IndexKwantySticker

Condensa

Bose–Einstein Condensate Physics

\[\frac{N_0}{N} = 1 - \left(\frac{T}{T_c}\right)^{3/2}\quad(T\le T_c)\]
Cena regularna $4.99 USD
Cena regularna Cena promocyjna $4.99 USD
W promocji Wyprzedane
Size
Surface

Can atoms share one state? Condensa is a Bose–Einstein condensate. Below a critical temperature, a large fraction of a gas of bosons drops into the single lowest-energy state. Bose and Einstein predicted it in 1924–25, and it was first made in a lab in 1995. A 3" pixel-art sticker; equation, symbols and sources in the physics panel below.

Shipping calculated at checkout by destinationMade to order, ships in 2–5 business days

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

Shipping

Shipping calculated at checkout by destination. Printed to order for you.

Delivery times & where we ship

Returns & replacements21 days

Every item is printed to order, so we can’t accept returns or exchanges for change of mind, or if you ordered the wrong size or colour.

Print defect, misprint, damage or the wrong item? We’ll send a free replacement, or a refund if you prefer. Report it within 21 days of delivery with a photo; no need to send it back.

Full refund & replacement policy

The physics

Below a critical temperature, a gas of bosons starts collecting in its lowest quantum state. The fraction in that state grows as the temperature drops, following 1 − (T/Tc)^(3/2), and the critical temperature depends on the gas's density and particle mass.

Condensa is what happens when bosons get cold enough to share one state.

Below a critical temperature T_c a macroscopic fraction of an ideal Bose gas piles into the ground state: N_0/N = 1 − (T/T_c)^{3/2}. At T = 0 everyone is downstairs; above T_c the condensate fraction is zero.

The chart on the sticker is that curve. ζ(3/2) ≈ 2.612 fixes T_c for a given density and mass. On the building, the upper floors are nearly empty and the ground floor is packed.

Satyendra Nath Bose and Albert Einstein predicted this in 1924–25; dilute atomic gases first crossed T_c in 1995.

Everyone in the ground floor.

Equations

\[\frac{N_0}{N} = 1 - \left(\frac{T}{T_c}\right)^{3/2}\quad(T\le T_c)\]
\[kT_c = \frac{2\pi\hbar^2}{m}\left(\frac{n}{\zeta(3/2)}\right)^{2/3}\]
Symbols
SymbolMeaningUnit
\(N_0\) number of bosons in the ground state —
\(N\) total number of bosons —
\(T\) temperature \(\mathrm{K}\)
\(T_c\) critical temperature for condensation \(\mathrm{K}\)
\(n\) number density \(\mathrm{m^{-3}}\)
\(m\) boson mass \(\mathrm{kg}\)
\(\zeta(3/2) \approx 2.612\) Riemann zeta value —

Sources

  1. Einstein (1925) Quantentheorie des einatomigen idealen Gases, Sitzungsberichte der Preussischen Akademie der Wissenschaften
  2. Bose (1924) Plancks Gesetz und Lichtquantenhypothese, Z. Phys. 26, 178
  3. Pethick & Smith, Bose–Einstein Condensation in Dilute Gases, Ch. 1
  4. Pathria & Beale, Statistical Mechanics, Ch. on ideal Bose gas

Source Einstein, A. (1925). Quantentheorie des einatomigen idealen Gases. Zweite Abhandlung. Sitzungsberichte der Preußischen Akademie der Wissenschaften (Berlin), Physikalisch-mathematische Klasse, 3–14.