Home - News ( United States | United Kingdom | Italy | Germany ) - Football scores

Showing content from https://github.com/qutip/qutip/releases/tag/v5.0.0 below:

Release QuTiP 5.0.0 · qutip/qutip · GitHub

QuTiP 5 is a redesign of many of the core components of QuTiP (Qobj,
QobjEvo, solvers) to make them more consistent and more flexible.

Qobj may now be stored in either sparse or dense representations,
and the two may be mixed sensibly as needed. QobjEvo is now used
consistently throughout QuTiP, and the implementation has been
substantially cleaned up. A new Coefficient class is used to
represent the time-dependent factors inside QobjEvo.

The solvers have been rewritten to work well with the new data layer
and the concept of Integrators which solve ODEs has been introduced.
In future, new data layers may provide their own Integrators
specialized to their representation of the underlying data.

Much of the user-facing API of QuTiP remains familiar, but there have
had to be many small breaking changes. If we can make changes to
easy migrating code from QuTiP 4 to QuTiP 5, please let us know.
A notebook to help with migration is available on colab.

An extensive list of changes follows.

QuTiP 5 has been a large effort by many people over the last three years.

In particular:

• Jake Lishman led the implementation of the new data layer and coefficients.
• Eric Giguère led the implementation of the new QobjEvo interface and solvers.
• Boxi Li led the updating of QuTiP's QIP support and the creation of qutip_qip.

Other members of the QuTiP Admin team have been heavily involved in reviewing,
testing and designing QuTiP 5:

• Alexander Pitchford
• Asier Galicia
• Nathan Shammah
• Shahnawaz Ahmed
• Neill Lambert
• Simon Cross
• Paul Menczel

Two Google Summer of Code contributors updated the tutorials and benchmarks to
QuTiP 5:

• Christian Staufenbiel updated many of the tutorials.
• Xavier Sproken update the benchmarks.

During an internship at RIKEN, Patrick Hopf created a new quantum control method and
improved the existing methods interface:

• Patrick Hopf created new quantum control package.

Four experimental data layers backends were written either as part of Google Summer
of Code or as separate projects. While these are still alpha quality, they helped
significantly to test the data layer API:

• qutip-tensorflow: a TensorFlow backend by Asier Galicia (https://github.com/qutip/qutip-tensorflow)
• qutip-cupy: a CuPy GPU backend by Felipe Bivort Haiek (https://github.com/qutip/qutip-cupy/)
• qutip-tensornetwork: a TensorNetwork backend by Asier Galicia (https://github.com/qutip/qutip-tensornetwork)
• qutip-jax: a JAX backend by Eric Giguère (https://github.com/qutip/qutip-jax/)

Finally, Yuji Tamakoshi updated the visualization function and added animation
functions as part of Google Summer of Code project.

We have also had many other contributors, whose specific contributions are
detailed below:

• Pieter Eendebak (updated the required SciPy to 1.5+, #1982)
• Pieter Eendebak (reduced import times by setting logger names, #1981)
• Pieter Eendebak (Allow scipy 1.12 to be used with qutip, #2354)
• Xavier Sproken (included C header files in the source distribution, #1971)
• Christian Staufenbiel (added support for multiple collapse operators to the Floquet solver, #1962)
• Christian Staufenbiel (fixed the basis used in the Floquet Master Equation solver, #1952)
• Christian Staufenbiel (allowed the bloch_redfield_tensor function to accept strings and callables for a_ops, #1951)
• Christian Staufenbiel (Add a guide on Superoperators, Pauli Basis and Channel Contraction, #1984)
• Henrique Silvéro (allowed qutip_qip to be imported as qutip.qip, #1920)
• Florian Hopfmueller (added a vastly improved implementations of process_fidelity and average_gate_fidelity, #1712, #1748 , #1788)
• Felipe Bivort Haiek (fixed inaccuracy in docstring of the dense implementation of negation, #1608)
• Rajath Shetty (added support for specifying colors for individual points, vectors and states display by qutip.Bloch, #1335)
• Rochisha Agarwal (Add dtype to printed ouput of qobj, #2352)
• Kosuke Mizuno (Add arguments of plot_wigner() and plot_wigner_fock_distribution() to specify parameters for wigner(), #2057)
• Matt Ord (Only pre-compute density matrices if keep_runs_results is False, #2303)
• Daniel Moreno Galán (Add the possibility to customize point colors as in V4 and fix point plot behavior for 'l' style, #2303)
• Sola85 (Fixed simdiag not returning orthonormal eigenvectors, #2269)
• Edward Thomas (Fix LaTeX display of Qobj state in Jupyter cell outputs, #2272)
• Bogdan Reznychenko (Rework kraus_to_choi making it faster, #2284)
• gabbence95 (Fix typos in expect documentation, #2331)
• lklivingstone (Added repr to QobjEvo, #2111)
• Yuji Tamakoshi (Improve print(qutip.settings) by make it shorter, #2113)
• khnikhil (Added fermionic annihilation and creation operators, #2166)
• Daniel Weiss (Improved sampling algorithm for mcsolve, #2218)
• SJUW (Increase missing colorbar padding for matrix_histogram_complex() from 0 to 0.05, #2181)
• Valan Baptist Mathuranayagam (Changed qutip-notebooks to qutip-tutorials and fixed the typo in the link redirecting to the changelog section in the PR template, #2107)
• Gerardo Jose Suarez (Added information on sec_cutoff to the documentation, #2136)
• Cristian Emiliano Godinez Ramirez (Added inherited members to API doc of MESolver, SMESolver, SSESolver, NonMarkovianMCSolver, #2167)
• Andrey Rakhubovsky (Corrected grammar in Bloch-Redfield master equation documentation, #2174)
• Rushiraj Gadhvi (qutip.ipynbtools.version_table() can now be called without Cython installed, #2110)
• Harsh Khilawala (Moved HTMLProgressBar from qutip/ipynbtools.py to qutip/ui/progressbar.py, #2112)
• Avatar Srinidhi P V (Added new argument bc_type to take boundary conditions when creating QobjEvo, #2114)
• Andrey Rakhubovsky (Fix types in docstring of projection(), #2363)

Previously Qobj data was stored in a SciPy-like sparse matrix. Now the
representation is flexible. Implementations for dense and sparse formats are
included in QuTiP and custom implementations are possible. QuTiP's performance
on dense states and operators is significantly improved as a result.

Some highlights:

• The data is still acessible via the .data attribute, but is now an
  instance of the underlying data type instead of a SciPy-like sparse matrix.
  The operations available in qutip.core.data may be used on .data,
  regardless of the data type.
• Qobj with different data types may be mixed in arithmetic and other
  operations. A sensible output type will be automatically determined.
• The new .to(...) method may be used to convert a Qobj from one data type
  to another. E.g. .to("dense") will convert to the dense representation and
  .to("csr") will convert to the sparse type.
• Many Qobj methods and methods that create Qobj now accepted a dtype
  parameter that allows the data type of the returned Qobj to specified.
• The new & operator may be used to obtain the tensor product.
• The new @ operator may be used to obtain the matrix / operator product.
  bar @ ket returns a scalar.
• The new .contract() method will collapse 1D subspaces of the dimensions of
  the Qobj.
• The new .logm() method returns the matrix logarithm of an operator.
• The methods .set_data, .get_data, .extract_state, .eliminate_states,
  .evaluate and .check_isunitary have been removed.
• The property dtype return the representation of the data used.
• The new data_as allow to obtain the data as a common python formats:
  numpy array, scipy sparse matrix, JAX Array, etc.

The QobjEvo type for storing time-dependent quantum objects has been
significantly expanded, standardized and extended. The time-dependent
coefficients are now represented using a new Coefficient type that
may be independently created and manipulated if required.

Some highlights:

• The .compile() method has been removed. Coefficients specified as
  strings are automatically compiled if possible and the compilation is
  cached across different Python runs and instances.
• Mixing coefficient types within a single Qobj is now supported.
• Many new attributes were added to QobjEvo for convenience. Examples
  include .dims, .shape, .superrep and .isconstant.
• Many old attributes such as .cte, .use_cython, .type, .const,
  and .coeff_file were removed.
• A new Spline coefficient supports spline interpolations of different
  orders. The old Cubic_Spline coefficient has been removed.
• The new .arguments(...) method allows additional arguments to the
  underlying coefficient functions to be updated.
• The _step_func_coeff argument has been replaced by the order
  parameter. _step_func_coeff=False is equivalent to order=3.
  _step_func_coeff=True is equivalent to order=0. Higher values
  of order gives spline interpolations of higher orders.
• The spline type can take bc_type to control the boundary conditions.
• QobjEvo can be creating from the multiplication of a Qobj with a coefficient:
  oper * qutip.coefficient(f, args=args) is equivalent to
  qutip.QobjEvo([[oper, f]], args=args).
• Coefficient function can be defined in a pythonic manner: def f(t, A, w).
  The dictionary args second argument is no longer needed.
  Function using the exact f(t, args) signature will use the old method for
  backward compatibility.

The solvers in QuTiP have been heavily reworked and standardized.
Under the hood solvers now make use of swappable ODE Integrators.
Many Integrators are included (see the list below) and
custom implementations are possible. Solvers now consistently
accept a QobjEvo instance at the Hamiltonian or Liouvillian, or
any object which can be passed to the QobjEvo constructor.

A breakdown of highlights follows.

• Solver options are now supplied in an ordinary Python dict.
  qutip.Options is deprecated and returns a dict for backwards
  compatibility.
• A specific ODE integrator may be selected by supplying a
  method option.
• Each solver provides a class interface. Creating an instance
  of the class allows a solver to be run multiple times for the
  same system without having to repeatedly reconstruct the
  right-hand side of the ODE to be integrated.
• A QobjEvo instance is accepted for most operators, e.g.,
  H, c_ops, e_ops, a_ops.
• The progress bar is now selected using the progress_bar option.
  A new progess bar using the tqdm Python library is provided.
• Dynamic arguments, where the value of an operator depends on
  the current state of the evolution interface reworked. Now a property of the
  solver is to be used as an arguments:
  args={"state": MESolver.StateFeedback(default=rho0)}

• The SciPy zvode integrator is available with the BDF and
  Adams methods as bdf and adams.
• The SciPy dop853 integrator (an eighth order Runge-Kutta method by
  Dormand & Prince) is available as dop853.
• The SciPy lsoda integrator is available as lsoda.
• QuTiP's own implementation of Verner's "most efficient" Runge-Kutta methods
  of order 7 and 9 are available as vern7 and vern9. See
  http://people.math.sfu.ca/~jverner/ for a description of the methods.
• QuTiP's own implementation of a solver that directly diagonalizes the
  the system to be integrated is available as diag. It only works on
  time-independent systems and is slow to setup, but once the diagonalization
  is complete, it generates solutions very quickly.
• QuTiP's own implementatoin of an approximate Krylov subspace integrator is
  available as krylov. This integrator is only usable with sesolve.

• A new .e_data attribute provides expectation values as a dictionary.
  Unlike .expect, the values are provided in a Python list rather than
  a numpy array, which better supports non-numeric types.
• The contents of the .stats attribute changed significantly and is
  now more consistent across solvers.

• The system, H, may now be a super-operator.
• The seed parameter now supports supplying numpy SeedSequence or
  Generator types.
• The new timeout and target_tol parameters allow the solver to exit
  early if a timeout or target tolerance is reached.
• The ntraj option no longer supports a list of numbers of trajectories.
  Instead, just run the solver multiple times and use the class MCSolver
  if setting up the solver uses a significant amount of time.
• The map_func parameter has been replaced by the map option.
• A loky based parallel map as been added.
• A mpi based parallel map as been added.
• The result returned by mcsolve now supports calculating photocurrents
  and calculating the steady state over N trajectories.
• The old parfor parallel execution function has been removed from
  qutip.parallel. Use parallel_map, loky_map or mpi_pmap instead.
• Added improved sampling options which converge much faster when the
  probability of collapse is small.

• New Monte-Carlo Solver supporting negative decay rates.
• Based on the influence martingale approach, Donvil et al., Nat Commun 13, 4140 (2022).
• Most of the improvements made to the regular Monte-Carlo solver are also available here.
• The value of the influence martingale is available through the .trace attribute of the result.

• Function call greatly changed: many keyword arguments are now options.
• m_ops and dW_factors are now changed from the default from the new class interface only.
• Use the same parallel maps as mcsolve: support for loky and mpi map added.
• End conditions timeout and target_tol added.
• The seed parameter now supports supplying numpy SeedSequence.
• Wiener function is now available as a feedback.

• The a_ops and spectra support implementations been heavily reworked to
  reuse the techniques from the new Coefficient and QobjEvo classes.
• The use_secular parameter has been removed. Use sec_cutoff=-1 instead.
• The required tolerance is now read from qutip.settings.

• The Krylov solver is now implemented using SESolver and the krylov
  ODE integrator. The function krylovsolve is maintained for convenience
  and now supports many more options.
• The sparse parameter has been removed. Supply a sparse Qobj for the
  Hamiltonian instead.

• The Floquet solver has been rewritten to use a new FloquetBasis class
  which manages the transformations from lab to Floquet basis and back.
• Many of the internal methods used by the old Floquet solvers have
  been removed. The Floquet tensor may still be retried using
  the function floquet_tensor.
• The Floquet Markov Master Equation solver has had many changes and
  new options added. The environment temperature may be specified using
  w_th, and the result states are stored in the lab basis and optionally
  in the Floquet basis using store_floquet_state.
• The spectra functions supplied to fmmesolve must now be vectorized
  (i.e. accept and return numpy arrays for frequencies and densities) and
  must accept negative frequence (i.e. usually include a w > 0 factor
  so that the returned densities are zero for negative frequencies).
• The number of sidebands to keep, kmax may only be supplied when using
  the FMESolver
• The Tsteps parameter has been removed from both fsesolve and
  fmmesolve. The precompute option to FloquetBasis may be used
  instead.

• The function essolve has been removed. Use the diag integration
  method with sesolve or mesolve instead.

• The method parameter and solver parameters have been separated. Previously
  they were mixed together in the method parameter.
• The previous options are now passed as parameters to the steady state
  solver and mostly passed through to the underlying SciPy functions.
• The logging and statistics have been removed.

• A new correlation_3op function has been added. It supports MESolver
  or BRMESolver.
• The correlation, correlation_4op, and correlation_ss functions have been
  removed.
• Support for calculating correlation with mcsolve has been removed.

• A class interface, qutip.Propagator, has been added for propagators.
• Propagation of time-dependent systems is now supported using QobjEvo.
• The unitary_mode and parallel options have been removed.

• The functions spectrum_ss and spectrum_pi have been removed and
  are now internal functions.
• The use_pinv parameter for spectrum has been removed and the
  functionality merged into the solver parameter. Use solver="pi"
  instead.

• Updated the solver to use the new QuTiP integrators and data layer.
• Updated all the HEOM tutorials to QuTiP 5.
• Added support for combining bosonic and fermionic baths.
• Sped up the construction of the RHS of the HEOM solver by a factor of 4x.
• As in QuTiP 4, the HEOM supports arbitrary spectral densities, bosonic and fermionic baths, Páde and Matsubara expansions of the correlation functions, calculating the Matsubara terminator and inspection of the ADOs (auxiliary density operators).

There have been numerous other small changes to core QuTiP features:

• qft(...) the function that returns the quantum Fourier
  transform operator was moved from qutip.qip.algorithm into qutip.
• The Bloch-Redfield solver tensor, brtensor, has been moved into
  qutip.core. See the section above on the Bloch-Redfield solver
  for details.
• The functions mat2vec and vec2mat for transforming states to and
  from super-operator states have been renamed to stack_columns and
  unstack_columns.
• The function liouvillian_ref has been removed. Used liouvillian
  instead.
• The superoperator transforms super_to_choi, choi_to_super,
  choi_to_kraus, choi_to_chi and chi_to_choi have been removed.
  Used to_choi, to_super, to_kraus and to_chi instead.
• All of the random object creation functions now accepted a
  numpy Generator as a seed.
• The dims parameter of all random object creation functions has
  been removed. Supply the dimensions as the first parameter if
  explicit dimensions are required.
• The function rand_unitary_haar has been removed. Use
  rand_unitary(distribution="haar") instead.
• The functions rand_dm_hs and rand_dm_ginibre have been removed.
  Use rand_dm(distribution="hs") and rand_dm(distribution="ginibre")
  instead.
• The function rand_ket_haar has been removed. Use
  rand_ket(distribution="haar") instead.
• The measurement functions have had the target parameter for
  expanding the measurement operator removed. Used expand_operator
  to expand the operator instead.
• qutip.Bloch now supports applying colours per-point, state or vector in
  add_point, add_states, and add_vectors.
• Dimensions use a class instead of layered lists.
• Allow measurement functions to support degenerate operators.
• Add qeye_like and qzero_like.
• Added fermionic annihilation and creation operators.

Previously qutip.settings was an ordinary module. Now qutip.settings is
an instance of a settings class. All the runtime modifiable settings for
core operations are in qutip.settings.core. The other settings are not
modifiable at runtime.

• Removed load. reset and save functions.
• Removed .debug, .fortran, .openmp_thresh.
• New .compile stores the compilation options for compiled coefficients.
• New .core["rtol"] core option gives the default relative tolerance used by QuTiP.
• The absolute tolerance setting .atol has been moved to .core["atol"].

• Added arguments to plot_wigner and plot_wigner_fock_distribution to specify parameters for wigner.
• Removed Bloch3D. The same functionality is provided by Bloch.
• Added fig, ax and cmap keyword arguments to all visualization functions.
• Most visualization functions now respect the colorblind_safe setting.
• Added new functions to create animations from a list of Qobj or directly from solver results with saved states.

• qutip.qip has been moved into its own package, qutip-qip. Once installed, qutip-qip is available as either qutip.qip or qutip_qip. Some widely useful gates have been retained in qutip.gates.
• qutip.control has been moved to qutip-qtrl and once installed qutip-qtrl is available as either qutip.control or qutip_qtrl. Note that quitp_qtrl is provided primarily for backwards compatibility. Improvements to optimal control will take place in the new qutip_qoc package.
• qutip.lattice has been moved into its own package, qutip-lattice. It is available from <https://github.com/qutip/qutip-lattice>.
• qutip.sparse has been removed. It contained the old sparse matrix representation and is replaced by the new implementation in qutip.data.
• qutip.piqs functions are no longer available from the qutip namespace. They are accessible from qutip.piqs instead.

• Support has been added for 64-bit integer sparse matrix indices, allowing
  sparse matrices with up to 2**63 rows and columns. This support needs to
  be enabled at compilation time by calling setup.py and passing
  --with-idxint-64.

• Support for OpenMP has been removed. If there is enough demand and a good plan for how to organize it, OpenMP support may return in a future QuTiP release.
• The qutip.parfor function has been removed. Use qutip.parallel_map instead.
• qutip.graph has been removed and replaced by SciPy's graph functions.
• qutip.topology has been removed. It contained only one function berry_curvature.
• The ~/.qutip/qutiprc config file is no longer supported. It contained settings for the OpenMP support.
• Deprecate three_level_atom
• Deprecate orbital

• Add dtype to printed ouput of qobj (#2352 by Rochisha Agarwal)

• Allow scipy 1.12 to be used with qutip. (#2354 by Pieter Eendebak)

RetroSearch is an open source project built by @garambo | Open a GitHub Issue

Search and Browse the WWW like it's 1997 | Search results from DuckDuckGo

HTML: 3.2 | Encoding: UTF-8 | Version: 0.7.4