ライフサイエンスコーパス: Cs

1 Cs and Li ions were added as integrated ISTDs to the BGE

2 Cs and Pb were the main elements to discriminate the win

3 Cs uses outer core 5s and 5p orbitals to bind the oxygen

4 Cs(+) acts as a soft Lewis acid to polarize the carbon-c

5 ) by forming a heterostructure comprising 0D Cs(4) PbI(6) and gamma-CsPbI(3) through tuning the stoic

6 As-received AN-102, Cs-depleted effluent, and sRF eluate fractions were comp

7 ctra show the presence of an additional (133)Cs NMR signal with a unique chemical shift that is attri

8 ng curves considering all possible (1)H-(133)Cs/(207)Pb spin pairs were then calculated.

9 re recorded using double resonance (1)H{(133)Cs} RESPDOR and (1)H{(207)Pb} S-REDOR experiments.

10 7)Cl, (39)K, (79/81)Br, (87)Rb, (127)I, (133)Cs, and (207)Pb nuclei) and locally and shedding light o

11 roscopy of quadrupolar nuclei ((115)In, (133)Cs, and (209)Bi), we show that there is a high degree of

12 l losses of nonreactive ultracold (87)Rb(133)Cs molecules, and compare our findings with the sticky c

13 , consistent with the surface-selective (133)Cs NMR experiments.

14 Surface-selective (133)Cs solid-state NMR spectra show the presence of an addit

15 We use (133)Cs, (87)Rb, (39)K, (13)C, and (14)N solid-state MAS NMR

16 termination of the presence of (137)Cs, (134)Cs, (131)I, and other gamma-emitting radionuclides in th

17 for (137)Cs, and 54 +/- 1 Bq.m(-3) for (134)Cs, appear to be influenced by ongoing releases from the

18 Here, time series measurements of (134)Cs and (137)Cs in seawater on Line P and on the CLIVAR-P

19 ma, Japan have become contaminated with (134)Cs and (137)Cs released in March 2011 from the damaged F

20 rmination of (135)Cs concentrations and (135)Cs/(137)Cs ratios in soil samples collected from Denmark

21 etection limit of 9.1 x 10(-17) g/g for (135)Cs and (137)Cs was achieved for 60 g samples.

22 for the determination of ultralow level (135)Cs in environmental samples by chromatographic separatio

23 for the determination of ultralow level (135)Cs, avoiding the problem of removal of a huge amount of

24 ce of Ba isotopes to the measurement of (135)Cs and (137)Cs in environmental samples negligible.

25 d (137)Ba) to the ICP-MS measurement of (135)Cs and (137)Cs was further suppressed to 8 x 10(-5) by u

26 sfully applied for the determination of (135)Cs concentrations and (135)Cs/(137)Cs ratios in soil sam

27 ndard for quantitative determination of (135)Cs without complete release and recover of radiocesium.

28 is work demonstrated the application of (135)Cs/(137)Cs as a unique fingerprint for discriminating th

29 The (135)Cs/(137)Cs isotopic ratios in Danish soil (2.08-2.68) we

30 itrogen content), (14) C, (210) Pb and (137) Cs analyses and were used to infer changes in peatland h

31 (137)Cs resulted <0.10Bqkg(-1) in all samples.

32 (134/137)Cs poisoning, and use for (131/137)Cs radiotherapy (brachytherapy).

33 or different radionuclides ((131)I, (134,137)Cs, (90)Sr-(90)Y, (103)Ru and (239,240)Pu) in terms of t

34 , administration as an antidote for (134/137)Cs poisoning, and use for (131/137)Cs radiotherapy (brac

35 ential applications as an effective (134/137)Cs remover from nuclear waste solutions, administration

36 se recordings, the level of cesium-137 ((137)Cs) contamination was determined for individual fruits.

37 cy of GT3-Nano was assessed after acute (137)Cs whole-body irradiation at a sublethal (4 Gy), a letha

38 topes to the measurement of (135)Cs and (137)Cs in environmental samples negligible.

39 time series measurements of (134)Cs and (137)Cs in seawater on Line P and on the CLIVAR-P16N 152 degr

40 Natural radionuclides and (137)Cs in twenty seven honeys produced in a region of the Ce

41 ve become contaminated with (134)Cs and (137)Cs released in March 2011 from the damaged Fukushima Dai

42 it of 9.1 x 10(-17) g/g for (135)Cs and (137)Cs was achieved for 60 g samples.

43 o the ICP-MS measurement of (135)Cs and (137)Cs was further suppressed to 8 x 10(-5) by using N(2)O a

44 lyzed for (236)U (as well as (238)U and (137)Cs).

45 ating, were confirmed using (210)Pb and (137)Cs: these show that the top 2 m of Sphagnum-peat has acc

46 of the energetic gamma rays emitted by (137)Cs, the individual will be exposed to a low dose rate, u

47 s from the FDNPP, with a characteristic (137)Cs/(90)Sr activity ratio of 3.5 +/- 0.2.

48 demonstrated the application of (135)Cs/(137)Cs as a unique fingerprint for discriminating the source

49 The (135)Cs/(137)Cs isotopic ratios in Danish soil (2.08-2.68) were signi

50 n of (135)Cs concentrations and (135)Cs/(137)Cs ratios in soil samples collected from Denmark, Sweden

51 Making use of discarded (137)Cs brachytherapy seeds, the VADER can provide varying lo

52 A distinguishable (137)Cs energy spectrum with comparable or better resolution

53 We report concentrations of FRNs (i.e. (137)Cs, (210)Pb(un) and (241)Am) and other contaminants (i.e

54 The VADER (VAriable Dose-rate External (137)Cs irradiatoR) allows modeling these exposures, bypassin

55 they are below the detection limit for (137)Cs and (226)Ra.

56 maximum (292 us for (204)Tl, 277 us for (137)Cs, 258 us for (22)Na).

57 roseconds (22 us for (204)Tl, 26 us for (137)Cs, 9 us for (22)Na).

58 (-3) for (90)Sr, 124 +/- 3 Bq.m(-3) for (137)Cs, and 54 +/- 1 Bq.m(-3) for (134)Cs, appear to be infl

59 e time series measurements of Fukushima (137)Cs indicate that the 2015-2016 results represent maximum

60 The current elevated Fukushima (137)Cs levels in seawater in the eastern North Pacific are e

61 groundwater collected in Sendai Bay had (137)Cs concentrations of up to 43 +/- 1 Bq.m(-3), while (90)

62 011-2015 was calculated from the (129)I/(137)Cs ratio of the ongoing (137)Cs releases and estimated t

63 d a quantitative removal of interfering (137)Cs in the deposition product and proved to be very effic

64 Intrinsic (137)Cs in the environmental samples measured by gamma spectr

65 e rate or a varying dose rate mimicking (137)Cs biokinetics in mouse or man.

66 e platters containing ~ 250 mCi each of (137)Cs brachytherapy seeds are mounted above and below the "

67 ini have significantly higher levels of (137)Cs contamination compared with those from all other meas

68 ivalent to fallout background levels of (137)Cs that prevailed during the 1970s and do not represent

69 presence of overwhelming activities of (137)Cs via the autodepostion of silver on a copper plate.

70 to the determination of the presence of (137)Cs, (134)Cs, (131)I, and other gamma-emitting radionucli

71 The mean concentrations of (137)Cs, (210)Pb(un) and (241)Am in cryoconite were 2,123 +/-

72 the (129)I/(137)Cs ratio of the ongoing (137)Cs releases and estimated to be about 100 g (which adds

73 Post (137)Cs removal, the cesium-loaded sRF column was eluted with

74 nd dominating gamma emitters, primarily (137)Cs, which results in increased detection limits in the g

75 progeny) and artificial radionuclides ((137)Cs) in various honey samples, as well as to compile a da

76 Fallout radionuclides ((137)Cs, (239)Pu, (240)Pu) were measured in soil samples (n =

77 f and by 2015 and early 2016 it reached (137)Cs values of 6-8 Bq/m(3) in surface water along Line P.

78 report also shows continuously recorded (137)Cs gamma radiation response of a unidirectionally-biased

79 t Na concentration to ~5.6 M and remove (137)Cs by spherical resorcinol-formaldehyde (sRF) ion-exchan

80 Th and (228)Th) and gamma spectrometry ((137)Cs, (40)K, (226)Ra and (228)Ra).

81 In the long term, (137)Cs is probably the most biologically important agent rel

82 accident, and we compare the results to (137)Cs collected at the same stations and depths.

83 s of global versus Chernobyl fallout to (137)Cs found in European soils.

84 been retained in the Hythe marsh, with (137)Cs and Cu depth profiles showing retention of input maxi

85 se to an unprecedented 16-coordinate (CN 16) Cs(+) cation in a likewise unprecedented tetracosahedral

86 ks have been synthesized: Cs(8)In(27)Sb(19), Cs(8)Ga(27)Sb(19), and Rb(8)Ga(27)Sb(19).

87 of them, Cs(0.4)La(0.6)Mn(0.25)Co(0.75)O(3), Cs(0.3)La(0.7)NiO(3), SrNi(0.75)Co(0.25)O(3), and Sr(0.2

88 t the intermediate solidification rate of 30 Cs(-1).

89 We predict that 261 of the 311 Cs(2)BB'Cl(6) compounds are likely synthesizable on the

90 phy, shows that quantum dots (QDs) of [Na(4) Cs(6) PbBr(4) ](8+) (not of CsPbBr(3) ) have formed.

91 solidified in the cooling rate range of 1-50 Cs(-1).

92 onally photostable material, [HC(NH2)2](0.83)Cs(0.17)Pb(I(0.6)Br(0.4))3, with an optical band gap of

93 e found to be obtained with the use of (i) a Cs(+) ion source and detection of H(-) and D(-) at low m

94 ment was also isolated by encapsulation of a Cs(+) counterion with 2.2.2-cryptand.

95 ew cycloparaphenylene derivative possesses a Cs point group symmetry.

96 t distal stereocontrol is achieved through a Cs-bridged interaction between the Lewis-basic C-termina

97 eadily prepared suspensions of APbBr(3) (A = Cs or methylammonium (MA)) type perovskite colloids (ca.

98 tes (A')(2)(A) (n-1)M (n) X(3n+1) [where A = Cs(+), CH(3)NH(3) (+), HC(NH(2))(2) (+); A' = ammonium c

99 In addition, all animals acquired Cs directly from the aqueous phase, but this accounted f

100 Cesium bis(perfluoro-triphenylborane)amide, Cs[H2NB2(C6F5)6] (1), has been prepared by the reaction

101 t ion species, such as Rb(+), NH(4) (+), and Cs(+), strongly promoted a pH-dependent activated confor

102 l that covalently modifies accessible As and Cs, than regions that encode protein domain junctions.

103 d Pt(II) complex compounds and Li, Na, K and Cs atoms.

104 onic adducts (H(+), NH4(+), Na(+), K(+), and Cs(+)).

105 Si/Al = 3.8 has been prepared in Na, K, and Cs forms and its structural response to dehydration meas

106 compared to its alkaline cousins (Li, K, and Cs).

107 Na-MER adopts Immm symmetry, while K- and Cs-MER display P4(2)/nmc symmetry, the difference attrib

108 ase by 9.8%, 7.7%, and 7.1% for Na-, K-, and Cs-MER, respectively.

109 In the stoichiometric form, while Xe, Kr and Cs are not captured, Br, I and Te exhibit strong encapsu

110 nce between the surface ammonium ligands and Cs and Pb were recorded using double resonance (1)H{(133

111 high-resolution atomic force microscopy and Cs-corrected scanning transmission electron microscopy u

112 g, S, Mn, Fe, Co, Cu, Zn Se, Br, Rb, Mo, and Cs) in less than 250 000 cells.

113 rage in barrels were differentiate by Na and Cs concentration.

114 The controlled reaction of Na and Cs, two alkali metals of different ionic sizes and bindi

115 3.091(11) angstrom) surrounded by Na(+) and Cs(+) ions.

116 Na- and Cs-MER show non-Type I isotherms and kinetically-limited

117 Conversely, Xe, Kr, Rb and Cs are unbound.

118 tion by several alkali metals (Li, K, Rb and Cs) and alkali-earth Ca.

119 n nine structures, A(+) (A=Li, Na, K, Rb and Cs), AE(2+) (AE=Ca, Sr, Ba) and Mn(2+) demonstrate that

120 icients between those reported for Rb(+) and Cs(+).

121 s, is examined; of these, certain K, Rb, and Cs compounds are predicted to be thermodynamically stabl

122 The low sublimation energies of K, Rb, and Cs were found to be key for initiation of the reactions.

123 tahydrotriborates (MB(3) H(8) ; M=K, Rb, and Cs) has been developed.

124 perconductors A(2)Cr(3)As(3) (A = K, Rb, and Cs).

125 t of AAuH2 compounds, A = Li, Na, K, Rb, and Cs, is examined; of these, certain K, Rb, and Cs compoun

126 The mobility of stable Sr and Cs (as analogs for their radioactive counterparts), Ce (

127 These species have C1 (unsym) and Cs (sym) symmetries, respectively, depending on the ster

128 maroon [K(crypt)](+) , [K(18-c-6)](+) , and [Cs(crypt)](+) salts of the [Sc(NR2 )3 ](-) anion are for

129 stallized with {K(+) (18-crown-6)(THF)} and {Cs(+) (2) (18-crown-6)(3) }.

130 cent experiments show that direct, anhydrous Cs(+)-K(+) exchange is kinetically viable and leads to t

131 econstitution and analysis of vertebrate APC/Cs under physiological conditions, we show how cyclin-de

132 e tunnel dimension was found to increases as Cs substitution in the tunnel increased.

133 ound binds large monovalent cations, such as Cs(+) and Tl(+), with a binding constant significantly l

134 some heavy stable elements (Rb, Sr, Zr, Ba, Cs, Ba, La, Ce, Nd, Sm, Dy, Lu, U, Th) in glassy fallout

135 acetylene via a successive addition of base (Cs(2)CO(3)) and a Pd(II) catalyst, allowing sufficient t

136 Using the integrated ISTDs, both Cs and Li improved the Na peak area reproducibility appr

137 r reversed when the h-current was blocked by Cs(+).

138 Cu(II), Cr, Mo, Co(II), Mg, Nd, Li, Ti, Ca, Cs, Ag, Tm, Er(III), La(III), Yb(III), Eu(III), Pr(III),

139 a gradually enhanced specific capacitance ( Cs) with increased flexibility (decreased storage moduli

140 ent a series of Bi(3+)/In(3+) mixed-cationic Cs(2)Bi(1-x)In(x)AgCl(6) HDP solid solutions that span t

141 In vivo, chitosan-loaded cyclodextrin (CDPE-Cs) hydrogels yield significantly lower amounts of blood

142 mixed cations of MA(+) , FA(+) , and cesium (Cs(+) ).

143 efficiency (PCE) of triple-A cation (cesium (Cs)/methylammonium (MA)/formaminidium (FA)) perovskite s

144 tal system for interacting with cold cesium (Cs) atoms.

145 loiting all-inorganic PVSCs by using cesium (Cs)-based perovskite materials, such as alpha-CsPbI(3) .

146 relaxation dynamics in LHP NCs with cesium (Cs), methylammonium (MA, CH(3)NH(3)(+)), and formamidini

147 ion of twenty-nine elements (Ag, As, Ce, Co, Cs, Cu, Eu, Fe, Ga, Gd, La, Lu, Mn, Mo, Nb, Nd, Ni, Pr,

148 of the nitride-bridged diuranium(IV) complex Cs[{U(OSi(OtBu)3)3}2(mu-N)]affords the first example of

149 rrimagnetic materials of the new composition Cs(2)MU(3)F(16) (M = Mn(2+), Co(2+), and Ni(2+)), which

150 tion mixed-halide perovskites of composition Cs(x) (FA(y) MA(1-) (y) )(1) (-x) Pb(I(z) Br(1) (-z) )(3

151 e discovery of a new superprotonic compound, Cs(7)(H(4)PO(4))(H(2)PO(4))(8), or CPP, which forms at e

152 ces (fs) and monovalent salt concentrations (Cs).

153 ibits a complex crystal structure containing Cs(+) cations, Pt(2-) and H(-) anions.

154 minase domains, PPR65 and PPR56, can convert Cs to Us in cognate, exogenous RNA targets co-expressed

155 THP-1 cells by treatment with cyclosporine (Cs) or its nonimmunosuppressive analogue SDZ-NIM811, ind

156 l-inorganic lead-free perovskite derivative, Cs(3) Bi(2) I(9) , exhibits strong light-matter interact

157 layer spacing ( approximately 0.7 A) during Cs(+) exchange is an example of "chemical-mechanical cou

158 benzyl bromides and arylhydrazines employing Cs(2)CO(3) as the base and t-Bu(3)PHBF(4) as the ligand

159 The Td -symmetric [CsO4 ](+) ion, featuring Cs in an oxidation state of 9, is computed to be a minim

160 citation and a maximum PLQY of 34 +/- 4% for Cs(2)Bi(0.085)In(0.915)AgCl(6).

161 nal quantum efficiencies (EQEs) of 17.6% for Cs(0.2) FA(0.8) PbI(2.8) Br(0.2) , 14.3% for CH(3) NH(3)

162 ns interlayer K(+) and has high affinity for Cs(+).

163 tructure is a promising crystalline host for Cs immobilization.

164 wer values, up to 250 muV.K(-1) at 300 K for Cs(8)In(27)Sb(19).

165 Although exchange of interlayer K(+) for Cs(+) is nearly thermodynamically nonselective, recent e

166 motion and by extension, the propensity for Cs release from hollandite.

167 However, higher selectivity for Cs(+) and Tl(+) was observed with this compound since it

168 b(10) family shows exclusive selectivity for Cs(+) over other alkalis, which is important for radioac

169 lycosyltransferases of the C-superfamily (GT-Cs), which are loosely defined as containing membrane-sp

170 ecreased in the order Li(+) > Na(+) > K(+) > Cs(+) , which agreed with an earlier theoretical predict

171 etal cations in order Li(+) > Na(+) > K(+) > Cs(+) as well as a notable luminescent response for cesi

172 The peaks in the emission spectra of Pb,Br,H,Cs,Na-X and the CsPbBr(3) NCs are both at about 520 nm.

173 The FWHM of Pb,Br,H,Cs,Na-X, however, is narrower than any previously report

174 The zeolite X product, Pb,Br,H,Cs,Na-X, shows superior stability toward moisture, maint

175 lution-processed triple-cation mixed-halide (Cs(0.06) MA(0.15) FA(0.79) )Pb(Br(0.4) I(0.6) )(3) perov

176 We also consider the addition of Li, He, Cs, and Bi, to probe the utility of the exo/ endo cages

177 , Mn, Fe, Co, Cu, Zn, Se, Br, Rb, Sr, Mo, I, Cs, and Ba) in 10 muL of serum and 12 elements (Mg, S, M

178 evel random Bi(3+)/In(3+) cationic mixing in Cs(2)Bi(1-x)In(x)AgCl(6) HDPs.

179 ion by two bowl-shaped sumanenyl anions in [Cs(C21 H11(-) )2 ](-) was revealed crystallographically.

180 In [{Cs(+) (18-crown-6)}(1 a(-) )].THF, asymmetric binding of

181 surface of 1 a(-) is observed, whereas in [{Cs(+) (18-crown-6)}(2) (1 a(2-) )], two Cs(+) ions bind

182 nt moieties, the [Nb6O19](8-) polyanion, its Cs(+) counterions, and the DMMP substrate, were tracked

183 alkali metal cations (Li(+) , Na(+) , K(+) , Cs(+) ) on the non-Nernstian pH shift of the step-relate

184 alkali hydroxide solutions (MOH, M = Na, K, Cs), OH* intermediates may be present, and at high overp

185 oforms of persistently active protein kinase Cs (PKMs) maintain distinct forms of long-lasting synapt

186 On the contrary, large Cs(+) ions blocked the WT channels, while displayed larg

187 ck mechanism in which exchange of the larger Cs(+) for the smaller K(+) significantly lowers the migr

188 several elements, including Mo, Er, Na, Li, Cs and Pb, varied by 10-fold across the 14 wines.

189 + Na)(+), (M + K)(+), (M + Rb)(+), and (M + Cs)(+), were successfully detected on the FAPCI mass spe

190 Their intensity order was as follows: (M + Cs)(+) > (M + Rb)(+) > (M + K)(+) > (M + Na)(+) > (M + L

191 sed on binary cation (MA(+) -FA(+) or MA(+) -Cs(+) ) 2D structures.

192 valent cation (e.g., methylammonium (MA(+)), Cs(+)), B is the divalent metal ion(s) (e.g., Pb(2+), Sn

193 d scanning transmission electron microscopy (Cs -corrected STEM).

194 d scanning transmission electron microscopy (Cs-STEM), nano-beam electron diffraction, electron holog

195 The N/Cs for all three tissue types are similar.

196 sulfonate groups (PES23) with Li(+), Na(+), Cs(+), or NBu(4)(+) counterions synthesized from step-gr

197 and 137Cs) signature with negligible natural Cs.

198 Here, blue-emission ( approximately 470 nm) Cs-based perovskite NCs are derived by directly mixing s

199 lates with the size of the alkali cation: NS/Cs(+)/NS > NS/Rb(+)/NS > NS/K(+)/NS > NS/Na(+)/NS > NS/L

200 R correlates with the interlayer spacing; NS/Cs(+)/NS has the lowest eta (0.45 V), while NS/Li(+)/NS

201 ers (eta and Tafel slope) associated with NS/Cs(+)/NS for the OER were superior to that of the bulk b

202 d for nearly all of the total body burden of Cs in these animals.

203 thesis and spectroscopic characterization of Cs-symmetric tris- and C2v-symmetric tetra-adducts of C7

204 is a transition-metal cation, as a class of Cs(2)BB'Cl(6) double perovskites with remarkable optical

205 MAS NMR to probe microscopic composition of Cs-, Rb-, K-, MA-, and FA-containing phases in double-,

206 The conductivity of Cs(7)(H(4)PO(4))(H(2)PO(4))(8) is moderate, 5.8 x 10(-4)

207 The content of Cs, Mg, Cu and Pb in wines characterized the SO(2) addit

208 ion channels due to the internal dialysis of Cs(+) , which increased the bleach-induced desensitizati

209 hich is eliminated upon internal dialysis of Cs(+) .

210 conductances during the internal dialysis of Cs(+) further desensitizes the photovoltage thereby elim

211 model indicated that the transfer factors of Cs from sediments and the trophic transfer factors from

212 performance solar cells based on mixtures of Cs, methylammonium, and formamidinium.

213 ould be considered in the migration model of Cs and radionuclides in the current environment surround

214 ere, we elucidate the atomic-level nature of Cs and Rb incorporation into the perovskite lattice of F

215 The rattling of Cs, low number of Cs I contacts, and high degree of octahedral distortion

216 We elucidate the degradation pathways of Cs-, MA-, and FA-based tin(II) halides and show that deg

217 PeNC of Cs(3)Bi(2)I(9) had the best photocatalytic activity for

218 rk, we systematically explore the portion of Cs-Pb-Br synthesis space in which many optically disting

219 the lower activation seen in the presence of Cs(+).

220 ion-metal-free conditions in the presence of Cs(2)CO(3) in dioxane at 100 degrees C and affords fused

221 e excellent optical and valley properties of Cs(3) Bi(2) I(9) arise from the unique parallel bands, a

222 anoparticles associated with a wide range of Cs concentrations (1.1-19 wt% Cs as Cs2O).

223 The rattling of Cs, low number of Cs I contacts, and high degree of octa

224 f 1 allows nearly quantitative separation of Cs(+) from water, which suggests potential applications

225 This off-center tendency of Cs, together with the distortion of SnX(6) (X = Br or I)

226 work function of 2.07 eV (lower than that of Cs) while remaining chemically inert, two properties usu

227 ly flat bands due to localized vibrations of Cs and I atoms.

228 cles in a SiO2 glass matrix (up to 30 wt% of Cs and 1 wt% of U mainly associated with Zn-Fe-oxide).

229 e-NO}(10) intermediate, key to formation of [Cs(crypt-222)][(TIMEN(Mes))Fe(NO)], (5) featuring a meta

230 sults indicate that grain size and optimized Cs stoichiometry control cation motion and by extension,

231 i carbonate (M(2)CO(3), where M(+) = K(+) or Cs(+)) dispersed over a mesoporous support.

232 3)Bi(2)I(9), in which cation A(+) = Rb(+) or Cs(+) or CH(3)NH(3)(+) (MA(+)), were synthesized with a

233 lytic stages in complex with K(+), Rb(+), or Cs(+) Comparison of these structures with apo TtDdl reve

234 s model predicts that Na(+) would outcompete Cs(+) by 1.8-2.1-fold; i.e., with Cs(+) in 2-fold excess

235 is no significant preference for Na(+) over Cs(+).

236 e in the all-inorganic layered RP perovskite Cs(2)PbI(2)Cl(2).

237 formamidinium-cesium lead iodide perovskite (Cs(0.08) FA(0.92) PbI(3) ) and also reduce the energy ba

238 c layered Ruddlesden-Popper (RP) perovskite, Cs(2)PbI(2)Cl(2), synthesized by the Bridgman method.

239 t, we identify the triple-alkali perovskites Cs(2)[Alk](+)[TM](3+)Cl(6), where Alk is a group 1 alkal

240 ork, 311 cesium chloride double perovskites (Cs(2)BB'Cl(6)) were selected from a set of 903 compounds

241 te the binary caesium salts of phenanthrene, Cs(C14H10) and Cs2(C14H10), to show that they are multio

242 ealed that AGB1 interacts with phospholipase Cs (PLCs), and Ca(o) induced InsP3 production in Col but

243 diamagnetic because of orbital polarization, Cs(C14H10) is a Heisenberg antiferromagnet with a gapped

244 ution method to grow large size high-quality Cs(3)Bi(2)I(9) perovskite single crystals (PSCs).

245 alkalis, which is important for radioactive Cs removal and sequestration.

246 iple bonds, [M]2[U(NR)4] (M = Li, Na, K, Rb, Cs).

247 ounds of the formula AMoO(2)F(3) (A = K, Rb, Cs, NH(4), Tl) have been known for decades, crystal stru

248 neN(3,5-(CF3)2C6H3)(TriNOx)] (M = Li, K, Rb, Cs; solv = TMEDA, THF, Et2O, or DME), was isolated and f

249 which has been studied by atomic-resolution Cs -corrected STEM.

250 dissociation on stepped sites adopted by Ru-Cs counterparts, giving new insights in activating N(2)

251 HR3 EC1 contacts C15a, and presumably all RV-Cs, in a unique cohesive footprint near the threefold ve

252 on of the molecular interface between the RV-Cs and their receptors provides new avenues that can be

253 rds a novel type of organometallic sandwich [Cs(C21 H11(-) )2 ](-) , which crystallized as a solvent-

254 ullerene containing a heptagonal ring, Sc2C2@Cs(hept)-C88, was isolated from the raw soot obtained by

255 The Sc2C2@Cs(hept)-C88 was purified by multistage high-performance

256 In this sense, Cs(+) resembles hypervalent Xe.

257 onium ligands substituting into some surface Cs sites, consistent with the surface-selective (133)Cs

258 conducting frameworks have been synthesized: Cs(8)In(27)Sb(19), Cs(8)Ga(27)Sb(19), and Rb(8)Ga(27)Sb(

259 bled the number of disease-associated target Cs able to be corrected preferentially over nearby non-t

260 rected preferentially over nearby non-target Cs.

261 n having K(+) as the permeant ion; (ii) that Cs(+) or Rb(+), known to halt C-inactivation, prevented

262 ressive analogue SDZ-NIM811, indicating that Cs-sensitive host cell cyclophilins other than CypA cont

263 h other structural parameters, suggests that Cs rattles in its coordination polyhedron.

264 The Cs(2)CO(3) base guides the reaction toward the coupling

265 The Cs-X-U-Si-O (X = F, Cl) pentanary phase space is used as

266 clathrate-like cage structure adopted by the Cs(+).(D(2)O)(20) ion.

267 , hydrogen-bonded water cages adopted by the Cs(+).(HDO)(D(2)O)(19) and D(3)O(+).(HDO)(D(2)O)(19) clu

268 ay diffraction studies were conducted in the Cs/Sn/P/Se system.

269 6)}(1 a(-) )].THF, asymmetric binding of the Cs(+) ion to the concave surface of 1 a(-) is observed,

270 asured the anisotropic kappa(L) value of the Cs(2)PbI(2)Cl(2) single crystal and observed an ultralow

271 ata and theoretical calculations suggest the Cs atom deviates from its ideal cuboctahedral geometry i

272 (charge, cation size) and suggests that the Cs sorption mechanism (cation exchange) is not similarly

273 ns with the Pb-Br frameworks compared to the Cs.

274 Remarkably, four of them, Cs(0.4)La(0.6)Mn(0.25)Co(0.75)O(3), Cs(0.3)La(0.7)NiO(3)

275 The presence of two or three Cs+ cations binding the nitride group is key for the iso

276 ltiply bound to two uranium and two or three Cs+ cations, these complexes transfer the nitride group

277 unique chemical shift that is attributed to Cs atoms terminating the surface of the particle and whi

278 ed by conformational switching from a C3h to Cs symmetry of mTBPB via rotation of m-phenylene units.

279 Group 1 of the periodic table from Li(+) to Cs(+), PFL-AE activity sharply maximizes at K(+), with N

280 The high conformational selectivity toward Cs-conformers is templated by the twofold coordination t

281 in [{Cs(+) (18-crown-6)}(2) (1 a(2-) )], two Cs(+) ions bind to both the concave and convex surfaces

282 U, Cs, Ba, Rb, K, and Ca isotopic ratios were determined on

283 a zigzag Sc2C2 unit inside an unprecedented Cs(hept)-C88 carbon cage containing 13 pentagons, 32 hex

284 trend: they show no octahedral tilting upon Cs-substitution but only a contraction of the lattice, l

285 sions of our previous publication which used Cs and Li as traditional ISTDs.

286 Using Cs(2)CuCl(4) as a model system, we demonstrate an altern

287 The valence Cs 6s orbital lies too high to be involved in bonding, a

288 Since differently activated VEGF-Cs are characterized by successively shorter N-terminal

289 While Cs occupies a single site from 100 to 150 K, it splits b

290 ) is exothermic by -10.4 kcal mol(-1), while Cs and Bi guests are too large to be accommodated but ar

291 Reduction of {Fe-NO}(9) with Cs electride finally yields the highly reduced {Fe-NO}(1

292 In contrast, controlled reaction of 1 a with Cs allowed the isolation of singly and doubly reduced fo

293 and (crypt) and 18-crown-6 (18-c-6) and with Cs in the presence of crypt.

294 outcompete Cs(+) by 1.8-2.1-fold; i.e., with Cs(+) in 2-fold excess of Na(+) the ion atmosphere would

295 Replacing Na(+) with Cs(+) does not alter the FRET efficiencies of the states

296 Reduction of the unstable red solid with Cs metal produces the dianion of the title compound, fro

297 also isolated as a contact-ion complex with {Cs(18-crown-6)}(+) cations, thereby adding the effect of

298 In contrast (to previous work), Cs as a traditional ISTD resulted in final RSDs of 2.5-8

299 wide range of Cs concentrations (1.1-19 wt% Cs as Cs2O).

300 d-cation compounds (FA(1-) (x) (-) (y) MA(x) Cs(y) PbI(3-) (z) Br(z) ) as photovoltaic absorbers, as