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1 walk approximations of the excitation in the antenna.
2 between two sensory organs, the eye and the antenna.
3 oes from all olfactory organs, including the antenna.
4 rties as the firing activity measured at the antenna.
5 the organization described in the Drosophila antenna.
6 PQ through quenching of the associated LHCII antenna.
7 ncident on the radar aperture using a single antenna.
8 receive input primarily from the ipsilateral antenna.
9 on and focusing, similar to a parabolic dish-antenna.
10 In this study, we extend our analysis to the antenna.
11 iological analysis of the Glossina morsitans antenna.
12 e bolometer pairs corresponding to each slot antenna.
13 nidentified components of the photosystem II antenna.
14 onents and their associated light-harvesting antenna.
15 tes the hygrosensory triad in the Drosophila antenna.
16 ens dipoles excited in an individual dipolar antenna.
17 to an inductor-capacitor resonator, i.e., an antenna.
18 k inserted between an RF transceiver and its antenna.
19 ed by the migration of the excitation in the antenna.
20 cal element to focus the IR radiation to the antenna.
21 ng the change of current passing through the antenna.
22 s as a function of the absorbed power by the antenna.
23 ce plasmon resonance (LSPR) modes in nanorod antennas.
24 en the excited dyes and plasmonically active antennas.
25 limits on radiation from electrically small antennas.
26 pplications for portable, electrically small antennas.
27 terahertz electric field of custom-tailored antennas.
28 ncrete, which can improve the performance of antennas.
29 s improves the bandwidth and S11 of embedded antennas.
30 such as lasers, grating couplers and optical antennas.
31 er in two closely-spaced, directive infrared antennas.
32 n general difficult to obtain for SSPP based antennas.
33 th, over phased array antennas and reflector antennas.
35 In this paper, an Advanced Short Backfire Antenna (A-SBFA), augmented with anisotropic metamateria
37 and steady-state mid-infrared semiconductor antennas.Achieving large tunability of subwavelength res
38 To show the new QCTO modified Luneburg lens antenna, an example lens antenna was designed at Ka-band
39 er-coated gold nanorod acting as a plasmonic antenna and biotin as a high-affinity biorecognition ele
42 ic trigger waves in a universal framework of antenna and percolation theory(25,26), and reveal a phas
43 how many fucose residues are on the specific antenna and provides additional information on the topol
44 ns share the ambiguous responses of a single antenna and receive input primarily from the ipsilateral
45 he functional organization of the tsetse fly antenna and that of the fruit fly Drosophila melanogaste
47 o prepare arrays of nanocube-based plasmonic antennas and deliberately place dyes with sub-nm precisi
48 compare fabrication techniques for flexible antennas and demonstrate that screen and stencil printin
49 cle, we fabricate chromium and tungsten nano-antennas and demonstrate that they can handle 110 and 30
55 o known as red chlorophylls) residing in the antenna are important for energy transfer dynamics and y
56 neuropils associated with the antennule and antenna are markedly pronounced when compared to the oth
61 comparable performance with that of a copper antenna array at 28 GHz, which is a target frequency in
64 mprovement of performance of a metaresonator antenna array in terms of a small shift in the resonance
65 bed here, a cross-polarized microstrip patch antenna array is connected to the source and drain probe
66 le and salient features of the proposed MIMO antenna array shows the potential for on-chip applicatio
67 over, it is demonstrated that an MXene patch antenna array with integrated feeding circuits on a conf
71 e microelectromechanical movement of silicon antenna arrays created in standard silicon-on-insulator
74 that of a standard 35 um thick copper patch antenna at about 15% of its thickness and 7% of the copp
76 he performance parameters of a novel on-chip antenna based on metasurface technology at terahertz ban
78 communication systems.The miniaturization of antennas beyond a wavelength is limited by designs which
79 ing Ln(3+) -bound water molecule as the CEST antenna but this design often added additional line-broa
80 y depends upon the in-plane structure of the antennas but also the size of the gap, which is regulate
81 ementing QCTO-enabled modified Luneburg lens antenna by designing a broadband anti-reflective layer a
82 ptical cross-section of the light-harvesting antenna by selectively reducing chlorophyll b levels and
84 ptical cross-section of the light-harvesting antenna can lead to substantial improvements in algal ph
89 ex vivo measurements, we designed mid-field antennas capable of operating efficiently in tissue at 1
94 nt spatio-temporal code at the output of the antenna circuits determines the level of complexity of o
96 The monomeric photosystem I-light-harvesting antenna complex I (PSI-LHCI) supercomplex from the extre
99 -green light, OCP binds to the phycobilisome antenna complex, providing an excitonic trap to thermall
101 Conformational changes of the photosynthetic antenna complexes activate dissipation by leveraging the
103 ent chromophores present in light-harvesting antenna complexes are introduced, and then we examine th
105 lisomes are highly organized pigment-protein antenna complexes found in the photosynthetic apparatus
107 N >= 9 carotenoids found in light-harvesting antenna complexes represent a vital compromise that reta
108 mbrane organization into small pools of core antenna complexes that rapidly trap energy absorbed by s
109 sfers energy efficiently through a series of antenna complexes to the reaction center where charge se
110 ical cross section of plant light harvesting antenna complexes which capture photons at a rate nearly
116 -magnitude improvement in the sensitivity of antenna-coupled nanothermocouple (ACNTC) infrared detect
123 Based on this nonreciprocity, our NbSe(2) antenna devices exhibit a reversible nonreciprocal sensi
124 trol of the nonreciprocal sensitivity of the antenna devices has been achieved by applying electromag
126 The detector consists of two orthogonal slot antennas, each loaded with two microbolometers at its ed
127 g NPS-SC4AD-NiB system exhibits an ultrahigh antenna effect (33.1) at a high donor/acceptor ratio (25
129 NH(2)-TPDC photoluminescence was due to the "antenna effect" of Gsp, as evidenced by spectroscopic st
134 the resonant coupling between molecular and antenna excitations as well as the spatial extent of the
135 Photoredox quenching of the carbostyril antenna excited states was observed for all Eu(III)-comp
136 (and hence radiation properties), developing antennas exploiting these distributions can challenge co
137 n with multiple CR-absorbing (water-soluble) antenna followed by intramolecular-FRET/TBET energy tran
138 nd used is the presence of a phenylacetylene antenna for optimal chirality recognition and CD/UV resp
139 remain in the development of high-efficiency antennas for biointegrated electronic/optoelectronic sys
140 mples range from dipole, monopole, and patch antennas for far-field RF operation, to magnetic loop an
142 for far-field RF operation, to magnetic loop antennas for near-field communication (NFC), where the k
143 is also beneficial for rapid recognition of antenna from core fucosylation in glycans detected with
146 troscopy experiments performed on individual antennas, further supported by electrodynamical simulati
148 nd grade, RENAL nephrometry score, number of antennas, generator power, and duration of ablation.
149 ight-harvesting devices using plasmonic nano-antenna gratings, that enhance the absorption of light o
153 ethodology, the swore-shaped surface plasmon antenna has both edges corrugated with an array of recta
154 nsisting of densely packed arrays of optical antennas have been demonstrated to provide an effective
161 epair economy by preserving intact PSII core antennas in a single complex available for PSII reassemb
162 plate made of anisotropic T-shaped plasmonic antennas in near-infrared wavelength range, where the ac
163 of 37.5 muW, 123 muW and 173 muW received by antennas in the respective locations, while keeping radi
165 one antenna outside the body, and the other antenna inside the body endoscopically, at the esophagus
167 The Johnston's organ (JO) in the insect antenna is a multisensory organ involved in several navi
169 n process of an emitter close to a plasmonic antenna is enhanced due to strong local electromagnetic
173 the proposed GaAs-based metasurface on-chip antenna is viable for applications in terahertz integrat
174 ure or function of primary cilia, ubiquitous antenna-like organelles essential for cellular signal tr
175 they dynamically localize in primary cilia, antenna-like solitary organelles present on most cells.
178 l light sources, the potential damage of the antennas limits their use with high power lasers: this l
179 he temperature difference between a resonant antenna locally heated by infrared radiation and the sub
180 ion efficiency of a 5.5 um thick MXene patch antenna manufactured by spray-coating from aqueous solut
181 es, arising from interference of 2 radiating antenna modes differently coupling light out of the nano
182 y parameters and to address the influence of antenna morphology and excitation wavelength on polariza
184 ny areas of science and technology, from the antennas of interferometric gravitational wave detectors
186 orders of magnitude smaller than electrical antennas offers the promise for orders of magnitude effi
187 sing system uses two facing microstrip patch antennas operating at 60 GHz, which are placed across in
190 vo in five anesthetized pigs, by placing one antenna outside the body, and the other antenna inside t
191 b lines exhibit a truncated light-harvesting antenna phenotype with reduced amounts of light-harvesti
192 otein dephosphorylation and the more complex antenna phosphorylation patterns in C. reinhardtii compa
194 pare the accuracy of freehand versus robotic antenna placement in CT-guided microwave ablation (MWA)
195 a concentric circular ring plasmonic optical antenna (POA) array using a simple lumped coupled circui
196 s and circuits, thinned silicon ICs, printed antennas, printed energy harvesting and storage modules,
197 tonal organs (Johnston's organ) of the adult antenna project into the centrolateral neuropil column o
198 in the minor light harvesting complex (LHC) antenna protein LHCB6, which was dependent on STN8 kinas
200 he PSII subunits (psbA, psbB, and PSBW), the antenna proteins (LHCA1, LHCB1, and LHCB4), the ribulose
202 t-protein complex does contain the PSII core antenna proteins CP47 and CP43, as well as most of their
204 io-temporal encoding model of the Drosophila antenna provides a theoretical foundation for understand
206 ansition from noble metals to aluminum based antenna-reactor heterostructures in plasmonic photocatal
207 -abundant embedded aluminum in cuprous oxide antenna-reactor heterostructures that operate more effec
208 of small, stretchable, radio frequency (RF) antennas realized using these strategies compare favorab
209 to the regulatory sites in proximity of the antenna region, NADH acts as a positive allosteric modul
211 roup of inhibitory primary interneurons, the antenna relay neurons (antRNs), which then project asymm
212 obotic antenna guidance reduces the need for antenna repositioning in microwave ablation to accuratel
216 However, the highest radiation efficiency antennas require size at the scale of the wavelength (he
217 (MOFs), can emulate the functionality of the antenna rings of chlorophylls in light-harvesting comple
222 nctional 3D devices including reconfigurable antenna, shape-shifting structures, and microfluidics.
223 , the fundamental reduction in efficiency as antenna size decreases below a wavelength (30 m at 1 MHz
224 rescence spectroscopy indicated that the PSI antenna size in vivo is even larger than that of the pur
225 nters, and an increase in the relative LHCII antenna size of photosystem I (PSI) compared to PSII.
226 int where further reductions or increases in antenna size reduce photosynthetic efficiency, tolerance
228 ed that there is an optimal light-harvesting antenna size that results in the greatest whole plant ph
231 By surveying a range of light harvesting antenna sizes achieved by reduction in chlorophyll b lev
233 levels and correspondingly light-harvesting antenna sizes by light-activated Nab1 repression of CAO
234 ystem to dynamically adjust light-harvesting antenna sizes for enhanced photosynthetic performance.
235 Significantly, algae having light-regulated antenna sizes had substantially higher photosynthetic ra
236 ve been linked to regulation of the relative antenna sizes of PSI and PSII (state transitions), the P
238 lectron mobility transistor (HEMT) with nano antenna structures was fabricated and demonstrated to be
239 gy transfer, in particular multichromophoric antenna structures, is shown to vary depending on the sp
240 -LHCI supercomplex can bind up to eight Lhcr antenna subunits, which are organized as two rows on the
242 Harvesting Complexes (LHC), constituting the antenna system of both photosystem I (PSI) and PSII.
245 ding to EET optimization of light-harvesting antenna systems while exploring the structure and functi
246 , electric field meters, fast electric-field antenna systems, and for two seasons, a Lightning Mappin
248 , bearing two specific picolinate two-photon antennas (tailor-made for each targeted metal) and one a
250 metamaterials, when applied to conventional antenna technology, can provide significant performance
252 re, we introduce a low-profile bidirectional antenna that can be mounted on a large ground plane and
253 This performance is unprecedented for an antenna that has seen widespread use, but few design cha
255 The flagellum has been recognized as an "antenna" that plays a core role in sensing environmental
256 expressed in multiple tissues, including the antenna, the male reproductive glands and is transferred
257 he ratio of the resistance change in the two antennas, the angle of arrival of the LWIR signal can be
258 s are related to the currents in the optical antennas, the LCC model provides a useful tool for the a
260 to structure the near field rely on optical antenna theory, involving nanostructures that locally co
261 l printing are both suitable for fabricating antennas; these different techniques are most useful at
265 device, by efficient coupling of a plasmonic antenna to hyperbolic phonon-polaritons in hexagonal-BN
266 s, energy is transferred from photosynthetic antenna to reaction centers via ultrafast energy transfe
267 the electric and magnetic resonances of such antennas to achieve a very strong dependence of the opti
271 mission line lengths required to connect the antennas to the lens for maximum re-radiation power is d
272 ically employed for cooling cellular network antennas) to achieve up to ~87% parahydrogen enrichment
273 -harvesting complexes, mimicking the modular antenna/transducer architecture of natural photosystems,
274 conditions and binds to the light-harvesting antenna, triggering the dissipation of captured light en
276 anding of humidity sensing in the Drosophila antenna, uncover a neuronal substrate for early sensory
279 diates to the far-field by coupling with the antenna via plasmonic states, whose presence increases t
280 ified Luneburg lens antenna, an example lens antenna was designed at Ka-band (26-40 GHz) and fabricat
282 MoS(2) rectifier with a flexible Wi-Fi-band antenna, we fabricate a fully flexible and integrated re
283 the Eu(III) center and the light-harvesting antenna were studied using cyclic voltammetry and steady
285 lications of these structures are leaky-wave antennas which utilize the low frequency dependence.
287 the incident radiation reflected back to the antenna, which significantly increases the detector sens
288 inates more than 90 chlorophylls in its core antenna while achieving near perfect quantum efficiency.
290 ange of resistance is sensed by biasing each antenna with a constant DC voltage and measuring the cha
291 er, we presented the four-element MIMO patch antenna with different types of EBG structures for the m
292 + Cu straight, 2r-rs strongly reclival, and antenna with homonomous flagellum, revealing new and imp
293 esting that the putative association of this antenna with the PSI supercomplex is absent or may be lo
295 lines with low-energy attenuation and patch antennas with high-power radiation at frequencies from 5
296 ndex dielectric gallium phosphide (GaP) nano-antennas with small mode volumes coupled to atomic mono-
298 ar systems, such as certain light-harvesting antennas, with cartwheeling charge motion upon excitatio
300 at extend the effective aperture area of the antenna without affecting its dimensions, and the concen