“…In fact, the illuminating source and the field position used to evaluate G 2 PW ( r m , k R ) in the PWA configuration (Figure b) differ dramatically from those used to evaluate G 2 Exp ( R , p loc Exp ) in the experimental configuration (Figure a). Some theoretical works have reported that G 2 PW ( r m , k R ) agrees well with G 2 Exp ( R , p loc Exp ) for the nanosphere monomer, dimer, and array over a wide spectral range based on analytical solutions of Maxwell’s equations using generalized Mie theory. , It was also found that G 2 PW ( r m , k ′) will deviate from G 2 Exp ( R , p loc Exp ) for 1 order of magnitude if the direction of k ′ is perpendicular to R . , Other theoretical work reported that G 2 PW ( r m , k R ) with an incident angle along the direction of − R deviates remarkably in the enhancement factor of the scattering cross section integral over all solid angles of the dipolar emitter–nanorod system over the isolated dipolar emitter system . However, it is still unclear how reliable it is to use G 2 PW ( r m , k R ) to quantitatively predict G 2 Exp ( R , p loc Exp ) (with the radiation angle opposite to the incident angle in PWA) in some important POA systems, such as the nanoparticle–substrate coupled system for SEF and SERS ,, with ultrahigh sensitivity and the scanning probe–substrate coupled system for tip-enhanced Raman spectroscopy (TERS) with ultrahigh spatial resolution (up to subnanometer and even chemical-bond resolution). − For example, it has been reported that the calculated enhancement factor of Raman intensities in a TERS system by using PWA can be more than 2 orders of magnitude larger than the measured enhancement factor in the experiments .…”