ライフサイエンスコーパス: formula

1 2+) or Pb(2+)) which is double of the AMX(3) formula.

2 ter and mire diameters using the Imbert-Fick formula.

3 te the absolute error for each eye with each formula.

4 spectively based on a previously established formula.

5 rcerated cases was estimated through Levin's formula.

6 culated as 22 ng/mL (n = 6) using the 3 Sb/m formula.

7 e error (0.31D versus 0.51D) than the Haigis formula.

8 cribed at the molecular level using chemical formulas.

9 the clinician by incorporating a variety of formulas.

10 las were ranked as follows: Kane keratoconus formula (0.81 D), SRK/T (1.00 D), Barrett Universal 2 (1

11 er 1.73 m(2) (IQR, 74-100) using the CKD-EPI formula, 30% had microalbuminuria, and 32% had diabetes.

12 w hybrid manganese bromides with the general formula A(m)MnBr(4) [m = 1 or 2, A = dimethylammonium (D

13 2D hybrid halide perovskites with the formula (A')(2) (A)(n) (-1) Pb(n) I(3) (n) (+1) have rem

14 d human milk oligosaccharides (HMOs) as baby formula additives, and interestingly also as dietary sup

15 e involvement was calculated using the Roach formula and compared with the PSMA PET/CT results.

16 ed refraction was calculated for each of the formulas and compared with the actual refractive outcome

17 refraction and IOL power predictions for all formulas and lenses (P < .05).

18 past decade, so many new optical biometers, formulas, and methods (whose accuracies have yet to be c

19 those in infants consuming soy-based infant formulas are infertile due in part to uterine implantati

20 ing steps such as noise removal or molecular formula assignment is growing, but an integrative tool w

21 lements, the tool offers high flexibility in formula attribution.

22 The analytical formula-based FFD method can potentially allow a multipl

23 the same data that were used to develop the formula being tested.

24 This novel concept of infant formula composition has given rise to concern and contro

25 When the modified Haigis-L formula considering spherical aberration for 8.0 mm prod

26 and total soluble fluorides (TSF) in 5 child formula dentifrices (CFD) using Inter-method reliability

27 Patients were randomized to receive a formula diet containing 60% of daily energy requirement

28 al supplementation (3 sachets/d) of either a formula enriched with l-arginine and omega-3 (n-3) fatty

29 m ~10 to 80%, with the highest estimated for formula-fed infants (age 0 to <1 year).

30 The essential amino acid requirements of formula-fed infants have been reassessed recently, enabl

31 tpartum women who were lactating (n = 12) or formula-feeding (n = 6) their infants and who were close

32 daily with 2.5 mg/kg ethanol or control milk formula for 5 d or from hypothalamic microglia cells obt

33 entropy-related barrier, we derive a simple formula for virus inactivation time as a function of tem

34 gnificantly improved in the immunomodulating formula group (81%; 95% CI: 67%, 89%) compared with cont

35 7 wk was equivalent between the mLP and CTRL formula groups (27.9 and 28.8 g/d, respectively; differe

36 ne keratoconus formula was the most accurate formula in this series.

37 ding the benefit of one formula over another formula intended for CMA management.

38 tic technology, new toric IOLs, updated lens formulas, intraoperative guidance, and advanced imaging

39 theless, feeding a "very-low" protein infant formula may cause limited protein synthesis during a pha

40 of intraocular lens (IOL) power calculation formulas, methods, and instruments.

41 ts of adding cropped rice straw to substrate formulas on the proximate composition and non-volatile t

42 n to be reached regarding the benefit of one formula over another formula intended for CMA management

43 , a series of phosphonium boranes of general formula [p-RPh(2) P(C(6) H(4) )BMes(2) ](+) have been sy

44 Feeding with breastmilk as opposed to formula reduces incidence of NEC.

45 Data on breastfeeding, consumption of infant formula (regular, pre-/probiotics, partially hydrolysed

46 We provide a simple formula relating AIS geometry and sodium conductance den

47 All normal IOL formulas resulted in hyperopic refractive outcomes that

48 F/DeltaT) was calculated using the following formula: (SBF37-SBFBT)/(37-basal temperature).

49 ), and we derive a cosmic baryon density of [Formula: see text] (95 per cent confidence; h(70) = H(0)

50 at a concentration [Formula: see text] 0.01 [Formula: see text] ([Formula: see text]).

51 erfaces, the stiffnesses were 0.15 and 0.18 [Formula: see text] (sigma: particle diameter), respectiv

52 (normal insulator) and [Formula: see text] [Formula: see text] (topological insulator).

53 f these complexes was entropically driven ( [Formula: see text] , [Formula: see text] KJ mol(-1)).

54 75 and 70%, respectively at a concentration [Formula: see text] 0.01 [Formula: see text] ([Formula: s

55 ); [Formula: see text] = -32.22 kJ mol(-1); [Formula: see text] = -31.84 kJ mol(-1)).

56 ( [Formula: see text] = -33.42 kJ mol(-1); [Formula: see text] = -32.22 kJ mol(-1); [Formula: see te

57 r values of DeltaG( degrees ) for binding ( [Formula: see text] = -33.42 kJ mol(-1); [Formula: see te

58 ch, we predict personality at broad domain ([Formula: see text] = 0.37) and narrow facet levels ([For

59 see text] = 0.37) and narrow facet levels ([Formula: see text] = 0.40) based on behavioral data coll

60 estimate a generalized reproduction number ([Formula: see text] = 3.60 [3.49 to 3.84]), the spectral

61 rostructures of GeTe (normal insulator) and [Formula: see text] [Formula: see text] (topological insu

62 as the appearance of Pauli paramagnetism in [Formula: see text] A unified and systematic picture of t

63 density functional theory (DFT) to resolve [Formula: see text] adsorption on the rutile [Formula: se

64 le and conclude that it is limited by the CO[Formula: see text] adsorption step.

65 t [Formula: see text] and successive boosts [Formula: see text] and [Formula: see text] and check the

66 e constants and level isotope shifts of the [Formula: see text] and [Formula: see text] states were d

67 the very large ordered magnetic moments in [Formula: see text] and [Formula: see text], the availabi

68 d successive boosts [Formula: see text] and [Formula: see text] and check their consistency with Thom

69 urface reconstructions from repeated US was [Formula: see text] and from US and CT was [Formula: see

70 during chemical weathering on land consumes [Formula: see text] and generates sulfate that is carried

71 ng dependence on the arbitrary scalar field [Formula: see text] and its kinetic term [Formula: see te

72 and splitting behaviors are observed at the [Formula: see text] and M points.

73 nt [Formula: see text], seed pulse duration [Formula: see text] and seed pulse amplitude a for the Ra

74 ic field tensors obtained by a direct boost [Formula: see text] and successive boosts [Formula: see t

75 ] by a factor of 2 to 19.2 nm, the measured [Formula: see text] and temperature distribution also inc

76 , we estimate the basic reproduction number [Formula: see text] and the overdispersion parameter [For

77 the energy balance equations to measure the [Formula: see text] and the temperature distribution of s

78 ent the detailed electronic structure of CrI[Formula: see text] and VI[Formula: see text] measured by

79 While CO, [Formula: see text], HCO, and [Formula: see text] are often abundant species in the col

80 d zones of the disk, [Formula: see text] or [Formula: see text] are only found in a few regions, and

81 tions (Delta'(17)O) of atmospheric O(2) and [Formula: see text] are primarily regulated by their rela

82 We show that even small saccades of just 14-[Formula: see text] are very effective in centering the s

83 he number of days being contagious, we find [Formula: see text] Assuming realistic contact networks w

84 ms per formula unit of ([Formula: see text])[Formula: see text] At pressures above 60 GPa, [Formula:

85 bubble collapses and releases metastable He[Formula: see text] at the droplet surface.

86 see text] and the overdispersion parameter [Formula: see text] at two regions in Indonesia: Jakarta-

87 we evaluate the GeTe-Sb[Formula: see text]Te[Formula: see text] band offset using X-ray photoemission

88 the EU ETS saved about 1.2 billion tons of [Formula: see text] between 2008 and 2016 (3.8%) relative

89 te the use of a 2-component ion circuit for [Formula: see text] bioenergetics and a 2nd 2-component i

90 magnetic moments of 10[Formula: see text]-10[Formula: see text] Bohr magnetons ([Formula: see text]).

91 By increasing the [Formula: see text] by a factor of 2 to 19.2 nm, the meas

92 d the bottlebrush correlation peak position [Formula: see text] by neutron scattering and in simulati

93 f a nontoxic dosage of GHz ultrasonic waves [Formula: see text] caused an average normalized fluoresc

94 ula: see text] matrix and magnetically hard [Formula: see text] cell walls.

95 ity with values ranging between 150 and 300 [Formula: see text] cm.

96 t] A unified and systematic picture of the U[Formula: see text] compounds may now be drawn, thereby p

97 The amount of the U 5[Formula: see text] configuration, however, varies consid

98 vicinity of the boundaries, manifest at all [Formula: see text] considered here, increasing with incr

99 ate of change (growth rate) in the trend of [Formula: see text] data such as the Keeling curve?

100 We achieve a metrological gain of [Formula: see text] decibels over the SQL by using an ens

101 ned "soft spots"-, which follow a universal [Formula: see text] density of states in the limit of low

102 The parameter [Formula: see text] describes the degree to which particl

103 dels with physical [Formula: see text] spin-[Formula: see text] electrons.

104 ns demonstrate that CA9 acts as a nonlinear [Formula: see text] equalizer at any [Formula: see text]

105 , suggestive of a pinned Wigner solid, when [Formula: see text] exceeds [Formula: see text] However,

106 Estimated [Formula: see text] fell below one again at the beginning

107 da(0) of an elastic medium is approximately [Formula: see text] for a >> d >> xi, [Formula: see text]

108 se amplitude a for the Raman seed pulse (or [Formula: see text] for Brillouin) must exceed a specific

109 4 meV/[Formula: see text] from about 42 meV/[Formula: see text] for SCAN.

110 heory successfully predicts the scaling law [Formula: see text] for the low-frequency shear modulus o

111 examer binding energies to less than 14 meV/[Formula: see text] from about 42 meV/[Formula: see text]

112 attice dynamics and superionic diffusion in [Formula: see text] from energy- and momentum-resolved ne

113 The observed [Formula: see text] has a positive correlation with tempe

114 lities as low as 10(-3) cm(2) V(-1) s(-1) , [Formula: see text] Here, mu(w) is the weighted mobility,

115 ner solid, when [Formula: see text] exceeds [Formula: see text] However, our sample makes a transitio

116 -lived radioisotopes [Formula: see text] or [Formula: see text] in one or more end-Devonian extinctio

117 O flux ranges from a low of 3.3 +/- 1.3 Tg N[Formula: see text] in the boreal spring to a high of 5.5

118 boreal spring to a high of 5.5 +/- 2.0 Tg N[Formula: see text] in the boreal summer.

119 e text], wherein the overall energy in ions [Formula: see text] increases by an order of magnitude.

120 ical power law of [Formula: see text] up to [Formula: see text] Intermittent fluctuations in the wall

121 ted experimentally for a Coulomb crystal of [Formula: see text] ions without descrystallising it.

122 itivity to quenched disorder characterizing [Formula: see text] is a consequence of this multiphase m

123 [Formula: see text] is an intermetallic compound with a b

124 The method to estimate [Formula: see text] is based on a sequential Bayesian met

125 ential Bayesian method, while the parameter [Formula: see text] is estimated by fitting the secondary

126 rators with respect to an orthonormal basis [Formula: see text] is not multiplicative on [Formula: se

127 Volume magnetometry indicates [Formula: see text] K with a magnetic coercive field of 3

128 entropically driven ( [Formula: see text] , [Formula: see text] KJ mol(-1)).

129 linear [Formula: see text] equalizer at any [Formula: see text] level in cells that grow in acidic ex

130 oys with a microstructure that comprises an [Formula: see text] matrix and magnetically hard [Formula

131 ude that the N-methylated analogs of HE and [Formula: see text] may be used as a scaffold for the des

132 c structure of CrI[Formula: see text] and VI[Formula: see text] measured by angle-resolved photoemiss

133 tly slower than the adiabatic expansion law [Formula: see text] Motivated by such observations, we pr

134 iction of our pure state to any atomic masa [Formula: see text] of diagonal operators with respect to

135 Given a binary tree [Formula: see text] of n leaves, each leaf labeled by a s

136 a giant effective piezoelectric coefficient [Formula: see text] of ~1098 picometers per volt with a h

137 dant species in the cold zones of the disk, [Formula: see text] or [Formula: see text] are only found

138 ting either of the long-lived radioisotopes [Formula: see text] or [Formula: see text] in one or more

139 xperiment to generate a weighted average of [Formula: see text] Our final result has a total uncertai

140 istinct respiratory enzymes, the ferredoxin:[Formula: see text] oxidoreductase (Rnf complex) and the

141 tor machine with linear kernel (0.780), and [Formula: see text] penalized logistic regression (0.780)

142 tion of strong bursts of neutrons and multi-[Formula: see text] photons by secondary processes now pr

143 reveal the presence of a Dirac state at the [Formula: see text] point of the Brillouin zone at 500 me

144 tive partial pressures, [Formula: see text]/[Formula: see text] Pyrite oxidation during chemical weat

145 monstrated to be 1,000-fold faster than the [Formula: see text] reaction while producing the same oxi

146 In this study, the [Formula: see text] reaction with reduced Hypocrea jecori

147 Electrochemical CO[Formula: see text] reduction is a potential route to the

148 d systems, especially those controlled by a [Formula: see text] renormalization group (RG) fixed poin

149 n, however, varies considerably across the U[Formula: see text] series, indicating an increase of U 5

150 7)O as a proxy for past [Formula: see text]/[Formula: see text] should consider both 1) alternative o

151 from breast cancer cells, yet showed other [Formula: see text] signals in LECs suggesting internaliz

152 We test this hypothesis with more than [Formula: see text] simulated particles with a range of a

153 successfully grown centimeter-sized layered [Formula: see text] single crystals under high oxygen pre

154 A concordance score was calculated as [Formula: see text] so that a higher score reflects great

155 t] symmetric models to models with physical [Formula: see text] spin-[Formula: see text] electrons.

156 otope shifts of the [Formula: see text] and [Formula: see text] states were determined for [Formula:

157 compounds with the tetragonal body-centered [Formula: see text] structure.

158 Employing epitaxial stress on rutile [Formula: see text] substrates, the transition can be tun

159 then achieved direct bonding between two Au [Formula: see text] surfaces operating at 200 degrees C f

160 us transition to a ferromagnetic state when [Formula: see text] surpasses 35, and then a phase with s

161 viously established in the large-M limit of [Formula: see text] symmetric models to models with physi

162 ahn-Teller distortion even for this layered [Formula: see text] system.

163 isorder are the origin of intrinsically low [Formula: see text] The breakdown of short-wavelength TA

164 The field equations for the resulting [Formula: see text] theory are obtained and show that par

165 Recently introduced [Formula: see text] theory is generalized by adding depen

166 seudo spin-valve devices based on amorphous [Formula: see text] thin films.

167 with a predicted increase of 0.03 (o)C for [Formula: see text] This paper paves the experimental fra

168 transformations at symmetric and asymmetric [Formula: see text] tilt GBs in elemental copper.

169 sion spectrum in the wavelength regime from [Formula: see text] to 12 [Formula: see text]m by adjusti

170 s of freedom needed for the hidden order in [Formula: see text] to occur, as well as the appearance o

171 ChIP assays showed enhanced binding of NF-[Formula: see text] to the Mef2c promoter.

172 Above [Formula: see text] traditional epidemiological dynamics

173 [Formula: see text] undergoes a crystalline transition at

174 ransport-follows the classical power law of [Formula: see text] up to [Formula: see text] Intermitten

175 ynamics and thermal conduction mechanism in [Formula: see text] We find that the heat-carrying long-w

176 is is done by first decorating each node of [Formula: see text] with an alignment context using (x),

177 text] undergoes a crystalline transition at [Formula: see text] with large changes in its electric co

178 Formula: see text] adsorption on the rutile [Formula: see text](110) surface, which presents a longst

179 nergies between the ionic liquid molecules ([Formula: see text]) and between the ionic liquid and wat

180 ations result in statistically significant ([Formula: see text]) correlation of 0.66/0.73/0.58 with t

181 However, investigation of potassium-ion (K[Formula: see text]) dynamics in materials using e.g. NMR

182 d at cryogenic temperature, a cold neutron ([Formula: see text]) flux of [Formula: see text]/pulse wa

183 tween the ionic liquid and water molecules ([Formula: see text]) for the [EMIM][MeSO(3)]/water binary

184 insically low lattice thermal conductivity ([Formula: see text]) in superionic conductors is of great

185 rger than that between the water molecules ([Formula: see text]) in the [EMIM][MeSO(3)]/water system.

186 lic compound with a bulk Curie temperature ([Formula: see text]) of 6-13 K.

187 setting at high pressures and temperatures ([Formula: see text]) places important limitations on our

188 is a signature of the passive parity-time ([Formula: see text]) symmetry breaking transition in the

189 It is also larger ([Formula: see text]) than a similarly adjusted total from

190 e-derived estimate is significantly larger ([Formula: see text]) than US national emissions for 2010

191 lative humidities (0-90%) and temperatures ([Formula: see text]) using gravimetric type dynamic vapor

192 en the [EMIM][MeSO(3)] and water molecules ([Formula: see text]) was found to be in the range of 45~4

193 tomography from 83 subjects (49 M/34 F, BMI [Formula: see text]) was used to derive two statistical s

194 le forms around the localized excitation (He[Formula: see text]) within 1 ps.

195 Formula: see text]), flood incubation rate ([Formula: see text]), and recovery rate ([Formula: see te

196 pic characteristics-flood propagation rate ([Formula: see text]), flood incubation rate ([Formula: se

197 Antiprotons ([Formula: see text]), negative pions (- pai), and helium

198 e.g. aortic diameter ([Formula: see text], [Formula: see text]), were also substantially heritable,

199 e ([Formula: see text]), and recovery rate ([Formula: see text])-in a system of ordinary differential

200 her than the corresponding CT measurements ([Formula: see text]).

201 e higher than at any point in history (15.9 [Formula: see text]).

202 ormula: see text] 0.01 [Formula: see text] ([Formula: see text]).

203 text]-10[Formula: see text] Bohr magnetons ([Formula: see text]).

204 shly admitted to an engineering department ([Formula: see text]).

205 to 0.48 hydrogen atoms per formula unit of ([Formula: see text])[Formula: see text] At pressures abov

206 ; P=0.008) and 11.6 units during follow-up ([Formula: see text], 11.6 [95% CI, 4.1-19.2]; P=0.01) in

207 cy was increased by 13.7 units at baseline ([Formula: see text], 13.7 [95% CI, 6.3-21.7]; P=0.008) an

208 ric quantities alone; e.g. aortic diameter ([Formula: see text], [Formula: see text]), were also subs

209 t a resonant X-ray diffraction study of ZrTe[Formula: see text], a model CDW system, with focus on th

210 ately [Formula: see text] for a >> d >> xi, [Formula: see text], and D > 1, where a is the size of th

211 considered here, increasing with increasing [Formula: see text], and suggest that an abrupt transitio

212 We investigate monolayers of the form [Formula: see text], based on the known material [Formula

213 s, this ion gradient is usually composed of [Formula: see text], but it can also be composed of Na(+)

214 r[Formula: see text]CaCu[Formula: see text]O[Formula: see text], cleaved and annealed in ozone to inc

215 While CO, [Formula: see text], HCO, and [Formula: see text] are oft

216 n needed to decrease the viscosity to zero, [Formula: see text], large-scale collective motion emerge

217 in vivo LRP expressing mouse brain tumors ([Formula: see text], n = 10).

218 akes a transition to an insulating state at [Formula: see text], preceding the onset of the spontaneo

219 the triple product of the coupling constant [Formula: see text], seed pulse duration [Formula: see te

220 a slender cylindrical cell of aspect ratio [Formula: see text], that the Nusselt number-the dimensio

221 magnetic moments in [Formula: see text] and [Formula: see text], the availability of orbital degrees

222 ld [Formula: see text] and its kinetic term [Formula: see text], to explore non-minimal interactions

223 rmometer based on the phase change material [Formula: see text], to precisely map thermal contours fr

224 al animals with a mean average precision of [Formula: see text], under a variety of settings.

225 ula: see text], based on the known material [Formula: see text], using density functional theory (DFT

226 nversion efficiency at background pressures [Formula: see text], wherein the overall energy in ions [

227 ells are responsible for this behaviour for [Formula: see text], which also increases the probability

228 declines with the distance approximately as [Formula: see text], which is significantly slower than t

229 ld like, near a characteristic temperature, [Formula: see text], which rises with decreasing hole con

230 ear dispersion are expected to have at most [Formula: see text], which sets an upper limit to the mag

231 of Cd(3)As(2), KMgBi, and rutile-structure ([Formula: see text]-) PtO(2).

232 anoislands have giant magnetic moments of 10[Formula: see text]-10[Formula: see text] Bohr magnetons

233 Arm/[Formula: see text]-catenin family proteins contain a con

234 ss is crucial for generating networks whose [Formula: see text]-core decomposition is close to the em

235 Here we study the [Formula: see text]-core decomposition of some empirical

236 least k neighbours within the set, known as [Formula: see text]-core decomposition, has been used for

237 co analyses revealed that 1 ATP synthase is [Formula: see text]-dependent and the other Na(+)-depende

238 [Formula: see text]-labeled glucose experiments did not r

239 ased on exchange interactions inferred from [Formula: see text]-oriented high-field spin wave measure

240 rparts, and examine the extent to which the [Formula: see text]-shell structure of the networks can b

241 In this paper, we use [Formula: see text]-statistics to formulate a statistical

242 pose a microscopic mechanism leading to the [Formula: see text]-symmetric effective model in the cont

243 theoretical results by fitting the derived [Formula: see text]-Weibull distributions with data from

244 include those that have half-lives down to [Formula: see text].

245 at lower fields in BiCu[Formula: see text]PO[Formula: see text].

246 ibe the alignment of a dynamic homology for [Formula: see text].

247 [Formula: see text] and from US and CT was [Formula: see text].

248 Formula: see text] is not multiplicative on [Formula: see text].

249 n following the relaxation of O 1s holes in [Formula: see text].

250 intermediate timescales of a week to months [Formula: see text].

251 vestigation of the model was implemented in [Formula: see text].

252 iffusion of water on Bi[Formula: see text]Te[Formula: see text].

253 ical insulator (TI), Bi[Formula: see text]Te[Formula: see text].

254 measured by the 3D roughness parameter with [Formula: see text].

255 ulated by their relative partial pressures, [Formula: see text]/[Formula: see text] Pyrite oxidation

256 of sulfate Delta'(17)O as a proxy for past [Formula: see text]/[Formula: see text] should consider b

257 cold neutron ([Formula: see text]) flux of [Formula: see text]/pulse was measured at the proximity o

258 cted maximum detectivity D* = 1.5 x 10(9) cm[Formula: see text]/W and noise equivalent difference tem

259 rognostic biomarker of Bayley Motor scores ([Formula: see text]= -12.59 [95% CI -18.70, -6.48] R(2) =

260 a higher PASP than uninfected individuals ([Formula: see text]=1.10, 95% CI 0.01, 2.20) but there wa

261 of a QSL state in [EDT-TTF-CONH(2)](2) (+)[[Formula: see text]] (EDT-BCO), where the EDT molecules w

262 ctroscopy studies of Bi[Formula: see text]Sr[Formula: see text]CaCu[Formula: see text]O[Formula: see

263 rmula: see text] states were determined for [Formula: see text]In.

264 ength regime from [Formula: see text] to 12 [Formula: see text]m by adjusting the size of and distanc

265 Much of the seasonal variations in global [Formula: see text]O emissions can be traced to seasonal

266 Here, we reconstruct climatological [Formula: see text]O emissions from the ocean by training

267 This [Formula: see text]O flux ranges from a low of 3.3 +/- 1.

268 rmula: see text] At pressures above 60 GPa, [Formula: see text]O further changes the structural behav

269 rvised learning algorithm with over 158,000 [Formula: see text]O measurements from the surface ocean-

270 lack of knowledge on the state of matter in [Formula: see text]O-rich setting at high pressures and t

271 [Formula: see text]Sr[Formula: see text]CaCu[Formula: see text]O[Formula: see text], cleaved and anne

272 nic phases occurring at lower fields in BiCu[Formula: see text]PO[Formula: see text].

273 ved photoemission spectroscopy studies of Bi[Formula: see text]Sr[Formula: see text]CaCu[Formula: see

274 he heterostructures, we evaluate the GeTe-Sb[Formula: see text]Te[Formula: see text] band offset usin

275 al insight into the diffusion of water on Bi[Formula: see text]Te[Formula: see text].

276 surface of a topological insulator (TI), Bi[Formula: see text]Te[Formula: see text].

277 As a result, the prepared solid/colored formula serves as an ideal formulation for such instable

278 This formula simply counts the fraction of vertices that have

279 formulation for such instable drug in liquid formula taking the advantage of the attractiveness of be

280 the convergence of the estimator, deriving a formula that links the TBR estimation error variance wit

281 Other formulas that performed well in the short-eye subgroup w

282 e, the procedure requires only the molecular formula, the calculated energy, and C, H, O, and N atomi

283 To support the analysis, we derived a formula to estimate the occurrence of coamplification in

284 We apply this formula to marine snow formation following a phytoplankt

285 First, we show the ability of the formula to predict the uncertainty of the TBR estimate i

286 ations support up to 0.48 hydrogen atoms per formula unit of ([Formula: see text])[Formula: see text]

287 At amounts of DHA in infant formula up to ~0.64%, AA contents should at least equal

288 versus GFR estimation (eGFR) by the CKD-EPI formula versus both] is unclear.

289 The Kane keratoconus formula was the most accurate formula in this series.

290 Starting from the Kubo formula, we derive the analytical expressions for the DC

291 ed (n = 8.694). Based on indirect population formulas, we calculated body fat percentage (%BF) and sk

292 tical formulation of biocultural complexity, formulas were derived to measure the specificity of biol

293 C intensity and number of assigned molecular formulas were increased by 48% and 20%, as compared to t

294 Barrett toric calculator, or Barrett True-K formulas were not used.

295 he mean absolute prediction error (MAE), the formulas were ranked as follows: Kane keratoconus formul

296 ur-containing DBPs, with 43 unique molecular formulas, were found by high-resolution mass spectrometr

297 a 7 h enrichment or 100 g of powdered infant formula with a 16 h enrichment.

298 We aimed to assess the safety of an infant formula with a modified amino acid profile and a modifie

299 For this reason, using a low-protein formula with an amino acid composition modified accordin

300 They have the formula (xAMPY)M(2)I(6) (x = 3 or 4, M = Sn(2+) or Pb(2+