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Wave functions complex conjugate

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]

It will be noticed that in the complex conjugate wave function the exponential terms containing the time are necessarily different from the corresponding terms in P itself, the minus sign being removed to form the complex conjugate. The amplitude functions (z), on the other hand, are frequently real, in which case i (x) = in(x). [Pg.63]

Because Y is a potentially complex function including an imaginary part, Y designates the complex conjugate wave function. The compact and quite famous "bracket" notation on the right-hand side of Equation (2.7) bears the name of Dirac, and the "bra" (Y and "ket" Y) symbols stand for Y and Y and their integration. Mathematically, an integral such as / Y Ydr has been re-written as a scalar product (Y Y) within a complex vector space. [Pg.50]

We note that the incoming wave boundary conditions in the bra state in Eqs. (2.2) and (2.4) can be enforced by not complex conjugating radial functions in bra states of Eq. (2.7). This inner product is called the biorthogonal inner product [29], and is formally related to the use of complex scaled coordinates and absorbing boundary conditions. [Pg.22]

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]

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]

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]

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]

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.
According to the correspondence principle the classical expression for the electron density p(r,t) can be converted to the quantum mechanical description by taking into account that the particle density is calculated by integration of the product of the iV-electron wave function 4 1 and its complex conjugate 4. We introduce the charge-weighted density by multiplication of the electron density with the electron charge,... [Pg.184]

In the response function formalism developed by Mukamel [1], all four wave-mixing spectroscopies are described by four response functions, R, ..., i 4, and their complex conjugates. Double-sided Feynman diagrams are shown in Fig. 12 representing these response functions. The response functions in turn are described by a single line shape function g t) given by... [Pg.161]


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See also in sourсe #XX -- [ Pg.63 , Pg.88 ]




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