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A long nonresonant transverse slot is utilized to realize a half mode resonator and generate radiation simultaneously so as to reduce the size and release the use of extra radiator.

Codesigned Wideband High-Efficiency Filtering SIW Slot Antenna with High Selectivity and Flat Gain Response

(the local minimum of [t.sup.T.sub.c](k), which is similar for both barrier widths, since nonresonant times [t.sup.T.sub.c](k) change little with the barrier width for opaque barriers, as is the case in Figures 3 and 4); a second peak in [[rho].sub.t]([tau]) is expected to occur around the local maximum of [t.sup.T.sub.c] (k), which corresponds to [tau] [approximately equal to] [t.sup.T.sub.c]([k.sub.0]) (this local maximum--corresponding to resonant wave numbers--changes significantly with the barrier widths; see, e.g., [28]).

A Probability Distribution for Quantum Tunneling Times

(ii) (E, [epsilon])-CNR (completely nonresonant) in B iff for all j < [L.sub.k+1]/[L.sub.k]

Surface Localization in Impurity Band with Random Displacements and Long-Range Interactions

Etchegoin, "Single-molecule surface-enhanced raman spectroscopy of nonresonant molecules," Journal of the American Chemical Society, vol.

A Review on Applications of Two-Dimensional Materials in Surface-Enhanced Raman Spectroscopy

Suppose that A is a constant matrix with different eigenvalues; they proved that if the eigenvalues of A and the frequencies of Q satisfy some nonresonant conditions, then for sufficiently small [[epsilon].sub.0] > 0, there exists a nonempty Cantor set E [subset] (0, [[epsilon].sub.0]), such that, for any [epsilon] [member of] E, system (6) is reducible.

On the Effective Reducibility of a Class of Quasi-Periodic Linear Hamiltonian Systems Close to Constant Coefficients

[17] are based on nonresonant electrothermal actuation.

The Designing of Magnetic-Driven Micromirror for Portable FTIRs

Peak intensities of the nonresonant Raman spectrum (in Stokes process) were calculated from the well-known expression [20]: I [??] [[absolute value of ([e.sub.s][Re.sub.i]].sup.2] [w.sup.-1](n + 1), where (n + 1) is the population factor for Stokes scattering with n = [exp([??][omega]/[[K.sub.B]T) - 1].sup.-1] denoting the Bose-Einstein thermal factor, [e.sub.i] ([e.sup.s]) is the polarization of the incident (scattered) radiation, and R is the Raman susceptibility tensor.

Vibrational Spectroscopy of Binary Titanium Borides: First-Principles and Experimental Studies

Asakawa, "Nonresonant singular two-point boundary value problems," Nonlinear Analysis: Theory, Methods & Applications, vol.

On a Singular Second-Order Multipoint Boundary Value Problem at Resonance