
Reactive Intermediate Chemistry
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630 NITRENIUM IONS
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Me |
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O2N |
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Me |
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O |
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N |
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Ar |
N |
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Me |
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Me |
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C |
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Me |
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Me |
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Me |
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124 |
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3* |
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3 |
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O |
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Me |
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Ph3CH O2N |
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O2N |
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O2N |
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Me |
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O |
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O |
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Ph3C |
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200 ns |
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2 s |
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N |
H |
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N |
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N |
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t-Bu |
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t-Bu |
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t-Bu |
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125 |
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123 |
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Figure 13.58. Evidence for a triplet ground-state arylnitrenium ion.
The 4-nitro derivative in the anthranilium ion series showed qualitatively different behavior (Fig. 13.58).119 For one thing, it proved impossible to trap it using any external nucleophile. On the other hand, significant yields of the iminium ion 124 and the parent amine were observed. Only the parent amine was observed when the decomposition was carried out through triplet energy transfer. Laser flash photolysis experiments were not successful at detecting the nitrenium ion, but instead showed that the excited triplet state of the precursor 125 was formed. Addition of a hydrogen atom donor, Ph3CH, resulted in formation and detection of the corresponding radical, Ph2C . The latter’s growth did not correlate with the disappearance of triplet state 125. Instead, there was a 2-ms delay (extrapolated to [Ph3CH] ¼ 0 M) between the disappearance of 125 and formation of Ph3C . The delay time corresponds to the lifetime of the triplet nitrenium ion. That no singlet products (i.e., 124) were formed in the triplet sensitization experiment led to the conclusion that either the nitrenium ion 123 was a ground-state triplet or else that the singlet was ground state but that intersystem crossing was anomalously slow in this system.
The parent nitrenium ion (NHþ2 ) is firmly established as a ground-state triplet: both extensive ab initio calculations as well as PES experiments all agree that the singlet–triplet energy gap is 30 kcal/mol. There have been several investigations on its behavior in solution. Takeuchi et al.141 showed that this species could be generated by photolysis of 1-amino-(2,4,6-triphenylpyridinium) ion. These photolyses were carried out in the presence of various aromatic compounds. It was found that the triplet state abstracted hydrogen atoms from traps such as toluene

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SPECTROSCOPIC AND KINETIC STUDIES OF NITRENIUM IONS 631 |
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toluidines |
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khyd |
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PhCH3 |
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CH3 |
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CH3 |
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1NH2+ |
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PhCH3 |
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NH3 |
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PhCH2+ |
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(+ ortho isomer) |
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H |
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CH2Ph |
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Ph |
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kST |
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NH3 + |
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PhCH2 |
PhCH2 |
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3NH2 |
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PhCH3 |
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PhCH2CH2Ph (bibenzyl) |
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Figure 13.59. Hydrogen atom transfer to triplet nitrenium ion.
(Fig. 13.59). Srivastava et al.158 carried out similar experiments and demonstrated that the singlet was formed initially upon photolysis. This species either inserts into the OH bond of water or it suffers intersystem crossing to the lower energy triplet. As in the former study, the only reaction found for the triplet was hydrogen atom transfer.
4.6. Intersystem Crossing
The interconversion of singlet states and triplet states is known as intersystem crossing. To date, a direct observation of this process has not been reported other than for the decay of the excited triplet state of the highly stabilized nitrenium ion 7 (Fig. 13.2). In several cases, intersystem crossing has been inferred from studies of product distributions. For example, the photolytic generation of NHþ2 creates the singlet state which abstracts a hydride from toluene to give the benzyl cation (Fig. 13.59). The latter adds to an additional molecule of toluene to give ortho and para benzyltoluenes. In contrast, the triplet abstracts a hydrogen atom from toluene. The resulting benzyl radicals dimerize in a head-to-head fashion giving bibenzyl. It was found that the ratio of bibenzyl to the benzyltoluenes increased with the addition of an unreactive diluent to the toluene trap. An analysis of these
data yields a ratio of the intersystem crossing rate constant, kST, to the rate constant for hydride transfer from the singlet, khyd, of kST=khyd ¼ 31 M.158 Assuming a diffusion limited rate constant for hydride transfer, khyd ¼ 1–10 109 M 1 s 1, it is
possible to estimate kST as between 3 1011 s 1 and 3 1012 s 1. Direct ultrafast measurements of these values would be desirable.
5. SPECTROSCOPIC AND KINETIC STUDIES OF NITRENIUM IONS
5.1. Brief Summary of Methods
Many studies of carbenium ions have made use of superacid media for their generation and characterization. Attempts to apply this method to the study of nitrenium ions have been largely unsuccessful. The reason is that singlet nitrenium




SPECTROSCOPIC AND KINETIC STUDIES OF NITRENIUM IONS |
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TABLE 13.5. N-tert-Butyl-N-aryl Nitrenium Ions |
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Generated through LFP of Anthranilium Ion Saltsa |
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Xb |
lmax |
t in MeCN (ns) |
ktrap |
(Trap)c |
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6 |
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Cl |
385 |
0.14 |
3:2 106 |
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Br |
395 |
0.13 |
1:3 107 |
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CH3 |
460 |
0.40 |
3:1 |
104 |
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Ph |
470 |
30 |
6:2 |
105 |
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OMe |
500 |
600 |
2:1 |
10 |
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a See Refs. 157 and 175.
b Aryl substituent para to the nitrenium ion. c The trap is water.
The study of more typically reactive nitrenium ions had to await the application of faster methods. Nearly two decades later, nanosecond LFP methods were applied to the ring opening of anthranilium ions (Fig. 13.29).174 A series of alkylarylnitre-
nium ions were characterized in this manner and the results are compiled in Table 13.5.117,157,175 These species in general had much shorter lifetimes (<50 ms)
than the quinone diimine. The 4-halonitrenium ions of this class show absorption maxima at wavelengths <400 nm, along with a weak tail that extends into the visible. For the 4-methyl derivative, only the weak tail can be detected. The UV maximum apparently overlaps with the absorption band of the starting material. Substitution by a phenyl ring or an alkoxy group shifts the absorption maximum into the visible region of the spectrum. Interestingly, it is the 4-phenyl substituent that has the most profound effect on the stabilization of the nitrenium ion toward attack by H2O.
The next development in direct detection of nitrenium ions came from McClelland et al.120 who applied the azide method to LFP measurements. This permitted the direct detection of those arylnitrenium ions implicated in carcinogenic
DNA damage. McClelland’s approach proved to be particularly useful in the study of 4-aryl2,129,131 and 4-alkoxy substituted phenylnitrenium ions.130 Apparently, the
corresponding singlet nitrenes are sufficiently long lived to allow for protonation in aqueous solution. Several arylnitrenium ions studied by this route are described in Table 13.6.
TABLE 13.6. Arylnitrenium Ions (Ar Nþ H) Generated from Arylazide Photolysis in Protic Media
Ar |
lmax |
t ðmsÞ |
Reference |
4-Biphenylyl |
465 |
0.35/H2O |
183 |
2-Fluorenyl |
460 |
75/H2O |
183 |
40-MeO-4-Biphenylyl |
500 |
633/H2O |
183 |
2-(1-Methylimidazolyl) |
235 |
100,000/H2O |
183 |
4-Stilbenyl |
520 |
0.16/H2O |
167 |
4-MeO-phenyl |
300 |
0.8/H2O |
183 |
2,4,6-Tribromophenyl |
420, 600 |
0.2/MeCN/H2O |
125 |
4-hydroxymethyl-2,3,5,6-tetrafluorophenyl |
375 |
>1000/MeCN |
128 |
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636 NITRENIUM IONS
TABLE 13.7. Absorption Maxima (nm), Lifetimes, and Trapping Rate Constants (M 1 s 1) of Nitrenium Ions Characterized by Laser Flash Photolysis of N-Aminopyridinium Saltsa
R1 |
R2 |
lmax |
tðmsÞ |
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ktrap |
(Trap) |
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5 |
(H2O) |
Ph |
Ph |
435, 690 |
1.6 (MeCN) |
6:1 104 |
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4-Tolyl |
4-Tolyl |
425,680 |
280 (MeCN) |
1:9 104 |
(H2O) |
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4-Biphenylyl |
Me |
460 |
24 (MeCN) |
9:3 106 |
(H2O) |
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4-Chlorophenyl |
Me |
340 |
0.95 (MeCN) |
8:9 |
104 |
(H2O) |
4-MeO-phenyl |
Me |
320 |
100 (MeCN) |
5:5 |
107 |
(H2O) |
4-Tolyl |
Me |
330 |
7.4 (MeCN) |
2:3 |
108 |
(H2O) |
1-Naphthyl |
Me |
500 |
0.8 (MeCN) |
1:7 |
10 |
(H2O) |
a See Refs. 145, 146, and 163.
The aminopyridinium route has been employed in flash photolysis studies of aryl as well as diarylnitrenium ions. Several examples of nitrenium ion species, along with their absorption maxima and some trapping rate constants are given in Table 13.7. To the extent the data are comparable, there is good agreement with the behavior of nitrenium ions generated by the azide route. For example, the 4- biphenylyl systems from the azide protonation and N-aminopyridinium routes both give absorption maxima at 460 nm and live for several microseconds in water. Likewise, the 4-methoxyphenyl systems show maxima at 300 nm (from azide) and 320 nm (from aminopyridinium ion). The discrepancy in this case can be attributed to the N-methyl substituent, present in the aminopyridinium route, but absent in the azide experiment.
5.3. Infrared and Raman Spectra of Nitrenium Ions
A promising recent development in the study of nitrenium ions has been the introduction of time-resolved vibrational spectroscopy for their characterization. These methods are based on pulsed laser photolysis. However, they employ either time resolved IR (TRIR) or time-resolved resonance Raman (TRRR) spectroscopy as the mode of detection. While these detection techniques are inherently less sensitive than UV–vis absorption, they provide more detailed and readily interpretable spectral information. In fact, it is possible to directly calculate these spectra using relatively fast and inexpensive DFT and MP2 methods. Thus, spectra derived from experiment can be used to validate (or falsify) various computational treatments of nitrenium ion structures and reactivity. In contrast, UV–vis spectra do not lend themselves to detailed structural analysis and, moreover, calculating these spectra from first principles is still expensive and highly approximate.
The first study of this nature involved the application of TRIR to diphenylnitrenium ion (Fig. 13.65).187 This species gave strong distinct transient IR bands at 1568, 1440, and 1392 cm 1. It was further demonstrated that the decay of these signals followed the same kinetics found by UV–vis detected LFP for the same