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10. Prove that the set of matrices of the form \[ \left(\begin{array}{lll}1 & x & y \\ 0 & 1 & z \\ 0 & 0 & 1\end{array}\right) \] is a group under matrix multiplication. This group, known as the Heisenberg group, is important in quantum physics. Matrix multiplication in the Heisenberg group is defined by \[ \left(\begin{array}{lll}1 & x & y \\ 0 & 1 & z \\ 0 & 0 & 1\end{array}\right)\left(\begin{array}{ccc}1 & x^{\prime} & y \\ 0 & 1 & z^{\prime} \\ 0 & 0 & 1\end{array}\right)=\left(\begin{array}{cc}1 & x+x^{\prime} \\ 0 & 1 \\ 0 & 0\end{array}\right) \]

Ask by Gray Hodges. in the United States
Mar 17,2025

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The set of matrices of the form \[ \begin{pmatrix} 1 & x & y \\ 0 & 1 & z \\ 0 & 0 & 1 \end{pmatrix} \] forms a group under matrix multiplication. This group, known as the Heisenberg group, satisfies the group axioms: closure, associativity, has an identity element, and every element has an inverse within the group.

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To show that the set of matrices of the form \[ \left(\begin{array}{lll}1 & x & y \\ 0 & 1 & z \\ 0 & 0 & 1\end{array}\right) \] is a group under matrix multiplication, we need to verify the group axioms: closure, associativity, identity, and inverses. First, consider closure: when you multiply two matrices of the given form, the resulting matrix is: \[ \left(\begin{array}{lll}1 & x & y \\ 0 & 1 & z \\ 0 & 0 & 1\end{array}\right)\left(\begin{array}{ccc}1 & x^{\prime} & y^{\prime} \\ 0 & 1 & z^{\prime} \\ 0 & 0 & 1\end{array}\right) = \left(\begin{array}{ccc}1 & x + x^{\prime} & y + y^{\prime} + xz^{\prime} \\ 0 & 1 & z + z^{\prime} \\ 0 & 0 & 1\end{array}\right). \] The resulting matrix is still of the desired form, thus the set is closed under multiplication. Next, we establish the identity element. The identity matrix in this context is \[ I = \left(\begin{array}{lll}1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1\end{array}\right) \] since multiplying any matrix of our form with this identity matrix yields the original matrix. For the inverses, consider a matrix \[ \left(\begin{array}{lll}1 & x & y \\ 0 & 1 & z \\ 0 & 0 & 1\end{array}\right). \] We need to find its inverse. By inspection, the inverse takes the form \[ \left(\begin{array}{lll}1 & -x & \cdots \\ 0 & 1 & -z \\ 0 & 0 & 1\end{array}\right), \] specifically, \[ \left(\begin{array}{lll}1 & -x & -y + xz \\ 0 & 1 & -z \\ 0 & 0 & 1\end{array}\right) \] since this matrix multiplied by the original returns the identity. Thus, every element has an inverse. Lastly, associativity is a core property of matrix multiplication, ensuring that \[ (AB)C = A(BC) \] for any matrices \(A, B, C\) in our group. Hence, the structure satisfies the group axioms and forms a group. --- The Heisenberg group is a fascinating structure linking algebra and geometry! It’s pivotal in quantum mechanics because it captures the uncertainty principle and the nature of quantum states. Essentially, this matrix group helps describe how the position and momentum of particles can be simultaneously understood in a non-deterministic framework. Want to see more of its importance? You can explore further into areas where the Heisenberg group holds influence—like representation theory and number theory! It's popping up everywhere from physics to cryptography, exploring the depths of symmetry and transformation.

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