wanyu/IteraTeR_full_sent huggingface dataset:
Original:  In particular, we measure the degree of market efficiency by using the non-Bayesian time-varying model approach of Ito et al. (2014, 2015), which provides a more accurate measurement of market efficiency than conventional statistical inferences (i.e., statistical tests using the moving window method).
Revised:  In particular, we measure the degree of market efficiency by using a time-varying model approach of Ito et al. (2014, 2015), which provides a more accurate measurement of market efficiency than conventional statistical inferences (i.e., statistical tests using the moving window method).
Edit intent: clarity
Original:  In particular, we measure the degree of market efficiency by using the non-Bayesian time-varying model approach of Ito et al. (2014, 2015), which provides a more accurate measurement of market efficiency than conventional statistical inferences (i.e., statistical tests using the moving window method).
Revised:  In particular, we measure the degree of market efficiency by using the non-Bayesian time-varying model approach .
Edit intent: coherence
Original:  The empirical results show that (1)  market efficiency changes over time in the TOPIX and TSE2 , (2) the  market efficiency of the TSE2 is lower than that of the TOPIX in most periods, and (3) the market efficiency of the TOPIX has evolved since the bursting of the bubble economy in the early 1990s , but that of the TSE2 has not.
Revised:  The empirical results show that (1) the degree of market efficiency changes over time in the TOPIX and TSE2 , (2) the market efficiency of the TSE2 is lower than that of the TOPIX in most periods, and (3) the market efficiency of the TOPIX has evolved since the bursting of the bubble economy in the early 1990s , but that of the TSE2 has not.
Edit intent: clarity
Original:  The empirical results show that (1)  market efficiency changes over time in the TOPIX and TSE2 , (2) the  market efficiency of the TSE2 is lower than that of the TOPIX in most periods, and (3) the market efficiency of the TOPIX has evolved since the bursting of the bubble economy in the early 1990s , but that of the TSE2 has not.
Revised:  The empirical results show that (1) market efficiency changes over time in the two markets , (2) the market efficiency of the TSE2 is lower than that of the TOPIX in most periods, and (3) the market efficiency of the TOPIX has evolved since the bursting of the bubble economy in the early 1990s , but that of the TSE2 has not.
Edit intent: clarity
Original:  The empirical results show that (1)  market efficiency changes over time in the TOPIX and TSE2 , (2) the  market efficiency of the TSE2 is lower than that of the TOPIX in most periods, and (3) the market efficiency of the TOPIX has evolved since the bursting of the bubble economy in the early 1990s , but that of the TSE2 has not.
Revised:  The empirical results show that (1) market efficiency changes over time in the TOPIX and TSE2 , (2) the level of market efficiency of the TSE2 is lower than that of the TOPIX in most periods, and (3) the market efficiency of the TOPIX has evolved since the bursting of the bubble economy in the early 1990s , but that of the TSE2 has not.
Edit intent: clarity
Original:  The empirical results show that (1)  market efficiency changes over time in the TOPIX and TSE2 , (2) the  market efficiency of the TSE2 is lower than that of the TOPIX in most periods, and (3) the market efficiency of the TOPIX has evolved since the bursting of the bubble economy in the early 1990s , but that of the TSE2 has not.
Revised:  The empirical results show that (1) market efficiency changes over time in the TOPIX and TSE2 , (2) the market efficiency of the TSE2 is lower than that of the TOPIX in most periods, and (3) the market efficiency of the TOPIX has evolved , but that of the TSE2 has not.
Edit intent: coherence
Original:  We present an outline of the correct proof , clarifying the structure of the relevant funding accounts, and show that the final result in "Funding beyond discounting" is correct, even if the self-financing condition used in the proof is not.
Revised:  We present an outline of the derivation that yields the correct statement of the self-financing condition , clarifying the structure of the relevant funding accounts, and show that the final result in "Funding beyond discounting" is correct, even if the self-financing condition used in the proof is not.
Edit intent: meaning-changed
Original:  We present an outline of the correct proof , clarifying the structure of the relevant funding accounts, and show that the final result in "Funding beyond discounting" is correct, even if the self-financing condition used in the proof is not.
Revised:  We present an outline of the correct proof , clarifying the structure of the relevant funding accounts, and show that the final result in "Funding beyond discounting" is correct, even if the self-financing condition stated is not.
Edit intent: clarity
Original:  Here, we describe the model and inference algorithm and apply them to a synthetic six-gene system, demonstrating that the model is detailed and flexible enough to account for activation and repression as well as synergistic and self-regulation, and that the algorithm can efficiently and accurately recover the parameters used to generate the data.
Revised:  Here, we describe the model and inference algorithm and apply them to a synthetic six-gene system, demonstrating that the model is detailed and flexible enough to account for activation and repression as well as synergistic and self-regulation, and the algorithm can efficiently and accurately recover the parameters used to generate the data.
Edit intent: fluency
Original:  The theoretical results relate the dependence consistency of CoVaR using conditioning on X>=VaR_\alpha(X) to well established results on concordance ordering of multivariate distributions or their copulas.
Revised:  We prove general results that relate the dependence consistency of CoVaR using conditioning on X>=VaR_\alpha(X) to well established results on concordance ordering of multivariate distributions or their copulas.
Edit intent: clarity
Original:  The counterexamples for CoVaR based on the stress event X=VaR_\alpha(X) include inconsistency with respect to correlation in the bivariate Gaussian model .
Revised:  We provide counterexamples showing that CoVaR based on the stress event X=VaR_\alpha(X) include inconsistency with respect to correlation in the bivariate Gaussian model .
Edit intent: clarity
Original:  The counterexamples for CoVaR based on the stress event X=VaR_\alpha(X) include inconsistency with respect to correlation in the bivariate Gaussian model .
Revised:  The counterexamples for CoVaR based on the stress event X=VaR_\alpha(X) is not dependence consistent. In particular, if (X,Y) is bivariate normal, then CoVaR based on X=VaR_\alpha(X) is not an increasing function of the correlation parameter. Similar issues arise in the bivariate Gaussian model .
Edit intent: meaning-changed
Original:  The counterexamples for CoVaR based on the stress event X=VaR_\alpha(X) include inconsistency with respect to correlation in the bivariate Gaussian model .
Revised:  The counterexamples for CoVaR based on the stress event X=VaR_\alpha(X) include inconsistency with respect to correlation in the bivariate t model and in the model with t margins and a Gumbel copula. In all these cases, CoVaR based on X>=VaR_\alpha(X) is an increasing function of the dependence parameter .
Edit intent: meaning-changed
Original:  We also derive a threshold for the capping rate, below which zeroth order characteristics are predicted to dominate the dynamics of the network for all accessible filament densities.
Revised:  We also derive a threshold for the capping rate, above which autocatalytic growth is predicted at sufficiently low filament number. Below the threshold, zeroth order characteristics are predicted to dominate the dynamics of the network for all accessible filament densities.
Edit intent: meaning-changed
Original:  We also derive a threshold for the capping rate, below which zeroth order characteristics are predicted to dominate the dynamics of the network for all accessible filament densities. For capping rates above this threshold, autocatalytic growth is predicted at sufficiently low filament density .
Revised:  We also derive a threshold for the capping rate, below which zeroth order characteristics are predicted to dominate the dynamics of the network for all accessible filament numbers. Together, this allows cells to grow stable actin networks over a large range of different conditions .
Edit intent: clarity
Original: In this paper we ask whether  arbitrage-free prices are obtained by utility maximization. This is found to be true for any given investor , provided that one considers the marginal utility-based prices relative to all initial endowments with finite utility  .
Revised: In this paper we ask whether arbitrage-free prices at which an utility-maximizing agent would always want to buy the derivative, irrespectively of his own initial endowment of derivatives and cash. We prove that this is false for any given investor , provided that one considers the marginal utility-based prices relative to all initial endowments with finite utility .
Edit intent: meaning-changed
Original:  This is found to be true for any given investor , provided that one considers the marginal utility-based prices relative to all initial endowments with finite utility  .
Revised:  This is found to be true for any given investor , provided that one considers the marginal utility-based prices relative to all initial endowments with finite utility , and that it can instead be true if one restricts to the endowments in the interior. We show however how the endowments on the boundary can give rise to very odd phenomena; for example, an investor with such an endowment would choose not to trade in the derivative even at prices arbitrarily close to some arbitrage price .
Edit intent: meaning-changed
Original: We report conducting probe atomic force microscopy (CP-AFM) measurements of electron transport (ETp), as a function of temperature and force, through monolayers of holo-azurin (holo-Az) and Cu-depleted Az (apo-Az)that retain only their tightly bound water, immobilized on gold surfaces.
Revised: The mechanisms of solid-state electron transport (ETp) via a monolayer of immobilized Azurin (Az) was examined by conducting probe atomic force microscopy (CP-AFM) measurements of electron transport (ETp), as a function of temperature and force, through monolayers of holo-azurin (holo-Az) and Cu-depleted Az (apo-Az)that retain only their tightly bound water, immobilized on gold surfaces.
Edit intent: meaning-changed
Original: We report conducting probe atomic force microscopy (CP-AFM) measurements of electron transport (ETp), as a function of temperature and force, through monolayers of holo-azurin (holo-Az) and Cu-depleted Az (apo-Az)that retain only their tightly bound water, immobilized on gold surfaces.
Revised: We report conducting probe atomic force microscopy (CP-AFM) , both as function of temperature and force, through monolayers of holo-azurin (holo-Az) and Cu-depleted Az (apo-Az)that retain only their tightly bound water, immobilized on gold surfaces.
Edit intent: clarity
Original: We report conducting probe atomic force microscopy (CP-AFM) measurements of electron transport (ETp), as a function of temperature and force, through monolayers of holo-azurin (holo-Az) and Cu-depleted Az (apo-Az)that retain only their tightly bound water, immobilized on gold surfaces. The changes in CP-AFM current-voltage ( I-V) curves for holo-Az and apo-Az, measured between 250 - 370K, are strikingly different.
Revised: We report conducting probe atomic force microscopy (CP-AFM) measurements of electron transport (ETp), as a function of temperature ( I-V) curves for holo-Az and apo-Az, measured between 250 - 370K, are strikingly different.
Edit intent: clarity
Original:  The changes in CP-AFM current-voltage ( I-V) curves for holo-Az and apo-Az, measured between 250 - 370K, are strikingly different. While ETp across holo-Az at low force (6 nN) is temperature-independent over the whole examined range, ETp across apo-Az is thermally activated , with calculated activation energy of 600%DIFDELCMD < \pm100 %%% meV.
Revised:  The changes in CP-AFM current-voltage ( I-V) curves for holo-Az and apo-Az, measured between 250 - 373K) and of applied tip force (6-12 nN). By varying both temperature and force in CP-AFM, we find that the ETp mechanism can alter with a change in the force applied via the tip to the proteins. As the applied force increases, ETp via Az changes from temperature-independent over the whole examined range, ETp across apo-Az is thermally activated , with calculated activation energy of 600%DIFDELCMD < \pm100 %%% meV.
Edit intent: meaning-changed
Original:  While ETp across holo-Az at low force (6 nN) is temperature-independent over the whole examined range, ETp across apo-Az is thermally activated , with calculated activation energy of 600%DIFDELCMD < \pm100 %%% meV.
Revised:  While ETp across holo-Az at low force (6 nN) is temperature-independent to thermally activated at high temperatures. This is in contrast to the Cu-depleted form of Az ( apo-Az is thermally activated , with calculated activation energy of 600%DIFDELCMD < \pm100 %%% meV.
Edit intent: meaning-changed
Original:  While ETp across holo-Az at low force (6 nN) is temperature-independent over the whole examined range, ETp across apo-Az is thermally activated , with calculated activation energy of 600%DIFDELCMD < \pm100 %%% meV.
Revised:  While ETp across holo-Az at low force (6 nN) is temperature-independent over the whole examined range, ETp across apo-Az %DIFDELCMD < \pm100 %%% meV.
Edit intent: coherence
Original:  While ETp across holo-Az at low force (6 nN) is temperature-independent over the whole examined range, ETp across apo-Az is thermally activated , with calculated activation energy of 600%DIFDELCMD < \pm100 %%% meV. These results confirm our results of macroscopic contact area ETp measurements via holo- and apo-Az, as a function of temperature, where the crucial role of the Cu redox centre has been observed. While increasing the applied tip force from 6 to 12 nN did not significantly change the temperature dependence of ETp via apo-Az, ETp via holo-Az changed qualitatively, namely from temperature-independent at 6 nN to thermally activated at forces \geq 9 nN, suggesting changes in the protein structure upon increasing the applied force.
Revised:  While ETp across holo-Az at low force (6 nN) is temperature-independent over the whole examined range, ETp across apo-Az is thermally activated , with calculated activation energy of 600%DIFDELCMD < \pm100 %%% ), where increasing the applied tip force from 6 to 12 nN did not significantly change the temperature dependence of ETp via apo-Az, ETp via holo-Az changed qualitatively, namely from temperature-independent at 6 nN to thermally activated at forces \geq 9 nN, suggesting changes in the protein structure upon increasing the applied force.
Edit intent: coherence
Original:  While increasing the applied tip force from 6 to 12 nN did not significantly change the temperature dependence of ETp via apo-Az, ETp via holo-Az changed qualitatively, namely from temperature-independent at 6 nN to thermally activated at forces \geq 9 nN, suggesting changes in the protein structure upon increasing the applied force.
Revised:  While increasing the applied force causes only small quantitative effects, that fit with a decrease in electrode spacing. At low force ETp via holo-Az changed qualitatively, namely from temperature-independent at 6 nN to thermally activated at forces \geq 9 nN, suggesting changes in the protein structure upon increasing the applied force.
Edit intent: meaning-changed
Original:  While increasing the applied tip force from 6 to 12 nN did not significantly change the temperature dependence of ETp via apo-Az, ETp via holo-Az changed qualitatively, namely from temperature-independent at 6 nN to thermally activated at forces \geq 9 nN, suggesting changes in the protein structure upon increasing the applied force.
Revised:  While increasing the applied tip force from 6 to 12 nN did not significantly change the temperature dependence of ETp via apo-Az, ETp via holo-Az is temperature-independent at 6 nN to thermally activated at forces \geq 9 nN, suggesting changes in the protein structure upon increasing the applied force.
Edit intent: clarity
Original:  While increasing the applied tip force from 6 to 12 nN did not significantly change the temperature dependence of ETp via apo-Az, ETp via holo-Az changed qualitatively, namely from temperature-independent at 6 nN to thermally activated at forces \geq 9 nN, suggesting changes in the protein structure upon increasing the applied force. The capability of exploring ETp by CP-AFM  over a significant range of temperatures, with varying tip force to detect possible pressure-induced changes in the sample , significantly adds to the ability to study ETp through proteins and of using ETp to study proteins, with this approach .
Revised:  While increasing the applied tip force from 6 to 12 nN did not significantly change the temperature dependence of ETp via apo-Az, ETp via holo-Az changed qualitatively, namely from temperature-independent and thermally activated via apo-Az. This observation agrees with macroscopic-scale measurements, thus confirming that the difference in ETp dependence on temperature between holo- and apo-Az is an inherent one that may reflect a difference in rigidity between the two forms. An important implication of these results, which depend on CP-AFM over a significant range of temperatures, with varying tip force to detect possible pressure-induced changes in the sample , significantly adds to the ability to study ETp through proteins and of using ETp to study proteins, with this approach .
Edit intent: meaning-changed
Original:  The capability of exploring ETp by CP-AFM  over a significant range of temperatures, with varying tip force to detect possible pressure-induced changes in the sample , significantly adds to the ability to study ETp through proteins and of using ETp to study proteins, with this approach .
Revised:  The capability of exploring ETp by CP-AFM measurements over a significant range of temperatures, with varying tip force to detect possible pressure-induced changes in the sample , significantly adds to the ability to study ETp through proteins and of using ETp to study proteins, with this approach .
Edit intent: clarity
Original:  The capability of exploring ETp by CP-AFM  over a significant range of temperatures, with varying tip force to detect possible pressure-induced changes in the sample , significantly adds to the ability to study ETp through proteins and of using ETp to study proteins, with this approach .
Revised:  The capability of exploring ETp by CP-AFM over a significant temperature range , significantly adds to the ability to study ETp through proteins and of using ETp to study proteins, with this approach .
Edit intent: clarity
Original:  The capability of exploring ETp by CP-AFM  over a significant range of temperatures, with varying tip force to detect possible pressure-induced changes in the sample , significantly adds to the ability to study ETp through proteins and of using ETp to study proteins, with this approach .
Revised:  The capability of exploring ETp by CP-AFM over a significant range of temperatures, with varying tip force to detect possible pressure-induced changes in the sample , is that for ETp measurements on floppy systems, such as proteins, the stress applied to the sample should be kept constant or, at least controlled during measurement .
Edit intent: coherence
Original:  We found that the reaction rates of two-dimensional systems consistently exhibit a maximum at a high volume fraction of molecules , such that two molecules in the vicinity cannot easily exchange their positions .
Revised:  We found that the signal flow of the system, defined as the activation rate of target protein, shows the following non-trivial variations against the change in the volume fraction of molecules , such that two molecules in the vicinity cannot easily exchange their positions .
Edit intent: meaning-changed
Original:  We found that the reaction rates of two-dimensional systems consistently exhibit a maximum at a high volume fraction of molecules , such that two molecules in the vicinity cannot easily exchange their positions .
Revised:  We found that the reaction rates of two-dimensional systems consistently exhibit a maximum at a high volume fraction of molecules or the affinity of the target protein to the membrane. For example, with an increase in the binding rate of target proteins to the membrane, the signal flow varies in the form i) monotonically increasing, ii) increasing then decreasing in a bell-shaped curve, or iii) increasing, decreasing then, increasing in an S-shaped curve .
Edit intent: meaning-changed
Original:  We further demonstrated that molecular crowding influences the hierarchical molecular distributions throughout the reaction process. The signaling proteins tend to surround the receptors, and the target proteins tend to become distributed around the signaling protein-receptor clusters.
Revised:  We further demonstrated that molecular crowding influences the hierarchical molecular distributions throughout the reaction processes. In particular, when the system exhibits large signal flow, the signaling proteins tend to surround the receptors, and the target proteins tend to become distributed around the signaling protein-receptor clusters.
Edit intent: meaning-changed
Original:  Here, the signaling proteins are activated by receptors  and these activated signaling proteins activate target proteins , causing that to unbind from the membrane . We found that the signal flow of the system, defined as the activation rate of target protein, shows the following non-trivial variations against the change in the volume fraction of molecules or the affinity of the target protein to the membrane.
Revised:  Here, the signaling proteins are activated by receptors and these activated signaling proteins activate target proteins , causing that to unbind from the membrane if activated. If the target proteins bind frequently, the volume fraction of molecules or the affinity of the target protein to the membrane.
Edit intent: meaning-changed
Original:  We found that the signal flow of the system, defined as the activation rate of target protein, shows the following non-trivial variations against the change in the volume fraction of molecules or the affinity of the target protein to the membrane. For example, with an increase in the binding rate of target proteins to the membrane , the signal flow varies in the form i) monotonically increasing , ii) increasing then decreasing in a bell-shaped curve , or iii) increasing, decreasing then, increasing in an S-shaped curve.
Revised:  We found that the signal flow of the system, defined as the activation rate of target protein, shows the following non-trivial variations against the change in the volume fraction of molecules on the membrane becomes so large that the excluded volume of the molecules for the reaction and diffusion dynamics cannot be negligible. We find that such excluded volume effects of the molecules induce non-trivial variations of the signal flow, defined as the activation frequency of target proteins, as follows. With an increase in the binding rate of target proteins to the membrane , the signal flow varies in the form i) monotonically increasing , ii) increasing then decreasing in a bell-shaped curve , or iii) increasing, decreasing then, increasing in an S-shaped curve.
Edit intent: meaning-changed