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Karteikarten

Quantum optics-Set 1

Gelöschter Nutzer Der Nutzer hat seine Fachbereichs-Information gelöscht. Englisch 15 Karten

Karten in diesem Stapel (15)

  1. 1π and π/2-Puls- π/2-Puls magtransfer superpos state into excited state
    - mixture will be not completely transferred
    - Rabifreq:
     π/ R0: the whole population in excited state
     π/2 R0: equal superposition
  2. 2Fluorescence and natural linewidth- natural: γ10=FWHM at atomic transition
    - fluorescence: fast decay
  3. 3Absorption imaging of ultracold Atoms- lens=imaging system
    - Bild des Schattens der Atome
    - Off resonant laser
  4. 4Suitable Atoms for laser cooling(Alkali and Alkaline Earths)- almost closed two-level transition
    - availability of tonable narrow-bandlasers
    - vapour pressure of the atomic gas in the range of mbar(102Pa) at reachable T (<1500°C)
    - Alkali Atoms: n2S1/2 → n2P3/2 transition
    - all isotopes posses spin (n2P1/2)[hyperfine structure] F=I-1/2; F=I+1/2
    - Alkaline: 2 electrons in s-state n1S0 → n1P1 transition
  5. 5Dipole selection rules- s‘=s
    - L‘=L±1
    - J‘=J; J±1
    - F‘=F; F±1
    - mF‘=mF; mF ±1
  6. 6Polarisation- ε0: describes linearly polarized light (mF‘=mF;π transition; quantization axis parallel to polarisation)
    - ε+1: describes circularly polarized light (mF‘=mF+1;σ+ transition; quantization axis parallel to direction of propagation)
    - ε-1: describes circularly polarized light (mF‘=mF-1;σ- transition; quantization axis parallel to direction of propagation)
  7. 7Principle of slowing atomsmomentum transfer due to absorption
    undirectional emission (spontaneous emission)
    slowing force: (formula)
  8. 8Doppler effect- due to doppler effect, the effective detuning depends on atom velocity
    - adjust such that δeff=0
    - solutions:
     white laser(all frequencies)
     adjust laser freq. (only pulsed possible)
     transition freq. adjust → Zeeman slower
  9. 9Zeeman slowerAbsorption Laserlicht und folgende Reemission von Fluoreszenzphotonen: Bremsen
    Magnetfeld: Zeemaneffekt vs. Dopplerverschiebung
    - B(z) has same shape as v(z)
  10. 10Optical Molassestwo counter propagating lasers to get rid of constant force of the dissipative force
    (F_OM ) ⃗=-β ̃v ⃗ β depends on δ(<0: red detuned) → velocity dep. friction force
  11. 11Doppler limitCooling rate in optical molasses equals heat rate due to isotropic emission
    T_Doppler1D= ħ γ_10/(2k_B )≈100μK
  12. 12Elastic collisions„good collisions“
    total kinetic energy is conserved
    only kinetic redistribution
    for distinguishable particles σ=4πa^2
    for undistinguishable particles r_Boson=8πa^2,σ_Fermion=0
    λ=1/nσ
    Important for evaporative cooling
  13. 13Inelastic collisions- „Bad collisions“
    - loss of energy (kinetic into internal) and far particles
    - Restgas collisions
    - Dipole relaxion (Coupling of two dipoles ↑↑)
    - 3 body-recombination (forming a molecule)
  14. 14BEC-Expansion- uncertainty principle ΔpΔt≥π/2
    - interactions between the atoms
  15. 15Measuring velocity distributions- sketch( laser beam frequency vs. velocity distribution)
    - same shape of velocity distribution than fluorescence signal

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Beschreibung
Der Nutzer hat seine Fachbereichs-Information gelöscht. Karteikarten am Quantum optics-Set 1, erstellt von Gelöschter Nutzer am 24/09/2017.
Erstellt von
Gelöschter Nutzer · Sep 2017
Aktualisiert
24 Sep 2017
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27
Verlauf
  • Erstellt von Tom Schobert · 21 Sep 2017
  • Kopiert von Tom Schobert · 24 Sep 2017
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