also were well documented.
93                            Here we show that backscattering interferometry (BSI) can accurately quant
94                                        Here, backscattering interferometry (BSI) has been shown to be
95                                              Backscattering interferometry (BSI) has been used to suc
96  first direct and quantitative comparison of backscattering interferometry (BSI) to fluorescence sens
97                  Here we describe the use of backscattering interferometry (BSI) to quantify the bind
98                             Here we employed backscattering interferometry (BSI), a free-solution lab
99 ce (SPR), biolayer interferometry (BLI), and backscattering interferometry (BSI), which can facilitat
100  based on refractive index (RI) sensing with backscattering interferometry (BSI).
101                               Finally, using backscattering interferometry and lipoparticles containi
102                             Here we show how backscattering interferometry in rectangular channels (B
103 in vitro is 6.5 +/- 1.0 nM, as determined by backscattering interferometry; KJ-Pyr-9 also interferes
104                                              Backscattering is a promising power-efficient communicat
105                      For massless particles, backscattering is completely forbidden in Klein tunnelli
106 tate of bismuth in the absence of TRS, where backscattering is predicted to occur.
107 topological edge states, where quasiparticle backscattering is suppressed by time-reversal symmetry (
108 ower, including all the mode reflections and backscattering, is below -40 dB, due to the adiabatic mo
109 el optical technology low-coherence enhanced backscattering (LEBS) spectroscopy, allows identificatio
110 es, confirming that the origin of suppressed backscattering lies with the near conservation of the va
111 nsulators offer the possibility to eliminate backscattering losses and improve the efficiency of opti
112 tomic number of manganese enhances the X-ray backscattering, making it possible to identify.
113                                   Rutherford backscattering measurements show good stability of the t
114 aperture objective (NA = 0.7), necessary for backscattering measurements.
115 provide a diversity of uncorrelated Rayleigh backscattering measurements.
116 l in situations where the conventional Raman backscattering method is hampered or fails because of ex
117 is iTRUE technique enables light focusing in backscattering mode.
118                                     Rayleigh backscattering not only sets the intrinsic loss limit fo
119           The structural defects and maximum backscattering of light clearly localized to the posteri
120                                              Backscattering of light, a function of corneal haze and
121 shear rates (0.1 s(-1)) can increase optical backscattering of natural microbial assemblages by more
122 the time reversal symmetry is a simultaneous backscattering of particles in all N channels.
123  the current saturation appears to be set by backscattering of the charge carriers by optical phonons
124                                              Backscattering of the intense forward-propagating CARS r
125                                              Backscattering of these chiral Frenkel excitons is prohi
126                             We find that the backscattering off electromagnetically-small prisms incr
127 eaking each of the two symmetries has on the backscattering off individual objects and 2D arrays.
128 r, resulting in undesirable localization and backscattering phenomena.
129 tical coherence tomography (OCT) showed some backscattering phenomenon with several alterations of re
130  Using optical fibers with enhanced Rayleigh backscattering profiles as distributed temperature senso
131 lity is due to differences in absorption and backscattering properties of phytoplankton and related c
132 veraged description of texture, and electron backscattering provides spatially resolved surface measu
133 tivity than that available from conventional backscattering Raman spectroscopy.
134 es an arbitrary, mode-by-mode control of the backscattering rate as a versatile tool for mode-locked
135 ection and counting (e.g., estimate electron backscattering rates, false positive rates, and data com
136                                   Rutherford backscattering (RBS) was employed to understand this unu
137 tomic force microscope (AFM) tip utilizing a backscattering reflection configuration.
138                               Suppression of backscattering results in a transport lifetime 10(4) tim
139 kaiA3B3C3) alters the period of the cellular backscattering rhythm.
140  The achieved structure exhibits an enhanced backscattering (see Figure), which has strong dependence
141 ion, more than 40-dB enhancement of Rayleigh backscattering signal was generated in silica fibers usi
142 tection was based on collecting the Rayleigh backscattering signatures with increased gain upon the e
143  perpendicular magnetic field suppresses the backscattering significantly and enables a junction 400
144 coupling within such crystals is probed with backscattering spectra, and the mode splitting (0.10 and
145                                  A high-flux backscattering spectrometer and a time-of-flight disk ch
146 le-induced X-ray emission (PIXE) and elastic backscattering spectrometry (EBS), can be used to explor
147                Simultaneous micro-Rutherford backscattering spectrometry (mu-RBS) and micro-particle
148  structural analyses using HRTEM, Rutherford backscattering spectrometry (RBS) and laser excitation t
149                                   Rutherford backscattering spectrometry (RBS) is used to calibrate a
150 s of the membrane active layer by Rutherford backscattering spectrometry (RBS) revealed the incorpora
151 anning electron microscopy (SEM), Rutherford backscattering spectrometry (RBS), and nuclear reaction
152            Using 1.5 MeV (4)He(+) Rutherford backscattering spectrometry (RBS), each lab has demonstr
153 dispersive spectroscopy (WDS) and Rutherford backscattering spectrometry (RBS).
154 ed by X-ray diffraction (XRD) and Rutherford backscattering spectrometry (RBS).
155         Supported by analyses via Rutherford backscattering spectrometry and energy-dispersive X-ray
156                                   Rutherford backscattering spectrometry and Fourier transform infrar
157 ques including Rutherford and non-Rutherford backscattering spectrometry and particle-induced X-ray e
158 oscopy characterization (TEM) and Rutherford backscattering spectrometry channeling (RBS-C) spectra s
159 etect the ligands after calcination, elastic backscattering spectrometry characterization demonstrate
160 scopy, X-ray diffractrometry, and Rutherford backscattering spectrometry to determine precisely struc
161 ne layers were characterized with Rutherford backscattering spectrometry while the nanopores were cha
162  measurements were obtained using Rutherford backscattering spectrometry with samples prepared at a r
163 mug/cm(2) dendrimers G2 and G3 by Rutherford backscattering spectrometry with the aid of heavy ion pr
164 m elastically backscattered ions (Rutherford backscattering spectrometry).
165 e after each monomer addition via Rutherford backscattering spectrometry, X-ray photoelectron spectro
166                                   Rutherford backscattering spectroscopy (RBS) and microscopy demonst
167 toichiometry (1:2) as analyzed by rutherford backscattering spectroscopy (RBS).
168 infrared spectroscopy (FTIR), and Rutherford backscattering spectroscopy (RBS).
169  using incoherent neutron time-of-flight and backscattering spectroscopy on the picosecond to nanosec
170                                      Neutron backscattering spectroscopy showed that the mean square
171 0 K temperature region using high-resolution backscattering spectroscopy to measure an identical moti
172 e states and the associated valley-protected backscattering suppression around the curved waveguide a
173 race the far-wake propagation using acoustic backscattering techniques in excess of 30D.
174 sult from differential spin transmission and backscattering that arise from chirality-induced spin sp
175 as well as phonon particle effects including backscattering, the dominant mechanism responsible for t
176 topological insulators, a protection against backscattering through the spin-momentum locking mechani
177 ors (DAS) using fiber with enhanced Rayleigh backscattering to recognize vibration events induced by
178                                              Backscattering topologies are used to significantly exte
179 distinct valleys to the pair kinematics of a backscattering type.
180 l information on the frequency dependence of backscattering, which is descriptive of the histologic f
181 in-momentum locking and are thus immune from backscattering, which is prohibited by time-reversal sym

 
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