[Q]eigenfunction of position operator and negative energy

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Discussion Overview

The discussion revolves around the properties of the position operator's eigenfunction in quantum mechanics, specifically the Dirac delta function, and the concept of negative energy in both classical and quantum mechanics. Participants explore the implications of these ideas, including normalization and the nature of energy states.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant states that the eigenfunction of the position operator is the Dirac delta function, \(\delta(x-x')\), and questions its normalization and the nature of its complex conjugate.
  • Another participant argues that the product of two delta functions is undefined and asserts that a particle is never in a true position eigenstate, as position measurements only create a sharp peak in the wavefunction.
  • A participant mentions that the eigenvalues of the Hamiltonian can be negative but must be bounded from below, suggesting that one can shift the Hamiltonian to ensure positive eigenvalues.
  • Another participant discusses the equation \(E^2=p^2c^2+m^2c^4\) and notes that while the positive energy is typically considered, the negative sign has physical significance, particularly in relation to antiparticles.
  • One participant reiterates the question of negative energy, stating that while potential energy can be negative in classical mechanics, it is unclear if total energy can be negative in quantum mechanics. They note that interaction potential energy can be negative, but the total energy for realistic systems remains positive.

Areas of Agreement / Disagreement

Participants express differing views on the normalization of the delta function and the implications of negative energy. There is no consensus on whether total energy can be negative in quantum mechanics, as some participants affirm the possibility of negative potential energy while others emphasize the positivity of total energy in realistic systems.

Contextual Notes

Participants highlight the divergence of integrals involving delta functions and the non-normalizability of the delta function as an eigenfunction. There are also discussions about the implications of energy states and the definitions of potential energy in different contexts.

good_phy
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Hi, Everybody know that eigenfunction of position operator x' is \delta(x-x')

But i also knew that integral of square of current state over entire space is 1(probability)

Then, \int_{-\infty}^{\infty}\delta(x-x')\delta(x-x')^{*} dx is 1?

What is conjugate of \delta(x-x')?


And i wandered whether negative energy exists. In classical mechanics, I know potential

energy can have negative sign such as product of electron(negative charge) and voltage.

If electron is at position which potential is larger and kinetic energy of electron, electron

can have negative energy.

Is it vaild in QM?
 
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I think the product of two delta functions is undefined. Also, a particle is never actually in a position eigenstate. A position measurement squeezes the wavefunction so that it gets a sharp peak, but it never actually becomes a delta function.

The eigenvalues of the Hamiltonian must be bounded from below, but they can be negative. Of course you can always replace H with H'=H+bI, where b is a number and I is the identity operator. With a suitable choice of b, the eigenvalues are going to be positive.
 
From

E^2=p^2c^2+m^2c^4 then E=\pm\sqrt(p^2c^2+m^2c^4). Usually we just take the positive sign of E, but actually we can't neglect the minus sign, there's a physical meaning to it.

In particle physics, a minus sign means its antiparticle.
 
good_phy said:
Hi, Everybody know that eigenfunction of position operator x' is \delta(x-x')

But i also knew that integral of square of current state over entire space is 1(probability)

Then, \int_{-\infty}^{\infty}\delta(x-x')\delta(x-x')^{*} dx is 1?

What is conjugate of \delta(x-x')?

\delta(x-x') is a non-normalizable (sometimes called "improper") eigenfunction. This is a real function, so it is equal to its complex conjugate \delta(x-x')^{*} = \delta(x-x'), and the integral you wrote is divergent. If you want to work with normalized eigenfunctions of position, you should consider localized functions, like \sqrt{\delta(x-x')}, though they are not frequently mentioned in the literature.


And i wandered whether negative energy exists. In classical mechanics, I know potential

energy can have negative sign such as product of electron(negative charge) and voltage.

If electron is at position which potential is larger and kinetic energy of electron, electron

can have negative energy.

Is it vaild in QM?

Yes, interaction potential energy can be negative in both classical and quantum mechanics. However, this does not mean that the total energy can be negative too. For realistic physical systems the (negative) potential energy is much smaller than the (positive) rest energy of involved particles mc^2. The sum of all energies (rest+kinetic+potential) is always positive.
 

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