ライフサイエンスコーパス: formula

1 ng the Modification of Diet in Renal Disease formula.

2 ease, and lung cancer using the parametric g-formula.

3 D) of six sterilised model systems of infant formula.

4 ose-free foods including lactose-free infant formula.

5 lling for confounding using the parametric g-formula.

6 to help with development of improved infant formulas.

7 and young children are fed nutritional milk formulas.

8 mulas and casein components in one of the EH formulas.

9 ff-Kraff/theoretical, Holladay 2, and Haigis formulas.

10 mean (SD) result of the Dresdner correction formula (17.6 [4.1] mm Hg) was closer to the DCT measure

11 he analysis of vitamin B9 (folate) in infant formula and adult/pediatric nutritional products is pres

12 The g-formula and agent-based models (ABMs) are 2 approaches u

13 o bimetallic NPs with well-defined molecular formula and atomically-controlled alloying sites in prot

14 ebye-Frohlich model (combined with the Zhang formula and parabolic barrier approximation) and spin-de

15 beta-lactoglobulin were found in the two PH formulas and casein components in one of the EH formulas

16 e relative intensity of individual molecular formulas and reactive species production demonstrate the

17 The "Follow-on formula" and "Infant formula" products contained the low

18 re one source of exposure in infants fed soy formula, and they result in high serum concentrations.

19 In both cases analytical formulas are derived for the spin-orbit torques in a hea

20 hermal decomposition effects on the detected formulas are taken into account, formula-derived volatil

21 curacy of intraocular lens (IOL) calculation formulas (Barrett Universal II, Haigis, Hoffer Q, Hollad

22 In comparison with formula-based bolus resuscitation, both semiautonomous a

23 ed resuscitation systems and compare them to formula-based bolus resuscitation.

24 2+) counterions of a preformed chiral MOF of formula Ca6(II){Cu(II)24[(S,S)-hismox]12(OH2)3}.212H2O (

25 Our formula calculation and fits to the previous experimenta

26 ons occurring during sterilisation of infant formulas can affect protein digestibility and release of

27 ted in the first domain type, leading to sum formula Ce4-0.5xLi3P18N35-1.5xO1.5x (x approximately 0.7

28 Seasonal influenza vaccine formulas change almost every year yet information about

29 Inspection of the [m/z; chemical formula; collision cross section] data sets shows that t

30 by these methods with only 9.9% of molecular formulas common to both.

31 differences highlight that changes in infant formula composition impact infant metabolism, and show t

32 Soy-based formulas contained polyglutamates of 5-formyl-tetrahydro

33 The ABM and g-formula correctly estimated mortality and causal effects

34 For example, highly aromatic, tannin-like formulas correlate positively with triplet formation rat

35 CI] slope, 0.71-0.76), giving the conversion formula: (creatinine plasma concentration in mumol/L) =

36 he detected formulas are taken into account, formula-derived volatilities can be reconciled with the

37 wer calculations according to the Holladay 2 formula differed in prepresbyopic eyes (P = .042), and r

38 e predictions with the Holladay 2 and Haigis formulas differed significantly in prepresbyopic eyes (P

39 stration of an extensively hydrolyzed casein formula (EHCF) containing the probiotic Lactobacillus rh

40 ields, as waters enriched in highly aromatic formulas exhibit much higher rates of light absorption,

41 cute malnutrition in Uganda with therapeutic formulas F-75 and F-100, we collected data on symptoms,

42 Seven rhenium(I) complexes of the general formula fac-[Re(CO)3(NN)(OH2)](+) where NN = 2,2'-bipyri

43 th and 9 months of age from 50 girls (28 soy formula-fed and 22 cow formula-fed).

44 ested differences in methylation between soy formula-fed and cow formula-fed infants at three CpGs in

45 r LH level was found in urine samples of soy formula-fed girls compared to cow formula-fed girls.

46 les of soy formula-fed girls compared to cow formula-fed girls.

47 methylation between soy formula-fed and cow formula-fed infants at three CpGs in the gene proline ri

48 fed and formula-fed infants may differ, with formula-fed infants growing more rapidly than breastfed

49 Formula-fed infants had lower birth-weight z scores than

50 Growth patterns of breastfed and formula-fed infants may differ, with formula-fed infants

51 microbiome of breastfed infants compared to formula-fed infants.

52 from 50 girls (28 soy formula-fed and 22 cow formula-fed).

53 Mothers chose whether to breastfeed or formula feed their children.

54 Interestingly, infants starting formula-feed as early as first week of life have higher

55 ), pumping and feeding breast milk (BM), and formula (FF) in the first months" (DBF/BM/FF) showed a s

56 Avoidance of cow's milk-based formula for infants with genetic susceptibility for type

57 structure of Au279 follows the mathematical formula for magic number shells: Au@Au12@Au42@Au92@Au54,

58 While CIA assigns elemental formulas for compounds containing C, H, O, N, S, and P,

59 O, N, S, and P, IPA is capable of assigning formulas for compounds containing other elements.

60 e to reduce the number of possible molecular formulas for organic compounds of relative high molecula

61 al length range, and was comparable with the formulas for T2 (0.321 D) and Holladay 1 (0.326 D).

62 S) and based on the calculation of elemental formulas from accurate m/z values, was helpful to annota

63 The VRF formula had the lowest median (0.305 diopter [D]) absolu

64 The g-formula has been used exclusively to estimate effects in

65 Girls fed soy formula have altered DNA methylation in vaginal cell DNA

66 ition, Bray-Curtis dissimilarity analysis of formulas identified in the isolates and their size fract

67 similar set of compounds (>90% of molecular formulas identity) to the matrix assisted laser desorpti

68 , and lactose-free UHT milk (ULF) and infant formula (IF) using tandem mass spectrometry (electron tr

69 k (SMP), phosphocasein (PCN) and infant milk formula (IMF) powders were determined by inverse gas chr

70 agnosis of CMA and the use of hypoallergenic formula in infancy were associated with the later develo

71 gher resolutions favored ranking the correct formula in the top 10.

72 hat is dominated by products whose empirical formula is (C2H2) n(+), just like ionized acetylene clus

73 Annotation with predicted chemical formulas is also not implemented and semiquantification

74 OF allowed the detection of 25 different raw formulas matching with AAGs.

75 Derivation of these formulas motivates an interesting question: Is there an

76 larity due to the removal of photolabile DOS formulas not present in the ocean.

77 The actual formula of this compound is thus (CH3NH3)PbI3-2x(I2)x wh

78 A blinded analysis of eight CM formulas, one nonhydrolyzed, two partially hydrolyzed (P

79 Three different infant formulas (P1, P2 and P3) were characterised, and changes

80 The "Follow-on formula" and "Infant formula" products contained the lowest average content (

81 ed aromatic formulas, with CHON-type COO KMD formulas relatively more abundant in the purified subfra

82 a: see text] is the ambient temperature and [Formula: see text] ([Formula: see text] 91 K A) is a new

83 xponent varying from [Formula: see text] to [Formula: see text] (Brownian).

84 gy terms [Formula: see text](intra-atomic), [Formula: see text] (electrostatic) and [Formula: see tex

85 c), [Formula: see text] (electrostatic) and [Formula: see text] (exchange), in contrast to standard f

86 ajor lipophilic anions such as salicylate ( [Formula: see text] ) and thiocyanate ( [Formula: see tex

87 e ( [Formula: see text] ) and thiocyanate ( [Formula: see text] ).

88 ABC bottlebrush triblock terpolymers (chiAC [Formula: see text] 0), promotes organization into a uniq

89 00 [Formula: see text]m bubbles coated with [Formula: see text] 1 [Formula: see text]m particles is p

90 ial rheology and macroscopic dissolution of [Formula: see text] 100 [Formula: see text]m bubbles coat

91 avior was observed in the same material for [Formula: see text] 40 K.

92 II-like superconductor ([Formula: see text] [Formula: see text] 6.2 K) with a Ginzburg-Landau paramet

93 st Carboniferous and very low values of 100 [Formula: see text] 80 ppm for the earliest Permian.

94 mbient temperature and [Formula: see text] ([Formula: see text] 91 K A) is a new elastobaric coeffici

95 xt] 6.2 K) with a Ginzburg-Landau parameter [Formula: see text] = 1.18.

96 weak-coupling type-II-like superconductor ([Formula: see text] [Formula: see text] 6.2 K) with a Gin

97 Crack-free semi-polar [Formula: see text] Al x Ga1-x N epilayers with AlN conte

98 like crystals achieving the maximum value: [Formula: see text] Although finite temperature equilibri

99 mula: see text] columns (dimensions), where [Formula: see text] and [Formula: see text] are proportio

100 exposures from drinking water and rice were [Formula: see text] and [Formula: see text], respectively

101 rmula: see text] with unknown probabilities [Formula: see text] and [Formula: see text], which can be

102 of the past century, OCO-2 measurements of [Formula: see text] and fluorescence record the impact of

103 rable modes are prismatic <c>, prismatic-II [Formula: see text] and pyramidal-II <c + a>, which are d

104 ts with a time-of-flight viscometer down to [Formula: see text] and up to [Formula: see text], reveal

105 lues [Formula: see text] approximately 0.6, [Formula: see text] approximately 0.2, [Formula: see text

106 arable to the expected physiological values [Formula: see text] approximately 0.6, [Formula: see text

107 0.6, [Formula: see text] approximately 0.2, [Formula: see text] approximately 1, and [Formula: see te

108 2, [Formula: see text] approximately 1, and [Formula: see text] approximately 10-30 mM.

109 ed 4E binding protein 2 (4E-BP2) protein in [Formula: see text] are explained by an excluded volume e

110 uctural propensities of 4E-BP2 dissolved in [Formula: see text] are observed, while changes to DNA an

111 (dimensions), where [Formula: see text] and [Formula: see text] are proportional to [Formula: see tex

112 on the topography of the environment, with [Formula: see text] assuming intermediate values in the w

113 la: see text], the relatively low values of [Formula: see text] at [Formula: see text] K show that th

114 an square displacement growing with time as [Formula: see text] at the beginning and eventually slowi

115 hermore, the absence of marked deviation in [Formula: see text] at the onset of long-range CDW order

116 th kappa zz being the largest component and [Formula: see text] being about 25%.

117 a: see text] dimer, the [Formula: see text]-[Formula: see text] bond in dizincocene, and the Mn-Mn bo

118 e quantum mechanical ballistic transport at [Formula: see text] but governed by electron hydrodynamic

119 spatial motion model (SMM), which explains [Formula: see text] by motions in real space.

120 The [Formula: see text] can be applied to any existing contig

121 teral sizes from [Formula: see text]m(2) to [Formula: see text] cm(2) Electron microscopy reveals the

122 with [Formula: see text] rows (vectors) and [Formula: see text] columns (dimensions), where [Formula:

123 in BaCr2As2 with respect to systems with a [Formula: see text] count closer to five.

124 ctron-doped FeSCs) and lower (Cr-pnictides) [Formula: see text] counts.

125 As the film thickness is decreased, [Formula: see text] decreases rapidly and the average fil

126 related to the recently observed universal [Formula: see text] density of states of quasilocalized l

127 mpounds are examined: a [Formula: see text]-[Formula: see text] dimer, the [Formula: see text]-[Formu

128 nt available methods based on Manhattan and [Formula: see text] dissimilarity measures.

129 We obtained high-density genotype data from [Formula: see text] DO mice, and localized 2.2 million CO

130 : see text], where the viscous contribution [Formula: see text] dominates over [Formula: see text] in

131 ecorded in fluorescence and the drawdown of [Formula: see text] during summer.

132 gest for materials closest to a half-filled [Formula: see text] electron shell (Mn compounds, hole-do

133 n the benthic-hyporheic zone, and the lower [Formula: see text] emission potential reflects the produ

134 a: see text] emission potentials: the upper [Formula: see text] emission potential results from produ

135 see text] production is bounded between two [Formula: see text] emission potentials: the upper [Formu

136 We show that the primary source of [Formula: see text] emissions varies with stream and rive

137 s of 0.19-0.53 Gt CO2 eqa(-1), 4.32-10.6 Gt [Formula: see text] eqa(-1), and 1.5-2.8 million km(2), w

138 icant impact on the reactivity at positions [Formula: see text] far away from point [Formula: see tex

139 and [Formula: see text] are proportional to [Formula: see text] For a variety of important determinis

140 trend was also observed between ROS/RNS and [Formula: see text] for all naphthalene SOA, regardless o

141 inear equations based on a random choice of [Formula: see text] frame vectors of [Formula: see text]

142 alized with more than a decade of values of [Formula: see text] from 5.1 m to 129 m, corresponding to

143 changing the composition of the molecule at [Formula: see text] has only local effects and does not h

144 he geometry with the most tunnel volume had [Formula: see text] higher permeability, but the bulk flo

145 e show that the time-evolving enrichment of [Formula: see text] in solution is a direct measure of bo

146 ribution [Formula: see text] dominates over [Formula: see text] in the hydrodynamic limit.

147 ounterparts, hydroxide (OH(-)) and ammonium [Formula: see text] ions.

148 perature and inhomogeneity lengthscale, and [Formula: see text] is a microscopic momentum-preserving

149 reversibility and show that significance at [Formula: see text] is best possible in general.

150 ations, however, the failure probability of [Formula: see text] is generally required.

151 becomes [Formula: see text] The coefficient [Formula: see text] is independent of temperature and inh

152 A dielectric constant as large as [Formula: see text] is observed at low temperatures.

153 We find that [Formula: see text] is significantly higher in West Coast

154 When the aspect ratio [Formula: see text] is small, the MANOVA spectrum tends t

155 ergy is given by [Formula: see text], where [Formula: see text] is the ambient temperature and [Formu

156 lting in quadrupolar satellites for nuclear [Formula: see text] isotopes, whereas NMR of the "bulk" l

157 a bending modulus ranging from 2.2 to 54 (x[Formula: see text] Jm).

158 tively low values of [Formula: see text] at [Formula: see text] K show that the pseudogap is a ground

159 ated with arbitrarily small error under the [Formula: see text] norm.

160 n a rigorous upper bound on the resistivity [Formula: see text] of an electron fluid whose electronic

161 This exponent is different from [Formula: see text] of dilute magnetic alloys that was as

162 seed set expansion problem": given a subset [Formula: see text] of nodes from a community of interest

163 nergy landscape, and is also different from [Formula: see text] of the conventional Debye relaxation

164 y [Formula: see text]25 nm thick, occupying [Formula: see text] of volume.

165 limit of unital copies of the Cuntz algebra [Formula: see text] or of the canonical anticommutation r

166 lowing below a glass transition temperature [Formula: see text] or whether motion continues to slow g

167 ptimally hole-doped cuprates, including its [Formula: see text] orbital character, hole filling level

168 tatic friction coefficient was found to be [Formula: see text] Pa.s, which is on the same order of m

169 tract length of 250 bp and a probability of [Formula: see text] per generation for a nucleotide to be

170 regates into one lamellar gel phase and one [Formula: see text] phase.

171 The thermal diffusivity in the [Formula: see text] plane of underdoped YBCO crystals is

172 ice of [Formula: see text] frame vectors of [Formula: see text] possible vectors and has a variety of

173 This analysis reveals that [Formula: see text] production is bounded between two [Fo

174 of long-range CDW order indicates that this [Formula: see text] reduction and the Fermi-surface recon

175 [Formula: see text] rows from a frame with [Formula: see text] rows (vectors) and [Formula: see text

176 We draw a random subset of [Formula: see text] rows from a frame with [Formula: see

177 m state whose variance in regions of volume [Formula: see text] scales as [Formula: see text] Systems

178 ormula: see text], [Formula: see text], and [Formula: see text] should be defined for a given system.

179 rmula: see text], exceeds the cost to self, [Formula: see text] Specifically, Hamilton's rule states

180 he superconducting phase in iron-based high-[Formula: see text] superconductors (FeSC), as in other u

181 ons of volume [Formula: see text] scales as [Formula: see text] Systems whose fluctuations decay fast

182 arance of waste products, including amyloid [Formula: see text] that may form pathological aggregates

183 -we show that the resistivity bound becomes [Formula: see text] The coefficient [Formula: see text] i

184 the fundamental Landauer's ballistic limit [Formula: see text] The effect is particularly striking f

185 istical symmetry for a further reduction of [Formula: see text] The resulting algorithms can efficien

186 otential, by computing the softness kernel, [Formula: see text] The softness kernel is nearsighted, i

187 ons [Formula: see text] far away from point [Formula: see text] This locality principle elucidates th

188 it value in a population is proportional to [Formula: see text] This rule is commonly believed to be

189 -P-26b's atmospheric heavy element content ([Formula: see text] times solar).

190 distribution with the exponent varying from [Formula: see text] to [Formula: see text] (Brownian).

191 ation encoded by the degree of stealthiness [Formula: see text] To establish a unified view, we propo

192 Using this approach, we report measures of [Formula: see text] up to 0.5 km.

193 y distributions, such as the skewed Student [Formula: see text] used here, when making forecasts of p

194 th respect to the values, by establishing a [Formula: see text] value under the null hypothesis that

195 The [Formula: see text] was designed to measure the dissimila

196 t] Systems whose fluctuations decay faster, [Formula: see text] with [Formula: see text], are called

197 The two dice land on side [Formula: see text] with unknown probabilities [Formula:

198 ccurate to the first order of eta C , reads [Formula: see text](DeltaT (2)).

199 ependent behavior of the three energy terms [Formula: see text](intra-atomic), [Formula: see text] (e

200 troducing a suitable nonlocal entropy rate ([Formula: see text]) and by analyzing field and simulated

201 binding of random sequences of hydrophobic ([Formula: see text]) and polar ([Formula: see text]) mono

202 column-averaged CO2 dry-air mole fraction ([Formula: see text]) as well as the fluorescence from chl

203 tion of the N-terminal 17-residue sequence ([Formula: see text]) facilitates polyQ aggregation by enc

204 adding the C-terminal polyproline sequence ([Formula: see text]) inhibits aggregation.

205 The self-Hermitian of this MTZF([Formula: see text]) is similar to that of the Majorana f

206 ydrophobic ([Formula: see text]) and polar ([Formula: see text]) monomers in a computational model.

207 uire the pairwise correlation coefficients ([Formula: see text]) of the variants.

208 ges the structure from the primitive cubic ([Formula: see text]) to the double diamond phase ([Formul

209 correlation-frequency ([Formula: see text]-[Formula: see text]) transport phase diagram.

210 la: see text]) to the double diamond phase ([Formula: see text]) whilst still allowing for modest inc

211 ssesses a high depinning current threshold ([Formula: see text]) with unconventional depinning charac

212 lar to that of the Majorana fermions (MFs) ([Formula: see text]).

213 used over a wide range of flow shear rates ([Formula: see text]).

214 even among experts as to how the quantities [Formula: see text], [Formula: see text], and [Formula: s

215 luctuations toward their limiting behavior, [Formula: see text], a uniformity similar to random close

216 to how the quantities [Formula: see text], [Formula: see text], and [Formula: see text] should be de

217 ions decay faster, [Formula: see text] with [Formula: see text], are called hyperuniform.

218 On a [Formula: see text], clusters of any size always prefer h

219 concentrated phase of phase-separated Ddx4, [Formula: see text], diffuses as a particle of 600-nm hyd

220 mula: see text], multiplied by relatedness, [Formula: see text], exceeds the cost to self, [Formula:

221 nonmonotonic behavior in the friction law, [Formula: see text], is present even if the dynamic and s

222 natural selection if the benefit to others, [Formula: see text], multiplied by relatedness, [Formula:

223 e manner the available experimental data on [Formula: see text], providing quantitative insights into

224 water and rice were [Formula: see text] and [Formula: see text], respectively, for the entire U.S. po

225 meter down to [Formula: see text] and up to [Formula: see text], revealing a reduction of viscosity b

226 ase in bed surface armoring with increasing [Formula: see text], suggesting channels accommodate chan

227 The larger [Formula: see text], the more uniform, with systems like

228 Above [Formula: see text], the relatively low values of [Formul

229 The energy is given by [Formula: see text], where [Formula: see text] is the amb

230 tance is found to obey an additive relation [Formula: see text], where the viscous contribution [Form

231 known probabilities [Formula: see text] and [Formula: see text], which can be arbitrarily low.

232 ann weights are still on the order of a few [Formula: see text], which may lead to significant discre

233 nificant change in dissolution mechanism at [Formula: see text], which we interpret as the onset of h

234 get distribution that has finite support in [Formula: see text], with [Formula: see text].

235 a: see text]-[Formula: see text] dimer, the [Formula: see text]-[Formula: see text] bond in dizincoce

236 lly characterized compounds are examined: a [Formula: see text]-[Formula: see text] dimer, the [Formu

237 d view, we propose a correlation-frequency ([Formula: see text]-[Formula: see text]) transport phase

238 that there is a simple nuclear nonseparable [Formula: see text]-algebra, which is not isomorphic to i

239 ng of the [Formula: see text]-symmetric and [Formula: see text]-broken phases for eigenvalues is theo

240 iscovery, a number of additional standalone [Formula: see text]-cyclases have been reported as potent

241 the distribution of singular values of the [Formula: see text]-subset matrix.

242 In this report, broadband mixing of the [Formula: see text]-symmetric and [Formula: see text]-bro

243 ties in this driven vortex state just above [Formula: see text].

244 finite support in [Formula: see text], with [Formula: see text].

245 tually slowing down to the diffusive spread [Formula: see text].

246 ased to exist at cooling rates greater than [Formula: see text].

247 fferences in aerosol carbon oxidation state [Formula: see text].

248 llations in sign language <5 Hz, peaking at [Formula: see text]1 Hz.

249 One is a structural transition at [Formula: see text]1.5 GPa, and the other is from a ferro

250 mula: see text]20 ppm rise after 7 kyBP and [Formula: see text]10 ppm fall between 1500 CE and 1600 C

251 olecular chromophores on typical timescales [Formula: see text]100 fs.

252 ns in atmospheric CO2 concentration between [Formula: see text]150 and 700 ppm for the latest Carboni

253 n unusually robust linear dispersion (up to [Formula: see text]2 eV) with multiple nondegenerate Dira

254 elated function of the [Formula: see text]2-[Formula: see text]2 loop.

255 ructural transition-related function of the [Formula: see text]2-[Formula: see text]2 loop.

256 Markov-state model analysis of [Formula: see text]2-[Formula: see text]s trajectories su

257 or particular variations in the CO2 record ([Formula: see text]20 ppm rise after 7 kyBP and [Formula:

258 to an antiferromagnetic (AFM) insulator at [Formula: see text]21 GPa whose AFM spin configuration is

259 e lamellea, bound by biopolymer layers only [Formula: see text]25 nm thick, occupying [Formula: see t

260 both class I and II HLA genes, taking only [Formula: see text]3 min to process a 30x whole-genome BA

261 ontinuum elasticity theory shows that up to [Formula: see text]3.5% compressive strain can be induced

262 ll understood: (i) the nanoscale thickness ([Formula: see text]300 nm) of nacre's building blocks, th

263 , especially at small spatial scales (up to [Formula: see text]4,000 km).

264 ents on recently designed superparamagnetic [Formula: see text]40-[Formula: see text]m-long microrods

265 When the colony consists of less than [Formula: see text]50,000 members it is eliminated, while

266 ter that can be readily drawn into uniform ([Formula: see text]6-[Formula: see text]m thick) "supramo

267 convolution analyses of atmospheric CO2 and [Formula: see text]C at different temporal scales to inve

268 a: see text]co2 slope, [Formula: see text]e/[Formula: see text]co2 nadir, or end-exercise [Formula: s

269 metabolic demand (high [Formula: see text]e/[Formula: see text]co2 relationship) is a common finding

270 osen metric (increased [Formula: see text]e-[Formula: see text]co2 slope, [Formula: see text]e/[Formu

271 nadir, or end-exercise [Formula: see text]e/[Formula: see text]co2), ventilatory inefficiency was clo

272 Regardless of the chosen metric (increased [Formula: see text]e-[Formula: see text]co2 slope, [Formu

273 a: see text]e-[Formula: see text]co2 slope, [Formula: see text]e/[Formula: see text]co2 nadir, or end

274 sponse to exertional metabolic demand (high [Formula: see text]e/[Formula: see text]co2 relationship)

275 ormula: see text]co2 nadir, or end-exercise [Formula: see text]e/[Formula: see text]co2), ventilatory

276 d membranes with thickness of 100 nm to 2.5 [Formula: see text]m and lateral sizes from [Formula: see

277 opic dissolution of [Formula: see text] 100 [Formula: see text]m bubbles coated with [Formula: see te

278 m bubbles coated with [Formula: see text] 1 [Formula: see text]m particles is presented and discussed

279 ly drawn into uniform ([Formula: see text]6-[Formula: see text]m thick) "supramolecular fibers" at ro

280 [Formula: see text]m and lateral sizes from [Formula: see text]m(2) to [Formula: see text] cm(2) Elec

281 ned superparamagnetic [Formula: see text]40-[Formula: see text]m-long microrods containing iron-oxide

282 nd women.The MFO and maximal oxygen uptake ([Formula: see text]O2 max) were determined with the use o

283 h 16.6% of the variability explained by the [Formula: see text]O2 max, sex, and SRPAL; dietary carboh

284 tate model analysis of [Formula: see text]2-[Formula: see text]s trajectories suggests that hydration

285 fants exposed to bifidobacteria-supplemented formula showed decreased occurrence of Bacteroides and B

286 omparing porewater and oceanic DOS molecular formulas, solar irradiation increased the similarity due

287 Over 100 molecules of this kind with formulas such as Au25(SR)18, Au38(SR)24, and Au102(SR)44

288 ectiveness of a partially hydrolyzed protein formula supplemented with nondigestible oligosaccharides

289 We derive an intuitive formula that approximates the probability of lysogeny fo

290 unambiguously assign one specific molecular formula to an experimental isotopic pattern.

291 ensively hydrolyzed (EH), and one amino acid formula, using biochemical techniques and specific antib

292 The new formula was comparable with well-known methods and was b

293 n DOM elemental composition as DOS molecular formulas were more photolabile than those without sulfur

294 We first determine elemental formulas, which are then used to query the "metabolic in

295 compared the performance of the new derived formula with existing GFR formulae.

296 d that a partially hydrolyzed protein infant formula with specific prebiotics modulated the gut micro

297 VRF intraocular lens (IOL) power calculation formula with well-known methods.

298 carboxylated aromatic and condensed aromatic formulas, with CHON-type COO KMD formulas relatively mor

299 ethylene to all 10 of the cumulenes with the formula X horizontal lineC horizontal lineY, where X, Y

300 It has transition-metal nodes of formula Zr6(mu3-OH)4(mu3-O)4(OH)4(OH2)4 that resemble hy