Md Arifur Rahman
Khan
a,
Swapna
Kalkar
a,
Besan
Khader
a,
Olubunmi O.
Ayodele
a,
Aleksandrs
Prokofjevs
*b and
Tetyana
Ignatova
*a
aDepartment of Nanoscience, Joint School of Nanoscience and Nanoengineering, University of North Carolina at Greensboro, NC, USA. E-mail: t_ignato@uncg.edu
bDepartment of Chemistry, North Carolina Agricultural and Technical State University, NC, USA. E-mail: aprokofjevs@ncat.edu
First published on 18th August 2025
Current methods for transferring 2D materials typically rely on non-biodegradable support polymers, which have a detrimental impact on the environment due to the extensive use of solvents required for polymer removal and the introduction of transfer-induced defects. In this study, we present an approach for synthesizing a biodegradable polyester, poly-angelica lactone (PAL) derived from bio-based raw materials, angelica lactone (α-AL). The biodegradability of the synthesized PAL is activated through a specific mechanism, which has been validated by FTIR and 1H NMR. The molecular weight and thermal properties of PAL have been characterized using GPC and DSC techniques, respectively. We employed PAL as a support layer for the transfer of 2D materials, such as graphene, demonstrating that the removal of PAL requires less than 30 min. The transferred graphene exhibited superior quality compared to conventional PMMA-based methods, with induced strain and doping levels maintained well below ±0.5% and 0.5 × 1012 e cm−2, respectively. Remarkably, the PAL support layer can be efficiently removed from graphene films using a fungus (e.g. yeast). This innovative approach not only emphasizes the eco-friendly nature of the process but also highlights its potential for enabling sustainable and efficient 2D materials transfer, paving the way for greener nanodevice fabrication methods.
The CVD process requires an appropriate growth surface, such as Cu or Ni, on which the graphene film is grown. Subsequently, the graphene film is carefully transferred onto an application-specific target substrate,23 which could be SiO2/Si,24 glass,25 paper,26 or flexible polymers.27 Transfer of CVD-grown graphene and other 2D materials is greatly facilitated using sacrificial polymer support. Historically, poly(methyl methacrylate) (PMMA) has held a predominant position as the preferred temporary supporting material for transferring 2D materials in device fabrication.28 PMMA has proven to be effective in transferring large-scale, high-quality 2D materials,29 and has also been widely used as resist in lithography process, including e-beam lithography.30 Currently, there is no viable substitute for PMMA in industrial-scale production, underscoring its value in established processes.
Current research efforts seek to assess alternative transfer support materials,31–33 such as polystyrene,34 polycarbonate,35 paraffin,36 and polymer blend,33 to ensure the high quality of transferred films.36–44 The quest for alternative transfer materials and techniques mandates addressing potential sample contamination by residual components of the polymeric substrate.45–47 Notably, most of the polymers used in this sector, including the widely used PMMA, fall under the category of non-biodegradable materials. Furthermore, substantial amounts of solvent waste generated during fabrication may carry significant environmental implications. In the realm of contemporary technological challenges, one prominent issue revolves around the compatibility of biodegradable materials within industrial settings, ensuring that they effectively serve their intended production purposes.
Poly-angelica lactone (PAL) synthesized from levulinic acid (LA), are considered an excellent potential substitute for currently used polymers (e.g., PMMA) in 2D materials transfer. LA is a highly desirable biobased chemical intermediate.48 Dehydration of LA causes intramolecular condensation, leading to the formation of the readily polymerizable α-angelica lactone (α-AL, 5-methyl-2(3H)furanone), a valuable intermediate in the synthesis of commodity chemicals.49,50 Interestingly, the biodegradability of α-AL polymers varies depending on the polymerization conditions. This stems from the fact that the α-AL monomer possesses two different reactive functional groups relevant for polymerization: the α,β-unsaturated ester, and the lactone. Polymerization involving the CC bond of the unsaturated ester moiety leads to the formation of the polyolefin chain decorated by lactone units and their derivatives and can be effected using BF3·Et2O catalyst (product Mw ∼ 800–900 g mol−1) or UV light.51,52 The lack of reactive functional groups in the resulting polyolefin backbone makes it resistant to biodegradation.51
In contrast, ring-opening polymerization (ROP) involving the lactone subunit leads to the formation of a biodegradable polyester product containing intact CC bonds (Fig. 1).51,53–56 This type of polymerization is induced by more selective transesterification catalysts, such as sodium hydroxide (Mw ∼ 840 g mol−1), sodium n-butoxide (Mw ∼ 1120 g mol−1) or stannous octoate (Mn ∼ 30
000 g mol−1).51,53
In this study, we demonstrate that biodegradable α-AL polyesters can successfully replace non-biodegradable polymers in nanomanufacturing, i.e., in the fabrication of 2D devices, which brings substantial environmental benefits in their mass production. To this end, we developed a straightforward procedure for synthesizing α-AL polyesters using a minimal amount (1 mol%) of sodium tert-butoxide as the catalyst. The resulting biodegradable polymer product exhibited excellent performance in the transfer of 2D materials, such as graphene and MoS2, onto the target substrate, SiO2/Si. To demonstrate this, we comprehensively explored transfer conditions employing our biodegradable polymer as the supporting medium. Specifically, we optimized key process parameters in etching and hydrogen bubbling, which are widely recognized for their effectiveness in transferring large, high-quality graphene films. While testing the biodegradability of our samples, we discovered that the polymeric support can be completely digested by yeast, leaving behind pristine graphene films. This remarkable finding not only underscores the eco-friendly nature of our approach but also showcases its potential for developing conceptually new and highly efficient 2D material transfer processes limited solely to biodegradable polymers.
Reaction time and catalyst loading significantly impacted the properties of the resulting polymer. The optimum sodium tert-butoxide loading was around 1 mol%, while increasing the catalyst loading to 5 mol% led to poor reaction control and difficulties in product isolation. Longer reaction times were observed to deliver higher molecular-weight polyester samples. Consequently, the optimized procedure employs a combination of low catalyst loadings and long reaction times.
To remove water-soluble residues, the crude polymer was washed with 10–20 portions of DI water until the aqueous layer remained clear. Volatile contaminants were removed by dissolving the material in a 70:
30 acetone
:
methanol mixture, followed by concentration and drying under reduced pressure at 60 °C for 18 h. Low molecular weight residues were eliminated by dissolving the material in ethyl acetate, followed by selective precipitation of the higher molecular weight fraction by dropwise addition of hexanes. This process also markedly improved the visual appearance of the polymeric material, delivering white or pale-yellow precipitates when a favorable ethyl acetate
:
hexanes ratio was applied. The purified polymer was finally dried under reduced pressure for 6 hours before characterization and application in graphene transfer. The PAL product is highly soluble in acetone, ethyl acetate and dichloromethane (DCM), partially soluble in methanol and isopropanol, and nearly insoluble in hexanes and water.
Sample | M w (g mol−1) | M n (g mol−1) | PDI | |
---|---|---|---|---|
PAL-1d | Crude | 466 | 341 | 1.37 |
Purified | 573 | 420 | 1.36 | |
PAL-14d | Crude, peak 1 | 290 | 277 | 1.05 |
Crude, peak 2 | 920 | 757 | 1.22 | |
Purified | 1490 | 1007 | 1.48 |
After 1 day (24 hours) reaction time, the molecular weights of the crude PAL-1d product are low (Mw 466 g mol−1, Mn 341 g mol−1), although the molar-mass dispersity (PDI) of 1.37 is typical for chain-growth ring opening polymerization.53,57 Dissolving the crude PAL-1d reaction product in ethyl acetate followed by precipitation with hexanes resulted in a slight increase of the molecular weights (Mw 573 g mol−1, Mn 420 g mol−1), leaving the PDI virtually unchanged (1.36). For this sample, the effect of the reprecipitation was primarily to remove monomer residues, which could not be properly quantified using our GPC setup.
Extending the reaction time to 14 days resulted in a noticeable increase in the polymer chain length (PAL-14d). The GPC analysis of the crude product showed bimodal molecular weight distribution, with the higher molecular weight peak (peak 2 in Table 1) having nearly double Mw value compared to that of the PAL-1d product. To isolate the highest molecular weight fraction from the crude PAL-14d product, the material was dissolved in ethyl acetate and subsequently precipitated with hexanes, as described above. This procedure delivered a sample with Mw 1490 g mol−1 and Mn 1007 g mol−1, entirely eliminating the low molecular weight fraction from the purified material. While the purified PAL-14d polymer sample showed a slightly increased PDI value of 1.48, it should be stressed that it is lower than the PDI of 1.8 observed for comparable molecular weight PAL samples reported in ref. 51, and considerably smaller than values seen in commercial polymers.58
The purified polymers PAL-1d and PAL-14d were further characterized by FTIR and 1H NMR spectroscopies. Overall, the spectroscopic data is consistent with the expected formation of the polyester backbone and with previous reports on α-AL ring-opening polymerization.53 Thus, a comparison of the polymer FTIR spectra with that of the α-AL monomer reveals the presence of the intact CC double bond in the polymers, as well as the expected presence of the C
O groups (Fig. 2a, b; ESI Fig. S2†).
The 1H NMR analysis, however, revealed considerable differences between the previously reported α-AL polyesters and the material prepared in this study (Fig. 3 and ESI Fig. S3†). While both PAL-1d and PAL-14d contain polyester products of the ring-opening polymerization beyond any reasonable doubt, the 1H NMR spectra suggest that the CC bonds of the product are mostly α,β-conjugated to the ester carbonyl groups. This suggests isomerization of the non-conjugated β,γ-unsaturated ester moiety in the α-AL to the more thermodynamically stable α,β-conjugated form under strongly basic reaction conditions. Furthermore, we also observed the presence of aliphatic fragments reminiscent of the β-AL oligomers produced in the presence of frustrated Lewis pairs.59 These fragments were also present in the precipitation supernatant obtained upon treatment of the polymer (ESI Fig. S4†). A cautious interpretation of the spectroscopic and GPC data thus suggests that both PAL-1d and PAL-14d samples are low molecular weight AL polyester oligomers that have undergone considerable isomerization to the α,β-unsaturated products while also containing a considerable fraction of the C–C linked AL units.
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Fig. 3 1H NMR spectra of (a) PAL-14d and (b) α-AL containing ca. 15% of the β-isomer. Note that the PAL-14d spectrum contains broad features (labeled with *) consistent with the previously reported angelica lactone polyesters,53 and sharp peaks apparently stemming from the previously reported β-AL dimer.59 Also note that the alkene proton peaks in PAL-14d appear in the same region as the conjugated alkene protons of the β-AL, suggesting considerable double bond migration under basic conditions. A broad peak around 12.2 ppm (not shown) in the PAL-14d spectrum suggests presence of COOH groups. |
Differential Scanning Calorimetry (DSC) analysis of PAL-1d revealed significant information regarding the thermal behavior of the polymer, as depicted by the heat flow vs. temperature plot in Fig. 2c. The experiment was performed in an inert nitrogen atmosphere in the temperature range of −30 °C to 200 °C. The amorphous nature of the polymer can be assumed by observing the wide range of glass transition temperature (Tg) from −6 °C to 70 °C. Additionally, the DSC curve indicates a unique degradation temperature of the polymer at 113 °C, which might be the melting point. At this stage, the polymer degrades to a phase with a fundamentally different thermal behavior than the initial phase. This crucial insight into the thermal property of the polymer allowed us to optimize the post-transfer heating temperature involved in the graphene transfer method.
The graphene transfer technique using PAL is straightforward as done conventionally, though several steps need to be optimized for a successful transfer. As-purchased CVD-grown graphene was spin coated in two steps by 75 wt% PAL solution in acetone. The spin coating was first performed at 400 rpm for 15 seconds, followed by drying on a hot plate at 70 °C for 30 minutes. The sample was then re-coated at 2000 rpm for 45 seconds, followed by drying at room temperature for 24 hours. The Cu substrate underneath the PAL/graphene was etched away with 0.5 M aqueous FeCl3 solution or delaminated using the hydrogen bubbling method. When using the hydrogen bubbling method, the NaOH solution (25 mM) utilized was 4 times more dilute than what is commonly used in our lab for PMMA-coated graphene transfers.
For both transfer techniques, the PAL/graphene sheet was subsequently washed 3 times in DI water, then scooped onto a desired substrate (SiO2/Si). The post-transfer heat treatment was done at 60 °C for 25 minutes to remove water trapped between the new substrate and PAL/graphene. The PAL coating was then removed by immersing the PAL/graphene/substrate composite into reagent-grade acetone for 20 minutes, followed by washing with isopropanol, cleaning with DI water, and purging with N2 gas. The result of this protocol is a layer of graphene deposited onto SiO2/Si substrate.
Unpurified PAL-1d was unsuitable for the bubbling method as the polymer film was breaking down under tension introduced during hydrogen bubble formation. Nevertheless, it proved successful for graphene transfer with the etching method (ESI Fig. S5†), although this method requires additional cleaning of the graphene to remove etchant residues. The bubbling method is generally more popular than etching because it is performed in DI water, improving cleanliness of the transfer. Unpurified PAL-14d was more suitable for the bubbling method, providing good quality graphene transfers that required only 20 minutes immersion of the sample in acetone for polymer removal (ESI Fig. S5†). To test whether insufficient mechanical strength of the unpurified PAL-1d films stems from low molecular-weight contaminants, graphene transfer experiments were repeated using PAL-1d purified by reprecipitation as described above. Noticeably, purified PAL-1d was able to sustain the hydrogen bubble pressure better than the crude polymer, resulting in a good quality graphene monolayer transfer by the bubbling method. Fig. 4 shows SEM images of graphene transferred using purified PAL-1d. Fig. 4a shows a large graphene area (approximately 80 μm × 80 μm) with minimal amounts of residual polymer. It is worth mentioning that edges of the transferred graphene are free from polymer residues and folding that is usually experienced in traditional transfer. Fig. 4b provides a more detailed illustration of the transfer quality at an approximate area of 16 μm × 16 μm. This area reveals high quality transfer with very few wrinkles and microcracks, and almost no residual polymer (hardly one or two spots). Several wrinkles and bi- or tri-layer of graphene are visible that can be formed during either the CVD growth67 or transfer processes.68 Transfer-related multilayers are usually formed near the cracks or edges by a folding mechanism with an irregular shape and no geometrical orientation, as the surroundings are extremely variable. Here, we see that the multilayer (bi- or tri-layer) is formed on the top of the perfect monolayer, exhibiting a homogenous geometry. This kind of formation is only probable if the sample is experienced with a homogenous environment, as is possible in the controlled surroundings of the CVD growth process. Thus, we attribute this bi-, or tri-layer formation to the CVD growth process and not to the transfer procedure. It is worth mentioning that polymer removal in our process is complete in under 30 minutes, while conventional PMMA-based transfers often require 3 to 5 hours.45,69 Additionally, the new procedure is more straightforward compared to the traditional transfer which requires additional steps for polymer removal.33,45,70
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Fig. 4 SEM images of graphene. Transferred by hydrogen bubbling method with clean PAL-1d support (magnification: (a) 1k and (b) 5k). |
In the analyzed area, the G and 2D Raman bands of graphene appeared around 1584.15 cm−1 and 2676.17 cm−1, respectively (Fig. 5b). The D Raman band of graphene emerged only at multilayer and wrinkle regions, with ID/IG ratios of 0.16 and 0.21, respectively (Fig. 5b and c). The I2D/IG intensity ratio was 1.29 for the multilayer and 2.41 for the wrinkle regions, compared to 2.53 for the monolayer. Additionally, the 2D peak exhibited a blue shift to 2687.74 cm−1 at the multilayer region, while its FWHM broadened to 37.48 cm−1, compared to 32.85 cm−1 for the monolayer.
The frequency correlation plot of the G and 2D bands is a reliable technique for evaluating strain and doping in transferred graphene.10,33,45,71,72 We analyzed and plotted approximately 3600 data points, as shown in Fig. 6a. The solid blue line corresponds to the 2.2 slope line axis for uniaxial (hydrostatic) strain, as reported in ref. 10, 73 and 74. The green solid line with a slope of 0.55 represents the hole doping axis, which follows a quasi-linearity between the G and 2D frequencies, as reported in ref. 75.
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Fig. 6 Frequency correlation plot of G and 2D Raman modes (a). Yoon et al.'s work76 was used to calculate the uniaxial strain-sensitivity of the G mode, which was derived as ΔωG/Δωε = −23.5 cm−1/%. Shifting of the 2D peak at a rate of 1.04 cm−1 per 1 × 1012 e cm−2 hole density has been used for parameterizing the p doping axis as reported in ref. 77. FWHM distribution of 2D peak (b) and G peak (c), intensity ratio of ID/IG (d) and I2D/IG (e). |
The black star (ωG0 = 1583 cm−1, ω2D0 = 2678 cm−1) in Fig. 6a corresponds to the G and 2D peak position for strain-free and undoped suspended graphene sample,78 representing an ideal situation. Our analysis revealed that the PAL-transferred graphene film experiences a slight strain and very weak p-doping, as the fitted data align along the 2.2 slope line (Fig. 6a). Although these data points are distributed over both tensile and compressive strain regions, the overall strain level remains below 0.1%. The calculated p-doping concentration is minimal, less than 1 × 1012 e·cm−2, as clearly observed in Fig. 6a. Moreover, the already mentioned I2D/IG intensity ratio can be used to evaluate doping in graphene, as p-doping increases the G peak intensity, the 2D peak intensity decreases.78–80 The distribution of the I2D/IG ratio in Fig. 6e shows an average value of 2.04 ± 0.28, supporting our observation of low p-doping of graphene from the correlation plot (Fig. 6a). The FWHM distribution across the entire Raman mapping area further indicates a high-quality graphene transfer, with an FWHM of 17.58 ± 1.43 for the G peak (Fig. 6c) and 32.91 ± 1.83 for the 2D peak (Fig. 6b). The low standard deviation in the G peak width is expected, as the G peak is more sensitive to doping than the 2D peak,75,77,78,81 aligning with the observed low doping effect in the correlation plot (Fig. 6a). This extended analysis suggests that our PAL-assisted transfer introduces negligible perturbations to the graphene surface, resulting in a high-quality transferred material.
In addition to graphene, MoS2, a member of the transition metal dichalcogenide (TMDC) family, is a widely recognized 2D material. In this study, we successfully transferred a MOCVD-grown MoS2 monolayer from a sapphire substrate to a SiO2/Si substrate using PAL as a supportive layer. SEM images confirmed the transferred monolayer, and its optoelectronic properties were characterized by photoluminescence (PL) and Raman spectroscopy (ESI Fig. S9†). Further details on PAL-MoS2 transfer are provided in the ESI.†
PAL spin-coated on graphene/copper was transferred onto a SiO2/Si substrate using the previously described bubbling method. Following an initial optical microscopy imaging step, the PAL/graphene/SiO2/Si composite was incubated in a liquid suspension of S. cerevisiae and maintained at 30 °C with constant shaking at 100 rpm. To observe the gradual degradation of PAL, the sample was gently rinsed with DI water, air-dried, and imaged every 24 hours. This process was repeated continuously for 33 days, with the liquid suspension of S. cerevisiae renewed every 7 days. On the final day, another optical microscopy image was taken (Fig. 7b) and compared with the initial one (Fig. 7a). Fig. 7b shows that the yeast almost completely removed PAL, while Fig. 7c confirms the exposure of graphene under an optical microscope, with only minor PAL residue remaining. It is important to note that the sample was only rinsed with DI water; thus, some minor residue of PAL was expected. Additional images and details on the daily degradation process of PAL by yeast can be found in the ESI (Fig. S6†).
Experimental observations suggest that PAL was completely removed well before the 33-day mark. Additionally, a point-by-point micro-Raman characterization was performed on a 15 μm × 15 μm area to obtain more concrete evidence of PAL biodegradation and graphene exposure. Fig. 8e shows the approximate area where Raman and SEM analyses were conducted. The heat maps of the D, G, and 2D bands (with the same color scale), shown in Fig. 8a, b, and c, respectively, confirm the exposure of high-quality graphene.
Color variations in a few spots are primarily attributed to multilayer graphene, as shown in Fig. 8f (red spectrum) for the red-circled spot in the G band heat map, along with minor PAL residues (black-circled spot in the 2D band heat map). These residues persisted due to the absence of vigorous washing, as the sample was only gently rinsed with DI water. More rigorous washing or additional treatments were intentionally avoided to focus exclusively on the yeast-assisted degradation of PAL. To further confirm PAL biodegradation and the environmentally friendly, yeasted-assisted graphene transfer, an SEM image was acquired (Fig. 8d). Additionally, we transferred graphene using PAL-14d as a supportive layer and confirmed its biodegradability through optical microscopy, SEM imaging, and Raman analysis (ESI Fig. S7†).
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5nr01206f |
This journal is © The Royal Society of Chemistry 2025 |