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Systematic attribution of heatwaves to the emissions of carbon majors

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Definition of occasions

From the EM-DAT database, we choose the occasions solely after 2000, as a result of the reporting is extra full after this date25,50, and since local weather change has been proven to exert rising affect on extremes over this era51.

The places reported for the occasions within the EM-DAT database are names of cities, provinces, states or entire nations (for instance, France). Geographical boundaries are needed for the evaluation, so the places of EM-DAT are matched to spatial parts from GADM52 utilizing the next algorithm.

  1. 1.

    The reported ISO code is used to pre-select the spatial parts of GADM for the nation and any connected disputed territories.

  2. 2.

    The reported location is ready: changing spatial characters (accents, numbers and punctuation); eradicating further areas; lowercase letters for all characters; synthesizing particular sentences (for instance, ‘Kadamjay district in Batken oblast’ changing into ‘Kadamjay’); correcting for any change in regional aggregation (for instance, ‘Haute & Basse Normandie’ changing into ‘Normandie’); translating any area with out its variant in GADM (for instance, ‘Voreio Aigaio’ changing into ‘North Aegean’).

  3. 3.

    Each preselected spatial factor is in contrast with every factor of the ready reported location by making use of a personality matcher53 on its names and variants.

  4. 4.

    Each retained spatial factor is filtered utilizing a ready listing of false positives. For occasion, the placement for the state of ‘Ohio’ triggers the identification of the county ‘Ohio’ within the states of Kentucky and West Virginia, which haven’t been reported.

  5. 5.

    The listing of spatial parts is in contrast with the preliminary reported location, checking whether or not it matches appropriately. If not, the difficulty is carried out by means of the ready lists of recognized points in steps 2 and 4.

Another work, the dataset GDIS, can also be used to match EM-DAT places to geographical boundaries54. Both approaches have been developed independently. GDIS differs in that the places of all classes of hazards are analysed, however solely as much as 2018. Here, solely the hazards for heatwaves had been analysed, however as much as 2023. Moreover, GDIS makes use of GADM v.3.6, whereas our work makes use of GADM v.4.1.

In the EM-DAT database, the dates of the heatwaves are sometimes reported with the beginning and ending days. When each days are supplied, we use the typical of the every day common temperature over this actual interval. Other indicators could also be attainable26, however the common aggregates the important options of those heatwaves55. In specific, this selection is motivated by its relevance for the reported influence somewhat than its meteorological rarity. Heatwaves have an effect on native populations not solely by means of every day most temperatures but additionally by means of lack of cooling at night time, which might be estimated utilizing every day common temperatures. Sustaining excessive temperatures over time modifies the influence of a heatwave as effectively, justifying using averages over the interval of the heatwave somewhat than its peak. The annual indicator is calculated first on every grid level, then averaged over the outlined area to maximise the relevance of the indicator1,56. Furthermore, some occasions had been reported with out the beginning and/or ending day(s). We observe that heatwaves reporting each days and lasting lower than a month final on common for 8 days. Therefore, we use as an indicator for occasions with lacking days the utmost of the 8 days working common over the reported month. In the case that a number of months had been reported with lacking beginning and/or ending days, we lengthen the length of the working common by 1 month for every supplementary month reported.

Training of conditional distributions

The statistical mannequin of attribution research is fastidiously chosen to mannequin the frequencies and intensities of utmost occasions1,56. To seize attainable tendencies and non-stationarities, the distribution relies on the parameters pushed by explanatory variables. In this research, we go for the generalized excessive worth (GEV) distribution with a linear evolution of its location as outlined in equation (1). For yearly y within the pattern, the typical temperature over the interval and area of the occasion Ty is assumed to observe a GEV distribution of location μ, scale σ and form ξ, whereas the placement varies with the change in international imply floor temperature smoothed over the three earlier years (GMST).

$$T sim mathrm{GEV}(mu ={mu }_{0}+{mu }_{1}mathrm{GMST},sigma ={sigma }_{0},xi ={xi }_{0})$$

(1)

Although the statistical mannequin in equation (1) is frequent for the EEA of heatwaves1,56, we’ve got in contrast its efficiency with different potential fashions. Apart from this GEV mannequin, we’ve got examined three different distributions with linear and non-linear evolutions of the parameters: Gaussian, skew regular and generalized Pareto. Overall, our comparisons assessed by means of quantile–quantile plots point out that the GEV performs one of the best among the many 4 distributions, particularly when it comes to higher tail behaviours. We calculate the classical Bayesian data standards (BIC) to check their performances whereas decreasing the danger of over-fitting57. We observe that for all heatwaves, a stationary GEV has the bottom BIC. We word that the linear mannequin of equation (1) will not be all the time one of the best distribution based on the BIC, though the achieve in BIC from the linear mannequin to one of the best answer is all the time marginal. More quantitatively, the development in BIC from the stationary GEV to the linear mannequin represents between 88% and 100% of the development from the stationary mannequin to one of the best answer over all heatwaves analysed, with a mean of 98%. In different phrases, sophisticating additional the statistical mannequin would, on common, enhance the efficiency by solely 2%. This consequence confirms that this expression is essentially the most applicable for many heatwaves.

These matches are obtained by minimization of the adverse log chance (NLL) of the coaching pattern58. The first guess has its robustness improved utilizing preliminary regression to approximate the coefficients42,59. The form parameter is bounded between −0.4 and 0.4 (ref. 1). Moreover, the pattern is weighted throughout minimization of the NLL, with weights equal to the inverse of the density of the GMST. This method helps in offering equal efficiency over the total interval of GMST.

The selection of whether or not to incorporate the occasion or not when estimating the statistical mannequin has been extensively mentioned, though no ultimate consensus has been reached1,31,60. The outcomes introduced on this paper have been obtained by estimating the occasion, to stop eradicating factors from the observational file. To guarantee numerical convergence, a minimal chance of 10−9 was set for every level of the total pattern. It implies that the attributed occasions below factual situations won’t have return durations greater than a thousand million years, which we contemplate lengthy sufficient.

Estimating return durations for unlikely occasions with comparatively brief observational information stays tough34; thus, we append extra traces of proof1,56. Conditional distributions are educated for ERA5, used as reference, but additionally with BEST29 (Extended Data Fig. 1) and simulations from Climate Model Intercomparison Phase 6 (CMIP6)30,61. The following Earth system fashions (ESMs) from CMIP6 are used: ACCESS-CM2, ACCESS-ESM1-5, AWI-CM-1-1-MR, BCC-CSM2-MR, CESM2, CESM2-WACCM, CMCC-CM2-SR5, CMCC-ESM2, CanESM5, EC-Earth3, EC-Earth3-CC, EC-Earth3-Veg, EC-Earth3-Veg-LR, FGOALS-g3, GFDL-CM4, GFDL-ESM4, INM-CM4-8, INM-CM5-0, IPSL-CM6A-LR, KACE-1-0-G, KIOST-ESM, MIROC6, MPI-ESM1-2-HR, MPI-ESM1-2-LR, MRI-ESM2-0, NESM3, NorESM2-LM, NorESM2-MM and TaiESM1. For each heatwave, solely the ESMs with adequate efficiency are used, as described within the subsequent part. For ERA5 and BEST, we begin the time collection in 1950 for enough spatial protection over all areas62, and these time collection end in 2022 for BEST and 2023 for ERA5. For CMIP6, the time collection is calculated over the historic (1850–2014) (ref. 63) and the SSP2-4.5 (2015–2100) (ref. 64). This situation is chosen as a result of its emissions are the closest to these noticed over 2015-202 (ref. 36). Only runs with the preliminary situations termed r1i1p1f1 are used, because it was run by most ESMs. Only one ensemble member is used to facilitate the comparability of the parameters and possibilities from ESMs to these based mostly on observations.

Evaluation of the uncertainties

During the intense occasion evaluation, two sources of uncertainties are dealt with—particularly, on the conditional distributions and on the dealing with of observations and simulations.

During the coaching of conditional distributions, the uncertainties on the parameters are obtained utilizing an ensemble of 1,000 bootstrapped members, with replacements allowed in the course of the resampling. The conditional distributions are then used to evaluate the possibilities and intensities of the occasion, below a factual local weather and a counterfactual local weather. The factual local weather is outlined because the GMST noticed on the time of the occasion. The counterfactual local weather is outlined as the typical of the GMST over 1850–1900.

ESMs exhibit completely different efficiency in reproducing native climates; thus, not all fashions could also be helpful for occasion attribution1. We calculate the seasonalities of ERA5 and every ESM over 1950–2020 in every grid level over the area. We then common their correlation. The most applicable ESMs are the ten most consultant ESMs that maximize this common correlation.

Following the WWA method, not all fashions are retained for additional evaluation1,65. The factual distributions on the time of the occasion are in contrast with these of ERA5. Both the size and the form parameters of ERA5 and the mannequin should have their 95% confidence intervals overlapping. Otherwise, the mannequin can be discarded. Thus, the general choice course of is to type the ESMs by correlation with ERA5 seasonality, take away these with parameters inconsistent with ERA5 and choose the ten finest ESMs on this listing.

At this level, chance ratios and alter in intensities are obtained for an ensemble of datasets, every with uncertainties. To synthesize over this huge ensemble, equal weights are given to every bootstrap member of ERA5 and BEST, summarized into one distribution for observations. All stored ESMs are additionally given equal weights and summarized into one distribution for fashions. Finally, these distributions are averaged to infer the median and 95% confidence intervals. We level out that synthesizing these traces of proof could possibly be performed with different approaches1, though with out affecting the principle messages of this work.

Goodness of match for the conditional distributions

Although utilizing a non-stationary GEV with its location various linearly with GMST is a well-established method for EEA to statistically mannequin extremes below international warming, this setup might not be well-suited in remoted instances66. To be certain that the GEV mannequin represents the information adequately, the goodness of match is verified for every conditional distribution used on this evaluation with the tactic utilized in ref. 67.

For each heatwave, a number of datasets are used for evaluation, from which conditional distributions are fitted. The location and scale of every of those fitted conditional distributions are used to remodel the respective coaching pattern onto a stationary GEV(0, 1, ξ) with the identical form because the fitted conditional distribution. This reworked pattern has noticed quantiles, that are in contrast with the theoretical quantiles of a GEV(0, 1, ξ) in a quantile–quantile plot. This quantile–quantile plot describes how effectively the GEV mannequin describes the pattern. The uncertainty within the GEV parameters determines a confidence band within the quantiles across the identification line, as proven in Extended Data Fig. 2.

The fraction of the pattern out of the boldness band is deduced, estimated as a 95% confidence interval on the ensemble obtained from bootstrapping of the coaching of the conditional distribution. For every heatwave, the ensemble of conditional distributions is in contrast with an out-of-sample threshold at 5%. The outcomes are proven in Extended Data Fig. 3. If the median out-of-sample fraction throughout the conditional distributions is beneath the brink, the goodness of match is confirmed, and the heatwave is stored for the following evaluation. As proven in Extended Data Fig. 3, 217 heatwaves are retained, and 9 are faraway from the following evaluation. These 9 occasions faraway from evaluation are summarized in Extended Data Table 1.

Out of the 9 occasions, eight occurred in India, and the final one occurred in Japan. In the 217 heatwaves stored for evaluation, eight occasions occurred in India. Besides this obvious regional clustering, no discernible traits emerge with regard to the season or size of the heatwave. More analysis is required to research why these matches don’t carry out in addition to elsewhere for these particular occasions, which lies past the scope of this research.

Causality utilizing Granger causal inference

The well-established method1 for EEA combines observations and simulations through the use of non-stationary distributions. These distributions correlate the evolution of the local weather indicator T for the heatwave to GMST. Deducing causality, that local weather change brought about the occasion, utilizing this correlation depends on the robust physics-based understanding5,6,31,41,65,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97 that rising GMST tends to additionally enhance regional temperatures, not solely by means of its imply but additionally by means of the entire distribution inferred from pure variability, thus shifting the regional extremes as effectively. Yet, though there’s a robust bodily foundation for this causality, we are able to additionally examine the validity of this causality from a statistical perspective. Using Granger causal inference98, we might assess the predictive relationship between GMST and T, the local weather indicator of the occasion4.

The frequent method for Granger causality4,98 requires that the enter variables are stationary to coach vector auto-regressive fashions99. This is often verified by differentiating the variables, in different phrases, taking the interannual variability. This methodology would then assess whether or not the interannual variability of GMST can predict the interannual variability of T, thus specializing in the predictability of short-term shocks. However, the pattern comprises a stronger sign in contrast with the interannual variability. To account for long-term tendencies in GMST and T, Granger causality might be generalized utilizing the vector error correction mannequin (VECM)100. It requires the seek for an enough VECM mannequin based mostly on the Akaike data criterion101 and a co-integration check, for example, utilizing a Johansen check99. Nevertheless, this methodology nonetheless fails to account for non-linear results. An different is to make use of machine studying, resembling Random Forest fashions educated to foretell T with GMST by means of their lagged results102. Permutation checks are performed to evaluate the efficiency of Random Forest fashions educated on permuted lagged GMST, in contrast with the non-permuted model103. Applying this methodology accounts for the evolution of GMST and T, whereas additionally accounting for non-linear results.

By utilizing the latter methodology, solely three occasions have a median worth for the check above 0.05. As proven in Extended Data Fig. 4, for 214 occasions out of 217, we reject the null speculation, concluding that the evolution of GMST is Granger-causing the evolution of T. The three different occasions are listed in Extended Data Table 2. We discover that the median worth for the Granger causality stays comparatively low. Using IPCC phrases, it’s doubtless (>66%) that GMST Granger-caused the evolution of T for the occasion within the United States in 2011, whereas it is vitally doubtless (>90%) for all of the others. These three occasions are faraway from this evaluation.

Contributions from the carbon majors to international warming

The contributions of emissions of the carbon majors to international imply floor temperature are assessed with the reduced-complexity Earth system mannequin OSCARv3.3 (refs. 104,105). The mannequin embeds an ensemble of modules that replicate the behaviour of fashions of upper complexity105. OSCAR options the ocean and land carbon cycles with a bookkeeping module for CO2 emissions from land use and land cowl change, wetlands, permafrost, tropospheric and stratospheric chemistry, and international and regional local weather responses to those forcers. It accounts for the results of greenhouse gases (CO2, CH4, N2O and 37 halogenated compounds), short-lived local weather forcers (stratospheric water vapour, tropospheric and stratospheric ozone, major and secondary natural aerosols, nitrates, sulfates and black carbon), floor albedo change, volcanic exercise, photo voltaic radiation and contrails37,105.

OSCAR is run over the historic interval (1750–2023), following three units of simulations: (1) The first set of simulations is pushed by concentrations of greenhouse gases to make sure a match with the most recent observations. (2) The second set is pushed by emissions, utilizing the appropriate emissions from the primary set obtained by means of mass steadiness106,107. This is a management run that confirms that the estimated appropriate emissions result in the noticed atmospheric concentrations and is used as a reference for the next attribution runs. (3) In the third set of simulations, for every carbon main, the management run is repeated, however the CO2 and CH4 emissions of the most important are subtracted from the appropriate emissions. The distinction in final result (for instance, international temperature) between the management and this simulation provides the contribution of the most important. This method known as a residual attribution methodology108.

In all simulations, the radiative forcings from species or forcers which are neither CO2 nor CH4 (that’s, forcers that aren’t attributed on this research) are prescribed as international time collection based mostly on the most recent model of the Indicators of Global Climate Change35. Global time collection of atmospheric concentrations for the primary set of simulations come from the identical supply. Emissions of short-lived species (that have an effect on the atmospheric sink of CH4) are taken from the most recent model of the CEDS dataset109,110 and the up to date GFED4s dataset111 that extends the unique CMIP6 emissions from biomass burning112. Land use and land cowl change information are the identical as within the newest Global Carbon Budget36, during which we use each an up to date LUH2 dataset113 and the FAO-based dataset114.

OSCAR runs in a probabilistic framework to characterize the uncertainty within the modelling of the Earth system. This uncertainty is sampled by means of a Monte Carlo method with n = 2,400 parts. The uncertainty within the pure processes governing the atmospheric focus of CO2 and CH4 comes from the accessible parametrizations of OSCAR105,115,116. The uncertainty within the enter radiative forcing follows that of the IPCC AR6 (ref. 117) and is utilized uniformly to the entire time collection. The uncertainty within the enter land use and land cowl change is sampled by working one-half of the simulations with one dataset and the opposite half with the opposite dataset. There isn’t any uncertainty within the enter emissions. Finally, the uncooked uncertainty vary from the Monte Carlo is constrained with observational information by weighting the weather of the ensemble based mostly on their distance to the observations within the management simulations37,116. As constraining values, we use decadal CO2 emissions from fossil fuels and trade over 2012–2021 from the GCB36, decadal anthropogenic CH4 emissions over 2008–2017 from the AR6 (ref. 118) offset with their preindustrial worth from PRIMAP third-party-based estimates119,120, and decadal international imply floor temperature change over 2011–2020 from the AR6 (ref. 9).

Contributions from the carbon majors to heatwaves

We assess whether or not the chance might be written as a sum of phrases, with every time period related to contributions from anthropogenic actors or pure drivers.

We outline a area in house S. Every yr y, the temperature discipline over the area is averaged over a interval p of the yr, then over the area S, ensuing within the temperature Ty. The heatwave is characterised by the exceedance of the heatwave stage u by Ty, with u a real-valued scalar. Ty represents a real-valued steady random variable (Borel σ-algebra on the reals). Given the heatwave stage u, the goal chance is a survival perform P(Ty > u).

We assume that the chance of the heatwave is conditional on GMTy and that it follows the statistical mannequin launched in equation (1) and represented in equation (2). Every yr, the temperature over the area and the interval Ty is sampled from a non-stationary GEV distribution27. The parameters of this GEV distribution are the placement μ, the size σ and the form ξ. The location varies linearly with a covariate, the change in GMSTy on the corresponding yr.

$$P({T}_{y} > u|{textual content{GMST}}_{y})=1-text{GEV}(u|mu ={mu }_{0}+{mu }_{1}textual content{GMT},sigma ={sigma }_{0},xi ={xi }_{0})$$

(2)

With the analytical expression for the cumulative distribution perform of the GEV that follows equation (3):

$$textual content{GEV}(u|0,1,xi )=left{start{array}{c}exp (-{(1+xi u)}^{-1/xi }),textual content{for};xi ne 0,textual content{and},1+xi u > 0 exp (-exp (-u)),textual content{for};xi =0end{array}proper.$$

(3)

This well-established statistical mannequin is extensively used for EEA1,56 and has already been used extensively for heatwaves. We acknowledge {that a} extra subtle mannequin with extra covariates might additional enhance the efficiency121,122. However, this statistical mannequin has been proven to have good efficiency for heatwaves normally13, and extra covariates can stop using local weather fashions as extra traces of proof. The former part supplies extra grounds for the selection of this mannequin.

The causal concept utilized to local weather change justifies the decomposition of possibilities in a Gaussian case123,124. Given a statistical mannequin constructed on a non-stationary Gaussian distribution linearly pushed by GMST, if GMST might be cut up right into a sum of contributions, then the possibilities might be approximated as a sum of their related contributions123,124. However, the statistical mannequin introduced in equation (2) makes use of a GEV as an alternative of a Gaussian. Even by making an attempt to jot down the decomposition utilizing Bayes’s theorem and the inclusion–exclusion precept, the precise analytical type of every time period stays difficult. This is usually as a result of the variations in chance when eradicating a contribution to GMST rely on the preliminary worth of GMST. In different phrases, the non-linearity and the excessive variety of phrases result in an answer that can’t be computed precisely.

Instead, we suggest to approximate the answer and to research the standard of this approximation. The regular method to calculate contributions to local weather change is to run the statistical mannequin with all contributors, then to run it once more with out one contributor, the distinction similar to the contributor. This method is thereafter referred to as All-But-One (ABO). Thus, an emitter e with a contribution to international warming GMSTy,e would contribute to the chance of the occasion utilizing this method.

$${P}_{y,e}^{textual content{ABO}}=P({T}_{y} > u|{textual content{GMST}}_{y})-P({T}_{y} > u|{textual content{GMST}}_{y}-{textual content{GMST}}_{y,e})$$

(4)

To account for non-linear results within the decomposition of possibilities, this method is complemented with a second method that calculates the distinction in GMSTy launched by including solely the emitter (Add-One-to-None, AON). According to this method, the emitter e would contribute to the chance of the heatwave as follows:

$$start{array}{c}{P}_{y,e}^{textual content{AON}}=Pleft({T}_{y} > u|{textual content{GMST}}_{y,e},+,{textual content{GMST}}_{y}-sum _{e}{textual content{GMST}}_{y,e}proper) ,-,Pleft({T}_{y} > u|{textual content{GMST}}_{y}-sum _{e}{textual content{GMST}}_{y,e}proper)finish{array}$$

(5)

The method based mostly on the elimination of a single entity (ABO) estimates the contribution of a state perturbed by all the opposite contributors. The method based mostly on the addition of a single entity (AON) evaluates the contribution in an unperturbed state, with out the opposite contributors interfering. Given the non-linearity of the system, we count on the bodily contribution to be between the 2 values. We select to calculate each approaches and common them. This method, calculated utilizing equation (6), known as the mixed ABU & AON (Extended Data Fig. 5).

$${P}_{y,e}=frac{{P}_{y,e}^{textual content{ABO}}+{P}_{y,e}^{textual content{AON}}}{2}$$

(6)

For every occasion, the chance is calculated for all datasets for the area and averaged over the datasets. Its 95% confidence interval is calculated utilizing bootstrapping. The whole chance of the occasion is decomposed into contributions of every carbon main, different local weather forcers and preindustrial chance. After decomposition, these phrases are summed up for comparability with the overall chance. The 95% confidence interval is proven for all occasions, and just one occasion (Cyprus, May–September 2022) doesn’t reproduce the overall chance. This occasion has been faraway from the evaluation of utmost occasions. As proven in Extended Data Fig. 5, the typical of ABO and AON supplies one of the best estimate, as a result of it accounts for non-linear results.

In EEA, possibilities are sometimes communicated utilizing chance ratios, quantifying what number of occasions local weather change has made the occasion extra doubtless. It is calculated utilizing the chance of the occasion in a preindustrial local weather, thus with a GMST averaged over 1850–1900:

$$textual content{PR},=,frac{P({T}_{y} > u|{textual content{GMST}}_{y})}{P({T}_{y} > u|{textual content{GMST}}_{1850mbox{–}1900})}$$

(7)

Because the contribution of the emitter e to the chance of the heatwave Py,e is a perturbation, the emitter multiplies the chance of the heatwave as in equation (8):

$${textual content{PR}}_{e}=1+frac{{P}_{y,e}}{P({T}_{y} > u|{textual content{GMST}}_{1850mbox{–}1900})}$$

(8)

Discussing another decomposition method

Alternatively to the method based mostly on GMST, a fundamental method could be to evaluate the contributions immediately with the emissions. The fraction within the cumulative emissions on the time of the occasion would characterize the share of accountability of the carbon main within the causes of the occasion. This fraction can be utilized for the change in depth and the change in chance of the occasion. This method might be in contrast with the precept utilized for the attributional life cycle assessments, taking the Earth system as an entire and utilizing the shares in its inputs to hint the perturbation125,126, whereas the method based mostly on GMST traces the results of the carbon majors by means of the Earth system. Therefore, GMST is extra just like the precept of the consequential life cycle evaluation. However, the method based mostly on cumulative emissions has a number of drawbacks.

First, the carbon majors gasoline local weather change with CO2 and different compounds, resembling CH4. As an approximation, it might nonetheless be attainable to combination these compounds utilizing a world warming potential for fossil CH4.

Then, the carbon cycle partially absorbs the emitted carbon over time. Thus, two corporations with the identical cumulated emissions might not share the identical accountability, if one has older emissions, thus with a decrease contribution to the atmospheric focus of CO2. Still, these previous emissions contributed to warming up the Earth system and saturating the carbon sinks.

Finally, the attribution evaluation might not reply linearly to adjustments in GMST. For our research, heatwaves are represented with a GEV with the placement various linearly with GMST. According to the Transient Climate Response to Emissions (TCRE), the GMST varies virtually linearly with cumulative emissions. Thus, the method based mostly on cumulative emissions would result in related outcomes to ours. However, for occasions for which the distributions don’t fluctuate linearly with GMST, as it could for excessive precipitations1,56, non-linearities could be launched.

To conclude, the method based mostly on cumulative emissions is an approximation that depends on the linearity of the Earth system. However, this technique will not be solely linear, and the TCRE is named an approximation with its limits127. Under the assumptions that the linearity of the system could be revered, this straightforward method would then result in related outcomes as these based mostly on the method used on this work.


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https://www.nature.com/articles/s41586-025-09450-9
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