Song
Liu
*abc,
Dianmin
Zhang
a,
Min
Xiao
a,
Chengling
Pu
a,
Xiaoqing
Zhang
a,
Xiuwen
Yang
a,
Tao
Zhang
*d and
Ruopeng
Bai
*b
aChongqing Key Laboratory of Environmental Materials and Remediation Technologies, College of Chemistry and Environmental Engineering, Chongqing University of Arts and Sciences, Chongqing, 402160, P. R. China. E-mail: sliu@cqwu.edu.cn
bSchool of Chemistry and Chemical Engineering, Chongqing University, Chongqing 400030, China
cChongqing Precision Medical Industry Technology Research Institute, Chongqing 400084, P. R. China
dZhengZhou JiShu Institute of AI Science, Zhengzhou, Henan, China 450000
First published on 24th November 2022
C–N bond metathesis is a straightforward and step-economical approach for C–N bond construction. Typically, the oxidation state of the transition metal remains unchanged during C–N bond metathesis. In this report, we present computational evidence that supports a mechanism in which a new type of reversible reductive elimination/oxidative addition mode is involved in the C–N bond metathesis reaction. This reversible reductive elimination/oxidative addition-induced C–N bond metathesis pathway was found to be lower in energy compared with transimination from a Huang-complex, which is important for understanding the mechanism of Pd-catalyzed C–N bond formation reactions. Non-covalent interaction analysis was conducted to elucidate the details of the diene 1,4-migratory insertion step process and to investigate the origin of stereoselectivity for this type of reaction. We anticipate that this novel C–N bond metathesis mode may extend to other cross-coupling processes and may provide a theoretical guide for further experimental investigations.
According to previous studies in this area, three possible reaction strategies were developed for the C–N bond metathesis (Scheme 1). In strategy A, the imine CN metathesis transfers an amine moiety in a manner analogous to alkene metathesis, which proceeds through a metal-nitrene-containing reversible [2 + 2] cycloaddition followed by a cycloreversion reaction (Scheme 1a).4 This strategy has been leveraged for the development of transition metal-catalyzed imine metathesis, which was reported by Bergman,4a,b Meyer,4c–e Mountford,4f Espenson4g and Bruno.4h In strategy B, two new amide C–N bonds can also be constructed via reversible carbonyl insertion/β-N elimination (Scheme 1b).5 Under the guidance of this principle, Gellman and Stahl documented the successful and elegant Zr-catalyzed C–N/C–N metathesis of tertiary amides.5 Moreover, a hydrogen-borrowing strategy, proceeding via the removal of hydrogen from an amine, transimination and return of the hydrogen from the catalyst, can also be applied for N–H/C–N metathesis reactions between two amines (Scheme 1c).6 Notably, nucleophilic addition of an amine to an imine, 1,3-proton transfer and elimination are involved in this transimination step. Recently, this hydrogen-borrowing strategy has attracted close attention for C–N metathesis. For example, Concilio et al. demonstrated the formation of a secondary amine from the parent primary amine using an Ru catalyst.6a,b Beller's group also developed successful N–H/C–N metathesis reactions between arylamines and primary amines.6c In addition, Williams and co-workers found that primary amines could be selectively alkylated with diisopropylamine in the presence of an Ir catalyst.6d Among these strategies, we found that the processes involved in C–N metathesis are usually reversible and the oxidation state of the transition metal remains unchanged during this step.
Although the above three C–N metathesis modes are commonly used as effective strategies in transition metal-catalyzed C–N bond formation reactions, the lack of a new type of reaction mode for C–N metathesis has hampered the development of constructing new C–N bonds in organic synthesis.2 In 2020, Huang and co-workers developed a new mode, proceeding through a reversible reductive elimination, 1,3-proton transfer, and oxidative addition sequence, to realize C–N bond metathesis.7 But the detailed mechanism and computational evidence for this new type of C–N bond metathesis is still not clear, which limits the development of such C–N bond metathesis reactions. In this reaction, the C–N bond metathesis was proposed to occur from an active Huang-complex. Notably, the iminium-coordinated Pd(0) cationic complex was one limiting resonance form of the active Huang-complex, which was confirmed by our previous DFT calculations.8 Thus, we propose that this reaction may also proceed via a transimination mechanism to realize C–N and N–H exchange (Scheme 2).9 With this in mind, we performed density functional theory (DFT) calculations to investigate the mechanism of this new Pd-catalyzed C–N bond metathesis and ring-closing reaction. The competition between the proposed reversible reductive elimination/oxidative elimination-induced C–N bond metathesis and transimination was investigated. A detailed reaction mechanism and reactivity profile for this reaction were revealed. Furthermore, the origin of enantioselectivity established by a chiral P–N ligand was also elucidated. The calculated results presented herein would provide a theoretical guide for further experimental investigations of C–N bond metathesis reactions.
ΔGM06/solvent = ΔEM06/solvent + ΔGcorrection/gas | (1) |
We also performed benchmarks for some frequently used calculation methods (see the ESI for details†). The calculated results indicated that this method used herein is reliable. The optimized structures were shown using CYLview.14
The calculated free energy profiles for the transimination mechanism are shown in Fig. 1. The dissociation of palladacycle-complex CP1 into an imine cation and Pd(0) occurs through two steps via transition states TS1 and TS2. The energy barrier for the dissociation of the amino from the Pd center was 11.3 kcal mol−1. In TS1, the length of the C–N bond being broken was 2.80 Å. From TS1, alkyl-Pd(II) intermediate CP2 was generated. The subsequent dissociation of the C–Pd bond occurs via transition state TS2 with an energy barrier of 12.2 kcal mol−1 to give CP3. In CP3, the Pd(0) was bonded to imine cations by two hydrogen bonds. After the dissociation of Pd(0), the imine cation was generated. The free energy of imine cation CP4 and Pd(0) was 24.3 kcal mol−1. The subsequent nucleophilic addition of the diene-tethered amine substrate to the imine cation occurred through transition state TS3 with an activation free energy of 31.6 kcal mol−1 to give amino cation intermediate CP5. Another pathway, the nucleophilic addition of the diene-tethered amine substrate to the imine in CP3, was also analyzed. The nucleophilic addition transition state TS4 has an energy barrier of 8.1 kcal mol−1 relative to CP3, and gave the amino cation Pd(0) intermediate CP6. Due to the high activation free energy of TS3 and TS4, the transimination process does not readily occur under the current reaction conditions at a temperature of 30 °C. The calculated results also indicate that no imine cation exists in the reaction system, and palladacycle-complex CP1 is the active catalyst in the catalytic cycle.
The calculated Gibbs energy profiles for the Pd-catalyzed reductive elimination/oxidative addition-induced C–N bond metathesis are presented in Fig. 2, where the (Xantphos)Pd-(CH2NBn2)+ Huang-complex CP1 was also set as the relative zero point. Because CP1 can be described as a resonance form of the square-planar nitrogen-coordinated aminomethyl-Pd(II) and triangular iminium-coordinated Pd(0) complex, the iminium cation group in CP1 is electrophilic enough to be attacked by exogenous secondary amine 1via transition state TS5 to form amino cation Pd(0) intermediate CP6. In CP6, there is a hydrogen bond between the hydrogen atom in the methylene group and the Pd(0) center. The calculated free energy barrier of this step was 23.9 kcal mol−1. The structural information of TS5 shows that the lengths of the C–N bond being formed and the C–Pd bond being broken were 2.27 and 3.15 Å, respectively. Notably, TS5 can also be considered as a reductive elimination transition state because Pd(0) was generated. The rapid proton transfer in CP6 gave another amino cation Pd(0) intermediate CP7. Subsequent oxidative addition of CP7 to the Pd(0) center occurred via transition state TS6 with an energy barrier of only 6.9 kcal mol−1 to generate CP8 with a concomitant release of an amine. In TS6, the lengths of the C–N bond being broken and the C–Pd bond being formed were 2.14 and 3.13 Å, respectively. The calculated results show that the desired C–N bond metathesis is furnished through a reversible process involving reductive elimination, hydrogen transfer, and oxidative addition. The overall activation free energy for this type of C–N bond metathesis was only 23.9 kcal mol−1, which is 5.8 kcal mol−1 lower than that of the transimination pathway via transition state TS4. This indicates that the reductive elimination/oxidative addition-induced C–N bond metathesis pathway is more favorable than transimination. Our theoretical studies also indicated that due to the participation of palladium, the imine cation generated online becomes stable and Huang-complex CP1 was generated. Because CP1 can be described as a triangular iminium-coordinated Pd(0) complex, the iminium cation group in CP1 can be attacked by a secondary amine directly, without dissociation of Pd(0), which results in this reaction via the C–N bond metathesis mechanism rather than transamination.
Owing to the stronger basicity of the secondary amine compared with that of the aminal, the amine substrate 1 would promote a rapid hydrogen transfer process (Fig. 2). The isomerization of amino cation Pd(0) intermediate CP6 gives intermediate CP9, in which the terminal alkene coordinates with the Pd(0) center. Then, intermolecular hydrogen transfer from CP9 to secondary amine substrate 1 occurs via transition state TS7 with an energy barrier of only 3.1 kcal mol−1. In this process, complex CP10 and secondary amine cation 1′ are generated. The subsequent intermolecular hydrogen transfer from 1′ to the terminal amino in CP10 gives the amino cation intermediate CP11via transition state TS8 with a free energy barrier of 13.6 kcal mol−1. CP11 then isomerizes to amino cation Pd(0) intermediate CP7. The direct intramolecular hydrogen transfer of CP8 has also been calculated. The results also show that the free energy of the direct intramolecular hydrogen transfer transition state TS9 is 16.3 kcal mol−1 higher than that of transition state TS8, which indicates that secondary amine substrate 1 promoted rapid hydrogen transfer process is more favorable. The calculated results also show that this secondary amine-promoted rapid hydrogen transfer process is reversible.
Based on the above-calculated results, we proposed a catalytic cycle for the palladium-catalyzed C–N bond metathesis for the ring-closing aminomethylamination reaction, where the Huang-complex A is set as the active catalytic complex (Scheme 4). The reversible reductive elimination, hydrogen transfer, and oxidative addition first induce the C–N bond metathesis. The generated palladacycle-complex intermediate D isomerizes to E, in which the internal alkene coordinates with the Pd(II) center. The subsequent intramolecular alkene migratory insertion generates the π-allylpalladium species F, which is intercepted by an aminal to form intermediate Gvia an SN2-type reductive elimination process. Finally, the SN2-type oxidation addition of the amino cation to the Pd(0) center delivers the saturated N-heterocycle together with regenerating the active palladium-complex A to complete the catalytic cycle.
Scheme 4 The proposed mechanism for the palladium-catalyzed C–N bond metathesis for ring-closing aminomethylamination reaction. |
Fig. 3 shows the free energy profiles for the migratory insertion of an internal alkene. The dissociation of the amino group and coordination of the internal alkene in palladacycle-complex intermediate CP8 forms cationic Pd(II) intermediate CP12. Migratory insertion of the internal alkene into the C(alkyl)–Pd bond was calculated to proceed via transition state TS10 with an energy barrier of 21.9 kcal mol−1. Alternatively, dissociation of the amino group and coordination of the terminal alkene in CP8 generate cationic Pd(II) intermediate CP13. Subsequent 1,4-insertion of the conjugated diene into the C(alkyl)–Pd bond gives the π-allylpalladium species CP14via transition state TS11. In transition state TS11, the lengths of the C–Pd bond being broken and the C–C bond being formed were 3.45 and 3.28 Å, respectively. The calculated free energy for TS11 was 16.7 kcal mol−1 lower than that of TS10, which indicates that the 1,4-insertion pathway is favorable. In addition, 1,2-insertion of the terminal alkene was also calculated. The calculated free energy for the 1,2-insertion of terminal alkene transition state TS12 was 48.4 kcal mol−1, which is 33.2 kcal mol−1 higher than that of TS11. Therefore, the 1,2-insertion of the terminal alkene pathway is also unfavorable.
The aminals used in this reaction system contain two tertiary amine moieties; each end of the nucleophile can potentially act as a nucleophile. Therefore, although the basicity of the aminal is lower than that of Bn2NH and aminodiene, the nucleophilicity of the aminal should be stronger than that of Bn2NH and aminodiene. It is reasonable that the more nucleophilic aminal should be the preferred agent to trap the π-allylpalladium intermediate to give the desired product. As shown in Fig. 4, π-allylpalladium species CP14 would be intercepted by an aminal via SN2-type reductive amination transition state TS13 with an energy barrier of 26.5 kcal mol−1 to form the alkene-coordinated Pd(0) complex CP15. In TS13, the length of the C–N bond being formed was 1.91 Å. The subsequent oxidative addition of the C–N bond to the Pd(0) center via transition state TS14 delivers saturated N-heterocycle product 3 together with regenerating the active palladium-complex CP1 to complete the catalytic cycle. The lengths of the C–N bond being broken and the C–Pd bond being formed in TS14 were 2.15 and 3.42 Å, respectively. The calculated results show that the reductive amination is the rate-limiting step, which is consistent with the inverse secondary kH/kD = 0.86 ± 0.2 observed in the competition experiments between aminodiene and deuterated aminodiene. The overall activation free energy for this reaction was 26.5 kcal mol−1, corresponding to the free energy difference between transition state TS13 and intermediate CP14. The π-allylpalladium species CP14 is the resting state in the catalytic cycle, which is also consistent with the dynamic experimental results.
Fig. 4 The calculated free energy profiles for amination. Values for bond lengths are given in angstroms. |
A primary enantioselective reaction was also established using chiral Pd/ligand complexes. As shown in Scheme 5, when a chiral phosphinamide ligand was used, chiral N-heterocyclic products were generated in 78% yield and 81% ee. DFT calculations were further performed to illustrate the enantiocontrol in this reaction.
The above calculations indicate that the stereoselectivity for this Pd-catalyzed C–N bond metathesis and ring-closing reaction is determined by the 1,4-insertion step. The calculated enantiotopic 1,4-insertion patterns of the two transition states (TS11-Si and TS11-Re) were examined. As shown in Fig. 5, the calculated relative energy of TS11-Si was 2.3 kcal mol−1 lower than that of TS11-Re, which is in accordance with the (R) selectivity observed experimentally. The structural information for TS11-Si and TS11-Re indicate that TS11-Re is generated posterior to TS11-Si as the C–C bond being formed in TS11-Si was 2.57 Å, while the C–C bond being formed in TS11-Re was 2.36 Å. The late transition state for TS11-Re results in its high relative energy.
Fig. 5 The calculated relative free energy for TS11-Si and TS11-Re. Values for bond lengths are given in angstroms. |
To better understand the origin of stereoselectivity in this type of reaction, NCI analysis was performed for the 1,4-insertion patterns of diene transition states TS11-Re and TS11-Si. As shown in Fig. 6, NCI calculations indicate that the steric repulsion of the terminal methylene in the chiral phosphinamide ligand in TS11-Re is stronger than that in TS11-Si, which contributes to the free energy difference between TS11-Re and TS11-Si. The structure information of TS11-Re and TS11-Si also indicated that the butadiene group is located at an axial bond in TS11-Re, and an equatorial bond in TS11-Si. The conformation of TS11-Re limits the position of the butadiene, which leads to the steric repulsion of the terminal methylene in the chiral phosphinamide ligand in TS11-Re stronger than that in TS11-Si.
Fig. 6 NCI calculations of TS11-Si and TS11-Re (blue is the attraction; green is the weak interaction; red is the steric effect). |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2qo01638a |
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