ライフサイエンスコーパス: glass

1 d artificial surfaces (i.e. plant leaves and glass).

2 goes various modes of detachment from silica glass.

3 the role of selenium in the formation of the glass.

4 r the stress-bearing properties of colloidal glass.

5 rradiation deep inside 35Li2O-35Nb2O5-30SiO2 glass.

6 , akin to the ones in supercooled liquids or glasses.

7 deo microscopy data of hard-sphere colloidal glasses.

8 havior for typical lanthanide based metallic glasses.

9 rcooled liquid is shown by the 85Al and 84Al glasses.

10 tope compositions measured in both trinitite glasses.

11 ion and 107 (11.9%) only needed prescription glasses.

12 ractical viable method to join bulk metallic glasses.

13 0.05-0.17]) for children not pretreated with glasses (1 RCT, 177 participants).

14 UVs shrink irreversibly because the membrane/glass adhesion creating the high-resistance seal (>1 GOm

15 FEM), the current paradigm of using the spin-glass algorithm to integrate gene expression and epigene

16 10 to 2.3 nm, and including other surfaces (glass, aluminum, and porcelain).

17 nsition in La32Ce32Al16Ni5Cu15 bulk metallic glass and can shed new light on the mechanisms of polyam

18 to join Pd43Cu27Ni10P20 (at.%) bulk metallic glass and characterized the properties of the joint.

19 salt systems and is also promising for waste glass and coal ash recycling.

20 Solid substrates (glass and crystalline silicon) covalently functionalized

21 oad exothermal peak was observed between the glass and crystallization temperatures.

22 ed on a range of substrates, including rigid glass and flexible plastic.

23 During the overlap period (2003-2011), GLASS and GLOBMAP exhibited a decreasing trend, TCDR no

24 ome structural homology between the metallic glass and its high temperature crystalline phase.

25 stic spheres having sharp interfaces, so the glass and jamming regimes can be distinguished more clea

26 used in photonics and optoelectronics, with glass and plastics as traditional choice of materials.

27 ined Brownian-motion of bacteria adhering to glass and their AFM force-distance curves and include th

28 afe guidewires were made from micropultruded glass and/or aramid fibers and epoxy resin with diameter

29 rystals, as well as amorphous phases such as glasses and gels.

30 ime evolution of avalanches in bulk metallic glasses and granular materials, we uncover a regime of u

31 mical bonds of similar strengths in basaltic glasses and iron-rich alloys, even at high pressure.

32 making this a universal phenomenon of oxide glasses and melts.

33 identify structural properties of quiescent glasses and relate them to glassy dynamics.

34 sses of industrial commodities such as iron, glass, and cement are carbon-intensive, accounting for 2

35 made nonrenewable materials such as plastic, glass, and metals, as well as more advanced applications

36 (FCMs) that include plastics, paper, metal, glass, and printing inks.

37 (001) and (112) grown by MOCVD are bonded to glass, and then the growth substrate is removed with a X

38 as augmented reality devices, smart surgical glasses, and smart windows.

39 substitution of selenium for sulphur in GLS glass are described.

40 F indicates that the Zr-Zr distances in this glass are significantly reduced compared to those quench

41 nce, of (A) Er(3+)(8%)Tm(3+)(0.5%):telluride glass are very similar to those of Er(3+) ions in (C) Er

42 Density and hardness of glasses are known to increase upon both compression at t

43 Glasses are often described as supercooled liquids, whos

44 The High Pressure Quenched glasses are stable in ambient conditions after decompres

45 our decades long studies of Pd-Ni-P metallic glasses, arguably the best glass-forming alloys.

46 Here, we use a colloidal glass as the model system to directly study this issue.

47 ight into the structural changes of silicate glasses as analogue materials for silicate melts at ultr

48 mpressing a sodium-magnesium aluminosilicate glass at 1 GPa at Tg, followed by sub-Tg annealing in-si

49 particle is resolvable from the surrounding glass at the 2sigma uncertainty level (where sigma repre

50 fluoride-containing phosphate-rich bioactive glass (BAG-F).

51 Algae are grown in glass based microfluidic chip, which contains integrated

52 f different pesticides with algae in a novel glass based microfluidic device with integrated optical

53 of pH cycling immersion on the corrosion of glass-based ceramic materials were investigated by exami

54 esence of molecular templates immobilised on glass beads (the solid-phase).

55 Utilizing glass beads and kaolinite as model collector surfaces, w

56 validated to produce homogeneous, flux-free glass beads of geochemical reference materials (GRMs), u

57 ot interact with the surfaces of acid-washed glass beads or standard Ottawa sand, which presented les

58 ovelty of the procedure is the production of glass beads using 9 parts high purity synthetic enstatit

59 collector particle composition (kaolinite vs glass beads) and nanoparticle surface chemistry (PVP, ci

60 rature is largely based on electrolysis in a glass beaker or H-cells that often give poor performance

61 The spin-glass behavior of graphite oxide is corroborated by the

62 and may be responsible for macroscopic spin-glass behavior.

63 roved resistance to recrystallization in the glass blends, able to remain fully amorphous for >1 mont

64 lastic deformation of Zr-based bulk metallic glass (BMG).

65 ted silicon network is directly derived from glass bottles via magnesiothermic reduction.

66 Multiple proteolytic processing sites in Glass bottom boat (Gbb), the Drosophila BMP7 ortholog, c

67 ratio for the 3D Edwards-Anderson Ising spin glass, by means of large-scale simulations on the specia

68 Complex states in glasses can be neatly expressed by the potential energy

69 cines are prepared by nanoprecipitation in a glass capillary microfluidics device.

70 f 150 mum diameter leak holes represented by glass capillary tubes, in recirculating solutions that a

71 ass, but only for non-polymeric beads (i.e., glass, ceramic, metallic).

72 to the high-translucency lithium disilicate glass-ceramic and zirconias, including the most transluc

73 d to account for the effect of pH cycling on glass-ceramic corrosion.

74 Thus, the severity of glass-ceramic degradation depends not only on the pH of

75 Glass-ceramic disks were immersed in each pH solution fo

76 zirconia (e.g., Zpex Smile) and lithia-based glass-ceramics (e.g., IPS e.max CAD HT).

77 ions and fatigue parameters for 3 reinforced glass-ceramics (fluormica [FM], leucite [LR], and lithiu

78 he market lack the aesthetics of competitive glass-ceramics and are therefore somewhat restricted in

79 mal mass micro thermostat and a microfluidic glass chip as central elements were designed and evaluat

80 A thin 3-sided glass coating on the inner channel walls prevents multi-

81 This discovery in Yb-based metallic glass, combined with the previous reports on other metal

82 airway abnormality, the percentage of ground glass component and the type of tumor margin.

83 ates covalently attached to the surface of a glass coverslip using a fixed ratio of a native nucleoti

84 Isolated blood eosinophils were incubated on glass coverslips coated with intravenous immunoglobulin

85 ms were modelled as in vitro "microcosms" on glass coverslips inoculated with the natural microbial p

86 erent and well-spread primary islet cells on glass coverslips is required for detailed imaging studie

87 Cells were attached to glass coverslips within flow chambers that allowed appli

88 We show higher melting-point silicate glass cross-cutting lower melting-point Al-Cu-Fe alloys,

89 Overall, individuals who consumed >1 glass/day had 30% higher risk for clinical AL progressio

90 CI: 0.30 to 0.89), whereas those drinking >1 glass/day had significantly higher risk (RR = 1.50; 95%

91 >1 glass/week and </=1 glass/day; and 4) >1 glass/day.

92 ) </=1 glass/week; 3) >1 glass/week and </=1 glass/day; and 4) >1 glass/day.

93 LS glass to about 15 microm for Se-added GLS glass defined by the 50% transmission point.

94 shear bands of the type observed in metallic glasses deforming under mechanical stress.

95 Stable smart coatings on glass demonstrate robust switching over 10(4) cycles, an

96 ree of softness of localized structures in a glass, determined by a coupling between internal stresse

97 to freshwater; that is, they are late-stage glass eels ( approximately 2 years old), not the pelagic

98 the behaviour of these late-stage freshwater glass eels, and their responses to magnetic fields, can

99 response from reference values obtained by a glass electrode was 0.2pH units.

100 icles (AuNPs)/fluorine doped tin oxide (FTO) glass electrode.

101 or aspects include band convergence, "phonon-glass electron-crystal", multiscale phonon scattering, r

102 ic pseudogaps offers an avenue to new phonon glass-electron crystal materials.

103 Every year many tons of waste glass end up in landfills without proper recycling, whic

104 suring a clear distinction between where the glass ends and where jamming begins becomes very difficu

105 Porous media made of nitrocellulose and glass fiber are common "paper" substrates for lateral fl

106 While the glass fiber filter disk has a higher capture efficiency

107 Improvements were made to include glass fiber filters as the substrate within the paper sp

108 y; HR-released histamine was quantified by a glass fiber-based fluorometric method; passive HR-IgE-st

109 of a new micro-SORS sensor, which uses bare glass fibers to transfer the laser radiation to the samp

110 olids (aramid fibers, and carbon fibers, and glass fibers).

111 The role of selenium is hypothesized in the glass formation to explain these changes.

112 d, for example, to play an important role in glass formation-the microscopic origin of fragility is p

113 ences between a bulk and thin film polymeric glass former can be understood by differences in local m

114 relaxation kinetics of a prototype molecular glass former over a temporal range of 13 decades and ove

115 h purity synthetic enstatite (MgSiO3) as the glass former with 1 part of sample (sample mass approxim

116 n the molecular dynamics of a small-molecule glass former.

117 e nonequilibrium shear response of a typical glass-former, squalane.

118 d measured R C to a minute fraction of known glass formers.

119 The glass forming ability (GFA) of metallic glasses (MGs) is

120 heterogeneity, along with other features of glass-forming (GF) liquids such as collective atomic mot

121 Pd-Ni-P metallic glasses, arguably the best glass-forming alloys.

122 Co-melts based on blends of two different glass-forming compounds were prepared with the goal of e

123 onal substitutions are studied to define the glass-forming region of the modified material.

124 re hydration or humidification of an organic glass-forming sample result in stiffer mechanical proper

125 t the out-of-equilibrium behavior of a model glass-forming system can be understood in terms of softn

126 Recovered glass fragments suggest permanent densification.

127 scopy performed on a red-blue-purple striped glass from the stained glass windows of the Sainte-Chape

128 ransient force balance is what distinguishes glasses from supercooled liquids.

129 The addition of selenium to GLS glass generally results in a lower glass transition temp

130 r0.4 )3 perovskite as the photoactive layer, glass-glass laminated devices are reported, which sustai

131 Proportion of lung occupied by ground glass, ground glass-reticular (GGR), honeycombing, emphy

132 ates in the (90)Y resin group than the (90)Y glass group (resin PFS 6.1 mo [95% confidence interval C

133 igated, Cox analyses showed that only in the glass group, the BCLC staging system and the serum AFP l

134 iods, and the differences followed the order GLASS>LAI3g>TCDR>GLOBMAP.

135 lities of global mean LAI followed the order GLASS>LAI3g>TCDR>GLOBMAP.

136 )-NDI-Delta(3(-*))(CoCp2(+))3] in an organic glass has a spin-frustrated doublet ground state and a t

137 e-induced polyamorphism in Ce-based metallic glass has attracted significant interest in condensed ma

138 The glass has been connected to an electronic system that dr

139 kening and inertial effects in bulk metallic glasses have strikingly similar effects on the slip dyna

140 by a laser-diode from the backside through a glass hemisphere, generating surface plasmon polaritons.

141 optically and thermally coupled with another glass hosting a microfluidic network made in polydimethy

142 The proposed System on-Glass hosts thin metal films acting as heating sources;

143 ogeneous dislocation of the particles in the glass, i.e., the appearance of shear bands of the type o

144 Patching plus glasses improved visual acuity by about 1 line after 1 y

145 agent was optimized from foliage, sand, and glass in a simulated biothreat scenario using bovine ser

146 very hard but at the same time as brittle as glass in as-quenched or low-temperature-tempered state.

147 the red stripe or a metastable overoxidized glass in the purple stripe.

148 ation group analysis of disordered models of glasses, in particular of the spin models at the origin

149 fluoride-containing phosphate-rich bioactive glass incorporated as micrometer-sized filler in dental

150 In LHZ an infinite-range spin-glass is mapped onto the low energy subspace of a spin-1

151 tion energy typical of beta relaxations in a glass; it has the same temperature dependence as fluctua

152 are stiffer, and the characteristics of the glass-jamming transition resemble more closely the situa

153 The GLASS linear trend and interannual variability were almo

154 ry has been reported in a number of metallic glass materials in which a broad exothermal peak was obs

155 Ps (with sizes of 2.0-3.4 mum) comprise SiO2 glass matrices and 10-nm-sized Zn-Fe-oxide nanoparticle

156 u, and Mn were adjusted to ensure a reducing glass matrix in the red stripe or a metastable overoxidi

157 responses of neutron irradiation in metallic glasses (MGs) have been investigated by making a series

158 The glass forming ability (GFA) of metallic glasses (MGs) is quantified by the critical cooling rate

159 All metallic glasses (MGs), irrespective of their compositions, becom

160 ctal models of packing structure in metallic glasses (MGs).

161 r OVA-TI, with comparable reproducibility to glass microdevice PAGE.

162 PAGE protein separations in a composite PDMS-glass microdevice, that toggles from an "enclosed" micro

163 of microfluidic PAGE without the need for a glass microfabrication infrastructure.

164 This technique involves a custom-made glass microfluidic platform, in which oil droplets can b

165 um obtained from a single drop of blood on a glass microscope slide.

166 nal review board approval is required before glass microspheres can be used under a compassionate-use

167 Because glass microspheres have a higher activity per particle,

168 Comparison between resin and glass microspheres revealed higher but not statistically

169 Comparison between resin and glass microspheres revealed no significant survival diff

170 performed on approximately 1 mg scale using glass microvials providing a miniaturized high-throughpu

171 The prepared organic glass monoliths provided fluorescence quantum yields and

172 bed of nails"-like approach that uses quartz glass nanopillars to anchor islets, solving a long-stand

173 et, and finally resulted in ordered metallic glass nanotube (MGNT) arrays after removal of the photor

174 size effects from one such class of metallic glass nanowires prepared by casting using molecular dyna

175 tuation electron microscopy of bulk metallic glasses of CuZrAl(Ag) demonstrates that medium-range ord

176 ation, resolution of the parenchymal "ground glass" opacity and absence of further episodes of hemopt

177 of numerous bronchial branches and a "ground glass" opacity in the anterior segment of the right uppe

178 much higher solubility in CaZrF6 than silica glass or crystobalite.

179 Transfer of skin oils by touching the glass or foil surfaces, or after washing the glass surfa

180 n or lipid diffusion is observed with either glass or stainless steel substrate.

181 rate to high myopia and difficulties wearing glasses or contact lenses.

182 0.53; resin OS 7.7 mo [95% CI, 7.2-8.2] and glass OS 7 mo [95% CI 1.6-12.4], P = 0.77).

183 mental mappings demonstrate that the colored glass parts are derived from the same base glass, to whi

184 Heating glass Petri dishes or squares of aluminum foil to about

185 mo [95% confidence interval CI, 4.7-7.4] and glass PFS 5 mo [95% CI, 0.9-9.2], P = 0.53; resin OS 7.7

186 quid phase, which forms the room-temperature glass phase on quenching.

187 xploration of important features of the spin-glass phase without requiring uncontrollable extrapolati

188 on different substrates such as the tip of a glass pipet, a double-barrel pipet, and a freestanding s

189 (LSPR) of gold nanoparticles deposited on a glass plate and on a long-period grating (LPG) induced i

190 ound that 16.0cm(2) area of polymer modified glass plate is sufficient enough to kill 10(5)CFUmL(-1)

191 -Pd) modified fluorine doped tin oxide (FTO) glass plate was fabricated for detection of consensus DN

192 Possible advantages and applications for MOF glasses produced by utilizing the tunable chemistry of t

193 jor changes in melt viscosity, together with glass Raman and Nuclear Magnetic Resonance measurements

194 The order in the centrifuged glasses reflects the ground state order in the dispersio

195 aling can be combined to access a "forbidden glass" regime that is inaccessible through thermal histo

196 features, such as diaplectic (i.e., shocked) glass, remain therefore controversial and unresolvable.

197 ion of lung occupied by ground glass, ground glass-reticular (GGR), honeycombing, emphysema, and norm

198 than the blackbody limit on centimeter sized glass samples without any specialized sample preparation

199 eling, the dependence of this interaction on glass shell thickness is elucidated and the experimental

200 Arrays of on-chip spherical glass shells of hundreds of micrometers in diameter with

201 the fingerprints were collected by swiping a glass slide across the forehead of consenting adults.

202 n, the samples are placed on a silver-coated glass slide with a thin spacer, and excited by a laser-d

203 m WSI was found equivalent to diagnosis from glass slides using TM in this statistically powerful stu

204 of this mimotope was immobilized onto epoxy-glass slides, and fumonisin B1 was detected in a competi

205 were deposited onto epoxy-activated standard glass slides, followed by immobilization of biotinylated

206 hole blood samples from thick blood films on glass slides.

207 The islet cell monolayer cultures on glass stably maintain distinct mono-hormonal insulin+, g

208 te, with the critical behavior, and with the glass state.

209 y processed to produce optically transparent glass structures with sub-millimeter features in forms r

210 the placement of the nanoparticles between a glass substrate and a sample medium (air, water).

211 a small footprint, which is fabricated on a glass substrate and integrated with a microfluidic chip.

212 retically deposited onto an indium-tin-oxide glass substrate and used for immobilization of anti-cyto

213 )/Cu (>100.0 nm) was deposited on a Si or K9-glass substrate by magnetron sputtering.

214 the first time, the integration on a single glass substrate of different thin film technologies in o

215 chip microscope and a surface-functionalized glass substrate prepared to specifically capture the tar

216 electrodes microarray was fabricated over a glass substrate using focused ion beam milling.

217 ide thin film nanostrtablucture deposited on glass substrate was used as a potential matrix for the r

218 in fluorescence intensity compared to a bare glass substrate, which enabled us to image single fluore

219 tation and properties of PSLR over arrays of glass substrate-supported single and double Au nanoparti

220 x SiON film on both SiO2/Si and borosilicate glass substrate.

221 ent ZnO nanorods (ZnO-NRs) were deposited on glass substrate.

222 gas using silver nanorods (AgNRs) arrays on glass substrates at ambient conditions.

223 jugate nanostructures on low-cost ink coated glass substrates through a facile and flexible single pu

224 gallium phosphide thin films on transparent glass substrates via transfer bonding.

225 .9 mA/cm(2) and a fill factor (FF) of 62% on glass substrates while a Jsc of 13.0 mA/cm(2) and FF of

226 evolution of macroscopic state in a metallic glass, such as ageing and rejuvenation, through a set of

227 Identifying heterogeneous structures in glasses-such as localized soft spots-and understanding s

228 e imaging) and to create a Wnt platform on a glass surface for stem cell maintenance and cell populat

229 approximately 5 nm sized Pt particles on the glass surface surrounding the electrode.

230 GNR assembly in vertical standing array on a glass surface was fabricated as plasmonic substrates, re

231 glass or foil surfaces, or after washing the glass surface with detergent and bare hands, was also ob

232 n of the stratum corneum of the skin and the glass surface.

233 immobilize Wnt3a proteins on microbeads or a glass surface.

234 Quantification of TATP solutions from glass surfaces by DBDI-MS, using TATP-3,6,9-(13)C as int

235 ndency of HA to inhibit colonization on bare glass surfaces when silver is absent.

236 defined locations on silicon and transparent glass surfaces: as proof of concept, clusters of either

237 with the previous reports on other metallic glass systems, demonstrates that pressure induced polyam

238 t a 200 nm-thick Zr-based thin-film metallic glass (TFMG), which acts as an effective diffusion barri

239 orphism of La32Ce32Al16Ni5Cu15 bulk metallic glass, the acoustic velocities, measured up to 12.3 GPa

240 Molecular processes of creep in metallic glass thin films are simulated at experimental timescale

241 tructure and hence the stability of metallic glasses through heat treatment.

242 d to be extended from about 9 microm for GLS glass to about 15 microm for Se-added GLS glass defined

243 The conversion from un-recycled glass to favorable materials is of great significance fo

244 d glass parts are derived from the same base glass, to which TMs were deliberately added.

245 frared spectroscopy (fNIRS) and eye-tracking glasses, to examine the neural systems linked to pupil d

246 el, a recurrent neural network based on spin glasses, to model the dynamics of cell cycle in HeLa (hu

247 andesite lapilli from temperatures below the glass transition ( 690 degrees C) to above inferred erup

248 Above the solvent glass transition (Tg approximately 180 K), the rebinding

249 However, the nature of both the glass transition and the high-to-low-density transition

250 The glass transition appears even for the 85Al alloy where t

251 On heating, the glass transition into the supercooled liquid is shown by

252 hree dimensions have similar behavior as the glass transition is approached, showing that the long-wa

253 The dynamical glass transition is typically taken to be the temperatur

254 , but the influence of dimensionality on the glass transition is unresolved.

255 ns can be interrupted to form gels either by glass transition or by crystallization.

256 Within our theoretical framework, the glass transition results in an avoided phase transition.

257 reased hydrodynamic radius (in solution) and glass transition temperature (in bulk materials) were ob

258 own to increase upon both compression at the glass transition temperature (Tg) and ambient pressure s

259 The glass transition temperature (Tg) for all of the powders

260 ambient temperatures, up to 60 K below their glass transition temperature (Tg), by subjecting them to

261 her supercooled liquids stop flowing below a glass transition temperature [Formula: see text] or whet

262 um to GLS glass generally results in a lower glass transition temperature and an extended transmissio

263 Annealing at the glass transition temperature at ambient pressure reverse

264 cm(-3) , even at a temperature close to the glass transition temperature of polymer (i.e., 217 degre

265 ind a pronounced thickness dependence of the glass transition temperature of ternary polymer/fulleren

266 thickness) at various temperatures below the glass transition temperature, [Formula: see text], of al

267 eta changes little with cooling towards the glass transition temperature, Tg.

268 We developed a method to estimate glass transition temperatures based on the molar mass an

269 rediction of the calorimetric and mechanical glass transition temperatures that demarcate the passage

270 rods at sufficiently high density exhibit a glass transition toward a disordered state characterized

271 se systems just above or below the dynamical glass transition, such as viscosity, can change by many

272 or when made viscous upon cooling toward the glass transition, suggesting a common theoretical basis.

273 increase of relaxation time approaching the glass transition.

274 be utilized in any material that exhibits a glass-transition temperature (T g ) and a rubbery platea

275 a fundamental distinction between 2D and 3D glass transitions.

276 We examine the nonlinear flow of a glass under deformation at finite strain rate.

277 orphism and structural evolution in metallic glasses under pressure.

278 We investigated the structure of SiO2 glass up to 172 GPa using high-energy X-ray diffraction.

279 r, 36 diffuse) with (90)Y TARE (41 resin, 36 glass) using pretreatment PMD.

280 which is usually observed for hot compressed glasses, vanishes for samples previously subjected to hi

281 d Si from the method-prescribed borosilicate glass vessels which appeared to suppress the release of

282 For this purpose, we coated a round glass wafer with photocatalytically active anatase-phase

283 be injected onto the rim of the TiO2-coated glass wafer, before the entire wafer is exposed to UV ir

284 Smooth glass was found to provide the upper and lower bounds fo

285 nescence in Er(3+)/Tm(3+) co-doped telluride glass was studied.

286 stems - granular materials and bulk metallic glasses - we show evidence that not only the statistics

287 d: 1) non-drinker; 2) </=1 glass/week; 3) >1 glass/week and </=1 glass/day; and 4) >1 glass/day.

288 Never-smoker males drinking </=1 glass/week had significantly lower risk for clinical AL

289 mption were defined: 1) non-drinker; 2) </=1 glass/week; 3) >1 glass/week and </=1 glass/day; and 4)

290 ITO, gold, platinum and glass were tested and the amount of superoxide anion pro

291 Optically transparent and stable organic glasses were prepared from these materials using a bulk

292 Here, we study hard-sphere glasses which either crystallize or age depending on the

293 The design included a chamber with glass windows allowing imaging with upright or inverted

294 d-blue-purple striped glass from the stained glass windows of the Sainte-Chapelle in Paris, France, d

295 s, attachment of a range of colloid sizes to glass with three levels of roughness was examined under

296 ranging from fluoropolymers to borosilicate glass, with etch rates in excess of 1 microm s(-1) .

297 of Er(3+) ions in (C) Er(3+)(0.5%):telluride glass, with respect to the shapes of their excitation sp

298 and Gibbs free energy for the interaction of Glass/ZnO-NRs/Protein-A/Anti-OTA with OTA were calculate

299 i-OTA) in order to form OTA-selective layer (Glass/ZnO-NRs/Protein-A/Anti-OTA).

300 Formed Glass/ZnO-NRs/Protein-A/BSA&Anti-OTA structures were int