If a particle has a complex mass, $p^2-m^2=0$ leads to $p^μ \notin \mathbb R^4$. What does it mean?

When you want to calculate S-matrix elements of decay process $\langle p_f,\ldots\mid p_i\rangle$, you compute the $n$-point correlation function $$\langle 0\mid Tφ(x_1)φ(x_2)\ldots\mid 0\rangle$$ and using the LSZ formula. Fourier transformation of the correlation function has the poles at $p_j^2=m_j^2$ ,because it includes the vacuum polarization amplitudes$$ = \frac i {p_j^2-m_j^2+O((p_j^2-m_j^2)^2)}\approx \frac i{p_i^2-m_i^2}$$ on each external legs in diagrams. The LSZ formula says when you multiply $Π_j(p_j^2-m_j^2)/i$ and take the limit $p_j^2→m_j^2$, you get S-matrix elements $\langle p_f,\ldots\mid p_i\rangle$. Therefore, you may know that you need to consider only "amputated diagrams" when you calculate S-matrix.

However, beyond the tree level, the vacuum polarization amplitude of unstable particle has the pole at not real but complex value. This means on shell limit $p_i^2→m_i^2$ leads to $p_i^\mu \notin \mathbb R^4$. On the other hand, if you take limit such as $p_i^2\to\operatorname{Re} m_i^2$, you cannot do the approximation "vacuum polarization amplitudes $ \approx \frac i{p_i^2-m_i^2}$", because $p_i^2$ is far from the pole.

After all, my question is how to compute decay rates of unstable particles correctly. Can I calculate S-matrix elements by computing "amputated diagrams" as usually done?

The related problem is noted in Srednicki's textbook on P.162 http://web.physics.ucsb.edu/~mark/qft.html
He said in and out state should consist of infinitely long-lived particles. He thought unstable particles present as intermediate states, and regarded decay late as a quantity related to the width of resonance. (p.165 (25.25))


Fourier transformation of $f(E)$ gives $g(t)=\exp(iE_0t-Γt/2)$, which seems something expressing decay. I want to know too the precise meaning of this procedure. (At first, I considered the time evolution of $|ψ\rangle = \int dE \, f(E)|E\rangle$ by Schrodinger equation, but $|ψ(t)\rangle\neq g(t)|ψ(0)\rangle$).


I'll discuss this in the context of Yukawa theory, and use renormalized perturbation theory. The way I understand it is this.

Setup: Consider the renormalization scheme

$$ \psi_R = \frac{1}{\sqrt{Z}}\psi_0 \\ m_R = \frac{1}{Z_m} m_0 $$

where $Z_i = 1 + \delta_i$. Then the renormalized propagator is.

$$G^R = \frac{1}{Z_2} G^{bare}. $$

Now recall that summing over all 1PI insertions we may write

$$iG^{bare} = \frac{i}{\not{p} - m_0 + \Sigma(\not{p})}$$

where $\Sigma$ is the sum over all 1PI insertions. Now, we can write $\Sigma = \Sigma_2 + {\cal O}(g^4)$ keeping only those insertions of order less than $g^4$. So that our renormalized propagator to order $g^2$ is

$$G^R = \frac{1}{1+\delta}\frac{i}{\not{p} - m_0 + \Sigma_2(\not{p})} \\ \boxed{G^R= \frac{i}{\not{p} - m_R + \Sigma_R(\not{p})} } $$

where we have defined

$$ \Sigma_R = \Sigma_2 + \delta \not{p} - (\delta + \delta_m)m_R $$

Now, recall that we define the physical mass as the pole of the propagator. Therefore,

$$ m_P - m_R + \Sigma_R(m_P) = 0 .$$

This implies that

$$ \boxed{\delta_m m_P = \Sigma_R(m_P)} $$

Your question: Let us call $\Sigma_2(\not{p}) = i\Delta m$, anticipating that the correction is purely imaginary. Then, our propagator is

$$\tilde{G}^R= \frac{i}{\not{p} - m_R+ i\Delta m} $$

where now we know that our propagator has a pole at $m_P$.

Recall that the amplitude for a particle to propagate from $x$ to $y$ is given by the fourier transform

$$D(x-y) = \int \frac{d^4p}{(2\pi)^4} \frac{i}{\not{p} - m_R + i\Delta m}e^{-ip(x-y)} $$

To make things easier suppose that y=0. Then we have

$$D(x) = \int \frac{d^4p}{(2\pi)^4} \frac{i}{\not{p} - m_R+ i\Delta m}e^{i\mathbf{p\cdot x}}e^{-iEt} $$

Where $E = \sqrt{p^2 + m_{rest}^2}$. What is the mass of the particle in its rest frame? Well by definition it's the pole of the propagator! And so we may replace

$$E = \sqrt{p^2 + (m_R - i \Delta m)^2} \\ =\sqrt[4]{\left(-{\Delta m}^2+m^2+p^2\right)^2+4 {\Delta m}^2 m^2} \left(i \sin \left(\frac{\phi}{2}\right)+\cos \left(\frac{\phi}{2}\right)\right)\\ \boxed{E \equiv \xi \left(i \sin \left(\frac{\phi}{2}\right)+\cos \left(\frac{\phi}{2}\right)\right) }$$

where $\phi$ is the $\mathrm{Arg}$ of the radicand.Finally, we obtain that

$$ \boxed{D(x) = \int \frac{d^4p}{(2\pi)^4} \frac{ie^{i\mathbf{p\cdot x}} e^{-i\xi\cos(\frac{\phi}{2}) t}}{\not{p} - m_R+ i\Delta m}e^{-\xi\sin(\frac{\phi}{2}) t}} $$

and so we see that indeed the probability for a particle to exist at a time $t$ decays exponentially.

  • $\begingroup$ Thank you for answering my questions! I clearly understand how to interpret decay rates. D(y-x)=<0|Tφ(y)φ(x)|0>=<$y_i|exp(-iH(y_0-x_0)|x_i$>, therefore the probability amplitude of the state will exponentially decrease as time goes on according to your calculation. I did not suppose Fourier transformation of f(E) appeared in the calculating D(y-x) from $\tilde G^R(p)$. I greatly appreciate your answer! $\endgroup$ Jan 9 '19 at 7:29
  • $\begingroup$ Right! That’s how I think about it at least $\endgroup$ Jan 9 '19 at 7:44

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