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Functions complex conjugates

It is sufficient to vary only the functions complex conjugate to the spinorbitals or only the spinorbitals (cf. p. 197), yet the result is always the same. We decide the first. [Pg.336]

The bra n denotes a complex conjugate wave function with quantum number n standing to the of the operator, while the ket m), denotes a wave function with quantum number m standing to the right of the operator, and the combined bracket denotes that the whole expression should be integrated over all coordinates. Such a bracket is often referred to as a matrix element. The orthonormality condition eq. (3.5) can then be written as. [Pg.55]

This space Jf is the set of all functions f(x) satisfying Eq. (8-2), and is in fact self-dual, because the complex conjugate of any function that satisfies Eq. (8-2), itself also satisfies Eq. (8-2), and so is in Jf. It is to be emphasized that the symbol /> represents the function f(x) with its entire range of values, not just the numerical value of the function at some arbitrary point. The variable x does not appear in the symbol /> for the element of... [Pg.428]

Similarly, for wave functions, hereafter called spinors, we define operations isomorphic to, r and complex conjugation. Thus if u is a column spinor we define... [Pg.524]

Complex conjugation, 492 Complex-valued random variables, 144 Compound distribution, 270 Conditional distribution functions, 148, 152... [Pg.771]

The product of a function and its complex conjugate is always real and is positive everywhere. Accordingly, the wave function itself may be a real or a complex function. At any point x or at any time t, the wave function may be positive or negative. In order that F(x, t)p represents a unique probability density for every point in space and at all times, the wave function must be continuous, single-valued, and finite. Since F(x, /) satisfies a differential equation that is second-order in x, its first derivative is also continuous. The wave function may be multiplied by a phase factor e , where a is real, without changing its physical significance since... [Pg.38]

Both W(x, t) and A p, i) contain the same information about the system, making it possible to find p) using the coordinate-space wave function W(x, t) in place of A(p, i). The result of establishing such a procedure will prove useful when determining expectation values for functions of both position and momentum. We begin by taking the complex conjugate oi A p, i) in equation (2.8)... [Pg.42]

Each of the integrands in equations (2.18), (2.19), and (2.20) is the complex conjugate of the wave function multiplied by an operator acting on the wave function. Thus, in the coordinate-space calculation of the expectation value of the momentum p or the nth power of the momentum, we associate with p the operator (h/f) d/dx). We generalize this association to apply to the expectation value of any function f p) of the momentum, so that... [Pg.43]

The functions tpi(x) are, in general, complex functions. As a consequence, ket space is a complex vector space, making it mathematically necessary to introduce a corresponding set of vectors which are the adjoints of the ket vectors. The adjoint (sometimes also called the complex conjugate transpose) of a complex vector is the generalization of the complex conjugate of a complex number. In Dirac notation these adjoint vectors are called bra vectors or bras and are denoted by or (/. Thus, the bra (0,j is the adjoint of the ket, ) and, conversely, the ket j, ) is the adjoint (0,j of the bra (0,j... [Pg.81]

To obtain ParsevaTs theorem for the function f x) in equation (B.17), we first take the complex conjugate of /(x)... [Pg.291]

Several systems have been reported regarding the connection between oligoferrocenylene multistep redox reactions and the functions of other molecular units. Colbert et al. have reported Mn and Ru complex-conjugated biferrocene derivatives, 20, showing large electron... [Pg.59]

A theory for nonequilibrium quantum statistical mechanics can be developed using a time-dependent, Hermitian, Hamiltonian operator Hit). In the quantum case it is the wave functions [/ that are the microstates analogous to a point in phase space. The complex conjugate / plays the role of the conjugate point in phase space, since, according to Schrodinger, it has equal and opposite time derivative to v /. [Pg.57]

Again, the time dependence off(t) is affected only by the roots of p(s). For the general complex conjugate roots -a bj, the time domain function involves e at and (cos bt + sin bt). The polynomial in the numerator affects only the constant coefficients. [Pg.21]

Note that here bracket does not mean just any round, square, or curly bracket but specifically the symbols and > known as the angle brackets or chevrons. Then ( /l is called a bra and Ivp) is a ket, which is much more than a word play because a bra wavefunction is the complex conjugate of the ket wavefunction (i.e., obtained from the ket by replacing all f s by -i s), and Equation 7.6 implies that in order to obtain the energies of a static molecule we must first let the Hamiltonian work to the right on its ket wavefunction and then take the result to compute the product with the bra wavefunction to the left. In the practice of molecular spectroscopy l /) is commonly a collection, or set, of subwavefunctions l /,) whose subscript index i runs through the number n that is equal to the number of allowed static states of the molecule under study. Equation 7.6 also implies the Dirac function equality... [Pg.114]

If <[>(f) is a wave function amplitude arising from a Hamiltonian that is time-inversion invariant, then we can choose <(>(—t) = (f) for real t, where the star denotes the complex conjugate. Then, the coefficients cm are all real. Next, factorize in products as... [Pg.224]

There needs to be some physical interpretation of the wave function and its relationship to the state of the system. One interpretation is that the square of the wave function, ip2, is proportional to the probability of finding the parts of the system in a specified region of space. For some problems in quantum mechanics, differential equations arise that can have solutions that are complex (contain (-l)1/2 = i). In such a case, we use ip ip, where ip is the complex conjugate of ip. The complex conjugate of a function is the function that results when i is replaced by — i. Suppose we square the function (a + ib) ... [Pg.36]

Because the expression obtained contains i, it is still a complex function. Suppose, however, that instead of squaring (a + ib) we multiply by its complex conjugate, (a — ib) ... [Pg.36]

As noted in Chap. 6, the roots of the characteristic equation, which are the poles of the transfer function, must be real or must occur as complex conjugate pairs. In addition, the real parts of all the poles must be negative for the system to be stable. [Pg.327]

Figure 7. The linear image contributions of a focal-series are located on the surface of two paraboloids obtained by 3D Fourier transformation of the focal series. The two paraboloids correspond to the electron wave function and its complex conjugate. Figure 7. The linear image contributions of a focal-series are located on the surface of two paraboloids obtained by 3D Fourier transformation of the focal series. The two paraboloids correspond to the electron wave function and its complex conjugate.
It is clear that in this approximation F(hkl) equals zero for all reflections for which h + k + l = 4n + 2. This is the reason that the observation of the (222) reflection of diamond led Bragg to conclude that bonding effects are detectable by X-ray diffraction (see chapter 3). If the Si atoms are not spherical, and their density contains antisymmetric components, such as dipolar or octupolar valence density functions, will be the complex conjugate of /fj1 and Eq. (1.12) is no longer valid. We can write = fc + ifa and /f, = fc — ifa, where c stands for the symmetric and a for the antisymmetric component of the atomic rest density. This gives... [Pg.248]

A point that initially surprises some is that many of the off-diagonal terms in Eq. (5.89) are complex-valued, even when the r-space basis functions and expansion coefficients are all real. However, the momentum density is always real because each off-diagonal ij term in Eq. (5.89) is the complex conjugate of the corresponding ji term. The electron density can be written as... [Pg.324]

Note that (2.17) and (2.18) are not unique all complex functions could be replaced by their complex conjugates, and the factor 1 /2it could appear either in (2.17) or (2.18). If we want our expressions to appear more symmetrical, both integrals can have the common multiplicative factor 1 / flfr. There is no universally accepted convention for Fourier transforms. However, once the form of the Fourier transform has been specified, the corresponding expression for the inverse Fourier transform is uniquely determined. [Pg.16]

The time-dependent relaxation rates are real, and the only difference between them is the complex conjugate of the combined modulation function, K+(t, t ). They can be very different for a complex correlation function. [Pg.164]


See other pages where Functions complex conjugates is mentioned: [Pg.12]    [Pg.12]    [Pg.12]    [Pg.12]    [Pg.97]    [Pg.70]    [Pg.232]    [Pg.324]    [Pg.447]    [Pg.143]    [Pg.94]    [Pg.204]    [Pg.57]    [Pg.201]    [Pg.300]    [Pg.222]    [Pg.229]    [Pg.61]    [Pg.83]    [Pg.78]    [Pg.386]    [Pg.46]    [Pg.110]    [Pg.135]    [Pg.238]    [Pg.76]    [Pg.179]    [Pg.67]   
See also in sourсe #XX -- [ Pg.12 ]

See also in sourсe #XX -- [ Pg.12 ]




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