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Reactive Intermediate Chemistry

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HYDROGEN ATOM ABSTRACTION

415

allyl hydrogen from the matrix alkenes to form arylmethyl-allyl radical pairs. These then undergo recombination, after equilibration within the matrix, to give final products (Scheme 9.13).

PhCH ↑ ↓

+

 

 

 

 

 

Ph

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

56

 

 

 

 

 

 

 

PhCH ↑ ↑

+

 

 

 

 

 

PhCH2

 

 

 

 

PhCH2

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

58

 

(Z) - 59

(E) - 59

Scheme 9.13

Alcohols are also used as diagnostic reagents for the spin state of reacting carbenes. Thus, singlet carbenes are trapped very efficiently by the O H bond to produce ethers, whereas the triplets undergo abstraction of hydrogen atom from the C H bonds, not from the OH bond, leading to product mixtures resulting from radical pairs. Eventually, double hydrogen abstraction products and radical dimers are formed (see Scheme 9.6).

The reaction patterns of arylcarbenes with solidified alcohol at 77 K are also completely different from those observed in alcohol solution. For example, generation of phenylcarbene (1e) in methanol matrices at 77 K results in the formation of alcohol (63) at the expense of benzyl methyl ether (62), which is the exclusive product in the reaction in alcoholic solution at ambient temperatures (Scheme 9.14).88 A similar dramatic increase in the CH ‘‘insertion’’ products is observed in the reaction involving other carbenes with alcohols.89

•• PhCH

 

 

 

 

O

 

 

+

OH

 

PhCH2

+

+

OH

 

 

 

 

 

PhCH2

OH

PhCH2

1e

62

63

64

0 °C

83.5%

~ 0%

0%

−196 °C

20.8

64.2

4.8

Scheme 9.14

By analogy with the mechanism proposed for the reaction with alkenes, C H insertion product formation can be explained in terms of a H abstraction–recom- bination process of triplet arylcarbenes. The observations that ground-state singlet carbenes, for example, chlorophenylcarbene (67), produce only O H insertion

416 TRIPLET CARBENES

product even at 77 K again suggests that the ground-state triplet intervenes in the formation of C H insertion products.

5.4.2. Kinetics of Hydrogen Atom Transfer. Reactions in alcohols in alkene matrices clearly indicate that, as the temperature is lowered, the reactions of the singlet come to be suppressed and the singlet undergoes intersystem crossing to generate the triplet ground state. The triplet then abstracts hydrogen from the matrix molecules to produce ultimately C H insertion products. In a fluid solution at room temperatures, most carbenes react in the singlet state regardless of the ground state multiplicity.

It is not easy to explain why the triplet reactions that are energetically much less favored than those of the singlets become dominant at low temperature. Based on Ea and log A measured for triplet carbene abstraction (see Section 5.3), one can estimate the rate constant at 77 K to be <10 5 M 1 s 1, suggesting that triplet carbene reactions in matrices at 77 K should not occur. Obviously, reactions of carbenes within matrices are controlled by factors that are not operating in solution phase, as one might expect from dramatic changes in reaction conditions.

An explanation for this conundrum is provided by kinetic experiments using EPR. The EPR spectra of simple triplet carbenes such as DPC (14) and FL (23) are produced by brief photolysis of the corresponding diazo compounds in a series of organic matrices at low temperatures. The rate of signal disappearance is measured immediately after photolysis is discontinued. The decay of the triplet carbenes is attributed to hydrogen-atom abstraction from the matrix based mainly on the observation that the rate of carbene decay roughly follows the expected order of hydrogen-atom-donating ability of the matrix. It is also decreased upon perdeuteration of the matrix. Decay is not observed in perfluorinated matrices, which have no abstractable hydrogens. The decay curves of the triplet carbenes are not single exponential functions because of a multiple-site problem, as is observed in the dynamic behavior in polycrystalline solids. An absolute rate constant for a specific site is determined based on the assumption that the first 20% of the carbene decay corresponds to the decay of the carbene in a single site, and both the Arrhenius activation energy and preexponential factors are determined. The data listed in Table 9.10 suggest that the parameters are much smaller than expected

TABLE 9.10. Pseudo-First-Order Rate Constants and Arrhenius Parameters for the Decay of Triplet Ph2C: (14a) in Organic Glasses

Solventa

Temp ( C)

103k ðs 1=2Þ

log A ðs 1=2Þ

Ea (cal/mol)

MeOH MTHF

184

51

1.464

470

PrOH MTHF

184

41

0.328

920

MTHF

184

61

0.690

1291

PhMe

196

35.6

0.85

1219

C6D5CD3

196

5.2

1.14

1773

c-C6H12

137

32

 

 

aMethyltetrahydrofuran ¼ MTHF, c-C6H12 ¼ cyclohexane.

HYDROGEN ATOM ABSTRACTION

417

for classical hydrogen atom transfer. Thus, QMT is proposed to be the mechanism for the matrix hydrogen atom transfer. The observation that the carbenes are completely stable in CCl4 matrices at 77–100 K suggests that the light hydrogen atom can tunnel, but the more massive Cl atom cannot.90

The members of the radical pairs generated by the hydrogen atom abstraction of the triplet carbenes usually diffuse apart in fluid solution. Product mixtures consisting of radical dimers, double hydrogen abstraction products and so on are formed (Scheme 9.6). In a rigid matrix, however, the members of the pairs are not able to diffuse apart (owing to the limited diffusibility within the matrix) and therefore recombine with high efficiency to give the C H ‘‘insertion’’ products upon thawing the matrix.

A hydrogen atom transfer reaction in which the reaction mechanism changes from a completely classical process in a soft warm glass to a completely quantum mechanical tunneling process in a cold hard glass has been more evidently demonstrated by using a technique with greater time resolution than a conventional EPR method: LFP. Thus, LFP of diazofluorene in a number of glasses generates singlet FL(23), which undergoes intersystem crossing to triplet 23.91

In contrast to the EPR studies, exponential decays of the triplet 23 are observed. The Arrhenius treatment of the data obtained in hydrogen donating glasses shows that there are two regions; a steep region at high temperatures and a flat, temperature-insensitive region with very low-activation parameters. Upon extrapolation of the high-temperature data to the low-temperature regime, one finds that the observed rate is hundreds of times faster than predicted. No such break in the Arrhenius plot is observed for the decays of 23 in perhalogenated solvents, which have no abstractable hydrogens.92 Thus, these broken Arrehnius plots observed in hydrogen donating solvents are best explicable in terms of a change in the reaction mechanism.

5.4.3. Why Can the Triplet Find a Tunneling Pathway? The exact reason why triplets can find a tunneling pathway, whereas singlet carbenes cannot is not clear. However, recent investigations on the low-temperature hydrogenation of carbenes provide some clues concerning this issue. It has been shown that a carbene with a triplet ground state, for example, phenyltrifluoromethylcarbene (65) undergoes hydrogenation when generated at 10 K in 2% H2/Ar matrix, followed by warming to 30 K in the dark to give the corresponding reduction product (66, Scheme 9.15). On the other hand, a carbene with singlet ground state, for example, phenyl(chloro)carbene (67) does not react at all upon annealing in an H2-doped Ar matrix even at 35 K (Scheme 9.15). Moreover, 65 is completely unreactive with D2 under comparable conditions, suggesting the presence of a large kinetic deuterium isotope effect. The results are interpreted as indicating that the triplet reacts through hydrogen-tunneling abstraction followed by recombination of the resultant radical pair to give the reduction product, whereas the singlet, requiring concerted addition, does not undergo tunneling reaction under cryogenic conditions.93

Energetics of carbenes and hydrogen reactions have been calculated at the B3LYP/6-31G** level of theory. They indicate that all the H2 additions are

418 TRIPLET CARBENES

••

 

10→30 K

 

 

H = - 90.6 kcal/mol

CF3

 

 

CF3

 

 

H2 / Ar

 

 

H =

5.7 kcal/mol

65

 

 

66

 

 

••

 

 

 

 

 

 

Cl

 

10→30 K

 

Cl

H = - 80.4 kcal/mol

 

 

H2 / Ar

 

 

H =

12.4 kcal/mol

67

 

 

68

 

 

Scheme 9.15

be very exothermic ( 80 90 kcal/mol), including those of chlorophenylcarbene (67). Thus overall exothermicity does not appear to be the reason for the lack of reactivity of the singlet carbene. Concerted addition of H2 to 67 is calculated to have a barrier of 12.4 kcal/mol, while hydrogen abstractions from H2 by triplet carbenes (65) are predicted to have significantly lower energy barriers (5.7 kcal/mol). Based on these calculations, it is suggested that the direct insertion of singlet 67 via quantum mechanical tunneling is less facile than stepwise reaction of the triplet carbenes 65 with H2, either because of a higher classical barrier or because of the lower probability of QMT involving two hydrogens simultaneously. However, much more reactive singlet carbenes, such as difluorovinylidene (F2C C:) appear to surmount the restrictions on concerted additions even at very low temperatures.94

On the other hand, it has been shown that even at very low temperature highly electrophilic triplet carbenes undergo thermal H2 additions in H2–Ar matrix as well as C H insertion into CH4. For example, triplet tetrafluoro-4-oxocyclohexa-2,5- dienylidene (69a) generated in an H2-doped Ar matrix reacts with H2 even at 35 K to give tetrafluoro-4-oxocyclohexa-2,5-dienone (70a). It also reacts with CH4 at 40 K to give a formal C H insertion product (71a). Interestingly, no deuterium isotope effects are observed in this case; the same reaction takes place at qualitatively the same rate in D2 and CD4. The reactivity decreases on going from tetrachloro (69b) to tetrahydro derivatives (69c). The tetrahydro derivative does not react at all under the same conditions (Scheme 9.16). DFT calculations (B3LYP/6-31G(d)) predict that the reaction of carbene (69) with H2 to give cyclohexadienenone (70) is highly exothermic (91.4 and 73.8 kcal/mol for the fluoro and chloro derivatives, respectively) but do not reveal a transition state for the reaction. These calculations suggest a thermal reaction with an extremely small or absent barrier. This unusual reaction is explained in terms of the philicity of triplet carbene.95 It has been proposed that the electron affinities (EA) can be used as a measure of the carbene philicity. The EA values were calculated [B3LYP/6- 311 þþ G(d,p)] for fluoro (69a), chloro (69b), and hydro (69c) derivatives are 3.32, 3.08, and 2.05 eV, respectively.96 The EAs for phenyl chlorocarbene (singlet, 167) and diphenylcarbenes (314) are 1.52 and 1.48 eV, respectively. These are well below the electrophilicity of the hydro derivative (69c).

 

 

O

 

 

 

X

 

 

 

X

10→30 K

X

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

CH4

/ Ar

 

X

 

 

 

X

X

 

 

 

 

 

H3C

 

 

H

 

 

 

O

• •

HYDROGEN ATOM ABSTRACTION

419

 

 

 

 

O

 

X

10→35 K

X

 

 

 

X

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

X

H2

/ Ar

X

 

 

 

X

 

 

 

 

 

 

 

 

 

 

 

71

H = −78.8 kcal/mol ∆H = −58.8 kcal/mol

69

70

a : X = F

H = −91.4 kcal/mol

b : X = Cl

H = −73.8 kcal/mol

c : X = H

 

Scheme 9.16

5.4.4. Tunneling in Intramolecular Reactions. Carbenes undergo intramolecular hydrogen insertions efficiently, when the structure allows. For example, 1,2- hydrogen migration forming an alkene is one of the most frequently documented rearrangement reactions of carbenes. It has been demonstrated that QMT plays an important role in some of intramolecular hydrogen migration processes.

2-Methylphenylcarbene (72) gives rise to o-quinodimethane (73). This reaction is explained in terms of an intramolecular 1,4-hydrogen shift (Scheme 9.17). This

 

H

 

 

 

 

 

CH3

 

72

 

 

H

 

 

 

 

 

 

 

CD3

72 - d3

dark

4.6 K

 

73

dark

CHD

 

 

 

65 K

CD2

73 - d3

Scheme 9.17

migration reaction was investigated in great detail by using matrix isolation spectroscopic techniques. Thus, 372 was generated in an argon matrix at low temperature and characterized by IR and UV–vis spectroscopy. Triplet carbene (72) is found to decay thermally to give singlet o-quinodimethane (73) even at temperatures as low as 4.6 K. The kinetics of carbene disappearance follow the standard (time)1/2 dependence, because of the multiple reaction sites in the matrix. The rate was monitored as a function of temperature from 4.6 to 30.0 K. A small temperature dependence of the rate and the nonlinear Arrhenius plot were noted. Moreover, 2(trideuteriomethyl)phenylcarbene (72-d3) was found to be thermally stable even at 19 K in an Ar matrix. In a Xe matrix, it was stable even at 59 K for

420 TRIPLET CARBENES

1150 min. These observations implicate a QMT mechanism for alkene formation.97

A similar QMT mechanism is proposed in a thermal 1,4-H shift of mesitylcarbene at 11 K.98

In contrast, 1-phenylethylidene (74), which can undergo 1,2-hydrogen migration to form styrene (75), was found to be thermally stable in argon or xenon matrix at 10 K. The carbene decay to give styrene only when warming to 65 K in xenon matrix (Scheme 9.18). From the disappearance rate constant for 74, a energy barrier

••

 

 

CH3

dark

 

 

10 K

 

74

 

75

Cl

dark

Cl

• •

10 K

 

 

 

76

 

77

Scheme 9.18

of 4.7 kcal/mol (at 65 K) was estimated. Thus, the thermal rearrangement of triplet

1-phenylethylidene to styrene likely occurs upon thermal population of the S1 state of 74 at 65 K.97

A 1,2-hydrogen shift in benzylchlorocarbene (76), which has a singlet ground state, forms b-chlorostyrene (77). This reaction has been found to involve a QMT. Thus, the carbene was found to decay thermally at temperature as low as 10 K. In contrast, deuterated carbene (76-d2) was stable at higher temperatures (up to 42 K) (Scheme 9.18). Arrhenius plots of the decay kinetics were obtained by following the reaction between 10 and 34.5 K in an argon matrix. Again the small temperature dependence of the rate at lower temperature and the curved Arrhenius plot at higher temperature zone were noted. From extrapolation of the data at room temperature, a rate of 10 2 s 1 at 80 K is expected. This value indicates that tunneling is important at low temperature.98

The difference in thermal stability of singlet benzylchlorocarbene (76) compared with that of triplet methylphenylcarbene (74) was noted, and was interpreted as being caused by the different spin states. In solution, a minimum barrier of 4.3 kcal/mol was assessed for the triplet carbene, which is in the range of the value which had been measured for 76 in solution. Tunneling at low temperatures was excluded for the triplet species since it is stable up to 30 K in argon. Intersystem crossing is not necessary in the reaction of the singlet species. Therefore, spin control may play an important role in the triplet molecule, resulting in a minimum activation barrier in the order of magnitude of the singlet–triplet gap.99

Singlet carbenes are also known to undergo intramolecular C H insertion when structurally favored. For example, tert-butylchlorocarbene (78) gives rise to

 

 

 

 

HYDROGEN ATOM ABSTRACTION

421

••

 

 

Cl

D3C

 

 

D3C

Cl

Cl

dark

 

••

 

 

 

 

11 K

 

Cl

45 K

D3C

D

 

 

D3C

CD3

 

 

 

 

 

 

 

 

 

 

 

 

D

D

78

 

79

78 - d9

 

79 - d9

Scheme 9.19

1,1-dimethyl-2-chlorocyclopropane (79) as a result of insertion of carbene into the C H bond of methyl group (Scheme 9.19). When 78 was generated in a nitrogen matrix at low temperature, it was detected by IR and UV–vis spectroscopy. However, the carbene decay on standing at 11 K in the dark produces the cyclopropane. The insertion rate was insensitive to temperature; warming the matrix from 11 to 30 K caused no abrupt increase in the disappearance of the carbene. The deuterated carbene (78-d9) was found to be thermally stable as the carbene survived up to 45 K. Thus, there is a minimal temperature dependence of the reaction at low temperatures and an unusual isotopic sensitivity of the kinetics all of this evidence suggests that the 1,3-CH insertion reaction of the carbene 78 involves QMT. The formation of C C bond during the reaction also suggests that heavy atom tunneling might be involved.100

5.4.5. Tunneling Reactions at Elevated Temperatures. Thus far, we have seen QMT reactions of carbenes at very low temperature. Many examples of QMT in reactions at elevated temperatures have also been reported. In fact, hightemperature QMT was demonstrated long before the low-temperature examples were discovered.

At cryogenic temperatures, the tunneling reaction proceeds mainly through the zero-point level and is sometimes referred to as deep tunneling. Low-temperature QMT is easily recognizable because deep tunneling is many orders of magnitude faster than the classical process, which is negligible at very low temperature. At elevated temperatures tunneling can occur through vibrational levels close to the top of the barrier. Consequently, the rates of a classical process and of a QMT process at ambient temperature may be comparable. A contribution of QMT to the overall rate of reaction at elevated temperatures can be revealed by measurement of kinetic isotope effects as a function of temperature. Differential activation energies greater than the difference in carbon–hydrogen and carbon–deuterium bond zero point energies [Ea(D)-Ea(H) >1.2 kcal/mol], and unusual ratio of preexponential factors (AH=AD < 0:7) signal a contribution of QMT to the overall rate of a reaction at elevated temperatures.101

In order to determine whether QMT may contribute to the overall reaction of diarylcarbenes with hydrogen atom donors in solution at ambient temperature, kinetic isotope effects for the benzylic hydrogen atom abstractions of the triplet states of several diarylcarbenes with toluene–toluene-d8 in fluid solution were determined over the temperature ranges of 75 to 135 C. The results are very much dependent on the structure of the carbene (Table 9.11).102 The differential

422 TRIPLET CARBENES

TABLE 9.11. Differential Activation Parameters of Triplet Carbene H(D) Atom Transfer

 

 

T (range)

EaðDÞ EaðHÞ

 

 

Carbenes

kH=kD

( C)

(kcal/mol)

AH=AD

1-Naphthyl(phenyl)carbene (a-51)

8.38

50 þ 150

1.77

0.42

2-Chlorodiphenylcarbene (14u)

8.00

50 þ 120

1.69

0.43

2-Trifluoromethyldiphenylcarbene (14v)

6.75

25 þ 120

1.88

0.31

Diphenylcarbene (14a)

7.00

75 þ 135

1.37

0.62

Dibenzocycloheptadienylidene (18)

5.26

75 þ 50

1.46

0.48

4-Biphenylphenylcarbene (14l)

5.58

75 þ 50

1.20

0.75

Fluorenylidene (23)

4.08

75 þ 25

0:80

0:20

1:05

0:10

Anthronylidene (52)

6.09

75 þ 25

0:89

0:20

1:35

0:10

kinetic isotope effects observed for 1-naphthylphenylcarbene (a-51), 2- chlorodiphenylcarbene (14u), and 2-trifluoromethyldiphenylcarbene (14v) were much larger than predicted by complete loss of all zero-point energy in the transition state. This observation indicates that there is a contribution of QMT to the H(D) atom transfer process. For diphenylcarbene (14a), dibenzocycloheptadienylidene (18), and 4-biphenylphenylcarbene (14l), the differential kinetic isotope effects were barely consistent with a completely classical atom-transfer reaction. For fluorenylidene (23) and anthronylidene (52), the data were completely consistent with a purely classical atom-transfer process. The lifetime of the carbenes undergoing QMT are probably longer than those of the other carbenes because of steric hindrance about the carbene carbon. The substituent may also widen the bond angle at the carbene carbon. These effects will decrease the amount of s character in the singly occupied orbitals of the carbene and lower the reactivity still further. Thus, the trends are interpreted as indicating that the relatively slow rate of the classical atom-transfer reaction in the hindered carbenes allows a QMT pathway to contribute more prominently to the overall hydrogen atom-transfer rate.102

Cl

CF3

 

• •

 

• •

 

14u

 

14v

 

 

 

 

A contribution of QMT in solution at room temperature is also observed in 1,2- hydrogen rearrangement of a singlet carbene.103,104

6. REACTIONS WITH OXYGEN

Molecular oxygen is an important participant in reactions of triplet carbene because of its triplet ground state and its ubiquity as an impurity in reaction

REACTIONS WITH OXYGEN

423

systems. Reaction of triplet carbenes with molecular oxygen is very efficient because the reaction is spin allowed process. So, the reaction with oxygen is sometimes used to judge the multiplicities of carbenes.

6.1. Product Studies

The photooxidation of diphenyldiazomethane yielded up to 73% benzophenone and no other products containing oxygen could be detected (Scheme 9.20). It was

hν

Ph2CN2

Ph2C

••

 

 

O2

 

 

 

 

3DPC

Ph2C = O + O2

Scheme 9.20

+ - Ph2CO O

80

O O

Ph2C CPh2

O O

81

postulated that the primary adduct arising from photooxidation is benzophenone oxide (80, Criegee intermediate), which transfers its terminal O atom to another molecule of carbene or diazomethane.60 When the photooxidation was carried out in solid chlorobenzene at 78 C, a tetroxane (81), a dimer of the oxide was isolated in 15% yield (Scheme 9.20). It was shown that the elimination of O2 from two molecules of the oxide does not proceed to a significant extent.105 More recent results show that if no trapping reagents are present, the extrusion of O2 from two separate oxides becomes the main reaction pathway for the oxide. The formation of the tetroxane does not occur in solution at room temperature.106 Other oxidation products arising from the oxidation are esters.107

6.2. Matrix Isolation Studies

Carbonyl oxides have been detected by matrix isolation and time-resolved laser spectroscopy. In a matrix, carbonyl oxides are easily generated upon annealing of O2-doped inert gas matrix containing triplet carbenes from 10 to 30– 40 K (Scheme 9.21). The carbonyl oxides (80) are characterized by a broad and strong absorption in the 380– 460-nm range. In most cases, the matrix turns intense yellow to red. The observed absorbance is assigned to a p–p* transition in accord with a CNDO/S computation that predicts n–p* transitions in the region 600–800 nm. The latter absorption is very weak and has not been directly measured experimentally, but its presence is indicated by the fact that photochemical conversion of the carbonyl oxide can be initiated by irradiation of this range (see below).108

Infrared spectroscopy has also been used to characterize carbonyl oxides in matrix isolation. The carbonyl oxides are identified by their intense O O stretching

424 TRIPLET CARBENES

R

hν

 

R

 

 

 

N2

 

 

 

••

 

 

 

 

 

 

 

 

 

 

 

 

R

O2 - Ar

 

R

 

10→30 K R +

-

hν′

R

 

 

 

O

O

 

 

 

 

 

 

 

 

 

O

 

 

 

 

 

 

 

 

 

 

R

 

 

R

 

 

 

O

80

 

 

 

82

 

 

 

 

 

 

 

 

 

 

hν

 

O2

 

 

 

 

 

 

 

 

R

 

 

 

O

 

+ O3

 

 

 

 

 

 

 

 

 

 

 

 

 

O

 

R

 

 

 

 

 

R

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

R

 

 

 

 

 

O

 

 

 

 

 

 

 

 

 

 

83

 

 

Scheme 9.21

vibrations 900–1000 cm 1. Isotope labeling with 18O in one and both oxygens has been used to assign vibrational bands as well as to confirm the structure. For example, the IR bands observed for cyclopentadienone oxide at 1014, 947, and 940 cm 1 exhibit a large shift ( 28, 22, and 15 cm 1, respectively) on double labeling with 18O and are therefore assigned to vibrations with a considerable O O stretching component. There are two 16O18O isotopomers for this species, as evidenced by the fact that the band at 1014 cm 1 is split into two (1001 and 995 cm 1), clearly indicating that the oxygen atoms are not equivalent. These

observations eliminate a dioxirane structure (82), which should show only one 16O18O isotopomer.109

These bands are in good accord with the calculated spectra for the oxides. Theoretical studies of the oxides aimed at the determination of electronic structures.

They tried to determine

whether

these

species

are diradicals

or

not (Eq. 23).

R

 

O

 

 

R

+

-

 

 

R

 

O

-

 

 

 

O

 

+ O

R

O

 

 

R

 

 

O

 

 

 

R

 

ð23Þ

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

It has been shown that different methods may ascribe different bond lengths to the O O and C O bonds and that the medium and substituents affect the electronic behaviors of carbonyl oxides.110 For example, recent computational studies (B3LYP/6-31 þ G (d, p)) of carbonyl oxides, synand anti-methyl carbonyl oxides and dimethylcarbonyl oxides in gas and solution reveal that dipolar character increases with the number of methyl groups, and the ionic configuration is stabilized in a polar medium. These effects result in a weakened O O bond and an increased double-bond character in the CO bond.111

Carbonyl oxides are extremely photolabile even under matrix conditions and irradiation with red light (600 nm) rapidly produces dioxiranes (82).109 The dioxiranes are stable under these conditions but at 400-nm irradiation are converted into esters (83) or lactones. Ketones have been observed as byproducts in the carbene– O2 reactions in frozen matrices. Since the reaction of triplet carbene with O2 is very

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