ライフサイエンスコーパス: emitter

1 (which tolerate ozone stress better than non-emitters).

2 ter interactions (e.g., the decay of quantum emitters).

3 led monolayer (SAM), and a ballistic carrier emitter.

4 n a coaxial gas flow is added around the ESI emitter.

5 loped as an efficient, stable phosphorescent emitter.

6 antage of the full electronic spectrum of an emitter.

7 nipulate particles using even a single-sided emitter.

8 localization precisions calculated for each emitter.

9 oiety remains intact and serves as the light emitter.

10 g the absorptivity and emissivity of thermal emitters.

11 ential decay, typical of single energy level emitters.

12 or-based AC devices and OLEDs using the same emitters.

13 ission is indistinguishable from spin-coated emitters.

14 al properties of single-molecule fluorescent emitters.

15 ologically protected, nonreciprocal acoustic emitters.

16 ectrometry via fully integrated electrospray emitters.

17 gning efficient Ir(III)-based phosphorescent emitters.

18 l dichalcogenide photodetectors, sensors and emitters.

19 let equilibration dynamics in this family of emitters.

20 TE-polarized III-Nitride-based deep UV light emitters.

21 region material for high performance deep UV emitters.

22 y bright and stable to be observed as single emitters.

23 ials, waveguides, light absorbers, and light emitters.

24 s that only good absorbers make good thermal emitters.

25 of chemical-vapour-deposited graphene light emitters.

26 fabrication of highly polarized white light emitters.

27 cts in layered hBN as reliable single photon emitters.

28 her high-affinity mAbs and short-lived alpha-emitters.

29 hly efficient pure-blue device based on TADF emitters.

30 low threshold for any laser using colloidal emitters.

31 ents aiming to investigate this new class of emitters.

32 e electrically-driven GaN:Eu based red light emitters.

33 anometal-halide-perovskite/polymer composite emitters.

34 ide a pathway to design tailored white-light emitters.

35 rticle emitter (177)Lu or the Auger electron-emitter (111)In.

36 en for the separation of the long-lived beta-emitters (129)I, (36)Cl and the alpha-emitters (154)Dy,

37 d beta-emitters (129)I, (36)Cl and the alpha-emitters (154)Dy, (148)Gd, (150)Gd, and (146)Sm from Ta

38 ked to DOTA for complexing the beta-particle emitter (177)Lu and to panitumumab for targeting epiderm

39 these bsRICs labeled with the beta-particle emitter (177)Lu or the Auger electron-emitter (111)In.

40 Results using the beta-emitters (188)Re, (177)Lu, and (90)Y and the alpha-emitt

41 The PSMA-targeting Auger emitter 2-[3-[1-carboxy-5-(4-(125)I-iodo-benzoylamino)-p

42 emitting diodes (W-OLEDs) composed of three emitters (2,7-bis(9,9-dimethyl-acridin-10-yl)-9,9-dimeth

43 rs (188)Re, (177)Lu, and (90)Y and the alpha-emitters (211)At, (213)Bi, and (212)Pb were compared.

44 The combined alpha-, gamma-, and x-ray emitter (213)Bi (half-life, 46 min) is promising for rad

45 t DNA scales was also compared with an alpha emitter, (223)Ra.

46 n addition to being the first approved alpha-emitter, (223)RaCl2 is the first radiopharmaceutical to

47 e designed and synthesized two isomeric TADF emitters, 2DPyM-mDTC and 3DPyM-pDTC, based on di(pyridin

48 shed through radiolabeling with the positron emitter (89)Zr.

49 posed to work as wideband spectral-selective emitters/absorbers due to the topological change in isof

50 tribution of measurements, where a few large emitters accounted for most of the emissions.

51 For a given nanoESI emitter, accurately controlled ion pulses ranging from 1

52 OLEDs fabricated with these TADF emitters achieved excellent efficiencies up to 16 % exte

53 antum yields than commonly employed infrared emitters across the entire infrared camera sensitivity r

54 ction, enabled by an integrated electrospray emitter, allows us to detect a short-lived radical metab

55 ochromic material composed of a metamaterial emitter and a bimaterial micro-electro-mechanical system

56 em using an organic crystal DSTMS as the THz emitter and a low temperature grown (LTG) InGaAs/InAlAs

57 d the desired impedance matching between the emitter and absorber modes along with their coupling to

58 t is achievable by using a selective thermal emitter and by eliminating parasitic thermal load, and e

59 mance is a novel photonic design forcing the emitter and cell single modes to cros resonantly couple

60 arge area suspended photonic crystal thermal emitter and electrical injection.

61 ere we show that the interference between an emitter and its image dipole induces a strong polarizati

62 potentials in the high efficient infra light emitter and photo-voltaic devices.

63 d receivers, calls are not beneficial to the emitter and should be selected against because of the co

64 320 mus by changing the distance between the emitter and the heated inlet to the mass spectrometer an

65 elayed fluorescence (TADF) materials both as emitters and as hosts is an exploding area of research.

66 mically thin, flexible and transparent light emitters and displays with low operation voltage and gra

67 r(III) complexes can serve as both deep blue emitters and efficient hole-conducting EBLs.

68 Synthesized molecules were used as emitters and electron transporters in three different de

69 provides a novel framework for creating new emitters and for interpreting observations in many field

70 The new complexes are efficient red emitters and have been used in the active layers in ligh

71 The use of theta-glass emitters and mass spectrometry to monitor reactions that

72 onfined photonic modes can couple to quantum emitters and mechanical excitations.

73 nteractions and a low-loss interface between emitters and optical fields.

74 er new iron-based materials for use as light emitters and photosensitizers.

75 tion paves the way to carbon-based polariton emitters and possibly lasers.

76 we employ surface-plasmon-polariton thermal emitters and silver-backed semiconductor-thin-film photo

77 Tailoring the interactions between quantum emitters and single photons constitutes one of the corne

78 development of N-heterocyclic carbene-based emitters and tetradentate cyclometalated Pt and Pd compl

79 to which this leads to inequity between GHG emitters and those impacted by the resulting climate cha

80 ved in the application of these molecules as emitters and transporters, a detailed photophysical char

81 y rotating an interdigitated photoconductive emitter, and by detecting the orthogonal components of t

82 Ds) embedded in an InGaAs quantum well as an emitter, and GaAs as an active mediator of surface plasm

83 orescence emission makes the molecule a good emitter, and the charge delocalization properties leadin

84 of POZ-DBPHZ in a device with more than one emitter, and the combination of the three materials, res

85 catterers, simultaneous photon absorbers and emitters, and all the way to simultaneous photon absorbe

86 ptical filters, thermophotovoltaics, thermal emitters, and hot-electron collection.

87 s as they are simultaneous photon absorbers, emitters, and scatterers.

88 d longer-lived excited states, were brighter emitters, and stored more free energy than did the non-i

89 tructures in photodetector, sensor and light emitter applications.

90 l-molecule, dendrimer, polymer, and exciplex emitters are all discussed within this review, as is the

91 Single-quantum emitters are an important resource for photonic quantum

92 High emitters are best predicted as unplugged gas wells and p

93 for the metal-free room-temperature triplet emitters are correlated with phosphorescence efficiency.

94 TADF emitters are cross-compared within specific color ranges

95 unately, the luminescent properties of these emitters are frequently degraded by blinking and photobl

96 These findings suggest that alpha-emitters are highly efficacious in MRD settings, where i

97 obtained using rapid mixing from theta-glass emitters are independent of protein identity.

98 According to the presented model, alpha-emitters are needed to achieve radiation doses high enou

99 quantum-mechanical correlations between the emitters are present.

100 Furthermore, these emitters are stable to material transfer to other substr

101 ts over 2 years show that flow rates of high emitters are sustained through time.

102 Small nanoelectrospray emitters are used to form protein and protein complex io

103 Theta-glass emitters are used to rapidly mix two solutions to induce

104 rmally-activated delayed fluorescence (TADF) emitter, are studied.

105 An electron emitter as a soft atmospheric pressure chemical ionizati

106 sing a doped NaCl film with a phosphorescent emitter as the emissive layer.

107 y via nanoelectrospray ionization (nano-ESI) emitters as a powerful tool for fast quantitative analys

108 the characterization of electroluminescence emitters as quantum light sources, which can be studied

109 w that the emission intensity of the thermal emitter at the CO(2) absorption wavelength is enhanced a

110 gnal enhancement relative to a single-nozzle emitter at the same total flow rate.

111 The energy deposition of most Auger electron emitters at DNA scales of 2 nm or less exceeded that of

112 een successfully applied to photonic-crystal emitters at moderate temperatures, but is exceedingly di

113 orescence spectroscopy, we interrogate these emitters at the single-molecule level and compare their

114 ers) in 4H-SiC, which serve as single-photon emitters at visible wavelengths, are used as a model sys

115 opens up a new route towards superior light emitters based on bulk quantum materials.

116 f earth abundant, inexpensive phosphorescent emitters based on metal-halide nanoclusters are reported

117 rmally activated delayed fluorescence (TADF) emitters based on U-shaped D-A-D architecture with a nov

118 a wavelength-selection mechanism for thermal emitters, both for the enhancement and the suppression o

119 ioactivity concentrations of alpha- and beta-emitters bound to mAbs were compared.

120 mediate the molecular configurations of the emitters, but also promote nonradiative quenching pathwa

121 thm determines the center of the fluorescent emitter by finding the position with the best-fit gradie

122 nce device based on 3DPyM-pDTC as the dopant emitter can reach an extremely high external quantum eff

123 indicate that rapid mixing with theta-glass emitters can be used to access significantly faster reac

124 de derivatives with the short-lived positron emitter carbon-11 (t1/2 = 20.4 min) in generally good to

125 diolabeled with the short-half-life positron emitter carbon-11, which is rather impractical for many

126 king advantage of the symmetry of the single emitter cavity mode.

127 uption of the excitonically coupled terminal emitter Chl trimer results in an increased sensitivity o

128 The absorption process of an emitter close to a plasmonic antenna is enhanced due to

129 Using recently-developed THz emitters constructed from single crystals of the high-Tc

130 w a lognormal distribution, with the top 10% emitters contributing 49 to 66% to the inferred total po

131 We achieve near unity emitter creation probability and a mean positioning accu

132 egistration techniques, we achieve a quantum emitter deterministically positioned at a chiral point a

133 The defects are single-photon emitters, do not blink, and have photoluminescence lifet

134 gy on a single Chl a pigment in the terminal emitter domain due to very specific pigment orientations

135 Our single-emitter DPA-MnQdots exhibit two emission bands, at 510nm

136 vidual chains still behave as single quantum emitters due to efficient excitation energy transfer, wh

137 Using these nanoparticles as emitters, efficient electroluminescence is achieved with

138 Ensembles of solid-state optical emitters enable broadband quantum storage and transducti

139 g on sequential localization of single point emitters enable spatial tracking at ~10-40 nm resolution

140 tional components (transistors, solar cells, emitters, etc.) that can enable a diversity of emerging

141 ission, we engineer a tungsten-based thermal emitter, fabricated in an industrial CMOS process, and d

142 the position and orientation of the quantum emitter for optimum coupling.

143 synthesis of a novel fluorene based organic emitter for potential use in organic light emitting devi

144 ates the applicability and robustness of the emitter for real scientific challenges using modern LC/M

145 acterized as promising green/yellowish green emitters for electroluminescent applications.

146 , providing a new platform of phosphorescent emitters for low-cost and high-performance light-emissio

147 ested for use as multiple electrospray (MES) emitters for mass spectrometry (MS).

148 ilayered metamaterials become good absorbers/emitters for visible light and good reflectors for IR li

149 ge over existing defect centre single-photon emitters (for example, diamond defect centres).

150 several promising low-energy beta- and alpha-emitters, for radionuclide therapy.

151 cient interfaces between photons and quantum emitters form the basis for quantum networks and enable

152 ite light delivery with three output grating emitters from a single laser input is demonstrated.

153 A comparison of differently shaped emitters, from flat over edged to pulled geometries, rev

154 ion wavelength of efficient ultraviolet (UV) emitters further into the deep-UV requires material with

155 d thus enhances TET from 5-CT to the rubrene emitter, further bolstering the upconverison QY.

156 These deep red emitters generally showed poor performance with electrol

157 atures, but is exceedingly difficult for hot emitters (>1,000 K).

158 Alpha-particle emitters have a high linear energy transfer and short ra

159 Quantum light emitters have been observed in atomically thin layers of

160 were substantially higher, with some "super emitters" having emission rates up to 3447 kg/h, more th

161 hyl oxalacetate (DOA) in the strong isoprene emitter hybrid aspen (Populus tremula x Populus tremuloi

162 and O2 concentrations in the strong isoprene emitter hybrid aspen (Populus tremula x Populus tremuloi

163 ds is to scatter coherent light from quantum emitters, imprinting quantum correlations onto the photo

164 unds are detected by direct contact with the emitter in aquatic environments and are perceived at hig

165 loparaphenylene derivative is involved as an emitter in low power light frequency conversion.

166 2 substrates can be used as a low-efficiency emitter in the mid-infrared range.

167 is previously unexplored solid-state quantum emitter in WSe2 generates single photons with emission p

168 which requires positioning of single quantum emitters in a deterministic fashion.

169 achieve a two-dimensional lattice of quantum emitters in an atomically thin semiconductor.

170 Room-temperature quantum emitters in gallium nitride (GaN) are reported.

171 The emergence of single quantum emitters in layered transition metal dichalcogenide semi

172 ce (TADF) have gained high attractiveness as emitters in organic light emitting diodes (OLEDs) and ot

173 scalable integration of high-quality quantum emitters in photonic quantum technologies.Inhomogeneous

174 Our method may enable the placement of emitters in photonic structures such as optical waveguid

175 rong-coupling regime.Effective use of single emitters in quantum photonics requires coherent emission

176 compounds either as host emitters or dopant emitters in suitable host matrix and exhibited green/yel

177 multaneous photon absorbers, scatterers, and emitters in the UV-vis wavelength region.

178 deterministic arrays of hundreds of quantum emitters in tungsten diselenide and tungsten disulphide

179 racterize key attributes that accompany high emitters, including depth, type, plugging status, and co

180 By directly embedding light emitters into subwavelength cavities of plasmonic interf

181 s when the experimental set-up enclosing the emitter is exposed to peak solar irradiance.

182 ear-omnidirectional and spectrally selective emitter is obtained as the emission changes due to mater

183 The application of plasmonics to thermal emitters is generally assisted by absorptive losses in t

184 rmally activated delayed fluorescence (TADF) emitters is highly desired for the practical application

185 A better characterization of super-emitters is needed to operationalize ways to identify th

186 The distribution of emitters is peaked in the 0-5 kg/h range, with a signifi

187 This layer acts as a gate between the emitter layer and the voltage contact.

188 (i) mass-signal frequency allometry and (ii) emitter-limited (maximum gape) signal directionality.

189 ct band gap, inorganic, stable and efficient emitter material for on-chip photonics without the need

190 For alpha-emitters, microtumors receive high doses (>20 Gy or 100

191 of thermally activated delayed-fluorescence-emitter molecules can be manipulated in the solid state

192 s Sm(III) and Dy(III), and the near-infrared emitters Nd(III) and Yb(III).

193 An emitter near a surface induces an image dipole that can

194 sion signals are enhanced by 40x that of the emitters not embedded in the metamaterial and display a

195 ral center of the metamaterial is opened and emitters occupy this light-confining and chirally sensit

196 now surpassing China as the world's largest emitter of anthropogenic SO2.

197 t subsequently oxidizes to oxyluciferin, the emitter of bioluminescence.

198 t, with 4 of the world's 10 largest national emitters of CO2.

199 repared by spin-coating a dilute solution of emitters on a microscope cover slip of silicate based gl

200 posed source can enable tunable, compact THz emitters, on-chip integrated spectrometers, inspire a br

201 nctional optical elements for flexible light emitter or on-chip all-optical devices.

202 ted employing these compounds either as host emitters or dopant emitters in suitable host matrix and

203 coatings for QDs for applications as robust emitters or high fidelity sensing platforms.

204 f less volatile radionuclides, pure beta-ray emitters or simply radionuclides with very long half-liv

205 The emitters originate from cubic inclusions in hexagonal la

206 The largest volcanic emitters outgas carbon with higher delta(13)C and are lo

207 ows spectral tunability of hBN single photon emitters over 6 meV, and material processing sharply imp

208 ia, an NYDF signatory, is the second highest emitter, peaking in 2012 at 0.362 Gt CO2 yr(-1) before d

209 The emitter planar plasmonic nature allows for high-power an

210 g light are direct modulation of the excited emitter population (for example, using semiconductor las

211 platform to manipulate the decay of quantum emitters, possibly leading to the exploration of qualita

212 The emitter presented here contains structural modifications

213 electrodes and temperature dependence of the emitter properties.

214 hene's edges, switchable atomic-scale phonon emitters provide the dominant dissipation mechanism.

215 norganic passivation of defect-based quantum emitters provides a new method for enhancing photostabil

216 n greatly reduce the lasing threshold of the emitter, providing a low-threshold laser system with sma

217 riodical nanocone-arrays were employed in an emitter region for high efficient Si solar cells.

218 However, identifying high emitters remains a challenge.

219 Conventional nonradioactive electron emitters require high vacuum (<10(-6) hPa) to prevent el

220 The overlapping emission contaminates each emitter's detection channel, referred to as cross-talk.

221 We found embedded information about the emitter's size in juvenile calls of several species, and

222 between the detected homodyne signal and the emitter's state, and map out the conditional back-action

223 neration of nearly transform-limited quantum emitters should facilitate the development of scalable s

224 all confirm the MES behavior of the 9-nozzle emitter, showing significant signal enhancement relative

225 This nanocone-arrayed selective emitter simultaneously satisfies optical and electrical

226 , as beam directionality increases with both emitter size (maximum gape) and signal frequency.

227 pling the point spread function due to small emitter size and intensity overlap of proximal objects.

228 for multiple Ln(III), including the visible emitters Sm(III) and Dy(III), and the near-infrared emit

229 age and conversion devices, actuators, field emitters, solid-phase microextraction, springs, and cata

230 spectrometer and the voltage applied to the emitter source.

231 Samples for single-emitter spectroscopy are usually prepared by spin-coatin

232 Single quantum emitters (SQEs) are at the heart of quantum optics and p

233 Auger electron emitters such as (125)I have a high linear energy transf

234 nd showed the benefit of instead using alpha-emitters such as (211)At.

235 or enabling deposition of metallic Ag on the emitter surface and precipitation of Ag nanocrystals wit

236 ith the radionuclide (131) I (beta(-) /gamma emitter, t1/2 8.02 d), and their activity in MCF-7 human

237 m (2) with >45% efficiency at 2100 degrees K emitter temperature and 60 Omega electrode square resist

238 mple performances include: at 1200 degrees K emitter temperature, output power density 2 W/cm(2) with

239 ngle-molecule experimental technique with an emitter that is sensitive to triplet dynamics, yet read

240 Near-infrared (NIR) emitters that can also be excited with NIR radiation via

241 nding can lead to a new generation of bright emitters that can be used as ECL labels.

242 citons towards isolated strain-tuned quantum emitters that exhibit high-purity single photon emission

243 an emerging class of synthetic single-photon emitters that hold vast potential for near-infrared imag

244 pon the specific structure of the individual emitters that lead to gain.

245 is strong motivation to develop electrospray emitters that operate at practical flow rates but give t

246 ells using surface-plasmon-polariton thermal emitters, that the resonant nature of the nanophotonic s

247 The photophysical properties of these emitters therefore involve new inherent complexities and

248 applications in absorption filters, thermal emitters, thermophotovoltaics and sensing.

249 et size, which can be varied by changing the emitter tip diameter, and on the solution composition.

250 ) with conventionally sized nanoelectrospray emitter tips but are resolved with 0.5 mum tips.

251 es in solution and the glass surfaces of the emitter tips that are negatively charged.

252 ns, corona discharge is commonly observed at emitter tips, resulting in low ion abundances and reduce

253 rospray ionization MS using 1.6 mum diameter emitter tips, resulting in no mass information.

254 is described here that employs a movable ES emitter to control the reactivity of charged microdrople

255 ultiroles as sample loading substrate and an emitter to generate electrospray.

256 tage of evanescent photon tunneling from the emitter to the absorber.

257 Coupling a quantum emitter to the band edge of a photonic crystal waveguide

258 upling of the emission from a single quantum emitter to the channel plasmon polaritons supported by a

259 suitable radiotracer able to deliver a beta- emitter to the tumor has to be identified.

260 for a radiotracer that can deliver a beta(-) emitter to the tumor is a fundamental step in the deploy

261 notubes (SWCNTs) are promising absorbers and emitters to enable novel photonic applications and devic

262 cifically, these polar dielectrics can cause emitters to preferentially decay by the emission of pair

263 Such devices range from novel coherent light emitters to reconfigurable potential landscapes for elec

264 e a road map to label-free detection of many emitters too weakly fluorescent for present approaches.

265 e generally not taken into account in single-emitter tracking and super-resolved imaging applications

266 51 GHz and close to lifetime-limited single-emitter transition linewidths down to 126+/-13 MHz corre

267 These results indicate that the terminal emitter trimer is thus an essential design principle for

268 For beta-emitters, tumors will receive almost entirely nonspecifi

269 w 50 nL.min(-1) very sharp, pulled nanospray emitters turned out to be mandatory for the generation o

270 Recently developed all-organic emitters used in display applications achieve high brigh

271 of the broad emission profile of each of the emitters used in fluorescence detection.

272 Emission rates of high emitters varied from 150-250 to 880-1470 kg/h and region

273 otonic cluster states using a single quantum emitter via time-delayed quantum feedback.

274 om the sample to the electrospray ionization emitter was determined using glycerol/methanol droplets

275 Each emitter was doped into a 4,4'-bis(N-carbazolyl)-1,1'-bip

276 interface separated in space from the spray emitter, was investigated in this work.

277 this concept to a large-area photoconductive emitter, we demonstrate diffraction-limited ultra-broadb

278 similar luminescence intensities with 2-4 Ln-emitters were identified.

279 cently, bright and photostable single photon emitters were reported from atomic defects in layered he

280 easure flow rates at the tip of electrospray emitters when the ionization voltage is turned off.

281 4-fold compared to a standard non-plasmonic emitter, which enables a proportionate increase in the s

282 fluorophores, our design uses only a single emitter, which simplifies ratiometric sensing and broade

283 rich toolbox to tailor properties of quantum emitters, which can facilitate design guidelines for dev

284 These inorganic emitters, which exhibit rich photophysics combined with

285 difference between independent and entangled emitters, which is at the heart of quantum mechanics, ca

286 the time-resolved photoluminescence of these emitters, which is dominated by static disorder in the p

287 ly the blinking and photoinduced recovery of emitters, which stimulated further development of photos

288 (99)Tc is an artificial beta emitter widely used in nuclear medicine for diagnostic t

289 emonstrate a proof-of-principle incandescent emitter with efficiency approaching that of commercial f

290 Bright green emitters with adjustable photoluminescence (PL) maxima i

291 requency range mainly due to the lack of THz emitters with broad bandwidth suitable for the purpose.

292 uced emission cross-talk between colocalized emitters with closely overlapping fluorescence, and vali

293 ay enable lithographic patterning of quantum emitters with electronic and molecular precision.

294 ng for MD information would aim to encourage emitters with large MDs to reduce their emissions.

295 cise position information on single-molecule emitters with limited photons.

296 noplatelets, which are efficient nanocrystal emitters with the electronic structure of quantum wells,

297 nic hybrid perovskites are emerging low-cost emitters with very high color purity, but their low lumi

298 Such emitters, with micron-scale dimensions and the freedom t

299 m dots-a mature class of solid-state quantum emitter-with low-loss Si3N4 waveguides.

300 havior of electromagnetic waves (directional emitter) without any reflectors.