Let ( A ) be a symmetric matrix, and let ( \mathbf{u} ) and ( \mathbf{v} ) be eigenvectors corresponding to distinct eigenvalues ( \lambda_1 ) and ( \lambda_2 ), respectively. By definition, we have ( A\mathbf{u} = \lambda_1 \mathbf{u} ) and ( A\mathbf{v} = \lambda_2 \mathbf{v} ). Taking the inner product of ( A\mathbf{u} ) with ( \mathbf{v} ), we get ( \langle A\mathbf{u}, \mathbf{v} \rangle = \lambda_1 \langle \mathbf{u}, \mathbf{v} \rangle ). Since ( A ) is symmetric, ( \langle A\mathbf{u}, \mathbf{v} \rangle = \langle \mathbf{u}, A\mathbf{v} \rangle = \lambda_2 \langle \mathbf{u}, \mathbf{v} \rangle ). Equating the two expressions yields ( \lambda_1 \langle \mathbf{u}, \mathbf{v} \rangle = \lambda_2 \langle \mathbf{u}, \mathbf{v} \rangle ). Since ( \lambda_1 \neq \lambda_2 ), this implies ( \langle \mathbf{u}, \mathbf{v} \rangle = 0 ), proving that the eigenvectors are orthogonal.
The Pauli matrices are a set of three 2x2 complex matrices commonly used in quantum mechanics, represented as ( \sigma_x ), ( \sigma_y ), and ( \sigma_z ). The eigenvalues of all three Pauli matrices are ±1. Specifically, ( \sigma_x ) has eigenvalues 1 and -1, ( \sigma_y ) also has eigenvalues 1 and -1, and ( \sigma_z ) likewise has eigenvalues 1 and -1. Each matrix's eigenvectors correspond to the states of a quantum system along different axes of the Bloch sphere.
corresponding
Yes, in the context of similar shapes.
Space can be divided into n different dimensions. Every dimension is orthogonal to rest all the dimensions. That is the dot product of x with y is zero (y not equal to x).
The corresponding angles in both cases are the same. With congruent triangles, the lengths of the corresponding sides are also equal.
The Pauli matrices are a set of three 2x2 complex matrices commonly used in quantum mechanics, represented as ( \sigma_x ), ( \sigma_y ), and ( \sigma_z ). The eigenvalues of all three Pauli matrices are ±1. Specifically, ( \sigma_x ) has eigenvalues 1 and -1, ( \sigma_y ) also has eigenvalues 1 and -1, and ( \sigma_z ) likewise has eigenvalues 1 and -1. Each matrix's eigenvectors correspond to the states of a quantum system along different axes of the Bloch sphere.
Vectors that go in different directions are called orthogonal vectors. This means that the vectors are perpendicular to each other, with a 90 degree angle between them.
corresponding
similar, as, akin, analogous or corresponding
Different countries have their corresponding "patent offices".
Yes, in the context of similar shapes.
Space can be divided into n different dimensions. Every dimension is orthogonal to rest all the dimensions. That is the dot product of x with y is zero (y not equal to x).
Math Prelude: Orthogonal wave functions arise as a natural consequence of the mathematical structure of quantum mechanics and the relevant mathematical structure is called a Hilbert Space. Within this infinite dimensional (Hilbert) vector space is a definition of orthogonal that is exactly the same as "perpendicular" and that is the natural generalization of "perpendicular" vectors in ordinary three dimensional space. Within that context, wave functions are orthogonal or perpendicular when the "dot product" is zero. Quantum Answer: With that prelude, we can then say that mathematically, the collection of all quantum states of a quantum system defines a Hilbert Space. Two quantum functions in the space are said to be orthogonal when they are perpendicular and perpendicular means the "dot product" is zero. Physics Answer: The question asked has been answered, but what has not been answered (because it was not was not asked), is why orthogonal wave functions are important. As it turns out, anything that you can observe or measure about the state of a quantum system will be mathematically represented with Hermitian operators. A "pure" state, i.e. one where the same measurement always results in the same answers, is necessarily an eigenstate of a Hermtian operator and any two pure states that give two different results of measurement are necessarily "orthogonal wave functions." Conclusion: Thus, there are infinitely many orthogonal wave functions in the set of all wave functions of a quantum system and that orthogonal property has no physical meaning. When one identifies the subset of quantum states that associated pure quantum states (meaning specifically measured properties) and then two distinguishable measurement outcomes are associated with two different quantum states and those two are orthogonal. But, what was asked was a question of mathematics. Mathematically orthogonal wave functions do not guarantee distinct pure quantum state, but distinct pure quantum states does guarantee mathematically orthogonal wave functions. You can remember that in case someone asks.
The corresponding angles in both cases are the same. With congruent triangles, the lengths of the corresponding sides are also equal.
Orthogonal views in radiology refer to imaging perspectives that are perpendicular to each other, typically used to provide a comprehensive assessment of a structure or area of interest. For example, in musculoskeletal imaging, a standard set might include anteroposterior (AP) and lateral views to visualize bones or joints from different angles. This approach helps in accurately diagnosing conditions by allowing for better visualization of spatial relationships and potential abnormalities. Orthogonal views are essential for ensuring that important details are not missed in diagnostic imaging.
The answer is no. When two triangles are congruent all three corresponding sides are the same and all three corresponding angles are the same. Two triangles with the same corresponding angles can have corresponding sides different so they are not congruent.
Different is an adjective and does not change. The corresponding nouns are:difference - plural form differencesdifferentness - plural form differentnesses