AKLTChain
full name: tenpy.models.aklt.AKLTChain
parent module:
tenpy.models.aklt
type: class
Inheritance Diagram
Methods
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Calculate bond energies <psi|H_bond|psi>. |
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Calculate the MPO Hamiltonian from the bond Hamiltonian. |
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Calculate the bond Hamiltonian from the MPO Hamiltonian. |
Shallow copy of self. |
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Repeat the unit cell for infinite MPS boundary conditions; in place. |
Returns the expected saving factor for RAM based on charge conservation. |
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Return a (shallow) copy with extracted segment of MPS. |
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Initialize a NearestNeighborModel from a model class defining an MPO. |
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Load instance from a HDF5 file. |
Get list of model-dependent extra default measurements. |
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Modify self in place to group sites. |
Initialize the chi=2 MPS which is exact ground state of the AKLT model. |
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Export self into a HDF5 file. |
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Return a NearestNeighborModel with same lattice, but trivial (H=0) bonds. |
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Reconstruct Hamiltonian for time-dependent models, potentially (!) in-place. |
Class Attributes and Properties
class attribute. |
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Reproducible numpy pseudo random number generator. |
- class tenpy.models.aklt.AKLTChain(model_params)[source]
Bases:
NearestNeighborModel
,MPOModel
A simple implementation of the AKLT model.
Here we define the Hamiltonian on a chain of S=1 spins as originally defined by Affleck, Kennedy, Lieb, Tasaki in [affleck1987], but dropping the constant parts of 1/3 per bond and rescaling with a factor of 2, such that we expect a ground state energy of
E_0 = - (L-1) 2/3 * J
.\[H = J \sum_i 2* P^{S=2}_{i,i+1} + const = J \sum_i (\vec{S}_i \cdot \vec{S}_{i+1} +\frac{1}{3} (\vec{S}_i \cdot \vec{S}_{i+1})^2)\]- psi_AKLT()[source]
Initialize the chi=2 MPS which is exact ground state of the AKLT model.
- Returns:
psi_aklt – The AKLT groundstate
- Return type:
- bond_energies(psi)[source]
Calculate bond energies <psi|H_bond|psi>.
- Parameters:
psi (
MPS
) – The MPS for which the bond energies should be calculated.- Returns:
E_bond – List of bond energies: for finite bc,
E_Bond[i]
is the energy of bondi, i+1
. (i.e. we omit bond 0 between sites L-1 and 0); for infinite bcE_bond[i]
is the energy of bondi-1, i
.- Return type:
1D ndarray
- calc_H_MPO_from_bond(tol_zero=1e-15)[source]
Calculate the MPO Hamiltonian from the bond Hamiltonian.
- calc_H_bond_from_MPO(tol_zero=1e-15)[source]
Calculate the bond Hamiltonian from the MPO Hamiltonian.
- Parameters:
tol_zero (float) – Arrays with norm < tol_zero are considered to be zero.
- Returns:
H_bond – Bond terms as required by the constructor of
NearestNeighborModel
. Legs are['p0', 'p0*', 'p1', 'p1*']
- Return type:
list of
Array
:raises ValueError : if the Hamiltonian contains longer-range terms.:
- enlarge_mps_unit_cell(factor=2)[source]
Repeat the unit cell for infinite MPS boundary conditions; in place.
This has to be done after finishing initialization and can not be reverted.
- Parameters:
factor (int) – The new number of sites in the MPS unit cell will be increased from N_sites to
factor*N_sites_per_ring
. Since MPS unit cells are repeated in the x-direction in our convention, the lattice shape goes from(Lx, Ly, ..., Lu)
to(Lx*factor, Ly, ..., Lu)
.
- estimate_RAM_saving_factor()[source]
Returns the expected saving factor for RAM based on charge conservation.
- Returns:
factor – saving factor, due to conservation
- Return type:
Options
- mem_saving_factor :: None | float
Quantizes the RAM saving, due to conservation laws, to be used by
estimate_simulation_RAM()
. By default it is 1/mod, or 1/4 in case of mod=1. However, for some classes this factor might be overwritten, if a better approximation is known. In the best case, the user can adjust this model parameter to enhance the estimate.
- extract_segment(*args, **kwargs)[source]
Return a (shallow) copy with extracted segment of MPS.
- Parameters:
first (int) – See
extract_segment()
.last (int) – See
extract_segment()
.enlarge (int) – See
extract_segment()
.
- Returns:
cp – A shallow copy of self with MPO and lattice extracted for the segment.
- Return type:
Model
- classmethod from_MPOModel(mpo_model)[source]
Initialize a NearestNeighborModel from a model class defining an MPO.
This is especially useful in combination with
MPOModel.group_sites()
.- Parameters:
mpo_model (
MPOModel
) – A model instance implementing the MPO. Does not need to be aNearestNeighborModel
, but should only have nearest-neighbor couplings.
Examples
The SpinChainNNN2 has next-nearest-neighbor couplings and thus only implements an MPO:
>>> from tenpy.models.spins_nnn import SpinChainNNN2 >>> nnn_chain = SpinChainNNN2({'L': 20, 'sort_charge': True}) >>> print(isinstance(nnn_chain, NearestNeighborModel)) False >>> print("range before grouping:", nnn_chain.H_MPO.max_range) range before grouping: 2
By grouping each two neighboring sites, we can bring it down to nearest neighbors.
>>> grouped_sites = nnn_chain.group_sites(2) >>> print("range after grouping:", nnn_chain.H_MPO.max_range) range after grouping: 1
Yet, TEBD will not yet work, as the model doesn’t define H_bond. However, we can initialize a NearestNeighborModel from the MPO:
>>> nnn_chain_for_tebd = NearestNeighborModel.from_MPOModel(nnn_chain) >>> isinstance(nnn_chain_for_tebd, NearestNeighborModel) True
- classmethod from_hdf5(hdf5_loader, h5gr, subpath)[source]
Load instance from a HDF5 file.
Same as
from_hdf5()
, but handlerng
.
- get_extra_default_measurements()[source]
Get list of model-dependent extra default measurements.
Extra measurements for a
Simulation
, which depend on the model itself - subclasses should override this method). E.g., aMPOModel
should measure the energy w.r.t. the MPO (Seem_energy_MPO()
). However, aNearestNeighborModel
should use the functionm_bond_energies()
. The extra measurements are added to the default measurements in_connect_measurements()
.- Returns:
m_extra_default_list
- Return type:
- group_sites(n=2, grouped_sites=None)[source]
Modify self in place to group sites.
Group each n sites together using the
GroupedSite
. This might allow to do TEBD with a Trotter decomposition, or help the convergence of DMRG (in case of too long range interactions).This has to be done after finishing initialization and can not be reverted.
- Parameters:
n (int) – Number of sites to be grouped together.
grouped_sites (None | list of
GroupedSite
) – The sites grouped together.
- Returns:
grouped_sites – The sites grouped together.
- Return type:
list of
GroupedSite
- logger = <Logger tenpy.models.model.Model (WARNING)>
class attribute.
- Type:
- Type:
An instance of a logger; see Logging and terminal output. NB
- property rng
Reproducible numpy pseudo random number generator.
If you want to add randomness/disorder to your model, it is recommended use this random number generator for reproducibility of the model:
self.rng.random(size=[3, 5])
Especially for models with time-dependence, you can/will otherwise end up generating a new disordered at each time-step!
Options
- random_seed :: None | int
Defaults to 123456789. Seed for numpy pseudo random number generator which can be used as e.g.
self.rng.random(...)
.
- save_hdf5(hdf5_saver, h5gr, subpath)[source]
Export self into a HDF5 file.
Same as
save_hdf5()
, but handlerng
.
- trivial_like_NNModel()[source]
Return a NearestNeighborModel with same lattice, but trivial (H=0) bonds.
- update_time_parameter(new_time)[source]
Reconstruct Hamiltonian for time-dependent models, potentially (!) in-place.
For
TimeDependentHAlgorithm
, we assume that the model reads out the parameterself.options['time']
, and reinitialize/update the model calling this method.- Parameters:
new_time (float) – Time at which the (time-dependent) Hamiltonian should be constructed.
- Returns:
updated_model – Model of the same class as self with Hamiltonian at time new_time. Note that it can just be a reference to self if modified in place, or an entirely new constructed model.
- Return type:
model