Bose-Einstein statistics

They interpreted this effect as due to Bose-Einstein statistics.

Bose-Einstein statistics is a theory that describes how collections of bosons behave.

Bose's "error" lead to what is now called Bose-Einstein statistics.

Bose-Einstein statistics are now used to describe the behaviors of any assembly of bosons.

These statistical properties are described as Bose-Einstein statistics.

In Bose-Einstein statistics, any number of identical bosons can be in the same state.

But if you look at the statistical properties alone, we find it has exactly the same statistics as the Bose-Einstein statistics.

It is these commutation relations that imply Bose-Einstein statistics for the field quanta.

It is also possible to derive approximate Bose-Einstein statistics in the canonical ensemble.

The theory becomes known as Bose-Einstein statistics.

These are different to the particles called bosons which are explained by Bose-Einstein statistics.

Objects that are exactly identical behave differently: they are said to obey Bose-Einstein statistics.

Exactly the same approach can be used to derive Fermi-Dirac and Bose-Einstein statistics.

Particles with integer spin, on the other hand, obey Bose-Einstein statistics, and are known as bosons.

Bosons follow a theory called Bose-Einstein statistics.

Keith Richards wrote a physics textbook that satisfactorily explained Bose-Einstein statistics!

A magnon in an antiferromagnetism carries spin 1 and thus obeys Bose-Einstein statistics.

Bosons are particles which satisfy Bose-Einstein statistics.

Both phonons and photons are bosons and thus, they obey Bose-Einstein statistics.

Fermions contrast with bosons which obey Bose-Einstein statistics.

Helium-4 atoms are bosons, and their superfluidity can be understood in terms of the Bose-Einstein statistics that they obey.

They obey Bose-Einstein statistics.

It is composed of bosons, which have an integer value of spin, and obey Bose-Einstein statistics.

This formula, apart from the first vacuum energy term, is a special case of the general formula for particles obeying Bose-Einstein statistics.

In Dirac's time, it was not yet known that all bosons, including photons, must obey Bose-Einstein statistics.