ライフサイエンスコーパス: antenna

1 e bolometer pairs corresponding to each slot antenna.

2 m when the lens is applied to a conical horn antenna.

3 nidentified components of the photosystem II antenna.

4 he transport of excitation within individual antenna.

5 acculus, a multi-chambered pocket within the antenna.

6 mechanism by which PsbS acts upon the LHCII antenna.

7 led to 2 GHz, and "cutting" into it the slot antenna.

8 imately 10 nm in diameter), which act as the antenna.

9 onents and their associated light-harvesting antenna.

10 ricate and to reliably couple to a nanoscale antenna.

11 tes the hygrosensory triad in the Drosophila antenna.

12 smission lines, their resonant networks, and antennas.

13 s, displays, sensors, and electrically small antennas.

14 ive candidate for spintronics and microstrip antennas.

15 ncrete, which can improve the performance of antennas.

16 ies directly reflect those of the individual antennas.

17 properties of various natural and artificial antennas.

18 ent not to damage the tissue surrounding the antennas.

19 s improves the bandwidth and S11 of embedded antennas.

20 orward in developing a new type of directive antennas.

21 0 W ex vivo, 65 W in vivo) for 5 minutes per antenna (10 and 15 minutes total ablation time for seque

22 microwave ablations were performed with the antenna a median distance of 4 mm from the heart in both

23 hot electron decay in a plasmonic nanoscale antenna, a coherent optical antenna field appears to be

24 and steady-state mid-infrared semiconductor antennas.Achieving large tunability of subwavelength res

25 An external loop antenna allows robust, straightforward application in a

26 cts anteriorly, bears a long stout uniramous antenna and a chelate limb followed by two biramous appe

27 enter; (2) structural remodeling of the LHCI antenna and adjustment of the effective absorption cross

28 NTD) is responsible for interaction with the antenna and induction of excitation energy quenching, wh

29 uipped with two peripheral olfactory organs, antenna and maxillary palp.

30 sensed by applying a dc bias voltage to each antenna and measuring the changes in the dc current caus

31 ctures, shape-changing soft robots, morphing antenna and RF devices, and biomedical devices.

32 lt in overexcitation of the light-harvesting antenna and the formation of reactive compounds capable

33 on of photoprotective zeaxanthin in the LHCI antenna and the PSI reaction center; (2) structural remo

34 isms influence transfer across assemblies of antenna and thus the photochemical yield at reaction cen

35 alog (All4941) was able to interact with the antenna and to induce permanent thermal energy dissipati

36 se blue light, binds to the light-harvesting antenna and triggers the dissipation of excess captured

37 esidue migration from the glycan core to the antenna and vice versa.

38 Here we report stretchable, multiresonance antennas and battery-free schemes for multichannel wirel

39 ar scattering response of dielectric optical antennas and metamaterials, and provide a strategy for d

40 rm the building blocks of nano-scale optical antennas and metamaterials.

41 allenge for achieving reconfigurable optical antennas and metasurfaces is the need to generate contin

42 en limited by bandwidth constraints of their antennas and photoconductor parasitics.

43 ealization to offer miniaturized waveguides, antennas and shielding patterns are on anvil.

44 The use of multiple antennas and simultaneous power delivery creates larger,

45 the design of bio-inspired light-harvesting antennas and the redesign of natural photosynthetic syst

46 ge absorption cross-section of semiconductor antennas and their weak near-field coupling open a uniqu

47 the phycobilisome (PBS), the cyanobacterial antenna, and induces excitation-energy quenching.

48 o bind to phycobilisomes, the cyanobacterial antenna, and to quench excess energy.

49 onant properties behave as nanoscale optical antennas, and have recently shown extraordinary promise

50 e the influence of power delivery, number of antennas, and tissue type.

51 urface structures consisting of phased array antennas are able to circumvent the phase-matching requi

52 High directive antennas are fundamental elements for microwave communic

53 Since the near-fields of the optical antennas are related to the currents in the optical ante

54 sed for spin wave excitation while two other antennas are used for detection of the inductive voltage

55 Two of these antennas are used for spin wave excitation while two oth

56 M beams utilising a custom-designed circular antenna array at 28 GHz.

57 The radiation beams of the proposed antenna array can scan in the end-fire area (60 degrees

58 The shared-aperture phased antenna array developed in the field of radar applicatio

59 and S21 characteristics of the metaresonator antenna array embedded in enhanced cement pastes.

60 mprovement of performance of a metaresonator antenna array in terms of a small shift in the resonance

61 steering angle of up to 35 degrees from the antenna array normal.

62 Two- and three-antenna arrays were evaluated in each model.

63 By introducing hybrid random antenna arrays with small metallic nanoparticles and ult

64 crystals, nano-undulators, metamaterials and antenna arrays) have enabled the development of nanoscal

65 d in combination with active motion-tracking antenna arrays, these devices enable multichannel optoge

66 gh large-area plasmonic photoconductive nano-antenna arrays.

67 re grown (LTG) InGaAs/InAlAs photoconductive antenna as the receiver.

68 nked to each other-serve as light-harvesting antennas as well as electron donors and are flexibly cou

69 ormance is affected more than other types of antennas, as typical building materials have a shielding

70 the light localizing properties of plasmonic antennas at pre-defined locations.

71 in vivo communication link using microscopic antennas at radiofrequency is severely limited by the re

72 The active tuning of plasmonic antennas attached to such junctions is analysed using a

73 xposure of synthesized aerosol to the insect antenna, AuNPs reached the brain within an hour.

74 The nanopillar optical antenna avalanche detector (NOAAD) architecture is utili

75 communication systems.The miniaturization of antennas beyond a wavelength is limited by designs which

76 roduction of stereodynamic zinc complexes of antenna biphenols, a new class of sensors bearing antenn

77 Next, the beta-GlcNAc terminating antenna can be converted into LacNAc by galactosylation

78 re we experimentally show that EET in single antennas can be characterized by 2D polarization imaging

79 Nanoscale bowtie aperture antennas can be used to focus light well below the diffr

80 and enhanced terahertz transmission by nano-antennas can effectively increase the molecular absorpti

81 ex vivo measurements, we designed mid-field antennas capable of operating efficiently in tissue at 1

82 alculation one can infer the coupling of the antenna chlorosome with the environment and the coupling

83 s 5,10-methenyltetrahydrofolate (MTHF) as an antenna chromophore with a unique binding site and mode.

84 e secondary pocket of CRY1, analogous to the antenna chromophore-binding pocket of photolyase.

85 n the miniaturization of microwave front-end antenna circuits.

86 circular ablations were achieved with three antennas compared with two antennas (P < .05).

87 rved by both LHCII and four light-harvesting antenna complex I (LHCI) subunits, Lhca1, 2, 3 and 4.

88 The monomeric photosystem I-light-harvesting antenna complex I (PSI-LHCI) supercomplex from the extre

89 he phosphorylation state of light-harvesting antenna complex II (LHCII).

90 ity of CpcA, a subunit of the photosynthetic antenna complex in cyanobacteria, for STORM and SIM imag

91 show that these transfer dynamics constrain antenna complex organization.

92 proportion of PsbS bound to the minor LHCII antenna complex proteins Lhcb4, Lhcb5 and Lhcb6.

93 One antenna complex, the Fenna-Matthews-Olson (FMO) antenna

94 energy transfer through the dense network of antenna complexes and into the reaction center.

95 ent chromophores present in light-harvesting antenna complexes are introduced, and then we examine th

96 lisomes are highly organized pigment-protein antenna complexes found in the photosynthetic apparatus

97 otosynthetic apparatus and protection of the antenna complexes from oxidation damage in contaminated

98 ements of PSII and (likely) light-harvesting antenna complexes into a photochemically quenched state.

99 n with the nearest chlorophylls in the plant antenna complexes LHCII, CP26, CP29 and LHCI.

100 Light-harvesting antenna complexes not only aid in the capture of solar e

101 he absorption of sunlight by pigments in the antenna complexes of photosystem II (PSII), followed by

102 PSII and cytochrome f, the light-harvesting antenna complexes of PSII remain stable throughout the c

103 mbrane organization into small pools of core antenna complexes that rapidly trap energy absorbed by s

104 sfers energy efficiently through a series of antenna complexes to the reaction center where charge se

105 ap energy absorbed by surrounding peripheral antenna complexes.

106 ts of energy transfer and photoprotection in antenna complexes.

107 state of the phycobilisome light-harvesting antenna components.

108 A loopless MR imaging antenna composed of a tuned microcable either 0.8 or 2.2

109 with its radiation characteristics in a lens antenna configuration have been studied numerically and

110 The devices combine subdermal magnetic coil antennas connected to microscale, injectable light-emitt

111 As a model system we investigate L-shaped antennas consisting of two orthogonal nanorods which len

112 The Drosophila antenna contains receptor neurons for mechanical, olfact

113 brid structure of single plasmonic nanopatch antennas coupled to colloidal quantum dots.

114 s shown that the graphene resonators produce antenna-coupled blackbody radiation, which manifests as

115 ex and a PSII core complex lacking the inner antenna CP43 (RC47), whereas Psb28-1 preferentially bind

116 xpression of the transcription factor distal antenna (dan) is highly similar to other prepatterning f

117 ning electron microscopy showed carapace and antenna deformities after exposure to fibers, with no de

118 n review recent developments in the areas of antenna design, fabrication, and characterization.

119 ier connected to a metamaterial-inspired 3-D antenna designed to be highly sensitive to the liquid-vo

120 roposed combination of DSTMS emission and PC antenna detection realizes a compact and low-cost THz-TD

121 Full physics simulations of the photonic antenna detector element that enables this instrument, s

122 m the summit of Ciemniak Mountain had larger antenna dimensions and chlorophyll content but a lower p

123 and tissue injury decreased with increasing antenna distance from the heart with both antenna orient

124 in Drosophila; it analyzes movements of the antenna due to sound, wind, gravity, and touch.

125 The detector consists of two orthogonal slot antennas, each loaded with two microbolometers at its ed

126 ution, indicating that the proton-collecting antenna effect is maximal already for a membrane area of

127 via sensitization through an intramolecular antenna effect.

128 Unfortunately, at d < 10 nm, antenna efficiency drops below 50%, owing to optical spr

129 Although the antennas' electric near-field distributions are commonly

130 eams is limited by the emitting angle of the antenna elements, and (ii) a larger steering angle may d

131 uadrupolar radiation from the two dielectric antenna elements.

132 while cells in limiting CO2 maintain a large antenna even in high light and switch on energy-dissipat

133 the resonant coupling between molecular and antenna excitations as well as the spatial extent of the

134 Photoredox quenching of the carbostyril antenna excited states was observed for all Eu(III)-comp

135 of a magnetic cross junction with four micro-antennas fabricated at the edges.

136 smonic nanoscale antenna, a coherent optical antenna field appears to be rectified directly in our de

137 with the electromagnetic wave, reducing the antenna footprint by up to 100.

138 advanced materials for engineering molecular antenna for harvesting solar energy.

139 al (MIM) metasurface composed of hybrid nano-antennas for comprehensive spatial engineering of the pr

140 Demonstrations include printed magnetic loop antennas for near-field communication devices.

141 al conveyance of information using plasmonic antennas for on-chip communication technology.

142 Antennas, from radiofrequencies to optics, are bound to

143 cal resonances that endow them with valuable antenna functions.

144 troscopy experiments performed on individual antennas, further supported by electrodynamical simulati

145 ission rate speedup approximately 115 x, for antenna gap spacing, d = 40 nm.

146 ry Brown that radio-pulses from two distinct antennas generate signals on the oscilloscope that wiggl

147 nd grade, RENAL nephrometry score, number of antennas, generator power, and duration of ablation.

148 The fibrils, functioning as quenched antennas, give intense excitonic couplets in the electro

149 ight-harvesting devices using plasmonic nano-antenna gratings, that enhance the absorption of light o

150 e wavelength, and further miniaturization of antennas has been an open challenge for decades.

151 ously demonstrated plasmonic photoconductive antennas has been limited by bandwidth constraints of th

152 Loop-type antennas have a strong magnetic near field and so dissip

153 nsisting of densely packed arrays of optical antennas have been demonstrated to provide an effective

154 Plasmonic photoconductive antennas have great promise for increasing responsivity

155 These ME antennas have potential implications for portable wirele

156 ll resonator antennas, such as metaresonator antennas, have narrow bandwidths, which limits their eff

157 When they are used as embedded antennas in building materials, their performance is aff

158 plate made of anisotropic T-shaped plasmonic antennas in near-infrared wavelength range, where the ac

159 he difficulty to mass-fabricate nano-optical antennas in parallel and reproducible fashion, and the c

160 of 37.5 muW, 123 muW and 173 muW received by antennas in the respective locations, while keeping radi

161 Ds, relies on specially designed stretchable antennas in which parallel capacitive coupling circuits

162 We construct a map of the Drosophila antenna, in which the abundant Obps are mapped to olfact

163 arvesting antenna (site); and changes in the antenna induced by DeltapH (change), which lead to the c

164 the phycobilisome (PBS), the cyanobacterial antenna, induced by the orange carotenoid protein (OCP).

165 ytic hydrogen desorption closely follows the antenna-induced local absorption cross-section of the Pd

166 one antenna outside the body, and the other antenna inside the body endoscopically, at the esophagus

167 ting the coupling between identical magnetic antennas inside a model of the body medium we show an in

168 ne or more types of high-index semiconductor antennas into a dense array with subwavelength spacings.

169 By incorporating slot-groove antennas into the metal electrode, we show that LED emis

170 The antenna is a shaped slot element in a 60 nm silver film.

171 natorial odor code supplied by the fruit fly antenna is a very simple one in which nearly all odors p

172 xhibit a directional bias according to which antenna is available to be used.

173 n process of an emitter close to a plasmonic antenna is enhanced due to strong local electromagnetic

174 The antenna is involved in finding food, oviposition sites a

175 To achieve this, the radiation field from an antenna is reversed and then gathered by high numerical

176 nowires with a highly dense array of bow-tie antennas is able to modify the polarization response of

177 The near field of these antennas is dominated by the magnetic field yet they don

178 As expected from a perfect antenna, LH2s showed funneling efficiencies close to uni

179 irmed that qH is localized to the peripheral antenna (LHCII) of photosystem II and demonstrated that

180 e to increase light-harvesting phycobilisome antenna like CS upon high-CO2 treatment.

181 na biphenols, a new class of sensors bearing antenna-like appendages that can extend the wavelength o

182 Primary cilia are highly specialized small antenna-like cellular protrusions that extend from the c

183 de proteins active at the primary cilium, an antenna-like organelle that acts as the cell's signaling

184 The primary cilium is an outward projecting antenna-like organelle with an important role in bone me

185 Primary cilia are antenna-like sensory microtubule structures that extend

186 Their antenna-like structure leads naturally to the assumption

187 Cilia are small, antenna-like structures on the surface of eukaryotic cel

188 results provide testable predictions of the antenna mechanism of actin-cable length control.

189 This "antenna mechanism" involves three key proteins: formins,

190 y parameters and to address the influence of antenna morphology and excitation wavelength on polariza

191 onal pathways conveying information from the antenna, not differences in pheromone detection by the o

192 ngenital deafness affect the sound reception antenna of cochlear sensory cells, the hair bundle.

193 sis of the stereociliary bundle, the sensory antenna of inner ear hair cells, and in the mechanoelect

194 ivation of LHCSR3-dependent quenching in the antenna of photosystem II.

195 ips) that are homologous to light-harvesting antenna of plants and algae.

196 ynamics and pathways in the light-harvesting antennas of various photosynthetic organisms.

197 However, recently demonstrated true magnetic antennas offer an alternative not covered in the previou

198 Further, triantennary isomers (antenna on alpha(1-3) or alpha(1-6) arms) were separated

199 nted graphene enabled transmission lines and antennas on paper substrates were designed, fabricated a

200 sing system uses two facing microstrip patch antennas operating at 60 GHz, which are placed across in

201 L = 1.58 mm (0.5lambda0) aiming at a compact antenna or radar systems.

202 ings within the context of higher plant PS I antenna organization is discussed.

203 ng antenna distance from the heart with both antenna orientations.

204 vo in five anesthetized pigs, by placing one antenna outside the body, and the other antenna inside t

205 hieved with three antennas compared with two antennas (P < .05).

206 a concentric circular ring plasmonic optical antenna (POA) array using a simple lumped coupled circui

207 king the microscopic RF in-vivo transmitting antenna possible.

208 f individual components such as a waveguide, antenna, power supply, and an oscillator.

209 tonal organs (Johnston's organ) of the adult antenna project into the centrolateral neuropil column o

210 from the same direction, making a directive antenna prone to receive echoes and reflections.

211 conformational and electronic changes at the antenna protein complexes as a response to specific chem

212 enna complex, the Fenna-Matthews-Olson (FMO) antenna protein from green sulfur bacteria, completely l

213 ond defect in the mutant, namely in CP26, an antenna protein known to be required for the formation o

214 Photosynthetic antenna proteins can be thought of as "programmed solven

215 rometry analysis to be mainly photosystem II antenna proteins, such as LIGHT-HARVESTING COMPLEX B (LH

216 erived by solving the inverse problem of the antenna radiation field.

217 Here, plasmonic antenna radiation mediates a three-step conversion proce

218 These observations indicate that antenna-reactor complexes may greatly expand possibiliti

219 The antenna-reactor geometry efficiently harnesses the plasm

220 ansition from noble metals to aluminum based antenna-reactor heterostructures in plasmonic photocatal

221 -abundant embedded aluminum in cuprous oxide antenna-reactor heterostructures that operate more effec

222 transition metal-based catalysts, known as 'antenna-reactor' nanostructures, holds promise to expand

223 sbS acts as a 'seeding' centre for the LHCII antenna rearrangement that is involved in NPQ.

224 These ME antennas receive and transmit electromagnetic waves thro

225 , spectroscopy, radar, and frequency scanned antenna reflectors.

226 State-of-the-art compact antennas rely on electromagnetic wave resonance, which l

227 at 200 THz, producing only a small shift of antenna resonance frequency.

228 n 'hot' and 'cold' sensors in the Drosophila antenna, revealing the existence of novel periphery-to-b

229 couplings are not only between the adjacent antenna rings, but also involve their second (2(nd)) nea

230 del reveals the mutual couplings between the antenna rings.

231 ng the absorption strongly resonant with the antenna's enhanced EM fields.

232 sitive to movement in different parts of the antenna's range, at different frequencies, or at differe

233 groups have looked to plasmonics to overcome antenna-scaling limits and to increase the confinement.

234 Vice versa, these antennas sense the magnetic fields of electromagnetic wa

235 We verified the performance of nano-antenna sensing chip by both THz spectra and images of t

236 proach based on passive harmonic transponder antenna sensor and frequency hopping spread spectrum (FH

237 ic transponder sensor, metamaterial-inspired antenna sensor, and FHSS pattern analysis based sensor d

238 ts harmonic band and re-radiates through the antenna sensor.

239 efficiency (plasmon --> plasmon) of 38% for antenna separation 4lambda0 (with lambda0 the free-space

240 5-GHz system capable of powering up to three antennas simultaneously.

241 ng complex II (LHCII), PSII light harvesting antenna (site); and changes in the antenna induced by De

242 The only solution was increasing the antenna size into hundreds of microns, which makes repor

243 o assess the influence of varying LHCI/LHCII antenna size on state transitions.

244 duce the amount of pigments per cell and the antenna size.

245 yt) b6f complex and Stt7 kinase regulate the antenna sizes of photosystems I and II through state tra

246 ectromagnetic wave resonance, which leads to antenna sizes that are comparable to the electromagnetic

247 rs, purification of complexes with different antenna sizes was achieved with mild detergent solubiliz

248 able wires and interconnects, reconfigurable antennas, soft sensors, self-healing circuits, and confo

249 a smaller vessel size (P = .036) and vessel-antenna spacing (P = .006).

250 dentified in the ablation zone, its size and antenna spacing were recorded and correlated with vascul

251 i does not change the cell fate (from eye to antenna-specific fate).

252 The bulk acoustic waves in ME antennas stimulate magnetization oscillations of the fer

253 sms for polarization conversion by plasmonic antennas: Structural asymmetry and plasmon hybridization

254 reen-sulfur bacteria sunlight is absorbed by antenna structures termed chlorosomes, and transferred t

255 lectron mobility transistor (HEMT) with nano antenna structures was fabricated and demonstrated to be

256 gy transfer, in particular multichromophoric antenna structures, is shown to vary depending on the sp

257 arization controls, artificial waveguides or antenna substrates and polarization-enabled resonators w

258 -LHCI supercomplex can bind up to eight Lhcr antenna subunits, which are organized as two rows on the

259 Small resonator antennas, such as metaresonator antennas, have narrow ba

260 quenching, occurs within the photosystem II antenna system by the action of two essential light-harv

261 The interaction of PsbS with the antenna system is affected by both DeltapH and the level

262 Therefore, the light-harvesting antenna system of photosystem II in thylakoid membranes,

263 ding to EET optimization of light-harvesting antenna systems while exploring the structure and functi

264 imic natural photosynthesis using artificial antenna systems, such as conjugated polymers (CPs), dend

265 t they require such a large current that the antenna temperature is raised to the thermal damage thre

266 re, we introduce a low-profile bidirectional antenna that can be mounted on a large ground plane and

267 the odorant receptors expressed in the male antenna that detect the pheromone.

268 et al. have developed acoustically actuated antennas that couple the acoustic resonance of the anten

269 a planar array with eight such bidirectional antennas that were configured as a sparse array in order

270 For dipole-like antennas the strong electric field dissipates too much p

271 By providing an external optical antenna, the balance can be shifted; spontaneous emissio

272 s are related to the currents in the optical antennas, the LCC model provides a useful tool for the a

273 ssion of single molecules close to plasmonic antennas, therefore, provides mixed information of both

274 antum yield achieved through coupling of the antenna-tip to the dark exciton out-of-plane optical dip

275 s, energy is transferred from photosynthetic antenna to reaction centers via ultrafast energy transfe

276 ed that siderocalin can act as a synergistic antenna to sensitize the luminescence of trivalent lanth

277 pattern from a sectional-uniform line source antenna to the focal volume of a 4Pi focusing system.

278 ology addresses the ability of an individual antenna to transfer its absorbed energy towards a single

279 the electric and magnetic resonances of such antennas to achieve a very strong dependence of the opti

280 nt transport of energy from light-harvesting antennas to photosynthetic reaction centres.

281 nctions as a "proton-collecting/distributing antenna" to facilitate rapid lactate flux via MCT1.

282 -harvesting complexes, mimicking the modular antenna/transducer architecture of natural photosystems,

283 As a result, antennas typically have a size greater than one-tenth of

284 anding of humidity sensing in the Drosophila antenna, uncover a neuronal substrate for early sensory

285 mechanically flexible transmission lines and antennas under various bended cases were experimentally

286 diates to the far-field by coupling with the antenna via plasmonic states, whose presence increases t

287 ntum dots in the near field of gold nanocone antennas, we enhance the radiative decay rates of monoex

288 rature, the proteins of the light-harvesting antenna were greatly down-regulated and the phycobilisom

289 Antennas were randomized to either parallel (180 degrees

290 These antennas were then characterized in vivo in five anesthe

291 lications of these structures are leaky-wave antennas which utilize the low frequency dependence.

292 hat excitation moves diffusively through the antenna with a diffusion length of 50 nm until it reache

293 + Cu straight, 2r-rs strongly reclival, and antenna with homonomous flagellum, revealing new and imp

294 as that couple the acoustic resonance of the antenna with the electromagnetic wave, reducing the ante

295 esting that the putative association of this antenna with the PSI supercomplex is absent or may be lo

296 To this end, DNA origami-based optical antennas with a height of around 125 nm are used, which

297 actuated nanomechanical magnetoelectric (ME) antennas with a suspended ferromagnetic/piezoelectric th

298 olled by the association of light-harvesting antennas with accessory quenchers such as carotenoids.

299 The ME antennas (with sizes as small as one-thousandth of a wav

300 iniaturization over state-of-the-art compact antennas without performance degradation.