ライフサイエンスコーパス: QD

1 nducting CdSe quantum dots on Si channel (Si-QD).

2 apy: ticagrelor 90 mg BID plus aspirin 81 mg QD).

3 of the electron wavefunction over the entire QD.

4 on of FRET as the dye diffuses away from the QD.

5 ats, and a predicted human dose of 120 mg of QD.

6 evel of target engagement at a dose of 45 mg qd.

7 velength, and structural fluctuations of the QD.

8 sum of the native recombination rates in the QD.

9 oquinone preserves the cubic phase of CsPbI3 QD.

10 eract with the core electronic states of the QD.

11 to QDs with different emission wavelengths (QD 520 nm, QD 565 nm and QD 610 nm) to serve as detectio

12 h different emission wavelengths (QD 520 nm, QD 565 nm and QD 610 nm) to serve as detection probes (Q

13 ission wavelengths (QD 520 nm, QD 565 nm and QD 610 nm) to serve as detection probes (QD-Ab).

14 mic diameter) and biocompatible quantum dot (QD) -Ab conjugates.

15 hronic calvarial bone window showed that our QD-Ab conjugates diffuse into the entire bone marrow and

16 Based on fluorescence of the QD-Ab probes, residues of the three antibiotics were det

17 PC-G residues, based on fluorescence of the QD-Ab probes.

18 and QD 610 nm) to serve as detection probes (QD-Ab).

19 rstand its origin, we suspended the graphene QD above the substrate.

20 bination of streptavidin-coated quantum dot (QD) acceptors and biotinylated, Tb(3+) sensitizing pepti

21 e an ultrathin freestanding ZnO quantum dot (QD) active layer with nanocellulose structuring, and its

22 icipated and suggest promising potential for QD administration.

23 nced by various factors such as cell damage, QD aggregation or the level of reactive oxygen species,

24 onfiguration that comprises a green-emitting QD, Alexa Fluor 555 (A555), and Alexa Fluor 647 (A647).

25 ld of photoinduced charge transfer between a QD and a molecular probe to even low-affinity binding ev

26 ssion channels to permit measurement of A555/QD and A647/QD PL ratios.

27 nd toxicity of intravesically instilled free QD and anti-CD47-QD in mice.

28 Ctrough levels were slightly lower with DRV QD and BID.

29 In turn, the sum of the QD and dye PL intensities, when adjusted for quantum yie

30 s in ultrafast electron transfer between the QD and FeTPP, enabled by formation of QD/FeTPP complexes

31 y of In over the entire height of an average QD and much narrower photoluminescence (PL) line.

32 ion pairing between the ligand shell of the QD and NR4(+) results from a combination of electrostati

33 he spectral coupling probability between the QD and the cavity mode.

34 xchange between a colloidal PbS quantum dot (QD) and a negatively charged small molecule (9,10-anthra

35 of this review is the colloidal quantum dot (QD) and specifically the interaction of the QD with prox

36 noparticles include a spherical quantum dot (QD) and three differing lateral areas of 4-monolayer-thi

37 acid (MPA)-capped CdSe quantum dot (MPA-CdSe QD) and visible light.

38 ate (MHA) ligand shell of a PbS quantum dot (QD) and water.

39 ploiting the spectral features of Tb(3+) and QD, and the high binding affinity of the streptavidin-bi

40 in doubling time on exposure to 25 mg/L CdTe QD ( approximately 4 nm) as compared to control.

41 physical properties of a doped quantum dot (QD) are strongly influenced by the dopant site inside th

42 Coherent QD arrays have a spatial distribution which is neither r

43 t of inter-diffusion of Ga and In within the QD as a function of height in the low-density region giv

44 ransfer and the use of the ligand shell of a QD as a semipermeable membrane that gates its redox acti

45 the QDs, and (iii) structural components of QD assemblies that dictate QD-QD or QD-molecule interact

46 r rates between quantum dots (QDs) in chiral QD assemblies.

47 des were assembled around a central CdSe/ZnS QD at different ratios, tuning the relative rates of FRE

48 HNC-SLs) self-assembled from quantum-dot-Au (QD-Au) satellite-type HNCs.

49 S QDs synthesis as well as for preparing the QD based MIP-coated composite by precipitation polymeriz

50 Here, we combine a multicolor quantum dot (QD)-based immunofluorescence assay and an array analysis

51 give a short outlook on future directions of QD-based bioimaging.

52 0 gene, promising a possibility to apply the QD-based biosensor for clinical investigations.

53 emonstrated by measuring the response of the QD-based FRET sensor microinjected into live HeLa cells

54 d their most important properties, different QD-based imaging applications will be discussed from the

55 rovide important and useful design rules for QD-based light harvesting applications using the exciton

56 Similarly, we prepared QD-based NPs densely decorated with an isatoic anhydride

57 achieved, which is among the most effective QD-based photocathode water-splitting systems.

58 ignal in QD-based sensors or photocurrent in QD-based photovoltaics.

59 QD-based quantification of copper on bacterial supernata

60 hat occurs in those QDs to amplify signal in QD-based sensors or photocurrent in QD-based photovoltai

61 illustrate selected examples of luminescent QD-based sensors taken from the recent literature.

62 , we show that the photoluminescence (PL) of QD bioconjugates can also be modulated by a combination

63 e dealing with the design and application of QD-bioconjugates for advanced in vitro and in vivo imagi

64 QDs and change the microenvironments of the QD-bound dyes such that the emissive properties of the d

65 e not only the excited state dynamics of the QD but also, in some cases, its ground state electronic

66 We find that the QD can rectify electrical charges generated from the pie

67 eft unprotonated, serves as a poison for the QD catalyst by adsorbing to its surface.

68 ematically investigated as a function of the QD-cavity detuning.

69 correlates with the strength of the acceptor QD circular dichroism (CD) spectrum.

70 Overall, this paper demonstrates that QD coat properties influence plant nanoparticle uptake a

71 We explored the impact of quantum dot (QD) coat characteristics on NP stability, uptake, and tr

72 +) or Eu(3+) doped luminescence glass or CdS-QD coated glass lenses provide additional visible light

73 doped borate glasses or CdS-quantum dot (CdS-QD) coated lenses efficiently convert UV light to 542 nm

74 Unlike previous studies, in which the QD concentrations used for NMR characterization were mor

75 opical (i.e. intravesical) administration of QD-conjugated anti-CD47.

76 mbination of the electronic structure of the QD core and the chemistry at its surface to use the ener

77 ing conditions (e.g., time, temperature, and QD core identity).

78 the yield of electron transfer (eT) from the QD core to AQ, increases as the steric bulk of NR4(+) in

79 romotes the incorporation of <1% Ag into the QD core where it causes p-type doping behavior.

80 e states or to the delocalized states of the QD core, (ii) energy or electron donors or acceptors for

81 stinguish QD surface atoms from those of the QD core, and environmental effects such as oxidation.

82 to selectively and discriminately probe the QD core, QD surface and capping ligands.

83 netic beads along with unreacted (uncleaved) QD-CPs by using a permanent magnet, ultrasensitive fluor

84 rands of DV RNA form heteroduplexes with the QD-CPs on the magnetic beads.

85 dized quantum dot-capped DNA capture probes (QD-CPs), an ultrasensitive assay for the detection and s

86 is accomplished by a judicious design of the QD-CPs.

87 r around of hybridization with the remaining QD-CPs.

88 gnetic beads in the removal of the unreacted QD-CPs.

89 pared across the 3 drugs (rivaroxaban: 20 mg QD, dabigatran: 150 mg BID, or warfarin) using 3-way pro

90 by more spatially regular nucleation as the QD density increases.

91 ase retention profiles, characterized by low QD deposition near the column inlet and increasing solid

92 We also present recent QD devices and discuss future prospects for QD materials

93 perties of QD surfaces and the interfaces in QD devices are of particular importance, and these enabl

94 ds has led to record-breaking performance in QD devices, such as electronic transistors and circuitry

95 hnology for the creation of optimized single QD devices.

96 The resulting QD dimers range in length from 6 to 16 nm and are produc

97 y, 2) use of high-boiling-point solvents for QD dispersion, and 3) limitations associated with one-st

98 e exposed to PAA-EG QDs, possibly due to PEI QD dissolution and direct metal uptake.

99 from an emissive semiconductor quantum dot (QD) donor to a dithiol-linked organic dye acceptor.

100 ublet in motif 1 of family 4 UDGa and in the QD doublet in motif 1 of family 1 UNG.

101 let in family 4 Thermus thermophilus UDGa to QD doublet increases the catalytic efficiency by over on

102 DT/oleate ligand shell of a PbS quantum dot (QD) dramatically reduces the permeability of the ligand

103 plasma HIV-1 RNA suppression on once-daily (QD) DRV-containing ART at screening.

104 excitonic hole in approximately 5 ps to form QD(*-); electron transfer to nitrobenzene or the interme

105 photon source based on an InAs quantum dot (QD) embedded in a photonic crystal cavity coupled with a

106 This results in enhanced QD emission and dye quenching.

107 imized by adjusting spectral overlap between QD emission and the J-aggregate absorption, which are co

108 Analysis of the QD emission enhancement as a function of distance reveal

109 ent mechanism for the temporal modulation of QD emission intensity at constant optical pumping rate.

110 nstrated electrical control of the colloidal QD emission provides a new approach for modulating inten

111 For each QD-ET mechanism, a working explanation of the appropriat

112 stry at its surface to use the energy of the QD excited state to drive chemical reactions.

113 Monitoring of the QD exciton by transient absorption reveals that, for eac

114 e findings imply that the CD strength of the QD exciton transition(s) may be used as a predictor for

115 s of radiative and nonradiative decay of the QD exciton.

116 en the QD and FeTPP, enabled by formation of QD/FeTPP complexes.

117 Herein, we suggest a new protocol for QD film deposition using electrical double-layered PbS Q

118 ilver resonators, excitation wavelength, and QD film thickness.

119 reparing a dense, smooth, 5.3-mum-thick PbSe QD film via doctor-blading.

120 e and visible quantification of glucose with QD films can be applied to low-cost, point-of-care biome

121 The treatment protocol results in PbS QD films exhibiting a deeper work function and band posi

122 ission behaviors from single- and multilayer QD films on silver resonators are described quantitative

123 eposition process yields high-quality n-type QD films quickly (within 1 min) while minimizing the amo

124 We describe the formation of alpha-CsPbI3 QD films that are phase-stable for months in ambient air

125 d was used to define fluorescent patterns on QD films, allowing for further applications in biosensin

126 d allows for facile hole extraction from the QD films, resulting in a power conversion efficiency of

127 and allow for efficient charge transport in QD films.

128 indicating improved carrier transport in the QD films.

129 Controlling the thickness of quantum dot (QD) films is difficult using existing film formation tec

130 tionic GNPs efficiently quenched the anionic QD fluorescence by forming nanoparticle hybrid.

131 n multifunctional applications, in which the QD fluorescence is combined with drug or gene delivery t

132 The brightness of the QD fluorescence is greatly enhanced on resonance with th

133 The mechanism of Cu(2+)-mediated QD fluorescence quenching was associated with nanopartic

134 QD-GNP pair was unlocked by NADH leading to QD fluorescence turn-on.

135 exposed to QDs had reduced performance, and QD fluorescence was detected in both T. ni bodies and fr

136 2 molecular and 6 semiconductor quantum dot (QD) fluorophores.

137 andomized to clopidogrel (600 mg, then 75 mg QD for 7-9 days) or ticagrelor (180 mg, then 90 mg BID f

138 ble theoretical picture for the mechanism of QD formation and growth.

139 owth intermediates during III-V quantum dot (QD) formation.

140 This work establishes QD FRET as a rapid, sensitive technique for probing stru

141 Typically, the QD-FRET constructs have made use of labeled targets or h

142 n important framework for the integration of QD-FRET methods with digital imaging for a ratiometric t

143 and was 10 nM (2 pmol), similar to analogous QD-FRET using labeled oligonucleotide target.

144 s, viruses, microorganisms and their toxins, QD-FRET-based immunoassays, and pH sensors.

145 Due to these benefits, QD-FRET-based nanosensors gained a wide spread popularit

146 ocking and unlocking the interaction between QD-GNP pair leading to differential fluorescent properti

147 Quenching interaction between QD-GNP pair was unlocked by NADH leading to QD fluoresce

148 leading to monomer formation and subsequent QD growth.

149 hene FETs, we find that a suspended graphene QD has an almost-identical noise level as an unsuspended

150 o control the optical properties of graphene/QD hybrid structures.

151 hieved by employing Stark effect into the Si-QD hybrid system.

152 mistry and the band edge positions of ligand/QD hybrid systems.

153 Our QD immunoconstructs were used for in vivo single-cell la

154 travesically instilled free QD and anti-CD47-QD in mice.

155 LBN 0.024% QD in the evening was noninferior to timolol 0.5% BID ov

156 randomized 2:1 to LBN instilled once daily (QD) in the evening and vehicle in the morning or timolol

157 The SMMs and QD-incorporated spore microspheres (QDSMs) were characte

158 rovskite phase when the concentration of the QD increases.

159 min) while minimizing the amount of the PbS QD ink used to less than 5 mg for one device (300-nm-thi

160 ent and the subsequent deposition of the PbS QD ink without requiring a post-deposition annealing tre

161 iques, which employ pre-ligand-exchanged PbS QD inks, because of several issues: 1) poor colloidal st

162 position using electrical double-layered PbS QD inks, prepared by solution-phase ligand exchange usin

163 that are still not fully understood such as QD interactions with gold and other metal nanoparticles

164 ly demonstrate that charge transfer rates at QD interfaces can be tuned by several orders of magnitud

165 how the 1/f noise for a microscopic graphene QD is substantially larger than that for a macroscopic g

166 10 mT) and that the electron donated to the QD is trapped in a surface state rather than delocalized

167 The QD/J-aggregate complexes form through electrostatic self

168 We show that QD labeling does not affect major biophysical properties

169 -based quantum dots (QDs), respectively, the QD labels are dissolved releasing Pb(II) and Cd(II) in t

170 oxide capped cadmium selenide quantum dots (QD) Langmuir monolayer.

171 ace state rather than delocalized within the QD lattice.

172 ently thick CdSe shells to impart new single-QD-level photostability, as evidenced by suppression of

173 ed antibodies were used for the fluorescence QD-LFIA and conventional reflection-mode Au NP-LFIA, res

174 OLED QD-LFIA exhibited superior performance in all signal asp

175 e the test line of a quantum dot-based LFIA (QD-LFIA).

176 limit of detection (LOD) of OLED integrated QD-LFIAs were compared to Au NP LFIAs.

177 ind that in addition to ligand dipole, inter-QD ligand shell inter-digitization contributes to the ba

178 inued development of such systems containing QD light absorbers and molecular catalysts for H2 format

179 form the nanocomposites of CdTe quantum dot (QD)-loaded SMMs by utilizing the endogenous functional g

180 cle tracking of Gal3- or STxB-functionalized QD-loaded DNA icosahedra allows us to monitor compartmen

181 An initial discussion of QD materials along with key concepts surrounding their p

182 QD devices and discuss future prospects for QD materials and device design.

183 Our results establish the utility of the QD-micelle approach for in vivo biological sensing appli

184 the photoluminescence quantum yield of these QD-molecular conjugates at varying ferrocene coverage, a

185 observed relationship can be used to design QD-molecular systems that maximize interfacial charge tr

186 Hence, QD-molecule conjugates are appealing platforms for devel

187 nents of QD assemblies that dictate QD-QD or QD-molecule interactions.

188 Nuclear magnetic resonance analysis of the QD-molecule systems shows that the photoproduct aniline,

189 re produced by oriented attachment of single QD monomers with diameters of 3.1-7.8 nm.

190 synthetic methods to directly react to form QD monomers, but rather they can generate in situ the sa

191 ticular, spin relaxation rate peaks when the QD motion is in the transonic regime, which we term a sp

192 verlayers as well as the bottom monolayer of QD multilayers exhibit significant PL enhancement mainly

193 verage number of hole acceptor molecules per QD, N, allowing us to measure PLQY as a function of N, a

194 The ultrathin ZnO QD-nanocellulose composite is obtained by hydrogel trans

195 irmed the initial formation of Janus-like Ag@QD nanoparticles in this process.

196 he QD (where it exchanges electrons with the QD) of 154 J/mol upon introduction of each additional ch

197 orescent nanoparticles such as quantum dots (QD) offer superior optical characteristics compared to o

198 ients were randomized to maintain DRV 800 mg QD or switch to twice-daily (BID) DRV 600 mg; all receiv

199 c absorbance increase to ground-state ligand/QD orbital mixing, as inferred by density functional the

200 ge, there was no significant accumulation of QD outside of the bladder, although in some mice we dete

201 g/mL) using both QD-Ox-Cyt-c (R(2)=0.93) and QD-Ox-Co-Q (R(2)=0.96).

202 Two probes were designed, QD-Ox-Cyt-c and QD-Ox-Co-Q, which were found to quench the fluorescence

203 1-100,000ng/mL (LOD of 0.01ng/mL) using both QD-Ox-Cyt-c (R(2)=0.93) and QD-Ox-Co-Q (R(2)=0.96).

204 Two probes were designed, QD-Ox-Cyt-c and QD-Ox-Co-Q, which were found to quench t

205 Excitation of adjacent QD pairs reveals orbital alignment, evidence for electro

206 ce resonance energy transfer interactions in QD-peptide-dye assemblies.

207 e of tunable photocurrent on/off ratio in Si-QD photodetector (ranging from 2.7 to 562) by applying s

208 were used to fabricate colloidal perovskite QD photovoltaic cells with an open-circuit voltage of 1.

209 The irradiance changes in QD PL indicate quantitatively the level of glucose prese

210 Notably, the dye/QD PL intensity ratio reflected changes in the relative

211 ls to permit measurement of A555/QD and A647/QD PL ratios.

212 ium(II) phenanthroline complex that quenched QD PL through electron transfer.

213 with either a fluorescent dye that quenched QD PL through FRET or a ruthenium(II) phenanthroline com

214 aldehyde and azide) are combined on the same QD platform, the nanocrystal can be specifically reacted

215 This yields redox-active QD platforms that can be used to track pH changes and de

216 This design yields QD platforms with distinct chemoselectivities that are g

217 d from the thiolate anion adsorbed on a CdSe QD plays a key role by abstracting the hydrogen atom fro

218 The micelle-encapsulated QD-porphyrin assemblies have been employed for in vivo m

219 Control of quantum dot (QD) precursor chemistry has been expected to help improv

220 After a short summary of QD preparation and their most important properties, diff

221 The QD probes specifically bind DC-SIGN, but not its closely

222 ulting CdSe/ZnSe gQDs exhibit unusual single-QD properties, principally emitting from dim gray states

223 ral components of QD assemblies that dictate QD-QD or QD-molecule interactions.

224 relation between AUC0-24 hr and C24 for both QD (r=0.96) and BID (r=0.94) formulations.

225 action variables including the new-ligand-to-QD ratio, the size of the particles, and the original li

226 on transition by an average of 1 carrier per QD requires that approximately 10% of the Pb be replaced

227 Conversion to Tac QD resulted in a significant improvement in intra-patien

228 r stage in the growth, independently of each QD's surroundings.

229 reports the fabrication of CdSe quantum dot (QD)-sensitized photocathodes on NiO-coated indium tin ox

230 leading to the construction of various CdSe QD-sensitized photocathodes.

231 To that end, we create QD single-photon sources, based on a circular Bragg grat

232 Further, the modified QD@SiO2 were efficiently conjugated with antibodies and

233 stability of the obtained silica coated QDs (QD@SiO2), modified with amino, carboxyl and epoxy groups

234 onversion is an important factor controlling QD size and size distribution.

235 veral orders of magnitude by engineering the QD size distribution.

236 The thermodynamics of QD/SMM interaction and antigen/QDSM interaction was also

237 We demonstrate QD solar cells based on PbI2 with power conversion effic

238 of preparing PbE (E = S or Se) quantum dot (QD) solar cells using metal halide (PbI2, PbCl2, CdI2, o

239 heory that depict band-like transport in the QD solid state.

240 Increased coupling in QD solids has led to record-breaking performance in QD d

241 The resulting QD solids have a significant reduction in the carbon con

242 band gap reduction commonly observed for PbS QD solids treated with thiol-terminating ligands can be

243 s and doping that have enabled high-mobility QD solids, as well as the experiments and theory that de

244 ed and hybridized states of strongly coupled QD solids, in analogy with the construction of solids fr

245 e oleate surface ligands and form conductive QD solids.

246 bility, colloidal semiconductor quantum dot (QD) solids has triggered fundamental studies that map th

247 e to even low-affinity binding events at the QD/solvent interface.

248 an electrostatic double-layer model for the QD/solvent interface.

249 ow that LED emission from randomly polarized QD sources can be polarized and directed at will.

250 the QDs, resulting in the modulation of the QD spontaneous emission rate, far-field emission intensi

251 spin-coating method was used to deposit CdSe QD stock solution onto the surface of NiO/ITO electrodes

252 ot (QD), we apply the thick-shell or "giant" QD structural motif to this notoriously environmentally

253 In addition, the QD structure is further optimized to fully exploit the d

254 we detected extravesical biodistribution of QD suggesting a route for systemic exposure under some c

255 polymer chain for tight coordination to the QD surface and a controllable number of zwitterion moiet

256 tively and discriminately probe the QD core, QD surface and capping ligands.

257 e majority of incorporated Ag remains at the QD surface and does not interact with the core electroni

258 trolled by density of charged ligands on the QD surface and the pH.

259 in this way are shown to clearly distinguish QD surface atoms from those of the QD core, and environm

260 Characterization of the QD surface by nuclear magnetic resonance (NMR) spectrosc

261 ns, we establish clear relationships between QD surface chemistry and the band edge positions of liga

262 bulky electrically insulating ligands at the QD surface coming from the synthetic procedure is mandat

263 d shell and its subsequent adsorption to the QD surface is well-described with an electrostatic doubl

264 Tuning the QD surface mannose valency reveals that DC-SIGN binds mo

265 -harvesting nanomaterials demonstrating that QD surface modification with suitable short conjugated o

266 Replacing only 21% of the oleates on the QD surface with PFDT reduces the yield of photo-oxidatio

267 permeate the ligand shell and adsorb to the QD surface.

268 oriented attachment directed by quantum dot (QD) surface chemistry.

269 ecomposed, indicating labile exchange at the QD surfaces and a photocatalytic cycle.

270 P and provide the bonding motifs between the QD surfaces and the capping ligands.

271 The chemical and physical properties of QD surfaces and the interfaces in QD devices are of part

272 coverage of these capping agents on the CdSe QD surfaces reveal that they affect system activity and

273 ntraparticle coalescence of Au satellites at QD surfaces transforms individual HNCs into heterodimers

274 These ligands were introduced onto the QD surfaces using a combination of photochemical ligatio

275 fied the coupling of dye-labeled peptides to QD surfaces using fluorescence resonance energy transfer

276 nts, which were previously inconceivable for QD surfaces, are demonstrated to be readily performed wi

277 ic double layer on electronic passivation of QD surfaces, which we find can be explained using the ha

278 heir higher coordination onto the metal-rich QD surfaces.

279 ategies directly on luminescent quantum dot (QD) surfaces that use click chemistry and hydrazone liga

280 anation for the shortcoming of current III-V QD syntheses and points to the need for a new generaliza

281 that were used in some of the original II-VI QD syntheses decades ago, i.e., hydrogen chalcogenide ga

282 vestigate the reaction mechanism behind CdSe QD synthesis, the most widely studied QD system.

283 Here we prepared a self-illuminating QD system by doping positron-emitting radionuclide (64)C

284 r per absorbed unit of photon energy) of the QD system is a factor of 18 greater than that of an anal

285 d CdSe QD synthesis, the most widely studied QD system.

286 Indeed, experimental results for other QD systems are consistent with the theoretical predictio

287 These results show the potential of QD systems to drive desirable oxidative chemistry withou

288 s: tacrolimus extended-release (Astagraf XL) qd, tacrolimus (Prograf) bid, or cyclosporine (CsA) bid.

289 onance energy transfer from the quantum dot (QD) to the palladium porphyrin provides a means for sign

290 We also briefly discuss QD toxicity issues and give a short outlook on future di

291 oxygen is used, the structure of the CsPbI3 QD transforms from cubic to orthorhombic, while usage of

292 ever, 8-fold more cadmium accumulated in PEI QD-treated leaves than in those exposed to PAA-EG QDs, p

293 with injecting a free charge carrier into a QD under equilibrium conditions, including a bleach of t

294 with 93% tumor growth inhibition at 50 mg/kg QD upon oral dosing.

295 In vivo biodistribution of anti-CD47-QD was assessed with inductively coupled plasma mass spe

296 Toward a truly photostable PbSe quantum dot (QD), we apply the thick-shell or "giant" QD structural m

297 Electronic structure modeling of a small PbS QD, when scaled for size, reveals Stark tuning and varia

298 AQ from bulk solution to the surface of the QD (where it exchanges electrons with the QD) of 154 J/m

299 (QD) and specifically the interaction of the QD with proximate molecules.

300 spin qubit confined in a moving quantum dot (QD), with our attention on both spin relaxation, and the

301 he charge density in the ligand shell of the QD, within an aqueous dispersion.