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Show that for any \(\alpha, \beta \in \mathbb{R}\) and any \(\mathbf{H} \in \operatorname{End}(\mathcal{V})\), we have $$ e^{\alpha \mathbf{H}} e^{\beta \mathbf{H}}=e^{(\alpha+\beta) \mathbf{H}} . $$

Short Answer

Expert verified
In conclusion, it's shown that for any \(\alpha, \beta \in \mathbb{R}\) and any \(\mathbf{H} \in \operatorname{End}(\mathcal{V})\), the expression \(e^{\alpha \mathbf{H}} e^{\beta \mathbf{H}}=e^{(\alpha+\beta) \mathbf{H}}\) indeed holds true.

Step by step solution

01

- Indicate the matrices

Let's begin by representing \(e^{\alpha H}\) and \(e^{\beta H}\) as infinite series. We have \(e^{\alpha H} = I + \alpha H + \frac{\alpha^2 H^2}{2!} + \frac{\alpha^3 H^3}{3!} + ... \) and \(e^{\beta H} = I + \beta H + \frac{\beta^2 H^2}{2!} + \frac{\beta^3 H^3}{3!} + ... \), where \(H\) is the matrix. Note that \(H\) is a linear transformation from a vector space to itself, and thus, the matrices commute.
02

- Compute the multiplication

Let's multiply \(e^{\alpha H}\) and \(e^{\beta H}\). Note that as the matrices commute (i.e \(H^i H^j = H^j H^i\)), each term in \(e^{\alpha H}\) can be expanded and rearranged to get a term in \(e^{(\alpha+ \beta) H}\). For instance, \(\frac{\alpha^2 H^2}{2!}\cdot\frac{\beta^3 H^3}{3!} = \frac{\alpha^2 \beta^3 H^5}{2!3!}\), which can be rearranged to be a term in the expansion of \(e^{(\alpha+ \beta) H}\).
03

- Applying Binomial theorem

We know that \((\alpha + \beta )^n = \sum_{i=0}^{n}{n \choose i} \alpha^i \beta^{(n-i)}\). Thus when we rearrange each term in \(e^{\alpha H} \cdot e^{\beta H}\), we get terms in \(e^{(\alpha+ \beta) H}\), which represent all the possible combinations of \(\alpha\) and \(\beta\) powers, as per the binomial theorem. We can extend this argument to all terms and thus conclude that \(e^{\alpha H}\cdot e^{\beta H}= e^{(\alpha+ \beta) H}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Linear Transformations
Linear transformations play a pivotal role in understanding matrix exponentiation. They are mappings from a vector space to itself that preserve vector addition and scalar multiplication. If you have a matrix, let's call it \( \mathbf{H} \), it can be seen as a linear transformation because when it acts on a vector, it provides a new vector in the same space.

One key aspect of linear transformations is that they can be represented using matrices. This matrix representation helps us perform operations like exponentiation in a systematic way.
For example, if you apply the transformation twice, it is equivalent to multiplying the matrix \( \mathbf{H} \) by itself, denoted as \( \mathbf{H}^2 \).
  • Linear transformations respect the operations of addition and scalar multiplication.
  • They map vectors in a vector space back into the same space.
Understanding these transformations is crucial, especially when dealing with expressions like \( e^\alpha \mathbf{H} \) as seen in matrix exponentiation.
Commutative Matrices
Commutative matrices are pairs of matrices that can be multiplied in any order with the same result. This property is essential for solving the exercise about the equality \( e^{\alpha \mathbf{H}} e^{\beta \mathbf{H}} = e^{(\alpha+\beta) \mathbf{H}} \).

Typically, matrices do not commute; \( \mathbf{A} \mathbf{B} eq \mathbf{B} \mathbf{A} \) in general. However, when dealing with the same matrix \( \mathbf{H} \,\), multiplied to different powers as in the given exercise, they do commute. This means:
  • \( \mathbf{H}^i \mathbf{H}^j = \mathbf{H}^j \mathbf{H}^i \)
This property simplifies the calculation significantly since you can reorder terms freely during multiplication. For example, when expanding \( e^{\alpha \mathbf{H}} \cdot e^{\beta \mathbf{H}} \), the commutativity ensures that all combinations of terms match with those in \( e^{(\alpha + \beta) \mathbf{H}} \).
Binomial Theorem
The binomial theorem is a crucial tool that helps simplify expressions involving powers, crucial for understanding how the matrices in the original exercise relate to one another. The theorem states that:

\[(\alpha + \beta)^n = \sum_{i=0}^{n} {n \choose i} \alpha^i \beta^{n-i}\]

In the context of matrix exponentiation, it allows us to systematically expand and rearrange the series into smaller, more manageable parts. When matrices commute, as with \( \mathbf{H} \) in our exercise, this theorem helps express the product \( e^{\alpha \mathbf{H}} \cdot e^{\beta \mathbf{H}} \) as \( e^{(\alpha + \beta) \mathbf{H}} \).

The theorem provides a framework to multiply terms by reorganizing the added powers of \( \alpha \) and \( \beta \) and fitting them into the exponential form needed.
Vector Spaces
Vector spaces provide the foundational structure on which linear transformations, like those discussed in matrix exponentiation, operate. A vector space is a collection of vectors that can be added together and multiplied by scalars while staying within the same space.

The concepts of linear transformations and commutative matrices are inherently tied to the properties of vector spaces. These spaces are equipped with two operations: vector addition and scalar multiplication. They serve as the domain and range for linear transformations represented by matrices.
  • Vectors in a vector space have both magnitude and direction.
  • They can be subject to linear transformations.
  • Operations within this space obey specific algebraic rules.
Understanding vector spaces helps in appreciating why we can represent transformations with matrices and why these matrices can behave differently under certain conditions.

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Most popular questions from this chapter

Show that \((\mathbf{U}+\mathbf{T})(\mathbf{U}-\mathbf{T})=\mathbf{U}^{2}-\mathbf{T}^{2}\) if and only if \([\mathbf{U}, \mathbf{T}]=\mathbf{0} .\)

Prove that if \(\mathbf{A}\) and \(\mathbf{B}\) are hermitian, then \(i[\mathbf{A}, \mathbf{B}]\) is also hermitian.

Let \(|f\rangle,|g\rangle \in \mathbb{C}(a, b)\) with the additional property that $$ f(a)=g(a)=f(b)=g(b)=0 . $$ Show that for such functions, the derivative operator \(\mathbf{D}\) is anti- hermitian. The inner product is defined as usual: $$ \langle f \mid g\rangle \equiv \int_{a}^{b} f^{*}(t) g(t) d t . $$

For the vector $$ |a\rangle=\frac{1}{\sqrt{2}}\left(\begin{array}{c} 0 \\ 1 \\ -1 \\ 0 \end{array}\right) $$ (a) find the associated projection matrix, \(\mathbf{P}_{a}\). (b) Verify that \(\mathbf{P}_{a}\) does project an arbitrary vector in \(\mathbb{C}^{4}\) along \(|a\rangle .\) (c) Verify directly that the matrix \(1-\mathbf{P}_{a}\) is also a projection operator.

Let \(\left|a_{1}\right\rangle \equiv \mathbf{a}_{1}=(1,1,-1)\) and \(\left|a_{2}\right\rangle \equiv \mathbf{a}_{2}=(-2,1,-1)\). (a) Construct (in the form of a matrix) the projection operators \(\mathbf{P}_{1}\) and \(\mathbf{P}_{2}\) that project onto the directions of \(\left|a_{1}\right\rangle\) and \(\left|a_{2}\right\rangle\), respectively. Verify that they are indeed projection operators. (b) Construct (in the form of a matrix) the operator \(\mathbf{P}=\mathbf{P}_{1}+\mathbf{P}_{2}\) and verify directly that it is a projection operator. (c) Let \(\mathbf{P}\) act on an arbitrary vector \((x, y, z) .\) What is the dot product of the resulting vector with the vector \(\mathbf{a}_{1} \times \mathbf{a}_{2} ?\) What can you say about \(\mathbf{P}\) and your conclusion in (b)?

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