Structural Elucidation of Amorphous Photocatalytic Polymers from Dynamic Nuclear Polarization Enhanced Solid State NMR Structural Elucidation of Amorphous Photocatalytic Polymers Dynamic Nuclear Polarization

: Dynamic nuclear polarization (DNP) solid-state nuclear magnetic resonance (NMR) o ﬀ ers a recent approach to dramatically enhance NMR signals and has enabled detailed structural information to be obtained in a series of amorphous photocatalytic copolymers of alternating pyrene and benzene monomer units, the structures of which cannot be reliably established by other spectroscopic or analytical techniques. Large 13 C cross-polarization (CP) magic angle spinning (MAS) signal enhancements were obtained at high magnetic ﬁ elds (9.4 − 14.1 T) and low temperature (110 − 120 K), permitting the acquisition of a 13 C INADEQUATE spectrum at natural abundance and facilitating complete spectral assignments, including when small amounts of speci ﬁ c monomers are present. The high 13 C signal-to-noise ratios obtained are harnessed to record quantitative multiple contact CP NMR data, used to determine the polymers ’ composition. This correlates well with the putative pyrene:benzene stoichiometry from the monomer feed ratio, enabling their structures to be understood. Details of porosity and surface area measurements, NMR experiments used, PXRD, overall sensitivity enhancement factor Σ † calculations, multiCP parameters, and additional ﬁ gures (PDF)


INTRODUCTION
Organic polymeric photocatalysts that generate hydrogen from water under electromagnetic irradiation have become an area of great interest in materials chemistry in recent years due to their potential greater diversity than classic metal based photocatalysts. 1−3 Organic photocatalysts such as graphitic carbon nitride 4 and poly(p-phenylenes) 5−7 are primarily active when irradiated with light in the UV region of the electromagnetic spectrum (just 3% of the solar light on the Earth's surface). 8 Recent developments in the field have targeted polymers active in the visible light region, the predominant wavelengths of radiation present in solar light, with tunable band gaps to optimize photocatalytic activity. 7−17 One of these families of polymers (Figure 1), which belongs to the conjugated microporous polymers (CMPs), 18 is specifically investigated in this work due to both their remarkable hydrogen evolution rates under visible light ( Figure  1) and their large accessible surface areas (Brunauer−Emmett− Teller surface areas (SA BET ) up to ∼1200 m 2 g −1 , Table S1, pore size distributions, Figure S1). These CMPs, known as copolymerized conjugated microporous polymers (CP-CMPs) are extended three-dimensional networks composed of copolymerized alternating pyrene and benzene monomer units in varying ratios to form multicomponent systems ( Figure   1). They are both insoluble and amorphous, making their atomic level structure very challenging or impossible to obtain using standard analytical methods such as X-ray diffraction ( Figure S2) or solution-state NMR. CP-CMPs' insolubility also prevents their physical properties such as particle size from being determined by chromatography-based techniques such as size exclusion or gel permeation chromatography. It is possible to empirically optimize photocatalytic activity of these materials; however, a targeted synthetic approach relies on the obtained polymer structure which cannot be assumed to be identical to the monomers input. The development of a robust method of characterization of CP-CMPs is vital to determining their compositions, and understanding and improving upon their remarkable activities.
Solid-state NMR spectroscopy is a well-established technique for short-range structure determination and has played an important role in elucidating extended polymer networks. 19,20 Nevertheless, the acquisition of quantitative directly excited 13 C spectra for these systems can be time-consuming as they are often multicomponent, containing repeat units at a low relative concentration 7,21−23 which can lead to their signals being obscured by higher intensity peaks and/or difficult to differentiate from baseline noise, and the 13 C spin−lattice relaxation times T 1 could be long. Although, Hartmann−Hahn cross-polarization 24 (CP) improves signal-to-noise ratio and time efficiency, this approach often requires substantial experimental times (hours) 19,20 and unlike direct 13 C excitation, CP spectra obtained with a single contact time only provide qualitative data, making the experiment redundant when quantification of 13 C signals is needed.
High field dynamic nuclear polarization (DNP) 25−28 is an emerging technology for enhancing solid-state NMR signals by multiple orders of magnitude, by transferring the large polarization of unpaired electrons to nuclei in close proximity to the electron source, with the hyperpolarization spreading between nuclei by spin diffusion before detection of the enhanced NMR signals. DNP has a long history of application to polymers such as polystyrene and polycarbonate derivatives 29−33 to enhance signal sufficiently to observe interfaces between domains within blended polymers. When combined with magic angle spinning (MAS) and 13 C CP, 34 this indirect DNP approach has been demonstrated as an extremely versatile technique for the characterization of polymers, 35−44 substantially reducing experimental times for microporous materials and delivering high throughput capability to solid-state NMR. 42 Nevertheless, quantification of the 13 C NMR resonances is still hampered by the nonquantitative nature of CP (vide supra).
Note that direct DNP (electron-13 C polarization transfer without 1 H polarization and CP step) is not quantitative due to the lack of spin diffusion to distribute the hyperpolarization in these systems. 45 A quantitative approach to CP known as multiCP was first reported in 1990 46 and consists of multiple short CP contact pulses, separated by delays long enough for substantial 1 H longitudinal relaxation but with minimal 13 C relaxation leading to cumulative polarization with each short contact pulse (the pulse program is shown in Figure S3d). MultiCP has recently regained popularity 47−52 to provide time efficient quantification of organic matter and materials such as pharmaceutical excipients and metal organic frameworks. This approach, when combined with DNP enhanced 13 C MAS NMR, provides an appealing route to obtain quantitative NMR spectra quickly and is explored here to determine the compositions of photocatalytically active CP-CMPs ( Figure 1).
Here we demonstrate that DNP represents a time efficient approach to obtain high signal-to-noise 13 C NMR spectra of CP-CMPs. We show that the high signal obtained facilitates the acquisition of a two-dimensional 13 C− 13 C through-bond correlation spectrum at natural abundance of amorphous macromolecules; such a spectrum could not be obtained without DNP. Enhancement values of up to ε C CP > 200 at 9.4 T are possible via the cross effect (CE) DNP mechanism, 53 allowing the 13 C NMR spectra of the series of polymers to be obtained quickly (hours) and which enables tracking minor changes in the polymeric structure. Combining these large  Table 1). The photocatalytic hydrogen evolution rates for 100 mg polymer in water containing 20 vol % diethylamine as an electron donor under visible light (λ > 420 nm from a 300 W xenon light source) are displayed below each name. In parts b and d, each unique 13 C environment resolvable by NMR (see below) has been attributed a name within the structure. The bracketed sections represent randomly distributed minor components. The C Pyr-Ph −C Ph-Pyr bonds that confirm copolymerization are given in orange, while homocoupling bonds of benzene and pyrene units are shown in cyan and magenta, respectively.

Macromolecules
Article DNP enhancements with the quantitative multiCP experiment, 49 we were able to determine the polymers' compositions, estimate the average polymeric structure and compare with the monomer feed ratio, a result that cannot be obtained by any other spectroscopic or analytical method.
NMR Procedures. For DNP, incipient wetness impregnation, slurry, and dried preparations were all used. For incipient wetness impregnation (used unless stated otherwise), a preweighed amount of CP-CMP powder (typically around 10 mg) was impregnated with 80 μL of 20 mM TEKPol biradical 55 in 1,1,2,2-tetrachloroethane (TCE), 56 until the powder appeared saturated with the solution, and was then mixed uniformly. Slurries were prepared with ∼10 mg of polymer, which was mixed homogeneously with 120 μL of 20 mM TEKPol in TCE. In the dried preparation ∼10 mg of polymer was homogeneously mixed with 50 μL of 20 mM TEKPol in TCE and was then left to dry for 48 h, allowing all of the solvent to evaporate. The CP-CMP/TEKPol/TCE mixtures were then packed directly into 3.2 mm sapphire rotors and sealed with zirconia caps. Where stated, the samples were freeze/thaw cycled five times to remove paramagnetic oxygen from the matrix ( Figure S4). 40,57 DNP spectra at 600 MHz were recorded on a commercial 14.1 T Bruker Avance III DNP solid-state NMR spectrometer equipped with a 395.20 GHz gyrotron microwave system. 58 Experiments were recorded with a 3.2 mm HXY triple-resonance MAS probe at ν 0 ( 1 H) = 600.084 MHz corresponding to the maximum enhancement 1 H position ε H for binitroxide radical TOTAPOL 59 at ν 0 (e − ) = 395.20 GHz, with the X channel tuned to 13 C at ν 0 ( 13 C) = 150.91 MHz. All experiments were performed under magic angle spinning (MAS) at ν r = 12.5 kHz and T ≈ 120 K, as determined by spin−lattice relaxation times (T 1 ) measurements of 79 Br on a very small amount of KBr added to rotor. 60 All 1 H pulses and SPINAL-64 heteronuclear decoupling 61 were performed at a radio frequency (rf) field amplitude of 100 kHz. All 13 C CP MAS experiments were obtained with a 13 C rf field of 72 kHz, while the 1 H rf field amplitude was ramped to obtain maximum signal at a 1 H rf field of approximately 100 kHz. CP contact times were optimized for maximum signal on each polymer.
All DNP NMR experiments at 400 MHz were performed on a commercial 9.4 T Bruker Avance III DNP solid-state NMR spectrometer equipped with a 263.715 GHz gyrotron microwave system. 62 Experiments were recorded with a 3.2 mm HXY tripleresonance MAS probe at ν 0 ( 1 H) = 400.07 MHz corresponding to the maximum enhancement 1 H position ε H for TOTAPOL at ν 0 (e − ) = 263.715 GHz, with the X channel tuned to 13 C at ν 0 ( 13 C) = 100.61 MHz and at T ≈ 110 K as above. 60 All 13 C CP MAS experiments were obtained with a 13 C rf field of 54 kHz, and all other parameters matched those at 600 MHz DNP. The INADEQUATE spectrum was recorded with 13 C rf field amplitude of 100 kHz, contact pulses at 90 kHz, while the 1 H rf field amplitude was ramped to obtain maximum signal at a 1 H rf field of approximately 100 kHz. A double quantum coherence delay of 3.4 ms was optimized, with a z-filter delay of 1.4 ms. All spectra were obtained with a recycle delay of a 1.3 × τ DNP ( 1 H) for optimal signal-to-noise per unit time. 63 All multiCP experiments were run with a 5 × τ DNP ( 1 H) recycle delay, and 2 × τ DNP ( 1 H) delays between contact pulses where τ DNP ( 1 H) is the DNP polarization buildup times (see Figure S3d, and section S5 in the Supporting Information). Contact pulses of 1 ms were used with the exception of the final contact, which was 0.8 ms in duration, and number of pulses optimized for each polymeric system ranging from 6 to 10 repeats, and 8 scans were accumulated. All multiCP spectra were fitted using the sola function in Topspin 3.5 including 13 C CSA.
All standard solid-state NMR experiments were performed on a commercial 9.4 T Bruker Avance III HD solid-state NMR spectrometer equipped with a 4 mm HXY triple-resonance MAS probe (in double resonance mode) with the 1 H Channel tuned to 1 H at ν 0 ( 1 H) = 400.13 MHz and the X channel was tuned to 13 C at ν 0 ( 13 C) = 100.67 MHz. All experiments were performed under MAS at ν r = 12.5 kHz and T = 298 K. All 1 H pulses and SPINAL-64 heteronuclear decoupling 61 were performed at an rf field amplitude of 83 kHz. All 13 C CP MAS experiments were obtained with a 13 C rf field of 45 kHz, while the 1 H rf field amplitude was ramped to obtain maximum signal at a 1 H rf field of approximately 60 kHz, and a contact time of 2 ms.
In all cases, T 1 and τ DNP were obtained using saturation recovery experiments ( Figure S3(a)). NMR data were obtained and analyzed using TopSpin 3.2, and all 1 H and 13 C spectra were referenced to H 2 O at 4.8 ppm and the tertiary 13 C on adamantane at 29.45 ppm (corresponds to TMS at 0 ppm), 64 respectively. The chemical shifts of all assigned peaks are quoted within a realistic accuracy of ±1 ppm due to the broad line widths.
EPR Experiments. The 9 GHz (X band) continuous-wave electron paramagnetic resonance (EPR) spectra were recorded on a Bruker Biospin EMX spectrometer fitted with an Oxford Instruments ESR900 cryostat. At room temperature the spectra were obtained with 1 mW microwave power and 0.5 G modulation under nonsaturating conditions. At 120 K the spectra were obtained with 0.02 mW microwave power and 0.5 G modulation. The samples used were those prepared in the NMR section above and packed into capillary tubes, or standard EPR tubes.
EPR spin-counting experiments were recorded on an X-band Bruker Biospin EMX Nano spectrometer operating at 9.6 GHz and at room temperature. Samples were packed into 3.2 mm sapphire NMR rotors and sealed with zirconia caps. Spin counting calculations were performed as per the Bruker Spin Counting Manual procedure. The error on the spin counting measurements was determined to be ±10% while the determination of the electron concentration had an estimated error of approximately ±60% (due to the rapid evaporation of TCE during the sample packing procedure).
Powder X-ray Diffraction Measurements. Powder X-ray diffraction (PXRD) data ( Figure S2) were collected in high throughput transmission mode on a Panalytical Empyrean diffractometer producing Cu Kα (λ = 1.5418 Å) radiation, equipped with an X-ray focusing mirror and PIXcel 3D detector.
Pore Size and Surface Area Measurements. The materials were degassed at 120°C for 900 min under dynamic vacuum (10 −5 bar) before analysis. Nitrogen adsorption and desorption isotherms were collected at 77.3 K using an ASAP2420 volumetric adsorption analyzer (Micromeritics Instrument Corporation). Brunauer−Emmett−Teller surface areas (SA BET ) were calculated in the relative pressure (P/P 0 ) range of 0.05−0.25. Pillared clay method of nonlocal density functional theory (NL-DFT) was used to determine the pore size distribution assuming a cylindrical pore geometry.

RESULTS AND DISCUSSION
Optimizing Sample Preparation. Figure 1 depicts the putative structures of the CP-CMP polymers investigated in this work, postulating that the polymer compositions match the pyrene to benzene ratio of the monomer feed. CP-CMP9 displays reasonable photocatalytic water splitting under visible light, and increasing pyrene concentration in the monomer feed by 25% (CP-CMP10, Figure 1c) leads to a substantial increase in photocatalytic water splitting likely resulting from slight decrease of the optical bandgap. A further 5% increase in monomeric pyrene concentration to CP-CMP11 leads to a sharp decline of photocatalytic activity, and a substantial drop in bandgap. CP-CMP1 and CP-CMP15 show no photocatalytic activity and contain only one polymeric repeat unit (CP-CMP15) or one base benzene unit alternating between di-and tetra-substituted (CP-CMP1). Figure 2 shows the DNP enhanced 13 C CP MAS NMR spectrum of CP-CMP10 using a range of sample preparation approaches for which full details are given in the experimental section, with enhancement given as ε C CP (defined in section S4 of the Supporting Information). Although, film casting has been demonstrated to show excellent DNP enhancement in linear polymers such as polystyrene after dissolution in the radical solution, 39 this method is not practical on CP-CMPs due to their insolubility, and as such other approaches were used. The dried preparation 37 showed a modest signal enhancement in our hands (ε C CP ∼ 5), while the slurry preparation gave a higher enhancement of ε C CP = 14. For CP-CMP10, incipient wetness impregnation 65 provides the largest ε C CP value (28). This is likely due to a reduction in paramagnetic bleaching due to the lower concentration of radical in the sample 66 and was therefore selected as the optimal sample preparation approach for all CP-CMPs studied here (as shown previously). 67 EPR of the dried sample ( Figure 2a) shows anisotropic line broadening of immobile TEKPol radical likely caused by electron−electron dipolar and/or exchange interactions, whereas the EPR spectrum of the slurry (Figure 2b) is much narrower, indicative of mobile radical. The EPR of CP-CMP10 prepared by incipient wetness impregnation suggests that the radical/solvent solution fills the pores of the polymer lattice (Figure 2c), as revealed by the EPR line shape showing a combination of narrow lines, indicative of TEKPol in solution, with broadened shoulders, illustrating the presence of immobile TEKPol within the polymer. 68 EPR at 120 K, reflective of the temperature at which the DNP experiments would be recorded, showed typical "powder" spectra ( Figure 2). The same line shape trends are observed as at room temperature, with the incipient wetness impregnation sample showing a hybrid line shape, between that of the dried sample and the slurry, which represents the free radical in frozen solution. It is possible that the additional broadening observed in the dried sample (and to a lesser extent, incipient wetness impregnation) could be attributed to dipolar broadening and/or weak exchange coupling, however, there is an absence of strong exchange coupling in all preparations. 69 The data therefore suggests that there is no further aggregation of radical occurring at low temperature. EPR spin counting experiment on this sample yielded (9 ± 1) × 10 17 electron spins in reasonable agreement with the (6 ± 4) × 10 17 spins anticipated from the DNP sample preparation procedure. This illustrates the absence of measurable degradation of TEKPol in contact to CP-CMP10.

Macromolecules
Article Spectral Assignment. In order to unequivocally assign the 13 C MAS spectrum of CP-CMP10, a 9.4 T DNP enhanced Jbased 13 C− 13 C correlation spectrum was obtained using the refocused INADEQUATE experiment and yields carbon− carbon connectivities (Figure 3). 70 Despite the inherently very low sensitivity of this experiment at 13 C natural abundance due to the very low probability of having a pair of 13 C nuclei (0.01% abundant), the sensitivity enhancement of DNP enables such an experiment to be readily obtained as demonstrated previously. 37,71 The corresponding 2D spectrum of CP-CMP10 is given in Figure 3 and reveals a clear correlation between the C Pyr-Ph at 136 ppm and the C Ph-Pyr at 138 ppm (shown in orange in Figure 1(c) and 3), confirming the formation of the pyrenebenzene bond and the successful polymerization. Three other correlations were identified (shown in black, Figure 3), allowing full spectral assignment of CP-CMP10 (Figures 3 and 4). The resonances of C IV Pyr and C′H Pyr overlap at 126 ppm, and thus in the second dimension their respective correlations with C Pyr-Ph are also unresolved.
To confirm this assignment, the DNP enhanced 13 C CP MAS NMR spectra of the homopolymers CP-CMP1 and CP-CMP15 are given in Figure 4, parts a and e; while the 13 C NMR spectrum of the entirely di-or tetra-substituted benzene polymer CP-CMP1 shows two distinct resonances at 138 and 128 ppm (assigned by 13 C− 13 C correlation experiment to the quaternary C Ph-Ph , and CH Ph respectively, details given in proceeding paragraphs), the spectrum of homocoupled pyrene, CP-CMP15, displays signals at 134, 128, and 124 ppm that are assigned to C Pyr-Pyr , C IV Pyr , C′H Pyr , and CH Pyr using a combination of short contact time cross-polarization and previous literature. 72 More importantly, both C Ph-Ph and C Pyr-Pyr quaternary carbons, which are typical of the benzene and pyrene moieties, appear at slightly different shifts, enabling observation of both pyrene and benzene monomers in the CP-CMP9, CP-CMP10, and CP-CMP11 polymers (Figure 4b−d). For example, the 13 C spectrum of CP-CMP9 displays both C Ph-Pyr and C Pyr-Ph resonances in addition to three others assigned to protonated carbons (vide inf ra). Note that although seven chemically inequivalent carbon environments are anticipated in CP-CMP9, only five 13 C NMR signals can be resolved (Figures 3 and 4), likely due to the substantial inhomogeneous line broadening and short T 2 ′ times. All five resolvable resonances of CP-CMP9 are also present in the DNP spectrum of CP-CMP10 albeit with slightly different intensities; this is consistent with a different ratio of the same monomeric units used during synthesis (Table 1, Figure 1). The DNP-enhanced 13 C CP MAS NMR spectrum of CP-CMP11 is very similar to those of CP-CMP9 and CP-CMP10, albeit with possibly an additional low intensity resonance at 134 ppm corresponding to a quaternary pyrene carbon directly bonded to another pyrene molecule (C Pyr-Pyr ); based on the monomer feed ratio this signal should only be present in one out of every 20 polymeric repeat units. Despite the inherent low intensity of this peak, it is observable within 20 min with DNP, and deconvolution of these spectra allows visualization of these changes with respect to the monomer feed (Figure 4).   13 C CP (green) and multiCP (light green) MAS NMR spectra of (a−e) CP-CMP1-15 recorded at ν 0 ( 1 H) = 400.07 MHz, with μw on (green), simulated (dashed black), spectral deconvolution (dashed gray) and difference between experimental and simulated spectra (solid gray). Left is the 13 C DNP enhancement and overall gain, and on the right is the pyrene to benzene unit ratio of the monomer feed.

Article
Quantifying Enhancement Using Overall DNP Gain Factor Σ † . In order to better reflect on the large enhancements observed, an overall DNP gain factor, Σ † C CP was also calculated (Table S2). 37,71,73,74 Σ † is a comparison of the 13 C DNP enhanced spectrum vs a standard 400 MHz NMR spectrum obtained at room temperature, a full discussion of which is beyond the scope of this work and is provided elsewhere. 37,71,73−75 Σ † compensates for weight, and accounts for time saving, signal bleaching due to introduction of paramagnetic radicals and temperature differences, and estimates the overall benefit of DNP (see section S4 of the Supporting Information to calculate these values). The Σ † C CP values determined for CP-CMP9, CP-CMP10, and CP-CMP11 are all around 140, showing time efficient acquisition of high signal-tonoise 13 C NMR spectra. The Σ † C CP values for CP-CMP1 and CP-CMP15 were a little lower than for the copolymers, a similar trend to that observed for their ε C CP . Although, this disparity is not immediately attributable to any one physical property (such as SA BET ), the two homopolymers are significantly different systems from the copolymers, and the result is reproducible. Note that there is a large paramagnetic bleaching effect (θ values between 0.2 and 0.4, Table S1); the large surface area of these materials offers intimate distribution of radical leading to a greater bleaching, although the signal bleaching is constant within a monomeric unit of the polymer.
DNP MultiCP at 400 MHz. While the DNP-enhanced 13 C CP MAS NMR spectra of selected CP-CMPs confirm that the final macromolecular structure is directly related to monomer feed ratio, quantitative data are needed to determine the polymer compositions and were obtained by recording 13 C multiCP DNP NMR experiments. 46−49 This methodology provides a robust quantification approach 51 that is also time efficient (versus alternative methods such variable contact times CP experiments) and allows assignment of polymeric structure which can be cross checked with monomer feed ratio ( Table 2). It has previously been reported that the enhancement of DNP can appear nonuniform in heterogeneous systems, due to microwave induced sample heating and temperature dependent relaxation times. 41 In the CP-CMP systems we investigated, the DNP enhancements observed are homogeneous throughout the 13 C NMR spectra ( Figure S6) due to the similar environments and relaxation times of all carbon resonances as well as the porosity of the materials leading to radical distribution throughout the system, facilitating 1 H− 1 H spin diffusion for homogeneous polarization transfer. The polymers studied met all conditions for the multiCP spectra as given in previous work (τ DNP ( 13 C) greatly exceeded 500 s as shown in Figure S7, satisfying τ DNP ( 13 C) > 10 × τ DNP ( 1 H), contact time <10% T 1ρ ( 1 H)), 49,51 a full discussion of which can be found in section S5 of the Supporting Information.
The DNP enhanced 13 C multiCP MAS NMR spectra of CP-CMP1−15 are shown in Figure 4, parts a−e, alongside the spectral simulation and difference between experimental and simulated data, while Table 2 provides a comparison between the predicted carbons ratio based on the monomers feed with the 13 C NMR data integration (examples of the full spectral fit can be found in Figure S8). The difference in integration between multiCP and CP spectra can be found in Table S3. Both homopolymers CP-CMP1 and CP-CMP15 were quantified using DNP multiCP (Figure 4, parts a and e) as an internal standard, both showing integrations closely matching their theoretical ratios from monomer feed ( Table  2). As the covalent geometry of both benzene and pyrene are known, the relative integration ratios of resonances were fixed to one another for deconvolution purposes, in order to elucidate the relative stoichiometry of benzene to pyrene more accurately.
In CP-CMP10, the equal stoichiometry of pyrene and benzene monomers reported in Table 2 is readily visualized by the equal integration of C Ph-Pyr (138 ppm) and C Pyr-Ph (136 ppm). The integration ratios of the pyrene compared to the benzene resonances obtained in CP-CMP9 matches the monomer feed (Table 2), notably showing the greater integration of the C Ph-Pyr /C Ph-Ph signal (138 ppm) compared to the C Pyr-Ph peak (at 136 ppm) and representing a larger concentration of benzene than pyrene units in the polymer network.
The multiCP spectrum of CP-CMP11 also shows that the unique C Pyr-Pyr carbon environment in this polymer (134 ppm) integrates consistently with a pyrene−pyrene component being present on average once in every 20 repeat units. From the full polymeric assignments made possible by the INADEQUATE spectrum, it was possible to relate the final structures with the monomer ratio and, within error, showing stoichiometric uptake of each monomer, giving a polymer network that reflects the feed ratio.

CONCLUSION
We have demonstrated that DNP permits the fast acquisition of high signal-to-noise ratio 13 C CP MAS NMR spectra of amorphous polymeric networks assembled from pyrene and benzene units and enables the observation of carbon environments that appear rarely in the repeating units (e.g., once in every 20). The gain of sensitivity allows natural abundance 13 C− 13 C correlation spectra of these amorphous polymers to be obtained, facilitating the 13 C NMR spectra assignments. DNP combined with the multiCP approach enabled quantitative 13 C NMR spectra to be recorded and yield the polymers' compositions which compare well with the monomer feed ratio. This work establishes the polymer composition and allows trends in band gap 8 to be directly related to the polymeric structure rather than inferring this from the monomers feed.

* S Supporting Information
The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acs.macro-