Hypershielding contributions to magnetic shielding of the nitrogen
N nucleus have been evaluated for some nitroso (R
NO) and isodiazene (R
1R
2N
N) compounds in the presence of an external spatially uniform, time-independent magnetic field, accounting for cubic response via Rayleigh−Schrdinger perturbation theory. Numerical estimates have been obtained at the coupled Hartree−Fock level of accuracy within the conventional common-origin approach. Medium-size basis sets of gaugeless (that is, without gauge-including phase factors) Gaussian functions have been employed in a numerical test to show that the isotropic hypershielding contribution τ
NB2, τ
N = 1/2Σ
αβγδN, eqs
2−
4 in the text, to average nitrogen shielding in Ph
NO (τ
N ≈ 1.1 × 10
−5 ppm T
−2), (CH
3)
3C
NO (τ
N ≈ 2.3 × 10
−5 ppm T
−2), and (CH
3)
2N
N (τ
N ≈ 4.4 × 10
−5 ppm T
−2) are similar and quite large. For
15N at the highest currently available high-resolution NMR field strength of 22.3 T (ω
H/2π = 950 MHz, ω
15N/2π = 96.3 MHz) the change due to the additional shielding contribution for these compounds is between 0.5 and 2 Hz to lower frequency (upfield). Employing modern NMR instrumentation, shielding perturbations of this magnitude are, in principle, within detection limits, although instrumental instabilities and other field-dependent shielding phenomena make unambiguous detection at different field strengths difficult.