What is the reason for positronium's short lifetime and instability?

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Discussion Overview

The discussion centers on the instability and short lifetime of positronium, a bound state of an electron and a positron. Participants explore the reasons behind its short lifetime, which is on the order of 10^-10 seconds, and the implications of wavefunction overlap in this context. The conversation includes theoretical considerations, mathematical formulations, and comparisons to hydrogen-like systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note that positronium is unstable due to the annihilation of the electron and positron, which occurs when their wavefunctions overlap in space.
  • Others argue that solving the Schrödinger equation for positronium is similar to that for hydrogen, with adjustments for the reduced mass of the electron.
  • It is suggested that there are bound states in positronium where the probability of finding the electron at the positron's location is zero, potentially leading to metastable states.
  • One participant mentions that certain excited states may mix, which could allow for annihilation despite having no overlap at the origin.
  • Another participant points out that positronium tends to minimize its energy, similar to hydrogen, and that excited states decay by emitting photons, although they clarify that positronium does not emit gamma rays during atomic transitions.
  • Mathematical expressions for the lifetimes of para-positronium and ortho-positronium are provided, along with measured values.
  • There is a correction regarding the naming of the ground state of positronium, clarifying that it is referred to as 1S0 rather than 1S1.

Areas of Agreement / Disagreement

Participants express a range of views on the mechanisms of positronium's instability, with some agreeing on the role of wavefunction overlap while others contest specific details about energy states and transitions. The discussion remains unresolved regarding the implications of these factors on the lifetime of positronium.

Contextual Notes

Participants highlight the complexity of energy states and the potential for mixing, which introduces uncertainty in the discussion of annihilation rates and lifetimes. There are also unresolved aspects regarding the definitions and implications of certain quantum states.

mrjeffy321
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I know positronium is an unstable pairing of an electron and positron in a Hydrogen-like system with a very short lifetime on the order of around E-10 seconds (depending on its initial state).

I would like to better-understand why positronium is so unstable, despite having bound energy states like those in stable atoms.

I have heard that the short lifetime is due to the partial wave function overlap between the two particles (which form a particle-antiparticle pair). This, very brief, explanation makes some sense to me. If the wave function’s overlap, there is some probability of the two particles being in the same space at the same time. If this should ever occur (which it is bound to after a sufficient amount of time has passed) then the electron-positron pair will annihilate each other and destroy the positronium atom, in the process releasing a couple of photons in order to conserve energy and momentum.

In order to get a better understanding (beyond what I just inferred) I asked my professor who is quite knowledgeable on the subject. The only kind of answer I could get was that ‘positronium is unstable because the electron and positron are annihilating each other’. This explanation, which feels somewhat unsatisfactorily basic, just leads me to believe that the two particles know the other is there and ‘wants’ to annihilate, so it does.

Where can I find a more detailed description of the process?
 
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I have also always thought that the wavefunctions are overlapping in the ground state thus allowing for annihilation.

It should be to solve the same Schrödinger eq. as for the hydrogen atom.
 
That's exactly it - there is a wavefunction overlap. (And not just for the ground state)
 
Vanadium 50 said:
That's exactly it - there is a wavefunction overlap. (And not just for the ground state)

Ah yes of course the other states ahve overlap, silly me :-)
 
Solving the Schrödinger equation for positronium should be virtually identical to solving it for Hydrogen except that one needs to use the reduced mass of the electron (more-so) in order to correct for the altered energy levels.
Like in Hydrogen there will be a small, but non-zero, probability of finding the electron in the “nucleus” (on in this case, the positron) when in one of the S orbitals (when l = 0 angular momentum). When this happens, the electron-positron pair annihilates and the positron atom decays into gamma rays.

Vanadium 50 said:
That's exactly it - there is a wavefunction overlap. (And not just for the ground state)
There are, however, bound states where (at least for Hydrogen, so I would assume also for positronium) there is zero probability of finding the electron in the “nucleus”. In these states then there would be no way for the wave functions to overlap and the electron-positron pair to annihilate. Would these correspond the metastable, longer-lived, states? From these states, the atom can relax by emitting a photon, and going to a lower energy level where there is an overlap in the wave functions and annihilation is possible.

Would this be an accurate explanation?
 
That's close. The one complication is that states may mix: for example 3D1 has no wavefunction overlap at the origin, but 3S1 does. Both have the same quantum numbers, so if there is any mixing at all, both states can annihilate. I don't know if they do mix - just that this would be the consequence if they did.
 
Well, also those energy levels are excited. The positronium WANTS to minimize it's energy, so it WANTS to be in the 1S1 state. Just like hydrogen---you don't find random excited hydrogen atoms floating around...they all decay by emitting gamma rays.
 
positronium lifetimes...


para-positronium lifetime (S = 0):
t_{0} = \frac{2 \hbar}{m_e c^2 \alpha^5}

\boxed{t_{0} = 1.244 \cdot 10^{-10} \; \text{s}}
t_{0} = 1.25 \cdot 10^{-10} \; \text{s} - measured

ortho-positronium lifetime (S = 1):
t_{1} = \frac{9 \pi \hbar}{2 m_e c^2 \alpha^6 (\pi^2 - 9)}

\boxed{t_{1} = 1.386 \cdot 10^{-7} \; \text{s}}
t_{1} = 1.420 \cdot 10^{-7} \; \text{s} - measured
[/Color]
Reference:
http://en.wikipedia.org/wiki/Positronium"
http://arxiv.org/PS_cache/hep-ph/pdf/0310/0310099v1.pdf"
 
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BenTheMan said:
Well, also those energy levels are excited. The positronium WANTS to minimize it's energy, so it WANTS to be in the 1S1 state. Just like hydrogen---you don't find random excited hydrogen atoms floating around...they all decay by emitting gamma rays.

Positronium doesn't want anything. It's an inanimate object.

It also doesn't emit gamma rays in atomic transitions - they are mostly in the ultraviolet. Only when there is annihilation do you get gamma rays.

There is no 1S1 state of positronium. Or anything else, for that matter. 1S1 means spin angular momentum is zero, orbital angular momentum is zero, and total angular momentum is 1. That's impossible. The ground state of positronium is 1S0.

Finally, annihilation can in fact be comparable in rate to atomic transitions. The classic example is that the 3S1 state can make a magnetic dipole transition to 1S0, but in fact tends to annihilate instead.
 

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