diff --git a/doc/source/pre/whatsnew/1.3.rst b/doc/source/pre/whatsnew/1.3.rst index 2970ce4142e1e93546df372b96398c898a6fe9ba..4f7a3f3274a04c16022ac7b889b71e08e5d58b5a 100644 --- a/doc/source/pre/whatsnew/1.3.rst +++ b/doc/source/pre/whatsnew/1.3.rst @@ -58,12 +58,12 @@ the following:: q = Q(psi) j = J(psi) -See :doc:`../../tutorial/operators` +See the tutorial: :doc:`../../tutorial/operators` Plotting of currents -------------------- Quantities defined on system hoppings (e.g. currents calculated using -`~kwant.operator.current`) can be directly plotted as a streamplot over the +`~kwant.operator.Current`) can be directly plotted as a streamplot over the system using `kwant.plotter.current`. This is similar to how `kwant.plotter.map` can be used to plot quantities defined on sites. The example below shows edge states of a quantum anomalous Hall phase @@ -91,7 +91,7 @@ related by symmetry. The discrete symmetries may be combined with conservation laws, such that if different blocks of the Hamiltonian are related by a discrete symmetry, the lead modes are computed to reflect this. -See the updated :doc:`../../tutorial/superconductors` +See the updated tutorial: :doc:`../../tutorial/superconductors` Named parameters for value functions ------------------------------------ @@ -142,7 +142,9 @@ The kernel polynomial method is now implemented within Kwant to obtain the density of states or, more generally, the spectral density of a given operator acting on a system or Hamiltonian. -See :doc:`../../reference/kwant.kpm` +See the tutorial: :doc:`../../tutorial/kpm` + +See the reference documentation: :doc:`../../reference/kwant.kpm` Finalizing builders with multiple translational symmetries ---------------------------------------------------------- @@ -193,7 +195,8 @@ increased. Pickling support ---------------- -It is now possible to pickle and unpickle Kwant ``Builder`` and ``System``. +It is now possible to pickle and unpickle `~kwant.builder.Builder` and +`~kwant.system.System` instances. Improved build configuration ----------------------------