Preferred direction about hydrogen atom

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Discussion Overview

The discussion revolves around the concept of a "preferred direction" in the context of the hydrogen atom as described by the three-dimensional Schrödinger equation. Participants explore the implications of spherical symmetry in quantum mechanics, particularly in relation to external influences such as magnetic fields, and the interpretation of probability distributions in spherical coordinates.

Discussion Character

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

Main Points Raised

  • Some participants note that while the Coulomb field is spherically symmetric, the solutions to the Schrödinger equation can exhibit a preferred direction, particularly in the context of specific angular momentum states (e.g., px, py, pz).
  • Others argue that the preferred direction in spherical coordinates (the z-axis) is physically arbitrary in the absence of external influences, and that actual experimental results remain spherically symmetric.
  • It is suggested that the introduction of a magnetic field creates a physically preferred direction, breaking the spherical symmetry and aligning the z-direction with the magnetic field.
  • Participants discuss that solutions with the same principal quantum number (n) and azimuthal quantum number (l) but different magnetic quantum numbers (m) are not spherically symmetric and have the same energy without a magnetic field.
  • Questions are raised about the implications of multiple free atoms having different orientations of their z-axes and whether the arbitrary direction is a physical reality or merely a mathematical construct.
  • There is a discussion about how the combination of solutions with different probability densities results in a spherical distribution, leading to questions about the interpretation of such measurements.

Areas of Agreement / Disagreement

Participants express both agreement and disagreement regarding the nature of the preferred direction and the implications of spherical symmetry. While some acknowledge the arbitrary nature of the z-axis in the absence of external fields, others emphasize the physical reality of angular momentum and its implications in different contexts.

Contextual Notes

Participants highlight limitations in understanding the physical existence of the arbitrary direction and the interpretation of combined probability distributions, indicating that these aspects remain unresolved and open to further exploration.

ENDLESSYOU
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When solving the three dimensional Schrödinger equation, we obtain a probability distribution on θ. But it seems like the procudure produces a particular direction the z-axis. While the Coulomb field is spherical symmetric, it shouldn't exist such a preferred direction. I'm puzzled.
 
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Hi ENDLESSYOU! :smile:

Individual solutions to a symmetric equation don't have to be symmetric.

Each of the (eg) px py and pz distributions

is a solution to the Schrödinger equation, and does of course have a preferred direction.

But any combination of them will be a new solution, pk, for some direction k.

All directions are treated equally. :wink:
 
If there are no external influences on the hydrogem atom (it's just sitting there) the "preferred direction" in spherical coordinates (the z-axis) is physically arbitrary. It could be up, to the east, to the south, etc. Any actual physical results of experiments that you calculate will be spherically symmetric.

However, when we apply a magnetic field, for example, that creates a physically preferred direction, which breaks the spherical symmetry. Then it is natural to align the z-direction along the magnetic field.

Notice the solutions of the SE with same n and l, but with different m, are not spherically symmetric. Without a magnetic field, they all have the same exact energy. With a magnetic field, they have different energies, and those energies are exact only if the z-axis is along the magnetic field direction.
 
jtbell said:
If there are no external influences on the hydrogem atom (it's just sitting there) the "preferred direction" in spherical coordinates (the z-axis) is physically arbitrary. It could be up, to the east, to the south, etc. Any actual physical results of experiments that you calculate will be spherically symmetric.

However, when we apply a magnetic field, for example, that creates a physically preferred direction, which breaks the spherical symmetry. Then it is natural to align the z-direction along the magnetic field.

Notice the solutions of the SE with same n and l, but with different m, are not spherically symmetric. Without a magnetic field, they all have the same exact energy. With a magnetic field, they have different energies, and those energies are exact only if the z-axis is along the magnetic field direction.

Thanks! But I still have some problems.
1. If there are several free atoms, their z-axes may be in different directions?
2. This arbitary direction is physically existence or just a mathematical construct?
3. The solutions with same n and l have different probability density, but when we add them together, it becomes spherical. How to interpret this by measurement?
 
Last edited:
tiny-tim said:
Hi ENDLESSYOU! :smile:

Individual solutions to a symmetric equation don't have to be symmetric.

Each of the (eg) px py and pz distributions

is a solution to the Schrödinger equation, and does of course have a preferred direction.

But any combination of them will be a new solution, pk, for some direction k.

All directions are treated equally. :wink:

Thanks for your interpretation in a mathematical way!
 
ENDLESSYOU said:
1. If there are several free atoms, their z-axes may be in different directions?

if there's a field, they will line up either with or opposite to it
2. This arbitary direction is physically existence or just a mathematical construct?

it's physical … the angular momentum can be transferred to another body
3. The solutions with same n and l have different probability density, but when we add them together, it becomes spherical. How to interpret this by measurement?

spherical means that the distribution is random, ie we measure the direction as random … we don't know anything about the particle, it is a mixture of all possible solutions :wink:
 

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