Widespread Higher Soil Respiration Rates at Nighttime Than Daytime Across Global Forest Ecosystems
Heng Huang, Jinyun Tang, Ben Bond‐Lamberty, Peter B. Reich, Thomas W. Crowther, Jinshi Jian, Kun Zhang, Lingli Liu, Jin Wu

TL;DR
Soil respiration rates are often higher at night than during the day in forests, which could affect predictions of carbon emissions and climate change.
Contribution
Discovery of widespread higher nighttime soil respiration rates in forests and their implications for climate models.
Findings
Nighttime soil respiration rates are higher than daytime rates across global forest ecosystems.
Using daytime temperature relationships underestimates nighttime soil respiration by up to 28.7%.
Current climate models likely underestimate nighttime root respiration dynamics.
Abstract
Soil respiration (R s) is the second largest terrestrial carbon flux and therefore its temporal dynamics exert a significant influence on the soil carbon budget. While the seasonal and annual dynamics of R s and its temperature sensitivity have been well documented, the diel R s dynamics remain poorly understood. Earth system models (ESMs) typically assume a constant temperature response of R s over the diel cycle, thereby predicting lower R s at night than during the warmer daytime. Here, by analyzing extensive in situ R s datasets from 36 global forest sites, we reveal an unexpectedly widespread pattern of higher nighttime than daytime R s, which is likely driven by the hourly temporal lag between recent photosynthetic assimilation and R s associated with the transportation of recent photosynthates to the roots. Moreover, applying daytime R s‐temperature relationships systematically…
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FIGURE 5- —National Natural Science Foundation of China10.13039/501100001809
- —HKU Seed Funding for Strategic Interdisciplinary Research Scheme
- —Hong Kong Research Grant Council Collaborative Research Fund
- —Young Talent Program from Guangdong Province
- —the Start‐up Grant from Sun Yat‐sen University
- —Fundamental Research Funds for the Central Universities from Sun Yat‐sen University
- —Innovation and Technology Fund (funding support to State Key Laboratory of Agrobiotechnology)10.13039/501100010428
- —Sun Yat‐sen University
- —Office of Science10.13039/100006132
- —Biological and Environmental Research10.13039/100006206
- —Chinese Universities Scientific Fund10.13039/501100005236
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Taxonomy
TopicsPlant Water Relations and Carbon Dynamics · Soil Carbon and Nitrogen Dynamics · Soil Moisture and Remote Sensing
Introduction
1
Global soils contain nearly three times the amount of carbon (C) present in the atmosphere, making them the largest terrestrial C reservoir (Lehmann and Kleber 2015). Soil respiration (R s) constitutes the second largest terrestrial C flux, releasing 75–100 Pg C per year into the atmosphere via the activity of plant roots and soil microorganisms (Hashimoto et al. 2023; Bond‐Lamberty et al. 2024). Despite its crucial role in regulating the soil C budget and overall ecosystem C storage (Bond‐Lamberty et al. 2024), R s cannot be observed directly through methods like eddy covariance towers or satellites, rendering it a highly uncertain component of the terrestrial C cycle (Warner et al. 2019). Improved understanding of how R s responds to climate change is essential for accurately predicting future soil C dynamics and evaluating the resilience of the land C sink (Ruehr et al. 2023).
Extensive research has explored the seasonal and annual variability of R s (Mo et al. 2005; Chen et al. 2014; Hursh et al. 2017) and its response to warming (Liang et al. 2024). Despite empirical evidence revealing significant differences in diel R s patterns observed at the single‐site level across diverse ecosystems (e.g., Xia et al. 2009; Ruehr et al. 2010; Brændholt et al. 2017; Hu et al. 2016; Makita et al. 2018; del Gutiérrez Arroyo and Wood 2020; Chu et al. 2023; Fekadu et al. 2022; Liu et al. 2024), the general cross‐site patterns of diel (day‐night) differences in R s, especially in forests, remain largely unclear (Han et al. 2023). Previous studies have reported overall higher R s during the day than at night (Liu et al. 2006; Ford et al. 2012), attributing this pattern primarily to fluctuations in soil temperature (T s) (Lloyd and Taylor 1994; Hirano 2005; Carey et al. 2016). In this study, we broadly evaluate both the questions at the heart of these reported findings and their interpretation, with a larger and more comprehensive dataset. For example, the idea that R s is higher at day than night due to higher daytime T s assumes that both the short‐term (minutes to hours) and long‐term (days to months) temperature sensitivity of R s (Q 10, the relative change in R s for a 10°C increase in temperature) remains constant throughout the day and night. Such a constant Q 10 assumption is often used in many current Earth system models (ESMs) to simulate R s and its components, that is, root respiration (R root) and soil microbial respiration (R h) (Ito et al. 2020; Guenet et al. 2024). However, recent in situ observations in a temperate forest have challenged this view, revealing significant diel differences in Q 10 (Han et al. 2023). These findings suggest that R s‐T s relationships can vary considerably between day and night, and that overlooking these variations may introduce substantial uncertainties into global R s flux estimates (Jian et al. 2018; Hashimoto et al. 2023; Bond‐Lamberty et al. 2024).
Investigating diel differences in R s and its temperature response is thus both timely and significant, especially in light of the growing evidence of a faster increase in minimum nighttime temperatures compared to maximum daytime temperatures in many regions worldwide (Doan et al. 2022). This asymmetric warming can directly impact biological metabolism and affect larger‐scale C fluxes (Peng et al. 2013). Therefore, understanding the diel difference in R s and its temperature response is of paramount importance, with direct relevance to reduce the high uncertainty in current ESMs' projection of soil C dynamics under climate change (Luo et al. 2016; Warner et al. 2019).
The growing availability of long‐term, continuous in situ R s measurements provides an opportunity to systematically evaluate these diel differences and their temperature sensitivity across various sites. This study aims to explore the diel difference in R s and R s‐T s relationships, as well as the associated uncertainty in estimating nighttime R s across global forest ecosystems. To achieve this, we utilize the global continuous soil respiration database (COSORE; Bond‐Lamberty et al. 2020), the global eddy covariance flux database (Pastorello et al. 2020), and ESM simulation outputs. Specifically, our research objectives are to (1) assess the consistency of diel patterns in R s across global forest sites and the potential underlying mechanisms; (2) evaluate the performance of current ESMs in capturing diel variations in R s and its components; and (3) quantify the uncertainty in nighttime R s estimation when not accounting for diel difference in R s‐T s relationships (e.g., using daytime R s‐T s relationships for nighttime estimation). To tackle these questions, we focused on R s data collected during the summer season (or equivalent in tropical forests), as it typically represents the peak season for R s and offers a greater availability of measurements. Results of diel R s dynamics for other seasons are provided in the Supporting Information, demonstrating similar findings especially in spring and autumn. We applied rigorous filtering procedures to focus on well‐characterized forest sites with sufficient daytime and nighttime soil respiration and temperature measurements, excluding data from manipulated experiments and potential outliers to ensure the robustness of data analysis. Following rigorous data preprocessing and quality control (detailed in Methods), our analysis included 36 sites across five forest types, as classified by the International Geosphere‐Biosphere Programme (IGBP; Figure 1a).
The diel patterns of soil respiration (R s) across global study sites. (a) Global map showing the geographic locations of forest sites. Two‐dimensional climate space superimposed onto Whittaker biomes. The number of sites for each forest type was shown. (b) The diel difference in soil respiration (∆R s = nighttime R s—daytime R s, μmol m−2 s−1) across study sites. Positive values indicate higher nighttime values than daytime values. Dark‐green and blue points indicate significant positive and negative ∆R s at each site (p < 0.05), while brown points indicate statistically nonsignificant diel difference (p ≥ 0.05). Error bars represent the standard error of the mean. Sites within each forest type were ordered sequentially based on an ascending gradient of site‐specific mean soil temperature. DBF, deciduous broadleaf forest; EBF, evergreen broadleaf forest; DNF, deciduous needleleaf forest; ENF, evergreen needleleaf forest; MF, mixed forest.
Materials and Methods
2
Investigating Diel R
s Differences Using the COSORE Database
2.1
In this study, we retrieved the sub‐hourly measurements of R s (μmol m^−2^ s^−1^), T s (°C), and soil water content (SWC, %) from the COSORE database to explore the diel patterns of R s and its temperature response across forest ecosystems. The COSORE database comprises continuous and long‐term chamber‐based measurements of soil‐atmosphere greenhouse gas fluxes from 89 sites across various ecosystems (Bond‐Lamberty et al. 2020). Our analysis focused on the summer season, defined as June to August for the Northern Hemisphere and December to February for the Southern Hemisphere. Results for other seasons were provided in Figure S1. To ensure the robustness and reliability of our findings, we implemented a series of filtering criteria: (1) focus on forest sites: we concentrated on forest sites due to the limited availability of data from other land cover types; (2) comprehensive data requirements: only sites with records of both daytime and nighttime T s and R s were included in the study. Daytime and nighttime periods for each study site were determined by calculating the sunrise and sunset times for each day based on the Jet Propulsion Laboratory Development Ephemeris (Mahooti 2025); (3) exclusion of treatment data: data from warming or drought treatments were excluded to prevent confounding effects on R s; (4) measurement frequency thresholds: we aggregated the sub‐hourly measurements of R s, T s, and SWC to an hourly time scale to minimize the heterogeneity arising from variations in the measurement frequency both within and across sites. Months with fewer than 10 days of measurements were then excluded to ensure that the selected sites have sufficient and representative measurements. Similarly, days with fewer than 3 h of measurements in both daytime and nighttime periods were also excluded to ensure a robust comparison of R s patterns between daytime and nighttime; (5) data quality control: non‐positive and outlier values of R s for each dataset, defined as values outside the range [25% quantile—1.5 × interquartile range, 75% quantile +1.5 × interquartile range], were removed, though this did not affect the qualitative findings of this study.
Given the varied soil depths for T s and SWC measurements across sites, we selected T s and SWC data at a 5 cm depth, or the nearest available depth if 5 cm data were unavailable, to ensure consistency. The 5 cm depth was selected since this layer usually accounts for the majority of R s relative to deeper soil profiles (Peng et al. 2009; Pries et al. 2017; Li et al. 2020). Our final dataset comprises 164,170 measurements of R s from 36 forest sites, representing five IGBP (International Geosphere‐Biosphere Program) land cover types: deciduous broadleaf forest (DBF), evergreen broadleaf forest (EBF), deciduous needleleaf forest (DNF), evergreen needleleaf forest (ENF), and mixed forest (MF).
For each site, we calculated the daily mean daytime and nighttime T s, SWC, and R s by averaging the corresponding hourly measurements during the daytime and nighttime periods and then used the Student's t‐test to examine the statistical significance of the diel differences in T s, SWC, and R s across sites. In addition, we used the hourly measurement data to fit the daytime and nighttime R s‐T s relationships using an exponential function, that is,
where R s0 and β are fitted constants. The temperature sensitivity of R s, denoted by Q 10 (Q10=e10β), represents the relative change in R s for a 10°C temperature increase. Because R s is regulated by multiple processes operating at different time steps, this Q 10 is intended as an integrated metric for long‐term average responses that include, but are not limited to temperature, given other drivers that co‐vary with temperature. To account for the effects of diel temperature variations on R s patterns, we further tested the statistical significance of the difference in temperature‐adjusted R s across sites by adjusting the raw daytime and nighttime R s values to a common temperature using daytime and nighttime Q 10 values, respectively, based on the following equation.
where Rsadj is the temperature‐adjusted soil respiration (μmol m^−2^ s^−1^) and Ts¯ is the site‐specific mean soil temperature (°C), which was calculated by averaging all soil temperature data during the summer period to fully reflect the long‐term climatic conditions of each site. Additionally, we conducted standardized major axis (SMA) regression analysis using the “lmodel2” function from the R package “lmodel2” (Legendre 2018) to compare daytime and nighttime R s across study sites.
Evaluating ESMs' Ability to Simulate Diel Dynamics of R
s
2.2
To evaluate the capacity of current ESMs in capturing diel patterns of R s, we ran two configurations of the ELM, the land surface component of the Earth system model E3SM (Burrows et al. 2020), to model global hourly dynamics of R s, R root, and R h during the 2005–2014 period, which is well represented in the COSORE database and allows for a robust long‐term validation of ESM simulations against observational data. ELM simulates the complex land‐atmosphere interactions including energy, water, C, and nitrogen cycles. Like most current ESMs, ELM adopts a CENTURY‐like formulation of soil biogeochemistry (Koven et al. 2013). We took advantage of the two representations of nutrient competition dynamics in ELM to account for model structural uncertainty. Of the two ELM configurations, the Equilibrium Chemistry Approximation (ECA) configuration employs a mechanistic framework to model the complex competition network among plant roots, soil microbes, and abiotic protection mechanisms, explicitly representing interactions between multiple consumers and substrates. The ECA model uniquely features dynamic plant resource allocation, variable plant stoichiometry constrained by empirical observations (Kattge et al. 2020), and nutrient uptake driven by root functional traits instead of photosynthetic demand (Riley et al. 2018). The other configuration represents nutrient competition using the relative demand (RD) approach, where plants and soil biogeochemical processes compete equally for available nutrients. For both configurations, plant biomass growth is modeled as being driven by vegetation net primary productivity (NPP). However, the ECA configuration does not allow nighttime plant growth, whereas the RD configuration allows nighttime plant growth through some allowance of C deficit that is subsequently replenished by photosynthesis during daytime. We ran both model configurations using the land module only mode, driven by reanalysis climate data from the Global Soil Wetness Project phase 3 (Danger et al. 2008), and surface dataset as used in Zhu et al. (2020, 2024). The models were spinup using the recommended strategies of 200‐year accelerated spinup, 600‐year regular spinup, and transient simulation from 1850 to 2014. Hourly data of R s, autotrophic root respiration, heterotrophic respiration, and 10‐cm soil temperature were output for analysis.
From the hourly model outputs, we extracted the modelled values of R s, R root, and R h from ECA and RD outputs for all 36 study sites. To ensure robustness, we calculated the site‐specific 10‐year average of daytime and nighttime means for R s, R root, and R h, respectively, during the 2005–2014 period. The daytime and nighttime periods for each pixel were determined by the time periods when GPP is equal to 0. We then applied SMA regression analysis to explore the diel difference in R s, R root, and R h, respectively.
Evaluating Biases in Predicting Nighttime R
s Using Daytime R s‐T s Relationships
2.3
To quantify the potential biases in estimating nighttime R s using daytime R s‐T s relationships, we first estimated the model parameters R s0 and β from Equation (1) for the daytime periods at each site, and then used these daytime parameters along with nighttime T s to yield nighttime R s estimates. We then calculated the biases in nighttime estimation for each study site using the following equation:
where Rspre and Rsobs are the predicted and observed R s, respectively. The Student's t‐test was used to detect the statistical significance of the difference between Rspre and Rsobs for each site. We roughly quantified, on a global scale, the approximate magnitude of error introduced by predicting nighttime R s using daytime R s‐T s relationships across different forest types in summer. This predictive error was determined by multiplying the difference between Rsobs and Rspre by the average area of each forest type, derived from the MODIS land cover product MCD12C1. Additionally, we used a subset of COSORE sites (n = 8) with measurements of both R s and R h to examine the relative contributions of R h and R root to the biases in nighttime R s estimation. The R h time series data were measured primarily using the soil trenching approach (Bond‐Lamberty et al. 2020) and the R root time series data were quantified as the difference between R s and R h. We then calculated the biases in predicting nighttime R root and R h using daytime R root‐T s relationships and R h‐T s relationships, respectively.
Examining the Correlations Between R
s and GPP
2.4
We investigated the relationships of daytime and nighttime R s with daily gross primary productivity (GPP) by leveraging the global (Pastorello et al. 2020) and AmeriFlux databases, which contains in situ eddy covariance measurements of CO_2_, water, and energy fluxes from different ecosystems across the globe. For this analysis, we selected forest sites (n = 11) with concurrent measurements of GPP from the FLUXNET and AmeriFlux networks and R s from the COSORE database. Daily GPP estimates (g C m^−2^ day^−1^) based on the daytime partitioning method (Lasslop et al. 2010), which used both daytime and nighttime data for model parameterizations, were chosen for all study sites. We examined the relationships of daytime and nighttime R s with daily GPP using the SMA regression analysis for each site to test whether nighttime R s exhibited more elevated or more positive relationships with GPP than daytime R s across sites. In addition, we analyzed the changes in the Pearson correlation coefficient between daily R s and GPP as a function of a temporal lag between R s and GPP, ranging from 0 to 45 days at each site. This time lag specifies the number of days prior to R s measurements that the GPP data were used for the correlation analysis.
Results
3
Unexpected and Widespread Elevated Nighttime R
s
3.1
We found an average diel difference of R s (∆R s = nighttime R s − daytime R s) of 0.25 ± 0.08 μmol CO_2_ m^−2^ s^−1^ (mean ± SEM; roughly a 5.17% ± 1.40% difference) across all 36 forest sites examined in the COSORE database. Notably, a considerably larger proportion of these sites exhibited a significantly positive ∆R s (n = 22, p < 0.05) than vice versa (n = 5, p < 0.05) (Figures 1b and 2), indicating a widespread (but not obligate) occurrence of higher nighttime R s relative to daytime R s. All forest types on average exhibited a positive ∆R s, though the magnitude of this difference varied among forest types. Mixed forests (MF) had the smallest difference (0.03 ± 0.06 μmol CO_2_ m^−2^ s^−1^), whereas deciduous broadleaf forests (DBF) had the largest (0.34 ± 0.13 μmol CO_2_ m^−2^ s^−1^), followed by evergreen broadleaf forests (EBF: 0.19 ± 0.25 μmol CO_2_ m^−2^ s^−1^) and evergreen needleleaf forests (ENF: 0.12 ± 0.07 μmol CO_2_ m^−2^ s^−1^). In addition, ∆R s was overall larger for sites with higher R s as evidenced by a bivariate regression analysis (slope = 1.14, 95% CI = 1.08 to 1.21, R ^2^ = 0.98, Figure 3a).
Density plots of daytime and nighttime R s (μmol m−2 s−1) across forest sites. Green and orange solid lines represent daytime and nighttime density curves, respectively. The green and brown dashed lines represent the site‐specific mean values of daytime and nighttime R s, respectively.
The comparison between daytime and nighttime R s (μmol m−2 s−1). (a) The comparison between measured daytime and nighttime R s across study sites. (b) The comparison between simulated daytime and nighttime R s during 2005–2014 across study sites from the two models (i.e., ECA and RD). Each point represents the site‐specific mean value of R s. The dashed and solid lines represent the 1:1 relationships and linear regression results, respectively. Shaded orange areas represent values with higher nighttime than daytime and light green areas represent the opposite pattern.
We then examined the potential drivers of the observed diel R s dynamics. A significant variation in ∆T s (nighttime T s − daytime T s) was observed across the 36 sites, ranging from −2.34 ± 0.07 to 2.52°C ± 0.07°C (cross‐site average: 0.07°C), with 19 and 13 sites exhibiting a significantly positive and negative ∆T s, respectively (all p < 0.05, Figure S2a). In contrast, there was little or no significant diel difference in soil water content (SWC, %) (Figure S2b), leading to similar daytime and nighttime R s‐SWC relationships (Figure S3). To assess whether the observed diel R s difference was solely due to differences in T s between day and night, we adjusted both daytime and nighttime R s to the site‐specific mean soil temperature (R s ^adj^) based on the site‐specific daytime and nighttime Q 10 value, respectively (see Equation (1) in Methods). We found consistently higher nighttime R s ^adj^ compared to daytime R s ^adj^ across sites (Figure S4), suggesting that diel R s dynamics were not primarily driven by the commonly considered ∆T s. In addition, both daytime and nighttime Q 10 values were not significantly correlated with T s and SWC (all p > 0.05, Figure S5).
Current ESM Underestimation of Nighttime R
s
3.2
To assess the accuracy of ESMs in capturing elevated nighttime respiration observed in our analysis, we simulated global hourly R s, R root, and R h for 2005–2014 using the land component of the Earth system model E3SM. We employed two model configurations, representing contrasting approaches to simulate nutrient dynamics: the equilibrium chemistry approximation (ECA) and the relative demand (RD) formulation (see Methods). Both configurations, representative of how R s is typically represented in existing Earth system models (ESMs), were simulated at a half‐hourly time step to capture the full diel cycle of C and water fluxes. These long‐term simulations enabled a comprehensive evaluation of ESM outputs against empirical R s data. Contrary to empirical observations, both ECA and RD simulations produced significantly lower nighttime R s compared to daytime R s (slope = 0.37 and 0.85, 95% CI = 0.34 to 0.40 and 0.81 to 0.90, R ^2^ = 0.94 and 0.98, both p < 0.01, respectively, Figure 3b). Across all sites, ECA‐ and RD‐estimated nighttime R s were on average 65.6% ± 1.2% and 21.2% ± 0.8% lower than daytime R s, respectively. This discrepancy primarily stemmed from the significantly underestimated nighttime R root simulated by both ECA (slope = 0.001, p > 0.05) and RD (slope = 0.71, 95% CI = 0.64 to 0.78, R ^2^ = 0.92, p < 0.01, Figure S6a), whereas R h exhibited a less pronounced day‐night difference across both models (Figure S6b).
Substantial Bias in Nighttime R
s Prediction Using Daytime R s‐T s Relationships
3.3
Given the notable differences in the parameters of R s‐T s relationships between day and night (Figure S7, Table S1), we investigated the extent of bias when using daytime R s‐T s relationships to estimate nighttime R s across study sites. Among 36 sites, we found that 31 sites exhibited significant underestimation of nighttime R s when daytime relationships were applied, with the underestimation ranging from 2.5% to 28.7% (Figures 4 and S8). These underestimations were mainly due to greater underestimation of nighttime R root than R h, a pattern consistently observed across most sites (Figure 5). Notably, in the three DBF sites, bias in R root prediction accounted for 61.4% to 98.9% of the bias in R s prediction (Figure 5). When extrapolated to the global scale using the average global area of each forest type, applying the daytime R s‐T s relationships to predict nighttime R s could result in an average summertime underestimation of nighttime R s by 0.51, 0.13, 0.06, and 0.07 Pg C on average for EBF, DBF, ENF, and MF, respectively.
The bias in estimating nighttime R s (%) using daytime R s‐T s relationships. The bias percentage was calculated as Rspre−Rsobs/Rsobs×100%, where Rspre is the predicted nighttime R s using daytime R s‐T s relationships and Rsobs is the observed nighttime R s. The bias is represented by colored bars corresponding to forest type as follows: Light blue (DBF), dark blue (DNF), light green (EBF), dark green (ENF), and pink (MF). The inset graph shows the additional nighttime C emission during the summer with respect to the predicted nighttime R s based on daytime R s‐T s relationships.
The bias in estimating nighttime R s and root respiration (R root) based on their relationships with temperature during the day, respectively. The red and blue bars represent biases in R root and R s estimation, respectively. The grey points represent the percentage contribution of roots to R s bias for different sites.
Discussion
4
These results collectively provide the first global‐scale evidence for the widespread higher nighttime than daytime R s in forest ecosystems during the summer season (Figure 1b). Notably, our synthesized cross‐site analysis aligns with recent work showing a higher nighttime R s in a temperate forest (Han et al. 2023) but contrasts with most prior single‐site studies that reported higher daytime R s due to warmer temperatures during the day across different ecosystems (Liu et al. 2006; Ford et al. 2012; Hu et al. 2016; Chu et al. 2023; Fekadu et al. 2022). This indicates the potentially important role of previously overlooked factors other than temperature in regulating diel R s dynamics (Makita et al. 2018). Here, we propose two potential mechanisms underlying the observed widespread higher R s at night than during the day. The first is related to the hourly‐scale lag between the assimilation and movement of new photosynthetic C and soil respiration (Baldocchi et al. 2006; Kuzyakov and Gavrichkova 2010; Han et al. 2014). In fact, recent photosynthates usually serve as a primary C source for R s in forest ecosystems (e.g., Tang et al. 2005; Vargas and Allen 2008; Heinemeyer et al. 2012). Previous studies have reported that the time lag between photosynthesis and R s is approximately 6–8 h in a mixed forest (Ruehr et al. 2010) and 7–12 h in an oak‐grass savanna (Tang et al. 2005). Consequently, greater rates of C fixation via daytime photosynthesis generally leads to an increased supply of recent photosynthates available to the roots. Due to this hourly temporal lag, the subsequent enhancement in the metabolic activities of roots and also soil microorganisms (i.e., rhizosphere priming effect; Kuzyakov and Cheng 2001) was observed to be significantly greater during the subsequent nighttime period than during the daytime (Vargas and Allen 2008). In addition, the time required for microbial decomposition of soil organic carbon can further contribute to the lagged CO_2_ efflux (Mencuccini and Hölttä 2010; Liu et al. 2024). This mechanism is at least partially supported by the evidence that (1) nighttime R s showed more elevated and/or more positive relationships with GPP than daytime R s across various forest sites (Figure S9); and (2) the correlation coefficient between daily R s and GPP changed across different time lags, with the peak coefficient value varying across sites (Figure S10). These results are consistent with previous work showing positive dependence of R s on photosynthesis (Xia et al. 2009). Furthermore, the magnitude of the diel difference in R s in spring was similar to that in summer, both of which were greater than those observed in autumn and winter (Figure S1). This trend is likely attributed to the relatively higher photosynthetic activity in spring and summer, which consequently leads to increased allocation of recent photosynthates to belowground processes (Han et al. 2023). The second hypothesis concerns root xylem CO_2_ flux, as evidenced by empirical observations suggesting that a significant portion of CO_2_ respired by tree roots during the day is transported to the shoot via the transpiration stream (Aubrey and Teskey 2009; Bloemen et al. 2013, 2016). This upward transport can result in a lower observed daytime R s and therefore contribute to the appearance of higher R s at night.
Nevertheless, we acknowledge that the inherent disturbances associated with the long‐term deployment of automated chamber systems, such as weeding and microclimatic changes, may introduce systematic biases influencing diel R s dynamics. In addition, empirical evidence suggests a potential overestimation of soil R s, especially at night, due to low atmospheric turbulence (Schneider et al. 2009; Brændholt et al. 2017), which is largely associated with the disruption of stratified air layers above the soil surface caused by the chamber movement during measurements (Görres et al. 2016). In fact, some datasets in the COSORE database have at least partially addressed this issue by utilizing fans or specialized designs to enhance air mixing or by discarding initial measurements to avoid closure effects. Crucially, the observed pattern of generally higher nighttime persists despite the inclusion of these mitigating approaches, underscoring the robustness of our results. Nevertheless, the overall impact of atmospheric turbulence on R s estimation remains inadequately understood and addressed in current studies. Our study highlights the need of future experimental efforts that minimize these methodological artifacts and also integrate direct measurements of photosynthate allocation and root CO_2_ transport processes alongside concurrent monitoring of plant community structure and functions to comprehensively investigate the relative contributions of these physiological processes to diel R s dynamics.
We observed higher nighttime than daytime T s across a large subset of our study sites (Figure S2a), which may be attributed to (1) soil thermal inertia that allows soil to retain heat absorbed during the day (Cheruy et al. 2017) and (2) reduced radiative cooling, whereby forest canopies absorb a portion of nocturnal longwave radiation emitted by the soil surface and reflect it back towards the ground (D'Odorico et al. 2013). However, accounting for diel temperature variation did not alter diel R s patterns across sites (Figure S4). According to Equation (1), diel R s dynamics can also arise from the combined influence of diel differences in the reference soil respiration (R s0) and temperature sensitivity (Q 10). For instance, higher nighttime R s can be attributed to a higher R s0 and/or a greater Q 10 at night than during the day. Indeed, we observed significant diel differences in R s‐T s relationships across sites, as reflected by the diel variations in the numerical values of Q 10 and R s0 (Table S1). While the negative cross‐site relationship between long‐term Q 10 and temperature has been well recognized (Xu et al. 2015; Li et al. 2020), our cross‐site analysis revealed that both long‐term daytime and nighttime Q 10 values were not significantly correlated with T s or SWC (all p > 0.05, Figure S5). This implies that long‐term Q 10 is not solely driven by climatic factors, but may instead reflect a complex interaction among biotic and abiotic drivers such as vegetation productivity and substrate quality (Davidson and Janssens 2006; Haaf et al. 2021). In addition, despite similar R s‐SWC relationships between day and night, SWC appears to exhibit a more pronounced influence on diel R s dynamics under extreme wet and dry conditions (Figure S3), which might be associated with the effect of extreme SWC conditions on vegetation production and photosynthate allocation (Phillips et al. 2011).
By representing the allocation of new photosynthates to plant organs as a function of NPP (Lawrence et al. 2019), the ECA configuration does not allow root growth at night. As a result, nighttime root respiration only reflects maintenance respiration, and therefore nighttime R s is dominated by soil microbial processes. Meanwhile, the RD configuration allows nighttime root growth based on a negative C storage pool that is only replenished during daytime, and this repletion acts to lower daytime growth respiration. Since empirical work indicates that plants continue root growth and nutrient uptake at night (Schimel et al. 1989; Riley et al. 2018; Tang and Riley 2021), these two representative model configurations and other similar models likely yield incorrect estimates of nighttime R root as well as the diel cycle of R root and its temperature sensitivity, as evidenced by the inconsistency in the diel R root patterns between model predictions (Figure S6a) and empirical observations (Figure S11). The uncertainty surrounding R root is further compounded by the challenge of partitioning R s measurements into R root and R h components (Tang et al. 2019), as well as varying estimates of the contributions of R root to R s, ranging from 10% to 90% depending on ecosystem types and climate conditions (Hanson et al. 2000). These factors result in yet poorly understood global spatial and temporal patterns of R root (Ballantyne et al. 2017) and introduce large uncertainty in ESM simulations of the soil C budget (Tang et al. 2019).
In contrast to the observed diel difference in soil Q 10 across sites (Table S1), many ESMs assume the same Q 10 for both above‐ and below‐ground plant respiration and do not account for diel Q 10 differences (Conant et al. 2011; Oleson et al. 2013; García‐Palacios et al. 2021), which may significantly increase uncertainty in simulating diel R s dynamics. In addition, we also discovered a significant diel difference in the reference soil respiration (R s0) (see Equation (1); Figure S7; Table S1), which represents R s at a reference temperature and therefore captures the responses of R s to key factors other than temperature such as substrate availability and microbial biomass (Buchmann 2000). This finding contradicts the common assumption of a constant R s0 between day and night (Oleson et al. 2013) and highlights the potential uncertainty introduced by this assumption in current ESMs. This diel difference can also contribute to the observed elevated nighttime R s and may be partially explained by the increased substrate availability at night due to the transport of recent photosynthetic C from leaves to roots (Baldocchi et al. 2006; Kuzyakov and Gavrichkova 2010; Han et al. 2014). However, more in‐depth analysis and mechanistic exploration is needed by future studies.
Our findings suggest a significant systematic underestimation of nighttime R s when extrapolated using daytime R s‐T s relationships (Figure 4). In fact, empirical studies usually extrapolate daytime R s observations (e.g., from the morning period) to infer daily‐scale R s when continuous R s measurements from automated chamber systems are unavailable (Cueva et al. 2017). However, this approach can introduce significant uncertainty when R s and its temperature response exhibit different diel patterns (Savage and Davidson 2003; Han et al. 2023). The availability of temporally‐continuous in situ R s measurements across diverse ecosystems remains limited (Bond‐Lamberty et al. 2020), especially compared to other ecosystem‐scale C flux databases such as FLUXNET (Pastorello et al. 2020). The observed diel differences in R s thus highlight the critical need for expanding R s measurement networks to better understand the day‐night difference in R s and its abiotic/biotic drivers across diverse ecosystems. Such expansion is vital not only for accurately quantifying the relative contribution of R s to the overall soil C budget across various timescales, but also supporting evidence‐based soil C management and climate mitigation strategies.
Our study reveals widespread elevated nighttime R s across global forest ecosystems, challenging the conventional view that R s responds uniformly to temperature changes throughout day and night. Although previous studies have emphasized temperature and SWC as key drivers of R s (Rytter 2013; Han et al. 2023; Liang et al. 2024), suggesting their potential to explain day‐night differences in R s, our analysis highlights the important role of diel difference in the temperature response of R s in influencing the diel dynamics of R s in forests. Together with evidence of asymmetric climate warming between day and night (Doan et al. 2022; Liu et al. 2024), our findings suggest that daytime and nighttime R s in forests can experience distinct changes, impacting the future trajectory of soil C emissions and many other ecological processes related to the soil C turnover (Bond‐Lamberty et al. 2024). We acknowledge that other ecosystems, such as grasslands, typically exhibit greater diel soil temperature fluctuations and faster C turnover than forests, which may result in distinct diel R s patterns that warrant further investigation. Enhancing the mechanistic understanding and model representation of diel dynamics of R s across ecosystems and the potentially distinct diel patterns of its components (i.e., R root and R h) is crucial for more accurate predictions of the temporal dynamics of soil C emissions under climate change.
Author Contributions
H.H.: conceptualization, investigation, methodology, validation, visualization, writing – original draft, writing – review and editing. J.T.: investigation, methodology, validation, visualization, writing – review and editing. B.B.‐L.: conceptualization, methodology, validation, visualization, writing – review and editing. P.B.R.: conceptualization, methodology, validation, visualization, writing – review and editing. T.W.C.: methodology, validation, visualization, writing – review and editing. J.J.: methodology, investigation, writing – review and editing. K.Z.: formal analysis, investigation, writing – review and editing. L.L.: methodology, supervision, writing – review and editing. J.W.: conceptualization, project administration, resources, supervision, writing – review and editing.
Funding
This work was supported by the National Natural Science Foundation of China, 31922090. HKU Seed Funding for Strategic Interdisciplinary Research Scheme. Hong Kong Research Grant Council Collaborative Research Fund, C5062‐21GF. Young Talent Program from Guangdong Province, 77010‐42150005. The Start‐up Grant from Sun Yat‐sen University, 77010‐12255006. Fundamental Research Funds for the Central Universities from Sun Yat‐sen University, 77010‐13130003. Innovation and Technology Fund (funding support to State Key Laboratory of Agrobiotechnology).
Conflicts of Interest
The authors declare no conflicts of interest.
Supporting information
Data S1: gcb70798‐sup‐0001‐Supinfo.pdf.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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