Fermions

Building blocks

All fermionic objects in struqture are expressed based on products of fermionic creation and annihilation operators, which respect fermionic anti-commutation relations \[ \lbrace c_k^{\dagger}, c_j^{\dagger} \rbrace = 0, \\ \lbrace c_k, c_j \rbrace = 0, \\ \lbrace c_k, c_j^{\dagger} \rbrace = \delta_{k, j}. \]

FermionProducts

FermionProducts are simple combinations of fermionic creation and annihilation operators.

HermitianFermionProducts

HermitianFermionProducts are the hermitian equivalent of FermionProducts. This means that even though they are constructed the same (see the next section, Examples), they internally store both that term and its hermitian conjugate. For instance, given the term \(c^{\dagger}_0 c_1 c_2\), a FermionProduct would represent \(c^{\dagger}_0 c_1 c_2\) while a HermitianFermionProduct would represent \(c^{\dagger}_0 c_1 c_2 + c^{\dagger}_2 c^{\dagger}_1 c_0\).

Examples

In both Python and Rust, the operator product is constructed by passing an array or a list of integers to represent the creation indices, and an array or a list of integers to represent the annihilation indices.

Note: (Hermitian)FermionProducts can only been created from the correct ordering of indices (the wrong sequence will return an error) but we have the create_valid_pair function to create a valid Product from arbitrary sequences of operators which also transforms an index value according to the anti-commutation and hermitian conjugation rules.

from struqture_py.fermions import FermionProduct, HermitianFermionProduct
from qoqo_calculator_pyo3 import CalculatorComplex

# A product of a creation operator acting on fermionic mode 0 and an
# annihilation operator acting on fermionic mode 20
fp = FermionProduct([0], [20])
# Building the term c^{\dagger}_1 * c^{\dagger}_3 * c_0
fp = FermionProduct.create_valid_pair(
    [3, 1], [0], CalculatorComplex.from_pair(1.0, 0.0))


# A product of a creation operator acting on fermionic mode 0 and an annihilation
# operator acting on fermionic mode 20, as well as a creation operator acting on
# fermionic mode 20 and an annihilation operator acting on fermionic mode 0
hfp = HermitianFermionProduct([0], [20])
# Building the term c^{\dagger}_0 * c^{\dagger}_3 * c_0 + c^{\dagger}_0 * c_3 * c_0
hfp = HermitianFermionProduct.create_valid_pair(
    [3, 0], [0], CalculatorComplex.from_pair(1.0, 0.0))

In Rust the equivalent string representation cannot be used in function and method arguments.

use qoqo_calculator::CalculatorComplex;
use struqture::fermions::{FermionProduct, HermitianFermionProduct};
use struqture::prelude::*;

// Building the term c^{\dagger}_0 c_20
let fp_0 = FermionProduct::new([0], [20]).unwrap();
// Building the term c^{\dagger}_1 * c^{\dagger}_3 * c_0
let (fp_1, coeff) = FermionProduct::create_valid_pair(
    [3, 1], [0], CalculatorComplex::from(1.0)).unwrap();


// A product of a creation operator acting on fermionic mode 0 and an annihilation
// operator acting on fermionic mode 20, as well as a creation operator acting on
// fermionic mode 20 and an annihilation operator acting on fermionic mode 0
let fp_0 = HermitianFermionProduct::new([0], [20]).unwrap();
// Building the term c^{\dagger}_0 * c^{\dagger}_3 * c_0 + c^{\dagger}_0 * c_3 * c_0
let (fp_1, coeff) = HermitianFermionProduct::create_valid_pair(
    [3, 0], [0], CalculatorComplex::from(1.0)).unwrap();

Operators and Hamiltonians

Complex objects are constructed from operator products are FermionOperators and FermionHamiltonians (for more information, see also).

These FermionOperators and FermionHamiltonians represent operators or Hamiltonians such as: \[ \hat{O} = \sum_{j=0}^N \alpha_j \left( \prod_{k=0}^N f(j, k) \right) \left( \prod_{l=0}^N g(j, l) \right) \] with \[ f(j, k) = \begin{cases} c_k^{\dagger} \\ \mathbb{1} \end{cases} , \] \[ g(j, l) = \begin{cases} c_l \\ \mathbb{1} \end{cases} , \] and \(c^{\dagger}\) the fermionionic creation operator, \(c\) the fermionionic annihilation operator \[ \lbrace c_k^{\dagger}, c_j^{\dagger} \rbrace = 0, \\ \lbrace c_k, c_j \rbrace = 0, \\ \lbrace c_k^{\dagger}, c_j \rbrace = \delta_{k, j}. \]

For instance, \(c^{\dagger}_0 c^{\dagger}_1 c_1\) is a term with a \(c^{\dagger}\) term acting on 0, and both a \(c^{\dagger}\) term and a \(c\) term acting on 1.

From a programming perspective the operators and Hamiltonians are HashMaps or Dictionaries with FermionProducts or HermitianFermionProducts (respectively) as keys and the coefficients \(\alpha_j\) as values.

In struqture we distinguish between fermionic operators and Hamiltonians to avoid introducing unphysical behaviour by accident. While both are sums over normal ordered fermionic products (stored as HashMaps of products with a complex prefactor), Hamiltonians are guaranteed to be hermitian. In a fermionic Hamiltonian , this means that the sums of products are sums of hermitian fermionic products (we have not only the \(c^{\dagger}c\) terms but also their hermitian conjugate) and the on-diagonal terms are required to have real prefactors. In the HermitianFermionProducts, we only explicitly store one part of the hermitian fermionic product, and we have chosen to store the one which has the smallest index of the creators that is smaller than the smallest index of the annihilators.

Examples

Here is an example of how to build a product and using it to build an operator, in Rust:

use qoqo_calculator::CalculatorComplex;
use struqture::prelude::*;
use struqture::fermions::{
    FermionProduct, FermionOperator, HermitianFermionProduct, FermionHamiltonian
};

// Building the term c^{\dagger}_1 * c^{\dagger}_2 * c_0 * c_1
let fp = FermionProduct::new([1, 2], [0, 1]).unwrap();

// O = (1 + 1.5 * i) * c^{\dagger}_1 * c^{\dagger}_2 * c_0 * c_1
let mut operator = FermionOperator::new();
operator.add_operator_product(fp.clone(), CalculatorComplex::new(1.0, 1.5)).unwrap();
println!("{}", operator);

// Or when overwriting the previous value
let mut operator = FermionOperator::new();
operator.set(fp.clone(), CalculatorComplex::new(1.0, 1.5)).unwrap();
println!("{}", operator);

// A FermionProduct entry is not valid for a FermionHamiltonian
let mut hamiltonian = FermionHamiltonian::new();
// This would fail, as it uses HermitianFermionProducts, not FermionProducts
hamiltonian.add_operator_product(fp, CalculatorComplex::new(1.0, 1.5)).unwrap();
// This is possible
let hfp = HermitianFermionProduct::new([0, 2], [0, 1]).unwrap();
hamiltonian.add_operator_product(hfp, CalculatorComplex::new(1.5, 0.0)).unwrap();
println!("{}", hamiltonian);

The equivalent code in python:

from qoqo_calculator_pyo3 import CalculatorComplex
from struqture_py import fermions

operator = fermions.FermionHamiltonian()

# This will work
hfp = fermions.HermitianFermionProduct([0, 1], [0, 2])
operator.add_operator_product(hfp, CalculatorComplex.from_pair(1.0, 1.5))
hfp = fermions.HermitianFermionProduct([3], [3])
operator.add_operator_product(hfp, CalculatorComplex.from_pair(1.0, 0.0))
print(operator)

Noise operators

We describe decoherence by representing it with the Lindblad equation. The Lindblad equation is a master equation determining the time evolution of the density matrix. It is given by \[ \dot{\rho} = \mathcal{L}(\rho) = -i [\hat{H}, \rho] + \sum_{j,k} \Gamma_{j,k} \left( L_{j}\rho L_{k}^{\dagger} - \frac{1}{2} \{ L_k^{\dagger} L_j, \rho \} \right) \] with the rate matrix \(\Gamma_{j,k}\) and the Lindblad operator \(L_{j}\).

To describe fermionic noise we use the Lindblad equation with \(\hat{H}=0\). Therefore, to describe the pure noise part of the Lindblad equation one needs the rate matrix in a well defined basis of Lindblad operators. We use FermionProducts as the operator basis.

The rate matrix and with it the Lindblad noise model is saved as a sum over pairs of FermionProducts, giving the operators acting from the left and right on the density matrix. In programming terms the object FermionLindbladNoiseOperator is given by a HashMap or Dictionary with the tuple (FermionProduct, FermionProduct) as keys and the entries in the rate matrix as values.

Examples

Here, we add the terms \(L_0 = c^{\dagger}_0 c_0\) and \(L_1 = c^{\dagger}_0 c_0\) with coefficient 1.0: \( 1.0 \left( L_0 \rho L_1^{\dagger} - \frac{1}{2} \{ L_1^{\dagger} L_0, \rho \} \right) \)

use qoqo_calculator::CalculatorComplex;
use struqture::prelude::*;
use struqture::fermions::{FermionProduct, FermionLindbladNoiseOperator};

// Setting up the operator and the product we want to add to it
let mut operator = FermionLindbladNoiseOperator::new();
let fp = FermionProduct::new([0], [0]).unwrap();

// Adding the product to the operator
operator
    .add_operator_product(
        (fp.clone(), fp.clone()),
        CalculatorComplex::new(1.0, 0.0)
    ).unwrap();
assert_eq!(operator.get(&(fp.clone(), fp)), &CalculatorComplex::new(1.0, 0.0));
println!("{}", operator);

The equivalent code in python:

from qoqo_calculator_pyo3 import CalculatorComplex
from struqture_py import fermions

# Setting up the operator and the product we want to add to it
operator = fermions.FermionLindbladNoiseOperator()
fp = fermions.FermionProduct([0], [0])

# Adding the product to the operator
operator.add_operator_product((fp, fp), CalculatorComplex.from_pair(1.0, 1.5))
print(operator)

# In python we can also use the string representation
operator = fermions.FermionLindbladNoiseSystem()
operator.add_operator_product((str(fp), str(fp)), 1.0+1.5*1j)
print(operator)

Open systems

Physically open systems are quantum systems coupled to an environment that can often be described using Lindblad type of noise. The Lindblad master equation is given by \[ \dot{\rho} = \mathcal{L}(\rho) =-i [\hat{H}, \rho] + \sum_{j,k} \Gamma_{j,k} \left( L_{j}\rho L_{k}^{\dagger} - \frac{1}{2} \{ L_k^{\dagger} L_j, \rho \} \right) \] In struqture they are composed of a Hamiltonian (FermionHamiltonian) and noise (FermionLindbladNoiseOperator). They have different ways to set terms in Rust and Python:

Examples

use qoqo_calculator::CalculatorComplex;
use struqture::prelude::*;
use struqture::fermions::{
    FermionProduct, HermitianFermionProduct, FermionLindbladOpenSystem
};

let mut open_system = FermionLindbladOpenSystem::new();

let hfp = HermitianFermionProduct::new([0, 1], [0, 2]).unwrap();
let fp = FermionProduct::new([0], [0]).unwrap();

// Adding the c^{\dagger}_0 c^{\dagger}_1 c_0 c_2 term to the system part of the open system
let operator = open_system.system_mut();
operator.add_operator_product(hfp, CalculatorComplex::new(2.0, 0.0)).unwrap();

// Adding the c^{\dagger}_0 c_0 part to the noise part of the open system
let noise = open_system.noise_mut();
noise
    .add_operator_product(
        (fp.clone(), fp), CalculatorComplex::new(1.0, 0.0)
    ).unwrap();

println!("{}", open_system);

The equivalent code in python:

from qoqo_calculator_pyo3 import CalculatorComplex
from struqture_py import fermions

open_system = fermions.FermionLindbladOpenSystem()

hfp = fermions.HermitianFermionProduct([0, 1], [0, 2])
fp = fermions.FermionProduct([0], [0])

# Adding the c_0^dag c_1^dag c_0 c_2 term to the system part of the open system
open_system.system_add_operator_product(hfp, CalculatorComplex.from_pair(2.0, 0.0))
# Adding the c_0^dag c_0 part to the noise part of the open system
open_system.noise_add_operator_product(
    (fp, fp), CalculatorComplex.from_pair(0.0, 1.0))

print(open_system)