Virtual laboratory/Physics/Thermodynamics/Bose–Einstein condensate — the fifth state of matter

Bose–Einstein condensate — the fifth state of matter

An extension of the topic of temperature and states of matter. At temperatures close to absolute zero (nanokelvins) bosonic atoms stop behaving like a classical gas — they collapse into one shared quantum state of the lowest energy, forming a Bose–Einstein condensate, a "superatom" (Nobel Prize 2001).

Bose–Einstein condensate — the fifth state of matter
Physics · Thermodynamics · Bose–Einstein condensate (FIZ.TERMO.PR.06)
Temperature of the atom cloud TT (T_c ≈ 200 nK)10.2 K
At temperatures close to absolute zero, bosonic atoms…
temperature T
10.2 K
threshold T_c
200 nK
condensate N₀/N
0.0%
state
classical gas
🎯 Challenge: identify the state
streak: 0

I will give you the atom cloud temperature — guess the state (no slider). Threshold T_c ≈ 200 nK.

What just happened?

We cooled the cloud of bosonic atoms far below the critical temperature TcT_c. Instead of each moving chaotically on its own, the atoms “merged” into one shared, lowest-energy quantum state — this is the Bose–Einstein condensate.

Condensate fraction:

N0N=1−(TTc)3(T<Tc)\dfrac{N_0}{N} = 1-\left(\dfrac{T}{T_c}\right)^{3} \quad (T<T_c)

— N₀ is the number of atoms in the condensate, N is the total number of atoms. The further below TcT_c, the larger the fraction of atoms that “fall” into the common ground state.

Why does this happen only near zero?

Each atom corresponds to a matter wave whose de Broglie wavelength grows as the atom slows down:

λdB=h2πmkBT\lambda_{dB} = \dfrac{h}{\sqrt{2\pi m k_B T}}

When TT drops to nanokelvins, λdB\lambda_{dB} becomes comparable to the spacing between atoms — their matter waves begin to overlap. The atoms lose their individual identity and are described by one shared wave function.

Why is it the fifth state of matter?

It is not a gas, liquid, solid, or plasma — the BE condensate is a macroscopic quantum object: millions of atoms behave like a single “superatomic” wave, with phase coherence and superfluid properties.

Nobel Prize 2001:

The first Bose–Einstein condensate was created in 1995 by Eric Cornell and Carl Wieman (rubidium atoms), and independently by Wolfgang Ketterle (sodium atoms), combining laser cooling with evaporative cooling. For this achievement they received the Nobel Prize in Physics in 2001. Today BE condensates are used in atomic clocks and precise quantum sensors.

Why you need this for the exam:

This extends the kinetic-molecular theory of gases and wave–particle duality (de Broglie). Trick: check whether TT is above or below TcT_c — that decides whether the gas is described by the Maxwell–Boltzmann distribution or by a single condensate wave function.

Remember: Bose–Einstein condensation occurs only below the critical temperature T_c, close to absolute zero — it is the fifth state of matter, in which atoms lose their individual identity and behave like one quantum wave.

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Theory & formulas

The fifth state of matter

At temperatures close to absolute zero (on the order of nanokelvins) bosonic atoms stop behaving like a classical gas — they all collapse into one shared quantum state of the lowest energy, forming a "superatom".

Why absolute zero is needed

Each atom corresponds to a thermal de Broglie wave, which grows longer as the temperature falls: λdB∼1T\lambda_{dB} \sim \dfrac{1}{\sqrt{T}} The condensate forms when these waves become longer than the distances between atoms — the matter waves begin to overlap and "merge".

Applications

Precise atomic clocks, studies of the foundations of quantum mechanics, simulations of quantum systems (Nobel Prize 2001).

Notation: λdB\lambda_{dB} — thermal de Broglie wavelength, TT — absolute temperature.

Frequently asked questions

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What is the fifth state of matter?

The Bose–Einstein condensate — a state of matter in which atoms merge into one shared quantum state.

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Why is such a low temperature needed?

Because only below the critical temperature do the atoms' matter waves begin to overlap and "merge".

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What is it used for?

In precise atomic clocks, studies of the foundations of quantum mechanics, and simulations of quantum systems.

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