Version 3.1.0 (January 1, 2015):
- MAJOR FEATURE: New module for quantum control (qutip.control).
- NAMESPACE CHANGE: QuTiP no longer exports symbols from NumPy and matplotlib, so those modules must now be explicitly imported when required.
- New module for counting statistics.
- Stochastic solvers now run trajectories in parallel.
- New superoperator and tensor manipulation functions
(super_tensor, composite, tensor_contract).
- New logging module for debugging (qutip.logging).
- New user-available API for parallelization (parallel_map).
- New enhanced (optional) text-based progressbar (qutip.ui.EnhancedTextProgressBar)
- Faster Python based monte carlo solver (mcsolve).
- Support for progress bars in propagator function.
- Time-dependent Cython code now calls complex cmath functions.
- Random numbers seeds can now be reused for successive calls to mcsolve.
- The Bloch-Redfield master equation solver now supports optional Lindblad type collapse operators.
- Improved handling of ODE integration errors in mesolve.
- Improved correlation function module (for example, improved support for time-dependent problems).
- Improved parallelization of mcsolve (can now be interrupted easily, support for IPython.parallel, etc.)
- Many performance improvements, and much internal code restructuring.
- Cython build files for time-dependent string format now removed automatically.
- Fixed incorrect solution time from inverse-power method steady state solver.
- mcsolve now supports Options(store_states=True)
- Fixed bug in hadamard gate function.
- Fixed compatibility issues with NumPy 1.9.0.
- Progressbar in mcsolve can now be suppressed.
- Fixed bug in gate_expand_3toN.
- Fixed bug for time-dependent problem (list string format) with multiple terms in coefficient to an operator.
Version 3.0.1 (Aug 5, 2014):
- Fix bug in create(), which returned a Qobj with CSC data instead of CSR.
- Fix several bugs in mcsolve: Incorrect storing of collapse times and collapse
operator records. Incorrect averaging of expectation values for different
trajectories when using only 1 CPU.
- Fix bug in parsing of time-dependent Hamiltonian/collapse operator arguments
that occurred when the args argument is not a dictionary.
- Fix bug in internal _version2int function that cause a failure when parsing
the version number of the Cython package.
Version 3.0.0 (July 17, 2014):
- New module qutip.stochastic with stochastic master equation and stochastic
Schrödinger equation solvers.
- Expanded steady state solvers. The function steady has been deprecated in
favor of steadystate. The steadystate solver no longer use umfpack by
default. New pre-processing methods for reordering and balancing the linear
equation system used in direct solution of the steady state.
- New module qutip.qip with utilities for quantum information processing,
including pre-defined quantum gates along with functions for expanding
arbitrary 1, 2, and 3 qubit gates to N qubit registers, circuit
representations, library of quantum algorithms, and basic physical models for
some common QIP architectures.
- New module qutip.distributions with unified API for working with
- New format for defining time-dependent Hamiltonians and collapse operators,
using a pre-calculated numpy array that specifies the values of the
Qobj-coefficients for each time step.
- New functions for working with different superoperator representations,
including Kraus and Chi representation.
- New functions for visualizing quantum states using Qubism and Schimdt plots:
plot_qubism and plot_schmidt.
- Dynamics solver now support taking argument e_ops (expectation value
operators) in dictionary form.
- Public plotting functions from the qutip.visualization module are now
prefixed with plot_ (e.g., plot_fock_distribution). The
plot_wigner and plot_wigner_fock_distribution now supports 3D views
in addition to contour views.
- New API and new functions for working with spin operators and states,
including for example spin_Jx, spin_Jy, spin_Jz and
- The expect function now supports a list of operators, in addition to the
previously supported list of states.
- Simplified creation of qubit states using ket function.
- The module qutip.cyQ has been renamed to qutip.cy and the sparse
matrix-vector functions spmv and spmv1d has been combined into one
function spmv. New functions for operating directly on the underlaying
sparse CSR data have been added (e.g., spmv_csr). Performance
improvements. New and improved Cython functions for calculating expectation
values for state vectors, density matrices in matrix and vector form.
- The concurrence function now supports both pure and mixed states. Added
function for calculating the entangling power of a two-qubit gate.
- Added function for generating (generalized) Lindblad dissipator
- New functions for generating Bell states, and singlet and triplet states.
- QuTiP no longer contains the demos GUI. The examples are now available on the
QuTiP web site. The qutip.gui module has been renamed to qutip.ui and
does no longer contain graphical UI elements. New text-based and HTML-based
- Support for harmonic oscillator operators/states in a Fock state basis that
does not start from zero (e.g., in the range [M,N+1]). Support for
eliminating and extracting states from Qobj instances (e.g., removing one
state from a two-qubit system to obtain a three-level system).
- Support for time-dependent Hamiltonian and Liouvillian callback functions that
depend on the instantaneous state, which for example can be used for solving
master equations with mean field terms.
- Restructured and optimized implementation of Qobj, which now has
significantly lower memory footprint due to avoiding excessive copying of
internal matrix data.
- The classes OdeData, Odeoptions, Odeconfig are now called
Result, Options, and Config, respectively, and are available in
the module qutip.solver.
- The squeez function has been renamed to squeeze.
- Better support for sparse matrices when calculating propagators using the
- Improved Bloch sphere.
- Restructured and improved the module qutip.sparse, which now only
operates directly on sparse matrices (not on Qobj instances).
- Improved and simplified implement of the tensor function.
- Improved performance, major code cleanup (including namespace changes),
and numerous bug fixes.
- Benchmark scripts improved and restructured.
- QuTiP is now using continuous integration tests (TravisCI).
Version 2.2.0 (March 01, 2013):
- Added Support for Windows
- New Bloch3d class for plotting 3D Bloch spheres using Mayavi.
- Bloch sphere vectors now look like arrows.
- Partial transpose function.
- Continuos variable functions for calculating correlation and covariance
matrices, the Wigner covariance matrix and the logarithmic negativity for
for multimode fields in Fock basis.
- The master-equation solver (mesolve) now accepts pre-constructed Liouvillian
terms, which makes it possible to solve master equations that are not on
the standard Lindblad form.
- Optional Fortran Monte Carlo solver (mcsolve_f90) by Arne Grimsmo.
- A module of tools for using QuTiP in IPython notebooks.
- Increased performance of the steady state solver.
- New Wigner colormap for highlighting negative values.
- More graph styles to the visualization module.
- Function based time-dependent Hamiltonians now keep the correct phase.
- mcsolve no longer prints to the command line if ntraj=1.
Version 2.1.0 (October 05, 2012):
- New method for generating Wigner functions based on Laguerre polynomials.
- coherent(), coherent_dm(), and thermal_dm() can now be expressed using analytic values.
- Unittests now use nose and can be run after installation.
- Added iswap and sqrt-iswap gates.
- Functions for quantum process tomography.
- Window icons are now set for Ubuntu application launcher.
- The propagator function can now take a list of times as argument, and returns a list of corresponding propagators.
- mesolver now correctly uses the user defined rhs_filename in Odeoptions().
- rhs_generate() now handles user defined filenames properly.
- Density matrix returned by propagator_steadystate is now Hermitian.
- eseries_value returns real list if all imag parts are zero.
- mcsolver now gives correct results for strong damping rates.
- Odeoptions now prints mc_avg correctly.
- Do not check for PyObj in mcsolve when gui=False.
- Eseries now correctly handles purely complex rates.
- thermal_dm() function now uses truncated operator method.
- Cython based time-dependence now Python 3 compatible.
- Removed call to NSAutoPool on mac systems.
- Progress bar now displays the correct number of CPU’s used.
- Qobj.diag() returns reals if operator is Hermitian.
- Text for progress bar on Linux systems is no longer cutoff.
Version 2.0.0 (June 01, 2012):
The second version of QuTiP has seen many improvements in the performance of the original code base, as well as the addition of several new routines supporting a wide range of functionality. Some of the highlights of this release include:
- QuTiP now includes solvers for both Floquet and Bloch-Redfield master equations.
- The Lindblad master equation and Monte Carlo solvers allow for time-dependent collapse operators.
- It is possible to automatically compile time-dependent problems into c-code using Cython (if installed).
- Python functions can be used to create arbitrary time-dependent Hamiltonians and collapse operators.
- Solvers now return Odedata objects containing all simulation results and parameters, simplifying the saving of simulation results.
This breaks compatibility with QuTiP version 1.x.
- mesolve and mcsolve can reuse Hamiltonian data when only the initial state, or time-dependent arguments, need to be changed.
- QuTiP includes functions for creating random quantum states and operators.
- The generation and manipulation of quantum objects is now more efficient.
- Quantum objects have basis transformation and matrix element calculations as built-in methods.
- The quantum object eigensolver can use sparse solvers.
- The partial-trace (ptrace) function is up to 20x faster.
- The Bloch sphere can now be used with the Matplotlib animation function, and embedded as a subplot in a figure.
- QuTiP has built-in functions for saving quantum objects and data arrays.
- The steady-state solver has been further optimized for sparse matrices, and can handle much larger system Hamiltonians.
- The steady-state solver can use the iterative bi-conjugate gradient method instead of a direct solver.
- There are three new entropy functions for concurrence, mutual information, and conditional entropy.
- Correlation functions have been combined under a single function.
- The operator norm can now be set to trace, Frobius, one, or max norm.
- Global QuTiP settings can now be modified.
- QuTiP includes a collection of unit tests for verifying the installation.
- Demos window now lets you copy and paste code from each example.
Version 1.1.4 (May 28, 2012):
- Fixed bug pointed out by Brendan Abolins.
- Qobj.tr() returns zero-dim ndarray instead of float or complex.
- Updated factorial import for scipy version 0.10+
Version 1.1.3 (November 21, 2011):
- Allow custom naming of Bloch sphere.
- Fixed text alignment issues in AboutBox.
- Added fix for SciPy V>0.10 where factorial was moved to scipy.misc module.
- Added tidyup function to tensor function output.
- Removed openmp flags from setup.py as new Mac Xcode compiler does not recognize them.
- Qobj diag method now returns real array if all imaginary parts are zero.
- Examples GUI now links to new documentation.
- Fixed zero-dimensional array output from metrics module.
Version 1.1.2 (October 27, 2011)
- Fixed issue where Monte Carlo states were not output properly.
Version 1.1.1 (October 25, 2011)
THIS POINT-RELEASE INCLUDES VASTLY IMPROVED TIME-INDEPENDENT MCSOLVE AND ODESOLVE PERFORMANCE
- Added linear entropy function.
- Number of CPU’s can now be changed.
- Metrics no longer use dense matrices.
- Fixed Bloch sphere grid issue with matplotlib 1.1.
- Qobj trace operation uses only sparse matrices.
- Fixed issue where GUI windows do not raise to front.
Version 1.1.0 (October 04, 2011)
THIS RELEASE NOW REQUIRES THE GCC COMPILER TO BE INSTALLED
- tidyup function to remove small elements from a Qobj.
- Added concurrence function.
- Added simdiag for simultaneous diagonalization of operators.
- Added eigenstates method returning eigenstates and eigenvalues to Qobj class.
- Added fileio for saving and loading data sets and/or Qobj’s.
- Added hinton function for visualizing density matrices.
- Switched Examples to new Signals method used in PySide 1.0.6+.
- Switched ProgressBar to new Signals method.
- Fixed memory issue in expm functions.
- Fixed memory bug in isherm.
- Made all Qobj data complex by default.
- Reduced ODE tolerance levels in Odeoptions.
- Fixed bug in ptrace where dense matrix was used instead of sparse.
- Fixed issue where PyQt4 version would not be displayed in about box.
- Fixed issue in Wigner where xvec was used twice (in place of yvec).
Version 1.0.0 (July 29, 2011)