qml.structure_constants

structure_constants(g, pauli=False, is_orthogonal=True)

Compute the structure constants that make up the adjoint representation of a Lie algebra.

Given a DLA \(\{iG_1, iG_2, .. iG_d \}\) of dimension \(d\), the structure constants yield the decomposition of all commutators in terms of DLA elements,

\[[i G_\alpha, i G_\beta] = \sum_{\gamma = 0}^{d-1} f^\gamma_{\alpha, \beta} iG_\gamma.\]

The adjoint representation \(\left(\text{ad}(iG_\gamma)\right)_{\alpha, \beta} = f^\gamma_{\alpha, \beta}\) is given by those structure constants, which can be computed via

\[f^\gamma_{\alpha, \beta} = \frac{\text{tr}\left(i G_\gamma \cdot \left[i G_\alpha, i G_\beta \right] \right)}{\text{tr}\left( iG_\gamma iG_\gamma \right)}.\]

The inputs are assumed to be orthogonal unless is_orthogonal is set to False. However, we neither assume nor enforce normalization of the DLA elements \(G_\alpha\).

Parameters

• g (List[Union[Operator, PauliWord, PauliSentence]]) – The (dynamical) Lie algebra for which we want to compute its adjoint representation. DLAs can be generated by a set of generators via lie_closure().

• pauli (bool) – Indicates whether it is assumed that PauliSentence or PauliWord instances are input. This can help with performance to avoid unnecessary conversions to Operator and vice versa. Default is False.

• is_orthogonal (bool) – Whether the set of operators in g is orthogonal with respect to the trace inner product. Default is True.

Returns

The adjoint representation of shape (d, d, d), corresponding to indices (gamma, alpha, beta).

Return type

TensorLike

See also

lie_closure(), center(), PauliVSpace, Demo: Introduction to Dynamical Lie Algebras for quantum practitioners

Example

Let us generate the DLA of the transverse field Ising model using lie_closure().

>>> n = 2
>>> gens = [X(i) @ X(i+1) for i in range(n-1)]
>>> gens += [Z(i) for i in range(n)]
>>> dla = qml.lie_closure(gens)
>>> print(dla)
[X(0) @ X(1), Z(0), Z(1), -1.0 * (Y(0) @ X(1)), -1.0 * (X(0) @ Y(1)), -1.0 * (Y(0) @ Y(1))]

The dimension of the DLA is \(d = 6\). Hence, the structure constants have shape (6, 6, 6).

>>> adjoint_rep = qml.structure_constants(dla)
>>> adjoint_rep.shape
(6, 6, 6)

The structure constants tell us the commutation relation between operators in the DLA via

\[[i G_\alpha, i G_\beta] = \sum_{\gamma = 0}^{d-1} f^\gamma_{\alpha, \beta} iG_\gamma.\]

Let us confirm those with an example. Take \([iG_1, iG_3] = [iZ_0, -iY_0 X_1] = -i 2 X_0 X_1 = -i 2 G_0\), so we should have \(f^0_{1, 3} = -2\), which is indeed the case.

>>> adjoint_rep[0, 1, 3]
-2.0

We can also look at the overall adjoint action of the first element \(G_0 = X_{0} \otimes X_{1}\) of the DLA on other elements. In particular, at \(\left(\text{ad}(iG_0)\right)_{\alpha, \beta} = f^0_{\alpha, \beta}\), which corresponds to the following matrix.

>>> adjoint_rep[0]
array([[ 0.,  0.,  0.,  0.,  0.,  0.],
       [-0.,  0.,  0., -2.,  0.,  0.],
       [-0.,  0.,  0.,  0., -2.,  0.],
       [-0.,  2., -0.,  0.,  0.,  0.],
       [-0., -0.,  2.,  0.,  0.,  0.],
       [ 0., -0., -0., -0., -0.,  0.]])

Note that we neither enforce nor assume normalization by default.

To compute the structure constants of a non-orthogonal set of operators, use the option is_orthogonal=False:

>>> dla = [qml.X(0), qml.Y(0), qml.X(0) - qml.Z(0)]
>>> adjoint_rep = qml.structure_constants(dla, is_orthogonal=False)
>>> adjoint_rep[:, 0, 1] # commutator of X_0 and Y_0 consists of first and last operator
array([-2.,  0.,  2.])

Mathematical details

Consider a (dynamical) Lie algebra \(\{iG_1, iG_2, .. iG_d \}\) of dimension \(d\). The defining property of the structure constants is that they express the decomposition of commutators in terms of the DLA elements, as described at the top. This can be written as

\[[i G_\alpha, i G_\beta] = \sum_{\gamma = 0}^{d-1} f^\gamma_{\alpha, \beta} iG_\gamma.\]

Now we may multiply this equation with the adjoint of a DLA element and apply the trace:

\[\begin{split}\text{tr}\left(-i G_\eta \cdot \left[i G_\alpha, i G_\beta \right] \right) &= \text{tr}\left(-i G_\eta \sum_{\gamma = 0}^{d-1} f^\gamma_{\alpha, \beta} iG_\gamma\right)\\ &= \sum_{\gamma = 0}^{d-1} \underset{g_{\eta \gamma}}{\underbrace{ \text{tr}\left(-i G_\eta iG_\gamma\right)}} f^\gamma_{\alpha, \beta} \\ \Rightarrow\ f^\gamma_{\alpha, \beta} &= (g^{-1})_{\gamma \eta} \text{tr}\left(-i G_\eta \cdot \left[i G_\alpha, i G_\beta \right] \right).\end{split}\]

Here we introduced the Gram matrix \(g_{\alpha\beta} = \text{tr}(-iG_\alpha i G_\beta)\) of the DLA elements. Note that this is just the projection of the commutator on the DLA element \(iG_\gamma\) via the trace inner product.

Now, if the DLA elements are orthogonal, as assumed by structure_constants by default, the Gram matrix will be diagonal and simply consist of some rescaling factors, so that the above computation becomes the equation from the very top:

\[f^\gamma_{\alpha, \beta} = \frac{\text{tr}\left(i G_\gamma \cdot \left[i G_\alpha, i G_\beta \right] \right)} {\text{tr}\left( iG_\gamma iG_\gamma \right)}.\]

This is cheaper than computing the full Gram matrix, inverting it, and multiplying it to the trace inner products.

For the case of an orthonormal set of operators, we even have \(g_{\alpha\beta}=\delta_{\alpha\beta}\), so that the division in this calculation can be skipped.

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