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Matrix hermitian adjoint

The matrix y5 = y°y1y2y3[(y5)2 = +1], anticommutes with all the y s. It therefore has the property that ysyu(y5) 1 — — / . Hence, a possible choice for D is y6. Further properties of the matrices A,B,D can be obtained as follows Consider for example the matrix A. Upon taking the hermitian adjoint of Eq. (9-259) and substituting therein Eq. (9-259) again, we obtain... [Pg.522]

B Complex Conjugate, Transpose, and Hermitian Adjoint of a Matrix... [Pg.309]

A square matrix A is hermitian or self-adjoint if it is equal to its adjoint, i.e., if A = A or ay = a -. Thus, the diagonal elements of a hermitian matrix are real. [Pg.336]

The eigenvalues of a hermitian matrix are real. To prove this statement, we take the adjoint of each side of equation (1.47), apply equation (1.10), and note that A = A ... [Pg.338]

Physicists use the term adjoint to designate A mathematicians use the term associate for A and use the term adjoint with an entirely different meaning.) A Hermitian matrix is equal to its Hermitian conjugate A = A. We illustrate the preceding definitions with an example ... [Pg.297]

A normal matrix is one that commutes with its adjoint, AA = A A. Normal matrices include diagonal, real symmetric, orthogonal, unitary, Hermitian (self-adjoint), permutation, and pseudo-permutation matrices. [Pg.419]

Therefore, the eigenvalues of a Hermitian matrix are real, and the eigenvalues of a skew-Hermitian matrix are pure imaginary. Now consider the eigenvectors x) and x ) belonging to two different eigenvalues a, a of a self-adjoint matrix A. [Pg.421]

A unitary matrix U satisfies li 1 = U1, where U 1 is the inverse and U1 = (U) the adjoint matrix (Magnasco, 2007). A matrix is said Hermitian if U = UL For real elements, unitary and orthogonal matrices coincide, so that we can use either of them indistinctly. [Pg.14]

In standard QM, the reversibility in time is a manifestation of a Hermifian (self-adjoint) system with stationary states and is reflected in the unitarity of the S-matrix. Unitarity entails the inclusion of the contribution of fime-reversed states. In other words, for a stationary state, invariance under time-reversal implies that if is a stationary wavefunction, then so is A major tool for deriving results in the framework of a Hermitian formalism, explicitly or implicitly, is the resolution of the identity operator, I, on the real axis, which is a Hermitian projection operator. [Pg.196]

A matrix is Hermitian or self-adjoint if B = BI. The matrices cr, a2, and ct3 introduced above are all Hermitian. [Pg.171]

If the matrix elements are complex, the adjoint matrix is defined by complex conjugation of the elements followed by transposition, and is denoted with a superscript f. Hermitian matrices are very common in quantum chemistry, and are defined as being self-adjoint, i.e. A = If all the matrix elements are real, the matrix is called symmetric, i.e. A = A . [Pg.516]

The combination of transposition and complex conjugation is called the adjoint operation, indicated by a dagger. A Hermitian matrix is thus self-adjoint. An eigenfunction of this matrix, operating in a function space, may be expressed as a linear combination... [Pg.247]

If matrix A is transposed and in addition all its elements are changed to their complex conjugate, we obtain the adjoint matrix denoted as A = (24 ) = (24 ). If, for a square matrix, we have 24 = 24, 24 is called Hermitian. If 24 is real, then, of course, 24 =. If, in addition, for a real square matrix 24 = 24, then 24 is called... [Pg.891]

The symmetry properties of the second-order density matrix are easy to establish. First, its Hermitian symmetry follows from the definition of Eq. (7.17) and from the adjoint relation ... [Pg.50]

This can also be stated in words that an operator A usually operates to the right on a function but it can also operate to the left on the complex adjoint i j = Hermitian operator. This also means that in the matrix mechanics form of quantum mechanics a given matrix-element of a Hermitian matrix is related to another element on the other side of the (upper left to lower right) diagonal of the matrix by the relationship Amn = A. The following theorem shows why this definition is useful. [Pg.248]


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See also in sourсe #XX -- [ Pg.310 ]




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