BOSE–EINSTEIN CONDENSATE

The fifth state of matter shows up only below temperatures colder than interstellar space. For a rubidium-87 gas the threshold Tc sits near 170 nano-kelvin, and below it a broad cloud piles into one sharp peak, the condensate fraction following N₀/N = 1 − (T/Tc)³. The reason lies in the de Broglie wavelength: the colder it gets the more that wavelength swells, until it exceeds the spacing between atoms, the matter waves overlap and the atoms can no longer be told apart. Fermions cannot do this, forbidden by the Pauli principle.

▸ Loading a dilute boson gas in a magneto-optical trap…
▸ Engaging laser cooling + evaporative cooling
▸ Calibrating the critical temperature Tc (nano-Kelvin)
▸ Tracking de Broglie wavelength overlap
▸ Piling bosons into the ground state — super-atom…
▸ Ready — Online. ✅
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Simulation room Bose–Einstein Condensate

Bose–Einstein Condensate
Online
boson · super-atom · de Broglie · fifth state of matter
Phenomenon shown
❄️ Ngưng tụ
Temperature T—
Versus Tc—
Condensate fraction—
λ de Broglie—
State—
Quantum notes
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Drag the temperature slider on the right to cool down → bosons pile into the centre as a super-atom. Pick a “Phenomenon” to switch scenes.
Particle distribution by energy level (sharp peak = BEC) densitycondensate peak
About Bose–Einstein Condensate

The fifth state of matter shows up only below temperatures colder than interstellar space. For a rubidium-87 gas the threshold Tc sits near 170 nano-kelvin, and below it a broad cloud piles into one sharp peak, the condensate fraction following N₀/N = 1 − (T/Tc)³. The reason lies in the de Broglie wavelength: the colder it gets the more that wavelength swells, until it exceeds the spacing between atoms, the matter waves overlap and the atoms can no longer be told apart. Fermions cannot do this, forbidden by the Pauli principle.

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