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Asymmetric retro-[1,4]-Brook rearrangement of 3-silyl allyloxysilanes via chirality transfer from silicon to carbon

Ya Wua, Hua Chenb, Wenyu Yangb, Yu Fanb, Lu Gao*b, Zhishan Suc, Changwei Huc and Zhenlei Song*b
aDepartment of Biological and Chemical Engineering, Chongqing University of Education, Chongqing 400067, China
bSichuan Engineering Laboratory for Plant-Sourced Drug, Research Center for Drug Industrial Technology, Key Laboratory of Drug-Targeting and Drug Delivery System of the Education Ministry, West China School of Pharmacy, Sichuan University, Chengdu, 610041, China. E-mail: lugao@scu.edu.cn; zhenleisong@scu.edu.cn
cKey Laboratory of Green Chemistry & Technology, Ministry of Education, College of Chemistry, Sichuan University, Chengdu, 610064, China

Received 17th July 2019 , Accepted 9th August 2019

First published on 21st August 2019


Abstract

An asymmetric retro-[1,4]-Brook rearrangement of 3-silyl allyloxysilanes has been developed via Si-to-C chirality transfer. Mechanistic studies reveal that the silyl group migrates with retention of configuration. The stereochemical outcome of the newly formed stereogenic carbon center, which has remained a longstanding question, is also clarified, suggesting a diastereoselective Si to C chirality transfer without loss of enantiomeric excess.


Introduction

Intramolecular O-to-C silyl migration, now called retro-Brook (or West) rearrangement, was first reported by Speier and later systematically studied by West.1 The retro-Brook rearrangement occurs only under special circumstances2 and so has been less investigated than Brook rearrangement.3 But, it comprises a powerful synthetic tool because diverse organosilanes could be constructed from more accessible silyl ethers by a rapid and regio- and stereoselective manner. A covalent Si–O bond is cleaved and a Si–C bond is formed via silyl migration. Thus, the stereochemical courses at the migrating silicon center and the stereochemical control at the forming carbon center comprise two important stereochemical issues. Tomooka and co-workers4 reported the first example of practically useful level of retro-[1,4]-Brook rearrangement of allyloxysilane by use of HMPA as a co-solvent. In this work, they also showed, for the first time, that the silyl migration proceeded with retention of configuration at the silicon center (Scheme 1). In contrast, more efforts have been directed toward diastereoselective formation of the Si–C bond to generate synthetically useful chiral organosilanes. Nearly all previous studies have used stereogenic C1,2b,d,e C2 (ref. 2h) or C3 (ref. 2a and j) centers in substrate I to control diastereoselective formation of the Si–C bond in III. When the migrating silicon is stereogenic,5 it might be used as a stereochemical controller by Si to C chirality transfer, which was redefined by Oestreich.6 Achieving this in practice is quite challenging. There are only two examples we know come from a preliminary study by Tomooka and co-workers.4 The 3-Me allyloxysilane with SiOMePht-Bu as the migrating silyl group afforded a dr of 83[thin space (1/6-em)]:[thin space (1/6-em)]17, while the corresponding 3-SiMe3 allyloxysilane only migrated with a dr of 66[thin space (1/6-em)]:[thin space (1/6-em)]34. In both cases, the stereochemistry of the formed stereogenic carbon center were not determined.
image file: c9ra05482k-s1.tif
Scheme 1 Diastereoselective retro-Brook rearrangement.

Oestreich rationalized the difficulties in achieving high diastereoselectivity during Si-to-C chirality transfer as follows.6 The relatively long Si–C bond disfavors formation of a compact transition state II, which weakens diastereoselectivity. At the same time, all three substituents on the migrating silyl group can affect the stereochemical course, requiring the careful selection of three substituents that together allow efficient stereochemical control. Despite these difficulties, Oestreich described an intermolecular Pd- catalyzed asymmetric hydrosilylation using chiral silane (Scheme 2a),7 and Leighton demonstrated an intramolecular Hosomi–Sakuraiallylation involving a chiral allylsilane intermediate (Scheme 2b).8 In both of these cases, either cyclic silanes or acyclic silane with three distinct, sterically demanding substituents were used to achieve the high stereochemical control.


image file: c9ra05482k-s2.tif
Scheme 2 Chirality Transfer from Silicon to Carbon.

Here we report an asymmetric retro-[1,4]-Brook rearrangement of 3-silyl allyloxysilanes 1 via an efficient Si-to-C chirality transfer (Scheme 2c). The combination of SiMePht-Bu as the migrating silyl group and SiPh3 as the terminal silyl group proved most effective, giving geminal bis(silyl) aldehyde 3 and enol derivatives 4 in good yield with high diastereoselectivity. The overall stereochemical outcome of the migrating silicon center and the newly formed carbon center were clarified by detailed mechanistic studies.

Results and discussion

This project arose from our interest in developing chiral geminal bis(silanes) reagents and synthons.9 These species contain two different silyl groups, making the carbon to which they are attached a stereogenic center. In previous work, we achieved asymmetric C–C or C–H bonds formation via 3,3-sigma tropic rearrangement of optically pure 3,3-bis(silyl) allylic alcohols, allowing asymmetric synthesis of crotyl geminal bis(silanes).10 We were curious whether asymmetric C–Si bond formation could be another efficient strategy to construct chiral geminal bis(silanes). Our s-BuLi-promoted retro-[1,4]-Brook rearrangement of 3-silyl allyloxysilanes11 appeared to be a suitable model to test this possibility. The reaction tolerates a wide range of migrating and non-migrating silyl groups, making it practical for identifying the best pair of silyl groups.

We initially fixed t-BuPhMeSi as the migrating silyl group (Table 1). Entries 1–7 showed an obvious steric bias for the non-migrating silicons (Si1) at the 3-position of 1. When Si1 was an SiMe3 group, geminal bis(silyl) aldehydes 3a were generated as a nearly 1[thin space (1/6-em)]:[thin space (1/6-em)]1 mixture of two diastereomers (entry 1). Even when one methyl was replaced with a phenyl group, dr did not improve for the corresponding products 3b (entry 2). These results imply that the small methyl group does not permit good diastereochemical control. Diastereoselectivity improved progressively when steric demand at Si1 increased from SiMe3 to SiEt3, Si(n-Pr)3, Si(i-Pr)3 and finally SiPh3 (entries 3–6). The largest SiPh3 group imposed the strongest stereochemical control, providing 3f at the highest dr of 90[thin space (1/6-em)]:[thin space (1/6-em)]10 (entry 6). Interestingly, an inverse steric bias for Si1 was observed when the migrating silicon was switched from t-BuPhMeSi to 1-NpPhMeSi. The largest SiPh3 group afforded a dr of only 65[thin space (1/6-em)]:[thin space (1/6-em)]35, while the smallest SiMe3 provided the best dr of 86[thin space (1/6-em)]:[thin space (1/6-em)]14 (entries 7–9). We also tested the silicon combination in which the t-BuPhMeSi functioned as a chiral auxiliary, while SiPh3 migrated (entry 10). The reaction gave the aldehyde 3f with a dr of 74[thin space (1/6-em)]:[thin space (1/6-em)]26 lower than that obtained in entry 5.

Table 1 Screening of Silyl Groupsa

image file: c9ra05482k-u1.tif

Entry Sub. Si1 Si2 Prod. Yieldb drc
a Reaction conditions: 1 (0.15 mmol), s-BuLi (0.60 mmol), HMPA (0.6 mmol), 0.5 mL of THF, at −78 °C for 0.5 h, then H2O at rt overnight.b Isolated yields.c Ratios were determined from 1H NMR analysis of crude product.
1 1a Me3Si t-BuPhMeSi 3a 62% 56[thin space (1/6-em)]:[thin space (1/6-em)]44
2 1b Me2PhSi t-BuPhMeSi 3b 65% 47[thin space (1/6-em)]:[thin space (1/6-em)]53
3 1c Et3Si t-BuPhMeSi 3c 53% 67[thin space (1/6-em)]:[thin space (1/6-em)]33
4 1d (n-Pr)3Si t-BuPhMeSi 3d 50% 65[thin space (1/6-em)]:[thin space (1/6-em)]35
5 1e (i-Pr)3Si t-BuPhMeSi 3e 45% 83[thin space (1/6-em)]:[thin space (1/6-em)]17
6 1f Ph3Si t-BuPhMeSi 3f 60% 90[thin space (1/6-em)]:[thin space (1/6-em)]10
7 1g Ph3Si 1-NpPhMeSi 3g 65% 65[thin space (1/6-em)]:[thin space (1/6-em)]35
8 1h Et3Si 1-NpPhMeSi 3h 73% 83[thin space (1/6-em)]:[thin space (1/6-em)]17
9 1i Me3Si 1-NpPhMeSi 3i 63% 86[thin space (1/6-em)]:[thin space (1/6-em)]14
10 1j t-BuPhMeSi Ph3Si 3f 55% 74[thin space (1/6-em)]:[thin space (1/6-em)]26


Next we examined the scope of electrophiles for quenching the lithium enolate intermediate generated from 1f. The reaction tolerated triethylsilyl chloride (entry 1), various acyl chlorides (entries 2–9) and chlorocarbonates (entries 10 and 11) to provide 3,3-bis(silyl) enol derivatives 4 in good yields with high diastereoselectivity (Table 2). The enol double bond formed exclusively with Z-selectivity. The relative stereochemistry of the products was unambiguously established based on X-ray diffraction analysis of 4d crystals.12 Methyl iodide was also a suitable electrophile, but less reactive than acyl chloride, giving 4l in 40% yield with O-alkylation selectivity (entry 12).

Table 2 Scope of Electrophilesa

image file: c9ra05482k-u2.tif

Entry Electrophiles Product Yieldb
a Reaction conditions: 1f (0.15 mmol), s-BuLi (0.60 mmol), HMPA (0.6 mmol), 0.5 mL of THF, at −78 °C for 0.5 h, then electrophile at rt for 2 h.b Isolated yields.c Ratios were determined from crude 1H NMR analysis of product.d 10.0 equiv. of MeI.
1 Et3SiCl image file: c9ra05482k-u3.tif 4a (60%)
2 image file: c9ra05482k-u4.tif image file: c9ra05482k-u5.tif 4b (R = H, 65%)
3 4c (R = Br, 65%)
4 4d (R = NO2, 60%)
5 image file: c9ra05482k-u6.tif image file: c9ra05482k-u7.tif 4e (67%)
6 image file: c9ra05482k-u8.tif image file: c9ra05482k-u9.tif 4f (50%)
7 image file: c9ra05482k-u10.tif image file: c9ra05482k-u11.tif 4g (66%)
8 image file: c9ra05482k-u12.tif image file: c9ra05482k-u13.tif 4h (R = Me, 50%)
9 4i (R = Ph, 55%)
10 image file: c9ra05482k-u14.tif image file: c9ra05482k-u15.tif 4j (R = Me, 70%)
11 4k (R = Ph, 70%)
12 Meld image file: c9ra05482k-u16.tif 4l (40%)
image file: c9ra05482k-u17.tif image file: c9ra05482k-u18.tif


The silicon can migrate with either retention or inversion of configuration. Thus, the relative stereochemistry of 3f may not reflect the stereochemical course of the migrating silicon, or how it controls the stereochemical outcome of the resulting stereogenic carbon center. In particular, if the enantiomerically defined silyl group racemizes during migration, the carbon center can be constructed diastereoselectively, but not enantioselectively. The observation by Tomooka and co-workers that silicon migrates with retention of configuration in their simple allyloxy system4 does not necessarily apply to our case, since the non-migrating silicon may affect the stereochemical course. To gain a definitive answer to this question, we used enantiomerically defined 10 as a stereochemical probe (Scheme 3).13 Following the procedure developed by Oestreich,14 a 1[thin space (1/6-em)]:[thin space (1/6-em)]1 mixture of 5 was separated by several cycles of silica gel chromatography, affording 6 in diastereomerically pure form. Reduction of 6 with DIBAL-H provided hydrosilane 7 in 77% yield. Subsequent chlorination of 7 with CCl4 delivered chlorosilane 8, which directly reacted with the potassium salt of 9, giving 10 in 90% yield. The high er of 10 (96[thin space (1/6-em)]:[thin space (1/6-em)]4) suggests that transformation from 6 to 10 proceeds in a stereospecific manner at the silicon center, and should follow the known sequence of retention-retention-inversion.15 Thus, the absolute configuration of the silicon in 10 was assigned as R. Under the optimal retro-[1,4]-Brook rearrangement conditions, 10 was converted into aldehyde 11. The major isomer showed an er of 96[thin space (1/6-em)]:[thin space (1/6-em)]4, indicating that the silicon migrated stereospecifically. X-ray diffraction analysis of 1116 unambiguously confirmed the R-configuration of the silicon, indicating that migration proceeds with retention of configuration as in Tomooka's case. The X-ray diffraction analysis of 11 also established the S-configuration of the new stereogenic carbon center. The result revealed that the migration proceeded by a diastereoselective Si to C chirality transfer without loss of enantiomeric excess.


image file: c9ra05482k-s3.tif
Scheme 3 Preparation of enantiomerically defined 10 and its retro-[1,4]-Brook rearrangement to form 11.

A plausible mechanism to explain our results is proposed in Scheme 4, based on the model we proposed for the racemic version of the reaction.11 The α-deprotonation of 10 gives the corresponding allylic anion, which adopts the endo-orientation assisted by Li–O coordination.17 The O-to-C silyl migration takes place irreversibly via two possible pentacoordinated silicate transition states or intermediates, TS-1 and TS-2.18 In this way, the configuration of the silicon center is retained without racemization. While TS-2 suffers a severely steric repulsion between the Ph group on Si1 and one of the Ph groups on Si2, the interaction between the Me group on Si1 and the Ph group on Si2 appears being tolerable in the case of TS-1. These considerations are supported by the preliminary results from density functional theory calculations, which showed TS-1 to be more stable than TS-2 by 6.2 kJ mol−1. Our model also explains the observed steric bias for substituents on Si1. Substituents smaller than the Ph group might not be large enough to create an appreciable difference between the non-bonded interaction with the Me group in TS-1 and with the Ph group in TS-2. As a result, 3 forms with poor diastereoselectivity (Table 1, entries 1–4).


image file: c9ra05482k-s4.tif
Scheme 4 Plausible reaction mechanism.

Conclusions

In summary, Si-to-C chirality transfer has been used as an efficient strategy to achieve asymmetric retro-[1,4]-Brook rearrangement of 3-silyl allyloxysilanes. The SiMePht-Bu and SiPh3 groups, in which SiMePht-Bu migrates, function as the best combination to give geminal bis(silyl) aldehyde and enol derivatives with high diastereoselectivity. The silyl group migrates with retention of configuration. Enantioselective generation of the stereogenic carbon center suggests that Si-to-C chirality transfer is a promising method to construct optically pure chiral organosilanes. Further applications of this strategy are being explored in our group.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

We are grateful for financial support from the NSFC (21622202, 21502125).

Notes and references

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Footnote

Electronic supplementary information (ESI) available: Experimental procedures, characterisation data for new compounds. CCDC 1901967 and 1901968. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c9ra05482k

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