Discussion Overview
The discussion revolves around the gravitational potential of a chargeless particle confined in a box, particularly when the particle is in a stationary state. Participants explore the relationship between gravitational potential, wavefunctions, and the implications of quantum mechanics on gravitational fields.
Discussion Character
- Exploratory
- Technical explanation
- Debate/contested
- Mathematical reasoning
Main Points Raised
- Einstone questions the gravitational potential of a chargeless particle in a stationary state within a box.
- Daniel provides a formula for gravitational potential, suggesting it is defined at the origin of a coordinate system.
- Einstone clarifies that the term 'particle' should refer to a 'microparticle' and notes that a box simplifies the wavefunctions.
- Daniel challenges the relevance of wavefunctions to the gravitational potential of the particle itself.
- Einstone inquires how the potential inside the box is determined, suggesting it should depend on the wavefunction.
- Daniel asserts that the potential is typically given, and wavefunctions are derived from it, referencing Schrödinger's equation.
- Zz emphasizes that the wavefunction is dependent on the potential, not the other way around, reinforcing the order of solving the Schrödinger equation.
- Einstone questions whether a particle interacts with its own gravitational field and reflects on the implications of this interaction.
- Daniel states that in classical theory, particles can interact with their own gravitational field, while reiterating the Newtonian potential.
- A participant discusses the lack of proper equations or theories to describe the gravitational field generated by a quantum particle, referencing a work by R. Wald.
- Einstone expresses confusion over the absence of a consistent theory for combining quantum mechanics with gravitational fields.
- Daniel explains that while both Dirac's equation and general relativity are valid theories, they cannot be easily combined without specific conditions.
Areas of Agreement / Disagreement
Participants express differing views on the relationship between gravitational potential and wavefunctions, with no consensus reached on how to properly describe the gravitational potential of a quantum particle. There are competing perspectives on the interaction of particles with their own gravitational fields and the theoretical frameworks necessary for such descriptions.
Contextual Notes
Participants note limitations in existing theories and equations regarding the gravitational potential generated by quantum particles, highlighting unresolved issues in combining quantum mechanics with classical gravity.