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1 he protection of surface Dirac fermions from backscattering.
2 was identified as a major contributor to the backscattering.
3 asurements of corneal sublayer thickness and backscattering.
4 states that are topologically protected from backscattering.
5 tes that are topologically protected against backscattering.
6 ing structures, it does not rely on multiple backscattering.
7 rized surface states that are protected from backscattering.
8 ropic nature of structures instead of strong backscattering.
9 clear NMR, mass spectrometry, and Rutherford backscattering.
10 analogy, we observe the suppression of 2k(F) backscattering, a characteristic of Dirac particles.
12 xhibits parity asymmetry, can remove elastic backscattering and provides robustness against disorder.
14 tinuclear NMR, mass spectrometry, Rutherford backscattering, and density functional theory (DFT) simu
15 gher and temperatures above 14 K, and phonon backscattering, as manifested in the classical size effe
17 cated Hg coordination by O atoms only and Fe backscattering atoms that is consistent with inner-spher
18 tion of Hg by Cl ligands, multiple Hg and Cl backscattering atoms, and concentration of Hg as small p
20 that, despite strong atomic scale disorder, backscattering between states of opposite momentum and o
22 le-in-cell simulations that stimulated Raman backscattering can generate and amplify twisted lasers t
23 lation, in conjunction with retrieval of the backscattering coefficient from remote-sensing reflectan
24 e simultaneous measurement of its integrated backscattering coefficient related to the cell size and
26 sing light in between scattering layers in a backscattering configuration and show that the light int
28 llary dual-bicell (DCDB) microinterferometic backscattering detection (MIBD) system was developed.
31 g non-local transport signals and suppressed backscattering due to the opposite spin polarizations of
32 c and aperiodic nanomeshes, and quantify the backscattering effect by comparing variable-pitch nanome
34 conventional SEM and FIB-SEM analyses was on backscattering efficiency, in some cases varying several
36 (such as pig) cannot be imaged using purely backscattering electron wave packets without molecular a
37 ation of the free carrier response by strong backscattering expected from these heavily disordered pe
38 action (Michael addition) was monitored with backscattering fiber optics under strongly attenuated la
40 a combination of optical gradient forces and backscattering forces, eliminating the need for electron
41 simulation of the experimental data involves backscattering from a histidine group with Cu-N of 1.92
42 small shear rates (0.001 s(-1)) can increase backscattering from blooms of large phytoplankton by mor
43 es it possible to distinguish between single backscattering from epithelial-cell nuclei and multiply
46 AFS spectrum was successfully interpreted by backscattering from two His residues (Fe-N at 1.99 A), a
48 E focus is far from ideal, especially in the backscattering geometry, which is more practical in many
50 se materials are characterized by Rutherford backscattering, high-resolution electron microscopy, and
51 al nature of this system, we further observe backscattering-immune propagation of a nontrivial surfac
54 c states are topologically protected against backscattering in the absence of valley-mixing scatterin
55 , consistent with our calculation of reduced backscattering in this 1D system, and suggests that tran
57 uantum matter exhibit unique protection from backscattering induced by disorders, making them ideal c
59 el (I2, describing the angular change of the backscattering intensity in the model), which presented
60 extent of lipid collections, which had a low backscattering intensity, also were well documented.
64 first direct and quantitative comparison of backscattering interferometry (BSI) to fluorescence sens
67 ce (SPR), biolayer interferometry (BLI), and backscattering interferometry (BSI), which can facilitat
71 in vitro is 6.5 +/- 1.0 nM, as determined by backscattering interferometry; KJ-Pyr-9 also interferes
72 ower, including all the mode reflections and backscattering, is below -40 dB, due to the adiabatic mo
73 el optical technology low-coherence enhanced backscattering (LEBS) spectroscopy, allows identificatio
77 l in situations where the conventional Raman backscattering method is hampered or fails because of ex
82 shear rates (0.1 s(-1)) can increase optical backscattering of natural microbial assemblages by more
83 the current saturation appears to be set by backscattering of the charge carriers by optical phonons
86 Using optical fibers with enhanced Rayleigh backscattering profiles as distributed temperature senso
87 lity is due to differences in absorption and backscattering properties of phytoplankton and related c
88 veraged description of texture, and electron backscattering provides spatially resolved surface measu
93 The achieved structure exhibits an enhanced backscattering (see Figure), which has strong dependence
94 ion, more than 40-dB enhancement of Rayleigh backscattering signal was generated in silica fibers usi
95 perpendicular magnetic field suppresses the backscattering significantly and enables a junction 400
96 coupling within such crystals is probed with backscattering spectra, and the mode splitting (0.10 and
98 structural analyses using HRTEM, Rutherford backscattering spectrometry (RBS) and laser excitation t
99 s of the membrane active layer by Rutherford backscattering spectrometry (RBS) revealed the incorpora
100 anning electron microscopy (SEM), Rutherford backscattering spectrometry (RBS), and nuclear reaction
105 ques including Rutherford and non-Rutherford backscattering spectrometry and particle-induced X-ray e
106 oscopy characterization (TEM) and Rutherford backscattering spectrometry channeling (RBS-C) spectra s
107 etect the ligands after calcination, elastic backscattering spectrometry characterization demonstrate
108 scopy, X-ray diffractrometry, and Rutherford backscattering spectrometry to determine precisely struc
109 measurements were obtained using Rutherford backscattering spectrometry with samples prepared at a r
110 mug/cm(2) dendrimers G2 and G3 by Rutherford backscattering spectrometry with the aid of heavy ion pr
112 e after each monomer addition via Rutherford backscattering spectrometry, X-ray photoelectron spectro
115 using incoherent neutron time-of-flight and backscattering spectroscopy on the picosecond to nanosec
117 0 K temperature region using high-resolution backscattering spectroscopy to measure an identical moti
118 e states and the associated valley-protected backscattering suppression around the curved waveguide a
119 as well as phonon particle effects including backscattering, the dominant mechanism responsible for t
120 topological insulators, a protection against backscattering through the spin-momentum locking mechani
121 l information on the frequency dependence of backscattering, which is descriptive of the histologic f
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