Measuring photosynthesis is critical for quantifying and modeling leaf to regional scale productivity of managed and natural ecosystems. This review explores existing and novel advances in photosynthesis measurements that are certain to provide innovative directions in plant science research. First, we address gas exchange approaches from leaf to ecosystem scales. Leaf level gas exchange is a mature method but recent improvements to the user interface and environmental controls of commercial systems have resulted in faster and higher quality data collection. Canopy chamber and micrometeorological methods have also become more standardized tools and have an advanced understanding of ecosystem functioning under a changing environment and through long time series data coupled with community data sharing. Second, we review proximal and remote sensing approaches to measure photosynthesis, including hyperspectral reflectance- and fluorescence-based techniques. These techniques have long been used with aircraft and orbiting satellites, but lower-cost sensors and improved statistical analyses are allowing these techniques to become applicable at smaller scales to quantify changes in the underlying biochemistry of photosynthesis. Within the past decade measurements of chlorophyll fluorescence from earth-orbiting satellites have measured Solar Induced Fluorescence (SIF) enabling estimates of global ecosystem productivity. Finally, we highlight that stronger interactions of scientists across disciplines will benefit our capacity to accurately estimate productivity at regional and global scales. Applying the multiple techniques outlined in this review at scales from the leaf to the globe are likely to advance understanding of plant functioning from the organelle to the ecosystem.

The terrestrial biosphere consists of an assemblage of diverse ecosystems. Its complexity is illustrated with a diversity of plants with distinct canopy structures subject to changing environmental conditions. Life on earth relies on the energy captured by these ecosystems through photosynthesis, which accounts for the single largest flux associated with the global carbon cycle [1]. Photosynthesis varies among plant functional types (e.g. C3 vs. C4) and over a wide range of spatial and temporal scales associated with changes in light, temperature, water and nutrients [2,3]. Global climate change driven by anthropogenic activities is having profound impacts on terrestrial ecosystems, with global temperatures rising faster than worst-case predictions [4]. Increasing agricultural demands associated with a growing population requires a doubling of crop yields by 2050 to keep up with demands [5], yet current rates of improvement fall short of this goal [6,7], which is likely to suffer with continued global warming [8–11].

Photosynthesis is a highly complex and relatively inefficient process, yet it is a critical component of the biosphere. Understanding photosynthetic responses over a range of spatial and temporal scales is needed to understand current and to predict future global carbon cycling. This understanding will also lead to improving photosynthesis, which can lead to higher productivity to meet growing agricultural demands [12,13]. These goals can only be achieved through the ability to measure photosynthesis over time and space, yet photosynthesis is difficult to measure directly. This is due to the multiple processes that are represented by the exchange of CO2 between plants/ecosystems and the surrounding air. For example, at the leaf scale CO2 is removed from the air by photosynthesis but this is partially countered by photorespiration and respiration, both of which release CO2 [14,15]. The combined fluxes of these three processes represents net carbon assimilation (A) and partitioning this net flux into the component fluxes is challenging [16]. Scaling beyond the leaf only presents additional challenges. At canopy or ecosystem scales, respiration from non-photosynthetic tissues and heterotrophic organisms also release CO2, which combined with A provide measures of Net Ecosystem Exchange (NEE; Table 1). In this review, we outline the current and emerging approaches to measure photosynthesis at multiple scales and address the challenges and opportunities at each scale (Figure 1). We begin with a focus on the well-established and widely used gas exchange techniques and follow with more recent approaches made available through recent technological advances.

Depiction of techniques and example data for gas exchange (A–C) and proximal/remote sensing (D–F) techniques used to measure photosynthesis.

Figure 1.
Depiction of techniques and example data for gas exchange (A–C) and proximal/remote sensing (D–F) techniques used to measure photosynthesis.

(A) Leaf-level gas exchange with one measured representative photosynthetic CO2 response curve. (B) Canopy photosynthesis chamber situated over a soybean field with representative diurnal Net Ecosystem Productivity (NEP) data (Image Credit: Anthony DiGrado). (C) Ecosystem-scale eddy covariance system situated over sorghum with representative Net Ecosystem Exchange (NEE; negative values signify downward flux from atmosphere toward land surface) partitioned into Gross Primary Productivity (GPP) and Ecosystem Respiration (ER). (D) leaf hyperspectral point sensor being used on the model crop tobacco and representative spectral reflectance measurements. (E) A hyperspectral imaging sensor measuring plots of the model crop tobacco and an example hypercube showing the visible surface and spectral information for each pixel with depth of image. (F) aircraft and satellite depicted over the earth surface and a map of GPP (public domain image courtesy of GeoEye/NASA SeaWIFS project). Other than where indicated, all images were taken by authors.

Figure 1.
Depiction of techniques and example data for gas exchange (A–C) and proximal/remote sensing (D–F) techniques used to measure photosynthesis.

(A) Leaf-level gas exchange with one measured representative photosynthetic CO2 response curve. (B) Canopy photosynthesis chamber situated over a soybean field with representative diurnal Net Ecosystem Productivity (NEP) data (Image Credit: Anthony DiGrado). (C) Ecosystem-scale eddy covariance system situated over sorghum with representative Net Ecosystem Exchange (NEE; negative values signify downward flux from atmosphere toward land surface) partitioned into Gross Primary Productivity (GPP) and Ecosystem Respiration (ER). (D) leaf hyperspectral point sensor being used on the model crop tobacco and representative spectral reflectance measurements. (E) A hyperspectral imaging sensor measuring plots of the model crop tobacco and an example hypercube showing the visible surface and spectral information for each pixel with depth of image. (F) aircraft and satellite depicted over the earth surface and a map of GPP (public domain image courtesy of GeoEye/NASA SeaWIFS project). Other than where indicated, all images were taken by authors.

Close modal
Table 1
Terminology associated with photosynthesis at both the leaf and ecosystem levels
TermDefinition
Gross photosynthesis The total CO2 fixed through carboxylation within the leaf chloroplasts. 
Apparent photosynthesis CO2 assimilated through carboxylation minus photorespiration, a process that involves the oxygenation of Rubisco. The term apparent photosynthesis excludes respiration. 
Net Carbon Assimilation (AGross photosynthesis, minus photorespiration and respiration 
Gross Primary Productivity (GPP) Ecosystem and canopy scale apparent photosynthesis. 
Net Primary Productivity (NPP) Ecosystem and canopy scale apparent photosynthesis minus plant respiration, which includes the CO2 emitted by both above- and root components (autotrophic respiration, Ra). 
NPP is defined with the following equation: NPP = GPP–Ra 
Net Ecosystem CO2 Exchange (NEE) Ecosystem net exchange of CO2 between an ecosystem and the atmosphere over a given time wich can be from hours to years. 
NEE can be measured using the eddy covariance (EC) as well as biometric methods. 
The eddy covariance method measures continuous NEE fluxes over time and it is the net balance between GPP and ecosystem respiration (Reco). Reco is the sum of Ra and soil microbial respiration in aerobic conditions (heterotrophic respiration, Rh). 
Biometric methods estimate NEE according to the following equation: NEE = NPP–Rh [116
TermDefinition
Gross photosynthesis The total CO2 fixed through carboxylation within the leaf chloroplasts. 
Apparent photosynthesis CO2 assimilated through carboxylation minus photorespiration, a process that involves the oxygenation of Rubisco. The term apparent photosynthesis excludes respiration. 
Net Carbon Assimilation (AGross photosynthesis, minus photorespiration and respiration 
Gross Primary Productivity (GPP) Ecosystem and canopy scale apparent photosynthesis. 
Net Primary Productivity (NPP) Ecosystem and canopy scale apparent photosynthesis minus plant respiration, which includes the CO2 emitted by both above- and root components (autotrophic respiration, Ra). 
NPP is defined with the following equation: NPP = GPP–Ra 
Net Ecosystem CO2 Exchange (NEE) Ecosystem net exchange of CO2 between an ecosystem and the atmosphere over a given time wich can be from hours to years. 
NEE can be measured using the eddy covariance (EC) as well as biometric methods. 
The eddy covariance method measures continuous NEE fluxes over time and it is the net balance between GPP and ecosystem respiration (Reco). Reco is the sum of Ra and soil microbial respiration in aerobic conditions (heterotrophic respiration, Rh). 
Biometric methods estimate NEE according to the following equation: NEE = NPP–Rh [116

In general, photosynthesis is defined as the process why which plants capture light energy and atmospheric CO2 to synthesize complex carbohydrates. Photosynthesis supports the production of food, fiber, wood, grain fed to livestock, and fuel for humanity and regulates the concentration of CO2 in the atmosphere. Quantifying global terrestrial photosynthesis is essential to understanding the global CO2 cycle in a changing environment and the climate system.

The fundamentals of gas exchange at any scale are relatively similar and require the ability to measure gas concentrations in air surrounding and the flow rate in which the air interacts with photosynthetic tissue. In addition to these measurements, numerous assumptions, corrections, and parameterizations are required to fully exploit the power of this technique [16,17]. Gas exchange methods have been applied at scales ranging from the organelle (e.g. [18,19]) to the whole ecosystem/region [20] to provide a basic understanding of how leaves, plants, and ecosystems function and respond to their environment (Figure 1). Historically, gas exchange measurements were limited to enclosed sampling chambers, ranging from sections of leaves to whole plant canopies, where the rate of CO2 exchange was measured over time. With the advent of micrometeorological techniques, gas exchange measurements at large scales (e.g. whole ecosystems) were developed that removed the need for enclosures (Table 2). Despite errors, uncertainties and challenges associated with gas exchange, the various techniques are the current ‘gold standard’ by which emerging techniques are compared. This section provides an overview of gas exchange measurements at the leaf to ecosystem scales as a baseline in the understanding of emerging techniques.

Table 2
Advantages and disadvantages of the canopy and eddy covariance methods to measure CO2 fluxes and estimate GPP at the ecosystem scale
Eddy covariance methodAutomated chamber methodsManual chamber methods
Ecosystem Short and tall vegetation Short and tall vegetation Short and tall vegetation 
Temporal sampling frequency Continuous real-time measurements Continuous measurements Measurements often made at weekly to monthly intervals for the growing season or an entire year, and over a specific period of the day believed to be representative of the daily CO2 flux. 
CO2 data as well as other data crucial to compute fluxes are obtained at high frequency (at or above 10 Hz) 
Spatial integration Integrates large spatial areas, called the flux footprint, between hundred meters to several kilometers Several meters per chamber Hundred meters as they are portable 
Scale up necessary Scale up necessary 
Accuracy Most accurate when the atmospheric conditions (wind, temperature, humidity, CO2) are favorable, vegetation is homogeneous and sensors are installed on flat terrain for an extended distance upwind. Soil and vegetation disturbance possible Soil and vegetation disturbance possible 
Significant alteration of canopy microclimate from enclosure Significant alteration of canopy microclimate from enclosure 
Gap filling to obtain annual CO2 fluxes Gap filling necessary due to the malfunctioning of sensors, power failures, harsh environmental conditions, sensor calibration, lack of turbulence, when wind is coming from an undesirable direction. Gap filling necessary due to the malfunctioning sensors, power failures, harsh environmental conditions, sensor calibration, lack of turbulence, when wind is coming from an undesirable direction. Gap filling necessary as measurements are not continuous 
Logistical effort Considerable, especially in remote sites and in hostile environments. Considerable, especially if appropriate spatial replication is desirable High personnel effort especially if several instruments are deployed at once to minimize confounding effects resulting from hourly variability 
Cost High due to the cost of fast response instruments High due to the number of instruments needed for appropriate spatial replication Lower costs but require more person-hours to collect data 
Eddy covariance methodAutomated chamber methodsManual chamber methods
Ecosystem Short and tall vegetation Short and tall vegetation Short and tall vegetation 
Temporal sampling frequency Continuous real-time measurements Continuous measurements Measurements often made at weekly to monthly intervals for the growing season or an entire year, and over a specific period of the day believed to be representative of the daily CO2 flux. 
CO2 data as well as other data crucial to compute fluxes are obtained at high frequency (at or above 10 Hz) 
Spatial integration Integrates large spatial areas, called the flux footprint, between hundred meters to several kilometers Several meters per chamber Hundred meters as they are portable 
Scale up necessary Scale up necessary 
Accuracy Most accurate when the atmospheric conditions (wind, temperature, humidity, CO2) are favorable, vegetation is homogeneous and sensors are installed on flat terrain for an extended distance upwind. Soil and vegetation disturbance possible Soil and vegetation disturbance possible 
Significant alteration of canopy microclimate from enclosure Significant alteration of canopy microclimate from enclosure 
Gap filling to obtain annual CO2 fluxes Gap filling necessary due to the malfunctioning of sensors, power failures, harsh environmental conditions, sensor calibration, lack of turbulence, when wind is coming from an undesirable direction. Gap filling necessary due to the malfunctioning sensors, power failures, harsh environmental conditions, sensor calibration, lack of turbulence, when wind is coming from an undesirable direction. Gap filling necessary as measurements are not continuous 
Logistical effort Considerable, especially in remote sites and in hostile environments. Considerable, especially if appropriate spatial replication is desirable High personnel effort especially if several instruments are deployed at once to minimize confounding effects resulting from hourly variability 
Cost High due to the cost of fast response instruments High due to the number of instruments needed for appropriate spatial replication Lower costs but require more person-hours to collect data 

The global eddy covariance network, called FLUXNET (https://fluxnet.org/about/), includes measurement sites linked across regional networks in North, Central and South America, Europe, Asia, Africa, and Australia.

Leaf scale gas exchange

Knowledge of leaf photosynthetic physiology stems from the development and application of leaf-level gas exchange systems [16]. Gas exchange technology has matured to the point where commercial gas exchange systems are widely available from many vendors. In addition to providing the key variables necessary to assess leaf scale carbon assimilation, these systems now provide the opportunity to precisely control the environmental conditions surrounding the photosynthetic tissue and to measure more than just carbon assimilation, including but not limited to transpiration, intercellular CO2 concentrations, and stomatal conductance. Gas exchange techniques have been used for decades and most recent advancements have focused on improvements in accuracy, precision, usability, environmental control, and reduction in time to stable measurements. Despite the ease with which leaf level gas exchange can be measured, the importance of understanding gas exchange theory to ensure proper measurement and analysis cannot be overstated.

Gas exchange systems are the most commonly utilized technique for leaf scale photosynthetic measurements. While systems provide measures of A, various techniques can be applied to separate fluxes of photosynthesis, photorespiration, and respiration. However, many challenges exist with gas exchange that limit the wide application of the technique. These include cost, usability, data processing requirements, and time needed for ensuring quality measurements. Off-the-shelf gas exchange systems cost tens of thousands of dollars and require frequent maintenance that challenges their widespread use. Most gas exchange systems limit the area of measurement to, at most, several cm2, which presents issues related to scaling photosynthesis beyond a small section of one leaf. Typical measurements of in situ gas exchange require a minimum of 2–3 min to allow for both the system and the leaf to stabilize. Using these systems to measure beyond a simple survey of gas exchange, for example to measure light response or CO2 response curves of A, requires substantially more time for each leaf. Recent techniques that exploit improved instrument precision can reduce the time for some measurements but generally at the expense of accuracy, and often require more advanced post-processing [21].

Canopy and ecosystem scale gas exchange

Scaling gas exchange measurements to the canopy or whole ecosystem presents significantly more challenges than at the leaf level, yet there are also more options (Table 2). Canopy chambers work in much the same way as leaf chambers, although at a larger scale. The general principle follows that of leaf-level measurements, although chambers are required to be much larger to encompass multiple plants and the potential is greater for errors associated with leaks or pressure fluctuations [17]. Canopy chambers have been extensively used to measure CO2 fluxes for a wide range of vegetation types and their strengths lie in their ability to address small-scale spatial variability (Table 2). Furthermore, canopy chambers have been used both as a measurement and treatment system in global change studies to impose treatments as open-top chambers and acting as sample chambers when enclosed (e.g. [22]). Canopy chambers, however, can be limited in sampling frequency and spatial integration (Table 2) while also having a profound impact on the canopy microclimate.

Micrometeorological approaches to gas exchange lack the need for chambers but require large spatial areas (>4 Ha) and a sensor suite that can measure the upward/downward movement of air coupled with the gas concentrations in the air [20]. The dominant micrometeorological technique, eddy covariance (EC), provides near-continuous measurements of NEE integrated over large spatial areas, called the flux footprint, with minimal disturbance (Table 2) [20]. Air flow over a canopy consists of numerous rotating eddies. Measuring the speed and CO2 concentrations of the eddies moving air upward and downward, provides the basic data needed to calculate fluxes of the footprint, which varies with wind speed and direction [23]. EC requires several important considerations to ensure the NEE data are robust and reliable [24], including ensuring sufficient atmospheric turbulence [23], applying corrections to exclude data fluxes extending beyond the area of measurements [25,26], and ensuring all measured fluxes follow the laws of thermodynamics [27,28] (Table 3). Because of inevitable gaps in data collection associated with field instrumentation, gap filling strategies are used to complete the time-series of flux data (Table 4). In addition to NEE, EC can apply to any measurable component of the atmosphere provided high temporal resolution sensors (≥10 Hz) exist (e.g. water vapor, methane, etc.). A global EC flux network, called FLUXNET, provides data from over 900 sites globally, allowing for a link between ecosystem and global NEE. This network provides unprecedented insights into environmental and biological drivers of ecosystem NEE [3,20,29–33]. Among other purposes, the long-term measurements of NEE from this network have improved understanding of ecosystem responses to climate and land-use change [34], and the data are essential to validate remote sensing and modeling products that scale to regions and the globe [35,36].

Table 3
Challenges for obtaining robust estimates of net ecosystem exchange (NEE), and thus gross primary productivity (GPP), from eddy covariance (EC) flux towers used for assessing ecosystem-scale photosynthesis, and description of how scientists working in the field of micrometeorology address these challenges to reduce uncertainty in NEE measurements and GPP estimates [24]
The obstacleThe causeThe remedy
Missing raw data Power failure, instrument malfunction, communication issues Gap fill meteorological variables and use these as divers to build a complete NEE timeseries [41,117
Atmospheric turbulence Periods of low atmospheric turbulence reduce the dominance of vertical turbulent transfer, thus violating the assumptions of eddy covariance theory. Calculate a turbulence threshold (u*) and apply it to flux data to exclude data below the u* limit
-Moving Point Threshold (MPT)
-Change Point Detection (CPD) [23,118
Footprint filters The measurement area of the flux instruments changes with turbulence. As atmospheric conditions become stable, the area the flux instruments sample from becomes larger. This can extend beyond the ecosystem of interest and bias flux measurements Apply a footprint exclusion filter [25,26
Canopy storage If turbulent mixing is reduced, fluxes can build up within the canopy of interest and result in underestimation of fluxes Install a profile system to quantify at multiple depths through the canopy [119
Gap filling uncertainty Uncertainty in the fluxes due to random errors occurring during measurement and modeling errors during gap filling Calculate random and model error to provide an estimate of flux uncertainty [120,121
Partitioning methods Uncertainty arising due to the flux partitioning model used to estimate GPP Partition with multiple methods and provide model fit statistics with GPP estimate [117
Energy balance closure Based on surface energy balance theory. Net radiation (Rn) minus ground heat flux (G) should be equal to the sum of sensible (H) and latent (LE) heat flux. When this is not the case, there in greater uncertainty in the fluxes. Calculate the linear regression to obtain the difference between available energy (Rn-G) and energy used in the fluxes (H + LE). The energy used in fluxes is often corrected using the slope of this linear relationship. [27,28
The obstacleThe causeThe remedy
Missing raw data Power failure, instrument malfunction, communication issues Gap fill meteorological variables and use these as divers to build a complete NEE timeseries [41,117
Atmospheric turbulence Periods of low atmospheric turbulence reduce the dominance of vertical turbulent transfer, thus violating the assumptions of eddy covariance theory. Calculate a turbulence threshold (u*) and apply it to flux data to exclude data below the u* limit
-Moving Point Threshold (MPT)
-Change Point Detection (CPD) [23,118
Footprint filters The measurement area of the flux instruments changes with turbulence. As atmospheric conditions become stable, the area the flux instruments sample from becomes larger. This can extend beyond the ecosystem of interest and bias flux measurements Apply a footprint exclusion filter [25,26
Canopy storage If turbulent mixing is reduced, fluxes can build up within the canopy of interest and result in underestimation of fluxes Install a profile system to quantify at multiple depths through the canopy [119
Gap filling uncertainty Uncertainty in the fluxes due to random errors occurring during measurement and modeling errors during gap filling Calculate random and model error to provide an estimate of flux uncertainty [120,121
Partitioning methods Uncertainty arising due to the flux partitioning model used to estimate GPP Partition with multiple methods and provide model fit statistics with GPP estimate [117
Energy balance closure Based on surface energy balance theory. Net radiation (Rn) minus ground heat flux (G) should be equal to the sum of sensible (H) and latent (LE) heat flux. When this is not the case, there in greater uncertainty in the fluxes. Calculate the linear regression to obtain the difference between available energy (Rn-G) and energy used in the fluxes (H + LE). The energy used in fluxes is often corrected using the slope of this linear relationship. [27,28

Some of these challenges include ensuring sufficient atmospheric turbulent conditions are met [23], applying footprint corrections to exclude data when a significant portion of fluxes occur outside the ecosystem region of interest [25,26], and quantifying energy balance closure at the site [27,28]. Improving the robustness of NEE estimates from flux towers is an area of active research in the flux community, and one which will lead to greater understanding of ecosystem photosynthesis across a diversity of biomes.

Table 4
Description of common methods to fill missing half-hour values in CO2 records and performance to obtain accurate annual CO2 sums (i.e. sum of half-hour CO2 fluxes over a year)
Gap filling methodDescriptionReliability of annual sum of the net CO2 exchange
Mean Diurnal Variation (MDV) [122,123Half-hour CO2 gaps are replaced by the mean for that half-hour time period based on adjacent days. Good 
Look-up Tables (LUT) [122,123Half-hour CO2 gaps are filled using tables created for each site based on the environmental variables associated with the missing data. These meteorological variables are gross radiation, air temperature and vapor pressure deficit, which are known to regulate CO2 fluxes. Gaps are filled with available CO2 data when this set of environmental variables are similar for the missing half-hour CO2 flux and the available CO2 data Good 
Marginal Distribution Sampling (MDS) [122,123Half-hour CO2 gaps are filled by a half-hour CO2 values with similar meteorological conditions in the temporal vicinity of the gap to be filled. This method is a moving LUT technique that exploits the temporal auto-correlation structure of CO2 fluxes. Good 
Combination of MDS and MDV [124When meteorological variables regulating CO2 fluxes are available, the half-hour CO2 gap is filled using the MDS method with a moveable time window. When meteorological variables are not available, the missing value is filled using the MDV method with a short window size (i.e. the same day) and the window size can increase until the value can be filled. Good 
Non-linear regressions [122,123Half-hour CO2 gaps are filled using the relationships between available CO2 fluxes and associated controlling environmental factors during the period of missing fluxes. Good performance in general, although outliers can contribute to a high bias in predicted fluxes 
Artificial Neural networks [123Half-hour CO2 gaps are filled using non-linear relationships between meteorological variables and available CO2 fluxes. The network is trained by presenting it with sets of regulating meteorological variables and available CO2 data to predict missing data. Good performance particularly when data can be smoothed over trained networks 
Gap filling methodDescriptionReliability of annual sum of the net CO2 exchange
Mean Diurnal Variation (MDV) [122,123Half-hour CO2 gaps are replaced by the mean for that half-hour time period based on adjacent days. Good 
Look-up Tables (LUT) [122,123Half-hour CO2 gaps are filled using tables created for each site based on the environmental variables associated with the missing data. These meteorological variables are gross radiation, air temperature and vapor pressure deficit, which are known to regulate CO2 fluxes. Gaps are filled with available CO2 data when this set of environmental variables are similar for the missing half-hour CO2 flux and the available CO2 data Good 
Marginal Distribution Sampling (MDS) [122,123Half-hour CO2 gaps are filled by a half-hour CO2 values with similar meteorological conditions in the temporal vicinity of the gap to be filled. This method is a moving LUT technique that exploits the temporal auto-correlation structure of CO2 fluxes. Good 
Combination of MDS and MDV [124When meteorological variables regulating CO2 fluxes are available, the half-hour CO2 gap is filled using the MDS method with a moveable time window. When meteorological variables are not available, the missing value is filled using the MDV method with a short window size (i.e. the same day) and the window size can increase until the value can be filled. Good 
Non-linear regressions [122,123Half-hour CO2 gaps are filled using the relationships between available CO2 fluxes and associated controlling environmental factors during the period of missing fluxes. Good performance in general, although outliers can contribute to a high bias in predicted fluxes 
Artificial Neural networks [123Half-hour CO2 gaps are filled using non-linear relationships between meteorological variables and available CO2 fluxes. The network is trained by presenting it with sets of regulating meteorological variables and available CO2 data to predict missing data. Good performance particularly when data can be smoothed over trained networks 

Good reliability of annual sum of the net CO2 exchange refers to methods that ranked the best based on a several statistical metrics to predict annual fluxes as reported in References [122,123]. These statistical metrics include Root Mean Square Error, Bias Error and the annual CO2 flux sum among others and were evaluated by comparing the filled NEE data with the observed values.

Whether using chamber-based or micrometeorological approaches, measured NEE provides an opportunity to explore changes in ecosystem-scale gas exchange at high temporal frequency. Photosynthesis at the ecosystem scale is generally defined as gross primary productivity (GPP), which is only one component of NEE. GPP is derived as the difference between measured NEE and modeled ecosystem respiration (ER; Table 5). Obtaining GPP from NEE involves modeling ER using temperature and light response functions; a process typically referred to as flux partitioning [24,32,37,38]. Flux partitioning allows for the investigation over time of GPP and ER in response to a variety of conditions [39–41]. A challenge with flux partitioning is introduced by the inhibitory effect of light on leaf respiration rates, known as the Kok effect [42]. In the light, autotrophic respiration can be significantly lower than at night resulting in GPP estimation errors when ignored [43].

Table 5
Partitioning methods to estimate Gross Primary Productivity (GPP) and ecosystem respiration (Reco)
Partitioning methodDescription
Night-time method [124This method uses night-time NEE to estimate the basal Reco at 15 Celsius and the sensitivity of respiration to temperature. These parameters are then combined to estimate daytime Reco. GPP is estimated summing daytime Reco and daytime NEE values. 
Day-time method [38This method uses daytime NEE to parameterize a light response curve, to calculate GPP. The fitted curve is used to estimate the basal Reco at 15 Celsius, and combined with a temperature response function, to estimate Reco. 
Partitioning methodDescription
Night-time method [124This method uses night-time NEE to estimate the basal Reco at 15 Celsius and the sensitivity of respiration to temperature. These parameters are then combined to estimate daytime Reco. GPP is estimated summing daytime Reco and daytime NEE values. 
Day-time method [38This method uses daytime NEE to parameterize a light response curve, to calculate GPP. The fitted curve is used to estimate the basal Reco at 15 Celsius, and combined with a temperature response function, to estimate Reco. 

Both methods assume that any difference between daytime and nighttime Reco is due to temperature alone.

Recent micrometeorological approaches have attempted to measure GPP using a sulfur-containing analog of CO2, carbonyl sulfide (COS) that acts as natural ‘tracer’ molecule for GPP. This molecule enters a leaf in the same manner as CO2 and is broken down by the enzyme carbonic anhydrase. Because of this, COS ‘uptake’ should scale with GPP, removing the need for partitioning NEE into the GPP and respiration components [44]. Studies using this method are showing promising insights with GPP estimated using CO2 vs. COS measurements agreeing within 15% in forests and crops [45]. Another study that investigated variability in COS uptake and release in forests found agreement to within 3.5% between the two methods when GPP was high [46]. These results suggest an opportunity to use indirect methods for assessing GPP at larger scales, although recent work also suggests that photosynthetic tissues are not the only sink for COS [46–48].

Obtaining photosynthetic carbon uptake measurements using gas exchange systems is laborious resulting in efforts to replace this technique with other high-throughput methods. There exists a rapid growth in plant phenotyping greenhouses with the goal of automated measurement capabilities [49] at scales ranging from leaf to globe (Figure 1). Even with the most modern technologies, direct monitoring of leaf or plant level gas exchange would require substantial effort and resources. Thus, there are emerging technologies that provide means to infer plant responses to their growth environments that overcome the limitation of gas exchange [50–53]. Commercial sensors are available that provide information about plant canopy architecture and volume, which is important to infer growth over time [54], yet disentangling the underlying factors that lead to this growth requires physiological understanding. In the field, plot-level estimations of photosynthetic traits have been successfully estimated using a variety of platforms [55–57]. However, there needs to be improvements to the precision, accuracy, repeatability, and data pipeline before we can use these methods to estimate photosynthesis. Nonetheless, these new methods have a large potential impact on leaf to canopy understanding of plant physiology, ecosystem functioning and improving breeding efforts to maximize crop yields. In this section, we will discuss emerging technologies to monitor photosynthesis using spectral reflectance or fluorescence techniques. We will first outline the tools used for these approaches followed by a description of how these tools are being used.

Hyperspectral approaches to measure photosynthesis

Hyperspectral analysis is a non-destructive means of analysis that uses light reflected from vegetation to infer leaf, plant, canopy, or ecosystem performance. At the leaf and single-plant level, spectral sensors funnel light reflected from vegetation through a holographic diffraction grating, which separates light by wavelength across the electromagnetic spectrum [58]. Hyperspectral imaging data is in three ‘cubed’ dimensions with spectral wavelength (z) across spatial co-ordinates (x,y). Depending on the size of a single-pixel hyperspectral cameras can image vegetation from the whole plant to ecosystem scale [58].

Reflected light has become a powerful tool to characterize plant traits, including photosynthesis, given the varying response of light to leaf structure and pigment content at different wavelengths. In the near infrared (770–1300 nm), differences in chlorophyll and plant nitrogen content indicate a variety of vegetation stressors such as nutrient deficiency [59,60], plant disease status [61,62], and ozone damage [63], while the short wave infrared (SWIR1; 1300–2500 nm) indicates plant water status based traits [64,65]. In the past, discrete spectral reflectance indices were used as proxies for crop status [66]. However, computational and technological advances make it possible to derive photosynthetic capacities (maximum rate of carboxylation for C3 and C4 plants, Vcmax and Vmax, respectively; and maximum rate of electron transport, Jmax) and make predictions about photosynthetic performance scaling from the leaf [67–71] to the plot [72,73] and ecosystem scales [74].

One significant advance is the commercial availability of high-resolution fiber optic leaf clip-attachments. Hyperspectral radiometers typically contain a radiometrically calibrated light source and standardized white and dark reference panels for calibration. Leaf-level reflective intensity is compared with the reference material. Computer models (discussed later) are then used to correlate portions of the leaf's reflective spectrum with traditional measurements of gas exchange. Hyperspectral data can provide significant information about leaf photosynthesis at a fraction of the time compared with gas exchange [67–71,75]. These measurements can offer insight for upscaling to the plot level using field push carts [76] or drones mounted with hyperspectral cameras for breeding and research trials.

In addition to the hyperspectral methods mentioned above, recently handheld multispectral tools (e.g. FluroPen, Photo Systems Instruments, Drásov, Czech Republic; MultispeQ, PHOTOSYNQ INC. East Lancing MI, U.S.A.; and LI-600, LiCOR Biosciences Lincoln NE, U.S.A.) are used to monitor fluorescence and other parameters associated with leaves. Compared with hyperspectral leaf clips or fluorescence chambers sold with gas exchange units, these leaf tools can be used to more quickly and inexpensively screen for the vitality of photosynthetic systems under biotic and abiotic stresses (e.g. [77]). Furthermore, these tools provide opportunity, in some cases, to specify wavebands of interest for specific phenotypes that can extend beyond photosynthetic measurements.

Inspired by the successful leaf-level estimations of photosynthetic capacities, hyperspectral imaging (HSI) techniques are increasingly applied to canopy-scale measurements [73,78]. Imaging hyperspectral spectrometers provide more spatial information than a leaf-clip portable radiometer. Because of this, these sensors are being utilized to reveal variability in photosynthetic traits of interest across leaves, plants, and/or over large geographic areas [72,74]. These HSI sensors can scan individual plants in a few seconds [79] or provide analysis spanning several km2 if mounted on aircraft or Earth-orbiting satellites [80,81]. Compared with point-based portable radiometers, these HSI sensors result in the accumulation of large amounts of data that need to be processed in an innovative way.

To link reflectance spectra to photosynthetic physiological parameters, data processing pipelines must be tailored to specific sensing platforms. These data pipelines are critical to applications such as field phenotyping in a high-throughput manner. For leaf-level estimations of photosynthetic variables using reflectance spectra, great efforts have been made to select statistical techniques that can provide the best predictive power [75]. Partial Least Square Regression (PLSR) [82] is currently the most common technique used to relate reflectance spectra to photosynthesis associated parameters [68,71] due to its ability to reduce tens to hundreds of spectral bands to just a few orthogonal principle components (also known as latent variables). There are also other machine learning algorithms such as Artificial Neural Network (ANN)-based regression and Least Absolute Shrinkage and Selection Operator (LASSO) that have been used to estimate photosynthesis [83]. The availability of these machine learning and empirical algorithms also poses a dilemma regarding the most effective approach. Collectively harnessing the strengths of individual empirical or machine learning algorithms through regression stacking shows promise [72] although further studies are needed to test its effectiveness across more plant species. For estimations of photosynthesis using reflectance spectra at the plot and ecosystem levels, further data processing steps are necessary to account for spurious variations in reflectance caused by sun-target-sensor geometry, canopy structure, leaf scattering, atmospheric contaminations, and background soil [75]. These steps are required to ensure that only reflectance data associated with photosynthesis are used for estimations. Although Radiative Transfer Models (RTMs) such as PROSAIL [84] are developed to remove those spurious variations, few of them can be directly used in the proximal sensing setting [85]. However, these RTMs provide an alternative way to reduce hyperspectral data into several meaningful leaf traits, such as chlorophyll concentration, that can serve as a proxy for photosynthesis. For example, RTMs-inverted traits were shown to explain up to 60% of variation in photosynthetic physiology in a crop species [72].

Remote-sensing products that measure GPP are traditionally based on the Light-Use Efficiency (LUE) concept of ecosystem modeling [86] and empirical models that rely on the relationships between remote sensing-derived variables and GPP [87–90]. These methods provide reasonable estimates of GPP compared with measured EC fluxes, however, new emerging spectral sensing technologies including Solar-Induced chlorophyll Fluorescence (SIF) are providing potential for estimating GPP at the ecosystem scale [91–93]. A fraction of solar radiation absorbed by chlorophyll is emitted as fluorescence, hence SIF is more physiologically based than other traditional remote sensing products [94] as it is a direct product of the photosynthetic process [95–97]. While pulse amplitude modulated chlorophyll fluorescence has long been used to measure photochemical efficiencies and heat dissipation in individual leaves [98], this should not be confused with SIF, which relies on measuring of the radiance chlorophyll fluorescence from an ecosystem.

Passive SIF measurements were first applied at the satellite scale (Table 6) [99] to assess regional and global scale patterns of SIF alongside GPP [91–93] and is now being implemented at flux towers across multiple ecosystem types to determine the physiological and structural relationship between SIF and photosynthesis at this scale [100–103]. Likewise, the near-infrared radiance of vegetation index (NIRv) has shown promising accuracy at detecting photosynthetic variability at the hourly scale over crop and forest system [104,105]. Therefore, both SIF and NIRv should enable real-time monitoring of productivity and stress.

Table 6
Spatial and temporal resolution major satellite sensors and platforms for Solar Induced Photosynthesis (SIF) estimations
Sensors/SatellitesStatusSpatial resolution (km × km)Temporal resolutionSampling strategySpatial coverage
Thermal and Near-infrared Sensor for carbon Observations — Fourier Transform Spectrometer (TNSO-FTS)/Greenhouse Gases Observing Satellite (GOSAT) In operation since 2009 10 × 10 3 days Sparse Global 
Global Ozone Monitoring Experiment–2 (GOME-2)/Metop satellites In operation since 2007 80 × 40 (40 × 40129 days Continuous Global 
SCanning Imaging Absorption SpectroMeter for Atmospheric ChartographY (SCIMACHY)/Envisat satellite 2002-2012 200 × 30 2 days Continuous Global 
TROPOspheric Monitoring Instrument (TROPOMI)/Sentinel- 5p In operation since 2017 7 × 3 1 day Continuous Global 
Orbiting Carbon Observatory 2 instrument/OCO-2 In operation since 2014 1.3 × 2.25 16 days Sparse Global 
Orbiting Carbon Observatory 3 instrument/OCO-3 In operation since 2019 at International Space Station 1.75 × 2.2 Not fixed Sparse Global 
Fluorescence Imaging Spectrometer (FLORIS)/Fluorescence Explorer (FLEX) In planning for 2022 0.3 × 0.3 27 days Continuous Global 
Sensors/SatellitesStatusSpatial resolution (km × km)Temporal resolutionSampling strategySpatial coverage
Thermal and Near-infrared Sensor for carbon Observations — Fourier Transform Spectrometer (TNSO-FTS)/Greenhouse Gases Observing Satellite (GOSAT) In operation since 2009 10 × 10 3 days Sparse Global 
Global Ozone Monitoring Experiment–2 (GOME-2)/Metop satellites In operation since 2007 80 × 40 (40 × 40129 days Continuous Global 
SCanning Imaging Absorption SpectroMeter for Atmospheric ChartographY (SCIMACHY)/Envisat satellite 2002-2012 200 × 30 2 days Continuous Global 
TROPOspheric Monitoring Instrument (TROPOMI)/Sentinel- 5p In operation since 2017 7 × 3 1 day Continuous Global 
Orbiting Carbon Observatory 2 instrument/OCO-2 In operation since 2014 1.3 × 2.25 16 days Sparse Global 
Orbiting Carbon Observatory 3 instrument/OCO-3 In operation since 2019 at International Space Station 1.75 × 2.2 Not fixed Sparse Global 
Fluorescence Imaging Spectrometer (FLORIS)/Fluorescence Explorer (FLEX) In planning for 2022 0.3 × 0.3 27 days Continuous Global 
1

The spatial resolution 40 by 40 km is available since July 2013 in Metop-A and B tandem operation;

SIF measurement was first applied at the satellite scale [99] to assess regional and global scale patterns of SIF alongside GPP [91–93]. Currently, it is being implemented at flux towers across multiple ecosystem types to determine the physiological and structural relationship between SIF and photosynthesis at this scale [100–103]. For comparison, the EC method has a spatial resolution between hundred meters and several kilometers, and a continuous temporal resolution (half-hour) with a fine spatial coverage at the ecosystem and landscape scales.

The relationship between SIF and GPP is primarily dominated by absorbed photosynthetic active radiation (APAR) [106,107], implying that the correlation between SIF and GPP is the highest when photosynthesis is primarily light-limited [108,109]. However, GPP is also controlled by environmental factors other than light, and recent insights suggest that SIF responded to environmental stresses in a similar way as GPP, encouraging the application of SIF to estimate photosynthesis [94]. A relationship between SIF and GPP was similar among ecosystems although the relationship was stronger for grasslands than forests, savannas and croplands, and for C4 grasslands and crops than C3 ecosystems [94]. This quasi-universal relationship indicates that SIF could be a valuable tool for inferring GPP of the land surface. More collaborative studies between the EC and remote sensing communities are needed to evaluate why the relationship between SIF and GPP varies among ecosystems and under differing environmental conditions to improve the ability of SIF products to estimate ecosystem GPP robustly to scale regionally and globally.

Much progress has been made to understand the relationship between SIF and GPP but many challenges remain [109–111]. Higher spatial and temporal resolution SIF measurements are needed to coincide with the continuous GPP measurements [112]. Promising solutions to these challenges would be to develop remote sensing approaches that can cross-calibrate and blend multi-source SIF and reflectance measurements for a consistent record in both spatial and temporal domains. For example, combining satellite SIF with satellite reflectance was used to generate a spatially and temporally continuous SIF dataset [113]. Another solution is to improve SIF sensor designs to facilitate measurements at a much higher spatial and temporal resolutions. For example, the Fluorescence Imaging Spectrometer (FLORIS) onboard the Fluorescence EXplorer (FLEX) satellite can provide SIF at a better spatial resolution than its predecessors (Table 6) [114] and the newly launched Orbiting Carbon Observatory 3 instrument (OCO-3) allow for more coverage globally at higher definition [115].

Interestingly, much of the work on remote sensing has initiated with large-scale measurements, yet there is a tremendous need to increase throughput of measurements at leaf and plot scales, particularly for application in high throughput phenotyping facilities. Whether these techniques are fully scalable remains uncertain, yet the opportunity for multidisciplinary research has advanced the versatility of the tools outlined in this review beyond their original users. Moving forward, simplifying data collection through ‘turn-key’ sensors and standardizing data analysis pipelines for the variety of techniques outlined here are certain to advance understanding of plant function from molecular to global scale.

  • Monitoring Photosynthesis at every scale, from leaf to ecosystem, is an important task given the challenges of climate change and growing human populations.

  • In the past 5 years there have been significant improvements to the technology and computational tools used to measure photosynthesis at every scale. And new facilities and equipment are being used around the world to monitor photosynthesis.

  • Hyperspectral imaging at the leaf, and canopy scale paired with improved computational modeling allows for rapid estimates of important biochemical parameters.

  • Micrometeorological approaches to estimate Gross Primary Productivity have been improved by the uses of sulfur tracing elements.

  • Monitoring Solar Induced Fluorescence is a promising satellite-based method that should enable real-time monitoring of global ecosystem productivity.

The authors declare that there are no competing interests associated with the manuscript.

M.H.S., N.G.-C., and C.J.B. conceived the outline, all authors contributed to the organization and writing of the manuscript, M.H.S. and N.G-C. Edited the manuscript, and C.J.B. supervised the project.

This work is supported by funding from Global Change and Photosynthesis Research Unit of the USDA Agricultural Research Service. Any opinions, findings, and conclusions or recommendations expressed in this publication are those of the author(s) and do not necessarily reflect the views of the U.S. Department of Agriculture. Mention of trade names or commercial products in this publication is solely for the purpose of providing specific information and does not imply recommendation or endorsement by the U.S. Department of Agriculture. USDA is an equal opportunity provider and employer.

COS

carbonyl sulfide

EC

eddy covariance

ER

ecosystem respiration

FLEX

fluorescence explorer

FLORIS

fluorescence imaging spectrometer

GPP

gross primary productivity

HSI

hyperspectral imaging

NEE

net ecosystem exchange

RTMs

radiative transfer models

SIF

solar induced fluorescence

1
Friedlingstein
,
P.
,
Jones
,
M.
,
O'sullivan
,
M.
,
Andrew
,
R.
,
Hauck
,
J.
,
Peters
,
G.
et al. (
2019
)
Global carbon budget 2019
.
Earth Syst. Sci. Data
11
,
1783
1838
2
Thornley
,
J.H.M.
(
2002
)
Instantaneous canopy photosynthesis: analytical expressions for sun and shade leaves based on exponential light decay down the canopy and an acclimated non-rectangular hyperbola for leaf photosynthesis
.
Ann. Bot.
89
,
451
458
3
Beer
,
C.
,
Reichstein
,
M.
,
Tomelleri
,
E.
,
Ciais
,
P.
,
Jung
,
M.
,
Carvalhais
,
N.
et al. (
2010
)
Terrestrial gross carbon dioxide uptake: global distribution and covariation with climate
.
Science
329
,
834
838
4
Schwalm
,
C.R.
,
Glendon
,
S.
and
Duffy
,
P.B.
(
2020
)
RCP8. 5 tracks cumulative CO2 emissions
.
Proc. Natl Acad. Sci. U.S.A.
117
,
19656
19657
5
Valin
,
H.
,
Sands
,
R.D.
,
van der Mensbrugghe
,
D.
,
Nelson
,
G.C.
,
Ahammad
,
H.
,
Blanc
,
E.
et al. (
2014
)
The future of food demand: understanding differences in global economic models
.
Agric. Econ.
45
,
51
67
6
Long Stephen
,
P.
,
Marshall-Colon
,
A.
and
Zhu
,
X.-G.
(
2015
)
Meeting the global food demand of the future by engineering crop photosynthesis and yield potential
.
Cell
161
,
56
66
7
Ray
,
D.K.
,
Mueller
,
N.D.
,
West
,
P.C.
and
Foley
,
J.A.
(
2013
)
Yield trends are insufficient to double global crop production by 2050
.
PLoS ONE
8
,
e66428
8
Ruiz-Vera
,
U.M.
,
Siebers
,
M.
,
Gray
,
S.B.
,
Drag
,
D.W.
,
Rosenthal
,
D.M.
,
Kimball
,
B.A.
et al. (
2013
)
Global warming can negate the expected CO2 stimulation in photosynthesis and productivity for soybean grown in the Midwestern United States
.
Plant Physiol.
162
,
410
423
9
Ruiz-Vera
,
U.M.
,
Siebers
,
M.H.
,
Drag
,
D.W.
,
Ort
,
D.R.
and
Bernacchi
,
C.J.
(
2015
)
Canopy warming caused photosynthetic acclimation and reduced seed yield in maize grown at ambient and elevated [CO2]
.
Glob. Change Biol.
21
,
4237
4249
10
Siebers
,
M.H.
,
Slattery
,
R.A.
,
Yendrek
,
C.R.
,
Locke
,
A.M.
,
Drag
,
D.
,
Ainsworth
,
E.A.
et al. (
2017
)
Simulated heat waves during maize reproductive stages alter reproductive growth but have no lasting effect when applied during vegetative stages
.
Agric. Ecosyst. Environ.
240
,
162
170
11
Siebers
,
M.H.
,
Yendrek
,
C.R.
,
Drag
,
D.
,
Locke
,
A.M.
,
Rios Acosta
,
L.
,
Leakey
,
A.D.
et al. (
2015
)
Heat waves imposed during early pod development in soybean (Glycine max) cause significant yield loss despite a rapid recovery from oxidative stress
.
Glob. Change Biol.
21
,
3114
3125
12
Kubis
,
A.
and
Bar-Even
,
A.
(
2019
)
Synthetic biology approaches for improving photosynthesis
.
J. Exp. Bot.
70
,
1425
1433
13
Niinemets
,
Ü.
,
Berry
,
J.A.
,
von Caemmerer
,
S.
,
Ort
,
D.R.
,
Parry
,
M.A.
and
Poorter
,
H.
(
2017
)
Photosynthesis: ancient, essential, complex, diverse… and in need of improvement in a changing world
.
New Phytol.
213
,
43
47
14
Walker
,
B.J.
,
VanLoocke
,
A.
,
Bernacchi
,
C.J.
and
Ort
,
D.R.
(
2016
)
The costs of photorespiration to food production now and in the future
.
Annu. Rev. Plant Biol.
67
,
107
129
15
Sharkey
,
T.D.
(
2020
)
Emerging research in plant photosynthesis
.
Emerg. Top. Life Sci.
4
,
137
150
16
Long
,
S.P.
and
Bernacchi
,
C.
(
2003
)
Gas exchange measurements, what can they tell us about the underlying limitations to photosynthesis? procedures and sources of error
.
J. Exp. Bot.
54
,
2393
2401
17
Bernacchi
,
C.
,
Diaz-Espejo
,
A.
and
Flexas
,
J.
(
2012
) Gas-exchange analysis: basics and problems. In
Terrestrial Photosynthesis in A Changing Environment: A Molecular, Physiological, and Ecological Approach
(
Loreto
,
F.
,
Medrano
,
H.
and
Flexas
,
J.
, eds), pp.
115
130
,
Cambridge University Press
,
Cambridge
18
Edwards
,
G.
,
Voznesenskaya
,
E.
,
Smith
,
M.
,
Koteyeva
,
N.
,
Park
,
Y.-I.
,
Park
,
J.
et al. (
2008
)
Breaking the Kranz Paradigm in Terrestrial C 4 Plants: Does it Hold Promise for C 4 Rice? Charting new Pathways to C4 Rice
,
World Scientific
, p.
249
273
19
King
,
J.L.
,
Edwards
,
G.E.
and
Cousins
,
A.B.
(
2012
)
The efficiency of the CO2-concentrating mechanism during single-cell C4 photosynthesis
.
Plant Cell Environ.
35
,
513
523
20
Baldocchi
,
D.
(
2014
)
Measuring fluxes of trace gases and energy between ecosystems and the atmosphere–the state and future of the eddy covariance method
.
Glob. Change Biol.
20
,
3600
3609
21
Stinziano
,
J.R.
,
Morgan
,
P.B.
,
Lynch
,
D.J.
,
Saathoff
,
A.J.
,
McDermitt
,
D.K.
and
Hanson
,
D.T.
(
2017
)
The rapid A–Ci response: photosynthesis in the phenomic era
.
Plant Cell Environ.
40
,
1256
1262
22
Ainsworth
,
E.A.
,
Davey
,
P.A.
,
Hymus
,
G.J.
,
Drake
,
B.G.
and
Long
,
S.P.
(
2002
)
Long-term response of photosynthesis to elevated carbon dioxide in a florida scrub-oak ecosystem
.
Ecol. Appl.
12
,
1267
1275
23
Papale
,
D.
,
Reichstein
,
M.
,
Aubinet
,
M.
,
Canfora
,
E.
,
Bernhofer
,
C.
,
Kutsch
,
W.
et al. (
2006
)
Towards a standardized processing of Net ecosystem exchange measured with eddy covariance technique: algorithms and uncertainty estimation
.
Biogeosciences
3
,
571
583
24
Aubinet
,
M.
,
Vesala
,
T.
and
Papale
,
D.
(
2012
)
Eddy Covariance: A Practical Guide to Measurement and Data Analysis
,
Springer Science & Business Media
25
Hsieh
,
C.-I.
,
Katul
,
G.
and
Chi
,
T.W.
(
2000
)
An approximate analytical model for footprint estimation of scalar fluxes in thermally stratified atmospheric flows
.
Adv. Water Resour.
23
,
765
772
26
Kljun
,
N.
,
Calanca
,
P.
,
Rotach
,
M.W.
and
Schmid
,
H.P.
(
2004
)
A simple parameterisation for flux footprint predictions
.
Bound. Layer Meteorol.
112
,
503
523
27
Leuning
,
R.
,
Van Gorsel
,
E.
,
Massman
,
W.J.
and
Isaac
,
P.R.
(
2012
)
Reflections on the surface energy imbalance problem
.
Agric. Forest Meteorol.
156
,
65
74
28
Stoy
,
P.C.
,
Mauder
,
M.
,
Foken
,
T.
,
Marcolla
,
B.
,
Boegh
,
E.
,
Ibrom
,
A.
et al. (
2013
)
A data-driven analysis of energy balance closure across FLUXNET research sites: the role of landscape scale heterogeneity
.
Agric. Forest Meteorol.
171
,
137
152
29
Falge
,
E.
,
Baldocchi
,
D.
,
Tenhunen
,
J.
,
Aubinet
,
M.
,
Bakwin
,
P.
,
Berbigier
,
P.
et al. (
2002
)
Seasonality of ecosystem respiration and gross primary production as derived from FLUXNET measurements
.
Agric. Forest Meteorol.
113
,
53
74
30
Gomez-Casanovas
,
N.
,
DeLucia
,
N.J.
,
Bernacchi
,
C.J.
,
Boughton
,
E.H.
,
Sparks
,
J.P.
,
Chamberlain
,
S.D.
et al. (
2018
)
Grazing alters net ecosystem C fluxes and the global warming potential of a subtropical pasture
.
Ecol. Appl.
28
,
557
572
31
Gomez-Casanovas
,
N.
,
DeLucia
,
N.J.
,
DeLucia
,
E.H.
,
Blanc-Betes
,
E.
,
Boughton
,
E.H.
,
Sparks
,
J.
et al. (
2020
)
Seasonal controls of CO2 and CH4 dynamics in a temporarily flooded subtropical wetland
.
J. Geophys. Res. Biogeosci.
125
,
e2019JG005257
32
Baldocchi
,
D.
,
Falge
,
E.
,
Gu
,
L.
,
Olson
,
R.
,
Hollinger
,
D.
,
Running
,
S.
et al. (
2001
)
FLUXNET: a new tool to study the temporal and spatial variability of ecosystem-scale carbon dioxide, water vapor, and energy flux densities
.
Bull. Am. Meteorol. Soc.
82
,
2415
2434
33
Wolf
,
S.
,
Keenan
,
T.F.
,
Fisher
,
J.B.
,
Baldocchi
,
D.D.
,
Desai
,
A.R.
,
Richardson
,
A.D.
et al. (
2016
)
Warm spring reduced carbon cycle impact of the 2012 US summer drought
.
Proc. Natl Acad. Sci. U.S.A.
113
,
5880
5885
34
Chu
,
H.
,
Baldocchi
,
D.D.
,
John
,
R.
,
Wolf
,
S.
and
Reichstein
,
M.
(
2017
)
Fluxes all of the time? A primer on the temporal representativeness of FLUXNET
.
J. Geophys. Res. Biogeosci.
122
,
289
307
35
Baldocchi
,
D.D.
(
2020
)
How eddy covariance flux measurements have contributed to our understanding of global change biology
.
Glob. Change Biol.
26
,
242
260
36
Ichii
,
K.
,
Ueyama
,
M.
,
Kondo
,
M.
,
Saigusa
,
N.
,
Kim
,
J.
,
Alberto
,
M.C.
et al. (
2017
)
New data-driven estimation of terrestrial CO2 fluxes in Asia using a standardized database of eddy covariance measurements, remote sensing data, and support vector regression
.
J. Geophys. Res. Biogeosci.
122
,
767
795
37
Lloyd
,
J.
and
Taylor
,
J.A.
(
1994
)
On the temperature dependence of soil respiration
.
Funct. Ecol.
8
,
315
323
38
Lasslop
,
G.
,
Reichstein
,
M.
,
Papale
,
D.
,
Richardson
,
A.D.
,
Arneth
,
A.
,
Barr
,
A.
et al. (
2010
)
Separation of net ecosystem exchange into assimilation and respiration using a light response curve approach: critical issues and global evaluation
.
Glob. Change Biol.
16
,
187
208
39
Beringer
,
J.
,
Hutley
,
L.B.
,
McHugh
,
I.
,
Arndt
,
S.K.
,
Campbell
,
D.
,
Cleugh
,
H.A.
et al. (
2016
)
An introduction to the Australian and New Zealand flux tower network – ozFlux
.
Biogeosciences
13
,
5895
5916
40
Baldocchi
,
D.
,
Chu
,
H.
and
Reichstein
,
M.
(
2018
)
Inter-annual variability of net and gross ecosystem carbon fluxes: a review
.
Agric. Forest Meteorol.
249
,
520
533
41
Pastorello
,
G.
,
Trotta
,
C.
,
Eleonora
,
C.
,
Housen
,
C.
,
Christianson
,
D.
,
You-Wei
,
C.
et al. (
2020
)
The FLUXNET2015 dataset and the ONEFlux processing pipeline for eddy covariance data
.
Sci. Data
7
,
225
42
Tcherkez
,
G.
,
Gauthier
,
P.
,
Buckley
,
T.N.
,
Busch
,
F.A.
,
Barbour
,
M.M.
,
Bruhn
,
D.
et al. (
2017
)
Tracking the origins of the Kok effect, 70 years after its discovery
.
New Phytol.
214
,
506
510
43
Keenan
,
T.F.
,
Migliavacca
,
M.
,
Papale
,
D.
,
Baldocchi
,
D.
,
Reichstein
,
M.
,
Torn
,
M.
et al. (
2019
)
Widespread inhibition of daytime ecosystem respiration
.
Nat. Ecol. Evol.
3
,
407
415
44
Protoschill-Krebs
,
G.
,
Wilhelm
,
C.
and
Kesselmeier
,
J.
(
1996
)
Consumption of carbonyl sulphide (COS) by higher plant carbonic anhydrase (CA)
.
Atmos. Environ.
30
,
3151
3156
45
Asaf
,
D.
,
Rotenberg
,
E.
,
Tatarinov
,
F.
,
Dicken
,
U.
,
Montzka
,
S.A.
and
Yakir
,
D.
(
2013
)
Ecosystem photosynthesis inferred from measurements of carbonyl sulphide flux
.
Nat. Geosci.
6
,
186
190
46
Whelan
,
M.E.
,
Lennartz
,
S.T.
,
Gimeno
,
T.E.
,
Wehr
,
R.
,
Wohlfahrt
,
G.
,
Wang
,
Y.
et al. (
2018
)
Reviews and syntheses: carbonyl sulfide as a multi-scale tracer for carbon and water cycles
.
Biogeosciences
15
,
3625
3657
47
Maseyk
,
K.
,
Berry
,
J.A.
,
Billesbach
,
D.
,
Campbell
,
J.E.
,
Torn
,
M.S.
,
Zahniser
,
M.
et al. (
2014
)
Sources and sinks of carbonyl sulfide in an agricultural field in the southern great plains
.
Proc. Natl Acad. Sci. U.S.A.
111
,
9064
9069
48
Berkelhammer
,
M.
,
Alsip
,
B.
,
Matamala
,
R.
,
Cook
,
D.
,
Whelan
,
M.
,
Joo
,
E.
et al. (
2020
)
Seasonal evolution of canopy stomatal conductance for a prairie and maize field in the midwestern United States from continuous carbonyl sulfide fluxes
.
Geophys. Res. Lett.
47
,
e2019GL085652
49
Mir
,
R.R.
,
Reynolds
,
M.
,
Pinto
,
F.
,
Khan
,
M.A.
and
Bhat
,
M.A.
(
2019
)
High-throughput phenotyping for crop improvement in the genomics era
.
Plant Sci.
282
,
60
72
50
Keller
,
B.
,
Vass
,
I.
,
Matsubara
,
S.
,
Paul
,
K.
,
Jedmowski
,
C.
,
Pieruschka
,
R.
et al. (
2019
)
Maximum fluorescence and electron transport kinetics determined by light-induced fluorescence transients (LIFT) for photosynthesis phenotyping
.
Photosynth. Res.
140
,
221
233
51
Keller
,
B.
,
Matsubara
,
S.
,
Rascher
,
U.
,
Pieruschka
,
R.
,
Steier
,
A.
,
Kraska
,
T.
et al. (
2019
)
Genotype specific photosynthesis × environment interactions captured by automated fluorescence canopy scans over two fluctuating growing seasons
.
Front. Plant Sci.
10
,
1482
52
Pérez-Bueno
,
M.L.
,
Pineda
,
M.
and
Barón
,
M.
(
2019
)
Phenotyping plant responses to biotic stress by chlorophyll fluorescence imaging
.
Front. Plant Sci.
10
,
1135
53
Yu
,
W.
,
Körner
,
O.
and
Schmidt
,
U.
(
2020
)
Crop photosynthetic performance monitoring based on a combined system of measured and modelled chloroplast electron transport rate in greenhouse tomato
.
Front. Plant Sci.
11
,
1038
54
Roitsch
,
T.
,
Cabrera-Bosquet
,
L.
,
Fournier
,
A.
,
Ghamkhar
,
K.
,
Jiménez-Berni
,
J.
,
Pinto
,
F.
et al. (
2019
)
Review: new sensors and data-driven approaches—A path to next generation phenomics
.
Plant Sci.
282
,
2
10
55
Bai
,
G.
,
Ge
,
Y.
,
Hussain
,
W.
,
Baenziger
,
P.S.
and
Graef
,
G.
(
2016
)
A multi-sensor system for high throughput field phenotyping in soybean and wheat breeding
.
Comput. Electron. Agric.
128
,
181
192
56
Zhang
,
C.
,
Marzougui
,
A.
and
Sankaran
,
S.
(
2020
)
High-resolution satellite imagery applications in crop phenotyping: an overview
.
Comput. Electron. Agric.
175
,
105584
57
Bandopadhyay
,
S.
,
Rastogi
,
A.
and
Juszczak
,
R.
(
2020
)
Review of Top-of-Canopy Sun-Induced fluorescence (SIF) studies from ground, UAV, airborne to spaceborne observations
.
Sensors
20
,
1144
58
Bannon
,
D.
(
2009
)
Cubes and slices
.
Nat. Photonics.
3
,
627
629
59
Ayala-Silva
,
T.
and
Beyl
,
C.A.
(
2005
)
Changes in spectral reflectance of wheat leaves in response to specific macronutrient deficiency
.
Adv. Space Res.
35
,
305
317
60
Filella
,
I.
,
Serrano
,
L.
,
Serra
,
J.
and
Peñuelas
,
J.
(
1995
)
Evaluating wheat nitrogen status with canopy reflectance indices and discriminant analysis
.
Crop Sci.
35
,
1400
1405
61
Knipling
,
E.B.
(
1970
)
Physical and physiological basis for the reflectance of visible and near-infrared radiation from vegetation
.
Remote Sensing Environ.
1
,
155
159
62
Bajwa
,
S.G.
,
Rupe
,
J.C.
and
Mason
,
J.
(
2017
)
Soybean disease monitoring with leaf reflectance
.
Remote Sensing
9
,
127
63
Peñuelas
,
J.
and
Filella
,
I.
(
1998
)
Visible and near-infrared reflectance techniques for diagnosing plant physiological status
.
Trends Plant Sci.
3
,
151
156
64
Gao
,
B.-C.
(
1996
)
NDWI—a normalized difference water index for remote sensing of vegetation liquid water from space
.
Remote Sensing Environ.
58
,
257
266
65
Chen
,
D.
,
Huang
,
J.
and
Jackson
,
T.J.
(
2005
)
Vegetation water content estimation for corn and soybeans using spectral indices derived from MODIS near- and short-wave infrared bands
.
Remote Sensing Environ.
98
,
225
236
66
Xue
,
J.
and
Su
,
B.
(
2017
)
Significant remote sensing vegetation indices: a review of developments and applications
.
J. Sensors
2017
,
1353691
67
Ainsworth
,
E.A.
,
Serbin
,
S.P.
,
Skoneczka
,
J.A.
and
Townsend
,
P.A.
(
2014
)
Using leaf optical properties to detect ozone effects on foliar biochemistry
.
Photosynth. Res.
119
,
65
76
68
Serbin
,
S.P.
,
Dillaway
,
D.N.
,
Kruger
,
E.L.
and
Townsend
,
P.A.
(
2012
)
Leaf optical properties reflect variation in photosynthetic metabolism and its sensitivity to temperature
.
J. Exp. Bot.
63
,
489
502
69
Yendrek
,
C.R.
,
Tomaz
,
T.
,
Montes
,
C.M.
,
Cao
,
Y.
,
Morse
,
A.M.
,
Brown
,
P.J.
et al. (
2017
)
High-throughput phenotyping of maize leaf physiological and biochemical traits using hyperspectral reflectance
.
Plant Physiol.
173
,
614
70
Silva-Perez
,
V.
,
Molero
,
G.
,
Serbin
,
S.P.
,
Condon
,
A.G.
,
Reynolds
,
M.P.
,
Furbank
,
R.T.
et al. (
2018
)
Hyperspectral reflectance as a tool to measure biochemical and physiological traits in wheat
.
J. Exp. Bot.
69
,
483
496
71
Meacham-Hensold
,
K.
,
Montes
,
C.M.
,
Wu
,
J.
,
Guan
,
K.
,
Fu
,
P.
,
Ainsworth
,
E.A.
et al. (
2019
)
High-throughput field phenotyping using hyperspectral reflectance and partial least squares regression (PLSR) reveals genetic modifications to photosynthetic capacity
.
Remote Sensing Environ.
231
,
111176
72
Fu
,
P.
,
Meacham-Hensold
,
K.
,
Guan
,
K.
,
Wu
,
J.
and
Bernacchi
,
C.
(
2020
)
Estimating photosynthetic traits from reflectance spectra: a synthesis of spectral indices, numerical inversion, and partial least square regression
.
Plant Cell Environ.
43
,
1241
1258
73
Meacham-Hensold
,
K.
,
Fu
,
P.
,
Wu
,
J.
,
Serbin
,
S.
,
Montes
,
C.M.
,
Ainsworth
,
E.
et al. (
2020
)
Plot-level rapid screening for photosynthetic parameters using proximal hyperspectral imaging
.
J. Exp. Bot.
71
,
2312
2328
74
Serbin
,
S.P.
,
Singh
,
A.
,
Desai
,
A.R.
,
Dubois
,
S.G.
,
Jablonski
,
A.D.
,
Kingdon
,
C.C.
et al. (
2015
)
Remotely estimating photosynthetic capacity, and its response to temperature, in vegetation canopies using imaging spectroscopy
.
Remote Sensing Environ.
167
,
78
87
75
Fu
,
P.
,
Meacham-Hensold
,
K.
,
Guan
,
K.
and
Bernacchi
,
C.J.
(
2019
)
Hyperspectral leaf reflectance as proxy for photosynthetic capacities: an ensemble approach based on multiple machine learning algorithms
.
Front. Plant Sci.
10
,
730
76
Deery
,
D.
,
Jimenez-Berni
,
J.
,
Jones
,
H.
,
Sirault
,
X.
and
Furbank
,
R.
(
2014
)
Proximal remote sensing buggies and potential applications for field-based phenotyping
.
Agronomy
4
,
349
379
77
Kuhlgert
,
S.
,
Austic
,
G.
,
Zegarac
,
R.
,
Osei-Bonsu
,
I.
,
Hoh
,
D.
,
Chilvers
,
M.I.
et al. (
2016
)
Multispeq beta: a tool for large-scale plant phenotyping connected to the open photosynQ network
.
R. Soc. Open Sci.
3
,
160592
78
Fu
,
P.
,
Meacham-Hensold
,
K.
,
Siebers
,
M.H.
and
Bernacchi
,
C.J.
(
2020
)
The inverse relationship between solar-induced fluorescence yield and photosynthetic capacity: benefits for field phenotyping
.
J. Exp. Bot.
,
eraa537
79
Liu
,
H.
,
Bruning
,
B.
,
Garnett
,
T.
and
Berger
,
B.
(
2020
)
Hyperspectral imaging and 3D technologies for plant phenotyping: from satellite to close-range sensing
.
Comput. Electron. Agric.
175
,
105621
80
Pignatti
,
S.
,
Cavalli
,
R.M.
,
Cuomo
,
V.
,
Fusilli
,
L.
,
Pascucci
,
S.
,
Poscolieri
,
M.
et al. (
2009
)
Evaluating hyperion capability for land cover mapping in a fragmented ecosystem: Pollino national park, Italy
.
Remote Sensing Environ.
113
,
622
634
81
Liu
,
Y.
,
Sun
,
D.
,
Hu
,
X.
,
Ye
,
X.
,
Li
,
Y.
,
Liu
,
S.
et al. (
2019
)
The advanced hyperspectral imager: aboard China's gaoFen-5 satellite
.
IEEE Geosci. Remote Sensing Mag.
7
,
23
32
82
Wold
,
S.
,
Sjöström
,
M.
and
Eriksson
,
L.
(
2001
)
PLS-regression: a basic tool of chemometrics
.
Chemom. Intell. Lab. Syst.
58
,
109
130
83
Heckmann
,
D.
,
Schlüter
,
U.
and
Weber
,
A.P.M.
(
2017
)
Machine learning techniques for predicting crop photosynthetic capacity from leaf reflectance spectra
.
Mol. Plant
10
,
878
890
84
Jacquemoud
,
S.
,
Verhoef
,
W.
,
Baret
,
F.
,
Bacour
,
C.
,
Zarco-Tejada
,
P.J.
,
Asner
,
G.P.
et al. (
2009
)
PROSPECT+SAIL models: a review of use for vegetation characterization
.
Remote Sensing Environ.
113
,
S56
S66
85
Jay
,
S.
,
Bendoula
,
R.
,
Hadoux
,
X.
,
Féret
,
J.-B.
and
Gorretta
,
N.
(
2016
)
A physically-based model for retrieving foliar biochemistry and leaf orientation using close-range imaging spectroscopy
.
Remote Sensing Environ.
177
,
220
236
86
Monteith
,
J.
(
1972
)
Solar radiation and productivity in tropical ecosystems
.
J. Appl. Ecol.
9
,
747
766
87
Hilker
,
T.
,
Coops
,
N.C.
,
Wulder
,
M.A.
,
Black
,
T.A.
and
Guy
,
R.D.
(
2008
)
The use of remote sensing in light use efficiency based models of gross primary production: a review of current status and future requirements
.
Sci. Tot. Environ.
404
,
411
423
88
Zhang
,
L.
,
Zhou
,
D.
,
Fan
,
J.
,
Guo
,
Q.
,
Chen
,
S.
,
Wang
,
R.
et al. (
2019
)
Contrasting the performance of eight satellite-based GPP models in water-limited and temperature-limited grassland ecosystems
.
Remote Sensing.
11
,
1333
89
Wu
,
C.
,
Munger
,
J.W.
,
Niu
,
Z.
and
Kuang
,
D.
(
2010
)
Comparison of multiple models for estimating gross primary production using MODIS and eddy covariance data in harvard forest
.
Remote Sensing Environ.
114
,
2925
2939
90
Yuan
,
W.
,
Liu
,
S.
,
Zhou
,
G.
,
Zhou
,
G.
,
Tieszen
,
L.L.
,
Baldocchi
,
D.
et al. (
2007
)
Deriving a light use efficiency model from eddy covariance flux data for predicting daily gross primary production across biomes
.
Agric. Forest Meteorol.
143
,
189
207
91
Guanter
,
L.
,
Zhang
,
Y.
,
Jung
,
M.
,
Joiner
,
J.
,
Voigt
,
M.
,
Berry
,
J.A.
et al. (
2014
)
Global and time-resolved monitoring of crop photosynthesis with chlorophyll fluorescence
.
Proc. Natl Acad. Sci. U.S.A.
111
,
E1327
E1E33
92
Guan
,
K.
,
Berry
,
J.A.
,
Zhang
,
Y.
,
Joiner
,
J.
,
Guanter
,
L.
,
Badgley
,
G.
et al. (
2016
)
Improving the monitoring of crop productivity using spaceborne solar-induced fluorescence
.
Glob. Change Biol.
22
,
716
726
93
Song
,
L.
,
Guanter
,
L.
,
Guan
,
K.
,
You
,
L.
,
Huete
,
A.
,
Ju
,
W.
et al. (
2018
)
Satellite sun-induced chlorophyll fluorescence detects early response of winter wheat to heat stress in the Indian indo-Gangetic plains
.
Glob. Change Biol.
24
,
4023
4037
94
Li
,
X.
,
Xiao
,
J.
,
He
,
B.
,
Altaf Arain
,
M.
,
Beringer
,
J.
,
Desai
,
A.R.
et al. (
2018
)
Solar-induced chlorophyll fluorescence is strongly correlated with terrestrial photosynthesis for a wide variety of biomes: first global analysis based on OCO-2 and flux tower observations
.
Glob. Change Biol.
24
,
3990
4008
95
Frankenberg
,
C.
and
Berry
,
J.
(
2018
)
3.10 - solar induced chlorophyll fluorescence: origins, relation to photosynthesis and retrieval
.
Compr. Remote Sensing.
3
,
143
162
96
Porcar-Castell
,
A.
,
Tyystjärvi
,
E.
,
Atherton
,
J.
,
van der Tol
,
C.
,
Flexas
,
J.
,
Pfündel
,
E.E.
et al. (
2014
)
Linking chlorophyll a fluorescence to photosynthesis for remote sensing applications: mechanisms and challenges
.
J. Exp. Bot.
65
,
4065
4095
97
Migliavacca
,
M.
,
Perez-Priego
,
O.
,
Rossini
,
M.
,
El-Madany
,
T.S.
,
Moreno
,
G.
,
van der Tol
,
C.
et al. (
2017
)
Plant functional traits and canopy structure control the relationship between photosynthetic CO2 uptake and far-red sun-induced fluorescence in a Mediterranean grassland under different nutrient availability
.
New Phytol.
214
,
1078
1091
98
Bolhar-Nordenkampf
,
H.
,
Long
,
S.
,
Baker
,
N.
,
Oquist
,
G.
,
Schreiber
,
U.
and
Lechner
,
E.
(
1989
)
Chlorophyll fluorescence as a probe of the photosynthetic competence of leaves in the field: a review of current instrumentation
.
Funct. Ecol.
3
,
497
514
99
Meroni
,
M.
,
Rossini
,
M.
,
Guanter
,
L.
,
Alonso
,
L.
,
Rascher
,
U.
,
Colombo
,
R.
et al. (
2009
)
Remote sensing of solar-induced chlorophyll fluorescence: review of methods and applications
.
Remote Sensing Environ.
113
,
2037
2051
100
Yang
,
X.
,
Shi
,
H.
,
Stovall
,
A.
,
Guan
,
K.
,
Miao
,
G.
,
Zhang
,
Y.
et al. (
2018
)
Fluospec 2—an automated field spectroscopy system to monitor canopy solar-induced fluorescence
.
Sensors
18
,
2063
101
Miao
,
G.
,
Guan
,
K.
,
Yang
,
X.
,
Bernacchi
,
C.J.
,
Berry
,
J.A.
,
DeLucia
,
E.H.
et al. (
2018
)
Sun-induced chlorophyll fluorescence, photosynthesis, and light use efficiency of a soybean field from seasonally continuous measurements
.
J. Geophys. Res. Biogeosci.
123
,
610
623
102
Gu
,
L.
,
Wood
,
J.D.
,
Chang
,
C.Y.
,
Sun
,
Y.
and
Riggs
,
J.S.
(
2019
)
Advancing terrestrial ecosystem science with a novel automated measurement system for sun-induced chlorophyll fluorescence for integration with eddy covariance flux networks
.
J. Geophys. Res. Biogeosci.
124
,
127
146
103
Grossmann
,
K.
,
Frankenberg
,
C.
,
Magney
,
T.S.
,
Hurlock
,
S.C.
,
Seibt
,
U.
and
Stutz
,
J.
(
2018
)
Photospec: a new instrument to measure spatially distributed red and far-red solar-Induced chlorophyll fluorescence
.
Remote Sensing Environ.
216
,
311
327
104
Badgley
,
G.
,
Anderegg
,
L.D.
,
Berry
,
J.A.
and
Field
,
C.B.
(
2019
)
Terrestrial gross primary production: using NIRV to scale from site to globe
.
Glob. Change Biol.
25
,
3731
3740
105
Wu
,
G.
,
Guan
,
K.
,
Jiang
,
C.
,
Peng
,
B.
,
Kimm
,
H.
,
Chen
,
M.
et al. (
2020
)
Radiance-based NIRv as a proxy for GPP of corn and soybean
.
Environ. Res. Lett.
15
,
034009
106
Yang
,
X.
,
Tang
,
J.
,
Mustard
,
J.F.
,
Lee
,
J.-E.
,
Rossini
,
M.
,
Joiner
,
J.
et al. (
2015
)
Solar-induced chlorophyll fluorescence that correlates with canopy photosynthesis on diurnal and seasonal scales in a temperate deciduous forest
.
Geophys. Res. Lett.
42
,
2977
2987
107
Walther
,
S.
,
Voigt
,
M.
,
Thum
,
T.
,
Gonsamo
,
A.
,
Zhang
,
Y.
,
Köhler
,
P.
et al. (
2016
)
Satellite chlorophyll fluorescence measurements reveal large-scale decoupling of photosynthesis and greenness dynamics in boreal evergreen forests
.
Glob. Change Biol.
22
,
2979
2996
108
Zhou
,
H.
,
Wu
,
D.
and
Lin
,
Y.
(
2020
)
The relationship between solar-induced fluorescence and gross primary productivity under different growth conditions: global analysis using satellite and biogeochemical model data
.
Int. J. Remote Sensing
41
,
7660
7679
109
Verma
,
M.
,
Schimel
,
D.
,
Evans
,
B.
,
Frankenberg
,
C.
,
Beringer
,
J.
,
Drewry
,
D.T.
et al. (
2017
)
Effect of environmental conditions on the relationship between solar-induced fluorescence and gross primary productivity at an ozFlux grassland site
.
J. Geophys. Res. Biogeosci.
122
,
716
733
110
Frankenberg
,
C.
,
O'Dell
,
C.
,
Berry
,
J.
,
Guanter
,
L.
,
Joiner
,
J.
,
Köhler
,
P.
et al. (
2014
)
Prospects for chlorophyll fluorescence remote sensing from the orbiting carbon observatory-2
.
Remote Sensing Environ.
147
,
1
12
111
Lu
,
X.
,
Cheng
,
X.
,
Li
,
X.
and
Tang
,
J.
(
2018
)
Opportunities and challenges of applications of satellite-derived sun-induced fluorescence at relatively high spatial resolution
.
Science Tot. Environment.
619–620
,
649
653
112
Joiner
,
J.
,
Yoshida
,
Y.
,
Vasilkov
,
A.P.
,
Schaefer
,
K.
,
Jung
,
M.
,
Guanter
,
L.
et al. (
2014
)
The seasonal cycle of satellite chlorophyll fluorescence observations and its relationship to vegetation phenology and ecosystem atmosphere carbon exchange
.
Remote Sensing Environ.
152
,
375
391
113
Li
,
X.
and
Xiao
,
J.
(
2019
)
A global, 0.05-degree product of solar-induced chlorophyll fluorescence derived from OCO-2, MODIS, and reanalysis data
.
Remote Sensing.
11
,
517
114
Drusch
,
M.
,
Moreno
,
J.
,
Bello
,
U.D.
,
Franco
,
R.
,
Goulas
,
Y.
,
Huth
,
A.
et al. (
2017
)
The FLuorescence EXplorer mission concept—ESA's earth explorer 8
.
IEEE Trans. Geosci. Remote Sensing.
55
,
1273
1284
115
Taylor
,
T.E.
,
Eldering
,
A.
,
Merrelli
,
A.
,
Kiel
,
M.
,
Somkuti
,
P.
,
Cheng
,
C.
et al. (
2020
)
OCO-3 early mission operations and initial (vEarly) XCO2 and SIF retrievals
.
Remote Sensing Environ.
251
,
112032
116
Campioli
,
M.
,
Malhi
,
Y.
,
Vicca
,
S.
,
Luyssaert
,
S.
,
Papale
,
D.
,
Peñuelas
,
J.
et al. (
2016
)
Evaluating the convergence between eddy-covariance and biometric methods for assessing carbon budgets of forests
.
Nat. Commun.
7
,
13717
117
Isaac
,
P.
,
Cleverly
,
J.
,
McHugh
,
I.
,
Van Gorsel
,
E.
,
Ewenz
,
C.
and
Beringer
,
J.
(
2017
)
Ozflux data: network integration from collection to curation
.
Biogeosciences
14
,
2903
2928
118
Barr
,
A.G.
,
Richardson
,
A.D.
,
Hollinger
,
D.Y.
,
Papale
,
D.
,
Arain
,
M.A.
,
Black
,
T.A.
et al. (
2013
)
Use of change-point detection for friction–velocity threshold evaluation in eddy-covariance studies
.
Agric. Forest Meteorol.
171–172
,
31
45
119
McHugh
,
I.
,
Beringer
,
J.
,
Cunningham
,
S.
,
Baker
,
P.
,
Cavagnaro
,
T.
,
MacNally
,
R.
et al. (
2017
)
Interactions between nocturnal turbulent flux, storage and advection at and “ideal” eucalypt woodland site
.
Biogeosciences
14
,
3027
3050
120
Keith
,
H.
,
Leuning
,
R.
,
Jacobsen
,
K.L.
,
Cleugh
,
H.A.
,
van Gorsel
,
E.
,
Raison
,
R.J.
et al. (
2009
)
Multiple measurements constrain estimates of net carbon exchange by a eucalyptus forest
.
Agric. Forest Meteorol.
149
,
535
558
121
Hollinger
,
D.Y.
and
Richardson
,
A.D.
(
2005
)
Uncertainty in eddy covariance measurements and its application to physiological models
.
Tree Physiol.
25
,
873
885
122
Moffat
,
A.M.
,
Papale
,
D.
,
Reichstein
,
M.
,
Hollinger
,
D.Y.
,
Richardson
,
A.D.
,
Barr
,
A.G.
et al. (
2007
)
Comprehensive comparison of gap-filling techniques for eddy covariance net carbon fluxes
.
Agric. Forest Meteorol.
147
,
209
232
123
Falge
,
E.
,
Baldocchi
,
D.
,
Olson
,
R.
,
Anthoni
,
P.
,
Aubinet
,
M.
,
Bernhofer
,
C.
et al. (
2001
)
Gap filling strategies for defensible annual sums of net ecosystem exchange
.
Agric. Forest Meteorol.
107
,
43
69
124
Reichstein
,
M.
,
Falge
,
E.
,
Baldocchi
,
D.
,
Papale
,
D.
,
Aubinet
,
M.
,
Berbigier
,
P.
, et al. (
2005
)
On the separation of net ecosystem exchange into assimilation and ecosystem respiration: review and improved algorithm
.
Glob. Change Biol.
11
,
1424
1439

Author notes

*

Authors request that M.H. Siebers and N. Gomez-Casanovas be considered co-first authors.

This is an open access article published by Portland Press Limited on behalf of the Biochemical Society and the Royal Society of Biology and distributed under the Creative Commons Attribution License 4.0 (CC BY-NC-ND).