28.7 Probability: the heisenberg uncertainty principle  (Page 4/11)

Why don’t we notice Heisenberg’s uncertainty principle in everyday life? The answer is that Planck’s constant is very small. Thus the lower limit in the uncertainty of measuring the position and momentum of large objects is negligible. We can detect sunlight reflected from Jupiter and follow the planet in its orbit around the Sun. The reflected sunlight alters the momentum of Jupiter and creates an uncertainty in its momentum, but this is totally negligible compared with Jupiter’s huge momentum. The correspondence principle tells us that the predictions of quantum mechanics become indistinguishable from classical physics for large objects, which is the case here.

Heisenberg uncertainty for energy and time

There is another form of Heisenberg’s uncertainty principle     for simultaneous measurements of energy and time . In equation form,

where $\mathrm{\Delta }E$ is the uncertainty in energy    and $\mathrm{\Delta }t$ is the uncertainty in time    . This means that within a time interval $\mathrm{\Delta }t$ , it is not possible to measure energy precisely—there will be an uncertainty $\mathrm{\Delta }E$ in the measurement. In order to measure energy more precisely (to make $\mathrm{\Delta }E$ smaller), we must increase $\mathrm{\Delta }t$ . This time interval may be the amount of time we take to make the measurement, or it could be the amount of time a particular state exists, as in the next [link] .

The uncertainty principle for energy and time can be of great significance if the lifetime of a system is very short. Then $\mathrm{\Delta }t$ is very small, and $\mathrm{\Delta }E$ is consequently very large. Some nuclei and exotic particles have extremely short lifetimes (as small as ${\text{10}}^{-\text{25}}\text{s}$ ), causing uncertainties in energy as great as many GeV ( ${\text{10}}^9\text{eV}$ ). Stored energy appears as increased rest mass, and so this means that there is significant uncertainty in the rest mass of short-lived particles. When measured repeatedly, a spread of masses or decay energies are obtained. The spread is $\mathrm{\Delta }E$ . You might ask whether this uncertainty in energy could be avoided by not measuring the lifetime. The answer is no. Nature knows the lifetime, and so its brevity affects the energy of the particle. This is so well established experimentally that the uncertainty in decay energy is used to calculate the lifetime of short-lived states. Some nuclei and particles are so short-lived that it is difficult to measure their lifetime. But if their decay energy can be measured, its spread is $\mathrm{\Delta }E$ , and this is used in the uncertainty principle ( $\mathrm{\Delta }E\mathrm{\Delta }t\ge h\text{/4}\pi$ ) to calculate the lifetime $\mathrm{\Delta }t$ .