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        <title>Quanty - documentation:standard_operators:magnetic_dipole</title>
        <description></description>
        <link>https://www.quanty.org/</link>
        <image rdf:resource="https://www.quanty.org/_media/wiki/dokuwiki.svg" />
       <dc:date>2026-04-30T14:33:39+00:00</dc:date>
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        <dc:date>2025-11-20T02:29:38+00:00</dc:date>
        <dc:creator>Anonymous (anonymous@undisclosed.example.com)</dc:creator>
        <title>Magnetic dipole operators (T)</title>
        <link>https://www.quanty.org/documentation/standard_operators/magnetic_dipole/start?rev=1763605778&amp;do=diff</link>
        <description>Magnetic dipole operators (T)
The magnetic dipole operator is defined as:
\begin{equation}
\vec{T} = \vec{S} - 3 \hat{r}\left(\hat{r}\cdot\vec{S}\right).
\end{equation}
They apear in the magnetic sum-rules for core level spectroscopy, where excitations from a core state that is split by spin-orbit coupling to a valence shell lead two two sets of separate peaks due to the core leve spin-orbit coupling. The weighted integrated difference between these two edges is related to $\vec{S}$$\vec{T}$magn…</description>
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        <dc:date>2025-11-20T02:29:38+00:00</dc:date>
        <dc:creator>Anonymous (anonymous@undisclosed.example.com)</dc:creator>
        <title>Tx</title>
        <link>https://www.quanty.org/documentation/standard_operators/magnetic_dipole/tx?rev=1763605778&amp;do=diff</link>
        <description>Tx
The x component of $\vec{T}$ is defined as:
\begin{equation}
T_x = S_x - 3 x\left(x S_x + y S_y + z S_z\right)/r^2.
\end{equation}
The equivalent operator in Quanty is created by:


OppTx = NewOperator(&quot;Tx&quot;, NF, IndexUp, IndexDn)

The operator can alternatively be created with the following function:


function Tx(indexup, indexdn, NF)
  if #indexup ~= #indexdn then
    error(&quot;Length of index up must be equal to length of index dn and equal to 2l+1 in Tx&quot;)
  end
  local l=(#indexup-1)/2
  if …</description>
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        <dc:creator>Anonymous (anonymous@undisclosed.example.com)</dc:creator>
        <title>Ty</title>
        <link>https://www.quanty.org/documentation/standard_operators/magnetic_dipole/ty?rev=1763605778&amp;do=diff</link>
        <description>Ty
The y component of $\vec{T}$ is defined as:
\begin{equation}
T_y = S_y - 3 y\left(x S_x + y S_y + z S_z\right)/r^2.
\end{equation}
The equivalent operator in Quanty is created by:


OppTy = NewOperator(&quot;Ty&quot;, NF, IndexUp, IndexDn)

The operator can alternatively be created with the following function:


function Ty(indexup, indexdn, NF)
  if #indexup ~= #indexdn then
    error(&quot;Length of index up must be equal to length of index dn and equal to 2l+1 in Ty&quot;)
  end
  local l=(#indexup-1)/2
  if …</description>
    </item>
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        <dc:date>2025-11-20T02:29:38+00:00</dc:date>
        <dc:creator>Anonymous (anonymous@undisclosed.example.com)</dc:creator>
        <title>Tz</title>
        <link>https://www.quanty.org/documentation/standard_operators/magnetic_dipole/tz?rev=1763605778&amp;do=diff</link>
        <description>Tz
The z component of $\vec{T}$ is defined as:
\begin{equation}
T_z = S_z - 3 z\left(x S_x + y S_y + z S_z\right)/r^2.
\end{equation}
The equivalent operator in Quanty is created by:


OppTz = NewOperator(&quot;Tz&quot;, NF, IndexUp, IndexDn)

The operator can alternatively be created with the following function:


function Tz(indexup, indexdn, NF)
  if #indexup ~= #indexdn then
    error(&quot;Length of index up must be equal to length of index dn and equal to 2l+1 in Tz&quot;)
  end
  local l=(#indexup-1)/2
  if …</description>
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