ライフサイエンスコーパス: cantilever

1 he solutes behind, adding to the mass of the cantilever.

2 of explosive vapors using a nanoporous TiO2 cantilever.

3 grated into an atomic force microscopy (AFM) cantilever.

4 of a microchanneled atomic force microscopy cantilever.

5 to the protein construct through a compliant cantilever.

6 ezoelectric polyvinylidene difluoride (PVDF) cantilever.

7 of forces that can be applied with a single cantilever.

8 g, and the full force can be measured by the cantilever.

9 th 18.4-48.9pg mass load on the MIP modified cantilever.

10 inding causes surface stresses that bend the cantilever.

11 limited by the mechanical properties of the cantilever.

12 dependent of the nature of attachment to the cantilever.

13 field and reducing the spring constant of a cantilever.

14 tical microscopy and measuring forces on the cantilever.

15 tes from the viscous damping of the dithered cantilever.

16 at is pulled with a relatively large bead or cantilever.

17 m Coh using an atomic force microscope (AFM) cantilever.

18 ed by the Euler-Bernoulli theorem for linear cantilevers.

19 e to those needed for linear carbon nanotube cantilevers.

20 ontrolled attachment of single live cells on cantilevers.

21 e do not cause significant deflection of the cantilevers.

22 zation of unspecific protein adsorption onto cantilevers.

23 ning probe systems that rely on conventional cantilevers.

24 arrays assembled on atomic-force-microscope cantilevers.

25 ging modes, which often work best with stiff cantilevers.

26 hybrid nematic liquid crystal network (LCN) cantilevers.

27 d attachment kinetics of biomolecules on the cantilevers.

28 vers as compared to that for control peptide cantilevers.

29 tors and an array of microfabricated silicon cantilevers.

30 at of state-of-the-art piezoelectric bimorph cantilevers.

31 n artefacts conflict with the use of smaller cantilevers.

32 for accurate calibration of rectangular AFM cantilevers.

33 5 or 8 microsensors culled from a group of 5 cantilever, 5 capacitor, and 5 calorimeter transducers c

34 e differential response between two adjacent cantilevers (a sensing/reference pair) is utilized to de

35 method that consists of measuring the local cantilever activity and deflection in a feedback generat

36 ration microscopy (SPAM), in which the TMAFM cantilever acts as an accelerometer to extract tip-sampl

37 ve fabricated a silicon-compatible thin-film cantilever actuator with a single flexoelectrically acti

38 on an analysis of ringing signal of the AFM cantilever after detaching the AFM probe from the sample

39 thin (~5 nm) tip by amorphous carbon to the cantilever allows us to image the surface structure of l

40 rm stability of AFM achieved using gold-free cantilevers allows folding-unfolding reactions of alpha/

41 ins between an atomic force microscopy (AFM) cantilever and a glass surface using HaloTag anchoring a

42 the dithering of an atomic force microscope cantilever and a single molecule attached to its end sys

43 ndicular to the filament axis: a deflectable cantilever and a stationary beam.

44 h only the tip conducting was used as an AFM cantilever and a working electrode in a three-electrode

45 obe that combines a sideways-mounted elastic cantilever and an optical-lever detection module with au

46 After adhering bacteria to the end of an AFM cantilever and approaching surfaces of mica, gold, or po

47 n principle, applicable to many parallelized cantilever and cantilever-free scanning probe molecular

48 ibronectin-patterned atomic-force microscope cantilever and coverslip.

49 -susceptible and drug-resistant targets on a cantilever and demonstrated significant differences in m

50 ically attach to the atomic force microscope cantilever and form a consistent pulling geometry to obt

51 ect transistor (MOSFET) into the base of the cantilever and recording decreases in drain current with

52 ent electrostatic effect between the AFM tip/cantilever and sample surface can occur.

53 ong electrostatic effect between the AFM tip/cantilever and sample surface, regardless of contact and

54 licated because of the collision between the cantilever and samples.

55 adhesion of biomolecules to a surface and a cantilever and, for proteins, the integration of the tar

56 n with IFM function, we used microfabricated cantilevers and a high resolution imaging system to stud

57 rochemical characterization of nonconductive cantilevers and appropriate use for closed systems.

58 ntly varying the mechanical stiffness of the cantilevers and collagen matrix revealed that cellular f

59 Using nanofabricated cantilevers and newly developed high-resolution detectio

60 y, which combines the use of colloidal probe cantilevers and of a bioinspired polydopamine wet adhesi

61 buffer solutions using Lorentz force excited cantilevers and present a careful comparison between mec

62 Explosive particles were mounted on AFM cantilevers and repeatedly brought in and out of contact

63 omega(r)/m(C), where m(C) is the mass of the cantilever), and this notion has motivated scaling of bi

64 bundle of actin filaments against an elastic cantilever, and a 2-d cell undergoing wave-like protrusi

65 n films are integrated on microfabricated Si cantilevers, and they are operated in a non-linear regim

66 objects can be brought into contact with the cantilever anywhere along its length, which considerably

67 Motion of the bilayer cantilever architecture results from the huge spontaneou

68 ction effects from finite sized or patterned cantilevers are exploited.

69 The cantilevers are fabricated using a complementary metal o

70 d by measuring the deflection of the probes' cantilever arms.

71 On an eight-cantilever array chip, four cantilevers were coated with

72 The cantilever array coated with a range of thiolated ligand

73 A multiplex capillary coating method for cantilever array creation is demonstrated and validated

74 Even with impressive recent advances in cantilever array design, such arrays tend to be highly s

75 The detection limit of the cantilever array sensor is as low as 0.2 nM, which is co

76 It is demonstrated that the cantilever array sensors can be used as a powerful tool

77 ar concentrations based on a microfabricated cantilever array.

78 Cantilever arrays have been used to monitor biochemical

79 Such effects are readily generalized to cantilever arrays, and allow transmission detection of m

80 l wall precursor analogues (mucopeptides) on cantilever arrays, with 10 nM sensitivity and at clinica

81 e developed a metrology using piezoresistive cantilevers as force-displacement sensors coupled to a f

82 Here, we use nanomechanical cantilevers as surface-stress sensors, together with equ

83 e using silica beads attached to the AFM tip-cantilever assembly, which were functionalized by coupli

84 s achieved by simultaneously driving the DCF cantilever at its resonant frequency in one dimension an

85 h a temporal resolution much faster than the cantilever bandwidth, determined by the modulation frequ

86 les prepared on a rigid substrate by using a cantilever based molecule deposition tool, and we tested

87 Cantilevers based on polycrystalline diamond surfaces ar

88 nds are discernible at macroscopic scales in cantilever-based bending measurements of Pt thin films u

89 hanical signal is ubiquitous for DNA, making cantilever-based detection a widely useful and complemen

90 We present a fully automated cantilever-based method for highly precise and sensitive

91 ography-overcomes the throughput problems of cantilever-based scanning probe systems and the resoluti

92 However, increasing the throughput of cantilever-based scanning probe systems while maintainin

93 Scanning probe microscopies (SPM) and cantilever-based sensors generally use low-frequency mec

94 Fracture mechanics concepts using double cantilever beam configuration were used to characterize

95 tu scanning electron microscopy based double cantilever beam test, allowing to directly view and meas

96 tu scanning electron microscopy-based double cantilever beam test, thus enabling viewing and measurem

97 model in which the neck region behaves as a cantilevered beam.

98 dicate 1) the primary cilium is not a simple cantilevered beam; 2) the base of the cilium may be mode

99 es resonance frequency and quality factor of cantilever beams immersed in a fluid to the viscosity an

100 surements were also made on two-dimensional, cantilevered beams and curved beams, each with intersect

101 asuring the modal response (at resonance) of cantilevered beams with embedded nanocomposite films.

102 mpression/tension stress trajectories of the cantilevered beams, and (3) trabecular tracts typically

103 erimentally determined data obtained via the cantilever bending method.

104 The flow rate effect on the cantilever bending response is also discussed.

105 The cantilever bending was specific toward glucose, but not

106 mobilized probe molecules on microfabricated cantilevers; binding causes surface stresses that bend t

107 (QIM) and atomic force microscopy (AFM) with cantilevers biofunctionalized by sialyl-Lewis(x) (sLe(x)

108 n this study, we use a mass-change sensitive cantilever biosensor and a probe, 2',7'-bis-(2-carboxyet

109 The cantilever biosensor was immobilized with a 27-base DNA

110 btained from 15 microsensors comprising five cantilever, capacitor, and calorimeter devices coated wi

111 tial measurements using an in-situ reference cantilever coated with a nonspecific sequence of DNA.

112 d monolayers (SAMs), using in situ reference cantilevers coated with nonionizable hexadecanethiol SAM

113 hanges in the resonance frequency (mass) and cantilever deflection (adsorption stress).

114 -120 and -40 mV resulted in a linear upward cantilever deflection equivalent to an increase in membr

115 In both reactions, the cantilever deflection is qualitatively detected from the

116 tection, compression, and storage of the raw cantilever deflection signal in its entirety at high sam

117 Modeling this bending as a cantilever deflection with uniform loading requires accu

118 ipids in bilayer, resulted in an increase in cantilever deflection.

119 This allows simultaneous imaging via cantilever deflections in normal AFM force feedback mode

120 We show here novel cantilever designs that express torsional and lateral mo

121 erhydrophobic substrates having membrane and cantilever designs with stiffness 0.5-7630 N/m.

122 A cantilever device based on competitive binding of an imm

123 scalable surface-acoustic-wave- (SAW-) based cantilevered device for portable bio-chemical sensing ap

124 A microcantilever array sensor with cantilevers differentially functionalized with self-asse

125 s (RPs) and produce bending responses of the cantilevers due to analyte-induced surface stresses.

126 The illumination of a cantilever edge causes an asymmetric diffraction pattern

127 assisted adsorption of Br onto a gold-coated cantilever, either in its pristine state or previously c

128 d perpendicularly to and from the stationary cantilever, eliminating the need to attach them to a car

129 lated the forces of the T cell using the AFM cantilever, even these actin-inhibited T cells became ac

130 e have been estimated for the polymer-coated cantilevers exposed to volatile organics in water.

131 yses, suggest that the SH2 domain moves in a cantilever fashion with respect to the small lobe of the

132 optimal excitation voltage that enables the cantilever fluctuations to fully sample the shape and de

133 and tuning of the physical properties of the cantilever for optimized AFM dynamic mode operation.

134 ding of micro-mechanical transducers such as cantilevers for atomic force microscopy.

135 to be used for coating exceptionally large, cantilever-free arrays that can pattern with electrochem

136 This cantilever-free dot-matrix nanoprinting will enable the

137 The concept of using cantilever-free scanning probe arrays as structures that

138 The recent development of cantilever-free scanning probe arrays has allowed resear

139 plicable to many parallelized cantilever and cantilever-free scanning probe molecular printing method

140 nting using polymer pen lithography (PPL), a cantilever-free scanning probe-based technique that can

141 Here, we report a cantilever-free SPL architecture that can generate 100 n

142 Here we describe a low-cost and scalable cantilever-free tip-based nanopatterning method that use

143 e approach, which relies on detecting either cantilever frequency or phase, we used it to detect elec

144 lineshape and the magnitude of the observed cantilever frequency shift as a function of field and ca

145 single and multiple T4P on retraction of the cantilever from the surfaces could be described using th

146 omplex, and T-shaped atomic force microscope cantilevers functionalized with complementary probe DNAs

147 optical feedback of atomic force microscope cantilevers has been used to modify their response chara

148 polymeric macro- and microscopic systems and cantilevers have been developed to image forces at inter

149 Nanoelectromechanical systems based on cantilevers have consistently set records for sensitivit

150 The novel cantilevered hybrid actuator characterised by light-weig

151 n the literature for the case of an uncoated cantilever in a viscous liquid medium and the case of a

152 scous liquid medium and the case of a coated cantilever in air or in a vacuum.

153 (Mg(1)/(3)Nb(2)/(3))O(3)-32PbTiO(3) (PMN-PT) cantilever in deionized water environment.

154 and coagulation factor VIII captured on the cantilever in the presence of competing stresses from th

155 The cantilevers in MCAs are differentially coated on one sid

156 While the reference cantilevers in the array are functionalized with 6-merca

157 The sensing cantilevers in the array are functionalized with self-as

158 rrays of MCs (different ligands on different cantilevers in the array) are used in conjunction with p

159 Results show that the cantilever-in-mass metamaterial is capable of mitigating

160 constituent material to create a 3D printed cantilever-in-mass metamaterial with negative effective

161 n-mass unit cell model is transformed into a cantilever-in-mass model using the Bernoulli-Euler beam

162 c/mechanical metamaterials is exhibited by a cantilever-in-mass structure as a proposed design for cr

163 An analytical model of the cantilever-in-mass structure is derived and the effects

164 The porous structure of the cantilever increases its thermomechanical sensitivity as

165 locally perturbed by atomic force microscopy cantilever indentation, and distal displacements are mea

166 The sensor uses a cantilevered indicator pin that responds to plate bendin

167 his capability by modifying a 40 x 18 mum(2) cantilever into one terminated with a gold-coated, 4 x 4

168 In the waiting-time protocol, the cantilever is held at a fixed distance above the surface

169 the constant-pulling-velocity protocol, the cantilever is moved at finite velocity away from the sur

170 bration of the atomic force microscope (AFM) cantilever is of fundamental importance for quantifying

171 ction AFM-in which the compliance of the AFM cantilever is removed.

172 a/beta protein, NuG2, by using low-drift AFM cantilevers is demonstrated.

173 rresponding thermal force noise for the best cantilevers is ~5.10(-19) N Hz(-1/2) at millikelvin temp

174 By patterning nanoscale wells onto a cantilever, its surface area is increased by 2 orders of

175 dissipation related to the dithering of the cantilever itself (i.e., to the change of boundary condi

176 included splinting implants together with no cantilever load, restoring the patient with a mutually p

177 nically and inductively, indicating that the cantilever magnet is not an appreciable source of spin-l

178 We present cantilever magnetometry measurements performed on mesosc

179 Unlike conventional cantilever mass sensors, our sensors retain a uniform ma

180 kely are elevated by a non-thermal, flexural cantilever mechanism which is perhaps the most clearly e

181 The direction and amplitude of motor-induced cantilever motion was tuneable via control of buffer pH

182 Validation of the developed cantilever nanosensor was performed in air with dip-and-

183 g membrane-coated silica spheres attached to cantilevers of an atomic-force microscope.

184 e of state-of-the-art single-crystal silicon cantilevers of similar dimensions by roughly an order of

185 xtures are demonstrated across the RP-coated cantilevers of the array.

186 is fabricated from a single-crystal silicon cantilever on a transmission electron microscope grid by

187 The cantilevers on the MC array were differentially coated o

188 hored piezoelectric excited millimeter-sized cantilever (PAPEMC) sensor with a sensing area of 1.5 mm

189 oated piezoelectric-excited millimeter-sized cantilever (PEMC) sensor of 6-mm2 sensing area was fabri

190 Piezoelectric-excited, millimeter-sized cantilever (PEMC) sensors having high-mode resonance nea

191 sing piezoelectric-excited, millimeter-sized cantilever (PEMC) sensors.

192 elaxation times (T (1)) as short as a single cantilever period.

193 A reference, uncoated cantilever permitted reliable subtraction of background

194 The reported peptide-based cantilever platform represents a new analytical approach

195 cer cells in conjunction with nanomechanical cantilever platform.

196 e detected as nanometer-scale movements of a cantilever positioned on top of the neurohypophysis.

197 cells were plated onto arrays of deformable cantilever posts for 2-24 h.

198 New cantilever probes for combined scanning electrochemical

199 nt frequency (-Deltaomega(r)) of a classical cantilever provides a sensitive measure of the mass of e

200 e force spectrum that can be probed, and the cantilever recoil after unfolding may mask the presence

201 te whose formation is otherwise prevented by cantilever recoil.

202 designed to compare the time to survival of cantilever resin-bonded fixed partial dentures and conve

203 investigated for both exciting and measuring cantilever resonance in various environments (vacuum, ai

204 Further, the general theory of cantilever resonance is discussed including fluid-struct

205 Similarly, details of dynamic cantilever response at sub-microsecond time scales, high

206 detection and closed loop bias feedback, the cantilever response is down-sampled to a single measurem

207 The theoretical framework relating cantilever response to the viscosity and mass density of

208 Bacterial adsorption inside the cantilever results in changes in the resonance frequency

209 We highlighted this cantilever's biological utility by first resolving a cal

210 MFS data quality is degraded by a commercial cantilever's limited combination of temporal resolution,

211 the deflection sensitivity and subsequently cantilever's spring constant were the main sources of er

212 using white-noise excitation to enhance the cantilever's thermal fluctuations.

213 r frequency shift as a function of field and cantilever-sample separation.

214 trate that the standard resolution limits of cantilever sensing in dynamic mode can be overcome with

215 trated using a novel asymmetrically anchored cantilever sensor and a commercially available antibody.

216 The cantilever sensor detects mass-changes through shifts in

217 The cantilever sensor shows a good linear relationship betwe

218 mprinted polymer (MIP) based micromechanical cantilever sensor system that has high specificity, fast

219 ing to the results obtained, micromechanical cantilever sensor system worked linearly for the concent

220 The cantilever sensor-based microRNA assay provides competit

221 Piezoelectric cantilever sensors are shown to exhibit sensitive and se

222 Current progress on the use of dynamic-mode cantilever sensors for biosensing applications is critic

223 rface Acoustic Wave devices, micro- and nano-cantilever sensors, gene Field Effect Transistors, and n

224 using gold (Au)-coated dynamic piezoelectric cantilever sensors.

225 es include a quartz crystal microbalance and cantilever sensors.

226 otube domains, or layered lamina or multiple cantilevered sheets).

227 rocantilever, the resonance frequency of the cantilever shifts in proportion to the chemical nature o

228 analytes on a functionalized surface of the cantilever shifts the resonant frequency of a SAW-genera

229 ng applications to date with focus given to: cantilever size (milli-, micro-, and nano-cantilevers),

230 nging from approximately 1 kHz to 10 MHz and cantilever size ranging from millimeters to nanometers.

231 obilize membrane receptors on nanomechanical cantilevers so that they can function without passivatin

232 experiments by changing the temperature and cantilever spring constant, and analyzed the results in

233 at different temperatures and with different cantilever spring constants enabled a more effective com

234 bio-bot consisted of a 'biological bimorph' cantilever structure as the actuator to power the bio-bo

235 The cantilever structure was seeded with a sheet of contract

236 evers, surface modification of the glass and cantilever substrates with a DETA SAM, a serum-free medi

237 -based alignment method that repositions the cantilever such that it is located directly above the mo

238 w that the area per receptor molecule on the cantilever surface influences ligand-receptor binding an

239 ajor techniques are employed: fabrication of cantilevers, surface modification of the glass and canti

240 f competing stresses from the top and bottom cantilever surfaces.

241 The deflection of cantilever systems may be performed by an indirect elect

242 iosensor was optimized regarding the type of cantilever, temperature and exchange of media; in combin

243 robe, that uses a micropipette as a flexible cantilever that can aspirate at its tip a bead that is c

244 sing an atomic force microscope (AFM) with a cantilever that was modified with an Aplysia cell adhesi

245 es surface stress that causes bending of the cantilevers that is detected as tip deflection using an

246 nhanced Raman spectra obtained from adjacent cantilevers that were functionalized with different thio

247 o: cantilever size (milli-, micro-, and nano-cantilevers), their geometry, and material used in fabri

248 In the present work, resonant cantilevers, thermally excited in an in-plane flexural m

249 several designs of bio-bots by changing the cantilever thickness.

250 chniques we integrated a microbead on an AFM cantilever thus realizing a system to efficiently positi

251 ents of all cohesins from ScaA with a single cantilever, thus promising improved relative force compa

252 molecules are covalently attached to an AFM cantilever tip and desorbed from hydrophobic self-assemb

253 ce for quantifying the force between the AFM cantilever tip and the sample.

254 ies on the use of antibodies tethered to the cantilever tip of an AFM probe to detect cognate antigen

255 We have created a specially designed cantilever tip that allows these interaction forces to b

256 re the change in thermal fluctuations of the cantilever tip with and without its coupling to a rigid

257 hanges in particle position, relative to the cantilever tip, to determine the electrophoretic mobilit

258 Using cantilever tips with different cross-linker lengths, we

259 rbed molecules using IR radiation causes the cantilever to bend due to temperature changes originatin

260 ria using infrared radiation (IR) causes the cantilever to deflect in proportion to the infrared abso

261 quivocally assign steps in deflection of the cantilever to membrane states during the SNARE-mediated

262 necessary to passivate the underside of the cantilever to prevent unwanted ligand adsorption, and th

263 l is attached to the atomic force microscopy cantilever to quantify the forces that drive cell-cell a

264 We relate the observed deflection of a cantilever to the changes in the surface free energy of

265 upling of the mechanical motion of a diamond cantilever to the spin of an embedded nitrogen-vacancy c

266 The SCPN is stretched by an AFM cantilever to unfold mechanically, which allows measurin

267 ce spectroscopy approach curves with tipless cantilevers to determine the actomyosin cortical tension

268 simple method for fabricating conducting AFM cantilevers to image pore structures at high resolution

269 rray, rather than tips mounted on individual cantilevers, to deliver inks to a surface in a "direct w

270 Cantilever torque magnetometry is used to elucidate the

271 gin of the observed friction domains using a cantilever torsion microscopy in conjunction with angle-

272 liquid-phase sensing applications, resonant cantilever transducers vibrating in their in-plane rathe

273 ies in liquids and indicate the potential of cantilever-type mass-sensitive chemical sensors operatin

274 This translates to apparent cantilever-type stiffness at the tip of the lever of 0.3

275 ine polyethylene nanofiber is deflected by a cantilever under an atomic force microscope.

276 to obtain mechanical vibrations on the PVDF cantilever under small thermal gradient.

277 10(6) times larger than that of traditional cantilever using planar surfaces.

278 Liquid-phase operation of resonant cantilevers vibrating in an out-of-plane flexural mode h

279 ith relatively high quality factors, such as cantilevers vibrating in vacuum, can show characteristic

280 Nanomechanical cantilever vibration is driven by photothermal excitatio

281 Detection of 127 MHz cantilever vibrations is demonstrated with a thermomecha

282 A micron-sized cantilever was used to extract membrane tethers from cel

283 onolayer binding of the MIP nanoparticles on cantilevers was provided by EDC/NHS activation.

284 y binds to SK channels, to the tip of an AFM cantilever, we are able to detect binding events between

285 On an eight-cantilever array chip, four cantilevers were coated with binding peptide (NHFLPKV-GG

286 ad zirconate titanate (PZT) millimeter-sized cantilevers were designed with two types of anchor asymm

287 These cantilevers were fabricated using a two-step anodization

288 For experiments, tipless AFM cantilevers were functionalized with PMMA microspheres a

289 hnique, where latex beads affixed on silicon cantilevers were used as the force transducer, we extrac

290 Free-standing cantilevers, which directly translate specific biochemic

291 g for the static behavior of rectangular AFM cantilevers, which reveals that the three-dimensional ef

292 resented antigenic stimulation using the AFM cantilever while simultaneously imaging with optical mic

293 By using a custom-fabricated cantilever with a 4 microm-diameter nickel tip, we achie

294 these cells when indented by an atomic force cantilever with a pyramidal tip, is also very sensitive

295 atomic force microscope uses a force-sensing cantilever with a sharp tip to measure the topography an

296 A cantilever with an attached microsphere is forced to osc

297 success rates, especially when designed as a cantilever with only 1 retainer.

298 Recently, we modified commercial cantilevers with a focused ion beam to optimize their pr

299 nical measurements of single-crystal diamond cantilevers with thickness down to 85 nm, thickness unif

300 on indirect oscillation of soft, nonmagnetic cantilevers, with spring constants <1 N m(-1).