ライフサイエンスコーパス: cantilever

1 tical microscopy and measuring forces on the cantilever.

2 tes from the viscous damping of the dithered cantilever.

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

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

5 of explosive vapors using a nanoporous TiO2 cantilever.

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

7 of a microchanneled atomic force microscopy cantilever.

8 to the protein construct through a compliant cantilever.

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

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

11 = 1 nm) excitation of higher eigenmodes of a cantilever.

12 the two mechanical resonant modes of the AFM cantilever.

13 field and reducing the spring constant of a cantilever.

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

15 ezoelectric polyvinylidene difluoride (PVDF) cantilever.

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

17 limited by the mechanical properties of the cantilever.

18 d using focused-ion-beam-modified ultrashort cantilevers.

19 d and calculated using the deflection of the cantilevers.

20 n artefacts conflict with the use of smaller cantilevers.

21 for accurate calibration of rectangular AFM cantilevers.

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

23 e to those needed for linear carbon nanotube cantilevers.

24 ontrolled attachment of single live cells on cantilevers.

25 e do not cause significant deflection of the cantilevers.

26 ning probe systems that rely on conventional cantilevers.

27 arrays assembled on atomic-force-microscope cantilevers.

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

29 talline diamond film and attached to tipless cantilevers.

30 zation of unspecific protein adsorption onto cantilevers.

31 hybrid nematic liquid crystal network (LCN) cantilevers.

32 at of state-of-the-art piezoelectric bimorph 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 ve fabricated a silicon-compatible thin-film cantilever actuator with a single flexoelectrically acti

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

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

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

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

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

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

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

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

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

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

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

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

49 ow the mechanical resonance frequency of the cantilever and is thus detectable by regular atomic forc

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

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

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

53 The quality factor of the cantilever and the local sample polarizability can be ma

54 energy between a silica colloid glued to AFM cantilever and the studied surfaces increased as the sur

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

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

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

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

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

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

61 bilised on trisNTA-Ni(2+) functionalized AFM cantilevers and the OH and COOH SAM surfaces were predom

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

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

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

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

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

67 The cantilevers are fabricated using a complementary metal o

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

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

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

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

72 ar concentrations based on a microfabricated cantilever array.

73 vices, silicon dioxide surface-micromachined cantilever arrays and zinc oxide surface-microfabricated

74 Cantilever arrays have been used to monitor biochemical

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

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

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

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

79 e lipid bilayer, typically by retracting the cantilever at a constant velocity.

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

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

82 This article aims to propose a cantilever based cooling device employing non-axis symme

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

84 Cantilevers based on polycrystalline diamond surfaces ar

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

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

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

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

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

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

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

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

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

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

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

96 The cantilevers' beating prevents the initial stage of bacte

97 erimentally determined data obtained via the cantilever bending method.

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

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

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

101 onditions), and retraction speeds of the AFM cantilever, could not be described in terms of the stand

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

103 ach is to maintain a zero amplitude harmonic cantilever deflection by CL control of a subsample piezo

104 Instead of the usual mode of recording cantilever deflection driven by sample expansion, the pr

105 -120 and -40 mV resulted in a linear upward cantilever deflection equivalent to an increase in membr

106 is of the quasi-steady state response of the cantilever deflection in terms of Fourier analysis.

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

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

109 mposition of the initial oscillations of the cantilever deflection when an impulsive excitation is gi

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

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

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

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

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

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

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

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

118 A conductive transparent cantilever electrically contacts individual nanoparticle

119 uring the maximum deflection of the actuated cantilever electrode.

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

121 Cantilever-enhanced photoacoustic spectroscopy coupled w

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

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

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

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

126 can be further improved about ~2 K (using 10 cantilevers) for a starting temperature of 358 K.

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

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

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

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

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

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

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

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

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

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

137 Retraction of a pDA-coated cantilever from an oxide surface shows the characteristi

138 array (MEA) were simultaneously probed with cantilever from atomic force microscope (AFM) system.

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

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

141 demonstrate that remotely actuated magnetic cantilevers grafted on a substrate act efficiently in pr

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

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

144 The novel cantilevered hybrid actuator characterised by light-weig

145 To overcome these issues, we moved the cantilever in a sawtooth pattern of 6-12 nm, offset by 0

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

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

148 citation of the resonance spectrum of an AFM cantilever in contact with the sample.

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

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

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

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

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

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

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

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

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

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

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

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

161 Here, by coupling an atomic force microscopy cantilever into a solid open-cell set-up in environmenta

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

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

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

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

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

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

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

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

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

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

172 We present cantilever magnetometry measurements performed on mesosc

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

174 chanical heterodyne signal detection between cantilever mechanical resonant oscillations and the phot

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

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

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

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

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

180 The cantilevers on the MC array were differentially coated o

181 hree amino acids, respectively, when using a cantilever optimized for 2 mus resolution.

182 he photothermal expansion mixes with the AFM cantilever oscillation to provide the PiFM signal.

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

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

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

186 A reference, uncoated cantilever permitted reliable subtraction of background

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

188 cer cells in conjunction with nanomechanical cantilever platform.

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

190 New cantilever probes for combined scanning electrochemical

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

192 te whose formation is otherwise prevented by cantilever recoil.

193 acteristic behavior in the piezoresponse and cantilever resonance hysteresis loops, which allows for

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

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

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

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

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

199 hanical vibrations produce large stresses in cantilevers resulting in elastocaloric effect associated

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

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

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

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

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

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

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

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

208 The cantilever sensor detects mass-changes through shifts in

209 The cantilever sensor shows a good linear relationship betwe

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

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

212 The cantilever sensor-based microRNA assay provides competit

213 Piezoelectric cantilever sensors are shown to exhibit sensitive and se

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

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

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

217 es include a quartz crystal microbalance and cantilever sensors.

218 A proof-of-concept material in a cantilever setup is used to show morphing, and analytica

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

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

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

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

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

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

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

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

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

228 The cantilever structure was seeded with a sheet of contract

229 By using the cantilever-structured AlGaN/AlN/GaN-based high electron

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

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

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

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

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

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

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

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

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

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

240 often disregarded transient response of the cantilever through a relatively modern mathematical tool

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

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

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

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

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

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

247 Using an AFM cantilever tip, mechanically compliant acicular microcry

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

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

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

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

252 -sized droplet to an atomic force microscope cantilever to directly measure adhesion and friction for

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

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

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

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

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

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

259 Further, design allows cascading of several cantilevers to achieve large cooling response.

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

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

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

263 zed to spatially and spectrally map multiple cantilevers, to isolate and record beam deflection from

264 Cantilever torque magnetometry is used to elucidate the

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

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

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

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

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

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

271 10(6) times larger than that of traditional cantilever using planar surfaces.

272 e and record beam deflection from individual cantilevers using distinct wavelength selection.

273 en developed to predict the amplitude of the cantilevers vertical deflection.

274 nating magnetic field, the flexible magnetic cantilevers vertically deflect from their initial positi

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

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

277 Nanomechanical cantilever vibration is driven by photothermal excitatio

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

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

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

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

282 (<<1 angstrom) at high frequency, and stiff cantilevers, we show how modulated nano/ angstrom-indent

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

284 These cantilevers were fabricated using a two-step anodization

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

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

287 o the reduction of resonant frequency of the cantilevers, whereas an increase in resistance has been

288 elated to the energy lost in the oscillating cantilever, which is a direct consequence of a molecule

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

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

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

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

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

294 from a cell inside a fluid-filled vibrating cantilever with a temporal resolution of < 1 min.

295 A cantilever with an attached microsphere is forced to osc

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

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

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

299 consisted of an array of four piezoelectric cantilevers with varying lengths to enhance sensitivity

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