diff --git a/demonstrations/tutorial_liesim.py b/demonstrations/tutorial_liesim.py index 0cb3ffabb2..6eebb7f1d0 100644 --- a/demonstrations/tutorial_liesim.py +++ b/demonstrations/tutorial_liesim.py @@ -66,7 +66,7 @@ Technically, the (dynamical) Lie algebra is formed by skew-Hermitian operators :math:`\{i h_i\}`. We avoid this distinction here since for all practical purposes one can also look at Hermitian operators and explicitly add imaginary units in the exponents where appropriate. - For more details, see the note in the "Lie algebras" section of our :doc:`Intro to (Dynamical) Lie Algebras for quantum practitioners `. + For more details, see the note in the "Lie algebras" section of our `Intro to (dynamical) Lie algebras for quantum practitioners `__. :math:`\mathfrak{g}`-sim theory ------------------------------- diff --git a/demonstrations/tutorial_quantum_chemistry.py b/demonstrations/tutorial_quantum_chemistry.py index 30362414dc..f36fe5fae5 100644 --- a/demonstrations/tutorial_quantum_chemistry.py +++ b/demonstrations/tutorial_quantum_chemistry.py @@ -255,7 +255,7 @@ ############################################################################## # In this case, since we have truncated the basis of molecular orbitals, the resulting # observable is an approximation of the Hamiltonian generated in the -# section :ref:`hamiltonian`. +# section `Building the Hamiltonian `__. # # OpenFermion-PySCF backend # ------------------------- diff --git a/demonstrations/tutorial_quantum_natural_gradient.py b/demonstrations/tutorial_quantum_natural_gradient.py index d2e87d4f87..c884caf4bd 100644 --- a/demonstrations/tutorial_quantum_natural_gradient.py +++ b/demonstrations/tutorial_quantum_natural_gradient.py @@ -26,7 +26,7 @@ The most successful class of quantum algorithms for use on near-term noisy quantum hardware is the so-called variational quantum algorithm. As laid out in the -:ref:`Concepts section `, in variational quantum algorithms +`Concepts section `__, in variational quantum algorithms a low-depth parametrized quantum circuit ansatz is chosen, and a problem-specific observable measured. A classical optimization loop is then used to find the set of quantum parameters that *minimize* a particular measurement expectation value