ライフサイエンスコーパス: GPa

1 pressure and disappears completely above 2.0 GPa.

2 -RuN4 to C2/c-RuN4 is also uncovered at 23.0 GPa.

3 0.5 GPa), and 4 (vD : 9256 m s(-1) ; P: 38.0 GPa) exhibit excellent detonation performances, which ar

4 38.7 GPa) and 6 (vD, 9271 m s(-1); P = 41.0 GPa) exhibit great detonation properties, superior to th

5 sibly with eclogite at 900 degrees C and 5.0 GPa, generating diamond and secondary minerals due to a

6 malous metal-semiconductor transition at 6.0 GPa and an unusual increased resistance with further com

7 locity values for the Young's modulus of 6.0 GPa.

8 a phase transition from F-43m to Imma at 7.0 GPa and explained the carrier-type inversion at approxim

9 d metallization of GaSb at approximately 7.0 GPa, which corresponds to a structural phase transition

10 and finally to a monoclinic phase above 9.0 GPa.

11 istence of magnetic moment of Cr2TiAlC2 at 0 GPa and disappearance at high pressures above 50 GPa.

12 the resultant UTS estimate is 0.66 +/- 0.08 GPa.

13 t p-xylene crystallizes at approximately 0.1 GPa.

14 he Pnnm-RuN2 is found to be stable above 1.1 GPa, in agreement with the experimental results.

15 brittle fracture at an average stress of 1.1 GPa.

16 exchange angle theta is decreased below 22.1 GPa, thus enhancing the PL quantum yield leading to Sn (

17 8138 m s(-1) , a detonation pressure of 30.1 GPa, an impact sensitivity of 2 J, and friction sensitiv

18 maximal hardness and elastic modulus of 46.1 GPa and 425 GPa, respectively.

19 temperature (Tc ) of 3.7 K, peaking at 47.1 GPa.

20 we estimate UTSs of 3.5 +/- 3.2-5.5 +/- 5.1 GPa for proteins with interfacial disulfide bonds, and 1

21 orm exothermically at mild pressure (about 1 GPa).

22 he alloy shows tensile strengths of almost 1 GPa, failure strains of approximately 70% and KJIc fract

23 edicted to experience pressures as high as 1 GPa.

24 sodium-magnesium aluminosilicate glass at 1 GPa at Tg, followed by sub-Tg annealing in-situ at 1 GPa

25 g, followed by sub-Tg annealing in-situ at 1 GPa.

26 conium diboride (ZrB2) ceramics can exceed 1 GPa at room temperature, but these values rapidly decrea

27 p substances in high pressurized (of order 1 GPa) on nanobubbles.

28 10 nm bubbles the pressure can be close to 1 GPa and may modify properties of a trapped material.

29 city-dependent UTSs increasing from 0.2 to 1 GPa in the available speed range, and 1.5 GPa extrapolat

30 t and Au nanoparticles at pressures below 10 GPa.

31 erconductor under high pressure exceeding 10 GPa.

32 es with remarkably high elastic modulus (>10 GPa) have been fabricated through the self-assembly of l

33 comparison between Sb2S3 and Sb2Se3 up to 10 GPa reveals a slightly diverse structural behavior for t

34 Upon unloading to 10 GPa, -KCl3 transforms to a yet unknown structure before

35 tronic behavior of Sb2S3 and Sb2Se3 up to 10 GPa, i.e. the absence of an insulator-metal transition i

36 lopes at different pressure intervals, 0 100 GPa, 100 250 GPa, 250-400 GPa, respectively, and the mom

37 ets emerge upon compression within the 0-100 GPa pressure range.

38 maintained at low pressure, below about 100 GPa in Fe2MnAl and 50 GPa in Mn2FeAl.

39 e lonsdaleite in a diamond anvil cell at 100 GPa and 400 degrees C.

40 st the metallisation of the compound at ~100 GPa.

41 We have now synthesized two oxides below 100 GPa (Xe2O5 under oxygen-rich conditions, and Xe3O2 under

42 Sapphire (Al2O3) crystals are used below 100 GPa as anvils and windows in dynamic-compression experim

43 the behaviour of Fe2O3 at pressures over 100 GPa and temperatures above 2,500 K employing single crys

44 of pure iron carbonate at pressures over 100 GPa and temperatures over 2,500 K using single-crystal X

45 gCl2 remains in a 2D layered phase up to 100 GPa and further, the 6-fold coordination of Mg cations i

46 roscopy using a diamond-anvil cell up to 100 GPa at room temperature and theoretically using first-pr

47 in a laser-heated diamond anvil cell to 103 GPa obtained by X-ray absorption spectroscopy, a techniq

48 e ~35 GPa (Phase IV) that metallizes at ~105 GPa.

49 0.5 ns) after releasing of pressure from 11 GPa.

50 At ultrahigh pressure (>110 GPa), H2 S is converted into a metallic phase that becom

51 ops above 70 GPa before increasing up to 110 GPa with a minimum at 85 GPa; it then dramatically drops

52 Li3Ar) are predicted to be stable above 112 GPa and 119 GPa, respectively.

53 pe structure and is stable at pressures >113 GPa.

54 the postperovskite stability field above 116 GPa.

55 predicted to be stable above 112 GPa and 119 GPa, respectively.

56 ssibility along the c-axis changes around 12 GPa, where a new superconducting phase of SC II appears.

57 change in the electronic structure around 12 GPa.

58 he melting temperature is only 5000 K at 120 GPa, a value lower than nearly all previous estimates.

59 ting transition temperature of 17.6 K at 120 GPa.

60 The sharp shrinkage of the lattice at 13 GPa and the solid state of the decompressed sample we ob

61 decreases with increasing pressure up to 13 GPa, which can be clearly correlated with the pressure d

62 ven laser-heated diamond anvil cell from 135 GPa and 2,500 K to 154 GPa and 3,000 K.

63 This martensitic transformation begins at 14 GPa and is attributed to suppression of the local magnet

64 ition to a tetragonal Xe(N2)2-II phase at 14 GPa; this phase appears to be unexpectedly stable at lea

65 e whole investigated pressure range up to 14 GPa, yet displaying a non-monotonic variation with press

66 A modulus of 147 GPa for ThC at ambient pressure was obtained and the sto

67 igh-pressure modification appearing above 15 GPa appears to trigger a structural disorder at ~20 GPa;

68 th a similar structure at pressures above 15 GPa.

69 eveals two phase transitions at 5 GPa and 15 GPa.

70 measurements in FeSe up to approximately 15 GPa, which uncover the dome shape of magnetic phase supe

71 lagioclase is on average weakly shocked (<15 GPa) and examples of high shock states (>30 GPa; maskely

72 results show that at low pressures up to 15 GPa, the carbon dioxide speciation is dominated by molec

73 kypaper/Parmax composite to 1145 MPa and 150 GPa, respectively, far exceeding those of Parmax and ali

74 d anvil cell from 135 GPa and 2,500 K to 154 GPa and 3,000 K.

75 nstrate a well-defined pressure window (7-17 GPa) with flat maximum PL yielding and sharp edges at bo

76 he direct formation of lonsdaleite above 170 GPa for pyrolytic samples only.

77 sized with La atoms in an fcc lattice at 170 GPa upon heating to about 1000 K.

78 continuously increases from 6 to 6.8 at 172 GPa.

79 igated the structure of SiO2 glass up to 172 GPa using high-energy X-ray diffraction.

80 and then a smaller linear decrease up to 172 GPa.

81 ssure, and collapses ultimately at about 175 GPa.

82 l to a peanut-like shape and collapses at 18 GPa.

83 his organic compound becomes metallic at 180 GPa, fueling the hope for the possible realization of su

84 to be unexpectedly stable at least up to 180 GPa even after heating to above 2000 K.

85 attice film has demonstrated modulus of 1.19 GPa and specific energy dissipation of 325.5 kJ/kg, surp

86 ave an elastic modulus of approximately 6-19 GPa, and hardness of approximately 120-170 MPa.

87 olycrystalline graphite to pressures from 19 GPa up to 228 GPa.

88 y and compositional relationships in the 1.2 GPa Malaspina Pluton meant it was never likely to have d

89 ring of excised cumulate material at P > 1.2 GPa.

90 th a transition region between 14.1 and 25.2 GPa is observed, accompanying with a volume collapse ref

91 elocity minima at 1.8 GPa for P wave and 3.2 GPa for S wave.

92 ves such as RDX (vD : 8724 m s(-1) ; P: 35.2 GPa) and HMX (vD : 9059 m s(-1) ; P: 39.2 GPa).

93 .2 GPa) and HMX (vD : 9059 m s(-1) ; P: 39.2 GPa).

94 at 96 hours (75.34 +/- 13.2 vs 134.4 +/- 8.2 GPa; p < 0.001).

95 duced visible photoluminescence (PL) above 2 GPa near 2 eV is observed.

96 Above 2 GPa, the energy absorption typically reaches 3-4 kJ/g; f

97 u shell exerts high stress ( approximately 2 GPa) on the seed by forming a core/shell structure in th

98 structural transformation at approximately 2 GPa, (301) the crystal plane fully occupied by organic m

99 pressure-induced superconductivity around 2 GPa.

100 We find moduli as low as 2 GPa, a value typical of soft materials and over one orde

101 rivial to a topological insulator phase at 2 GPa, which is caused by an energy gap close then reopen

102 At compressive stress below 2 GPa, relatively small amounts of energy (<0.3 kJ/g) are

103 ere determined at upper mantle conditions (2 GPa and 750-900 degrees C).

104 ical properties (Young's modulus exceeding 2 GPa).

105 ssurizing pure water to pressures of order 2 GPa or more.

106 high ultimate compressive strengths (over 2 GPa), high compressive failure strain (over 20%), and su

107 on hardness, typically in the range of 10-20 GPa.

108 ease followed by an increase at around 15-20 GPa, depending on the composition.

109 e NTs, with an ultimate strength of about 20 GPa, are likely to find numerous applications in reinfor

110 the C2 phase in MgV2O6 was detected above 20 GPa, and both phases coexisted up to the highest pressur

111 s stable at pressures up to approximately 20 GPa and is significantly harder than cubic delta-NbN; it

112 morphous, one-dimensional (1D) polymer at 20 GPa (Phase III); and an extended 3D network above ~35 GP

113 ears to trigger a structural disorder at ~20 GPa; full decompression from 53 GPa leads to the recover

114 stable phases between approximately 160-200 GPa.

115 ered cubic (fcc) structure, stable above 200 GPa, and LaH8 a C2/m space group structure.

116 n of the phase diagram of hydrogen above 200 GPa.

117 able and superconducting between 100 and 200 GPa.

118 osphorus (PHn, n = 1-6) at 100, 150, and 200 GPa.

119 itional compound SnH4 with Tc of 52 K at 200 GPa.

120 With stability below 200 GPa, the superhydride is thus the closest analogue to so

121 essible and has a high shear rigidity of 201 GPa to rival hard/superhard material gamma-B ( approxima

122 en phosphine was subject to pressures of 207 GPa in a diamond anvil cell may result from these, and o

123 tic (AFM) insulator at [Formula: see text]21 GPa whose AFM spin configuration is different from the A

124 Tc calculated for LaH10 is 274-286 K at 210 GPa.

125 at low pressure and remains stable up to 215 GPa.

126 perhard material gamma-B ( approximately 227 GPa).

127 graphite to pressures from 19 GPa up to 228 GPa.

128 Fe0.6 N solid solution at between 15 and 23 GPa and up to 2500 K.

129 erent pressure intervals, 0 100 GPa, 100 250 GPa, 250-400 GPa, respectively, and the moment collapses

130 room temperature, reaching 305-326 K at 250 GPa.

131 - 0.53 GPa for SAM2X5-600 and 11.76 +/- 1.26 GPa for SAM2X5-630.

132 (G) and Young's (E) moduli of Fe2MnAl at 270 GPa, where the second moment collapse occurs.

133 increasing pressure up to approximately 0.3 GPa and then an increase in band gap up to a pressure of

134 Pressures of 1.2+/-0.3 GPa are found using Raman spectrometry for molecular lay

135 low Vickers hardness values of 10.6 +/- 0.3 GPa, compared to other transition metal borides, and ult

136 ransforms to a ReO3 -type cubic phase at 0.3 GPa.

137 ts at 24 hours (1.37 +/- 0.2 vs 6.13 +/- 0.3 GPa; p = 0.001) and 96 hours (5.57 +/- 0.5 vs 6.13 +/- 0

138 ) and 96 hours (5.57 +/- 0.5 vs 6.13 +/- 0.3 GPa; p = 0.006).

139 opy (up to 3.5x) and elastic modulus (0.03-3 GPa).

140 COH fluids interacting with silicates at 1-3 GPa and 800 degrees C display unpredictably high CO2 con

141 Here, we present experimental data at 1-3 GPa, 800 degrees C, and FMQ approximately -0.5 for the v

142 i alloy improve to strength levels above 1.3 GPa, failure strains up to 90% and KJIc values of 275 MP

143 the acoustic velocities, measured up to 12.3 GPa using ultrasonic interferometry, exhibit velocity mi

144 disulfide bonds, and 1.6 +/- 1.5-2.5 +/- 2.3 GPa for the reduced form.

145 nation performance (D=7759.0 m s(-1), P=27.3 GPa), make it a competitive replacement as a green prima

146 superconductivity in In2 Se3 occurs at 41.3 GPa with a critical temperature (Tc ) of 3.7 K, peaking

147 +/- 2.8 GPa, respectively, compared to 43.3 GPa for pure WB4 under an applied load of 0.49 N.

148 tration of 3.6 vol.% approach 119.1 MPa, 5.3 GPa and 2.4 x 10(-4) S m(-1), with increases of 17%, 32.

149 t-pressed antigorite at pressures of 4 and 3 GPa, respectively, and at temperatures reaching 1073 K.

150 ity with over 13% recoverable strain, over 3 GPa yield strength, repeatable stress-strain response ev

151 diamond anvil cell experiments but at 25-30 GPa higher pressure.

152 GPa) and examples of high shock states (>30 GPa; maskelynite) are uncommon.

153 affected by moderate to weak shock ( 5 to 30 GPa) we couple REE+Y abundances with FTIR analyses for F

154 ultralow Young's modulus (36 GPa, versus ~30 GPa for human bone) and high ultimate strength (853 MPa)

155 e does not metallize by band overlap at ~300 GPa, as suggested previously by measured non-equilibrium

156 ical stability in any binary AuHn at P < 300 GPa was overcome by introducing alkali atoms as reductan

157 lus comparable to steel, on the order of 300 GPa.

158 ally investigated at high pressure up to 300 GPa.

159 temperature and pressure of 1200 K and 31 GPa, respectively.

160 ressure rises, it polymerizes and, above 314 GPa, reacts with water to form orthocarbonic acid (H4CO4

161 e III); and an extended 3D network above ~35 GPa (Phase IV) that metallizes at ~105 GPa.

162 se, stable in calculations between 20 and 35 GPa and up to 800 K, features MgO6 octahedral units arra

163 %) alloy with ultralow Young's modulus (36 GPa, versus ~30 GPa for human bone) and high ultimate st

164 ttice distortion occurring between 34 and 39 GPa.

165 ing compression over a pressure range of 0-4 GPa for individual 1.2 mum ZIF-8 microcrystals, and the

166 y transforms to a hexagonal structure at 0.4 GPa, and then completely transforms to an orthorhombic p

167 change of the molecular configuration at 1.4 GPa from the abrupt change of splitting, disappearance,

168 tural silks, including a modulus of 11 +/- 4 GPa, even higher than natural spider silk.

169 ron x-ray total scattering method up to 38.4 GPa.

170 ectic curves were measured, beginning at 4.4 GPa and 165 degrees C (where it exists in a quadruple eq

171 y transforms to an orthorhombic phase at 7.4 GPa and finally to a monoclinic phase above 9.0 GPa.

172 hat relatively mild pressure conditions (7.4 GPa at 300 K) are sufficient to transform ammonia monohy

173 of vanadium ions (from 5+1 to 6) at around 4 GPa.

174 lline sample yielded the hardness of 11.8(4) GPa.

175 Cl3 at 40-70 GPa and trigonal -KCl3 at 20-40 GPa in a laser-heated diamond anvil cell (DAC) at temper

176 polyhydrides of Na (NaH3 and NaH7) above 40 GPa and 2,000 K.

177 e similar hardness values ( approximately 40 GPa at 0.49 N loading) as well as having a similar therm

178 0.52-0.98), exhibit a local maximum at 40 GPa, likely caused by the spin transition of iron.

179 n2FeAl shows an increasing tendency below 40 GPa and decreases subsequently with pressure, and collap

180 extending into the superhard region (HV > 40 GPa) have guided synthesis and identification of novel s

181 mpositions are considered superhard (Hv > 40 GPa), likely due to extrinsic hardening that plays a key

182 n is sluggish, occurring over a range of >40 GPa.

183 e intervals, 0 100 GPa, 100 250 GPa, 250-400 GPa, respectively, and the moment collapses finally at 4

184 ured at a broad range of pressures up to 400 GPa, where it is known experimentally that hydrogen is n

185 lore the C-H-O system at pressures up to 400 GPa.

186 were investigated in high pressures up to 41 GPa.

187 ain amorphous under pressure values up to 42 GPa.

188 ttice a axis becomes stiffer above about 420 GPa, ultimately presenting the same axial compressibilit

189 ness and elastic modulus of 46.1 GPa and 425 GPa, respectively.

190 ng exceptionally high values (as large as 44 GPa).

191 investigated by Raman spectroscopy up to 44 GPa.

192 ine vanadium as a function of pressure to 45 GPa.

193 ely, and the moment collapses finally at 450 GPa.

194 ecomes thermodynamically unstable above ~460 GPa.

195 buildup of internal stress not exceeding 0.5 GPa.

196 1 GPa in the available speed range, and 1.5 GPa extrapolated to the speeds expected in the sonicatio

197 uctural transition at [Formula: see text]1.5 GPa, and the other is from a ferromagnetic (FM) metal to

198 700-1,050 degrees C and pressures of 0.5-1.5 GPa.

199 lline platinum (n-Pt) were collected at 12.5 GPa with a single 5 s X-ray exposure, showing that the i

200 tion through a pressure cycle of 0 <--> 17.5 GPa.

201 rich fluids at 600-700 degrees C and 1.5-2.5 GPa and the discovery of methane-rich fluid inclusions i

202 at lower shock pressures ( approximately 2.5 GPa), and amorphization and structural collapse at highe

203 nsition via layer sliding, beginning at 28.5 GPa and not being completed up to around 60 GPa.

204 sodium acetate at 300 degrees C and 2.4-3.5 GPa and that over a broader range of pressures and tempe

205 sion (p-type to n-type) at approximately 4.5 GPa before metallization.

206 carrier-type inversion at approximately 4.5 GPa.

207 ith a microhardness reaching as high as 40.5 GPa (under an applied load of 0.49 N).

208 for example, 1 (vD : 9541 m s(-1) ; P: 40.5 GPa), and 4 (vD : 9256 m s(-1) ; P: 38.0 GPa) exhibit ex

209 ic crystal with unit cell parameters (at 6.5 GPa and 20 degrees C) of a = 5.88 A, b = 6.59 A, c = 6.9

210 At 300 K and 5 GPa Xe(N2)2-I is synthesised, and if further compressed,

211 nary Xe-N2 mixtures at pressures as low as 5 GPa.

212 to 53 GPa reveals two phase transitions at 5 GPa and 15 GPa.

213 , local melting (with conditions exceeding 5 GPa and 1,200 degrees C in some locations), and rapid co

214 ronic topological transition in Sb2S3 near 5 GPa.

215 he magnetic moment will collapse at about 50 GPa.

216 Above 50 GPa, the estimated coordination number continuously incr

217 and disappearance at high pressures above 50 GPa.

218 ssure, below about 100 GPa in Fe2MnAl and 50 GPa in Mn2FeAl.

219 r from fourfold to sixfold between 15 and 50 GPa, in agreement with previous investigations.

220 I with Pmm2 space group) at approximately 50 GPa and 1400 K.

221 's geotherm at pressures to approximately 50 GPa FeCO3 partially dissociates to form various iron oxi

222 At a shock pressure of 45 approximately 50 GPa, multiple planar faults, slightly deviated from maxi

223 ion from a Mott insulator to a metal at 50 GPa.

224 rve the transition to diamond starting at 50 GPa for both pyrolytic and polycrystalline graphite, we

225 of the EXAFS oscillations persists up to 500 GPa and 17000 K, suggesting an enduring local order.

226 transforms from P-1 to C2/c structure at 51 GPa.

227 ts Young modulus and fracture strength of 52 GPa and 300 MPa, respectively.

228 niot Elastic Limit (HEL) to be 8.58 +/- 0.53 GPa for SAM2X5-600 and 11.76 +/- 1.26 GPa for SAM2X5-630

229 order at ~20 GPa; full decompression from 53 GPa leads to the recovery of an amorphous state.

230 copy and x-ray diffraction of Sb2S3 up to 53 GPa reveals two phase transitions at 5 GPa and 15 GPa.

231 and IR wavelengths at pressures above ca. 56 GPa, suggesting the imminent closure of its optical band

232 of ThC from B1 to P4/nmm at pressure of 58 GPa at ambient temperature.

233 the average oxidation state of +2.25 at 12.6 GPa.

234 t, an ultra-high tensile strength of 2.4-2.6 GPa, a significant elongation of 4-10% and a good fractu

235 se on shock release in only 2.4 ns from 33.6 GPa.

236 m temperature and high pressures (up to 40.6 GPa) yielded a bulk modulus of B0 = 306(6) GPa and its p

237 ch other, with Young's moduli of 4.9 and 9.6 GPa for Forms I and II, respectively.

238 esistance with further compression above 9.6 GPa.

239 e normal states of the high-Tc phase above 6 GPa.

240 Above approximately 6 GPa the sudden enhancement of superconductivity (Tc</=38

241 At pressure <6 GPa, the PAW-GGA can be described by a Birch-Murnaghan e

242 tor and metallic states can be closed near 6 GPa.

243 6 GPa) yielded a bulk modulus of B0 = 306(6) GPa and its pressure derivative B0' = 6.4(5).

244 2O3 and Fe3O4 observed at pressures above 60 GPa and temperatures of 2,000 K leads to crystallization

245 The metallic character of (MA)PbI3 above 60 GPa was confirmed using both IR reflectivity and variabl

246 cular bond of the nitrogen molecule above 60 GPa, while transmission measurements in the visible and

247 GPa and not being completed up to around 60 GPa.

248 Relatively low shear modulus of ~64 GPa from theoretical calculations suggests a complicated

249 e hardness of W0.92Zr0.08B4 is 34.7 +/- 0.65 GPa under an applied load of 4.9 N, the highest value ob

250 study are measured to be 0.85 GPa and 34.65 GPa, respectively.

251 ered CdI2-type structure (beta-MgCl2) at 0.7 GPa: the stacking sequence of the Cl anions are altered

252 e observed for pressures between 1.0 and 1.7 GPa and merge into a single first-order transition for p

253 K at ambient pressure and up to 30 K at 1.7 GPa.

254 uperconducting in decompression down to 10.7 GPa.

255 erature up to maximum value of 8.2 K at 11.7 GPa.

256 Upon continuous compression to 2.7 GPa this cubic polymorph converts into a putative orthor

257 increase in band gap up to a pressure of 2.7 GPa, in excellent agreement with our DFT calculation pre

258 dulus and its pressure derivative are = 33.7 GPa, and = 2.9.

259 = 9086 m s(-1); detonation pressure P = 38.7 GPa) and 6 (vD, 9271 m s(-1); P = 41.0 GPa) exhibit grea

260 Beyond 4.7 GPa it separates into crystalline and amorphous fraction

261 equation of state with = 687.4 A(3), = 51.7 GPa, and = 4.7.

262 partial dislocation 1/6 <110> {111} and 6.7 GPa for the full dislocation (1/2) <110> {110}.

263 through a broad pressure range of 28.2-61.7 GPa, where a mixed semiconducting and metallic feature i

264 strength (826 MPa) and Young's modulus (65.7 GPa) owing to the large length and the alignment of nano

265 ermined electron density distribution at 7.7 GPa; the observations presented in this work are validat

266 he carbon cage deforms significantly above 7 GPa, from spherical to a peanut-like shape and collapses

267 transition for pressures greater, similar1.7 GPa, reminiscent of what has been found for the evolutio

268 We have synthesized cubic -KCl3 at 40-70 GPa and trigonal -KCl3 at 20-40 GPa in a laser-heated di

269 on concentration in silicates drops above 70 GPa before increasing up to 110 GPa with a minimum at 85

270 ed by transmission electron microscopy at 70 GPa (determined by a corresponding VISAR experiment).

271 r quasi-hydrostatic loading to as high as 71 GPa indicate the existence of substantial reduction of g

272 ite and gabbro were emplaced at 1.2 and 1.8 GPa are parts of the Western Fiordland Orthogneiss (WFO)

273 The 1.8 GPa Breaksea Orthogneiss includes suitably dense minor c

274 terferometry, exhibit velocity minima at 1.8 GPa for P wave and 3.2 GPa for S wave.

275 solved shear stress was estimated to be 13.8 GPa for the partial dislocation 1/6 <110> {111} and 6.7

276 50.9 +/- 2.2, 55.9 +/- 2.7 and 51.6 +/- 2.8 GPa, respectively, compared to 43.3 GPa for pure WB4 und

277 he Vickers hardness can be increased to 42.8 GPa, creating a new superhard metal.

278 sults indicate elastic softening between 6-8 GPa.

279 d anvil cells with pressures up to 54.0-62.8 GPa.

280 llapse at higher pressures ( approximately 8 GPa).

281 ear the critical pressure PC approximately 8 GPa, which is in good agreement with the experiments.

282 Superconducting transition appears at 8 GPa with a critical temperature TC of 5.3 K.

283 viously unreported phase transition at ca. 8 GPa and dramatic piezochromism from translucent red-oran

284 ecture with no phase change apparent up to 8 GPa.

285 achieved by the application of pressure to 8 GPa.

286 At 80 GPa, phases with the PH2 stoichiometry, which are compos

287 ss relations in the ultrahard range (HV > 80 GPa) by examining single-crystal boron-doped diamond (BD

288 expansion of Mo have been measured up to 80 GPa at 300 K, and 92 GPa at 3470 K, respectively.

289 of N-H system in a pressure range up to 800 GPa through evolutionary structure prediction.

290 The X-ray diffraction (XRD) pattern at 0.84 GPa suggests that the crystallized p-xylene had a monocl

291 igated in this study are measured to be 0.85 GPa and 34.65 GPa, respectively.

292 ncreasing up to 110 GPa with a minimum at 85 GPa; it then dramatically drops in the postperovskite st

293 local structure of liquid gallium up to 1.9 GPa.

294 tals became completely depolarized under 3.9 GPa compression.

295 N2O5 becomes stable at 9 GPa, and transforms from P-1 to C2/c structure at 51 GPa

296 3m, Phase I) to bent OCS (Cm, Phase II) at 9 GPa; an amorphous, one-dimensional (1D) polymer at 20 GP

297 been measured up to 80 GPa at 300 K, and 92 GPa at 3470 K, respectively.

298 tal transition at high pressures close to 96 GPa is thus truly remarkable.

299 ith a Ki value of 143 nM against human liver GPa.

300 nanoparticle arrays to pressures of tens of GPa, demonstrating pressure-driven assembly beyond the q