Metadata-Version: 2.1
Name: feynman-path
Version: 0.1.0
Summary: Visualization tool for the Feynman Path Integral applied to quantum circuits
Home-page: https://github.com/cduck/feynman_path
Author: Casey Duckering
License: UNKNOWN
Download-URL: https://github.com/cduck/feynman_path/archive/0.1.0.tar.gz
Keywords: quantum computing,feynman path,path integral,jupyter
Platform: UNKNOWN
Classifier: License :: OSI Approved :: MIT License
Classifier: Development Status :: 3 - Alpha
Classifier: Programming Language :: Python :: 3
Classifier: Programming Language :: Python :: 3.7
Classifier: Programming Language :: Python :: 3.8
Classifier: Framework :: IPython
Classifier: Framework :: Jupyter
Description-Content-Type: text/markdown
Requires-Dist: drawSvg (~=1.8)
Requires-Dist: latextools (~=0.4)
Requires-Dist: sympy (~=1.7)

# Feynman Path Integral Diagram for Quantum Circuits

A visualization tool for the Feynman Path Integral applied to quantum circuits.
The [path integral formulation](https://en.wikipedia.org/wiki/Path_integral_formulation) is an interpretation of quantum mechanics that can aid in understanding superposition and interference.

Path integral:

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/no-entanglement.png" width="991.5" />

Circuit diagram:

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/no-entanglement-circuit.png" width="388" />

How to read a path integral diagram:
- Time flows from left to right as gates are executed on qubits.
- Arrows transition from one state to another and traversing the arrows gives a path to an output.
- Two diverging arrows indicate a split into two potential outcomes.
- An orange arrow indicates a negative sign is added to that outcome.
- When two arrows converge, the amplitudes are summed.
- Quantum interference is when positive and negative amplitudes cancel in this sum.
- The rightmost column lists the possible measurement outcomes along with the final probability amplitudes of measuring each outcome.

See also: [Bloch sphere visualization](https://github.com/cduck/bloch_sphere)

# Install

feynman\_path is available on PyPI:

```bash
python3 -m pip install feynman_path
```

## Prerequisites

Several non-python tools are used to generate the graphics and various output formats.
These non-python dependencies are listed below and platform-specific installation instructions can be found [here](https://github.com/cduck/latextools/#prerequisites).

- LaTeX: A distribution of LaTeX that provides the `pdflatex` command needs to be installed separately.
- [Inkscape](https://inkscape.org/): Used to convert the LaTeX expressions into SVG elements and output the PDF format.
- [Cairo](https://www.cairographics.org/download/) (optional): Only required for the PNG output format.

### Ubuntu

```bash
sudo apt install texlive inkscape libcairo2  # Or texlive-latex-recommended, or texlive-latex-extra
```

### macOS

Using [homebrew](https://brew.sh/):

```bash
brew install --cask mactex inkscape
brew install cairo
```


# Usage

This package provides a command line tool to generate diagrams.

### Examples
```bash
feynman_path interference 2 h0 cnot0,1 z1 h0 h1 cnot1,0 h1
```
<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/interference.png" width="1355" />

```bash
feynman_path interference 2 h0 cnot0,1 z1 h0 h1 cnot1,0 h1 --circuit
```
<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/interference-circuit.png" width="488" />

### Command line options
```
$ feynman_path -h
usage: feynman_path [-h] [--svg] [--png] [--pdf] [--sequence] [--circuit]
                    [--scale SCALE] [--verbose]
                    name n_qubits gate [gate ...]

Renders a Feynman path integral diagram for a sequence of quantum gates.

positional arguments:
  name           The file name to save (excluding file extension)
  n_qubits       The number of qubits in the quantum circuit
  gate           List of gates to apply (e.g. h0 z1 cnot0,1)

optional arguments:
  -h, --help     show this help message and exit
  --svg          Save diagram as an SVG image (default)
  --png          Save diagram as a PNG image
  --pdf          Save diagram as a PDF document
  --sequence     Save a sequence of images that build up the diagram from left
                 to right as <name>-nn.svg/png/pdf
  --circuit      Save a standard quantum circuit diagram named
                 <name>-circuit.svg/png/pdf instead of a Feynman path diagram
  --scale SCALE  Scales the resolution of the diagram when saved as a PNG
  --verbose      Print extra progress information
```

### Python Package
feynman\_path also provides a Python 3 package as an alternative to the command line tool.  Diagrams can be viewed directly in a Jupyter notebook or saved.

```python
import feynman_path

n_qubits = 3
font = 12
ws_label = 4+0.55*n_qubits  # Label width relative to font size
w_time = 60+ws_label*font  # Diagram column width
f = feynman_path.Diagram(
    n_qubits, font=font, ws_label=ws_label, w_time=w_time)

f.perform_h(0)
f.perform_cnot(0, 1)
f.perform_z(1)
f.perform_cnot(1, 2, pre_latex=r'\color{red!80!black}')
f.perform_h(0)
f.perform_h(1)
f.perform_cnot(1, 0)

f.draw()  # Display in Jupyter
```
```python
f.draw().saveSvg('output.svg')  # Save SVG
f.draw().setPixelScale(2).savePng('output.png')  # Save PNG
import latextools
latextools.svg_to_pdf(f.draw()).save('output.pdf')  # Save PDF
```
<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/no-interference.png" width="1626" />

See [examples/render\_examples.py](https://github.com/cduck/feynman_path/blob/master/examples/render_examples.py) for more example code.

# Examples

### Using the CNOT gate to entangle qubits
The [CNOT gate](https://en.wikipedia.org/wiki/Controlled_NOT_gate) (⋅–⨁) can be used to entangle two qubits, creating a [Bell pair](https://en.wikipedia.org/wiki/Bell_state), but for certain input qubit states, the CNOT will have no effect.

**Create a Bell pair by using a CNOT on the |+0⟩ state (q0=|+⟩, q1=|0⟩):**

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/entanglement-circuit.png" width="337.5" />

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/entanglement.png" width="810" />

Note the output (rightmost) column is an entangled state: |00⟩+|11⟩

```bash
feynman_path no-entanglement 2 h0 cnot0,1 h0 h1
```

**Fail to create a bell pair by using a CNOT on the |++⟩ state (q0=|+⟩, q1=|+⟩):**

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/no-entanglement-circuit.png" width="388" />

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/no-entanglement.png" width="991.5" />

```bash
feynman_path no-entanglement 2 h0 h1 cnot0,1 h0 h1
```

Note the output (rightmost) column is a separable state: |00⟩

### Copying an intermediate qubit state onto an ancilla ruins interference
In classical computing, it is common to inspect intermediate steps of a computation.  This can be very useful for debugging.  In quantum computing however, this destroys the effect of interference.  We can use a [CNOT gate](https://en.wikipedia.org/wiki/Controlled_NOT_gate) (⋅–⨁) to copy an intermediate value onto another qubit to inspect later.  Shown below, copying the intermediate value of q1 to q2 changes the output of q0, q1.

**Original circuit that compute the output q0=1, q1=0:**

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/interference-circuit.png" width="488" />

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/interference.png" width="1355" />

```bash
feynman_path interference 2 h0 cnot0,1 z1 h0 h1 cnot1,0 h1
```

**The addition of CNOT1,2 to inspect the intermediate value of q1 changes the output of q0:**

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/no-interference-circuit.png" width="538" />

<img src="https://raw.githubusercontent.com/cduck/feynman_path/master/examples/no-interference.png" width="1626" />

Note how the path diagram is the same except the arrows at H1 are now split into the upper and lower halves of the diagram and don't interfere anymore.

```bash
feynman_path no-interference 3 h0 cnot0,1 z1 cnot1,2 h0 h1 cnot1,0 h1
```


