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Diagonalizable Matrix Calculator

Diagonalizable Matrix Check:

A matrix is diagonalizable if it has n linearly independent eigenvectors, where n is the dimension of the matrix.

e.g., 1,2;3,4

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1. What is a Diagonalizable Matrix?

A square matrix is diagonalizable if it can be written in the form A = PDP⁻¹, where D is a diagonal matrix and P is an invertible matrix. This means the matrix has enough linearly independent eigenvectors to form a basis.

2. How Does the Calculator Work?

The calculator checks two main conditions:

1. The matrix must have n distinct eigenvalues (where n is the matrix size)
2. For repeated eigenvalues, the geometric multiplicity must equal the algebraic multiplicity

Explanation: The calculator first computes the eigenvalues, then checks if there are enough linearly independent eigenvectors.

3. Importance of Diagonalizability

Details: Diagonalizable matrices are easier to work with for computations like matrix powers and exponentials. Many applications in physics, engineering, and data analysis rely on diagonalization.

4. Using the Calculator

Tips: Enter the matrix elements separated by commas for columns and semicolons for rows. For example, "1,2;3,4" represents a 2×2 matrix.

5. Frequently Asked Questions (FAQ)

Q1: What makes a matrix diagonalizable?
A: A matrix is diagonalizable if it has n linearly independent eigenvectors (where n is the matrix size).

Q2: Are all symmetric matrices diagonalizable?
A: Yes, all real symmetric matrices are diagonalizable with real eigenvalues and orthogonal eigenvectors.

Q3: What's the difference between diagonal and diagonalizable?
A: A diagonal matrix has non-zero elements only on its main diagonal. A diagonalizable matrix can be transformed into a diagonal matrix.

Q4: Can a matrix be diagonalizable over complex numbers but not reals?
A: Yes, some matrices with complex eigenvalues are diagonalizable over complex numbers but not reals.

Q5: How is diagonalization useful in applications?
A: Diagonalization simplifies matrix computations, solves systems of differential equations, and is fundamental in quantum mechanics.

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