ライフサイエンスコーパス: nm

1 As a model system, 10.9 +/- 1.0 nm Au NPs were analyzed to demonstrate the effects of in

2 and water phases are separated by a 2.3-3.0 nm surfactant interface.

3 - 18.7 nm and mesoporous SNPs 466.0 +/- 86.0 nm) upon single dose intravenous administration to femal

4 concentration of source-resolved 50 - 1,000 nm particles and particle mixing state in Pittsburgh, Pe

5 le (350-700 nm) and near-infrared (700-1,000 nm) wavelengths.

6 d approached maximum values of 0.09 and 0.06 nm/s in the binary systems with montmorillonite and kaol

7 at the fundamental frequency (lambda = 1,064 nm) to ablate Ag and graphite composite target submerged

8 tal observations of ion transport across 1.1 nm inner diameter RNT porins (RNTPs) of various lengths

9 ctors operating with fluences near 253 +/- 1 nm of 13.9-49.6 mJ cm(-2) efficiently inactivate coronav

10 ng AGR based on ASV is 17.8 +/- 0.6% for 4.1 nm diameter Au NPs, 87.2 +/- 2.9% for 1.6 nm Au NPs, and

11 , PNS with a hydrodynamic radius of R(h) ~ 1 nm is formed and (ii) following this rapid initial forma

12 , and it was possible to detect movements <1 nm of the domains with respect to each other.

13 Biological proton channels are sub-1-nm protein pores with ultrahigh proton (H(+)) selectivit

14 SAG: sulfonic acid groups), which have sub-1-nm windows and a high density of sulfonic acid groups mi

15 ansmission electron microscopy revealed 2-10 nm crystallites of fcc-UO(2) or alpha-UO(3) depending on

16 The ability to measure distances of 2-10 nm is particularly important: deformations arising from

17 igh resolution beneath an approximately 5-10 nm thick layer of the fluid components of the interfibri

18 croscopy in the TIR geometry to achieve a 10 nm spatial resolution.

19 ly cleaved CrCl(3) flakes with thickness >10 nm is performed.

20 , 30 nm (or larger) pixel size/linewidth, 10 nm position accuracy and 50 nm overlay precision.

21 The sensitizing effect of 10 nm PGE(2) was attenuated in weakly IB4+ and IB4- neurons

22 ers (BCPs) enables nanofabrication at sub-10 nm dimensions, beyond the resolution of conventional lit

23 rovided a path to emulate synapses at the 10 nm scale, a scalable neuron analogue is yet to be found.

24 rticle size cutoff was reduced from 35 to 10 nm post-treatment with 0.8% NaOH for 20 min.

25 interactions in the less than or equal to 10 nm range.

26 ses in PNC within the size range of 10 - 100 nm, PLC, and PSC were associated with an increase of MI

27 ined shapes and sizes in the range of 10-100 nm remains challenging.

28 ELVs are 100 nm diameter membrane vesicles shed into the urine by the

29 e importance of achieving nanoscale (ca. 100 nm) dimensions, as opposed to microscale examples that a

30 m exposure to ultrafine particles (UFP; <100 nm in diameter), which are present at high concentration

31 particles (UFP; particles with diameter <100 nm) causing chronic health effects independent of fine p

32 QAC adjuvant system forms nanocarriers (<100 nm) that efficiently encapsulate nucleic acid cargo, exh

33 ispersed pyrite FeS(2) nanoparticles of ~100 nm diameter linked to porous carbon.

34 ze distributions with peak diameters of ~100 nm.

35 elies on unscattered light to detect sub-100 nm dielectric nanoparticles.

36 tune DMI in a range that stabilizes sub-100 nm skyrmions at room temperature in zero field.

37 y of these biological-nanoparticles (sub-100 nm) necessitate rigorous biophysical characterization of

38 ase in viscosity for particles less than 100 nm in diameter.

39 r (T(D) ~ 300 K) from ~ 500 nm down to ~ 100 nm.

40 5 ns for a 20 um diameter capacitor in a 100-nm-thick film).

41 ma membrane "nanopore-like" structures (~100-nm diameter) form rapidly due to lipid peroxidation, all

42 In particular, a single skyrmion with 100-nm size can be created at the desired position using a f

43 infectious extracellular vesicles, 100~1000 nm in diameter, secreted from host cells.

44 the MOF UiO-66(Hf) over an area of ca. 1000 nm and with a spatial resolution ca. 5 nm to reveal doma

45 CPP-based fluorophore showing a dramatic 105 nm red-shift in emission and striking 237 nm effective S

46 nced activities against BRD4 BD1 (IC(50) =11 nm) and HDAC1 (IC(50) =21 nm).

47 sition (~985 nm) fluoresce brightly at ~1160 nm.

48 300 nm) consisting of nanowires (diameter 12 nm), the SWING filters exhibit high efficiency (>99.995%

49 ped GaAsSb nanowires with diameters ~100-120 nm were grown on a p-type Si(111) substrate by molecular

50 tic coercive field of 30 mT at 5 K for a 125-nm-thick film.

51 <c> loops, routinely seen no smaller than 13 nm in diameter, are the source of the problem.

52 zed as a series of loops around a thin (<130 nm) MukBEF axial core, whose length is ~1,100 times shor

53 The resulting conical crater (0.6 mum x 130 nm ) morphology in a Au-coated glass target and carbon-c

54 ssing neurons for 920 nm two-photon and 1320 nm three-photon excitation.

55 cellulose matrix with an average size of 140 nm and with antimicrobial activity against both sensitiv

56 absorption feature in the range of 700-1400 nm.

57 spheric PM samples in the size range from 15 nm to 10 mum collected in an urban environment in Austri

58 les that cross the NPC, even very large (>15 nm) cargoes such as pathogens, mRNAs and pre-ribosomes c

59 Small extracellular vesicles (sEVs), 50-150 nm in diameter, have been proposed to mediate cell-cell

60 Exosomes are naturally derived 50-150 nm nanovesicles that play important roles in cell-to-cel

61 The smaller particles (50 and 150 nm) show a lower glass transition (T(g)) and thermal dec

62 piezoluminescence of wavelength of 800-1500 nm at microstrain levels, which is enhanced by the ferro

63 te electrolyte, thicker walled CNTs (100-160 nm diameter) are synthesized during a 4 h CO(2) electrol

64 f the optical band gap of CdSe QDs (R = 1.17 nm) of up to 111 meV while the colloidal stability of th

65 more than 30 cm with diameters as low as 170 nm.

66 cond near-infrared window (NIR-II, 1000-1700 nm) fluorescence imaging (FI) and photoacoustic imaging

67 atterning with feature sizes as small as 180 nm and 1 mum line spacing was achieved, resulting in the

68 etween a short UV absorption edge, below 190 nm, and a large SHG response, 2.8xKDP.

69 d to tetravalent UO(2) as nanocrystals (~1-2 nm) with random orientations inside nanowires.

70 ds is attributed to the close proximity (1.2 nm) between photoredox and Lewis acid catalysts in Hf(12

71 than the unit cell crystal size of MHs (1.2 nm), as exemplified in the experimental case study perfo

72 capped MoS(2)@TiO(2) as 12.6, 11.7 and 10.2 nm, respectively.

73 [Formula: see text] by a factor of 2 to 19.2 nm, the measured [Formula: see text] and temperature dis

74 oams consisting of ordered micropores (2-2.2 nm) and disordered meso and macropores (50 nm to 200 mum

75 LyP-1-QU-NPs had a desirable diameter (203.2 nm) and a negatively charged surface (-12.7 mV).

76 stable holes with an estimated diameter of 2 nm, as long as the glycine zipper motif remains intact.

77 ework membranes with pore sizes lower than 2 nm based on their chemistry: inorganic microporous frame

78 onsistent phototherapy with 33-103 uW/cm(2) *nm for 9.2 +/- 1.1 hours/day kept B(T) and B(T) /A withi

79 K-1 (IC(50) = 24 nm) and IRAK-4 (IC(50) = 20 nm), with only minimal TAK1-inhibiting activity (IC(50)

80 orescent polystyrene nanospheres (PS-NPs; 20 nm), and water leachate of weathered single-use plastics

81 nal grids, with diameters on the order of 20 nm and molecular weights greater than 65 kDa, through a

82 stable aqueous colloidal solutions of sub-20 nm crystalline imine-based COF particles at room tempera

83 light scattering identified nonfibrillar ~20-nm oligomers, while at high concentrations elongated fib

84 We report the results of 20-nm gold and magnetic iron oxide nanoparticles-assisted l

85 region spectral range (wavelength, 700-1,200 nm), making them suitable as tracers for photoacoustic i

86 Large gold nanoparticles (~10-200 nm), such as those required for long blood circulation t

87 RNTPs) of various lengths in the range 5-200 nm.

88 into arbitrarily defined patterns with a 200 nm (or smaller) pitch (>125,000 DPI), 30 nm (or larger)

89 articles with diameters of approximately 200 nm, and the residual Fe concentration in the acid was 0.

90 ined the KTP-rich droplet size at around 200 nm, which was smaller than in HPMC solutions without sur

91 it, switches on conjugation, leads to a >200 nm red-shift in the absorbance spectrum and injects a ch

92 Liposomes (~200 nm diameter) loaded with Fe(CN)(6)(4-) are driven out of

93 cordance with the morphology and size (< 200 nm).

94 surement of device-relevant thin films (<200 nm thickness), is exploited to deduce the precise compos

95 erage particle diameter on a nanoscale (<200 nm), high homogeneity and stability, high thermal stabil

96 study signal exchange in and out of the 200 nm cytoplasmic pole-organizing protein popZ (PopZ) micro

97 e yielded uniform fiber morphology with ~200 nm and ~900 nm average fiber diameter, respectively.

98 D4 BD1 (IC(50) =11 nm) and HDAC1 (IC(50) =21 nm).

99 l conductivity of ~15 100 S cm(-1) for a 214 nm thick film, which are both the highest values compare

100 showed average particle sizes of 107 and 222 nm, encapsulation efficiency (EE) and loading efficiency

101 Instead of shrinking from 32 nm to 23 nm (to match the mass loss to ions), TEM scans of partic

102 05 nm red-shift in emission and striking 237 nm effective Stokes shift while retaining a large quantu

103 selectivity toward both IRAK-1 (IC(50) = 24 nm) and IRAK-4 (IC(50) = 20 nm), with only minimal TAK1-

104 , we document the phase transformation of 25 nm thick nanocrystalline (NC) free-standing gold thin-fi

105 spectrum line width is broadened to over 25 nm by the coexistence of multiple reduced-dimensional pe

106 Free and bound lipids in the 25 nm thick intercellular spaces were directly detected for

107 A-origami barrel of ~90 nm diameter and ~250 nm height, that provides a rhombic-lattice canvas of a t

108 To compensate, large film thicknesses (250 nm or greater) have been employed at the expense of devi

109 e ionic liquid films ranged from ~50 to ~250 nm.

110 n used to carve (micromachining) out 100-250-nm-thin regions (called lamella) in the intact frozen ce

111 de spectral absorption in the range 200-2500 nm.

112 iconductors in this spectral range (800-2500 nm) remains largely unexplored.

113 (2)Cl, while UV photolysis of NH(2)Cl at 255 nm generated higher concentrations of HO(*), ClO(*), and

114 and individual wavelength (240, 255, and 275 nm) detection modes.

115 ) ~ 0.12, a full width at half maximum of 29 nm, and a T80 (time to 80% of the initial luminance) of

116 ~52% at room temperature for emission at 295 nm.

117 nsverse electric (TE) polarized light at 295 nm.

118 ed by tunable (~4.3-4.9 nm), uniform (+/-0.3 nm) cage-like scaffolds.

119 (K(D) values of 4.2 +/- 0.3 and 3.0 +/- 0.3 nm).

120 ing in a mean particle size of 125.6 +/- 2.3 nm and drug loading of 10 +/- 1.0% (w/w) while the same

121 efficient CuPd nanoparticle (NP) catalyst (3 nm CuPd NPs deposited on carbon support) is designed for

122 MD simulations on small ESI droplets (3 nm radius) showed CRM behavior regardless of the protein

123 asmall ordered Pt(3) M intermetallic NPs (~3 nm) due to confinement effect of 3D porous structure.

124 t for samples with initial Ni thickness of 3 nm.

125 200 nm (or smaller) pitch (>125,000 DPI), 30 nm (or larger) pixel size/linewidth, 10 nm position accu

126 s 5%), a good size tunability (from 7 to ~30 nm), an indirect bandgap, photoconductivity (responsivit

127 ed in the capture of many small vesicles (30 nm diameter) at the mitochondrial surface.

128 straight and "intermediate-curved" (100-300 nm diameter) in pH 7.5 solution and formed some bundles

129 Steiner-tree-structured pores (size 200-300 nm) consisting of nanowires (diameter 12 nm), the SWING

130 Atomic force microscopy revealed 40-300 nm diameter OMVs from control and stressed biofilm cells

131 V photolysis of NHCl(2) at 265, 285, and 300 nm generated higher concentrations of radicals (e.g., HO

132 l mass size distribution with a peak at ~300 nm.

133 can be operated in both scanning (230 to 300 nm) and individual wavelength (240, 255, and 275 nm) det

134 al resolution, resolving eight colors in 300-nm width, about 37.5-nm per color.

135 ry selectivity, bnn-1-Ca (pore diameter 0.31 nm) offers ideal selectivity for H(2) /CO(2) and H(2) /N

136 akes selective excitation possible using 310 nm excitation and 380 nm emission, separating the signal

137 g solar simulated UVR or narrowband UVB (311 nm).

138 ted with a characteristic size of 129 +/- 32 nm.

139 Instead of shrinking from 32 nm to 23 nm (to match the mass loss to ions), TEM scans

140 water addition fluorescence (excitation 325 nm / emission 410 nm) as indicator of tyrosine oxidation

141 surface coverage at the same wavelength (330 nm).

142 had z-average droplet diameters of 92 to 337 nm without any energy input.

143 Whereas bnn-1-Ca-H(2) O (pore diameter 0.34 nm) exhibits ultra-high CO(2) /N(2) , CO(2) /CH(4) , and

144 to -40.8), and particle size (74.23 to 55.35 nm).

145 -1)bar(-1) and a particle size cut off of 35 nm.

146 ing up the limit of spatial resolution of 35 nm.

147 eparated by a distance ranging from 10 to 35 nm.

148 del indicated a larger layer thickness (~350 nm) but tended to result in larger uncertainties in the

149 entials under both dark and illuminated (365 nm, 125 mW cm(-2)) conditions to elucidate the nature of

150 robe that undergoes photoactivation upon 365 nm UV treatment and enables intracellular deubiquitinati

151 duced electron transfer, initiated using 365 nm light-emitting diodes, affords radicals at room tempe

152 Irradiation with 365 nm light (5 mW cm(-2) ) in the presence of a soluble thi

153 the PE(4) segment to NDI when excited at 370 nm, but it does not produce a charge-separated state whe

154 imaged the binding lifetime and location (38-nm resolution) of single, fluorescently labeled boron-di

155 735 nm LEDs, was supplemented with UV-A 380 nm, green 510 nm, yellow 595 nm or orange 622 nm LED wav

156 ion possible using 310 nm excitation and 380 nm emission, separating the signals of interest from oth

157 se to the theoretically predicted value (0.4 nm).

158 allow exfoliation of Bi(4)O(4)SeCl(2) to 1.4 nm height.

159 bre, we have achieved a sensitivity of - 1.4 nm/ degrees as a vector bending sensor and - 17.5 nm/m(-

160 er wall, the POF material (aperture size 2.4 nm) concentrates over 90% of aromatic species into the p

161 dered BCP line arrays with half-pitch of 6.4 nm are demonstrated on stripes >80 nm wide.

162 egularly distributed along the filament at 4-nm intervals and we can determine the domains that assoc

163 to produce monolayer PbI(2) nanodisks (30-40 nm in diameter and > 99% monolayer purity) and deposit t

164 liculi are linked to smaller channels of ~40 nm diameter, occupying spaces between fibrils.

165 (meso-MPN particles) with a large-pore (~40 nm) single cubic network (Pm3m).

166 ved from flow-cells showed an increase to 40 nm.

167 ging of trace metals, both performed with 40 nm spatial resolution, on primary rat hippocampal neuron

168 sceptibility to the ultraviolet (UV: 290-400 nm) radiation in sunlight, which limits their persistenc

169 velengths of light (UVB and UVA from 300-400 nm) but instead is maximally induced by higher wavelengt

170 nia shows the peaks present at and above 400 nm are ascribed to the defects in the crystalline struct

171 uced system operates with visible light (400 nm) and achieves borylation of a wide range of chloroare

172 ved photoconductance using UV light with 400 nm wavelength, arising from excitation across the nanosu

173 - 15% of average BrC light absorption at 405 nm (BrC Abs(405)) measured in the first few hours of plu

174 ominantly sensitive to wavelengths below 405 nm (ultraviolet) and above 565 nm (orange & red) and tha

175 91 cm(2) s(-1) and a diffusion length of 405 nm along the in-plane direction.

176 rradiated in the wavelength range of 360-410 nm, whereas the E-isomer cyclization (Phi(c) = 0.006-0.0

177 uorescence (excitation 325 nm / emission 410 nm) as indicator of tyrosine oxidation and carbonyl cont

178 , whereas the monomeric form absorbed at 420 nm (catalytically incompetent form).

179 a charge-separated state when excited at 420 nm (T(4)).

180 idth of these nanoribbons between 50 and 430 nm by varying the total phosphine dosage during the surf

181 geted blocking of lower wavebands (up to 430 nm) using light restricting materials reduces pest popul

182 the blue fluorescence intensity of GO at 440 nm increases with the progression of oxidation by MPO/H(

183 form of the dimeric protein absorbed at 448 nm (catalytically competent form), whereas the monomeric

184 rge bending modulus is in part due to the 45 nm separation between the two membranes, which supports

185 on in five sizes (50, 150, 300, 350, and 450 nm).

186 dyes exhibit absorption maxima close to 450 nm and emission above 600 nm.

187 The basal lighting, consisting of blue 455 nm, red 627 and 660 nm and far red 735 nm LEDs, was supp

188 icial virus-like capsids of approximately 47 nm in size.

189 n diffusion lengths in the range of 20 to 47 nm.

190 cond and picosecond Raman pump pulses at 488 nm.

191 s of spectra at wavelength ranges of 484-490 nm and 508-518 nm, are the most effective features for p

192 or laser diode with high output power at 493 nm.

193 rmation of THF-rich nanoclusters (R(g) ~ 0.5 nm) on the nonpolar cellulose surfaces and on hydrophobi

194 esis of ultrasmall nickel nanoclusters (~1.5 nm) deposited on defect-rich boron nitride (BN) nanoshee

195 The required EUV light, at 13.5 nm wavelength, is produced in a hot and dense laser-driv

196 egrees as a vector bending sensor and - 17.5 nm/m(-1) as a curvature sensor.

197 singly, many MD runs on larger droplets (5.5 nm radius) culminated in IEM ejection of ubiquitin, as l

198 A control model containing a 5 nm bubble in pure water is also created.

199 1000 nm and with a spatial resolution ca. 5 nm to reveal domain morphology and distribution.

200 ike structure with a preexisting bubble of 5 nm radius.

201 aracteristics at a separation distance of ~5 nm, the dynamics differ considerably.

202 mineralized nanostructures consisting of 2.5-nm crystalline particles self-assembled into nanoleaves.

203 ing eight colors in 300-nm width, about 37.5-nm per color.

204 d an exosome population averaging 100 +/- 50 nm in diameter and containing a defined set of constitut

205 aphene with a curvature radius down to 25-50 nm are systematically investigated and the ambipolar ele

206 ze/linewidth, 10 nm position accuracy and 50 nm overlay precision.

207 sity distribution with a voxel size below 50 nm.

208 the "range" of molecular electronics to >50 nm and avoid the usually strong temperature dependence o

209 cellular and subcellular organelles at <=50 nm resolution.

210 2 nm) and disordered meso and macropores (50 nm to 200 mum) as well as ordered macropores (1.5 mm to

211 gnet with a lateral spatial resolution of 50 nm.

212 osition using a focused X-ray spot of sub-50-nm size.

213 d by higher wavelengths ranging from 450-500 nm in skin to 500-600 nm in both brain and liver).

214 d narrow gaps were dozens of microns and 500 nm, respectively.

215 cold photodetector (T(D) ~ 300 K) from ~ 500 nm down to ~ 100 nm.

216 e reared in quasi-monochromatic red (410-510 nm) or blue (585-660 nm) light beginning before eye-open

217 was supplemented with UV-A 380 nm, green 510 nm, yellow 595 nm or orange 622 nm LED wavelengths at to

218 wavelength ranges of 484-490 nm and 508-518 nm, are the most effective features for porosity recogni

219 nm, 2.13 eV) in comparison to DJP(n=1) (523 nm, 2.37 eV); thus, DJP(n=2) can be used for efficient p

220 esponsivity of 0.16 mA/W was achieved at 532 nm.

221 icles (LSP) was found to be 420, 606 and 535 nm, respectively.

222 is, we find an unexpected PL increase (~ 540 nm) at the oil/shell interface.

223 etermined by UV-Vis spectrophotometer at 555 nm.

224 ths below 405 nm (ultraviolet) and above 565 nm (orange & red) and that targeted blocking of lower wa

225 er carrier lifetime and absorption edge (580 nm, 2.13 eV) in comparison to DJP(n=1) (523 nm, 2.37 eV)

226 d with UV-A 380 nm, green 510 nm, yellow 595 nm or orange 622 nm LED wavelengths at total photosynthe

227 .1 nm diameter Au NPs, 87.2 +/- 2.9% for 1.6 nm Au NPs, and an unprecedented full 100% Ag for 0.9 nm

228 7% Pt following replacement with 4.1 and 1.6 nm diameter Au NPs, respectively, consistent with qualit

229 n a porous medium of mean pore diameter 28.6 nm.

230 average molecular weight of 18.2 kDa and 3.6 nm in helical height, exhibits the highest anion-transpo

231 When the Pt layer is thinner than 6 nm, switching the ferroelectric polarization even change

232 ies, but with improved PLQY of 36%, for a 60 nm thick film, among the highest reported for lead-free

233 acitor, scalable down to a device area of 60 nm(2).

234 Most cells form large vesicles of 350-600 nm in diameter at their apical side, continuously intern

235 s ranging from 450-500 nm in skin to 500-600 nm in both brain and liver).

236 axima close to 450 nm and emission above 600 nm.

237 best known BODIPY photocages absorbing >600 nm, validating the effectiveness of a strategy for desig

238 performance, we show that devices up to 600 nm thick maintain efficiencies of >8% because domains ca

239 3+)-GTP association to RAS, monitored at 615 nm, and subsequent Eu(3+)-GTP-loaded RAS interaction wit

240 e an exceptional deep red (lambda(max) = 621 nm, = 0.32, tau(av) = 366 ns) thermally activated delaye

241 m, green 510 nm, yellow 595 nm or orange 622 nm LED wavelengths at total photosynthetic photon flux d

242 of 15 000 cm(-1) to generate emission at 633 nm.

243 (CRDS) technique using a diode laser at 644 nm and a right-angled prism for evanescent field generat

244 served variant affinities between ~1 and 650 nm and activation potencies ranging from 1.8-fold that o

245 ng only white light and also with only a 655-nm diode laser that causes calculus to fluoresce.

246 is prospective study was to evaluate the 655-nm InGaAsP diode laser in detecting subgingival calculus

247 ochromatic red (410-510 nm) or blue (585-660 nm) light beginning before eye-opening.

248 , consisting of blue 455 nm, red 627 and 660 nm and far red 735 nm LEDs, was supplemented with UV-A 3

249 od, the hue (color) value of thousands of 67 nm Au nanoparticles immobilized on a glass coverslip sur

250 Having emission peaks from 670 nm to 720 nm, the next generation of miRFPs should becom

251 its a wide light-harvesting range (up to 674 nm), a optical energy gap (2.04 eV), and highest energy

252 em becomes near-infrared (NIR) emissive (675 nm).

253 y (Stober SNPs 46 +/- 4.9 and 432.0 +/- 18.7 nm and mesoporous SNPs 466.0 +/- 86.0 nm) upon single do

254 e-functionalized tantalum oxide NPs (d ~ 5.7 nm) were synthesized via a one-pot two-step reverse micr

255 FPE (dewaxed)) is within the range 64.5-64.7 nm corresponding to the 9(th) and 10(th) order peaks.

256 y is poor, with an undesirable shift (over 7 nm) toward longer wavelengths under operating conditions

257 persistently, and blocking p150 led to a 70 nm/s plus-end shift in the average velocity of the compl

258 nd near-infrared window (NIR-II, 1,000-1,700 nm), where tissues are highly transparent, have expanded

259 tofluorescence in tissue at visible (350-700 nm) and near-infrared (700-1,000 nm) wavelengths.

260 ocages that absorb light strongly around 700 nm.

261 Having emission peaks from 670 nm to 720 nm, the next generation of miRFPs should become versatil

262 Previous work noted that a CT band at 726 nm formed when ET-FAD was reduced and Bf-FAD was oxidize

263 is is corroborated by persistence of the 726 nm species during gentle protein denaturation and simple

264 sociation constant [K (d)] = 44.47 +/- 15.73 nm).

265 ction with RAF-RBD-Alexa680 monitored at 730 nm.

266 e 455 nm, red 627 and 660 nm and far red 735 nm LEDs, was supplemented with UV-A 380 nm, green 510 nm

267 In DM-PSI preparations excited at 740 nm, the excitation remained localized on the long-wavele

268 nd was illuminated by a NIR diode laser (755 nm, 10 mW/cm(2)).

269 the near UV through the far red (330 to 760 nm).

270 o-PANI:PSS fibres (diameter of ~50.3 +/- 4.8 nm) for the detection of NH(4)(+) with a wide linear ran

271 of a thousand pixels each, with pitch of ~8 nm, on its inner and outer surfaces.

272 Backsteps are usually 8 nm but can be larger.

273 ch of 6.4 nm are demonstrated on stripes >80 nm wide.

274 ~30-kb-long single-segmented RNA in the ~80-nm-diameter lumen.

275 his beamline is measured to be 11 fs for 800 nm excitation.

276 5 s and recovery in 2 s) when exposed to 800 nm light at an average output power of ~1.0 W cm(-2) , w

277 tNP electrocatalysts covered by a 100 to 800 nm thick layer of the proton exchange membrane Nafion.

278 f the hydrogel and with the treatment of 808 nm laser irradiation, tumors are eradicated and no recur

279 rmions with diameters ranging from 35 to 825 nm.

280 s, and an unprecedented full 100% Ag for 0.9 nm diameter Au NPs.

281 fferent tetralactam macrocycles around a 1.9 nm dumbbell-shaped nitrogenated nanographene.

282 sting nanotubes enabled by tunable (~4.3-4.9 nm), uniform (+/-0.3 nm) cage-like scaffolds.

283 NETs (~90 nm diameter) were fabricated from hemoglobin-depleted mi

284 f a 100 megadalton DNA-origami barrel of ~90 nm diameter and ~250 nm height, that provides a rhombic-

285 The 702-900 nm range of the NIR spectrum was associated with the cha

286 iform fiber morphology with ~200 nm and ~900 nm average fiber diameter, respectively.

287 sients in GCaMP6s-expressing neurons for 920 nm two-photon and 1320 nm three-photon excitation.

288 Continuous-wave (nonpulsed) 920-nm illumination at the same average power was as damagin

289 rd tensile strength up to ~570 MPa for a 940 nm thick film and electrical conductivity of ~15 100 S c

290 A W(-1) in the NIR spectral region (920-960 nm), which is the highest among organic photodiodes.

291 probe could be fluorescently imaged with 980 nm excitation, having deep penetration depth, by a fluor

292 their first order excitonic transition (~985 nm) fluoresce brightly at ~1160 nm.

293 NIR) fluorescence intensity of SWCNTs at 998 nm is either unchanged or decreases depending on the sur

294 remely high pore density of 1 sub-nm channel nm(-2) , TPT CNMs let water molecules rapidly pass, whil

295 ngth of 414.234 (Fe I) nm and 396.054 (Al I) nm, and the kurtosis of spectra at wavelength ranges of

296 spectra at the wavelength of 414.234 (Fe I) nm and 396.054 (Al I) nm, and the kurtosis of spectra at

297 and is found to vary between 300 and 1800 K nm for a wide range of particle compositions.

298 d a surface Pt density of around 0.6 Pt site/nm(2).

299 g their extremely high pore density of 1 sub-nm channel nm(-2) , TPT CNMs let water molecules rapidly

300 79.76% after exposure to ultraviolet (UVA385 nm), while viabilities of non-protected spores under the