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adding simons algorithm tutorial #327

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25 changes: 25 additions & 0 deletions tutorials/ExploringSimonsAlgorithm/ExploringSimonsAlgorithm.csproj
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{
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"metadata": {},
"source": [
"# Exploring Simon's Periodicity Algorithm: Classical Component\n",
"\n",
"This is a companion notebook to the [Exploring Simon's Periodicity Algorithm: Quantum Component](./ExploringSimonsAlgorithmQuantumPart.ipynb) tutorial. It will teach you about the classical post-processing component of Simon's Algorithm."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Classical Post-Processing for Simon's Algorithm\n",
"\n",
"The quantum circuit we ran at the end of the companion tutorial output the binary string $\\mathbf{j}$ with length $n$, where $\\mathbf{j} \\in\\ \\{0, 1\\}^n$ and satisfies $\\mathbf{s} \\cdot\\ \\mathbf{j} = 0$. Is this enough information to solve for $\\mathbf{s}$?\n",
"\n",
"The answer is yes, but with caveats. We need to run the quantum circuit $n - 1$ times to produce $n - 1$ binary strings $\\mathbf{j_{1}}, ... , \\mathbf{j_{n-1}}$ such that\n",
"\n",
"$$\\mathbf{j_{1}} \\cdot\\ \\mathbf{s} = 0$$\n",
"$$\\mathbf{j_{2}} \\cdot\\ \\mathbf{s} = 0$$\n",
"$$.$$\n",
"$$.$$\n",
"$$.$$\n",
"$$\\mathbf{j_{n-1}} \\cdot\\ \\mathbf{s} = 0$$\n",
"\n",
"However, we still have a non-trivial chance of failure. To arrive at a solution, $\\mathbf{j_{1}}, ... , \\mathbf{j_{n-1}}$ must be linearly independent and we must also be lucky.\n",
"\n",
"If we have linear independence, we can solve the under-determined system of $n-1$ equations and $n$ unknowns to get a candidate solution $\\mathbf{s'}$. We can then test this candidate solution, and if we find that $f(0^n) = f(\\mathbf{s'})$, we know that $\\mathbf{s} = \\mathbf{s'}$. The problem is solved!\n",
"\n",
"A standard way to solve this system employs [Gaussian elimination with back substitution](http://mathonline.wikidot.com/gaussian-elimination-and-back-substitution). Links to resources are provided if you need a refresher on concepts like [Gaussian elimination](https://en.wikipedia.org/wiki/Gaussian_elimination). Let's practice writing functions in Python to help us achieve our goal!\n",
"\n",
"> **Note:** The [linear algebra tutorial](https://github.com/microsoft/QuantumKatas/blob/master/tutorials/LinearAlgebra/LinearAlgebra.ipynb) notebook contains example implementations of some linear algebra functions in Python.\n",
"\n",
"Let's start by setting up a few things necessary for testing the exercises. **Do not skip this step.**\n",
"\n",
"Click the cell with code below this block of text and press `Ctrl+Enter` (`shift+return` on Mac)."
]
},
{
"cell_type": "code",
"execution_count": 1,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Success!\n"
]
}
],
"source": [
"# Run this cell using Ctrl+Enter (shift+return on Mac).\n",
"from tests import exercise\n",
"from typing import List\n",
"\n",
"Matrix = List[List[float]]"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Recall that the goal of Gaussian elimination is to transform a matrix to [row echelon form](https://en.wikipedia.org/wiki/Row_echelon_form); i.e. into an [upper triangular matrix](https://en.wikipedia.org/wiki/Triangular_matrix). To achieve this form, there are three types of elementary row operations we can perform:\n",
"* Swapping two rows,\n",
"* Multiplying a row by a nonzero number, and\n",
"* Adding a multiple of one row to another row.\n",
"\n",
"Let's try using these operations to transform a matrix to row echelon form in Python.\n",
"\n",
"## Exercise 3. Row echelon form of a matrix\n",
"\n",
"**Input:**\n",
"\n",
"* A matrix $\\mathbf{J}$ of dimensions $n-1$ x $n$\n",
"\n",
"**Output:**\n",
"\n",
"* [Upper triangular form](https://en.wikipedia.org/wiki/Triangular_matrix) of the matrix $\\mathbf{J}$\n",
"\n",
"**Example:**\n",
"\n",
"$\\begin{bmatrix} 0 & 1 & 1 \\\\ 1 & 1 & 1 \\end{bmatrix}$ should be transformed to $\\begin{bmatrix} 1 & 1 & 1 \\\\ 0 & 1 & 1 \\end{bmatrix}$\n",
"\n",
"> **Note:** Beware of [singular matrices](https://en.wikipedia.org/wiki/Singular_matrix)"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"@exercise\n",
"def row_echelon_form(J : Matrix) -> Matrix: \n",
" # ...\n",
" \n",
" return ..."
]
},
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"cell_type": "markdown",
"metadata": {},
"source": [
"The final step in Gaussian elimination is to solve the system using [back substitution](https://algowiki-project.org/en/Backward_substitution).\n",
"\n",
"The matrix $\\begin{bmatrix} 1 & 1 & 1 \\\\ 0 & 1 & 1 \\end{bmatrix}$ can be represented as the system of equations\n",
"\n",
"$$x_0 + x_1 = 1$$\n",
"$$ x_1 = 1$$\n",
"\n",
"Substituting $x_1 = 1$ into the first equation yields the result $x_0 = 0$ and our system is solved. We can return $[x_0, x_1] = [0, 1]$.\n",
"\n",
"Next, try implementing a Python function to perform back substitution.\n",
"\n",
"## Exercise 4. Back substitution\n",
"\n",
"**Input:**\n",
"\n",
"* A matrix $\\mathbf{J}$ in row echelon form that contains a unique solution\n",
"\n",
"**Output:**\n",
"\n",
"* The unique solution as a list $[x_0, ..., x_n]$"
]
},
{
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"source": [
"@exercise\n",
"def back_substitution(J : Matrix) -> List: \n",
" # ...\n",
" \n",
" return ..."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"We learned earlier that the output of our quantum circuit is some $\\mathbf{j}$ that satisfied the property $\\mathbf{s} \\cdot\\ \\mathbf{j} = 0$. This property is more accurately described as $\\mathbf{s} \\cdot\\ \\mathbf{j} = 0$ modulo $2$.\n",
"\n",
"Now let's implement a Python function to compute the [dot product](https://en.wikipedia.org/wiki/Dot_product) mod 2.\n",
"\n",
"## Exercise 5: Dot product modulo 2\n",
"\n",
"**Inputs:**\n",
"\n",
"1. A vector $\\mathbf{a} = [a_0, ... , a_n]$\n",
"2. A vector $\\mathbf{b} = [b_0, ... , b_n]$\n",
"\n",
"**Output:**\n",
"\n",
"The scalar value that represents the dot product of $\\mathbf{a}$ and $\\mathbf{b}$ mod $2$\n",
"\n",
"**Examples:**\n",
"\n",
"* If $\\mathbf{a} = [1, 0, 0, 1]$ and $\\mathbf{b} = [1, 0, 1, 0]$, the function should output $1$\n",
"* If $\\mathbf{a} = [1, 1, 1]$ and $\\mathbf{b} = [0, 1, 1]$, the function should output $0$\n",
"\n",
"> **Hint:** This function should only output 0 or 1"
]
},
{
"cell_type": "code",
"execution_count": null,
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"source": [
"@exercise\n",
"def dot_product(a : Matrix, b : Matrix) -> float:\n",
" # ...\n",
" \n",
" return ..."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"At this stage you have learned the tools necessary for the classical post-processing part of Simon's algorithm. This concludes the discussion of Simon's peridocity algorithm.\n",
"\n",
"# What's next?\n",
"\n",
"We hope you've enjoyed this tutorial and learned a lot from it! If you're looking to learn more about quantum computing and Q#, here are some suggestions:\n",
"* The [Quantum Katas](https://github.com/microsoft/QuantumKatas/) are sets of programming exercises on quantum computing that can be solved using Q#. They cover a variety of topics, from the basics like the concepts of superposition and measurements to more interesting algorithms like Grover's search.\n",
"* In particular, [SimonsAlgorithm quantum kata](https://github.com/microsoft/QuantumKatas/tree/master/SimonsAlgorithm) offers more exercises on quantum oracles and a different presentation of Simon's algorithm."
]
}
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