ライフサイエンスコーパス: diamond

1 tions of adjective-noun phrases (e.g., "dark diamond").

2 d in the diet-induced animal model of NAFLD (DIAMOND).

3 iclase that is commonly trapped in superdeep diamond.

4 f both properties challenging, especially in diamond.

5 sation of solid-state quantum photonics with diamond.

6 system of 27 coupled (13)C nuclear spins in diamond.

7 e to the hardness and chemical resistance of diamond.

8 chemical inertness, and biocompatibility of diamond.

9 rs realized with nitrogen vacancy centres in diamond.

10 been little research into such approaches in diamond.

11 m it into fluids, magmas, volcanic gases and diamonds.

12 one of the most important sources of natural diamonds.

13 led into the deep mantle to potentially form diamonds.

14 influence spectators to choose the three of diamonds.

15 nts benefitted from the emergent features of Diamonds.

16 re identified better than Xs when flanked by Diamonds.

17 ilized and concentrated to form lower-mantle diamonds.

18 toughness up to five times that of synthetic diamond(10), even greater than that of magnesium alloys.

19 hbour particles, which is required for cubic diamond(15,17).

20 regions related by symmetry - also toughens diamond(2).

21 return missions or inclusions in deep Earth diamonds, a nondestructive method is preferred.

22 We then use the DIseAse Module Detection (DIAMOnD) algorithm to expand the proto-modules into comp

23 erstanding of nitrogen-containing defects in diamond-alone and in association with vacancies, hydroge

24 alysis of human fecal microbiomes when using DIAMOND, an alignment tool that is up to 20,000 times fa

25 specific strengths surpassing those of bulk diamond and average performance improvements up to 639%

26 Formula: see text] for both room temperature diamond and heated diamond to 500 K.

27 rogen and phosphorus-doped (semi-conducting) diamond and hydrogen-terminated undoped diamond electrod

28 search driven by the prospects of harnessing diamond and its colour centres as suitable hardware for

29 ultralarge elastic deformation in nanoscale diamond and machine learning of its electronic and phono

30 ut only internally generated noise, only the diamond and not the FFL evolves.

31 The coexistence of large monocrystalline diamonds and nanodiamonds in a highly shocked ureilite c

32 hydrous ringwoodite and ice VII in superdeep diamonds and the relatively low water content in bulk MT

33 Diamonds and their inclusions are unique fragments of de

34 acent chevrons either pointing in opposite ('Diamonds' and 'Xs'), or the same (both up or down) direc

35 ngle- and double-network versions of gyroid, diamond, and "plumber's nightmare".

36 l of nitrogen incorporation in the resulting diamond, and how the diamond produced by either method c

37 g electrochemical oxidation at a boron-doped diamond anode with a low potential for the generation of

38 e lower than reported values for boron-doped diamond anodes.

39 (2)O hydrate, based on Raman spectroscopy in diamond anvil cell and ab initio molecular dynamics simu

40 ) Br(5) ; pressure-dependent Raman-PL with a diamond anvil cell as a dynamic probe further rules out

41 ) via direct reactions between elements in a diamond anvil cell at pressures exceeding 100 GPa is rep

42 a reaction between rhenium and nitrogen in a diamond anvil cell at pressures from 40 to 90 GPa and is

43 mples of various average grain sizes using a diamond anvil cell coupled with radial X-ray diffraction

44 ide CeH(9) at 80-100 GPa in the laser-heated diamond anvil cell coupled with synchrotron X-ray diffra

45 Here we report diamond anvil cell experiments that identify the followi

46 ique, and then integrated into a 500 um size diamond anvil cell for high-pressure studies.

47 spectroscopies, measured up to 2.1 GPa in a diamond anvil cell on single crystals, are in excellent

48 ze this rare compound under compression in a diamond anvil cell with laser heating.

49 g experiments of Nb and Ta in a laser-heated diamond anvil cell, at pressure and temperature conditio

50 observed over a broad pressure range in the diamond anvil cell, from 140 to 275 gigapascals, with a

51 Using a diamond anvil cell, monocrystalline (TaSe(4) )(2) I is c

52 e partitioning experiments in a laser-heated diamond anvil cell, we show that carbon becomes signific

53 X-ray powder diffraction of samples within a diamond anvil cell.

54 X-ray diffraction using a resistively heated diamond anvil cell.

55 rees C at approximately 1 GPa pressure using diamond anvil cells (DACs) with heating capabilities.

56 amorphous silicates compressed statically in diamond anvil cells (up to 157 GPa at room temperature)

57 High-pressure synthesis in diamond anvil cells can yield unique compounds with adva

58 ossbauer source spectroscopy in laser-heated diamond anvil cells to investigate the magnetic transiti

59 ts up to 105.2 GPa at room temperature using diamond anvil cells.

60 the temperature plateau seen in laser-heated diamond-anvil cell (DAC) experiments at temperatures hig

61 40 GPa through a combination of laser-heated diamond-anvil cell experiments and first-principles mole

62 large-volume devices and in one laser-heated diamond-anvil cells experiment, in which the speckle met

63 ynchrotron X-ray diffraction in laser-heated diamond-anvil cells, and theoretically, using ab initio

64 achieved by sandwiching a sample between two diamond anvils and using a ramped laser pulse to slowly

65 NV) color centers directly into the culet of diamond anvils.

66 An ever-growing fraction of the supply of diamond appearing on the world market is now lab-grown.

67 and future research directions of conductive diamond are discussed and outlined.

68 Nitrogen-vacancy (NV) quantum defects in diamond are sensitive detectors of magnetic fields.

69 hat among wide band gap materials 4H-SiC and diamond are two optimal semiconductors due to the combin

70 Diamond as a chemically inert material allows treatment

71 inciples by which individual concepts (e.g., diamond, baseball) combine into more complex phrases (e.

72 ction and found to be triply interpenetrated diamond-based dia topology.

73 chemical vapour deposition to produce 'black diamond' (bD) nanostructures.

74 an sp(2)-bonded carbon microspot boron doped diamond (BDD) electrode for voltammetric measurement of

75 anisms for biofouling control at boron-doped diamond (BDD) electrode surfaces polarized at low applie

76 ones, directly integrated into a boron-doped diamond (BDD) electrode, is investigated.

77 ndows of polished and unpolished boron doped diamond (BDD) electrodes with hydrogen and oxygen termin

78 We investigated fragments of three diamond-bearing ureilites (two from the Almahata Sitta p

79 ap transitions can be achieved reversibly in diamond below threshold strain levels for phonon instabi

80 Diamond Blackfan Anemia (DBA) is a congenital bone marro

81 linical use of steroids for the treatment of Diamond Blackfan anemia (DBA), the mechanisms through wh

82 present the case of a 34-year-old woman with Diamond-Blackfan anaemia (DBA).

83 Diamond-Blackfan anemia (DBA) is a congenital erythrobla

84 Diamond-Blackfan anemia (DBA) was the first ribosomopath

85 riants in ribosomal protein (RP) genes drive Diamond-Blackfan anemia (DBA), a bone marrow failure syn

86 proteins have thus far been associated with Diamond-Blackfan anemia, a rare inherited bone marrow fa

87 ratosis congenita), and ribosome biogenesis (Diamond-Blackfan anemia, Shwachman-Diamond syndrome).

88 In contrast to observations from Diamond-Blackfan anemia, we detected no evidence of sign

89 quitous in both natural and laboratory-grown diamond, but the number and nature of the nitrogen-conta

90 hically precise patterning of large areas of diamond by self-assembled masks and their release into u

91 The hardness of diamond can be increased through nanostructuring strateg

92 th retracted sticky patches, colloidal cubic diamond can be self-assembled using patch-patch adhesion

93 e into more complex phrases (e.g., "baseball diamond") can illuminate not only how the brain combines

94 Inclusion-free diamonds cannot provide information on depth of formatio

95 ance while protecting the top surface of the diamond channel from dry etch damage.

96 trument is based on a commercially available diamond chip, into which an NV ensemble is ion-implanted

97 re, we present a protocol for fabricating NV diamond chips and for constructing and operating a simpl

98 bo-current is generated by sliding an N-type diamond coated tip on a P-type or N-type Si wafers.

99 ) probes for force spectroscopy using robust diamond-coated spheres, i.e., colloidal particles.

100 We found superior performance with all Diamonds compared to all Xs, indicating that display uni

101 report the structural characterization of a diamond composite hierarchically assembled with coherent

102 Neoproterozoic West African diamonds contain sulfide inclusions with mass-independen

103 aces at around 50% of the value for the flat diamond control.

104 reported as a bis-mu-oxo Fe(IV)(2)(mu-O)(2) diamond core but was recently described to have an open

105 eported a high-valent Co(III,IV)(2)(mu-O)(2) diamond core complex (1) that is highly reactive with sp

106 ing 9,10-dihydroanthracene (DHA) compared to diamond core complexes of other first-row transition met

107 Our findings indicate that the diamond core isomerization is likely a practical enzymat

108 culations showed that both species possess a diamond core structure with a short Co...Co distance of

109 out that a Q-like intermediate (high-valent diamond-core bis-mu-oxo-[Fe(IV)](2) unit) is involved in

110 ical system of [Formula: see text] nuclei in diamond coupled to Nitrogen Vacancy (NV) centers over a

111 d DNP using nitrogen-vacancy (NV) centers in diamond coupled to substitutional nitrogen impurities, t

112 -assembling colloidal particles in the cubic diamond crystal structure could potentially be used to m

113 polarize target samples in contact with the diamond crystal.

114 In addition, the bandgap in diamond crystals appears at a refractive index contrast

115 he formation of "large" (as opposed to nano) diamond crystals could have been enhanced by the catalyt

116 The first single-diamond cubic phase in a liquid crystal is reported.

117 anocrystals show stability with the alpha-Sn diamond cubic structure.

118 wer-mantle mineral inclusions and their host diamonds (deeper than 660 kilometres) have a narrow rang

119 ime characterizes mesoscopic quantum dot and diamond defect systems, as we see no numerical tendency

120 Recently however, an entire suite of other diamond defects has emerged-group IV colour centres-name

121 ues for engineering and characterizing these diamond defects, discuss the current state-of-the-art gr

122 clusions in sublithospheric, or 'superdeep', diamonds (derived from depths greater than 250 kilometre

123 ion methods and fabricate compact and robust diamond devices with unique specifications.

124 This is the first report on the coating of diamond dicing blades with metallic glass (MG) coating t

125 Diamond electrochemical devices utilizing micro-scale, u

126 wo different type of electrodes, boron-doped diamond electrode (BDD) and boron-doped carbon nanowalls

127 relative electrochemical window from various diamond electrode types from reported results.

128 ing) diamond and hydrogen-terminated undoped diamond electrodes.

129 in properties of nitrogen-vacancy defects in diamond enable diverse applications in quantum computing

130 g from a multistage process that starts from diamond encapsulation of ferropericlase followed by deco

131 age etched surface roughness of 0.47 nm at a diamond etch rate of 45 nm/min and 16.9:1 selectivity.

132 rospheres were coated with a nanocrystalline diamond film and attached to tipless cantilevers.

133 solvent treatments, whilst pin-holing of the diamond film was observed following RCA-1 treatment.

134 ultra-thin ultra-stiff films, including CVD diamond films (~1000 GPa stiffness), as well as the tran

135 vity to the morphological granularity of the diamond films.

136 on with improved ohmic contacts, will enable diamond FinFETs for various high-power applications.

137 irst time, space charge limited transport in diamond FinFETs with a short channel length was demonstr

138 eived to stand out more strongly from X than Diamond flankers.

139 easured He-Sr-Pb isotope ratios in superdeep diamond fluid inclusions from the transition zone (depth

140 least locally, ultra-depleted at the time of diamond formation, as opposed to the melt-metasomatized,

141 ures >20 GPa in a large planetary body, like diamonds formed deep within Earth's mantle.

142 in the Earth could also provide insight into diamond-forming processes at depth in the planet.

143 In geology, diamond forms as part of the deep carbon cycle and typic

144 ombining a pre-test probability (PTP) model (Diamond-Forrester approach using sex, age, and symptoms)

145 nd 0.71 for [50] and [70], respectively) and Diamond-Forrester risk scores (area under the curve=0.68

146 ficient strain pathways that would transform diamond from an ultrawide-bandgap material to a smaller-

147 magnetite grains from a so-called superdeep diamond from the Earth's mantle.

148 pe measurements of mineral inclusions within diamonds from Kankan, Guinea that are derived from depth

149 Younger diamonds from the Kaapvaal, Zimbabwe, and West African c

150 Here, impact diamonds from the Popigai crater were characterized with

151 grafting of terminal alkenes to surfaces of diamond, glassy carbon, and polymeric carbon dots.

152 superconducting transition was observed for diamond grown on oxygen plasma treated silicon nitride,

153 around 3 billion years ago and reworking and diamond growth around 650 million years ago.

154 face-centred-cubic structures(9,10), because diamond has a much wider bandgap and is less sensitive t

155 hese highly desirable attributes, conductive diamond has found extensive use as an enabling electrode

156 Colour centres in diamond have emerged as leading solid-state 'artificial

157 Quantum spin sensors like the NV center in diamond have long spin lifetimes and their relaxation ca

158 Impact diamonds, however, often exhibit structural disorder in

159 The origin of diamonds in ureilite meteorites is a timely topic in pla

160 mes, which makes it unlikely that any of the diamonds in ureilites formed in bodies as large as Mars

161 by adjective-noun combinations (e.g., "dark diamond") in male and female human subjects.

162 e carbon is hosted in metals, rather than in diamond, in the reduced, volatile-poor lower mantle(2),

163 that the sulfur isotope record in worldwide diamond inclusions is consistent with changes in tectoni

164 Seismic studies and diamond inclusions(6,7) have shown that recycled materia

165 carbon and nitrogen isotope contents of the diamonds, indicate that carbonated igneous oceanic crust

166 , brightness) in a given noun concept (e.g., diamond) influences how the adjective and noun concepts

167 Diamond is a highly attractive coating material as it is

168 Diamond is a material of immense technological importanc

169 apour deposition (CVD) grown nanocrystalline diamond is an attractive material for the fabrication of

170 y charged nitrogen-vacancy (NV(-)) defect in diamond is attracting particular current interest in acc

171 However, self-assembly of colloidal diamond is challenging.

172 , the nitrogen vacancy (NV) colour centre in diamond is one of the leading candidates for such applic

173 Cubic diamond is preferred for these applications over more ea

174 Diamond is the hardest natural material, but its practic

175 In this letter we report a diamond lateral FinFET fabricated using an ohmic regrowt

176 Because particles in a diamond lattice are tetrahedrally coordinated, one appro

177 trated demixing and recrystallization into a diamond lattice, implying the breaking of the original c

178 a diffractive element that can generate the diamond lattice.

179 tothermal vibrational nanoprobe developed at Diamond Light Source (DLS), capable of measuring mid-inf

180 esigned to be tunable to long wavelengths at Diamond Light Source has opened the possibility to nativ

181 Follow-up beamtimes at ESRF and Diamond Light Source using submicro-SR-XRF allowed resol

182 a Ni-Cu test sample recorded at I13-1 of the Diamond Light Source, UK.

183 Lubricity between stainless steel (SS) and diamond-like carbon (DLC) is experimentally demonstrated

184 This work aims to utilize diamond-like carbon (DLC) thin films for bioreceptor imm

185 olid lubricants such as MoS(2), graphite, or diamond-like carbon films demonstrate excellent tribolog

186 turing a unique Ni(2)(OR)(2) (OR = alkoxide) diamond-like core complemented by a mu-iodo bridge betwe

187 In particular, sp(3) bonded, diamond-like materials represent appealing targets becau

188 These diamond-like molecular rods with extraordinarily small t

189 from graphite-like sp(2)-bonded structure to diamond-like sp(3)-bonded structure.

190 (3) -carbon frameworks, and nanothreads with diamond-like structures were synthesized by compressing

191 The laser irradiated spherically curved diamond-like-carbon targets with intensity 4 x 10(18) W/

192 , we applied elastic geothermobarometry to a diamond-magnesiochromite (mchr) host-inclusion pair from

193 ng defects can have a profound effect on the diamond material and its properties.

194 h improvement in ALT and dyslipidemia in the DIAMOND mice.

195 Conductive diamond microcrystalline and nanocrystalline films, stru

196 Interestingly, a 4-node "diamond" motif also emerges as a short spurious signal f

197 hods to overcome constraints of cutting-edge diamond nanofabrication methods and fabricate compact an

198 on (ALD) cycles of zinc oxide onto suspended diamond nanomembranes, strongly reduces the threshold vo

199 le recent experiments have demonstrated that diamond nanoneedles can sustain exceptionally large elas

200 um achievable tensile strain and strength of diamond nanoneedles with various diameters, oriented in

201 tatic self-assembly of a hydrogen-terminated diamond nanoparticle monolayer.

202 We systematically functionalized diamond nanoparticle surfaces with five different cation

203 article, we present phantoms of tissue with diamond nanoparticles dedicated to magnetic resonance ca

204 Furthermore, the use of diamond nanoparticles in phantoms allowed us to tune the

205 fracture occurs, a crack propagates through diamond nanotwins of the 3C (cubic) polytype along {111}

206 The DIAMOND (NCT03227861) study using darunavir/cobicistat/e

207 The DIAMOND (NCT03227861) study using darunavir/cobicistat/e

208 fractures, with local transformation into 3C diamond near the fracture surfaces.

209 The diamond needles were then chemically terminated with H,

210 To exploit the exceptional properties of diamond, new high quality fabrication techniques are nee

211 Nitrogen vacancy (NV) centers in diamond offer an appealing platform because these parama

212 e volcanic rocks that are the source of most diamonds, offer rare insights into aspects of the compos

213 and growth processes for the fabrication of diamond on silicon nitride devices.

214 ters(5), such as quantum dots and defects in diamond or silicon carbide(6-10), have emerged as promis

215 idence that formation of micrometer(s)-sized diamonds or associated Fe-S-P phases in ureilites requir

216 Targets were flanked by Diamonds or Xs, resulting in conditions with different l

217 quantum dots or nitrogen-vacancy centers in diamond, our proposal does not require any photon assist

218 Diamond photonics is an ever-growing field of research d

219 abricate a metasurface composed of nanoscale diamond pillars that acts as an immersion lens to collec

220 hically assembled with coherently interfaced diamond polytypes (different stacking sequences), interw

221 Conductive diamond possesses unique features as compared to other s

222 that makes the present technique suitable to diamond powders and settings where the field is heteroge

223 on disease onset and test frequency from the Diamond Princess cruise ship outbreak, to quantify the c

224 ration in the resulting diamond, and how the diamond produced by either method can be further process

225 However, current diamond quantum optics experiments are restricted to sin

226 The structural characterization of such diamonds remains a challenge.

227 ate spin memory integrated in a nanophotonic diamond resonator(17-19) to implement asynchronous photo

228 l elasticity and Griffith strength limits of diamond, respectively.

229 ty and performance of the NV centre near the diamond's surface are the major obstacle in the practica

230 T), that most NVs are within 3.6 nm from the diamond's surface.

231 ith different commercial beer yeast (Abbaye, Diamond, SafAle, SafLager) in order to monitor the forma

232 ine the bulk temperature of a single crystal diamond sample at an X-Ray free electron laser using ine

233 The burgeoning availability of diamond samples grown under well-defined conditions has

234 h compares favourably with the commonly used diamond sandwich technique and could be important for ne

235 lowing for the optimisation of electrostatic diamond seeding densities.

236 sweat, using a surface-modified boron-doped diamond sensing interface (cross-validated with laborato

237 at 3.6 angstrom resolution, revealed that a diamond-shaped TreS tetramer forms the core of the compl

238 A nanocrystalline diamond sheet (NDS) attached over the ZnO is described.

239 The diamonds show a striking texture pseudomorphing inferred

240 among different layers of the lesions using DIAMOND software against the Kyoto Encyclopedia of Genes

241 ng and operating a simple, low-cost 'quantum diamond spectrometer' for performing NMR and electron sp

242 ylsiloxane (PDMS) show that the manufactured diamond spheres, even though possessing a rough surface,

243 loidal particles in the self-assembled cubic diamond structure are highly constrained and mechanicall

244 The diamond structure was synthesized in a Microwave Plasma

245 ossible to dry the suspension and retain the diamond structure.

246 revealed nanoscale twinning within the cubic diamond structure.

247 dic lattices like gyroid, rotated cubic, and diamond structures.

248 tigated concerning the interaction with flat diamond substrates in air.

249 Despite the relatively low quality of the diamond substrates used and the simplicity of our PIII s

250 .7 to 10 MPa) on 4 different polycrystalline diamond substrates with topography characterized across

251 depending on the availability of equipment, diamond substrates, and user experience.

252 en shown that inversion-symmetric defects in diamond, such as the negatively charged silicon vacancy

253 ization of target fluids in contact with the diamond surface or the use of hyperpolarized particles a

254 of the group IV dopants pre-deposited onto a diamond surface.

255 ion-implanted at a depth of ~10 nm below the diamond surface.

256 sonance spectroscopy of nanoscale samples on diamond surfaces.

257 ectric-contrast photonic crystals with cubic diamond symmetry.

258 caused by mutations in the Shwachman-Bodian-Diamond Syndrome (SBDS) gene.

259 Shwachman-Diamond Syndrome (SDS) is a rare and clinically-heteroge

260 Shwachman-Diamond syndrome (SDS) is a recessive disorder typified

261 rognosis is poor for patients with Shwachman-Diamond syndrome and myelodysplastic syndrome or acute m

262 tially identified 37 patients with Shwachman-Diamond syndrome and myelodysplastic syndrome or acute m

263 astic syndrome) were known to have Shwachman-Diamond syndrome before development of a myeloid maligna

264 laboration with the North American Shwachman-Diamond Syndrome Registry.

265 nts with the rare genetic disorder Shwachman-Diamond syndrome reproduced key haematopoietic defects a

266 of the allosteric regulator Shwachman-Bodian-Diamond syndrome that cooperates with elongation factor-

267 ias and pancreatic dysfunction) of Shwachman-Diamond syndrome who developed myelodysplastic syndrome

268 ogenesis (Diamond-Blackfan anemia, Shwachman-Diamond syndrome).

269 ome or acute myeloid leukaemia and Shwachman-Diamond syndrome, an inherited bone marrow failure disor

270 ia predisposition in patients with Shwachman-Diamond syndrome.

271 survey recent progress in two complementary diamond synthesis methods-high pressure high temperature

272 er refrigeration, including color centers in diamond that have recently been proposed to realize the

273 Slave craton diamonds that formed 3.5 billion years ago do not contai

274 of boron arsenide is second only to that of diamond, the best thermal conductor, which may be of ben

275 In materials other than diamond, there are several other promising approaches to

276 rconductivity in nanocrystalline boron doped diamond thin films is reported.

277 equent growth of boron-doped nanocrystalline diamond thin films on modified silicon nitride, under CV

278 for both room temperature diamond and heated diamond to 500 K.

279 Etching and patterning diamond to depths beyond one micron has proven challengi

280 Enabled by high channel quality, the diamond transistor behavior was shown to transit from a

281 ntimate association of large monocrystalline diamonds (up to at least 100 um), nanodiamonds, nanograp

282 The diamond uses expression dynamics rather than path length

283 hen coated with a conformal uniform layer of diamond using hot filament chemical vapour deposition to

284 rite arrays of optically active defects into diamond via momentum transfer from a Xe(+) focused ion b

285 er opportunities for tailoring properties of diamond via strain engineering for electronic, photonic,

286 influence of the surface termination of the diamond was investigated concerning the interaction with

287 neous integration of 'quantum microchiplets'-diamond waveguide arrays containing highly coherent colo

288 f hexagonal stacking on the Raman spectra of diamond were investigated computationally and found to b

289 Despite high target-flanker similarity, Diamonds were identified better than Xs when flanked by

290 of target conspicuity, however, showed that Diamonds were not perceived to stand out more strongly f

291 Inclusions in diamonds, which remain uncorrupted over geological times

292 they can readily probe force interactions of diamond with different substrate materials under varying

293 vides detailed insight into the interface of diamond with other materials and/or solvents.

294 nsight into surface chemistry and physics of diamond with other materials concerning long and short-r

295 Can diamond, with an ultrawide bandgap of 5.6 eV, be complet

296 ation engineering to boost spin lifetimes in diamond, with applications including engineered quantum

297 d what an ultrawide bandgap material such as diamond, with many appealing functional figures of merit

298 e destabilizes carbon-bearing metals to form diamond, without disturbing the ambient-mantle stable-is

299 ength, the appropriate e-value threshold for DIAMOND would then need to be more strict than the defau

300 ructive analysis of inclusions in deep Earth diamonds, yielding in situ quantitative information abou