ライフサイエンスコーパス: diamond

1 ransverse stiffness are inferior to those of diamond.

2 Darwinism, e.g., using nitrogen vacancies in diamond.

3 gnificantly higher than that for boron-doped diamond.

4 on, charge diffusion and trapping in type-1b diamond.

5 ctive with reduced ambient mantle, producing diamond.

6 hanism of graphene growth on polycrystalline diamond.

7 s in silicon and nitrogen-vacancy centers in diamond.

8 c orientation as those for inclusions in the diamond.

9 chnique of Fourier magnetic imaging using NV-diamond.

10 copy using individual atomlike impurities in diamond.

11 idotite, its clinopyroxene and a gem-quality diamond.

12 on of diamondene, an atomically thin form of diamond.

13 to analyze and to identify nickel defect in diamonds.

14 images can arise from thickness effects of c-diamonds.

15 calculations of fluorinated and hydrogenated diamond (111) surfaces interacting with single water mol

16 reflection ATR (attenuated total reflection) diamond accessory.

17 The diamonds act as a chemical inert container and therefore

18 design of a novel Disease Module Detection (DIAMOnD) algorithm to identify the full disease module a

19 The hexagonal form of diamond, also known as lonsdaleite, was discovered in th

20 igh-throughput DNA-to-protein alignment tool DIAMOND and by providing a new program MeganServer that

21 Nanotwinning within both diamond and cBN domains further contributes to a bulk ha

22 nanocomposites consist of randomly-oriented diamond and cBN domains stitched together by sp(3)-hybri

23 sutures accommodate lattice mismatch between diamond and cBN.

24 ials, including tungsten, silicon, graphite, diamond and graphene, for point defects such as vacancie

25 protein alignment tools: BLASTX, RAPSearch2, DIAMOND and Lambda, using empirically obtained reads.

26 Furthermore, shock synthesis of diamond and lonsdaleite, a speculative hexagonal carbon

27 faster than the best performing alternative, DIAMOND and nearly 8000 times faster than BLASTX.

28 eraction between nitrogen-vacancy centres in diamond and photonic and/or broadband plasmonic nanostru

29 ues, as well as percolating low-coordination diamond and pyrochlore sublattices never assembled befor

30 ite at 900 degrees C and 5.0 GPa, generating diamond and secondary minerals due to a decrease in pH a

31 n established platforms including defects in diamond and self-assembled quantum dots, albeit often wi

32 polarization of individual nuclear spins in diamond and SiC reaches 99% and beyond, it has been limi

33 attempts of metal-induced transformation of diamond and silicon carbide into graphene suffers from m

34 t has bulk modulus comparable to crystalline diamond and that it can be recovered under ambient condi

35 he shock-induced transition from graphite to diamond and uniquely resolves the dynamics that explain

36 patterns of carbonatitic melt inclusions in diamonds and HIMU lavas indicate that the metasomatism o

37 ert glassy carbon into "quenchable amorphous diamond", and recover it to ambient conditions.

38 s in silicon and nitrogen vacancy centres in diamond, and for orbital motion in InAs quantum dots.

39 Although boron-doped diamond anodes mineralized haloacetic acids after format

40 rigonal -KCl3 at 20-40 GPa in a laser-heated diamond anvil cell (DAC) at temperature exceeding 2000 K

41 near the center of a sample, compressed in a diamond anvil cell (DAC), with a very high pressure grad

42 (PDF) measurements at high pressure using a diamond anvil cell (DAC).

43 ases as pressure transmitting media within a diamond anvil cell along with a single-crystal of a poro

44 sample through diffraction measurements in a diamond anvil cell and discover a new thermodynamic boun

45 inelastic X-ray scattering experiments in a diamond anvil cell and molecular dynamic simulations to

46 ion and Raman spectroscopy in a laser-heated diamond anvil cell and theoretical random structure sear

47 he synthesis of almost pure lonsdaleite in a diamond anvil cell at 100 GPa and 400 degrees C.

48 ental predictions, close to that measured in diamond anvil cell experiments but at 25-30 GPa higher p

49 We performed laser-heated diamond anvil cell experiments combined with state-of-th

50 s whereas about twice as large as those from diamond anvil cell experiments.

51 iffraction in a membrane-driven laser-heated diamond anvil cell from 135 GPa and 2,500 K to 154 GPa a

52 ine was subject to pressures of 207 GPa in a diamond anvil cell may result from these, and other, dec

53 elting temperature of iron in a laser-heated diamond anvil cell to 103 GPa obtained by X-ray absorpti

54 ing and annealing followed by compression in diamond anvil cell to tailor the intrinsic and extrinsic

55 e Stimulated Light Scattering coupled with a diamond anvil cell up to 96 GPa.

56 rption method to the small dimensions of the diamond anvil cell, enabling density measurements of amo

57 and subsequent high-pressure synthesis in a diamond anvil cell, we report the discovery of a thermod

58 radial plastic flow under compression in the diamond anvil cell, which lowers the energy barrier by "

59 superconducting order via measurements in a diamond anvil cell.

60 when filled with methanol molecules within a diamond anvil cell.

61 rapidly quenching samples in a laser-heated diamond anvil cell.

62 sembly beyond the quasi-static regime of the diamond anvil cell.

63 Using synchrotron x-ray diffraction in diamond anvil cells and multiscale simulations with dens

64 ombination of a multichannel collimator with diamond anvil cells enabled the measurement of structura

65 nsport measurement of single crystal WSe2 in diamond anvil cells with pressures up to 54.0-62.8 GPa.

66 ynchrotron x-ray diffraction in laser-heated diamond anvil cells, we show that MgO and oxygen react a

67 res using both conventional and double-stage diamond anvil cells, with accurate pressure determinatio

68 n and Mossbauer spectroscopy in laser-heated diamond anvil cells.

69 tem at high pressures using the laser-heated diamond-anvil cell and show that the liquidus and solidu

70 fraction measurements on Ir2P powder using a diamond-anvil cell at room temperature and high pressure

71 er, recent first-principles calculations and diamond-anvil cell experiments indicate that the thermal

72 y diffraction and Raman spectroscopy using a diamond-anvil cell up to 100 GPa at room temperature and

73 ed planets, using a dynamically laser-heated diamond-anvil cell.

74 onic acid, was observed in the high-pressure diamond-anvil cell.

75 its bandgap evolution during compression in diamond-anvil cells using absorption spectroscopy and ob

76 Diamond-anvil-cell experiments and ab initio modelling h

77 Microscale helical diamond architectures are formed by controlled debonding

78 Sensors using nitrogen-vacancy centers in diamond are a promising tool for small-volume nuclear ma

79 sumed that mineral inclusions and their host diamonds are 'syngenetic' in origin, which means that th

80 Many inclusions in superdeep diamonds are best explained by carbonate melt-peridotite

81 in non-coated, monocrystalline-lithospheric diamonds are protogenetic.

82 instead, were formed earlier with respect to diamonds are termed protogenetic.

83 individual nitrogen-vacancy centre spins in diamond at room temperature, with nanometre-scale resolu

84 about one million dipolar spin impurities in diamond at room temperature.

85 CARTO-3(c) (Biosense Webster Inc, Diamond Bar, CA) maps in patient undergoing VT ablation

86 Diamond based materials, and specifically nanostructured

87 nclusively the protogenesis of inclusions in diamonds, based upon data from an exceptional fragment o

88 sing a ruggedized optical fiber probe with a diamond-based ATR, we have conducted mid-infrared sensor

89 g exciting opportunities for future graphene/diamond-based electronics.

90 apture at a boron-doped ultrananocrystalline diamond (BD-UNCD) electrode in a microfluidic dielectrop

91 EF with boron-doped diamond (BDD) anode ensured the gradual TOC removal unde

92 It is based on boron-doped diamond (BDD) electrodes and a competitive magneto-enzym

93 esponse of many redox species on boron-doped diamond (BDD) electrodes can be strongly dependent on th

94 nts was evaluated on Ti-IrO2 and boron-doped diamond (BDD) electrodes using a suite of trace organic

95 separated glassy carbon (GC) and boron-doped diamond (BDD) electrodes.

96 e) assembly consists of an inner boron doped diamond (BDD) layer and an outer undoped diamond layer.

97 he development of a voltammetric boron doped diamond (BDD) pH sensor is described.

98 h-oxidation-power anodes such as boron-doped diamond (BDD) were employed.

99 GPa) by examining single-crystal boron-doped diamond (BDD) with boron contents ranging from 50-3000 p

100 ciency (>95%) with an integrated boron doped diamond (BDD) working electrode offering a wide potentia

101 s, including glassy carbon (GC), boron-doped diamond (BDD), and screen-printed graphitic electrodes (

102 atalytically inactive electrode, boron-doped diamond (BDD), is found to be active for CO2 and CO redu

103 activity (6.6 x 10(-14) M) with boron-doped diamond (BDD, 7.4 x 10(-14) M) electrodes.

104 Here, oxygen-terminated lightly boron-doped diamond (BDDL) thin films were synthesized as a semicond

105 upon data from an exceptional fragment of a diamond-bearing peridotite, its clinopyroxene and a gem-

106 is well correlated with the origin depths of diamond-bearing xenoliths and corresponds to the transit

107 In this study, we describe a novel universal diamond biosensor, which enables the specific detection

108 Diamond Blackfan anaemia (DBA) is a congenital bone marr

109 Finally, RNA from patients with Diamond Blackfan Anemia (DBA), shows, on average, a lowe

110 are Fanconi anemia, dyskeratosis congenita, Diamond Blackfan anemia, and Shwachman Diamond syndrome.

111 genetic bone marrow failure diseases such as Diamond-Blackfan anaemia, are not treatable with erythro

112 al manifestations; we use the well-described Diamond-Blackfan anemia (DBA) as a specific example to h

113 Diamond-Blackfan Anemia (DBA) is a bone marrow failure d

114 Diamond-Blackfan anemia (DBA) is a congenital bone marro

115 Diamond-Blackfan anemia is a congenital form of PRCA.

116 nts (235 acquired, 85 Fanconi anemia, and 10 Diamond-Blackfan anemia) and their unrelated donors who

117 and inherited GATA1 mutations contribute to Diamond-Blackfan anemia, acute megakaryoblastic leukemia

118 graphite can be hypothetically derived from diamond by stretching it along its [111] axis, many 3D m

119 tribution for the P1 electronic spin bath in diamond by using an ensemble of nitrogen-vacancy centres

120 nterior region where the formation of double-diamond cages (DDCs) is favored in comparison with the b

121 Here, we show that in small diamond cages, called diamondoids, the electron-vibratio

122 integration.Nitrogen vacancy (NV) centres in diamond can be used for NMR spectroscopy, but increased

123 hermetic container, comprising a transparent diamond capsule and platinum wire feedthroughs.

124 iter-volume solutions using a nanostructured diamond chip with dense, high-aspect-ratio nanogratings,

125 iform samples covering the surface of a bulk diamond chip.

126 The presence of carbonates in inclusions in diamonds coming from depths exceeding 670 km are obvious

127 Garnet inclusions and host diamonds comprise two compositional suites formed under

128 itial surface that will produce a lattice of diamonds connected by steep, sharp ridges, and we experi

129 These sublithospheric diamonds contain inclusions of solidified iron-nickel-ca

130 ted magnesia catalyst (Au/MgO) and a natural diamond containing Fe-rich inclusions.

131 that the intermediate possesses a di-mu-oxo diamond core structure with a terminal hydroxide ligand

132 igh-valent diiron model complexes, including diamond-core [Fe(IV)2(mu-O)2(L)2](ClO4)4] (3) and open-c

133 stance, supports the view that X contains a "diamond-core" Fe(III)/Fe(IV) center, with the irons brid

134 xes affords isolable oxo species with M2 O2 "diamond" cores, including the first example of a crystal

135 nt microspheres arranged like the atoms in a diamond crystal.

136 Well-crystallized diamond crystals are obtained at the tips of the carbon

137 interfaces formed between the materials with diamond cubic crystal structures studied in this work, t

138 interfaces comprised of materials exhibiting diamond cubic crystal structures, higher conductances ar

139 s in a dominant shear band starting with the diamond-cubic (dc) to diamond-hexagonal (dh) phase trans

140 Diamond-cubic germanium is a well-known semiconductor, a

141 Gilbert-Diamond D, Emond JA, Baker ER, Korrick SA, Karagas MR.

142 ia, South Africa, showing that two suites of diamonds define two isochrons, showing the importance of

143 itrogen-vacancy centres spin state in an all-diamond device.

144 incompressibility comparable to crystalline diamond.Diamond's properties are dictated by its crystal

145 onto a diazonium-functionalized boron doped diamond electrode (BDD) modified with multi-walled carbo

146 A diamond electrode is surface-functionalized with polyclo

147 y with a cathodically pretreated boron-doped diamond electrode, using 0.30molL(-1) H2SO4 as supportin

148 m) gold nanoparticles (AuNPs) on boron doped diamond electrodes using three different electrode fabri

149 el irrigated RF catheter was designed with a diamond-embedded tip (for rapid cooling) and 6 surface t

150 gen-vacancy (NV) sensors in room temperature diamond enables detection of individual target nuclear s

151 empts to produce MH were unsuccessful due to diamond failure before the required pressures were achie

152 from 2D platelets leads to the formation of diamond-fiber hybrid structures.

153 raphenes, organic light-emitting diodes, and diamond films fabricated via chemical vapor deposition a

154 monoenergetic aluminum ions to heat gold and diamond foils uniformly and isochorically.

155 ults constitute a new quantitative theory of diamond formation as a consequence of the reaction of de

156 matic processes responsible for harzburgitic diamond formation beneath Venetia from the Archaean to t

157 Diamond formation has typically been attributed to redox

158 ed in situ X-ray diffraction measurements of diamond formation on nanosecond timescales by shock comp

159 bduction, mantle metasomatism and fluid-rich diamond formation, emphasizing the importance of subduct

160 perties of the lithospheric root, as well as diamond formation, yet the origin and composition of the

161 ined material but is instead defective cubic diamond formed under high pressure and high temperature

162 We sought to compare the Diamond-Forrester (DF) score with the 2 CAD consortium s

163 igate 20 to 200 nm sized inclusions in milky diamonds from Rio Soriso, Juina area, Brazil.

164 licic and carbonatitic deep mantle melts, in diamonds from the Northwest Territories, Canada.

165 data on individual garnet inclusions within diamonds from Venetia, South Africa, showing that two su

166 idual garnet inclusions from 26 harzburgitic diamonds from Venetia, South Africa.

167 s of benzene and cyclobutadiene, or those of diamond, graphene, and C60 , possess nearly identical pa

168 Kehayias et al. present a nanostructured diamond grating with a high density of NV centres, enabl

169 sults demonstrate that resolving the time of diamond growth events requires dating of individual incl

170 Precise dating of diamond growth is required to understand the interior wo

171 has implications for all genetic aspects of diamond growth, including their ages.

172 d materials, and specifically nanostructured diamond has attracted much attention due to its extreme

173 y charged nitrogen vacancy (NV(-)) center in diamond has attracted strong interest for a wide range o

174 he shock-induced transition from graphite to diamond has been of great scientific and technological i

175 y charged silicon vacancy centre (SiV(-)) in diamond has emerged as a novel promising system for QIP

176 The nitrogen-vacancy (NV) defect in diamond has emerged as a promising candidate for such a

177 This transparent quenchable amorphous diamond has, to our knowledge, the highest density among

178 Spin impurities in diamond have emerged as a promising building block in a

179 iting physical properties comparable to pure diamond have recently become necessary.

180 equality using entangled electronic spins in diamonds (Hensen et al., Nature 526, 682-686) provided t

181 band starting with the diamond-cubic (dc) to diamond-hexagonal (dh) phase transition and then proceed

182 ll mass and high thermal conductivity of the diamond host make the time response of our technique sho

183 The diagnostic features of n-diamond in TEM images can arise from thickness effects o

184 interest since the discovery of microscopic diamonds in remnants of explosively driven graphite.

185 wever, minerals can have the same age as the diamonds in that they become enclosed in and isolated fr

186 diamond, is resistant to perforation with a diamond indenter and shows a reversible drop in electric

187 or potentially exceeding the hardness of the diamond indenter, leading to debate about methodology an

188 semblages and reduced volatiles in large gem diamonds indicate formation under metal-saturated condit

189 direct approach to transform polycrystalline diamond into high-quality graphene layers on wafer scale

190 sing nitrogen-vacancy (NV) colour centres in diamond is a leading modality for nanoscale magnetic fie

191 Undoped CVD diamond is an insulating material with superior chemical

192 The nitrogen-vacancy (NV) centre in diamond is emerging as a promising platform for solid-st

193 These values of T(i) make it clear that the diamond is not melting, contradicting a recent suggestio

194 aphitic planes of the precursor to hexagonal diamond is supported by first principles calculations of

195 r hydrogens.The synthesis of two-dimensional diamond is the ultimate goal of diamond thin-film techno

196 ewidth magnetometer based on single spins in diamond is used to sense nanoscale magnetic fields with

197 the Proterozoic.Dating of inclusions within diamonds is used to reconstruct Earth's geodynamic histo

198 nsverse stiffness and hardness comparable to diamond, is resistant to perforation with a diamond inde

199 next-generation electronic materials such as diamond.Isolated attosecond pulses are produced using hi

200 Diamond laboratory shows that the rhythmic neuronal acti

201 Diamond lattices formed by atomic or colloidal elements

202 mental realization by assembling two variant diamond lattices, one with and one without atomic analog

203 ped diamond (BDD) layer and an outer undoped diamond layer.

204 interface between the doped and the undoped diamond layers.

205 Here we report that large, exceptional gem diamonds like the Cullinan, Constellation, and Koh-i-Noo

206 The influence of diamond-like carbon (DLC) films on bacterial leakage thr

207 to tune resonant transmission in disordered diamond-like carbon (DLC) superlattices as conventional

208 lly, the resulting tribofilms are similar to diamond-like carbon.

209 ted high-T c superconductivity in hole-doped diamond-like cubic crystalline hydrocarbon K 4-CH (space

210 nfiguration controls the conformation of the diamond-like film, in a multilayer film it hinders the p

211 he two-layer graphene film transforms into a diamond-like film, producing both elastic deformations a

212 schemes rely on accurately quantifying HV of diamond-like materials approaching or potentially exceed

213 e observed high surface charge mobilities of diamond-like materials.

214 ple method for the synthesis of linear-chain diamond-like nanomaterials, so-called diamantane polymer

215 ad to syndromic neutropenia with a Shwachman-Diamond-like phenotype.

216 e transformation of multilayer graphene into diamond-like ultrahard structures.

217 To date, however, NV-diamond magnetic imaging has been performed using 'real-

218 NV diamond magnetometry is noninvasive and label-free and d

219 stable and atomically thick two-dimensional diamond material, named here as diamondene, is still for

220 The investigation of these specific diamonds may open a new window to deeper parts of the Ea

221 A diamond microcrystal fixed on the fiber tip is heated by

222 The fabrication of an all-diamond microprobe is demonstrated for the first time.

223 We apply a quantum diamond microscope for detection and imaging of immunoma

224 he operating open-pit and underground Diavik diamond mine, Northwest Territories, Canada.

225 DIAMOND: multicenter, 24-week, randomized trial investig

226 Levitated diamond nanocrystals with nitrogen-vacancy (NV) centres

227 onal trap for diamagnetic particles, such as diamond nanocrystals, with stable levitation from atmosp

228 ur results show that twins are widespread in diamond nanocrystals.

229 licon-vacancy (SiV) color centers coupled to diamond nanodevices.

230 Nanocrystalline diamond nanomembranes with thinning-reduced flexural rig

231 odification of a gold electrode with undoped diamond nanoparticles (DNPs) and its applicability to th

232 ydrodynamic and electrokinetic properties of diamond nanoparticles (DNPs) functionalized with the pol

233 Diamond nanoparticles at low NOM-to-DNP ratios attach to

234 e (ODMR) of nitrogen-vacancy (NV) centers in diamond nanoparticles provides a pathway toward backgrou

235 like single silicon vacancy (SiV) centres in diamond nanostructures via focused ion beam implantation

236 loy samples were coated with nanocrystalline diamond (NCD) layers of different thicknesses, grown in

237 Electron spins of diamond nitrogen-vacancy (NV) centres are important quan

238 e experimentally realize this platform using diamond nitrogen-vacancy centers and use it to investiga

239 they satisfy a rigorous threshold for FTQEC (diamond norm </=6.7 x 10(-4)).

240 l errors, and cannot be compared directly to diamond norm thresholds.

241 ld for general errors is quantified by their diamond norm.

242 Nitrogen-vacancy (NV) centres in diamond offer an alternative detection strategy for nano

243 bed nitrogen-vacancy (NV) quantum defects in diamond, operated under ambient conditions and with the

244 ntional covalent superhard materials such as diamond or cubic boron nitride.

245 le approach for spontaneously growing double-diamond (or B32) crystals that contain a suitable diamon

246 Many natural, 'superdeep' diamonds originating in the deep upper mantle and transi

247 Diamond owes its unique mechanical, thermal, optical, el

248 nging the widespread idea of fish favoring a diamond pattern to swim more efficiently, we observe tha

249 ve cubic ([Formula: see text]) to the double diamond phase ([Formula: see text]) whilst still allowin

250 th a significant retention of the metastable diamond phase.

251 By placing SiV centers inside diamond photonic crystal cavities, we realize a quantum-

252 rapped within diamonds when they form and so diamonds provide a unique means of directly characterizi

253 x or low-coordination architectures, such as diamond, pyrochlore and other sought-after lattices, hav

254 continuously protected logical qubit using a diamond quantum processor.

255 robe that integrates a nitrogen-vacancy (NV) diamond quantum sensor with optical and microwave wavegu

256 structures, which then form tetrahedral and diamond quaternary topologies with unprecedented complex

257 used to study the wetting of F/H-terminated diamond, revealing a pronounced correlation between adso

258 of alpha-helical solenoids organized into a diamond ring conformation and is strikingly reminiscent

259 Hence, the diamond self-assembly problem is solved via its mapping

260 ted under ambient conditions and with the NV diamond sensor in close proximity ( approximately 10 mic

261 A freestanding film of boron-doped diamond serves as both an X-ray window and the electrode

262 gy increased, the spin excitations assumed a diamond shape, and they dispersed outward until the ener

263 r PLLA led to the formation of novel, hollow diamond-shaped assemblies.

264 Dirac cones that form a Fermi surface with a diamond-shaped line of Dirac nodes.

265 Specifically, we describe the formation of diamond-shaped platelet micelles and concentric "patchy"

266 While we observe the transition to diamond starting at 50 GPa for both pyrolytic and polycr

267 nd (or B32) crystals that contain a suitable diamond structure, using DNA to direct the self-assembly

268 trode array was embedded in a single-crystal diamond substrate (4 x 4 muG-SCD MEA) for real-time moni

269 The 1.8 billion years younger Proterozoic diamond suite formed by melt-dominated metasomatism rela

270 The Archaean diamond suite formed from relatively cool fluid-dominate

271 We report a strategy for creating a diamond superlattice of nano-objects via self-assembly a

272 cal composition of molecules tethered to the diamond surface or to investigate thermally or chemicall

273 um CHF of 7-8 kW/cm(2) may be achieved using diamond surface structures.

274 -vacancies located a few nanometers from the diamond surface to detect the NMR spectrum of roughly 1

275 ndividual ubiquitin proteins attached to the diamond surface.

276 While diamond symmetry crystals have been grown from much smal

277 Mutations in the Shwachman-Bodian-Diamond Syndrome (SBDS) gene cause Shwachman-Diamond Syn

278 f-function mutations in the Shwachman-Bodian-Diamond syndrome (sbds) gene.

279 Shwachman-Diamond syndrome (SDS) (OMIM #260400) is a rare inherite

280 e congenital neutropenia (SCN) and Shwachman-Diamond syndrome (SDS) are congenital neutropenia syndro

281 Diamond Syndrome (SBDS) gene cause Shwachman-Diamond Syndrome (SDS), a rare congenital disease charac

282 ound heterozygous mutations in the Shwachman-Diamond syndrome-associated SBDS gene with concurrent TP

283 nita, Diamond Blackfan anemia, and Shwachman Diamond syndrome.

284 Despite the advanced stage of diamond thin-film technology, with applications ranging

285 -dimensional diamond is the ultimate goal of diamond thin-film technology.

286 us nanowire network films exhibited a single diamond topology of symmetry Fd3m (Q227) which was verif

287 with type 1 diabetes in the CGM group of the DIAMOND trial were randomly assigned via the study websi

288 Rolled-up diamond tubular microcavities exhibit pronounced defect-

289 first thermotropic structure of the "double diamond" type.

290 beams to vibrational states of a macroscopic diamond under ambient conditions.

291 sociated with the nitrogen vacancy centre in diamond, using coherent feedback to overcome the limitat

292 with a tunable frequency and bandwidth in a diamond waveguide.

293 sociated with the nitrogen vacancy center in diamond, we experimentally demonstrate that quantum inte

294 PL excitation (PLE) spectra of Ni defect in diamond, we observed a distinct PLE line at 215 nm for t

295 ess in optical control of motional states of diamonds, we report an experimental demonstration of qua

296 Such fluids are trapped within diamonds when they form and so diamonds provide a unique

297 iscovery of superconductivity in boron-doped diamond with a critical temperature (TC) near 4 K, great

298 g single-shot readout of an electron spin in diamond with fast feedback.

299 rials combining the hardness and strength of diamond with the higher thermal stability of cubic boron

300 involve the Fe-C phases can readily produce diamond with the observed low delta(13)C values.