diff --git a/README.md b/README.md
index 8f0abad24..50d27c79b 100644
--- a/README.md
+++ b/README.md
@@ -21,7 +21,7 @@ Unfortunately, this means that we will probably never cover every algorithm ever
 That said, we'll still cover a few algorithms for fun that have very little, if any practical purpose.
 
 If you would like to contribute, feel free to go to any chapter with code associated with it and implement that algorithm in your favorite language,
-and then submit the code via pull request, following the submission guidelines found in `chapters/how_to_contribute.md` (or [here](chapters/introduction/how_to_contribute.md) if you are reading this on gitbook).
+and then submit the code via pull request, following the submission guidelines found in `contents/how_to_contribute/how_to_contribute.md` (or [here](contents/how_to_contribute/how_to_contribute.md) if you are reading this on gitbook).
 
 Hopefully, this project will grow and allow individuals to learn about and try their hand at implementing different algorithms for fun and (potentially) useful projects.
 If nothing else, it will be an enjoyable adventure for our community.
diff --git a/SUMMARY.md b/SUMMARY.md
index a498a9838..569142807 100644
--- a/SUMMARY.md
+++ b/SUMMARY.md
@@ -1,38 +1,38 @@
 # Summary
 
 * [Algorithm Archive](README.md)
-* [Introduction](chapters/introduction/introduction.md)
-* [How To Contribute](chapters/introduction/how_to_contribute.md)
-* [Version Control](chapters/introduction/version_control.md)
-* [Data Structures](chapters/data_structures/data_structures.md)
-    * [Stacks and Queues](chapters/data_structures/stacks_and_queues/stacks_and_queues.md)
-* [Mathematical Background](chapters/general/mathematical_background/mathematical_background.md)
-    * [Complexity Notation](chapters/general/notation/notation.md)
-    * [Bit Logic](chapters/general/bitlogic/bitlogic.md)
-    * [Convolutions](chapters/algorithms/convolutions/convolutions.md)
-    * [Taylor Series](chapters/general/taylor_series_expansion/taylor_series_expansion.md)
-* [Sorting and Searching](chapters/general/sorting_and_searching/sorting_and_searching.md)
-    * [Bubble Sort](chapters/algorithms/bubble_sort/bubble_sort.md)
-    * [Bogo Sort](chapters/algorithms/bogo_sort/bogo_sort.md)
-* [Tree Traversal](chapters/algorithms/tree_traversal/tree_traversal.md)
-* [Euclidean Algorithm](chapters/algorithms/euclidean_algorithm/euclidean_algorithm.md)
-* [Monte Carlo](chapters/algorithms/monte_carlo_integration/monte_carlo_integration.md)
-* [Matrix Methods](chapters/general/matrix_methods/matrix_methods.md)
-    * [Gaussian Elimination](chapters/algorithms/gaussian_elimination/gaussian_elimination.md)
-    * [Thomas Algorithm](chapters/algorithms/thomas_algorithm/thomas_algorithm.md)
-* [Computational Geometry](chapters/general/computational_geometry/computational_geometry.md)
-    * [Gift Wrapping](chapters/general/gift_wrapping/gift_wrapping.md)
-        * [Jarvis March](chapters/algorithms/jarvis_march/jarvis_march.md)
-        * [Graham Scan](chapters/algorithms/graham_scan/graham_scan.md)
-* [FFT](chapters/algorithms/cooley_tukey/cooley_tukey.md)
-* [Decision Problems](chapters/general/decision_problems/decision_problems.md)
-    * [Stable Marriage Problem](chapters/algorithms/stable_marriage_problem/stable_marriage_problem.md)
-* [Differential Equation Solvers](chapters/general/differential_equations/differential_equations.md)
-    * [Forward Euler Method](chapters/algorithms/forward_euler_method/forward_euler_method.md)
-* [Physics Solvers](chapters/general/physics_solvers/physics_solvers.md)
-    * [Verlet Integration](chapters/algorithms/verlet_integration/verlet_integration.md)
-    * [Quantum Systems](chapters/general/quantum_systems/quantum_systems.md)
-        * [Split-Operator Method](chapters/algorithms/split-operator_method/split-operator_method.md)
-* [Data Compression](chapters/general/data_compression/data_compression.md)
-    * [Huffman Encoding](chapters/algorithms/huffman_encoding/huffman_encoding.md)
-* [Quantum Information](chapters/general/quantum_information/quantum_information.md)
+* [Introduction](contents/introduction/introduction.md)
+* [How To Contribute](contents/how_to_contribute/how_to_contribute.md)
+* [Version Control](contents/git_and_version_control/git_and_version_control.md)
+* [Data Structures](contents/data_structures/data_structures.md)
+    * [Stacks and Queues](contents/stacks_and_queues/stacks_and_queues.md)
+* [Mathematical Background](contents/mathematical_background/mathematical_background.md)
+    * [Complexity Notation](contents/notation/notation.md)
+    * [Bit Logic](contents/bitlogic/bitlogic.md)
+    * [Convolutions](contents/convolutions/convolutions.md)
+    * [Taylor Series](contents/taylor_series_expansion/taylor_series_expansion.md)
+* [Sorting and Searching](contents/sorting_and_searching/sorting_and_searching.md)
+    * [Bubble Sort](contents/bubble_sort/bubble_sort.md)
+    * [Bogo Sort](contents/bogo_sort/bogo_sort.md)
+* [Tree Traversal](contents/tree_traversal/tree_traversal.md)
+* [Euclidean Algorithm](contents/euclidean_algorithm/euclidean_algorithm.md)
+* [Monte Carlo](contents/monte_carlo_integration/monte_carlo_integration.md)
+* [Matrix Methods](contents/matrix_methods/matrix_methods.md)
+    * [Gaussian Elimination](contents/gaussian_elimination/gaussian_elimination.md)
+    * [Thomas Algorithm](contents/thomas_algorithm/thomas_algorithm.md)
+* [Computational Geometry](contents/computational_geometry/computational_geometry.md)
+    * [Gift Wrapping](contents/gift_wrapping/gift_wrapping.md)
+        * [Jarvis March](contents/jarvis_march/jarvis_march.md)
+        * [Graham Scan](contents/graham_scan/graham_scan.md)
+* [FFT](contents/cooley_tukey/cooley_tukey.md)
+* [Decision Problems](contents/decision_problems/decision_problems.md)
+    * [Stable Marriage Problem](contents/stable_marriage_problem/stable_marriage_problem.md)
+* [Differential Equation Solvers](contents/differential_equations/differential_equations.md)
+    * [Forward Euler Method](contents/forward_euler_method/forward_euler_method.md)
+* [Physics Solvers](contents/physics_solvers/physics_solvers.md)
+    * [Verlet Integration](contents/verlet_integration/verlet_integration.md)
+    * [Quantum Systems](contents/quantum_systems/quantum_systems.md)
+        * [Split-Operator Method](contents/split-operator_method/split-operator_method.md)
+* [Data Compression](contents/data_compression/data_compression.md)
+    * [Huffman Encoding](contents/huffman_encoding/huffman_encoding.md)
+* [Quantum Information](contents/quantum_information/quantum_information.md)
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+++ b/contents/choosing_a_language/choosing_a_language.md
@@ -1,4 +1,4 @@
-## Choosing a Language
+# Choosing a Language
 
 I'm not going to beat around the bush here.
 Every single time I try something new, I fail at it.
diff --git a/chapters/languages/compiled/compiled.md b/contents/compiled_languages/compiled_languages.md
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-## Compiled Languages
+# Compiled Languages
 
 Programming is hard because we need to write instructions for our computer.
 The computer then reads this set of instructions and executes them accordingly.
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diff --git a/chapters/general/data_compression/data_compression.md b/contents/data_compression/data_compression.md
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index b666fa21a..709d43748 100644
--- a/chapters/general/data_compression/data_compression.md
+++ b/contents/data_compression/data_compression.md
@@ -6,7 +6,7 @@ It would naively seem that better hardware means that there are less restriction
 
 That said, there will always be new devices on the market that require minimizing data storage.
 In fact, some of the most revolutionary algorithms and methods in existence today fall in the category of data compression.
-From lossless data compression with [Huffman encoding](../../algorithms/huffman_encoding/huffman_encoding.md) to genetic compression algorithms and machine learning, there is a lot to learn about this field, and we'll go through it piece-by-piece.
+From lossless data compression with [Huffman encoding](../huffman_encoding/huffman_encoding.md) to genetic compression algorithms and machine learning, there is a lot to learn about this field, and we'll go through it piece-by-piece.
 
 All that said, no discussion about data compression is complete without first discussing the information, itself -- specifically how information is represented in computer systems.
 Now, we've discussed this in some depth before with [bitlogic](../../principles_of_code/building_blocks/bitlogic.md), but there is much more to the story than what we let on before.
@@ -119,7 +119,7 @@ L_2 &= 0.1\times 3 + 0.2 \times 3 + 0.3 \times 2 + 0.4 \times 1 = 1.9
 $$
 
 Here, it's clear that $$L_2 < L_1$$, and thus the second set of codewords compresses our data more than the first.
-This measure can be used as a direct test of certain simple data compression techniques, notably those created by Shannon, Fano, and [Huffman](../../algorithms/huffman_encoding/huffman_encoding.md), which will be covered soon!
+This measure can be used as a direct test of certain simple data compression techniques, notably those created by Shannon, Fano, and [Huffman](../huffman_encoding/huffman_encoding.md), which will be covered soon!
 
 
 <script>
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diff --git a/chapters/languages/compiled/FORTRAN.md b/contents/fortran/fortran.md
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index d41677620..02deebc15 100644
--- a/chapters/languages/compiled/FORTRAN.md
+++ b/contents/fortran/fortran.md
@@ -1,3 +1,3 @@
-### FORTRAN
+# FORTRAN
 
 Alright, so here's the thing about Fortran. It's old.
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diff --git a/chapters/algorithms/forward_euler_method/forward_euler_method.md b/contents/forward_euler_method/forward_euler_method.md
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index cf368e849..fd2fbadd3 100644
--- a/chapters/algorithms/forward_euler_method/forward_euler_method.md
+++ b/contents/forward_euler_method/forward_euler_method.md
@@ -4,7 +4,7 @@ The Euler methods are some of the simplest methods to solve ordinary differentia
 They introduce a new set of methods called the Runge Kutta methods, which will be discussed in the near future!
 
 As a physicist, I tend to understand things through methods that I have learned before.
-In this case, it makes sense for me to see Euler methods as extensions of the [Taylor Series Expansion](../general/taylor_series_expansion/taylor_series_expansion.md).
+In this case, it makes sense for me to see Euler methods as extensions of the [Taylor Series Expansion](../taylor_series_expansion/taylor_series_expansion.md).
 These expansions basically approximate functions based on their derivatives, like so:
 
 $$
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diff --git a/chapters/algorithms/graham_scan/graham_scan.md b/contents/graham_scan/graham_scan.md
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diff --git a/chapters/introduction/how_to_contribute.md b/contents/how_to_contribute/how_to_contribute.md
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rename from chapters/introduction/how_to_contribute.md
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index 8847ae01a..a9c433fa2 100644
--- a/chapters/introduction/how_to_contribute.md
+++ b/contents/how_to_contribute/how_to_contribute.md
@@ -2,7 +2,7 @@
 
 The *Algorithm Archive* is an effort to learn about and teach algorithms as a community.
 As such, it requires a certain level of trust between community members.
-For the most part, the collaboration can be done via GitHub and gitbook, so it is important to understand the basics of [version control](version_control.md).
+For the most part, the collaboration can be done via GitHub and gitbook, so it is important to understand the basics of [version control](../git_and_version_control/git_and_version_control.md).
 Ideally, all code provided by the community will be submitted via pull requests and discussed accordingly; however, I understand that many individuals are new to collaborative projects, so I will allow submissions by other means (comments, tweets, etc...).
 As this project grows in size, it will be harder and harder to facilitate these submissions.
 In addition, by submitting in any way other than pull requests, I cannot guarantee I will be able to list you as a collaborator (though I will certainly do my best to update the `CONTRIBUTORS.md` file accordingly).
@@ -23,7 +23,7 @@ We use two gitbook plugins to allow users to flip between languages on different
 One is the theme-api, and the other is the include-codeblock api.
 We need the following statements in the markdown file for these to work together:
 
-[import](codeblock.txt)
+[import](res/codeblock.txt)
 
 For this example, we are starting the theme-api `method` and importing lines 1-17 from a sample Julia snippet from the code directory.
 Note that to standardize the language capitalization schemes, we ask that each language's `sample lang` is the file extension for their code, `cpp` for C++, `hs` for Haskell, etc...
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index 416fc26ac..2ce131261 100644
--- a/chapters/algorithms/huffman_encoding/huffman_encoding.md
+++ b/contents/huffman_encoding/huffman_encoding.md
@@ -8,7 +8,7 @@ He managed to rip the heart out of the methods described by leaders of the field
 It was in that moment, I knew I would never amount to anything.
 I have since accepted that fact and moved on.
 
-Huffman encoding follows from the problem described in the [Data Compression](../../general/data_compression/data_compression.md) section.
+Huffman encoding follows from the problem described in the [Data Compression](../data_compression/data_compression.md) section.
 We have a string that we want to encode into bits.
 Huffman encoding ensures that our encoded bitstring is as small as possible without losing any information.
 Because it is both lossless and guarantees the smallest possible bit length, it outright replaces both Shannon and Shannon-Fano encoding in most cases, which is a little weird because the method was devised while Huffman was taking a course from Fano, himself!
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+++ b/contents/quantum_systems/quantum_systems.md
@@ -65,7 +65,7 @@ p = \frac{h}{\lambda}
 $$
 
 where $$h$$ is Planck's constant and $$\lambda$$ is the wavelength.
-This means that we can ultimately move between real and momentum space by using [Fourier Transforms](../../algorithms/cooley_tukey/cooley_tukey.md), which is incredibly useful in a number of cases!
+This means that we can ultimately move between real and momentum space by using [Fourier Transforms](../cooley_tukey/cooley_tukey.md), which is incredibly useful in a number of cases!
 
 Unfortunately, the interpretation of quantum simulation is rather tricky and is ultimately easier to understand with slightly different notation.
 This notation is called _braket_ notation, where a _ket_ looks like this:
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@@ -6,7 +6,7 @@ $$
 i \hbar \frac{\partial \Psi(\mathbf{r},t)}{\partial t} = \left[-\frac{\hbar^2}{2m}\nabla^2 + g|\Psi(\mathbf{r},t)|^2 \right] \Psi(\mathbf{r},t),
 $$
 
-which follows from the notation provided in the [quantum systems](../../general/quantum_systems/quantum_systems.md) chapter: $$\Psi(\mathbf{r},t)$$ is a quantum wave-function with spatial ($$\mathbf{r}$$) and time ($$t$$) dependence and $$\nabla^2$$ is a laplacian; however, in this case, we also add an interaction tern $$g$$ next to a nonlinear $$|\Psi(\mathbf{r},t)|^2$$ term.
+which follows from the notation provided in the [quantum systems](../quantum_systems/quantum_systems.md) chapter: $$\Psi(\mathbf{r},t)$$ is a quantum wave-function with spatial ($$\mathbf{r}$$) and time ($$t$$) dependence and $$\nabla^2$$ is a laplacian; however, in this case, we also add an interaction tern $$g$$ next to a nonlinear $$|\Psi(\mathbf{r},t)|^2$$ term.
 By adding in the $$V(\mathbf{r})$$ term, we get an equation used to study superfluid Bose--Einstein Condensate (BEC) systems:
 
 $$
@@ -17,7 +17,7 @@ This is the system I studied for most of my PhD (granted, we played a few tricks
 
 At it's heart, the split-op method is nothing more than a pseudo-spectral differential equation solver... That is to say, it solves the Schrodinger equation with [FFT's](../cooley_tukey/cooley_tukey.md).
 In fact, there is a large class of spectral and pseudo-spectral methods used to solve a number of different physical systems, and we'll definitely be covering those in the future.
-As mentioned in the [quantum systems](../../general/quantum_systems/quantum_systems.md) section, we can represent a a quantum wavefunction in momentum space, which is parameterized with the wavevector $$k$$.
+As mentioned in the [quantum systems](../quantum_systems/quantum_systems.md) section, we can represent a a quantum wavefunction in momentum space, which is parameterized with the wavevector $$k$$.
 In the hamiltonian shown above, we can split our system into real-space components, $$\hat{H}_R = \left[V(\mathbf{r}) + g|\Psi(\mathbf{r},t)|^2 \right] \Psi(\mathbf{r},t)$$, and momentum space components, $$\hat{H}_M = \left[-\frac{\hbar^2}{2m}\nabla^2 \right]\Psi(\mathbf{r},t)$$.
 If we assume a somewhat general solution to our quantum system:
 
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@@ -1,4 +1,4 @@
-### Stacks and Queues
+# Stacks and Queues
 
 Stacks and Queues are two sides of the same coin in computer science. They are both simple data structures that hold multiple elements, but allow you to use a single element at a time. The biggest difference between the two structures is the order in which you can access the elements in the data structure.
 
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