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1 tely the same size and density but different compressibility.
2 o exhibits both positive and negative linear compressibility.
3 re-response range due to the poor structural compressibility.
4 ime scale and suggesting regions of variable compressibility.
5 uding free energy, partial molar volume, and compressibility.
6 amatic decrease in clot volume and a peak in compressibility.
7 ase in the lipid assemblies' total adiabatic compressibility.
8  compression tests to evaluate stiffness and compressibility.
9 temperature dependence of a solute's partial compressibility.
10 emoral and popliteal veins were assessed for compressibility.
11 icant changes in density, heat capacity, and compressibility.
12  under decompression, i.e., exhibit negative compressibility.
13 nd it also prevents reordering the atoms for compressibility.
14  shift that reflects local variations in the compressibility.
15 nced Fermi velocity, and interaction-reduced compressibility.
16  at velocities controlled by the interface's compressibility.
17 c moment and occurrence of axial alternative compressibility.
18  properties unique to bulk materials such as compressibility.
19 ing to curvature localization and a negative compressibility.
20 pansibility while resulting in a decrease in compressibility.
21 ivity), which dictates viscosity and affects compressibility.
22 when stretched, so they have positive linear compressibilities.
23 s contain four parameters: bilayer thickness compressibility 1/B, bilayer bending rigidity Kc, the ch
24 e the density (0.1-1% relative uncertainty), compressibility (1% relative uncertainty), scattering co
25 he density (0.1-1% relative uncertainty) and compressibility (1-3% relative uncertainty) of previousl
26  is also accompanied by a positive change in compressibility, 14 x 10(-4) cm3 x mol(-1) x bar(-1), bu
27     Pressure shifts of holes allow the local compressibility about the APT to be determined.
28                                    The axial compressibility along a axis is more than five times sti
29             X-ray diffraction data show that compressibility along the c-axis changes around 12 GPa,
30                                    The layer compressibility also decreased with increasing carbohydr
31 ntify a molecular basis for the variation in compressibility among globular proteins.
32 )), Hepler's coefficient, hydration numbers, compressibilities and Jones-Dole coefficient B, among ot
33 ncluding negative Poisson's ratios, negative compressibilities and phononic bandgaps.
34                                         Both compressibilities and relative volume fluctuations in PL
35                    However, because the area compressibility and bending moduli of SM:cholesterol bil
36 m lengthscales yields the membranes' lateral compressibility and bending rigidity and demonstrates th
37 that relates etas to the pure DPPC monolayer compressibility and collapse pressure.
38 lar expansibility, apparent molar isentropic compressibility and compressibility hydration number.
39 t specific volume, isentropic apparent molar compressibility and compressibility hydration numbers an
40                   Finally, from the obtained compressibility and density, the acoustic scattering coe
41 ein (CRP) has been shown to modulate protein compressibility and dynamics.
42 e that provides its mechanical properties of compressibility and elasticity, is one of the first matr
43  water-binding capacity of aggrecan provides compressibility and elasticity.
44  the data reveal interaction-driven negative compressibility and electron-hole asymmetry in N = 0, 1
45  proposed that accounts for non-constant gas compressibility and enables systematic identification of
46                              Analysis of our compressibility and expansibility data reveals that the
47 sive molecular orientational disorder, giant compressibility and highly anharmonic lattice dynamics o
48                    Liquid water's isothermal compressibility and isobaric heat capacity, and the magn
49 etic surface activities, yielding lower film compressibility and lower maximum dynamic surface tensio
50 er MoTe(2) by combining the local electronic compressibility and magneto-optical measurements.
51 d several anomalies: maxima in the adiabatic compressibility and nonmonotonic density dependence of t
52 structural integrity of the nanotubes or the compressibility and porosity of the nanotube network.
53   The influence of the antiviral compound on compressibility and positional fluctuations is reported.
54 d result in rare properties: negative linear compressibility and stretch densification.
55 sibility reflects both the protein intrinsic compressibility and the difference between the compressi
56  capacity of unfolding infers a link between compressibility and the enthalpy of unfolding.
57 ther, a newly recognized correlation between compressibility and the heat capacity of unfolding infer
58 ctures, effectively enhancing the structural compressibility and the pressure-response range.
59                                     Both the compressibility and the thermal expansion of the eluent
60  solutions have been studied via volumetric, compressibility and viscometric properties at T = (288.1
61 an predicts full coexistence curves, osmotic compressibilities, and second virial coefficients under
62 the DPPC bilayer; bulk compressibility, area compressibility, and bending modulus were only perturbed
63  surface layer, but its charge, thicknesses, compressibility, and mass are significantly larger on mi
64 yer thickness (which we refer to as length), compressibility, and spacing between the individual mole
65 at low temperature in the heat capacity, the compressibility, and the coefficient of thermal expansio
66 lar atoms is somewhat larger than bulk water compressibility, and the compressibility of water around
67 he nonpolar antiviral compound increases the compressibility, and thus the conformational flexibility
68 and partial molar volumes, apparent specific compressibility, apparent specific volume, transfer volu
69  for achieving such negative linear and area compressibilities are described for single crystals and
70 t regimes, characterized by their degrees of compressibility, are isolated in the parameter space.
71 hanical properties of the DPPC bilayer; bulk compressibility, area compressibility, and bending modul
72                          A sharp drop in the compressibility as a function of the electron density, a
73 their isentropic apparent molar and specific compressibilities, as well as their compressibility hydr
74 s,2,varphi, and apparent specific isentropic compressibilities, ASIC, were calculated from measured d
75 tandard partial molar volumes and isentropic compressibilities at infinite dilution of saccharides, t
76      These many-body states exhibit negative compressibility but the compressibility returns to posit
77 ulted in condensed films with lower in-plane compressibilities, but consistently larger cross-section
78 ate also has no significant influence on the compressibility calculated for cyt c, although a slightl
79 aracterized by similar changes in volume and compressibility calculated per mole Co(NH(3))(6)(3+): De
80                              An effective 2D compressibility can arise, for example, from the converg
81 ity), as a result of dynamic changes in bead compressibility causing the displacement of the bead fro
82 ependence of the volume change, the standard compressibility change (Delta K(o)T), is typically assum
83 a were fitted to a model that assumes a zero compressibility change, the Delta G(o) value of 4.0 +/-
84 compressive modulus), volumetric or apparent compressibility changes (as further indicated by apparen
85                                          The compressibility changes are consistent with changes in s
86  first transition is evidenced by noticeable compressibility changes in distinct Raman-active modes,
87                               The isothermal compressibility coefficient (beta(T)(lipid)) of PLFE LUV
88 isothermal compressibility, their respective compressibility coefficients, partial specific volume, a
89 ignificantly larger bending modulus and area compressibility compared to DPPC.
90 ti-string BWT is also shown to have a higher compressibility compared with the input multi-string BWT
91 er-tetrahedral bond angle, resulting in high compressibility, continual breakup of tetrahedral connec
92 n and molten silicates, indicating that melt compressibility controls siderophile-element partitionin
93                               An increase in compressibility correlates with an entropically more fav
94                           Because electronic compressibility corresponds solely to the charge respons
95       Analysis of the elastic moduli of area compressibility (Cs(-1)) as a function of molecular area
96 chieved by using only density and isothermal compressibility data at atmospheric pressure through the
97                          We convert our area compressibility data into interfacial tension values to:
98                                    We report compressibility data on single-domain, globular proteins
99  by a volume decrease of 0.014 cm3 g-1 and a compressibility decrease of 3.8 x 10(-6) cm3 g-1 bar-1.
100 els, the nucleoid becomes spherical, and its compressibility decreases significantly.
101 olar volume (DeltaV degrees ) and isothermal compressibility (Deltabeta(T)) of conformational substat
102 artial molar volumes (DeltaV) and isothermal compressibilities (DeltakappaT ) between all the states
103  by high-precision measurements of the local compressibility, density, and pressure.
104 illouin quasilongitudinal results with axial compressibilities determined from high-pressure x-ray di
105       We also assess whether hydration water compressibility determined from small compound data can
106 bstantial impact across thermal expansivity, compressibility, dielectric constant, enthalpy of vapori
107 ion can be incorrect and that the neglect of compressibility differences can skew the interpretation
108 ives of Gibbs free energy (specific heat and compressibility) diverge at the transition point, result
109 eriments(7,8), and we predict an increase in compressibility due to ionization of the inner-core orbi
110 he data suggests a nonlinear increase of the compressibility due to the dense crowding that induces h
111 olar volume and the apparent molar adiabatic compressibility due to the interaction have been obtaine
112 poly[d(A-T)].poly[d(A-T)] complex volume and compressibility effects correspond to one direct or two
113                               The volume and compressibility effects of Ni(2+)-EDTA complex formation
114                                   Volume and compressibility effects of the first process are positiv
115  range from 11.7 to 23.9 cm(3)mol(-1)and the compressibility effects range from 19.3 x 10(-4)to 43.1
116  G+C content gives an increase in volume and compressibility effects, indicating a rise in the extent
117 g difficulties posed by woody roots and peat compressibility, enabling retrieval of relatively undist
118                                          The compressibility, estimated from the density fluctuations
119                      Imminent divergences of compressibility etc. unfortunately cannot be confirmed d
120 e properties (solubility, thermal stability, compressibility, etc.) of both new and existing drugs.
121 creases (two- to fourfold) in the "in-plane" compressibility for all three lipid types.
122 id mixtures yield smaller molecular area and compressibility for monolayers containing more saturated
123 bers, apparent massic volumes and isentropic compressibilities have also been determined.
124 ts of Co(NH(3))(6)(3+) binding on volume and compressibility have been obtained.
125 s, such as flyweight density, 80% reversible compressibility, high fatigue resistance, high electrica
126 pparent molar isentropic compressibility and compressibility hydration number.
127 sentropic apparent molar compressibility and compressibility hydration numbers and reported.
128 specific compressibilities, as well as their compressibility hydration numbers have been calculated a
129                       Their transfer values, compressibility hydration numbers, apparent massic volum
130             We present results for the local compressibility in all phases, observing a strong suppre
131 by taking the advantage of the difference in compressibility in oxide and selenide layers.
132 is for an adhesive-cohesive model of protein compressibility in which attractive forces from solvent
133 real and model networks, we demonstrate that compressibility increases with two common network proper
134                                          The Compressibility Index (CI=29.09-32.25%) and Hausner Rati
135 uir monolayer studies on EO revealed its low compressibility, indicating its low emulsifiability, and
136                                     Negative compressibility is a sign of thermodynamic instability o
137 l dependence of local lipid area and bilayer compressibility is also nonmonotonic in the first shell
138                         The observed maximum compressibility is consistent with theoretical models th
139 ulated for cyt c, although a slightly larger compressibility is predicted for myoglobin.
140                           Because isothermal compressibility is related to volume fluctuation, this s
141 uli for bending rigidity (kappa(C)) and area compressibility (K(A)).
142 es, for example heat capacity and isothermal compressibility kappaT, show a large increase.
143 reflected in an 8% increase in the intrinsic compressibility, kM, of the protein "native" state.
144  v(zero), and the partial specific adiabatic compressibilities, ks(zero), of globular proteins from t
145  V2( degrees ), and partial molar isentropic compressibilities, Ks,2( degrees ) at infinite dilution,
146 ific volumes, ASV, apparent molar isentropic compressibilities, Ks,2,varphi, and apparent specific is
147 ogether with the adhesive-cohesive model for compressibility, leads to the conclusion that folded pro
148 the macroscopic current density relation and compressibility matrix of the system and hence accessibl
149 oid intermediate formation, and the negative compressibility may be due to the effect of pressure on
150                                The increased compressibility may be due to the high concentrations of
151     Here, by performing dual conductance and compressibility measurements in the Kondo regime, we unc
152            Here, we present local electronic compressibility measurements of the FQH effect in the lo
153                              Here we perform compressibility measurements on electrons on liquid heli
154                      Absolute volumetric and compressibility measurements reveal that all three hairp
155                Here, through bulk electronic compressibility measurements, we investigate the LL stru
156 twisted BLG enabled by high-resolution local compressibility measurements.
157 e compared by determining their elastic area compressibility moduli (Cs-1) as a function of lateral p
158                       The calculated bilayer compressibility moduli agree with values estimated previ
159      Extraction from simulations of the area compressibility moduli of the monolayers in a bilayer is
160 ft bilayers are thicker and have larger area compressibility moduli than nonraft bilayers.
161 uid-condensed and liquid-expanded phase area compressibility moduli that are significantly larger tha
162 e provided by analyzing the interfacial area compressibility moduli.
163  for area/lipid (A = 47.2 +/- 0.5 A(2)), the compressibility modulus (K(A) = 500 +/- 100 dyn/cm), var
164 etics of bilayer bending, including the area compressibility modulus (K(a)), bilayer bending modulus
165 sition and ethanol concentration on the area compressibility modulus (K(a)), overall mechanical behav
166 cylate effectively reduces the apparent area compressibility modulus and bending modulus of membranes
167 ematically decreased with increasing bilayer compressibility modulus and bilayer thickness.
168 the known effects of cholesterol on the area-compressibility modulus and membrane structure, reaffirm
169 in the absence of tubule formation, the area compressibility modulus and, as such, the bending rigidi
170  tension, dipole density difference, and the compressibility modulus at surface pressures up to the s
171 ut does not greatly alter the actual elastic compressibility modulus at the maximal tested concentrat
172            Quantitatively, the trend in area compressibility modulus follows Traube's rule of interfa
173                                     Our area compressibility modulus K(A) decreased with increasing t
174 rements indicate that the lipid bilayer area compressibility modulus KA is increased by a large amoun
175  mainly attributed to a decrease in the area compressibility modulus KA We propose that the insertion
176 oncentration required to reach the same area compressibility modulus was reduced roughly by a factor
177                             The elastic area compressibility modulus was unaffected between pH 3 and
178 atches to the pore rim and the apparent area compressibility modulus, an intrinsic elastic modulus mo
179 as a decrease in their bending modulus, area compressibility modulus, and viscosity.
180 cohol concentration in the bilayer, and area compressibility modulus, as a function of alcohol chain
181 ette aspiration to directly measure the area compressibility modulus, bending modulus, lysis tension,
182  dependent on the bilayer area per molecule, compressibility modulus, or dipole potential, but did de
183 ted proteins by proteases decreases the area compressibility modulus, whereas fixation and cross-link
184 ding to lower lateral diffusion and a higher compressibility modulus, which agrees well with availabl
185  bilayer midplane) and k(m) is the monolayer compressibility modulus.
186 al that exhibits the strongest negative area compressibility (NAC) effect ever observed-a remarkable
187 ts the strongest ever observed negative area compressibility (NAC), an extremely rare property, as at
188 ined by radiography, revealed an increase in compressibility near 100 gigapascals indicative of such
189 as strong asymmetric jumps of the electronic compressibility near integer fillings of the moire latti
190 ons at the fivefold axis and the increase in compressibility near the WIN pocket are discussed in rel
191 spectroscopy (ARPES) for negative electronic compressibility (NEC) in the quasi-three-dimensional (3D
192 ectroscopic signature of negative electronic compressibility (NEC), a result of electron-electron int
193 is a direct signature of negative electronic compressibility (NEC).
194 tructures, which may exhibit negative linear compressibility (NLC) (that is, they expand in one or mo
195 of mechanical anisotropy and negative linear compressibility (NLC) along its c axis.
196 )](3) exhibits the strongest negative linear compressibility (NLC) effect over the largest pressure r
197 unterintuitive phenomenon of negative linear compressibility (NLC) is a highly desirable but rare pro
198 lous elastic behavior (e.g., negative linear compressibility, NLC), transitions between crystalline p
199 ized in terms of differences in their linear compressibilities occasioned by changes in the degree of
200 e backbone promoted closer packing and lower compressibilities of ceramide analogs in interfaces rela
201 t, in the entire temperature range examined, compressibilities of PLFE LUVs are low, comparable to th
202                            In this work, the compressibilities of seven MOFs belonging to two topolog
203           The relative thermal expansion and compressibilities of the cubic and orthorhombic forms ca
204 rmation decreases the total volume adiabatic compressibilities of the multilamellar vesicle assemblie
205    A natural definition then emerges for the compressibility of a network: the amount of information
206 pore area (~40%) when combined with the area compressibility of alpha-HL revealed an effective membra
207                            By leveraging the compressibility of biological scenes in a specific domai
208  around polar atoms is about the same as the compressibility of bulk water.
209 lysis for the measurement of the density and compressibility of cells and microbeads; these being the
210 force microscope, we have measured the axial compressibility of DNA and observed the buckling of the
211 proach provides a measure of the algorithmic compressibility of each data series.
212 aluminous perovskites, I have calculated the compressibility of end-member defect-bearing perovskites
213 is for the marked extensibility and negative compressibility of fibrin gels based on the structural a
214 nt a model which incorporates effects due to compressibility of gas in magma.
215 data cannot be used directly to estimate the compressibility of hydration water surrounding proteins.
216 ll compound data can be used to estimate the compressibility of hydration water surrounding proteins.
217 ffraction data also allow us to document the compressibility of ice at these extreme conditions and a
218 56 atmospheres give an estimate for the area compressibility of KA = 188 dyn/cm.
219                        The heat capacity and compressibility of liquid water anomalously increase on
220             Changes in unit cell volumes and compressibility of Ln(3) O(2) (CN(3) ) (Ln=La, Eu, Gd, T
221 onclusions about the origin of the anomalous compressibility of nanocrystals.
222 of multiple mutually coupled subsystems, the compressibility of one subsystem can be negative if it i
223 here that the cause of this softening is the compressibility of plutonium's thermally excited electro
224 of the structural variables that dictate the compressibility of porous materials.
225  for adjusting quality scores to improve the compressibility of quality scores without adversely impa
226                We report phase stability and compressibility of rhombohedral 3R-MoN(2), a newly disco
227 ater reduction in sedimentation velocity and compressibility of sediment formed than corn syrup solid
228                    The area per molecule and compressibility of SM condensed phases depended upon the
229 ideration of the effects of inertial forces, compressibility of solid and fluid, and arbitrary reflec
230                 CS methods demonstrating the compressibility of spin-echo spectra are presented for s
231     Conversely, hydration does not alter the compressibility of stoichiometric MnPt(CN)(6), but chang
232 or meconium, on the other hand, modifies the compressibility of surfactant films though optimal compr
233 n transistor to measure the local electronic compressibility of suspended graphene, and we observed a
234 s, the growth plates, and the elasticity and compressibility of the bone.
235 l as compressive strength while reducing the compressibility of the composite.
236            The partial volume and isothermal compressibility of the folded state are 100 mL mol(-1) a
237 on of soft gels need to account for both the compressibility of the gel network and a nonzero surface
238  to explore the dependence of the isothermal compressibility of the hydration shell surrounding globu
239  this capacitance originates from a negative compressibility of the interface electron system.
240                                          The compressibility of the intermediate is larger than that
241                                          The compressibility of the melt after the completion of the
242  SNAREs is interpreted as an increase in the compressibility of the membranes, which translates to a
243 oparticle volume fraction, and from this the compressibility of the microparticles is inferred.
244                Furthermore, we find that the compressibility of the nucleoid is not significantly aff
245 n be negative if it is countered by positive compressibility of the others.
246 me probed in the experiments represented the compressibility of the outer region of spectrin loops an
247  terms of an interplay between the intrinsic compressibility of the protein and solvation effects.
248 ical interferometry to examine the thickness compressibility of the red cell membrane in situ.
249 upled with mass-spectrometry (MS) to explore compressibility of the secondary structure of proteins u
250                 Their presence increases the compressibility of the solvent with the added effect of
251 ntropy of the quality scores and thereby the compressibility of these data (in FASTQ or SAM/BAM/CRAM
252 flux results from the piston-like mechanism, compressibility of water (increase in density of water d
253                              The density and compressibility of water adjacent to a melittin dimer is
254 ger than bulk water compressibility, and the compressibility of water around polar atoms is about the
255 s lower than bulk water compressibility, the compressibility of water hydrating apolar atoms is somew
256                                          The compressibility of water hydrating charged atoms is lowe
257                                          The compressibility of water in the protein hydration shell
258 mpressibility and the difference between the compressibility of water in the protein hydration shell
259 glect the simultaneous effects of the slight compressibility of water, sea-bed elasticity, and static
260 es may occur to the transport properties and compressibility of, e.g., fluids in planetary interiors,
261 tabilizes the negative bulk modulus (inverse compressibility) of the inclusions.
262 evealed no significant dependence of TM bulk compressibility on the presence of collagen XI.
263 y an integral role in either the diminution (compressibility) or retention (incompressibility) of ori
264                      Furthermore, volume and compressibility parameters of cation binding show hydrat
265 ialV&cjs1171;H2O/ partial differentialT) and compressibility ( partial differentialV&cjs1171;H2O/ par
266 .89 mol kg(-1).The apparent molar isentropic compressibility (PhiK(s)) and hydration number (nH) conf
267 ssibility of surfactant films though optimal compressibility properties recover on repetitive compres
268 dynamic property of folded proteins, protein compressibility provides important information about the
269  scholars have been studying the pore volume compressibility (PVC) of porous media.
270    The experimental determination of protein compressibility reflects both the protein intrinsic comp
271    Because of their lower density and higher compressibility relative to water, GVs experience strong
272 biomechanical properties (size, density, and compressibility), resulting in inherently label-free and
273 tes exhibit negative compressibility but the compressibility returns to positive in ultrahigh B.
274 y and the matrix thermodynamic dimensionless compressibility, S(0)(T) (which also quantifies the ampl
275            The temperature dependence of the compressibility, sound velocity and pseudo-Gruneisen par
276 -Vdpi arrangement despite the greater c-axis compressibility, suggesting that the hydride anions act
277 ctuations consistent with water's isothermal compressibility temperature trends.
278                           The data require a compressibility term, beta(o)(double dagger), to obtain
279 ygen vacancies do have significantly greater compressibilities than those without such vacancies.
280 exceptional sensitivity the dot's electronic compressibility, that is, its ability to accommodate cha
281 he onset of superfluidity is observed in the compressibility, the chemical potential, the entropy, an
282 ating charged atoms is lower than bulk water compressibility, the compressibility of water hydrating
283              Because of their large size and compressibility, the fNACPs robustly trap along the pres
284  to the increase in density fluctuations and compressibility, the positional fluctuations decreased d
285                In the regime of intermediate compressibility, the two different regularizations give
286 ed partial specific adiabatic and isothermal compressibility, their respective compressibility coeffi
287                          We relate intrinsic compressibility to stability by using molecular dynamics
288 nation number (6-9) and different polyhedral compressibilities, together with the observation of sign
289    The strain-driven counterpart of negative compressibility transitions is a force amplification phe
290  to design metamaterials exhibiting negative compressibility transitions, during which a material und
291 20 GPa, ultimately presenting the same axial compressibility trends with those of nonmagnetic compoun
292                   Not only is the duality in compressibility triggered by the availability of potenti
293 egapascal in pore pressure in rocks with low compressibility triggers earthquakes, including the 4.8-
294 f stretchability (up to approximately 100%), compressibility (up to approximately 25%) and bendabilit
295 ce measurements to probe the bulk electronic compressibility, we find that SOC leads to the formation
296 , using measurements of the local electronic compressibility, we show that these correlated phases or
297 the change in the partial specific adiabatic compressibility which accompanies the transition.
298 ers influences monolayer viscoelasticity and compressibility which, in turn, influence monolayer coll
299 he product of surface tension and isothermal compressibility, which is another fundamental lengthscal
300 gate the interplay between cell motility and compressibility within the CPM and find that the CPM pre

 
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