diff --git a/tutorials-v4/time-evolution/002_larmor-precession.md b/tutorials-v4/time-evolution/002_larmor-precession.md index 554bb288..8aecd8fc 100644 --- a/tutorials-v4/time-evolution/002_larmor-precession.md +++ b/tutorials-v4/time-evolution/002_larmor-precession.md @@ -21,7 +21,7 @@ Author: C. Staufenbiel, 2022 This notebook guides you through the process of setting up a Schrödinger equation in QuTiP and using the corresponding solver to obtain the time evolution. We will investigate the example of the Larmor precession to -explore the functionality of [`qutip.sesolve()`](https://qutip.readthedocs.io/en/latest/apidoc/functions.html?highlight=sesolve#module-qutip.sesolve). +explore the functionality of [`qutip.sesolve()`](https://qutip.readthedocs.io/en/latest/apidoc/solver.html#module-qutip.solver.sesolve). You can also find more on time evolutions with QuTiP [here](https://qutip.readthedocs.io/en/latest/guide/guide-dynamics.html). @@ -85,7 +85,7 @@ b.show() ## Simulation with varying magnetic field -Above we passed a constant Hamiltonian to `sesolve`. In QuTiP these constant operators are represented by `Qobj`. However, `sesolve` can also take time-dependent operators as an argument, which are represented by [`QobjEvo`](https://qutip.readthedocs.io/en/latest/apidoc/classes.html?highlight=qobjevo#qutip.QobjEvo) in QuTiP. In this section we define the magnetic field with a linear and a periodic field strength, and observe the changes in the expecation value of $\sigma_y$. +Above we passed a constant Hamiltonian to `sesolve`. In QuTiP these constant operators are represented by `Qobj`. However, `sesolve` can also take time-dependent operators as an argument, which are represented by [`QobjEvo`](https://qutip.readthedocs.io/en/latest/apidoc/time_dep.html#qutip.core.cy.qobjevo.QobjEvo) in QuTiP. In this section we define the magnetic field with a linear and a periodic field strength, and observe the changes in the expecation value of $\sigma_y$. You can find more information on `QobjEvo` in [this notebook](https://nbviewer.jupyter.org/github/qutip/qutip-notebooks/blob/master/examples/qobjevo.ipynb). We start by defining two functions for the field strength of the magnetic field. To be passed on to `QobjEvo` the functions need two arguments: the times and optional arguments. diff --git a/tutorials-v4/time-evolution/003_qubit-dynamics.md b/tutorials-v4/time-evolution/003_qubit-dynamics.md index 74efefac..2592d178 100644 --- a/tutorials-v4/time-evolution/003_qubit-dynamics.md +++ b/tutorials-v4/time-evolution/003_qubit-dynamics.md @@ -21,7 +21,7 @@ Modified by: C. Staufebiel (2022) ### Introduction In this notebook we will explore the dynamics of a single-qubit interacting with an environment. The evolution of the qubit state is governed by the Master equation. We will make use of the master equation solver `qutip.mesolve` implemented in qutip, to obtain the time-evolution of the qubit for different settings. -You can read more about the master equation solver (and the theory behind it) in the [QuTiP docs](https://qutip.readthedocs.io/en/latest/apidoc/functions.html?highlight=sesolve#module-qutip.sesolve). +You can read more about the master equation solver (and the theory behind it) in the [QuTiP docs](https://qutip.readthedocs.io/en/latest/apidoc/time_dep.html#qutip.core.cy.qobjevo.QobjEvo). ### Import Here we import the required modules for this example. diff --git a/tutorials-v5/heom/heom-5b-fermions-discrete-boson-model.md b/tutorials-v5/heom/heom-5b-fermions-discrete-boson-model.md index bc2e23e5..7e139d8d 100644 --- a/tutorials-v5/heom/heom-5b-fermions-discrete-boson-model.md +++ b/tutorials-v5/heom/heom-5b-fermions-discrete-boson-model.md @@ -20,7 +20,7 @@ kernelspec: Here we model a single fermion coupled to two electronic leads or reservoirs (e.g., this can describe a single quantum dot, a molecular transistor, etc), also coupled to a discrete bosonic (vibronic) mode. -Note that in this implementation we primarily follow the definitions used by Christian Schinabeck in his Dissertation https://opus4.kobv.de/opus4-fau/files/10984/DissertationChristianSchinabeck.pdf and related publications. In particular this example reproduces some results from https://journals.aps.org/prb/abstract/10.1103/PhysRevB.94.201407 +Note that in this implementation we primarily follow the definitions used by Christian Schinabeck in his Dissertation https://open.fau.de/items/36fdd708-a467-4b59-bf4e-4a2110fbc431 and related publications. In particular this example reproduces some results from https://journals.aps.org/prb/abstract/10.1103/PhysRevB.94.201407 Notation: diff --git a/tutorials-v5/time-evolution/002_larmor-precession.md b/tutorials-v5/time-evolution/002_larmor-precession.md index 053a722c..c066154a 100644 --- a/tutorials-v5/time-evolution/002_larmor-precession.md +++ b/tutorials-v5/time-evolution/002_larmor-precession.md @@ -21,7 +21,7 @@ Author: C. Staufenbiel, 2022 This notebook guides you through the process of setting up a Schrödinger equation in QuTiP and using the corresponding solver to obtain the time evolution. We will investigate the example of the Larmor precession to -explore the functionality of [`qutip.sesolve()`](https://qutip.readthedocs.io/en/latest/apidoc/functions.html?highlight=sesolve#module-qutip.sesolve). +explore the functionality of [`qutip.sesolve()`](https://qutip.readthedocs.io/en/latest/apidoc/solver.html#module-qutip.solver.sesolve). You can also find more on time evolutions with QuTiP [here](https://qutip.readthedocs.io/en/latest/guide/guide-dynamics.html). @@ -85,7 +85,7 @@ b.show() ## Simulation with varying magnetic field -Above we passed a constant Hamiltonian to `sesolve`. In QuTiP these constant operators are represented by `Qobj`. However, `sesolve` can also take time-dependent operators as an argument, which are represented by [`QobjEvo`](https://qutip.readthedocs.io/en/latest/apidoc/classes.html?highlight=qobjevo#qutip.QobjEvo) in QuTiP. In this section we define the magnetic field with a linear and a periodic field strength, and observe the changes in the expecation value of $\sigma_y$. +Above we passed a constant Hamiltonian to `sesolve`. In QuTiP these constant operators are represented by `Qobj`. However, `sesolve` can also take time-dependent operators as an argument, which are represented by [`QobjEvo`](https://qutip.readthedocs.io/en/latest/apidoc/time_dep.html#qutip.core.cy.qobjevo.QobjEvo) in QuTiP. In this section we define the magnetic field with a linear and a periodic field strength, and observe the changes in the expecation value of $\sigma_y$. You can find more information on `QobjEvo` in [this notebook](https://nbviewer.jupyter.org/github/qutip/qutip-notebooks/blob/master/examples/qobjevo.ipynb). We start by defining two functions for the field strength of the magnetic field. To be passed on to `QobjEvo` the functions need two arguments: the times and optional arguments. diff --git a/tutorials-v5/time-evolution/003_qubit-dynamics.md b/tutorials-v5/time-evolution/003_qubit-dynamics.md index 804f0849..d0efd3bf 100644 --- a/tutorials-v5/time-evolution/003_qubit-dynamics.md +++ b/tutorials-v5/time-evolution/003_qubit-dynamics.md @@ -21,7 +21,7 @@ Modified by: C. Staufebiel (2022) ### Introduction In this notebook we will explore the dynamics of a single-qubit interacting with an environment. The evolution of the qubit state is governed by the Master equation. We will make use of the master equation solver `qutip.mesolve` implemented in qutip, to obtain the time-evolution of the qubit for different settings. -You can read more about the master equation solver (and the theory behind it) in the [QuTiP docs](https://qutip.readthedocs.io/en/latest/apidoc/functions.html?highlight=sesolve#module-qutip.sesolve). +You can read more about the master equation solver (and the theory behind it) in the [QuTiP docs](https://qutip.readthedocs.io/en/latest/guide/dynamics/dynamics-master.html). ### Import Here we import the required modules for this example.