Abstract
Engineered living materials (ELMs) exhibit desirable characteristics of the living component, including growth and repair, and responsiveness to external stimuli. Escherichia coli (E. coli) are a promising constituent of ELMs because they are very tractable to genetic engineering, produce heterologous proteins readily, and grow exponentially. However, seasonal variation in ambient temperature presents a challenge in deploying ELMs outside of a laboratory environment because E. coli growth rate is impaired both below and above 37 °C. Here, a genetic circuit is developed that controls the expression of a light‐absorptive chromophore in response to changes in temperature. It is demonstrated that at temperatures below 36 °C, the engineered E. coli increase in pigmentation, causing an increase in sample temperature and growth rate above non‐pigmented counterparts in a model planar ELM. On the other hand, at above 36 °C, they decrease in pigmentation, protecting the growth compared to bacteria with temperature‐independent high pigmentation. Integrating the temperature‐responsive circuit into an ELM has the potential to improve living material performance by optimizing growth and protein production in the face of seasonal temperature changes.
Keywords: engineered living materials, synthetic biology, thermal control
Escherichia coli (E. coli) are a promising constituent of engineered living materials (ELMs), but growth slows below and above 37 °C. E. coli is engineered to enable temperature‐controlled expression of a light‐absorptive chromophore in a model planar ELM. When grown below 36 °C, the cells produce pigment, absorbing light and increasing in temperature and growth rate above a non‐pigmented strain. When grown above 36 °C, the ELM remains unpigmented, protecting growth compared to a strain with always‐on pigmentation.
1. Introduction
The field of engineered living materials (ELMs) aims to confer desirable properties of living cells and naturally‐occurring biomaterials to designed materials either by incorporating biological cells into a synthetic material, or through the formation of a material by living cells and their synthesized biopolymers.[ 1 , 2 , 3 ] These properties include self‐assembly, self‐healing, and sensing and responding to signals. In the last decade, engineering microbe‐derived or living building materials has become of particular interest to researchers because of the possibility of growing these materials in situ, using local resources, obviating the need to transport large amounts of material to remote environments.[ 4 , 5 , 6 ] Biomineralized living materials have the potential to comprise the structure of buildings, akin to cement blocks, or to form a protective surface coating, as in roofing shingles or tiles. The cells of microbial species including yeast,[ 7 ] cyanobacteria,[ 4 ] and Bacillus subtilis [ 8 , 9 , 10 , 11 , 12 ] have been used in ELMs, with Escherichia coli (E. coli) an especially common focus of ELM researchers[ 2 , 13 , 14 , 15 ] because of its extensive characterization and tractability for genetic engineering.[ 16 ]
While E. coli is a laboratory workhorse, it normally lives in the intestines of warm‐blooded animals, where the host maintains a stable temperature of ≈37 °C.[ 17 , 18 ] However, outside of the laboratory or intestinal environment, cells are exposed to fluctuations in temperature, nutrients, and moisture, all of which affect their viability and growth rate. Indeed, E. coli is known to live in freshwater and soil only in tropical ecosystems, which maintain an appropriate temperature, nutrient level, and humidity.[ 17 ] In the laboratory, the minimum temperature for the growth of E. coli is ≈7.5 °C in minimal media,[ 19 ] but even a decrease in temperature from 37 °C to 25 °C reduces the rate of growth of E. coli cultures in exponential phase by ≈38%.[ 20 ] The reduction in growth rate with temperature correlates with a reduced ability to synthesize protein. On the other hand, exposure to temperatures above 37 °C is also detrimental to E. coli, with growth inhibited above ≈44 °C, due to protein instability at high temperatures.[ 21 ] Thus, exposure to nonideal temperature limits the potential for outdoor environmental or exterior building materials applications for an ELM in which E. coli is a living component.
Here, we develop a genetic circuit that senses temperature and turns on the formation of a light‐absorptive pigment below 36 °C. We demonstrate that this circuit enables E. coli growing in dense patches under simulated sunlight to improve its growth rate over unpigmented E. coli at a suboptimal environmental temperature of 32 °C by capturing light and warming up. At the same time, when growing at 42 °C, an above‐optimal temperature, our engineered E. coli remains unpigmented and grows faster than bacteria with temperature‐independent pigmentation. We anticipate that this temperature switch circuit will confer a protective effect on E. coli in ELMs on a seasonal basis. During extended periods below 36 °C, the cells will produce pigment and improve growth throughout the cool season. However, they will stop producing pigment for the hot season, when light absorption becomes detrimental.
2. Results
E. coli within ELMs in outdoor applications, such as building exteriors, will be exposed to changes in ambient temperature, which will challenge their ability to grow and produce proteins of interest. For E. coli, the optimal growth temperature is 37 °C. We propose that when the ambient temperature drops below the optimum, the cells should produce a light‐absorptive pigment, allowing them to warm up when exposed to sunlight, whereas at or above the optimum, they should remain unpigmented, to avoid overheating (Figure 1a).
We repurposed a chemical compound designed to enable the use of β‐galactosidase as a gene reporter, 3,4‐cyclohexenoesculetin‐β‐d‐galactopyranoside (S‐gal), as our genetically‐encodable pigment (Figure 1b). S‐gal, which is yellow in solution, consists of galactose linked to 3,4‐cyclohexenoesculetin by a glycosidic bond. β‐galactosidase hydrolyzes this bond, which frees the esculetin group to complex with ferric iron (provided in the growth medium as ferric ammonium citrate, which is brown in solution) to form a black light‐absorptive pigment.[ 22 ]
We used the TlpA36 transcriptional repressor as a genetically‐encodable sensor with a temperature threshold of 36 °C[ 23 ] and constructed a gene circuit to invert its action, enabling E. coli to turn on enzymatic pigment production below 36 °C (Figure 1c). At these temperatures, TlpA36 represses expression of CI repressor from the PTlpA promoter. The LacZα peptide of β‐galactosidase, which presents a much lower metabolic burden to the cell than the complete enzyme, is expressed from the CI‐regulated PR‐PL tandem promoter. Above 36 °C, TlpA36 loses repressor function, so CI repressor is expressed from the PTlpA promoter and represses expression of LacZα. The concentration of CI repressor is tuned down by placing a weak terminator and weak ribosome binding site upstream. The complementary LacZω peptide is induced from the genome of E. coli DH10B by addition of isopropyl β‐d‐1‐thiogalactopyranoside (IPTG) to the growth medium; neither LacZα nor LacZω are enzymatically active on their own, but combine to form functional β‐galactosidase.[ 24 ] mWasabi (GFP) serves as a marker of high temperature.
We measured the optical density (OD) at visible light wavelengths of planktonic E. coli DH10B containing our temperature switch construct after growth in pigment induction media (containing S‐gal, ferric ammonium citrate, and IPTG) at temperatures ranging from 43.7 °C to 32.3 °C (Figure 1d,e; Figure S3, Supporting Information). Cultures of E. coli containing the temperature switch construct increase in optical density across the visible light spectrum from 400 – 700 nm below 35.9 °C, compared to at and above 35.9 °C. In comparison, cultures of E. coli containing a pigmented control construct (Tables S1 and S2 and Figure S1, Supporting Information) exhibit high optical density across the visible light spectrum from 32.3 °C through 42.9 °C, with a decrease at the highest temperature of 43.7 °C (Figures S2 and S3, Supporting Information). These measurements include both the absorbance of light by the pigment (if present) and the scattering of light due to the presence of cells, as both would contribute to heat transfer with illumination. The OD600 of cultures of E. coli grown at temperatures in this range is maximal at 37–38 °C (Figure S4, Supporting Information). Extracellular pigment in filtered media shows higher optical density across the visible light spectrum than filtered media containing S‐gal and ferric ammonium citrate (Figure S5, Supporting Information).
After constructing the temperature switch for expression of pigment below 36 °C and demonstrating its function in liquid culture, we grew E. coli containing the construct in a dense, centimeter‐scale patch format to simulate the environment of an ELM. We suction‐coated a suspension of cells grown to saturation overnight at 38 °C onto a polycarbonate membrane backing and placed it on a media‐saturated melamine foam growth substrate (Figure 2a). We placed the samples in a home‐built illuminated growth chamber and monitored the relative temperature of the samples compared to the melamine foam using a lightweight 32 × 24 thermal IR sensor array (Figure 2b). The LED light source was placed at a distance of 120 mm from the samples to achieve an average light flux of 120 000 lx, slightly higher than direct sunlight. Between the light source and the samples, we placed a 3.175 mm sheet of glass to filter IR and a 1.5 mm sheet of colorless, transparent acrylic to filter UV, while allowing visible light illumination of the samples. We placed the thermal IR sensor array on a motorized arm that retracts when not imaging to avoid casting a shadow. After 48 h growth in illuminated conditions at 42 °C, patches of E. coli containing our temperature switch construct produce little pigment, whereas, at 32 °C, they become nearly opaque when imaged with white light transillumination (Figure 2c; Figure S10, Supporting Information). Because the melamine foam is opaque in transillumination, we transferred the patches of E. coli on their polycarbonate membranes to LB agar plates for imaging.
We tested the ability to turn on pigmentation to confer protection against slowed growth at 32 °C with and without illumination by comparing the growth rate of E. coli containing our temperature switch construct against the growth rate of E. coli containing a control construct encoding mWasabi under the control of TlpA36[ 23 ] (unpigmented control). While patches containing our temperature switch construct express pigment at this temperature, the control patches have no mechanism for pigment production and remain translucent (Figure 3a; Figures S8 and S9, Supporting Information). Due to the low spatial resolution of the sensor array, the precise temperature of the samples cannot be determined; however, the pigmented patches clearly warm above the background temperature (Figure 3b).
We monitored the growth of the patches via their thickness, quantified from optical coherence tomography cross‐sectional images, and their area, quantified from white light transillumination images. With illumination, the patches containing the temperature switch construct grow to twice the thickness of patches containing the control construct over the course of 72 h (Figure 3c–e; Figure S6a,b, Supporting Information), whereas without illumination, the patches grow to the same thickness at each timepoint (Figure 3f; Figure S6c,d, Supporting Information). In addition, with illumination, the temperature switch allows the patches to grow in area linearly with time, while the rate of increase in area of unpigmented patches slows over time (Figure 3g, Figure S7a, Supporting Information). On the other hand, without illumination, patches containing both constructs grow in area linearly at approximately the same rate (Figure 3h; Figure S7b, Supporting Information). Due to lower humidity in the home‐built illuminated growth chamber than in the incubator used for growth without illumination, the amount of growth with and without illumination cannot be directly compared. However, our results suggest that expressing pigment at 32 °C using the temperature switch construct gives E. coli in a dense patch format a growth advantage under illumination compared with unpigmented patches.
While pigmentation is advantageous at below‐optimal ambient temperatures, we hypothesized that it would be deleterious at above‐optimal temperatures by exacerbating overheating. To test this hypothesis, we compared the growth at 42 °C of patches of E. coli containing our temperature switch construct against the growth rate of E. coli containing a control construct encoding IPTG‐inducible LacZα (pigmented control). We supplemented the media with 0.1% d‐glucose to catabolically repress[ 25 ] the expression of LacZω (and hence, the formation of pigment) during sample preparation at room temperature and while the samples equilibrated to 42 °C. After 48 h, the patches containing our temperature switch construct lack pigmentation and appear translucent, while the control patches turn black and opaque, warming above the background temperature (Figure 4a,b).
To avoid exposing the samples to laboratory room temperatures of 16 – 25 °C by handling them during the experiment, we measured the area and thickness of the patches only at the endpoint of 48 h. The area of the patches containing the temperature switch compared with the patches containing the pigmented control showed no statistical difference either with or without illumination (Figure S12, Supporting Information). However, the patches containing the temperature switch were thicker than the patches containing the control construct under illumination (Figure 4c–e, Figure S11a, Supporting Information). Without illumination, the patch thickness was not statistically different (p = 0.1214), although there was a trend toward greater thickness for the switch, potentially due to the burden of protein overexpression from the IPTG‐induced control construct (Figure 4f, Figure S11b, Supporting Information). Thus, turning off expression of pigment at 42 °C using the temperature switch construct confers an advantage on E. coli in a dense patch format grown under illumination compared with temperature‐independent, chemically‐induced pigmentation.
3. Discussion
This work establishes a proof of concept for a genetically‐encoded mechanism for supporting E. coli in an ELM under non‐optimal ambient temperature. We demonstrated a genetic circuit for expression of a dark, light‐absorptive pigment below 36 °C. At 32 °C, dense patches of E. coli containing this circuit become nearly opaque with black pigment, allowing them to warm above background and grow in both area and thickness at a greater rate than unpigmented patches. Conversely, at 42 °C, patches remain translucent, avoiding further overheating and growing to a greater thickness than chemically‐induced pigmented patches. Because E.coli‐based ELMs rely on E. coli growth and protein production to form the material, as well as confer engineered properties, such as environmental sensing, to the material, long‐term exposure to temperatures below or above 37 °C will be detrimental to their function. Our temperature switch genetic construct is in principle compatible with any cloning strain of E. coli with the lacZΔM15 genotype, allowing it to be used in existing E. coli‐based ELMs, such as biomineralized E. coli biofilms.[ 26 , 27 ]
While this study provides a proof of concept for temperature self‐regulation, additional work is needed to improve the kinetics of the temperature switch. Because our system does not include a mechanism for degradation of the pigment complex, even brief low‐temperature excursions allow pigment to accumulate in the ELM. While protective in the case of long‐term exposure to low temperatures, this could cause overheating once the ambient temperature reaches 37 °C or above.
To avoid producing pigment at night in climates or seasons where day‐time temperatures exceed 37 °C, but night‐time temperatures drop below, our circuit could be modified to incorporate a light sensor, such as phytochrome,[ 30 ] using an AND gate,[ 31 ] turning on pigment production only with both light and cold temperature. In addition, to accelerate the transition from dark to translucent in response to a change in environment from low to high temperature, an enzyme cassette for biodegradation of the esculetin‐based pigment could be developed from coumarin degradation pathways found in soil bacteria.[ 32 ] To increase protection from heat, this degradation cassette, or a cassette encoding light‐scattering proteins such as gas vesicles,[ 33 , 34 ] could be turned on at high temperature in place of the GFP marker currently incorporated in our construct, clearing pigment from the ELM or scattering incoming light.
Finally, the S‐gal‐derived black pigment used in our system is deposited extracellularly (Figure S13, Supporting Information). Additionally, a possible alternative light‐absorptive pigment, eumelanin, can be produced extracellularly by E. coli via expression of tyrosinase.[ 35 , 36 ] Tyrosinase oxidizes tyrosine intracellularly, but polymerization of eumelanin is completed outside the cell. For both S‐gal‐derived pigment and eumelanin, pigment degradation enzymes thus need to be exported outside the cell to remove the pigment. However, it may be possible for future mechanisms for ELM media exchange – bringing fresh nutrients to the ELM and removing waste – to also wash away pigment. In this scenario, the pigment would be replaced only when it is needed, during periods of cool temperature. With our thermal bioswitch circuits and these future improvements, ELMs will gain the ability to harness sunlight to keep warm or stay cool in the face of seasonal temperature changes.
4. Experimental Section
Plasmid Construction and Molecular Biology
All plasmids were designed using SnapGene (GSL Biotech) and assembled via reagents from New England Biolabs for KLD mutagenesis (E0554S) or HiFi Assembly (E2621L). After assembly, constructs were transformed into NEB Turbo (C2984I) E. coli for growth and plasmid preparation. Integrated DNA Technologies synthesized all PCR primers. TlpA36 and mWasabi[ 37 ] (GFP) were obtained from our previous work.[ 23 ] LacZα was tagged at the C‐terminus with the AAV ssrA tag[ 38 ] (amino acid sequence AANDENYAAAV). The weak terminator in the temperature switch construct is Part:BBa_B1002.[ 39 ] The weak RBS in the temperature switch construct is RBSF.[ 40 ] Plasmids were transformed into DH10B E. coli (ThermoFisher) for downstream experiments. Gene circuit diagrams were created using the DNAplotlib[ 41 ] library in Python.
Visible Light Absorbance Assays
1 mL cultures of LB medium (Sigma) with 100 µg mL−1 ampicillin were inoculated with a single colony per culture and grown at 38 °C, 250 rpm for 18.5 h. 30 µL were diluted into 2 mL LB with 300 µg mL−1 3,4‐cyclohexenoesculetin‐β‐d‐galactopyranoside (S‐gal) (Sigma), 500 µg mL−1 ferric ammonium citrate (Sigma), 100 µM IPTG, 100 µg mL−1 ampicillin and propagated at 38 °C, 250 rpm for 90 min. The cultures were dispensed in 100 µL aliquots into 8‐well PCR strips (Bio‐Rad) and incubated for 24 h in a thermal gradient using a DNA Engine Tetrad 2 Peltier Thermal Cycler (Bio‐Rad) with the lid set to 50 °C. PCR strips were imaged using a ChemiDoc MP Gel Imaging System (Bio‐Rad). Contrast was adjusted using ImageJ software.[ 42 ] 90 µL were transferred into 96‐well plates (Corning 3631) and absorbance spectra were measured using a Spark multi‐mode microplate reader (Tecan). Data analysis was performed using custom Python scripts.
Preparation of Dense Patches of E. coli
Cultures of LB medium (2 mL) (Sigma) with 100 µg mL−1 ampicillin (and 25 µM IPTG for pigmented controls) were inoculated with a single colony per culture and grown at 38 °C, 250 rpm for 18.5 h. Nalgene Rapid‐Flow sterile disposable filter units (cellulose nitrate, 75 mm diameter, 0.2 µm pore size) (ThermoFisher 450‐0020) were rinsed with 1x PBS (Corning) and track‐etched polycarbonate membranes (25 mm diameter, 0.2 µm pore size) (Sartorius 23007 unless Whatman Nuclepore 10417006 is indicated) were placed on the filter surface. 200 µL bacterial culture was dispensed onto each membrane and a vacuum was applied to the filter unit to coat the cells onto the membrane. E. coli containing the temperature switch construct and the unpigmented control construct express mWasabi after the overnight growth at 38 °C, so the freshly prepared membranes were imaged in epifluorescence using a ChemiDoc MP Gel Imaging System (Bio‐Rad) to confirm that the E. coli were coated onto the membranes. The thickness of the freshly prepared patches was below the axial resolution of the optical coherence tomography system and the freshly prepared patches were undetectable using transillumination white light imaging.
Growth of E. coli Patches in ELM‐like Conditions
LB medium (90 mL (32 °C experiments) or 100 mL (42 °C experiments)) (Sigma) with 75 µg mL−1 S‐gal, 125 µg mL−1 ferric ammonium citrate, 25 µM IPTG, 100 µg mL−1 ampicillin (and 0.1% d‐glucose for 42 °C experiments) was added to ≈0.7 g melamine foam (Amazon) in a petri dish until foam was saturated. For 42 °C experiments, the saturated foam was prewarmed using a heat lamp. Patches of E. coli coated on polycarbonate membranes were placed onto the surface of the saturated foam. Patches were incubated either in a custom illuminated incubator or in a conventional incubator for 72 h (32 °C experiments) or 48 h (42 °C experiments). At 24 h intervals, Petri dishes were weighed to determine the amount of evaporation and the equivalent volume of LB with 75 µg mL−1 S‐gal, 125 µg mL−1 ferric ammonium citrate, 25 µM IPTG, 100 µg mL−1 ampicillin (and 0.1% d‐glucose for 42°C experiments) at room temperature (for 32 °C experiments) or prewarmed to 42 °C (for 42 °C experiments) was added.
Design and Construction of Illuminated Incubator with In Situ Temperature Monitoring
The enclosure of the illuminated incubator was a 203.2 mm × 254 mm × 180.34 mm aluminum box with a lid consisting of a 3.175 mm layer of glass (IR‐filtering) and a 1.5 mm layer of acrylic (UV‐filtering) held in a 3D‐printed polylactic acid (PLA) collar. The weatherproofing foam was used to provide a tight fit between the lid and the box. The sample holder was located 120 mm from the 100 W LED grid light source (Mifxion), receiving an average light flux of 120 000 lx. The light source was plugged into a power relay (Digital Loggers). The light source heats the interior of the chamber; the temperature was adjusted by adding or removing insulation.
An MLX90640 32 × 24 thermal IR sensor array (Grove or Adafruit) was attached to an SG92R micro servo motor (Tower Pro) via 3D‐printed PLA fittings reinforced with wooden craft sticks for monitoring the samples. MCP9808 temperature sensors (Adafruit) were used to monitor the air temperature inside and outside the sample enclosure. All sensors, the servo motor, and the power relay were connected to a Feather M4 Express microcontroller (Adafruit) for data acquisition and control. A custom Bokeh application was used to interface with the microcontroller.
For comparison, E. coli patches were grown without illumination using a conventional incubator, as turning off the light source or shading the samples in the illuminated growth chamber would result in lowering the ambient temperature.
Imaging and Analysis of E. coli Patches
E. coli patches on polycarbonate membranes were transferred from melamine foam growth substrate to 20 mL PBS agar plates for imaging.
White light transillumination imaging was performed using a ChemiDoc MP Gel Imaging System (Bio‐Rad). E. coli patch area was measured by using the Canny edge detector algorithm for image segmentation to find the edges of each patch, counting the number of pixels within each patch, and converting to area in square millimeters. In addition, pixel intensity was quantified (normalized to polycarbonate membrane background and opaque black plastic) and averaged. Analysis was performed via custom Python scripts.
Optical coherence tomography was performed using a Ganymede 210 Series Spectral Domain OCT Imaging System with an OCTP‐900 scanner and 8 µm lateral resolution scan lens (Thorlabs). Cross‐sectional images with a 10 mm / 2560 pixel (x) by 1 mm / 491 pixels (z) field of view were acquired at a 5.5 kHz A‐scan rate with 7 B‐scan averages and 5 A‐scan averages per acquisition. The despeckle filter in the ThorImageOCT software (Thorlabs) was applied before exporting. E. coli patch thickness was measured using a custom Python script. Briefly, after applying a Gaussian filter, the three narrowest peaks with height and width fulfilling adjustable thresholds were detected in each column and arranged by distance from the top of the image to correspond with the top of the patch, the top of the polycarbonate membrane, and the bottom of the polycarbonate membrane. The vectors for each interface were Hampel filtered to reduce outliers due to imaging artifacts. The thickness was defined as the distance from the top of the patch to the top of the polycarbonate membrane. The mean thickness and standard deviation of each patch between x = 3.5 mm and x = 9.0 mm (avoiding the edges of the patch) were calculated. Then, the mean for each construct, illumination condition, and temperature was calculated, propagating the standard deviation to calculate the standard error of the mean.
Statistical Analysis
Continuous variables were expressed as mean +/‐ standard error of the mean. The sample size was n = 4 biological replicates. Plasmid for each genetic circuit construct was transformed into E. coli and colonies were cultured on agar plates; each biological replicate was a bacterial culture derived from a single colony. Groups (e.g., pigmented control samples versus temperature switch samples) were compared using a two‐tailed unpaired t‐test. Statistical significance was defined as p ≤ 0.05. Statistical analysis was performed using the Python SciPy Stats package.
Conflict of Interest
The authors declare no conflict of interest.
Author Contributions
L.L.X. and M.G.S. conceived the study. L.L.X. and M.A.G. planned and performed experiments. L.L.X. analyzed data. J.A.K. provided input on research design and data interpretation. L.L.X. and M.G.S. wrote the manuscript with input from all other authors. M.G.S. and J.A.K. supervised the research.
Supporting information
Acknowledgements
The authors thank Hanwei Liu, David Tirrell, Priya Chittur, Seunghyun Sim, and Jolena Jie Zhou for helpful discussions about engineered living materials, as well as Red Lhota, Robert Learsch, and Justin Bois for assistance with instrument design. This research was supported by the Defense Advanced Research Project Agency (HR0011‐17‐2‐0037 to M.G.S. and J.A.K.), the Institute for Collaborative Biotechnologies (W911NF‐19‐D‐0001 to M.G.S.), the Jacobs Institute for Molecular Engineering for Medicine (to J.A.K.), and the Elizabeth W. Gilloon Chair (to J.A.K.). L.L.X. was supported by the NSF Graduate Research Fellowship Program. M.A.G. was supported by the NIH MBRS Research Initiative for Scientific Enhancement Program. M.G.S. was an Investigator at the Howard Hughes Medical Institute. Related research in the Shapiro lab was supported by the David and Lucile Packard Foundation and the Dreyfus Foundation.
Xiong L. L., Garrett M. A., Kornfield J. A., Shapiro M. G., Living Material with Temperature‐Dependent Light Absorption. Adv. Sci. 2023, 10, 2301730. 10.1002/advs.202301730
Contributor Information
Julia A. Kornfield, Email: jak@cheme.caltech.edu.
Mikhail G. Shapiro, Email: mikhail@caltech.edu.
Data Availability Statement
The data that support the findings of this study are available from the corresponding author upon reasonable request.
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Data Availability Statement
The data that support the findings of this study are available from the corresponding author upon reasonable request.