00:02
So we have to consider a system in equilibrium at temperature t.
00:09
So the probability that this system is in a particular quantum state when the energy e is proportional to e to the negative e sub i or kt.
00:25
So a p state, a p state is equal to a constant c, c, c, e to the negative e, the initial energy, e sub i.
00:47
Quote kt.
00:49
And let's call this equation one.
00:54
P is the probability where it sees the constant of personality.
01:00
And e to the negative e sub i over kt is a bolstmann factor, which is named after the physicist lou grink -bostman.
01:15
K is given as our constants, which is 3 .18 times 10 to the negative 23.
01:30
Or k could be equal to 8 .62 times 10 to the fifth.
01:53
So we're given a quantum system consisting of two spins.
02:00
Half particles is in a magnetic field and this system has four possible states.
02:10
The first state is the upward trajectory indicated by the two arrows...