This$^1$ has to do with the uncertainty relation for energy and time:
$$\Delta E \Delta t \approx \hbar$$
where $\hbar\sim10^{-15}\,\mathrm{eV\cdot s}$ is Dirac's constant (or Planck's constant divided by $2\pi$). This means conservation of energy can apparently be broken for very short time scales. The emphasis is on the very. A particle can therefore be created from the vacuum, as long as it disappears again within some time scale governed by the above approximate equality. This phenomenon is called a quantum fluctuation.
For example, if you wanted to create a proton (mass of approximately $10^9\,\mathrm{eV}$) in a vacuum, it would only be around for about
$$\frac{10^{-15}\,\mathrm{eV\cdot s}}{10^9\,\mathrm{eV}} = 10^{-24}\,\mathrm{s}$$
which is obviously not very long. And a proton has a negligible mass compared to your entire body.
Of course, if your body is around, it's likely not happening in a vacuum. So then Neuneck's answer is probably more appropriate. The particles are created using energy available in the environment. In this case however, there's no reason for them to necessarily disappear since there was no breaking of energy conservation. So although this is probably the situation more in tune with your question, it is most likely not the situation that is meant in the quote. (quantum fluctuations are more likely)
$^1$ In the vacuum of space at least, and I think that's what they're talking about in this particular quote. In presence of other matter, it is (or should be) more conceivable to people that it is possible to create particles using some energy from the matter in the environment. Though upon re-reading the quote, perhaps they're talking about quantumtunneling as well.