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- W88001514 startingPage "A883" @default.
- W88001514 abstract "The magnetic multipole transition probability is calculated in terms of the matrix elements of the magnetic multipole. The magnetic $mathrm{jm}$ moment ${{Q}_{mathrm{jm}}}^{(mathrm{mg})}$ is defined as $(frac{e}{ensuremath{mu}}){[frac{4ensuremath{pi}}{(2j+1)}]}^{frac{1}{2}}ensuremath{Sigma}stackrel{}{i}(ensuremath{nabla}{{r}_{i}}^{j}{Y}_{mathrm{jm}})[{(j+1)}^{ensuremath{-}1}{mathrm{l}}_{i}+{mathrm{s}}_{i}],$ where $e$ and $ensuremath{mu}$ are electron charge and electron mass, ${r}_{i}$, ${mathrm{l}}_{i}$, and ${mathrm{s}}_{i}$ are the coordinate, orbital angular momentum, and spin-angular momentum of the $imathrm{th}$ electron and ${Y}_{mathrm{jm}}$ is the spherical harmonic. Magnetic quadrupole and octupole moments are explicitly given. It is shown that for the ${^{3}ensuremath{Sigma}_{u}}^{+}ensuremath{leftrightarrow}{^{1}ensuremath{Sigma}_{g}}^{+}$ transition of the hydrogen molecule, the magnetic quadrupole transition is more important than the conventional spin-orbit electric dipole transition. The magnetic octupole transition has the same order of magnitude as the spin-orbit magnetic dipole transition." @default.
- W88001514 created "2016-06-24" @default.
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- W88001514 date "1964-05-18" @default.
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- W88001514 title "<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>Δ</mml:mi><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:mo>±</mml:mo><mml:mn>1</mml:mn></mml:math>Magnetic Multipole Radiative Transitions" @default.
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- W88001514 doi "https://doi.org/10.1103/physrev.134.a883" @default.
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