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The scattering intensity follows a typical cos2φ dependence due to the decomposition of the excitation electric field vector along either the bisector of the dimer for the radiative antibonding mode or its orthogonal direction for the radiative bonding mode.
This is because the excitation E-field vector can be decomposed along either the bisector of the dimer for the radiative antibonding mode or its orthogonal direction for the radiative bonding mode.
Under the excitation of light with S-polarization, the individual dipoles oscillate symmetrically at 672 nm and produce a resultant dipoles along the bisector of the dimer (Fig. 3b upper-left), which give rise to the corresponding resonance scattering peak in the spectrum (red circle).
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One is along the bisector of the nanorod dimer which is related to the excitation of the radiative antibonding mode and the other is orthogonal and related to the radiative bonding mode.
With the increase of φ, as we can see for the S-polarization, the peak at 672 nm reaches a maximum when the polarization of excitation is parallel to the bisector of the nanorod dimer (φ = 0°), and decreases to zero when it is perpendicular to the bisector (φ = 90°).
The correct structure of the dimer.
(A) Closed-up view of the dimer formation of mTORC1.
The Voronoi diagram of multiple curves is constructed to generate bisector of the geometric domain.
The main vertical sections are located along the coordinate axes and the bisector of the angle between them.
Two principal sections are located along the coordinate axes and the third one – along the bisector of the angle between them.
As a result, we conclude that the line O K ¯ is the bisector of the angle ∠PON.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com