ライフサイエンスコーパス: room temperature

1 larizing medium to realize the detection at "room temperature".

2 escence detection of sulfur mustard (SM) at "room temperature".

3 D1, T1 and Q1 vs 48% for [Ru(bpy)(3)](2+) at room temperature).

4 7](2+)) under mild conditions (observable at room temperature).

5 = 0.52 T at 2 K (2.2 MJ m(-3) and 0.44 T at room temperature).

6 ime periods characterized herein (45 days at room temperature).

7 synthesize Pt NPs in an aqueous solution at room temperature.

8 unced upon increasing the temperature toward room temperature.

9 ew macroscopic quantum phenomena observed at room temperature.

10 urate quality assessment of meat spoilage at room temperature.

11 ss dehydrogenation of tetrahydroquinoline at room temperature.

12 50 are achieved on TEMPOL/H(2)O solutions at room temperature.

13 o 1:5 (Z) for the monoacetylated products at room temperature.

14 of >4 kb at a rate of ~200 bp per second at room temperature.

15 lexes (n != 10) show sizable luminescence at room temperature.

16 emical catalysis facilitates the reaction at room temperature.

17 s well as thermal initial state evolution at room temperature.

18 l Hg(0) concentration of 260-300 mug/m(3) at room temperature.

19 2) upon exposure to mTorr pressures of CO at room temperature.

20 macroscopic quantum phenomena observable at room temperature.

21 n of injectable PEDOT:PSS hydrogel fibers at room temperature.

22 ent value of ~0.3 at 10 kHz were obtained at room temperature.

23 he subthreshold swing of 60 mV decade(-1) at room temperature.

24 100 ppm) and reaction temperatures as low as room temperature.

25 implified storage and shipping conditions at room temperature.

26 etic Weyl semimetal candidate, Co(2)MnAl, at room temperature.

27 up to 18% under continuous-wave condition at room temperature.

28 ing for the fixation of a temporary shape at room temperature.

29 1 and 2) display a bowl-to-bowl inversion at room temperature.

30 en be spontaneously assembled upon mixing at room temperature.

31 ble of reversible Ca deposition/stripping at room temperature.

32 edium before deswelling either at 31 C or at room temperature.

33 rent is achieved in Bi(2) WO(6) /SrTiO(3) at room temperature.

34 nds is limited by their lack of stability at room temperature.

35 1-2 mol% catalyst loading and operational at room temperature.

36 cases, these reactions can be carried out at room temperature.

37 ered substrates, the reaction can proceed at room temperature.

38 uency to scatter heat-carrying phonons up to room temperature.

39 motifs and that assembly can be performed at room temperature.

40 gold from the surface of activated carbon at room temperature.

41 des (1.0 equiv) in dichloromethane (3 mL) at room temperature.

42 ntain functionality for at least 4 months at room temperature.

43 d into a Mobius strip or a simple origami at room temperature.

44 into its quantum ground state of motion from room temperature.

45 lly obtained for X = H and F after a week at room temperature.

46 ffectively retain small gaseous molecules at room temperature.

47 and antiferromagnetic phases are bistable at room temperature.

48 nt conditions, manifesting ferromagnetism at room temperature.

49 e an order of magnitude hyperpolarisation at room temperature.

50 for excellent photodetecting performances at room temperature.

51 an amide carbonyl oxygen atom in solution at room temperature.

52 d its OLPL duration reaches more than 1 h at room temperature.

53 ultiferroic (ferroelectric-ferromagnetic) at room temperature.

54 the molecules neither diffuse nor rotate at room temperature.

55 and that they are stable for up to 5 days at room temperature.

56 ncluding melting point and physical state at room temperature.

57 namics contribute to Lithium-ion mobility at room temperature.

58 he transition can be tuned to occur close to room temperature.

59 anol (1:1 v/v) and 0.2 m KHCO(3) solution at room temperature.

60 6.5 x 10(10) cm Hz(1/2) W(-1) at 1.55 mum at room temperature.

61 F, and moderate activity toward C-F bonds at room temperature.

62 Switching behavior persists from 15 K up to room temperature.

63 ic separation of all three xylene isomers at room temperature.

64 ed, even 90 min in the presence of oxygen at room temperature.

65 d mutual isomerization or remained intact at room temperature.

66 the direct detection of thermal neutrons at room temperature.

67 PhINTs as a nitrene (NT) source in water at room temperature.

68 nductivities of less than 1 W.m(-1).K(-1) at room temperature.

69 y of (4.2 +/- 1.2) x 10(-27) N m Hz(-1/2) at room temperature.

70 avior with a remarkably high conductivity at room temperature.

71 Seebeck coefficient 390 (+/-10) muV K(-1) at room temperature.

72 c C-H bonds and alpha-C-H bonds of ethers at room temperature.

73 nce with 2% quantum yield in acetonitrile at room temperature.

74 .020) starch with 3% OSA and 4-h reaction at room temperature.

75 ow a reversible structural transformation at room-temperature.

76 universal hydrodynamic description, even at room temperature(1,2).

77 A new approach for room-temperature (17)O enrichment of zeolites reveals a

78 3 degrees C and 37 degrees C) and reduced at room temperature (22 degrees C).

79 spin-crossover in solution with T(1/2) above room temperature (300-368 K).

80 f-life of anthocyanin in the microcapsule at room temperature (37 degrees C) clearly indicated greate

81 successful structure solution achieved from room-temperature 3D-ED data with a resolution as low as

82 in charge-neutral, high-mobility graphene at room temperature(4).

83 v), using dichloromethane as the solvent, at room temperature, 4-methylene-3-(organoselanyl)-selenoch

84 mate a detection limit of 700 nT Hz(-1/2) at room temperature, 80 nT Hz(-1/2) at 4.2 K, and 3 muT Hz(

85 At room temperature, a polymeric network of units is create

86 At room temperature, a submicrometre whisker grows under an

87 , when doped into the commercially available room-temperature achiral liquid crystal host 5CB, which

88 The two catalysts had similar initial room-temperature activities per Rh atom for ethylene con

89 In this work we describe a simple, room-temperature, ambient method to visualize real-space

90 a record value ([Formula: see text]) at the room temperature among magnetic conductors.

91 A room temperature amorphous ferromagnetic oxide semicondu

92 nsitions with programmable waveforms between room temperature and 45 degrees C with an air objective.

93 ollably varied over 3 orders of magnitude at room temperature and 6 orders of magnitude from 10 to 30

94 rs of the migrants, whereas the temperature (room temperature and 60 degrees C) did not show signific

95 To this end, tunable ferromagnetism at room temperature and a thermally induced spin flip (TISF

96 including a large exciton binding energy at room temperature and a very small piezoelectric coeffici

97 s is introduced, which gives good results at room temperature and above, and for mobilities as low as

98 ica-silicon conversion becomes reversible at room temperature and accessible within a narrow potentia

99 This process is facile at room temperature and allows for the generation of highly

100 of the position accuracy below lambda/300 at room temperature and ambient conditions.

101 e bulk CuO, PbO, and Sb(2)S(3) precursors at room temperature and ambient pressure to generate an ink

102 nm crystalline imine-based COF particles at room temperature and ambient pressure.

103 hydrogenation of unsaturated hydrocarbons at room temperature and atmospheric pressure has been perfo

104 VE-1-Ni adsorbs propylene but not propane at room temperature and atmospheric pressure, whereas the i

105 ements, which are are routinely performed at room temperature and below, in materials with mobilities

106 using a universal reaction condition, i.e., room temperature and constant ionic concentration.

107 The reaction can be carried out at room temperature and employs readily available reagents;

108 that these manipulable defects are stable at room temperature and feature enhanced functionalities, a

109 407-CM-T solution is an injectable liquid at room temperature and gels near body temperature.

110 ility, is present and substantial already at room temperature and grows by an order of magnitude upon

111 d is recoverable and suitable for working at room temperature and in a wide range of humidity levels.

112 ntegration, flexibility, good workability at room temperature and in severe environments, etc.

113 r hydrogen adsorption on MoSe(2) deposits at room temperature and insight into the possible active si

114 This material can be facilely synthesized at room temperature and is water stable, highlighting FeNi-

115 minoxidil nanofiber was stable if stored at room temperature and protected from light with only loss

116 hieving a limit of detection of 0.01 vol% at room temperature and sensitivity up to 1.9 nm vol%(-1) ,

117 nd in body-centered cubic (Bcc) metals under room temperature and slow strain rates.

118 lms also display low thermal conductivity at room temperature and strongly favors achievement of high

119 ormed from the cubic phase during cooling to room temperature and subsequently deforms in compression

120 results can then be erased by cooling below room temperature and the material repeatedly re-patterne

121 of the phenylene ring at temperatures above room temperature and thus may be considered the first cr

122 tion of biologically diverse 2H-indazoles at room temperature and under ambient air.

123 with respect to amorphous silica at pH = 9, room temperature and under anoxic conditions.

124 ation or protein enzymes, while operating at room temperature and with single base-pair resolution.

125 onal redox probe in the aqueous solution (at room temperature and without addition of surfactant) is

126 btained shortly after deposition was kept at room temperature and yielded 3.760 L of water, which was

127 endent PL linewidth and PL lifetime (between room temperature and ~5 K).

128 ances in terms of storage (up to 3 months at room temperature) and working (up to 25 measurements on

129 gnetization of 3.5 emu/cm(3) was observed at room temperature, and it retains ferromagnetic ordering

130 Each stage of the process is performed at room temperature, and the total reaction time is only 1.

131 ability to withstand heat stress, storage at room temperature, and three freeze-thaw cycles.

132 eport the demonstration of an aqueous-phase, room-temperature approach to CdS MSCs, together with an

133 When a room temperature aqueous solution containing 10 uM myogl

134 ur findings show there is a viable avenue to room-temperature aqueous-phase formation of CdS MSCs.

135 s remain isolated because microwave links at room temperature are noisy and lossy.

136 m light-emitting diodes, affords radicals at room temperature as observed by electron paramagnetic re

137 ws access to both traditional C-N adducts at room temperature as well as a large range of previously

138 (100 ms), followed by fast quenching back to room temperature at a cooling rate of 10(5) K/s to inhib

139 ompetitive epimerization (>30:1 dr), and two room-temperature atroposelective intramolecular S(N)Ar c

140 nductor optomechanical resonator >20 K below room temperature based on the emission of upconverted, a

141 tten information is stable during reading at room temperature, but it can also be erased at will, ins

142 hibit higher thermoelectric performance near room temperature by eliminating grain boundary resistanc

143 mage viscous Dirac fluid flow in graphene at room temperature by measuring the associated stray magne

144 ot only determined during growth but also at room temperature by post-processing.

145 that manifests as triggering of seizures at room temperature by the GABA(A) receptor (GABA(A)R) posi

146 ermitian-controlled chiral light emission at room temperature can be further scaled up for simultaneo

147 ic deformation under triaxial compression at room temperature can rejuvenate bulk MG samples sufficie

148 aboratory settings and that operates at near room temperature, can enhance Temozolomide (TMZ) cytotox

149 an intramolecular, benzylic C-H amination at room temperature, chemical reduction of ((tBu)dmx)Cu(2)(

150 tures up to 242 degrees C and a 7500-oersted room-temperature coercivity.

151 to show large anomalous Hall effect (AHE) at room temperature comparable to ferromagnets.

152 ide electrochemical stability window, a high room-temperature conductivity of 1.5 x 10(-4) S cm(-1) ,

153 enerate unconventional spin-orbit torques at room temperature corresponding to out-of-plane and Dress

154 isotropic first-order phase transition near-room temperature, corresponding to a 4% volumetric chang

155 We argue that the primary amine facilitates room-temperature decomposition of thiourea when CdCl(2)

156 Observation of the THz AHE at room temperature demonstrates the ultrafast readout for

157 es integrated on flexible polymers, enhanced room-temperature dielectric permittivity with large mech

158 e high external quantum efficiency of ~6% at room temperature due to efficient recombination of injec

159 sphates to react with organozinc reagents at room temperature during palladium-catalyzed reactions.

160 The room temperature electric polarization is comparable to

161 The proposed liquid-metal-based room-temperature electrochemical route can be expanded t

162 Notably, however, the room-temperature emission efficiency and the fluorescenc

163 ata transfer between cryogenic (0.1-4 K) and room temperature environments is essential for the reali

164 le quantum wells (IO-MQWs) show utility from room-temperature exciton emission features (binding ener

165 ))(0.5)((Bi,Sm)(2)O(3))(0.5), we demonstrate room temperature ferroelectricity and ferromagnetism wit

166 ttern of octahedral rotation leads to robust room-temperature ferroelectricity in CaTiO(3), which is

167 However, no spontaneous room-temperature ferroic property has been observed to d

168 Our recent discovery of the strong room temperature ferromagnetism in single layers of VSe(

169 cyclic double bond is hindered, resulting in room-temperature fluorescence.

170 ring real-time storage in dark conditions at room temperature for 22 months.

171 high internal quantum efficiency of ~52% at room temperature for emission at 295 nm.

172 ](2) , which is stable in the solid state at room temperature for extended periods (48 h).

173 ve enzymes was observed, with no browning at room temperature for more than 3 days.

174 Finally, it is demonstrated that these room-temperature-formed PEDOT:PSS hydrogels (RT-PEDOT:PS

175 icon-based manufacturing methodologies, this room-temperature gas sensing array can be fabricated rep

176 one thousand bending cycles and exceptional room-temperature gas sensing performance.

177 DOT:PSS hydrogels by taking advantage of the room-temperature gelation property of PEDOT:PSS.

178 al emitter within nanometer distances from a room-temperature germanium photodetector to form a therm

179 toriously difficult-to-study drug targets at room temperature, has now been adapted for use in synchr

180 best known thermoelectric material for near room temperature heat-to-electricity conversion is bismu

181 This manipulation could be accomplished at room temperature; hence this opens avenues for magnetoop

182 elds remarkable device performance featuring room temperature high sensitivity (NEP of 82 pW[Formula:

183 he latter is capable of chemisorbing O(2) at room temperature in a highly selective manner.

184 l presented here allows to synthesize GeH at room temperature in a significantly shorter time (a few

185 ursor quantities and short reaction times at room temperature in a wide range of solvents while also

186 west (S(1) ) singlet excited states, even at room temperature in air.

187 design to oxidise an L-proline derivative at room temperature in continuous flow.

188 sted by a catalytic amount of NaF, occurs at room temperature in EtOAc, where XtalFluor-E behaves as

189 ide range of chloroarenes with B(2)pin(2) at room temperature in excellent yields and with high selec

190 roalanines have been assessed effectively at room temperature in good to excellent yields without nee

191 The reaction proceeds at room temperature in high yields and is applicable to a b

192 Magnetoelectric coupling at room temperature in multiferroic materials, such as BiFe

193 greater than 1600 watts per meter-kelvin at room temperature in samples with enriched (10)B or (11)B

194 experiments pave the way for more ambitious room temperature in situ dynamic nuclear polarisation st

195 omplexes have displayed emission >1000 nm at room temperature in solution up to now.

196 ooling, the TADF mechanism takes over around room temperature in solution when the aggregates dissolv

197 endothermicities in the range 5-10 k(B)T at room temperature in solution.

198 alization of tree-like conductance states at room temperature in strongly correlated perovskite nicke

199 olymerize under visible-light irradiation at room temperature in the absence of a catalyst.

200 (111), to produce CO(2), was investigated at room temperature in the mTorr pressure regime.

201 king it possible to realize quantum gates at room temperature in these systems.

202 ange that stabilizes sub-100 nm skyrmions at room temperature in zero field.

203 ection, with no signal loss after 14 days at room temperature, in contrast to PCR that showed signifi

204 mpregnated 2D and 3D COFs show a significant room-temperature ion conductivity of 1.8 x 10(-4) S/cm a

205 Multiplexed gas detection at room temperature is critical for practical applications,

206 sembled nanostructures on bulk insulators at room temperature is crucial towards the fabrication of f

207 xcitons in a disordered organic thin film at room temperature is demonstrated, where the major fracti

208 luoromethylation of beta-ketodithioesters at room temperature is reported.

209 The magnetic hardness parameter of 3.7 at room temperature is the highest observed for any rare-ea

210 At room temperature, isobutanal is obtained selectively fro

211 In storage at room temperature, it presents a short shelf life due to

212 oach to measure site-specific dynamics using room temperature lineshape analysis.

213 e deep-eutectic K-Na alloying approaches for room temperature liquid anodes.

214 We visualize, at room temperature, long-range incoherent transport of del

215 Correspondingly, the room-temperature magnon BEC differs essentially from oth

216 nsition-metal oxide that demonstrates a near-room-temperature metal-insulator transition that may be

217 A rapid metal- and additive-free room temperature method for C(sp(2))-H thiocyanation of

218 vantages of the reaction include metal-free, room-temperature, mild reaction conditions and broad fun

219 Thermodynamic characterization indicates a room-temperature miscibility for D18:Y6 and D18:IT-4F ne

220 er activity indicate that products stored in room temperature must be protected against the influence

221 Here, we combine room-temperature nano-optical imaging and spectroscopic

222 Here, we present the room-temperature neutron structure of 3CL M(pro), which

223 We demonstrate strong room-temperature nonlinear excitation intensity dependen

224 e kinetically trapped, enabling atomic-scale room-temperature observations.

225 ic, large-scale, color tunable, and low-cost room-temperature OLPL applications become possible.

226 However, present room-temperature OLPL emitters are mainly based on a bim

227 hes for production of metallic structures at room temperature, on-demand fluid-in-fluid structuring,

228 mal conductivity of about 4 W m(-1) K(-1) at room temperature, one order of magnitude smaller than Ga

229 species can be densely covering surfaces at room temperature only when in equilibrium with a suffici

230 uality factor (Q(E) ~ 7.4) and off resonant, room temperature operation, we are able to parametrize s

231 lly in diamond anvil cells (up to 157 GPa at room temperature) or dynamically by laser-generated shoc

232 t Hall sensors reported in the literature at room temperature, outperform other Hall sensors at 4.2 K

233 trical conductivity of up to 10(-2) S/cm and room-temperature paramagnetic behavior with a spin conce

234 Long-lived room temperature phosphorescence from organic molecular

235 dots were designed and fabricated, enabling room temperature phosphorescence material with simultane

236 However, it is hard to achieve a room temperature phosphorescence material with simultane

237 a universal strategy to construct metal-free room temperature phosphorescence materials with ultralon

238 mally activated delayed fluorescence (TADF), room-temperature phosphorescence (RTP), mechanoluminesce

239 Room temperature photolysis of the bis(azide)cobaltate(I

240 Even higher room-temperature proton conductivity of 1.7 x 10(-2) S/c

241 cal predictions show that upconversion-based room-temperature receivers can outperform state-of-the-a

242 rganic perovskite CsPbI(3) to be unstable at room temperature remain mysterious, especially since man

243 ching about 4 and 6 microvolts per kelvin at room temperature, respectively, close to the highest val

244 and silicon oxide are used to obtain stable room-temperature responses to ammonia (NH(3) ), hydrogen

245 al DMI in TI/ferrimagnet heterostructures at room temperature, resulting in small-size (radius ~ 100

246 ota data from unstabilized samples stored at room temperature (RT) and samples placed in PERFORMAbiom

247 stals, thereby reducing damage, has rendered room temperature (RT) data collection more practical and

248 Here, room-temperature (RT) diffusion coefficients of 3.4 x 10

249 vskites are remarkable because of the robust room-temperature (RT) performance, broad wavelength tuna

250 modes or charge transfer, and are limited to room-temperature samples containing no liquids.

251 Room-temperature sonication of digenite (Cu(1.8)S) in tr

252 rystallographic unit cell to give 1.CHD as a room temperature stable product.

253 intestinal microbiome effects of RBX7455, a room temperature-stable, orally administered investigati

254 sent the synthesis and characterization of a room-temperature-stable compound with two separated two-

255 in H(3) S at 203 K marked an advance towards room-temperature superconductivity and demonstrated the

256 enable the preservation of the properties of room-temperature superconductivity at lower pressures.

257 n experimental physics is the observation of room-temperature superconductivity(1,2).

258 Room-temperature synthesis of 2D graphitic materials (2D

259 Here, a room-temperature technique for the synthesis of a variet

260 in basal activity and agonist sensitivity at room temperature than the Pro to Gln substitution in the

261 Owing to sluggish kinetics at room temperature, the spinel phase coexists with the tet

262 cal plating of Li above 0 V vs. Li(0)/Li(+) (room temperature) thermodynamically favorable.

263 polymerization of different cyclic esters at room temperature; they are among the most active metal-f

264 that occurs over hundreds of picoseconds at room temperature, three orders of magnitude slower than

265 This paper presents a study of noise in room-temperature THz radiometers that use THz-to-optical

266 s can outperform state-of-the-art cooled and room-temperature THz receivers based on low-noise amplif

267 pulsion of dinitrogen (N(2)) was observed at room temperature to afford a ligand functionalized produ

268 turn undergo spontaneous C-C homocoupling at room temperature to furnish symmetrical (bis)aryls in go

269 diradicaloid 4 readily splits dihydrogen at room temperature to yield the elusive bis-hydridogermyle

270 emonstrated exciting properties such as near-room-temperature topological insulation in bismuthene, e

271 -assembled molecular-electronic films, whose room-temperature transport properties are controlled by

272 talyst for OCM in a flow reactor operated at room temperature under atmospheric pressure for the firs

273 These reactions occur at room temperature under visible light irradiation and are

274 undec-7-ene (DBU) as a base, and proceeds at room temperature under visible light irradiation.

275 e, light-induced tuning of ferromagnetism at room temperature using a halide perovskite/oxide perovsk

276 non modes with previous measurements made at room temperature using inelastic X-ray scattering and ne

277 classes that are not effectively coupled at room temperature using previous catalysts, led to the de

278 ow as 6 x 10(-5) RIU) in bulk RI of gases at room temperature, using a high-resolution LSPR spectrosc

279 charge carriers on phonon heat transport at room temperature, using a modified transient thermal gra

280 Here we report the structure of TbIMPDH at room temperature utilizing free-electron laser radiation

281 Here, we demonstrate room-temperature voltage-driven nitrogen transport (i.e.

282 f pectin fractions respectively extracted by room temperature water, 90 degrees C-water, CDTA and Na(

283 rature is thickness-dependent and approaches room temperature when the layer is thin.

284 The entanglement persists at room temperature, where we verify the inseparability of

285 i-metallic transport behavior is observed at room temperature, whereas at low temperature, the pGNRs

286 ts contribute to this breadth in solution at room temperature, which raises the question as to what t

287 Later, pH detection was conducted at room temperature, which showed an impressive sensitivity

288 Pentoses are readily converted at room temperature, while hexoses and their oligosaccharid

289 ing peptides underwent conjugate addition at room temperature, while Z-DeltaAbu- and DeltaVal-contain

290 lfate (CH(3)OSO(3)H) at ambient pressure and room temperature with a molecular catalyst of vanadium (

291 The charges are found to be highly stable at room temperature with a trapping energy barrier of ~2 eV

292 y-quantum cascade laser (EC-QCL) operated at room temperature with an optimized double-beam optical s

293 cids reacted in a self-catalyzed reaction at room temperature with ketones, imines, and indoles to gi

294 It operates at near room temperature with light as the source of energy.

295 ) and a specific activity of 9.3 mA/cm(2) at room temperature with only 15.9% loss of mass activity a

296 ition step occurred in less than a minute at room temperature with total regioselectivity toward indo

297 dband sensitive photoresponse is realized at room temperature, with excellent stability without degra

298 ructures capable of maintaining 3D shapes at room temperature without the need for any actuation are

299 Here we report the room temperature X-ray structure of unliganded SARS-CoV-

300 provides a measurement of the high-pressure, room temperature Xe and CO(2) sorption isotherms.