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Adjoint operator of a complex number?

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How can we show that the position operator is Hermitian?

To show that the position operator is Hermitian, we need to demonstrate that its adjoint is equal to itself. In mathematical terms, this means proving that the integral of the complex conjugate of the wave function multiplied by the position operator is equal to the integral of the wave function multiplied by the adjoint of the position operator. This property is essential in quantum mechanics as it ensures that the operator corresponds to a physical observable.


Can you make momentum operator non self adjoint?

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How can one determine if an operator is Hermitian?

To determine if an operator is Hermitian, one must check if the operator is equal to its own conjugate transpose. This means that the operator's adjoint is equal to the operator itself. If this condition is met, then the operator is Hermitian.


What is a Hermitian operator?

A Hermitian operator is a linear operator that is equal to its own adjoint. In other words, the adjoint of a Hermitian operator is the same as the operator itself. Hermitian operators play a key role in quantum mechanics as they correspond to observable physical quantities.


Is momentum hamiltonian operator is hermitian operator?

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How can you create a new operator through operator overloading?

You cannot create a new operator through operator overloading. You can only redefine an existing operator, with certain limitations. As an example, for a class of complex numbers, having a real and an imaginary part, you might want an addition operator. This is the skeleton of code to do that. I only show the operator, not any constructors or other operators or methods, etc.class complex {private:double real, imaginary;public:complex operator+ (complex operand) {complex temp;temp.real = this.real + operand.real;temp.imaginary = this.imaginary + operand.imaginary;return temp;}};The above answer is for C++. Since this question is also categorized in Java Programming it's important to note that operator overloading is not currently possible in Java.


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What is the significance of the adjoint spinor in the context of quantum field theory?

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Write a program to write the sum of two complex number using friend function and overloading constractor?

#include<iostream.h> #include<conio.h> class complex { int r; int i; public: complex() { } complex(int a,int b) { r=a;i=b; } friend complex operator+(complex,complex); friend show(complex); complex operator+(complex c1,complex c2) { complex c3; c3.r=c1.r+c2.r; c3.i=c1.i+c2.i; return(c3); } show(complex c) { cout<<c.r<<"i+"<<c.i<<endl; } void main() { complex a,b,c; clrscr(); a.complex(3,6); b.complex(4,7); c=a+b; show(a); show(b); show(c); getch() }


What is the function of operator 'j' in alternating current?

The operator 'j' represents the imaginary unit in alternating current circuits. It is used to denote the phase difference or angular displacement between voltage and current waveforms in complex impedance calculations. The use of 'j' helps in simplifying mathematical calculations in AC circuits by treating the impedance as a complex number.