ライフサイエンスコーパス: emitter

1 oot of the average number of activations per emitter.

2 n approximately 1,455-kelvin silicon carbide emitter.

3 stal evanescent zone and Fresnel zone of the emitter.

4 lied to mainland China-the largest global Hg emitter.

5 al upper bound on squeezing from a two-level emitter.

6 us(A206) homodimer behave as a single-photon emitter.

7 a strained superlattice and a heterojunction emitter.

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

9 loped as an efficient, stable phosphorescent emitter.

10 e example of a non-triangulene-based MR-TADF emitter.

11 e energy (DeltaE(ST) < 1600 cm(-1)) in these emitters.

12 n structured subwavelength arrays of quantum emitters.

13 ution of phase angles between multiple sound emitters.

14 e, which was not possible using conventional emitters.

15 ently been reported as efficient white light emitters.

16 s is linked to structural defects of bilayer emitters.

17 he probability to match randomly distributed emitters.

18 fine structure, as exhibited by most quantum emitters.

19 erovskites are promising next generation NIR emitters.

20 riton-based electrically pumped mid-infrared emitters.

21 ttention as highly efficient broadband light emitters.

22 eneration of stable blue carbene-metal-amide emitters.

23 mmercially employed Ir(III)- or Pt(II)-based emitters.

24 es compared to oral-emitters and other nasal emitters.

25 xene as the acceptor subunit of soluble blue emitters.

26 s expected for excited-state proton-transfer emitters.

27 ture applications of metallic spintronic THz emitters.

28 nt challenges to the studies of these unique emitters.

29 t antibunching as required for single-photon emitters.

30 enabling efficient fiber-coupling of quantum emitters.

31 But, active modes of transport are not zero emitters.

32 g the absorptivity and emissivity of thermal emitters.

33 low threshold for any laser using colloidal emitters.

34 ential decay, typical of single energy level emitters.

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

36 properties of the widely used Eu(III)-based emitters.

37 s to boost radiation efficiencies of quantum emitters.

38 on of these colors from organic, white light emitters.

39 types of high-performance ultraviolet light emitters.

40 e of different physical properties, the beta-emitters (177)Lu and (90)Y offer specific radiologic-bio

41 ults: In a dose-response study with the beta-emitter 177Lu-DOTA-daratumumab, the lowest tested dose,

42 DOTAylated-huCC49 was labeled with the alpha-emitter (225)Ac to target tumor-associated glycoprotein

43 In contrast, the alpha-emitter 225Ac-DOTA-daratumumab had a dose-dependent effe

44 They comprise the alpha-emitter (227)Th complexed to a 3,2-hydroxypyridinone che

45 rmally activated delayed fluorescence (TADF) emitters, 2tDMG and 3tDMG, are synthesized for high-effi

46 Solid-state emitters(5), such as quantum dots and defects in diamond

47 perconducting qubit(5-7) or a single optical emitter(8-12).

48 rved distribution is skewed with the top two emitters accounting for 20% of the total methane emissio

49 Methane 'super-emitter' activity occurs in every sector surveyed, with

50 Beyond green emitters, Aequorea species express purple- and blue-pigm

51 Interactions between a single emitter and cavity provide the archetypical system for f

52 icropillars, separating the high-temperature emitter and low-temperature receiver, manufactured withi

53 nsically limited by the distance between the emitter and nanostructure surface, owing to a tightly-co

54 ass (m*)] are determined for both the n-type emitter and p-type bulk wafer Si of an industrially prod

55 iffusion length are calculated in the n-type emitter and p-type wafer Si with the results also being

56 of distance and relative orientation between emitter and receiver and evaluate it in a sample of 401

57 ts normally associated with both the thermal emitter and sensor; allowing step-change increases in bo

58 ansfer from the PbS NC light absorber to the emitter and thus a higher photon upconversion QY.

59 both an (active) blue-color-emitting nanorod emitters and a (passive) normal reflector of phosphor em

60 the far-field emission patterns of embedded emitters and allow the reconstruction of dipole position

61 form has been modified for static native ESI emitters and an extended mass-to-charge range (20 kDa m/

62 n sources, we finally were able to embed two emitters and an ion transfer tubing into a small, hand-h

63 the only route to charging localized quantum emitters and another path forward is through band struct

64 ties, enabling applications as single-photon emitters and bio-imaging agents.

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

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

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

68 nt step toward the direct writing of quantum emitters and other functionalities at the molecular leve

69 intermediate cranial shapes compared to oral-emitters and other nasal emitters.

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

71 ations, in particular photovoltaics, thermal emitters and sensors.

72 cal maximum (5%) of conventional fluorescent emitters and that with linear analogue (6.9%).

73 s that includes uncertainty in the number of emitters and the background structure, and a set of coor

74 ploited for the development of new, improved emitters and their fabrication into OLEDs/LECs with high

75 electronically carbonyl CH(3)CO(*) is the CL emitter, and the silicon-oxygen skeleton in the organosi

76 related to photocatalysis, solid-state light emitters, and chemical sensing will be addressed.

77 ewed interest in therapy with alpha-particle emitters, and their potential for sterilizing disseminat

78 tructures in photodetector, sensor and light emitter applications.

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

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

81 y, the nonradiative decay rates of these ICT emitters are decreased and become lower than the radiati

82 using lead-tin (Pb-Sn) halide perovskite as emitters are demonstrated.

83 tion about the refractive index in which the emitters are embedded, their nanometric distance from th

84 Remote sensing and manipulation of quantum emitters are functionalities of significant practical im

85 Immobilized on a surface, the emitters are initially dark (>99.8% quenched), providing

86 However, present room-temperature OLPL emitters are mainly based on a bimolecular exciplex syst

87 Such thermal emitters are necessary for a wide variety of application

88 Thermal emitters are open systems that can benefit from the rich

89 the crystal structures of key RGB and yellow emitters are reported.

90 Copper(I)-based emitters are well-known to suffer from weak spin-orbit c

91 le light source comprised of a silicon Field Emitter Array integrated with a silicon nanograting that

92 on and decoherence-free subspaces of quantum emitter arrays at the many-body level(10-13).

93 collective excitonic phases(19) and quantum emitter arrays(20,21) via domain-pattern engineering.

94 ooling improvement of this selective thermal emitter as compared to that of a non-selective emitter a

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

96 sitely sensitive to radiation, and the alpha-emitter astatine-211 (211At) deposits prodigious energy

97 itter as compared to that of a non-selective emitter at night, and 5 degrees C sub-ambient cooling un

98 otential of these plasmonic "crystal balls." Emitters at the center are now found to live indefinitel

99 interfaces impede photon collection, and the emitters' atomic scale necessitates the use of free spac

100 Here, we consider a series of emitters based on substituted triarylamine (TAA) donors

101 restricted to single devices and few quantum emitters because fabrication constraints limit device fu

102 t detected using conventional MS with larger emitters because nanoscale emitters significantly reduce

103 twist angles of approximately 20 degrees the emitters become two orders of magnitude dimmer; however,

104 ) can be tuned as a single ionic white light emitter by a simple modification of the coordination env

105 problem of spectral diffusion in solid-state emitters by engineering the electrical environment while

106 lular lethality from a PARP-1-targeted Auger emitter, calling for further investigation into targeted

107 lular lethality from a PARP-1 targeted Auger emitter, calling for further investigation into targeted

108 gas supply chain, this work finds that super-emitters can arise naturally due to variability in under

109 These emitters can be excited at the same wavelength and revea

110 emselves in the excited state, the resulting emitters can obtain a sensory function.

111 nteraction can be obtained to realize a TADF emitter capable of photoluminescence (PL) close to 1000

112 es were ionized using an etched fused-silica emitter capable of stable operation at the ~20 nL/min fl

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

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

115 rtz) for germanium-vacancy (silicon-vacancy) emitters, close to the lifetime-limited linewidth of 32

116 Emitter concentration is varied (x = 1, 2, 5, 10, 20, 50

117 We show how, given proper consideration for emitter concentration, we can design a unique nanopartic

118 itectures, e.g., comprising a single quantum emitter coupled to a nano-mechanical resonator.

119 tichelator construct labeled with a positron emitter (Cu-64, t(1/2) = 12.7 h) is coupled to the viral

120 truction of an in situ 3D response of single emitters directly from single-molecule blinking datasets

121 et of the 77 K afterglow spectra from a TADF-emitter-doped film is not necessarily reliable for deter

122 This is because in some TADF-emitter-doped films, optical excitation can generate cha

123 The emitters exhibit strong circular polarization of the sam

124 be achieved using low-mobility single-layer emitter films with varying thicknesses and energy barrie

125 be a Bayesian inference approach to multiple-emitter fitting that uses Reversible Jump Markov Chain M

126 The emitters fluoresce brightly once switched on by integrin

127 2-oxohexa-3,5-dienoic acid form as the light emitter (fluorescent state) in water solution.

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

129 ngineering and controlling selective thermal emitters for applications in sensing and energy conversi

130 The application of NIR-II emitters for gastrointestinal (GI) tract imaging remains

131 ternet) and the increasing prevalence of THz emitters for imaging (e.g., concealed weapon detection i

132 11 ((11)C) is one of the most ideal positron emitters for labeling bioactive molecules for molecular

133 oadly deployed as photosensitizers and light emitters for numerous synthetic and optoelectronic appli

134 rmally activated delayed fluorescence (TADF) emitters for organic light-emitting diodes (OLEDs).

135 s for replacing traditional rare-metal-based emitters for solar-energy conversion and photoluminescen

136 CCs) have emerged as promising single-photon emitters for solid-state quantum technologies, chemicall

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

138 The emitter g-factors are homogeneous across the same sample

139 bricated with the macrocycle compound as the emitter has achieved a high external quantum efficiency

140 tion of nanomaterials and Cerenkov radiation emitters has been revolutionizing the way nanomaterials

141 widespread introduction of solid-state light emitters has increased the urgency of this problem.

142 ith systematic integration of single quantum emitters has so far been lacking.

143 the incoming light using an array of quantum emitters-has not yet been experimentally demonstrated.

144 ganic light-emitting diodes (OLEDs), The two emitters have a tilted face-to-face alignment of donor (

145 bwavelength arrays of atoms or other quantum emitters have attracted significant interest recently.

146 Radiobiological studies of alpha-particle emitters have been few as they require detailed consider

147 ane antigen (PSMA)-targeting beta- and alpha-emitters have been introduced, with promising response r

148 ts (TDMs) in zero to two-dimensional optical emitters have been well investigated, those in quantum r

149 However, SWIR emitters have not been developed as molecular labels for

150 e photons are generated from passive thermal emitters, have long been limited by low power density.

151 on speed can lead to clusters of overlapping emitter images in the raw super-resolution image data.

152 (EQE), making the search of alternative NIR emitters important for the community.

153 2tDMG used as the emitter in evaporation-processed OLEDs achieves a high e

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

155 t conductor plays the same role as the point emitter in optical imaging.

156 advantages and drawbacks of varying the beta-emitter in PSMA-targeting radioligand therapy.

157 that the waste sector is the largest methane emitter in the GTA.

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

159 More recently, quantum emitters in atomically thin materials such as tungsten d

160 The largest methane emitters in California are a subset of landfills, which

161 ain Monte Carlo to identify and localize the emitters in dense regions of data.

162 Emitters in different locations radiate spots, rings, an

163 pplicability of this new class of low-energy emitters in future photonic applications, such as noncla

164 of applied magnetic field for select quantum emitters in h-BN.

165 ble materials which have recently emerged as emitters in high-performance organic light-emitting diod

166 ules have been devised as high quantum yield emitters in modern organic light-emitting diode technolo

167 le structure-property information on quantum emitters in monolayer WSe(2).

168 Narrow-bore emitters in native MS with inner diameters of ~300 nm we

169 cance owing to the omnipresence of microwave emitters in our daily lives (e.g., food preparation, tel

170 roposed as scalable and color-tunable single emitters in quantum optics, but they have typically suff

171 the growth of monolithic phosphor-free white emitters in the future.

172 ss conditions explain the existence of super-emitters in the natural gas supply chain, this work find

173 cal incorporation of targeted alpha-particle emitters in the treatment of several cancer types.

174 lysis container, microreactor, and nano-ESI emitter) in the experiments.

175 ve mass spectrometry (MS) with nanoscale ion emitters indicate that netropsin can simultaneously and

176 advantage of any prior information, such as emitter intensity and density.

177 Plasmon-emitter interactions are of central importance in modern

178 omplete account of both plasmons and plasmon-emitter interactions at the nanoscale, constituting a si

179 We consider a broad array of plasmon-emitter interactions ranging from dipolar and multipolar

180 plitude and spectral distribution of plasmon-emitter interactions.

181 ained by incorporating a near-infrared (NIR) emitter into the backbone of a polymer host to develop a

182 of an unprecedented well-organization of the emitters into 2D rectangular columnar-like supramolecula

183 inhibitor, (125)I-KX1, we delivered an Auger emitter iodine-125 to PARP-1: a chromatin-binding enzyme

184 )F(4) (exterior shell), where sensitizer and emitter ions are partitioned into core and interior shel

185 0.8)Gd(0.2)F(4) (shell), with sensitizer and emitter ions codoped in the core.

186 Here, a non-Hermitian selective thermal emitter is experimentally demonstrated, which exhibits p

187 behavior opposite to that of hot fluorescing emitters is expected.

188 etry (IMS) via fully integrated electrospray emitters is introduced.

189 e structure that gives rise to these quantum emitters is poorly understood.

190 l and scientific challenge of THz spintronic emitters is to increase their intensity and frequency ba

191 Thus, M2biQ acts as a nearly universal emitter (lambda(em) = 468-690 nm) with large Stokes shif

192 ar cells, light-emitting diodes, white-light emitters, lasers, and polaritonic emission, have followe

193 duced, e.g., by a radioactive alpha-particle emitter like (210)Po.

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

195 interior shell for strong emission, and (3) emitter localization near the nanoparticle surface for e

196 zation algorithms in the literature estimate emitter locations by frame-by-frame localization (FFL),

197 both a posterior probability distribution of emitter locations that includes uncertainty in the numbe

198 correlations, both providing information of emitter locations.

199 While most selective emitter materials are inadequate or inappropriate for bu

200 emission controls targeting relatively large emitters may help significantly reduce both methane and

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

202 tegies in urban areas to be effective, large emitters must be identified.

203 pin qubits, Majorana fermions, single photon emitters, nanoprocessors, etc.

204 er studies in the region, but the top 10% of emitters observed in this study contributed 77% of the t

205 n is currently the largest single industrial emitter of CO(2), accounting for ~8% (2.8 Gtons/y) of gl

206 China is currently the single largest emitter of CO(2), responsible for approximately 27 per c

207 animal feeding operations (CAFOs) are major emitters of both ammonia (NH(3)) and methane (CH(4)).

208 ional emission of the fundamentally smallest emitters of light, i.e., dipoles, as an indicator.

209 Alternatively, radioimmunotherapy with alpha-emitters offers the advantage of depositing much higher

210 is hierarchically designed selective thermal emitter on alleviating global warming and temperature re

211 is hierarchically designed selective thermal emitter opens a new pathway towards large-scale applicat

212 -, or nano-scaled materials, as well as weak emitters or non-radiative materials.

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

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

215 pecies generally coincides with fewer Ln(3+) emitters per unit volume.

216 irborne HAT system implemented using two 256-emitter phased arrays and manipulate individually up to

217 such as chemical sensing, solid-state light emitters, photocatalysis, and optoelectronics.

218 rmation sharing provides fitness benefits to emitter plants, and, therefore, whether selection by her

219 presence of concomitant and dominating gamma emitters, primarily (137)Cs, which results in increased

220 BN) has emerged as a robust host for quantum emitters, promising efficient photon extraction and atom

221 (SMS) provides a detailed view of individual emitter properties and local environments without having

222 fully controlled, phase-stabilized QCL-comb emitters proves that this technology is mature for metro

223 l therapeutic efficacy of beta- versus alpha-emitter radioimmunotherapy using radiolabeled DOTA-darat

224 tracers for imaging and with beta- and alpha-emitter radionuclides for radioimmunotherapy.

225 Alpha-emitter radiopharmaceutical therapy (alpha-RPT) is a tre

226 he design and optimization of alpha-particle emitter radiopharmaceutical therapy (alphaRPT) is especi

227 However, almost all existing unidirectional emitters rely on the use of materials or structures that

228 ce imaging, we developed a force-activatable emitter reporting single-molecular tension events and th

229 u < 2 mus) are obtained for yellow and green emitters, respectively.

230 mpared to rare earth and silver-based NIR-II emitters, RNase-A@AuNCs had excellent biocompatibility,

231 e of infrared technologies including thermal emitters, sensors, active IR filters and detectors.

232 Usually, an emitter should be placed inside the cavity to increase t

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

234 al MS with larger emitters because nanoscale emitters significantly reduce the extent of salt adducti

235 footprint in China-the world's largest CO(2) emitter-simultaneously considering both international an

236 Integrated single photon emitters (SPEs) are central building blocks for such qua

237 At low temperatures, single-photon emitters (SPEs) are present across an OPEN-WSe(2) film,

238 ques, recording excitation spectra of single emitters still poses a significant challenge.

239 ng many of the problems inherent in internal emitter studies.

240 hotonic systems, which utilize active photon emitters such as light-emitting diodes, have the potenti

241 Quantum emitters such as the diamond nitrogen-vacancy (NV) cente

242 lasmonics and are generally maximal at short emitter-surface separations.

243 for mitigation are presented by point-source emitters-surface features or infrastructure components t

244 ell by actively tuning the gap between a hot-emitter (T(E) ~ 880 K) and the cold photodetector (T(D)

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

246 otovoltaic efficiency of 29.1 +/- 0.4% at an emitter temperature of 1,207 degrees C.

247 ive to increasing cell bandgap or decreasing emitter temperature.

248 how that judicious engineering of the single-emitters that comprise the metasurface, enables to obtai

249 A central challenge is identifying emitters that exhibit coherent optical and spin transiti

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

251 nary thermal radiation, generated by thermal emitters that have been modulated well beyond their ther

252 sign of lead halide perovskite-based quantum emitters that have fast emission, wide spectral tunabili

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

254 a poorly characterized population of methane emitters that often appear intermittently and stochastic

255 Here, we demonstrated ultrathin thermal emitters that violate this one-to-one relationship via t

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

257 to sensitize a blue multiple-resonance TADF emitter, the corresponding device simultaneously realize

258 When paired with 9,10-diphenylanthracene emitters, these particles readily upconvert 488-640 nm p

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

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

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

262 n even a single analyte molecule with 210 nm emitter tips.

263 By attaching a fused silica capillary emitter to a vibrating glass slide, improved signal qual

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

265 However, the deposition of high-energy alpha-emitters to tumor markers adjacent to a typical leaky tu

266 ss wearable sensor, consisting of ultrasound emitter, ultrasound receiver, data acquisition and wirel

267 facile approach toward highly emissive TADF emitters using a 1,3,4-oxadiazole motif.

268 The ability to tailor quantum emitters via site-selective defect engineering is essent

269 de-out" approach to deliver nanoscopic light emitters via the intrinsic circulatory system and switch

270 Continuous infusion of droplets to an nESI emitter was demonstrated for as long as 2.5 h, correspon

271 and a monolithically integrated electrospray emitter was developed.

272 The structure of fungal oxyluciferin (light emitter) was proposed in 2017, being different and more

273 Using an archetypal phosphorescent emitter, we achieve a two-fold increase in operational s

274 st to those in other two-dimensional optical emitters, we find that TDMs in CdSe quantum rings show a

275 tial location of tungsten diselenide quantum emitters, we uncover the possibility of realizing large-

276 Stable and fluctuating emitters were observed, as well as a surprising splittin

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

278 ons reflected and re-absorbed by the thermal emitter, where their energy can have another chance at c

279 sion surveillance targeting relatively large emitters, which can help achieve emission reductions for

280 iral sensors, and circularly polarized light emitters will require a greater control of the energetic

281 erface of the Taylor cone in an electrospray emitter with a large orifice, thus allowing continuous c

282 d thermal light sources and even an infrared emitter with a laser-like input-output characteristic.

283 rmally activated delayed fluorescence (TADF) emitter with a radiative rate constant k(r) of ca. 9 x 1

284 ent thermally activated delayed fluorescence emitters with concomitantly decreased singlet-triplet en

285 Highly fluorescent light emitters with medium-tunable clear colors were obtained

286 These complexes are yellow emitters with modest quantum yields.

287 ace the stronger cyano one to construct blue emitters with multiple donors and acceptors.

288 omparable to state of the art phosphorescent emitters with noble metals such as Ir and Pt.

289 e design and realization of tailored triplet emitters with nonconventional elements.

290 Use of these emitters with small tips is advantageous for clearly dis

291 con (QRB), consisting of solid-state quantum emitters with spin-dependent fluorescence, to provide su

292 but this aggregation can be eliminated using emitters with sufficiently small tips.

293 ailed information on the interactions of the emitters with their nanoscopic environment.

294 Electrospray ionization emitters with tip sizes between 210 nm and 9.2 mum were

295 dvance the rational design of TMC-based TADF emitters with tunable ligands and the subsequent fabrica

296 m a vast number of natural and anthropogenic emitters with unprecedented sensitivity, revealing sourc

297 nce, the design and fabrication of selective emitters, with emission strongly dominant in the transpa

298 sperma panamensis, but most species acted as emitters, with emissions declining exponentially with he

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

300 hat enables precise positioning of a thermal emitter within nanometer distances from a room-temperatu