ライフサイエンスコーパス: biological tissue

1 ectral region of the "transparency window of biological tissues".

2 of two-photon excited fluorescence (TPEF) in biological tissue.

3 s, amides, triazine, imidazole, protein, and biological tissue.

4 ue three-dimensional image reconstruction of biological tissue.

5 ies observed from amino groups but none from biological tissue.

6 ey role in characterizing soft media such as biological tissue.

7 th diffusion, convection and reaction in the biological tissue.

8 ivery device and the subsequent transport in biological tissue.

9 ly improves quantitative imaging accuracy in biological tissue.

10 load for self-healing hydrogels or repair of biological tissue.

11 formal wrapping around 3D objects, including biological tissue.

12 h while retaining high spatial resolution in biological tissue.

13 be used to quantify important properties of biological tissue.

14 use the NIR light penetrated effectively the biological tissue.

15 ds (GNRs) that are weakly constrained by the biological tissue.

16 ation of structures close in architecture to biological tissue.

17 s significantly reducing photo damage to the biological tissue.

18 a 3D rendered image of stained and embedded biological tissue.

19 processes and the spatial organization of a biological tissue.

20 ption, autofluorescence, and scattering from biological tissue.

21 release to the surrounding porous medium or biological tissue.

22 lied when the laser light propagates through biological tissue.

23 in a sample that is placed behind a slice of biological tissue.

24 imaging 14C-labelled tracers in sections of biological tissue.

25 ogies to slices that originate from the same biological tissue.

26 color recovery retrieves absolute colors of biological tissue.

27 sses deep penetration and high resolution in biological tissue.

28 o predict the disease status of the examined biological tissue.

29 monitor changes in the water content within biological tissues.

30 with high spatial and temporal resolution in biological tissues.

31 of multiply charged lipids and proteins from biological tissues.

32 monstrated for the analysis of collagen-rich biological tissues.

33 ion of an elevated water content deep within biological tissues.

34 ms, and absorb light that penetrates through biological tissues.

35 echanical forces are generated and sensed in biological tissues.

36 trometry (DESI-MS) with a stable dication on biological tissues.

37 embedded in opaque scattering layers such as biological tissues.

38 hibits excellent light-guiding efficiency in biological tissues.

39 he more interesting as they make most of the biological tissues.

40 ced scattering of photons traversing through biological tissues.

41 tion is fundamentally incompatible with soft biological tissues.

42 sophisticated thermal modeling with complex biological tissues.

43 eds of microns beneath the surfaces of large biological tissues.

44 -signal and low-background labeling of thick biological tissues.

45 nd point objects, which often occurs in many biological tissues.

46 for in-situ extracellular ATP measurement in biological tissues.

47 dy of the distribution of small molecules on biological tissues.

48 ailed assessment of structural morphology in biological tissues.

49 ed cell phone radiation in aqueous media and biological tissues.

50 k fracture that can optimize the strength of biological tissues.

51 ly applied to oligosaccharide pools in other biological tissues.

52 fluorescent probes in the context of living biological tissues.

53 ce and second-harmonic generation imaging of biological tissues.

54 ng electron microscopy (FIB/SEM)' applied to biological tissues.

55 ous in porous media, composite materials and biological tissues.

56 nanoparticles in the extracellular matrix of biological tissues.

57 suited for biofluid analysis and imaging of biological tissues.

58 ations concerning their effects and fates in biological tissues.

59 drug and metabolite detection directly from biological tissues.

60 k-fabricated for applying shearing forces to biological tissues.

61 optical absorption contrast in subcutaneous biological tissues.

62 blue wavelengths are strongly attenuated in biological tissues.

63 arises in complex or turbid samples such as biological tissues.

64 lar signals secreted from a large variety of biological tissues.

65 the absorption and scattering properties of biological tissues.

66 and sensitive tool for the mapping of PLs in biological tissues.

67 sting membrane potential and excitability of biological tissues.

68 uman oesophagus resemble those of other soft biological tissues.

69 nation of acrolein metabolically produced in biological tissues.

70 iled resolution imaging of highly scattering biological tissues.

71 n used extensively to study and characterize biological tissues.

72 in unraveling the bioinorganic chemistry of biological tissues.

73 nal (3D) spatial mapping of free radicals in biological tissues.

74 plied successfully to microscale analysis of biological tissues.

75 of endothelial function and vascular tone in biological tissues.

76 is booming and becoming more integrated with biological tissues.

77 e imaging and strain calculation within soft biological tissues.

78 ile platform for understanding and mimicking biological tissues.

79 es influence the development and behavior of biological tissues.

80 where light penetration depth is limited in biological tissues.

81 ric current dispersion by different types of biological tissues.

82 le in vivo and real-time surface analyses of biological tissues.

83 scale imaging of protein molecules in intact biological tissues.

84 tworks and 2D and 3D vertex models for dense biological tissues.

85 s and scaffolds for targeted interfaces with biological tissues.

86 rstanding biochemical processes occurring in biological tissues.

87 eporter molecules can monitor pH at depth in biological tissues.

88 to probe deeply through turbid media such as biological tissues.

89 vel by measuring random movement of water in biological tissues.

90 behind the linear, electrical properties of biological tissues.

91 rly those operating in the optical window in biological tissues.

92 predicting the scattering properties of many biological tissues.

93 tial for characterization of a wide range of biological tissues.

94 aterials and probing their interactions with biological tissues.

95 terials, from complex formulated products to biological tissues.

96 ents the random bending of light that clouds biological tissues.

97 of porous media [8, 9], and the invasion of biological tissues [10-12].

98 tration depth through various media, notably biological tissue(4).

99 trate the ability of the approach to analyze biological tissue, a monolayer of onion epidermis was im

100 of the DNA methylation-based biomarkers for biological tissue age and the construction of various ep

101 tems that mimic the function or mechanism of biological tissues, agents, and behaviors.

102 tials (APs) pass largely unperturbed through biological tissue, allowing magnetic measurements of AP

103 become an important tool for 2D profiling of biological tissues, allowing for the visualization of in

104 n by forward-peaked scattering media such as biological tissue and cells.

105 hree-dimensional tomographic imaging of soft biological tissue and other specimens whose details exhi

106 rals yields localized inorganic adhesion for biological tissue and reversible focal encapsulation for

107 ging because of the high scatter of light in biological tissue and the ill-posed nature of the recons

108 The molecular complexity of biological tissue and the spatial and temporal variation

109 e sensitive and accurate analysis of complex biological tissue and tumor samples by comparison of lig

110 ry supplements, pharmaceutical formulations, biological tissues and body fluid.

111 nge of length scales: from nanometers, as in biological tissues and bundles of carbon nanotubes, to m

112 ge of the high native optical contrast among biological tissues and can treat microvessels without ca

113 enabled the in situ and in vivo analysis of biological tissues and cells.

114 the inherent light-scattering properties of biological tissues and cells.

115 second harmonic generation (SHG) imaging of biological tissues and demonstrate its utility for monit

116 mple, and rapid analyses from highly complex biological tissues and fluids.

117 networked materials that are similar to soft biological tissues and have highly variable mechanical p

118 to the understanding of piezoelectricity in biological tissues and its building blocks.

119 maging and depth profiling of metabolites in biological tissues and live organisms.

120 -sensor pairs laminated on a variety of soft biological tissues and organ systems in animal models pr

121 Mechanical assessment of soft biological tissues and organs has broad relevance in cli

122 surgeons to molecularly target a variety of biological tissues and processes.

123 issimilarities between soft, wet, and living biological tissues and rigid, dry, and synthetic electro

124 al domain, of probing bulk media, to imaging biological tissues and single cells at the micro scale,

125 al deformability allow intimate contact with biological tissues and solution-processable printing tec

126 s for structure-function characterization of biological tissues and their cellular inhabitants, seaml

127 dict the local mechanical environment within biological tissues and to investigate the relationship b

128 nic interfaces, due to their similarities to biological tissues and versatility in electrical, mechan

129 that is compatible with the transparency of biological tissues and with the emission of low-cost sem

130 Mechanical properties of biological tissues and, above all, their solid or fluid

131 demonstrate in-vivo feasibility using simple biological tissue) and human heads (to demonstrate feasi

132 Cellular structures also occur in biological tissue, and in magnetic, ferroelectric and co

133 mic response of 3D printed phantoms, ex vivo biological tissue, and in vivo mouse and rat models of c

134 A reflecting metal plate was placed within biological tissue, and the point spread function (PSF) w

135 se combinations are, however, commonplace in biological tissues, and are therefore needed for applica

136 driven complex fluids, active metamaterials, biological tissues, and collections of robots or organis

137 Synthetic materials lack the complexity of biological tissues, and man-made materials that respond

138 netration into bulk materials, in particular biological tissues, and reduced radiation damage due to

139 e, which can modify delicate specimens, like biological tissues, and ultimately destroy the transduce

140 composition, and classification accuracy for biological tissues are considered.

141 ions of high-frequency radio waves (RF) with biological tissues are currently being investigated as a

142 The characteristics of biological tissues are determined by the interactions of

143 d delivery of light to targeted locations in biological tissues are essential to neuroscience researc

144 The mechanical properties of soft biological tissues are essential to their physiological

145 Phantoms of biological tissues are materials that mimic the properti

146 It has been shown that human skin and other biological tissues are memristors.

147 in the region of the optical spectrum, where biological tissues are most transparent: as a result, up

148 Biological tissues are multiresponsive and functional, a

149 g's modulus (YM) and Poisson's ratio (PR) in biological tissues are often early indicators of the ons

150 Biological tissues are rarely transparent, presenting ma

151 nmental matrices (water, soil, sediment, and biological tissues) are needed to address concerns about

152 derivative viscoelasticity observed in some biological tissue arises as a mechanical consequence of

153 to low concentrations in the environment and biological tissues as well as the complexity of the samp

154 Low-energy UVA waves penetrate further into biological tissue, as compared to UVB, UVC and ionizing

155 experimental protocols for STFN measures on biological tissues, as well as optimized device design f

156 ssues at an unprecedented depth of 2.5 mm in biological tissues at a lateral resolution of 36 mumx52

157 e spatially targeted molecular assessment of biological tissues at cellular resolutions.

158 acquiring high-quality HR-MAS NMR spectra of biological tissues at low spinning rates (down to a few

159 ld be the most dominant HBCD diastereomer in biological tissues because it was metabolized to the low

160 electrophysiological studies of a variety of biological tissues both in vitro and ex vivo.

161 In the analysis of biological tissue by imaging mass spectrometry (IMS), th

162 h degree of scattering of optical photons in biological tissue by making use of the photoacoustic eff

163 thods can facilitate deep optical imaging in biological tissue by reducing light scattering and this

164 -resolution fluorescence imaging deep inside biological tissues by digitally time-reversing ultrasoun

165 accurate determination of energy transfer in biological tissues by lifetime measurements of sensitize

166 Volumetric images of biological tissues can be formed by two-dimensional rast

167 ring and absorption limit the depth at which biological tissues can be imaged with light.

168 ficial imaging depth as random scattering in biological tissues causes exponential attenuation of the

169 A typical NIR spectroscopy workflow for biological tissue characterization involves sample prepa

170 Biological tissues contain micrometer-scale gaps and por

171 Biological tissues contain variable amounts of unlabeled

172 trated as is the ability to obtain ions from biological tissue, currency, and other objects placed in

173 nterpreting the collective behaviors of some biological tissues, cytoskeletal systems and collections

174 Macroscopic properties and shapes of biological tissues depend on the remodeling of cell-cell

175 These include synthetic replacements for biological tissues, designing materials for specific med

176 abling deep-tissue ultrasensitive imaging of biological tissues, disease biomarkers and physiological

177 nformation is often inaccessible at depth in biological tissue, due to the highly scattering nature o

178 Conventional analyses of these biological tissues employ liquid chromatography (LC) wit

179 firmly yet gently attach to an inorganic or biological tissue enabling enclosure of, for example, ne

180 pic fine structure information directly from biological tissues, enabling the rapid assignment of mol

181 fluoroethylene) (PTFE), stainless steel, and biological tissues, even without any chemical reaction.

182 plications of light in medicine because many biological tissues exhibit a layered structure of indepe

183 Biological tissues exhibit complex spatial heterogeneity

184 e constituting the cytoskeleton of a cell or biological tissue, exhibit a nonlinear strain-stiffening

185 associated with the physiological status of biological tissue, existing high-resolution optical imag

186 cal models used for studying the response of biological tissues exposed to electric fields.

187 ation (LAESI), the native water molecules in biological tissues facilitate sampling by a focused mid-

188 which the dictation forms a stable bond with biological tissue fatty acids and lipids.

189 sity) may be most specifically adapted among biological tissues for high rate and complexity of infor

190 rovide a promising electrical interface with biological tissues for sensing and stimulation, owing to

191 ze metallic ENPs in environmentally relevant biological tissues for the first time.

192 can perform multiscale structural imaging of biological tissues, from nanometres to micrometres.

193 mapping of metabolites directly onto intact biological tissues, giving a spatial context to metaboli

194 Metabolic fingerprinting of biological tissues has become an important area of resea

195 Consequently, their analysis in biological tissues has received increased attention.

196 However, limited light penetration into most biological tissues have so far prevented its widespread

197 Biological tissues have the remarkable ability to remode

198 nsor to measure extracellular ATP content in biological tissues (i.e., porcine intervertebral disc).

199 ear electrical properties of the underlying (biological) tissue; if it is done with an alternating cu

200 r electromagnetic radiation in reacting with biological tissues, (ii) nanostructured metamaterial (Au

201 s detection, natural products discovery, and biological tissue imaging, among other applications.

202 food water activity by the immersion of the biological tissue in hypertonic solutions.

203 rated endogenous field-dependant contrast in biological tissues in good agreement with reference data

204 d laser (PIRL) is capable of cutting through biological tissues in the absence of significant thermal

205 Ferritin protein is involved in biological tissues in the storage and management of iron

206 ly targeting, imaging, and treating specific biological tissues in vivo.

207 Articular cartilage is one of several biological tissues in which swelling effects are importa

208 tection of trace amounts of nanoparticles in biological tissues, in which MRI provides volume detecti

209 lices, is the primary building block of many biological tissues including bone, tendon, cartilage, an

210 method for chemical transformation of intact biological tissues into a hydrogel-tissue hybrid, which

211 isodesmosine as biomarkers in many types of biological tissues involving elastin degradation.

212 l transmission through complex media such as biological tissue is fundamentally limited by multiple l

213 The growth of several biological tissues is known to be controlled in part by

214 Visualizing structures deep inside opaque biological tissues is one of the central challenges in b

215 Delta(199)Hg in marine biological tissues is thought to reflect marine Hg photo

216 esion to wet and dynamic surfaces, including biological tissues, is important in many fields but has

217 This extrinsic control is superimposed by a biological, tissue-level control; tissue-specific chemic

218 surements of NO and CO generated from living biological tissue (mouse, c57, kidney) surfaces, for the

219 corresponded to a limit of quantification in biological tissue of 10 pmol/g for all analytes except 2

220 In the biological tissues of numerous animal and plant species,

221 ation with the soft, curvilinear surfaces of biological tissues offer important opportunities for dia

222 se of ICP-MS to measure metal ion content in biological tissues offers a highly sensitive means to st

223 Compound extraction from biological tissue often presents a challenge for the bio

224 ategory of soft glassy substances, including biological tissue, often exhibit a mechanical complex mo

225 lambdaem = 804 nm), which are much above the biological tissue opaque window (400-700 nm) ensuring be

226 trastructure in the mechanical response of a biological tissue or manufactured material to be studied

227 able new insights into the microstructure of biological tissues or be of great value in diagnostics.

228 ronments, such as porous media, wet soil, or biological tissue, or act as a selection pressure in evo

229 How the collective motion of cells in a biological tissue originates in the behavior of a collec

230 f materials with high water content, such as biological tissues, over large volumes whereas designs w

231 , leads novel and precise communication with biological tissue, particularly with the nervous system.

232 cal analysis of SmicroXRD measurements using biological tissue paves the way for further structural i

233 offers superior optical sectioning deep into biological tissues, permitting analysis of large, hetero

234 ractions of acoustic cavitation bubbles with biological tissues play an important role in biomedical

235 g, the dominant light interaction process in biological tissues, prevents tissues from being transpar

236 Current advances in staining and imaging of biological tissues provide a wealth of data, but there a

237 n can help circumvent complex extractions of biological tissues, provide more accurate information on

238 Imaging of nanomaterials in biological tissues provides vital information for the de

239 In biological tissues, radiation causes the formation of re

240 ogical abnormalities in epithelial and other biological tissues, raising novel predictions for future

241 reveal detailed angiographic information in biological tissues ranging from the rodent brain to the

242 s and quantitation of their concentration in biological tissue remain challenging tasks in microscopy

243 icroscopy now allow imaging of cleared large biological tissue samples and enable the 3D appreciation

244 In this work, DESI DM-MSI experiments on biological tissue samples such as sea algae and mouse br

245 at allows for the study of the complexity of biological tissue samples to overcome the limitations of

246 to investigate the molecular distribution of biological tissue samples.

247 o image metabolites, lipids, and proteins in biological tissue samples.

248 (e.g., polycyclic aromatic hydrocarbons) in biological tissue samples.

249 ument for site-specific chirality mapping of biological tissue samples.

250 nd accurate mechanics measurements of moving biological tissue samples.

251 kDa) from various materials including urine, biological tissue sections, paper, and plant material on

252 ntification of FA isomers from heterogeneous biological tissue sections, yielding spatially resolved

253 have been unmasked and imaged directly from biological tissue sections.

254 ues allow mapping of various analytes within biological tissue sections.

255 istributions of lipids and drug molecules in biological tissue sections.

256 :1 were obtained from the direct analysis of biological tissue sections.

257 ar distributions of elements and proteins in biological tissue sections.

258 uccess in imaging several lipid classes from biological tissue sections.

259 mpare the effectiveness of a laser-activated biological tissue solder with that of standard sutures f

260 er to achieve a comprehensive description of biological tissue, spectral information about proteins,

261 , we use hydrogel-based substrata matched to biological tissue stiffness to investigate the effects o

262 holds great promise for the in vivo study of biological tissue structure with substantially improved

263 ber directions in structurally heterogeneous biological tissue substantially contributes to an unders

264 absorption coefficients of many homogeneous biological tissues such as muscle, skin, white matter in

265 permittivity of two-dimensional anisotropic biological tissues such as skeletal muscle using the fou

266 llows clear imaging through extremely turbid biological tissue, such as the skull, over an extended c

267 ly modulate friction with soft materials and biological tissues, such as human fingertips.

268 o control the behavior of in vitro excitable biological tissue, suggesting their potential for clinic

269 hnique enables the study of microrheology of biological tissues that produce or detect sound.

270 Within the biological tissue, the model can account for nonlinear s

271 rtioned among four human groups in a natural biological tissue, the placenta.

272 In the case of living biological tissue, the spatiotemporal patterns formed by

273 labeled Probody molecule is incubated with a biological tissue, thereby enabling its activation by ti

274 port-proteins and cell-cell heterogeneity in biological tissues, these findings generalize across mos

275 In development, cells organize into biological tissues through cell growth, migration, and d

276 ased structures can now be built from within biological tissue to allow subsequent removal of lipids

277 The thermodynamic response of biological tissue to pulsed infrared laser irradiation w

278 nts have incorporated thinner, more flexible biological tissues to streamline safer deployment throug

279 irectly monitor the distribution of drugs in biological tissues, to evaluate the distribution of TAA

280 l processing of porous samples such as fixed biological tissues typically relies on molecular diffusi

281 This investigation into the behavior of biological tissue under high C60(+) fluxes not only allo

282 y techniques for deep subsurface analysis of biological tissues unlocks new prospects for medical dia

283 he quantitative analysis of lipid species in biological tissues using internal standards for each lip

284 icroplastics (NMPs) in water, sediments, and biological tissues using pyrolysis gas chromatography co

285 Intra- and interday precision in biological tissue was routinely approximately 20% or low

286 ive period of infection and in whom surgical biological tissues were cultured (n = 429).

287 Singlet oxygen can severely damage biological tissue, which is exploited in photodynamic th

288 the complex refractive index distribution of biological tissue, which scrambles the incident light an

289 which enabled imaging both fixed and living biological tissue with 3D precision, high-resolution flu

290 We present imaging of biological tissue with a proton microscope.

291 rrying mechanism suitable for stimulation of biological tissue with a safe charge injection limit of

292 eover, we present a first tomography scan of biological tissue with complementary information in atte

293 structural and functional imaging of living biological tissue with label-free, optical absorption co

294 thermal damage generated during treatment of biological tissue with lasers and other sources of heat.

295 Acoustically probing biological tissues with light or sound, photoacoustic an

296 nsive mapping of chemical species throughout biological tissues with typical spatial resolution in th

297 cisely to match the non-linear properties of biological tissues, with application opportunities that

298 ze a variety of semisolid systems, including biological tissues, with virtually no sample preparation

299 tool for purifying metabolites from complex biological tissues would be of obvious utility to the fi

300 ivity, an elastic compliance similar to soft biological tissue (Young's modulus < 100 kPa), and the c