Isotopes of heavier gases including carbon (13C/14C), nitrogen (13N), and oxygen (18O) are highly important because they can be substituted for naturally occurring atoms without significantly perturbing the biochemical properties of the radiolabelled parent molecules. These labelled molecules are employed in clinical radiopharmaceuticals, in studies of brain disease and as imaging probes for advanced medical imaging techniques such as positron-emission tomography (PET). Established distillation-based isotope gas separation methods have a separation factor (S) below 1.05 and incur very high operating costs due to high energy consumption and long processing times, highlighting the need for new separation technologies. Here, we show a rapid and highly selective adsorption-based separation of 18O2 from 16O2 with S above 60 using nanoporous adsorbents operating near the boiling point of methane (112 K), which is accessible through cryogenic liquefied-natural-gas technology. A collective-nuclear-quantum effect difference between the ordered 18O2 and 16O2 molecular assemblies confined in subnanometer pores can explain the observed equilibrium separation and is applicable to other isotopic gases.
Stable isotope technologies have attracted increasing interest over the last decade due to their indispensable role in plant, aquatic, and animal life1,2,3,4. They are widely used as radiolabelled probes in isotopic analysis methods5,6,7,8, therapeutic cancer drugs9,10, and environmental studies11,12. Naturally occurring heavier gas isotopes including carbon (13C and other isotopes), nitrogen (13N), and oxygen (18O) are extensively used for such radiolabeling because their molecular weight difference from their main isotope is quite minor compared to the lighter hydrogen (1H)-deuterium (2H) molecules, resulting in a lower isotopic effect and hence only a minor perturbation to the biochemical behavior1,2,13. The positron (β+)-emitting isotopes, including 15C/11C, 13N, and 18F, can be used as imaging probes in the radionuclide-based molecular imaging positron emission tomography (PET) technique and other useful clinical radiopharmaceuticals2. In particular, 18O2 acts as a target in cyclotrons for producing [18F]-labeled 2-deoxyglucose (FDG) as a β+-emitting radioisotope for PET biomedical imaging. Of all of the β+ emitters employed in PET, the 18F isotope is the preferred probe in radiopharmaceuticals because of its relatively long half-life (110 min), which allows its use in clinical PET imaging centers that lack radiochemistry facilities, and its low positron energy (0.64 MeV) that enhances the spatial resolution to produce optimal physical characteristics2. Other β+ emitters involving 11C or 13N exhibit short half-lives and can only be utilized at imaging centers with a cyclotron and radiochemistry facility2. PET imaging can show abnormalities that cannot be detected by other techniques, resulting in the early and more accurate diagnosis of infected or cancerous tissues14. Furthermore, 18O2 can be introduced into the body by simple inhalation to study the function of the brain for the treatment of patients with diseases, such as schizophrenia, manic depression2,10,15,16. Therefore, enhanced production of 18O is indispensable for achieving improvements in healthcare, environmental protection, and basic sciences.
The natural abundance of oxygen isotope 18O is very low and is only 0.204 at.% compared to the principal 16O isotope (99.76 at.%). Isotopic separation is currently only possible with a limited number of techniques, such as cryogenic distillation of oxygen/nitric oxide/water17,18, membrane distillation19,20, isotope exchange reaction21, and thermal diffusion22. These methods require complex equipment and are time and energy-intensive. Consequently, alternative technologies are needed to meet the high demand for 18O in healthcare and environmental science fields.
Recently, low-temperature adsorption-based separation enabled by the differences in isotope adsorption in nanopores due to the higher zero-point energy of translational motion of light isotope molecules (so-called quantum molecular sieving, QMS) has been demonstrated23,24. Consequently, QMS is the most promising alternative to the currently used methods for the separation of light isotopes such as hydrogen or helium25,26. However, the effective size differences for heavier gas isotopes such as 18O2 and 16O2 or 13CH4 and 12CH4 at 112 K, as estimated from the thermal de Broglie wavelength for the QMS effect, are only 0.0017 nm and 0.0012 nm, respectively. In addition, the Feynman–Hibbs potential calculation shows a difference of only 0.07 K for both isotope gases (Supplementary Fig. 1 and Supplementary Note 1), showing that QMS is ineffective for heavier gas isotopes. Therefore, we cannot expect that efficient separation of oxygen, methane, or other heavier gas isotopes can be achieved with nanoporous materials through the QMS mechanism.
The O2 or CH4 molecule has other vibrational and rotational degrees of freedom that depend on the molecular weight. The vibrational states are essentially the same in the gas and adsorbed phases and cannot lead to the selective adsorption of 18O2 or 13CH4. By contrast, the rotational degrees of freedom of the molecules adsorbed in the nanopores are highly restricted below 130 K, unlike those of gaseous molecules27. Nevertheless, a very small difference in the rotational energies of these isotope molecules coupled with translational motion28 is not sufficient to induce the selective adsorption of 18O2 or 13CH4. However, when O2 or CH4 molecules are densely packed at quasi-solid densities in nanopores at low temperature, collective quantum motion associated with vibrational and rotational modes can give rise to a sufficiently large adsorption-energy difference for oxygen and methane isotope molecules to enable the selective separation, as described in this article.
In this work, we report an industrially applicable adsorption-separation route of 18O2 from a 16O2–18O2 mixture using nanoporous solids at ~112 K, utilizing the cryogenic facilities of liquefied natural gas industries to save energy. The observed dynamic selectivity or separation factor S(18O2/16O2) exceeds 60, depending on the nanoporous adsorbent, as is further confirmed by breakthrough curve experiments. We also demonstrate an equally successful separation of 13CH4/12CH4 under similar conditions.
Dynamic adsorption separation of CDC
The dynamic adsorption-based separation was measured at different temperatures using a custom-made flow-type mixed gas adsorption apparatus coupled to a quadrupole mass spectrometer (MS) (Supplementary Figs. 2 and 3; Supplementary Notes 2 and 3)29. High purity 16O2 (99.99995%) and 18O2 (≥98%) gases were mixed to achieve different compositions (18O2% varied from 4.8 to 70 at.%) and then were introduced into the sample cell at a constant temperature. Similarly, 12CH4 (99.9999%) and 13CH4 (99%) were used to prepare isotopic mixtures. The adsorbents employed were carbide-derived carbon (CDC) produced by the chlorination of TiC30 and activated carbon fibers (ACFs) with slit-shaped pores. The effective pore widths determined from the N2 adsorption isotherms at 77 K are 0.7 nm for CDC and ACF5 and 0.8 nm and 1.1 nm for ACF10 and ACF20, respectively (Supplementary Figs. 4–6 and Supplementary Table 1). For theoretical calculations, the pore widths were also converted into the effective pore widths by subtracting 0.334 nm (the average graphite interlayer spacing) from the actual diameters31. We also considered open single-walled carbon nanotubes (SWCNTox) with cylindrical 1.5-nm and 1.0-nm wide pores and zeolites MS4A, MS5A, MFI, and BEA with interconnected cylindrical pores with the widths 0.40, 0.50, 0.55, and 0.66 nm, respectively; these materials were pre-evacuated prior to the dynamic and equilibrium adsorption measurements.
The adsorption selectivity S for 18O2 against 16O2 is defined as:
where (18O2/16O2)ads are the mole fractions of 18O2 and 16O2 in the adsorbed phase and (18O2/16O2)g are the mole fractions of 18O2 and 16O2 in the bulk gas phase, respectively. For simplicity, S(18O2/16O2)(ads-g) hereafter will be denoted as S.
Figure 1 illustrates that our cryogenic adsorption separation is much simpler, more energy-efficient, and compact than traditional cryogenic distillation involving sophisticated equipment with a distillation column with a height of tens of meters. For the selectivity observed from the present adsorption separation, only three adsorption stages are estimated to be required to obtain >95% purity of 18O2. The cryogenic adsorption-separation method utilizes nanoporous adsorbents that can selectively adsorb 18O2 in a gaseous 18O2–16O2 mixture as shown in Fig. 2a–d; the details of the selectivity calculations are presented in Supplementary Figs. 7 and 8. The CDC adsorbent packed cell at 112 K shows the excellent selective separation of 18O2 from the 18O2–16O2 gaseous mixture with different 18O2 at.%. Surprisingly, the dynamic adsorption selectivity S of CDC (Fig. 2a) is greater than 60 at the initial stage, irrespective of the 18O2 concentration, and decreases to 1.6–1.2 after 40 min (Fig. 2a, inset). Supplementary Fig. 9 shows the reproducibility of the selectivity. This decrease in the selectivity may be due to the decreased availability of the adsorption sites over time. CDC preferentially adsorbs 18O2 even from the mixed gas with a very low content of 18O2 (18O2 4.8%, 16O2 95.2%). However, the initial drop in S with time depends on the 18O2 concentration. A smaller 18O2% leads to a slower decay of S with time. The time for which S > 2.5 decreases with increasing 18O2%, as shown in Fig. 2b. The mixed gas with lower 18O2 content (4.8% and 10.5%) exhibits S > 2.5 for 28 ± 2 min, while higher 18O2 concentrations show less satisfactory performance. This result suggests that high selectivity persists under a wide range of isotopic concentration ratios, indicating the applicability of CDC for the separation of a more 18O2 diluted mixed feed gas. This phenomenon is crucial for the industrial separation of these isotopes because the atmospheric content of 18O is very low. The high selectivity can be demonstrated by comparing the adsorbed amounts of 18O2 and 16O2 by CDC for the equimolar mixture of oxygen isotopes at 112 K (Supplementary Figs. 10 and 11). 18O2 is preferentially adsorbed from the beginning, creating a concentration difference of 20 µmol g−1 over 120 min, resulting in high adsorption selectivity. Notably, the difference in the adsorption amounts of 18O2 and 16O2 can be observed from the beginning of the experiment; however, the selectivity can only be analyzed when the pore volumes of CDC are sufficiently crowded to allow few 18O2 molecules to reach the MS, as shown in Supplementary Fig. 7 (Supplementary Note 4). Here, the pore volume filling, which is the ratio of the adsorbed O2 volume derived from the liquid density of O2 compared with the measured nanopore volume, is 2% for 18O2; the expression for the adsorption by the pore filling is convenient for adsorption in nanopores. Moreover, the pore volume filling of the CDC depends on various factors, such as the amount of mixture gas introduced, dosing rate of introduction, and temperature. If an adsorption experiment is performed with more mixed gas at a higher dosing rate, then the pore volume filling % will be higher, as demonstrated in Supplementary Fig. 12. The high selectivity trend in the initial stage is retained in the temperature range of 100–150 K, as shown in Fig. 2c. However, the S at 1% pore volume filling and the time period for which S > 2.5 both decrease with increasing temperature (Fig. 2d). In addition, the pore volume filling of the mixed gas is larger at lower temperatures, and at 90 min, it decreases from 2.5% to 0.25% as the temperature increases from 100 K to 140 K (Supplementary Fig. 13). Consequently, the highly selective separation of 18O2 from the mixed gas (18O2 + 16O2) with a CDC of ~112 K is highly promising for the design of an efficient separation process.
The cryogenic adsorption separation demonstrates that S > 60 in the initial stage of adsorption (~1 min) arises from the selective adsorption of 18O2 in the narrow sites of the pores (<0.4 nm) present in the CDC structure32. In our previous work, atomistic models of CDCs were generated via molecular dynamics simulation and validated by experimental adsorption measurements33. A slice with a depth of 3.5 nm and a side of 10.4 nm of a representative CDC model containing realistic slit-shaped pores is shown in Fig. 2e, left panel. The CDC porosity was evaluated by filling the structure with nonoverlapping spheres according to the Gubbins method34. Rendering of the spheres within the CDC structure aids the visualization of the pores, as shown in the right panel, where each sphere is colored according to its diameter. Narrow pores with diameters <0.4 nm are identified by dashed white ovals, confirming the presence of preferential adsorption sites for the 18O2 molecules in CDCs. Figure 2f shows the experimental S values of CDC at 100 K and 112 K compared with those of the other separation methods reported in the literature. The high selectivity S = 116 ± 14 at 100 K or S = 60 ± 15 at 112 K is ascribed to the preferential adsorption of 18O2 molecules at the narrow pore sites (left inset in Fig. 2f). Even after 30 min, the CDC pores are filled with S > 2 (right inset in Fig. 2f), which is still twice that of the other separation methods. To further ascertain the observed high selectivity trends, adsorption–separation experiments are performed using CDC adsorbent for only 10, 15, and 20 min at 112 K. The mole fractions of the feed and adsorbed mixture isotope gas are monitored using the time evolution of mass intensity. The molar ratio for the feed gas 18O2:16O2 = 1. The observed mole fraction of the desorbed mixed gas is 18O2:16O2 = 1.4 ± 0.005 (17.5 Pa 18O2 + 12.5 Pa 16O2) after adsorption for 10 min. When adsorption was performed for 20 min, the desorbed mixed gas displayed 18O2:16O2 = 1.3 ± 0.006 (Supplementary Fig. 14). This shows that ∼8% higher adsorption of 18O2 occurs during the 10-min selective adsorption experiment compared to the experiment carried out for 20 min, corresponding to a maximum difference of 1.33 mg/g between 18O2 and 16O2. These results confirmed that the initial high selectivity tends to decrease over time.
In addition, we have verified that this method is applicable to other gaseous heavy isotope pairs involving 13CH4 and 12CH4. The CDC demonstrates selective separation of 13CH4 from the mixed gas (13CH4 + 12CH4) at 112 K with S(13C/12C) = 56 ± 6 initially and maintains S > 2.5 for more than 40 min (Fig. 2g).
Dynamic adsorption separation of different nanoporous adsorbents
Other nanoporous materials with different pore geometries show similar selectivity trends even though their selective absorptivities are slightly inferior to that of CDC, as shown in Fig. 3a, b. The equilibration time depends on the pore aperture. ACF5 (slit pore width: 0.7 nm) shows high selectivity for an extended time interval with S > 1.2 up to 120 min (complete experiment time, see inset Fig. 3a). SWCNTox with 1 nm cylindrical pore maintains S > 1.2 for more than 60 min, while zeolite MFI (pore width 0.55 nm) shows S > 1.2 for only 30 min (inset Fig. 3a, b). We have also measured the selectivity in AFC10, AFC20, SWCNTox (1.5 nm), and zeolites BEA and MS5A, all of which exhibit lower selectivity. In addition, the adsorbents with pore widths of < 0.4 nm do not demonstrate significant selective separation performance (Supplementary Figs. 15 and 16). A significant difference in the adsorbed amounts of 18O2 and 16O2 can be observed in Fig. 3c, d. For ACF5, the adsorbed gas amount increases gradually, reaching a maximum adsorption difference of 13 µmol g−1, while the corresponding values for SWCNTox (1 nm) and zeolite MFI after 120 min are 10 µmol g−1 and 16 µmol g−1, respectively. The pore volume filling percent after 120 min varies from 0.6% for ACF20 (pore volume of 0.81 ml g−1) to 5.2% for zeolite MFI (pore volume of 0.16 ml g−1) (Supplementary Fig. 17). Figure 3e summarizes the S values for all the nanoporous adsorbents at a pore volume filling of 1%, demonstrating the best selective adsorption behavior of CDC. This implies that the observed selectivity depends strongly on the pore size and the pore geometry (shape). The narrow pores present in the CDC structure have a 2D structure, while SWCNTox (cylindrical pores) or zeolites (interconnected channeled cylindrical pores) have 1D channels and inferior selectivity compared to CDC. The observed maximum adsorption difference of 1.33 mg/g between 18O2 and 16O2 under the present experimental setup during only 10 min of adsorption separation appears to be highly promising for dynamic separation. If we increase the sample amount to 1 kg of adsorbent, the available adsorption system can give rise to a preferential 18O2 adsorption of 0.8 L(STP) and will be quite useful. A new type of adsorption-separation system with a large sample holder and mixed gas reservoir can be constructed that utilizes the initial large selective adsorption of 18O2; this will enable human society to obtain a promising isotope separation technology, considering that the present 18O2 separation technology using distillation requires 10 months.
Furthermore, we confirmed this by performing breakthrough measurements with an adsorption column packed with a comparatively large amount of commercially available ACFs to evaluate the separation performance. We used ACFs because the breakthrough experiments required larger sample sizes than the amount of the lab-synthesized CDC available. The experimental conditions and the selectivities for the breakthrough experiments are listed in Supplementary Table 2. A custom-made apparatus for measuring the breakthrough curves is schematically shown in Supplementary Fig. 18 (Supplementary Note 5). The breakthrough curves for ACF5 and ACF10 are shown in Fig. 4a, b. The concentration C/C0 of 16O2 at the outlet in the initial stage is much larger than that of 18O2 for both ACFs, clearly indicating the preferential adsorption of 18O2 under continuous flow conditions using He as the carrier gas. The high S values of 1.5 and 3.0 for ACF5 and ACF10, respectively, in the initial stage qualitatively correspond to the results from mixed gas adsorption experiments, as pictorially described in Fig. 4c. This reflects that the adsorbed molecules can mostly occupy the pore entrance sites during the initial stage of high selectivity and then diffuse to the inner pore region. The selectivity decreases with time as 18O2 reaches full breakthrough and the flow approaches a stationary state. These selectivity values from the breakthrough measurement are much larger than the S ∼1.04 of the current separation methods (Fig. 2f). However, the selectivity from the breakthrough experiment is smaller than that obtained from the mixed gas adsorption method discussed above.
Theoretical selectivity of oxygen isotope adsorption
Above, we have presented experimental results demonstrating 18O2/16O2 selectivity but did not provide a clear explanation of the origin of these results. It is known that nuclear-quantum effects (NQEs) in the vibrational, rotational and translational motion of the condensed phase can each contribute to isotope selectivity35,36,37. O2 molecules in the nanopores at low temperature form an ordered solid-like assembly in the nanopores due to the strong O2–nanopore and O2–O2 interactions. We have performed simulations of 18O2 and 16O2 isotopes in MFI and SWCNTs using the path-integral formalism35 to explicitly account for the NQEs in each of the degrees of freedom to identify the origin of the observed isotope selectivity. We note that isotopic selectivity is an inherently quantum mechanical phenomenon; we, therefore, employed path-integral molecular dynamics methods to compute the free energy differences for the gas and adsorbed phases of the different isotopes. In addition, adsorption selectivity is a thermodynamic equilibrium property, so that it is appropriate to use equilibrium path integral methods. In addition, we note that tunneling does not contribute in any way to the thermodynamic properties, and therefore does not need to be considered here. The experimental results give kinetic selectivity as a function of time. This quantity is not the true equilibrium selectivity but rather is related to a breakthrough process of dynamic adsorption. This process cannot be modeled using atomistic path integral methods because it would require detailed knowledge of the time-dependent pore filling process, including diffusion barriers through the irregularities in the adsorbent materials. Thus, it is only possible to model equilibrium selectivity. However, this modeling does provide a proof-of-concept that collective NQEs are responsible for the long-term (near-equilibrium) selectivity observed in the experiments. Details of the calculations are given in Supplementary Methods 1. We chose MFI and SWCNT because their atomistic structures are known precisely and therefore, these materials are amenable to accurate modeling. We note that these calculations represent equilibria and cannot account for the kinetic (time-dependent) selectivities observed in Fig. 3a, b but do explain the long-term (equilibrated) experimental results. We carried out simulations at both zero-loading (one O2 per simulation cell) and at the loadings corresponding to the equilibrium amounts of O2 adsorbed at a relative pressure P/P0 of 0.12 at the temperatures of 90.2, 112, and 130 K to account for the effects of the adsorbate-adsorbate interactions on selectivity.
Path-integral calculations in the low O2 coverage limit were carried out for SWCNTs having atom-center-to-atom-center tube diameters ranging from 0.54 to 1.35 nm (effective diameters of 0.21–1.02 nm) to obtain the relationship between the selectivity and tube diameter; the results are shown in Fig. 5a and Supplementary Table 3. The (4,4) and (5,5) SWCNTs with extremely narrow diameters of 0.54 nm (0.21 nm effective diameter) and 0.69 nm (0.36 nm effective diameter), respectively, give high selectivity values at zero loadings through strong O2–SWCNT interactions, resulting in mass-dependent NQEs in the rotational, vibrational, and translational degrees of freedom. However, these pores are too small to induce the observable O2 adsorption experimentally. In contrast, adsorption in the (7,7) and (10,10) SWCNTs at zero loading shows very low selectivities (1.004 ± 0.002 and 1.006 ± 0.0037, respectively), indicating that the experimentally observed results cannot be explained by simulations at low coverages.
We, therefore, simulated O2 adsorbed in (7,8) and (10,10) SWCNTs with the actual diameters of 1.02 (0.7 nm effective diameter) and 1.36 nm (1.03 nm effective diameter), respectively, at 90.2 K using amounts of adsorbate close to that reported for SWCNTox(1 nm) at P/P0 = 0.12 (Supplementary Fig. 19). The selectivities obtained from the finite loading simulation were 1.164 ± 0.024 for the (7,8) SWCNT and 1.02 ± 0.007 for the (10,10) SWCNT, similar to the long-time experimental value for the SWCNTox (1 nm) of 1.09, as shown in the inset of Fig. 3a. The origin of the significant increase in selectivity with finite loading relative to the low coverage limit can be found in the highly ordered state of the O2 molecules observed in the simulations. The initial random configuration shown on the left of inset Fig. 5a transforms to a highly ordered state (right) during the PIMD simulation. This highly ordered state gives rise to a collective NQE not obtained at low coverage, resulting in higher selectivity.
Furthermore, we calculated O2 isotope selectivities for finite adsorption in MFI for P/P0 = 0.12 to mimic experiments (Supplementary Figs. 20 and 21). The obtained selectivities were 1.092 ± 0.028, 1.095 ± 0.019, and 1.038 ± 0.02 for the temperatures of 90.2, 112, and 130 K, respectively (Fig. 5b and Supplementary Table 4), in agreement with the experimental results shown in Fig. 3b.
Our simulation results indicate that (1) narrow pores give higher selectivity and (2) the observed selectivity is a result of both pore confinement and the cooperative or collective NQEs due to the ordering of the O2 molecules when a high amount of O2 molecules is adsorbed in the preferable pores (close to saturation). These observations are consistent with our hypothesis that narrow pore sites give rise to higher selectivities because they have higher confinement and are more likely to produce ordered O2-adsorbed phases than the larger nanopores within CDC. Furthermore, we measured the difference in the activation energy (Eaads) for the overall adsorption rates of 18O2 and 16O2 on CDC at 112 K using the linear driving force model described in Supplementary Fig. 22 (Supplementary Methods 2). The Eaads values obtained for 18O2 and 16O2 are 9.1 ± 0.1 kJ mol−1 and 9.4 ± 0.1 kJ mol−1, respectively. This small activation energy difference of 0.3 ± 0.1 kJ mol−1 between 18O2 and 16O2 may be associated with the potential energy difference in the transition state for adsorption.
Adsorption isotherms and energetics
Figure 5c shows the experimental adsorption isotherms for 18O2 and 16O2 on CDC at 90.2, 112, and 130 K. All of the adsorption isotherms exhibit Type I behavior in the IUPAC classification, indicating the filling of oxygen molecules in highly uniform nanopores38. The 18O2 uptake is essentially the same as the 16O2 uptake below P/P0 = 10−4 (Fig. 5d). However, the 18O2 uptake is slightly higher than that of 16O2 at higher relative pressures (Supplementary Fig. 23). The isosteric heat of adsorption (qst) was evaluated from the Clausius–Clapeyron equation using the adsorption isotherms at different temperatures (Supplementary Fig. 14 and Supplementary Methods 3). The qst values for both oxygen isotopes decrease from 18 kJ mol−1 to 15 kJ mol−1 at the filling of 0.5 (Fig. 5e), and is much larger than the heat of condensation of bulk O2 ~6.8 kJ mol−1 39 due to the favorable interactions with the pores. The absolute adsorption amount difference of 18O2 and 16O2 is not sufficiently large to obtain an evident difference in the qst of the oxygen isotope molecules in the low fractional filling range. It is noteworthy that qst for 18O2 is larger than that of 16O2 above the fractional filling of 0.1, giving a difference of 0.2 ± 0. 005 kJ mol−1 for CDC (inset in Fig. 5e). Similarly, the qst difference between 18O2 and 16O2 for SWCNTox (1 nm) is 0.7 ± 0. 04 kJ mol−1 at the filling of 0.3 (Fig. 5f) but much smaller differences are obtained at low coverage, consistent with our calculations. On the other hand, the qst of MFI gradually increases with fractional filling with no clear difference in the qst between 18O2 and 16O2 (Fig. 5f).
Since CDC gives the highest selectivity, we discuss the relationship between the pore shape and qst results. The large qst for CDC at the initial stage arises from the highly confined state of the oxygen molecules in the narrow pore sites with very deep interaction potential wells, forming the ordered molecular solids, as mentioned above. The qst gradually decreases with fractional filling due to the changes to the adsorption sites of the shallower interaction potential wells. To evaluate the contribution of the narrowest pore sites toward the total adsorption, we simulated N2 adsorption on our CDC model as shown in Fig. 2e left. The geometrical cumulative pore volume using nitrogen as a probe atom was calculated using Poreblazer40. It is noted that the pore highlighted within the small cyan circle contains spheres of diameter <0.4 nm and that space is not accessible to nitrogen (Supplementary Fig. 25). The cumulative pore volume of such narrow spaces is Vnarrow-pore (d < 0.4 nm) = 0.021 cm3 g−1, contributing to 3.5% of the total pore volume. These narrow sites exhibit 2D accessibility and this may facilitate the preferential adsorption of 18O2 as pictorially demonstrated in Fig. 5g. The 18O2 molecules strongly confined at the narrow spaces in the pores of CDC can form an ordered molecular solid-like assembly that leads to a collective NQE. Furthermore, 1D pores of SWCNTs and zeolites display less accessibility and weaker interaction potentials than the 2D narrow pores of CDC. Consequently, the collective NQE in SWCNTs and zeolites is not as remarkable as that in CDC. The interaction potential of ACFs is weaker than that of the narrow pore sites of CDC, even though ACF has well-accessible slit-shaped pores.
We have demonstrated very high 18O2 adsorption selectivity of nanoporous materials that increases with decreasing temperature and has a strong dependence on the pore geometry of nanoporous materials. In particular, at approximately the boiling temperature of methane (112 K) CDC shows S(18O2/16O2) exceeding 60 ± 15 for the initial stage of adsorption because 18O2 molecules are kinetically and thermodynamically preferentially adsorbed over 16O2. Such high adsorption selectivity was also evident for the separation of 13CH4 with S(13C/12C) = 56 ± 6. The highly efficient separation of 18O2 or 13CH4 evidenced in this study can be implemented in the industry by designing a rapid adsorption-separation instrument and will facilitate medical and other applications of these O and C isotopes. The CDC with highly accessible 0.4 nm wide pore spaces has a strong interaction potential for O2 and gives the highest adsorption selectivity compared with activated carbon fibers, single-walled carbon nanotubes, and zeolites. Nanoporous materials consisting of graphitic walls and having an abundance of very narrow open pores are promising for achieving high separation selectivity and high separation capacity. The collective nuclear-quantum effect (NQE), which is different from the well-known translational motion-based QMS effect, can explain the equilibrium selective adsorptive separation of 18O2 or 13CH4 by subnanometer pores.
Synthesis and characterizations
Pitch-based activated carbon fibers (ACF20, ACF10 and ACF5) were procured from Ad’all Co., Ltd. The CDC sample derived from TiC was synthesized by following the previously reported method41,42. Single-walled carbon nanotubes (SWCNT) grown by the CVD method were obtained from MEIJO NANO CARBON Co., Ltd. The samples were oxidized under dried air at 823 K for 10 min with the heating rate 1 K/minute. A typical steam-assisted crystallization synthetic method has been used for the synthesis of pure silica zeolite BEA43. Silicalite-1 or zeolite MFI was synthesized by following the seed surface crystallization mechanism discussed by Ren et al.44. Molecular sieves MS5A and MS4A were purchased from Nakarai Tesque. High purity 16O2 (99.99995%) and 12CH4 (99.9999%) were procured from JAPAN FINE PRODUCTS-JFP, 18O2 (≥98%) from TAIYO NIPPON SANSO Corporation, and 13CH4 (99%) from ISOTEC. The adsorption isotherms of the adsorbents were measured using a Microtrac MRB’s apparatus (BELSORP MAX) after pre-evacuation at 423 K/3 h.
The authors declare that the data supporting the findings of this study are available from the authors and are presented in the paper and its supplementary information files.
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K.K. acknowledges project Japan Science Technology Agency (JST) CREST “Creation of Innovative Functional Materials with Advanced Properties by Hyper-nanospace Design” and partial support by the Grant-in-Aid for Scientific Research (B) (17H03039) and the OPERA JST project (JPMJOP1722). SKU was supported by the JST-CREST and OPERA projects. H.T., R.F., and F.V.-B. are supported by TAKAGI Co., Ltd. Funding for A.B. and J.K.J. was provided by the National Science Foundation under Award No. CBET1703266. Simulations were performed using the computational resources provided by the Center for Research Computing at the University of Pittsburgh and Extreme Science and Engineering Discovery Environment (XSEDE), which is supported by National Science Foundation grant number ACI-1548562, under allocation No. TG-DMR110091 and the Pawsey Supercomputing Centre, with funding from the Government of Australia and the Government of Western Australia. C.D.T. and I.S.M. are supported by the Australian Research Council under grant FT140100191. CDC synthesis was supported as part of the Fluid Interface Reactions, Structures and Transport (FIRST) Center, an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science, and Office of Basic Energy Sciences.
The authors declare no competing interests.
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Ujjain, S.K., Bagusetty, A., Matsuda, Y. et al. Adsorption separation of heavier isotope gases in subnanometer carbon pores. Nat Commun 12, 546 (2021). https://doi.org/10.1038/s41467-020-20744-6