krotov.mu module

Routines for mu in krotov.optimize.optimize_pulses()

The first-order Krotov update equation is usually written as

\[\begin{split}\Delta \epsilon(t) \propto \Im \Bigg\langle \chi_k^{(i)}(t) \Bigg\vert \Bigg( \left.\frac{\partial \Op{H}}{\partial \epsilon}\right\vert_{ {\scriptsize \begin{matrix} \phi^{(i+1)}(t)\\\epsilon^{(i+1)}(t) \end{matrix}}} \Bigg) \Bigg\vert \phi_k^{(i+1)}(t) \Bigg\rangle\,,\end{split}\]

where \(\ket{\chi_k}\) are states backward-propagated from a boundary condition determined by the functional, \(\ket{\phi_k}\) are forward-propagated from the initial states, and \(\frac{\partial \Op{H}}{\partial \epsilon}\) is the derivative of the Hamiltonian with respect to the field. However, this is true only for Hilbert-space states evolving under a Schrödinger equation.

More generally (e.g. when the states \(\chi_k\) and \(\phi_k\) are density matrices and the equation of motion is the master equation in Lindblad form), the correct formulation is

\[\frac{\partial \Op{H}}{\partial \epsilon} \rightarrow \mu = \frac{\partial H}{\partial \epsilon}\,,\]

where \(H\) is now the abstract operator appearing in the equation of motion of the abstract state

\[\dot\phi_k(t) = -i H \phi_k(t)\]

For density matrices, we have

\[\frac{\partial}{\partial t}\Op{\rho}_k(t) = \Liouville \Op{\rho}_k(t)\]

and thus \(H = i \Liouville\).

To allow for arbitrary equations of motion, a routine mu may be passed to optimize_pulses() that returns the abstract operator \(\mu\) as a Qobj, or alternatively as a callable that takes \(\phi_k\) as its argument and evaluates \(\mu \phi_k\). The default mu is derivative_wrt_pulse(), which covers the most common equation of motions:

  • standard Schrödinger equation

  • master equation, where either the H attribute of the objective contains a Hamiltonian and there are Lindblad operators in c_ops, or the H attribute contains a super-operator \(\Liouville\) directly (the case discussed above).

Alternative implementations of mu must have the same signature as derivative_wrt_pulse(), but should only be required in rare circumstances, such as when the derivative still depends on the control values or on the states. (Or, if you can provide a more efficient problem-specific implementation).

Summary

Functions:

derivative_wrt_pulse

Calculate ∂H/∂ϵ for the standard equations of motion.

__all__: derivative_wrt_pulse

Reference

krotov.mu.derivative_wrt_pulse(objectives, i_objective, pulses, pulses_mapping, i_pulse, time_index)[source]

Calculate ∂H/∂ϵ for the standard equations of motion.

Parameters

  • objectives (list) – List of Objective instances

  • i_objective (int) – The index of the objective in objectives whose equation of motion the derivative should be calculated.

  • pulses (list) – The list of pulses occuring in objectives

  • pulses_mapping (list) – The mapping of elements of pulses to the components of objectives, as returned by extract_controls_mapping()

  • i_pulse (int) – The index of the pulse in pulses for which to calculate the derivative

  • time_index (int) – The index of the value in pulses[i_pulse] that should be plugged in to ∂H/∂ϵ. Not used, as this routine only considers equations of motion that are linear in the controls.

Returns

The quantum operator or super-operator that represents ∂H/∂ϵ. In general, the return type can be any callable mu so that mu(state) calculates the result of applying ∂H/∂ϵ to state. In most cases, a Qobj will be returned, which is just the most convenient example of an appropriate callable.

Return type

callable

This function covers the following cases:

  • the H attribute of the objective contains a Hamiltonian, there are no c_ops (Schrödinger equation: the abstract H in ∂H/∂ϵ is the Hamiltonian directly)

  • the H attribute of the objective contains a Hamiltonian \(\Op{H}\), and there are Lindblad operators \(\Op{L}_i\) in c_ops (master equation in Lindblad form). The abstract H is \(i \Liouville\) for the Liouvillian defined as

    \[\Liouville[\Op{\rho}] = -i[\Op{H},\Op{\rho}]+\sum_{i} \left( \Op{L}_i \Op{\rho} \Op{L}_i^\dagger - \frac{1}{2} \left\{ \Op{L}_i^\dagger \Op{L}_i, \Op{\rho}\right\} \right)\]

  • the H attribute of the objective contains a super-operator \(\Liouville\), there are no c_ops (general master equation). The abstract H is again \(i \Liouville\).