1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
// Copyright © 2021-2023 HQS Quantum Simulations GmbH. All Rights Reserved.
//
// Licensed under the Apache License, Version 2.0 (the "License"); you may not use this file except
// in compliance with the License. You may obtain a copy of the License at
//
// http://www.apache.org/licenses/LICENSE-2.0
//
// Unless required by applicable law or agreed to in writing, software distributed under the
// License is distributed on an "AS IS" BASIS, WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either
// express or implied. See the License for the specific language governing permissions and
// limitations under the License.
//! Mapping from bosonic operators to spin operators.
//!
//! This mapping was developped by Juha Leppäkangas at HQS Quantum Simulations. The paper detailing
//! the mapping, as well as its use in the context of open system dynamics, can be found at:
//! <https://arxiv.org/pdf/2210.12138>
//!
//! The mapping is given by:
//!
//! $ \hat{b}_i^{dagger} \hat{b}_i \rightarrow \sum_{j=1}^{N} \hat{\sigma}_+^{i,j} \hat{\sigma}_-^{i,j} $
//! $ \hat{b}_i^{dagger} + \hat{b}_i \rightarrow \frac{1}{\root{N}} \sum_{j=1}^{N} \hat{\sigma}_x^{i,j} $
//!
//! For a direct mapping, N is set to 1. For a Dicke mapping, N > 1.
use crateStruqtureError;