- Page 1 and 2: Copyright by Gabriel Noam Price 200
- Page 3 and 4: Single-Photon Atomic Cooling by Gab
- Page 5 and 6: Acknowledgments First, I would like
- Page 7 and 8: Rubidium group when I first joined.
- Page 9 and 10: Single-Photon Atomic Cooling Public
- Page 11 and 12: 2.5.2.4 Magneto-Optical Trap . . .
- Page 13 and 14: List of Tables 2.1 87 Rb Physical P
- Page 15 and 16: 3.1 Vacuum Chamber . . . . . . . .
- Page 17 and 18: Chapter 1 Introduction This chapter
- Page 19 and 20: the momentum kicks due to absorptio
- Page 21 and 22: samples by allowing for very long i
- Page 23 and 24: Figure 1.2: The energy level struct
- Page 25 and 26: quency regime [19]. This then led t
- Page 27 and 28: Figure 1.4: Depiction of a simple,
- Page 29 and 30: demonstrates the cooling power of a
- Page 31 and 32: a) b) c) external potential one-way
- Page 33 and 34: worked on by Brillouin [27-29], ide
- Page 35 and 36: the atomic ensemble. Not surprising
- Page 37 and 38: are untrappable. The SI unit for en
- Page 39: the atomic transition and is called
- Page 43 and 44: constant which is given by α = e2
- Page 45 and 46: only one value of J is possible fro
- Page 47 and 48: the latter of which only applies to
- Page 49 and 50: Figure 2.1: 87 Rb D2 Transition Hyp
- Page 51 and 52: Pluging Eq. 2.18 into this Hamilton
- Page 53 and 54: Following the same logic leads to a
- Page 55 and 56: gF = −1/2 using the approximate e
- Page 57 and 58: mize their energy in high magnetic
- Page 59 and 60: If we now consider the field from t
- Page 61 and 62: where P is in torr. The lifetime of
- Page 63 and 64: component of the dipole oscillation
- Page 65 and 66: maxima. Our experiment makes extens
- Page 67 and 68: atoms its wavefunction Ψ(t) is typ
- Page 69 and 70: In this equation we let H = H0 + Hc
- Page 71 and 72: The significance of Isat is that at
- Page 73 and 74: Δ ω =ω−Δ ω =ω−Δ Δ
- Page 75 and 76: where I/Isat ≪ 1 has been assumed
- Page 77 and 78: λ λ Figure 2.9: The Sisyphus cool
- Page 79 and 80: process repeats. If however, it dec
- Page 81 and 82: σ σ σ Figure 2.10: Geomet
- Page 83 and 84: to vary linearly with position alon
- Page 85 and 86: 0, ±1 and ∆mF = 0, ±1, allow ex
- Page 87 and 88: this figure only the relevant hyper
- Page 89 and 90: D2 transition in 87 Rb has a natura
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2.7.2 Saturation Absorption Spectro
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ground state depletion due to the p
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oadened background can be removed f
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where n is the number density of at
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where σ 2 c = σ 2 2 kBTt n + m .
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Chapter 3 Experimental Apparatus Th
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Figure 3.1: The vacuum chamber duri
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Nor-Cal Products Inc. (AMV-1502-CF)
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and monitor the necessary vacuum le
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3.1.3 Lower Chamber The lower chamb
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a) top ridge 1 cm b) metal jacket h
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to the appropriate frequency throug
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plexiglass cover piezo U stack grat
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λ Figure 3
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Voltage a b c d e f Frequency Figur
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eams. For example the MOT and optic
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λ Figure 3.12: The slave lasers
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λ λ λ
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λ λ λ λ
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needed when forming a MOT or optica
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master laser is dithered at 20 kHz.
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λ λ
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Output Power > 10 W Wavelength 532
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labeled 1, 2 and 3 in the Fig. 3.21
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λ λ λ λ
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process. The two coils are arranged
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19) connected in parallel. This arr
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3.4.2 Horizontal Imaging The horizo
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Chapter 4 Single-Photon Atomic Cool
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1 s, after which time ∼ 10 8 87 R
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(a) x z magnetically trapped atoms
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h x z magnetically trapped atoms y
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z y x magnetically trapped atoms cr
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Figure 4.5: The effective potential
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depopulation present and it indicat
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numbers sufficiently large to quant
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μ μ μ
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the potential landscape due to the
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Figure 4.12: The number of atoms lo
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Figure 4.13: Incremental atom captu
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netic trap and transfer into the op
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temperature TB of atoms loaded into
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used to construct it into the remai
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μ μ μ Figure 4.18: Side view of
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Figure 4.20: Geometry of the optica
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could potentially have undergone th
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detunings. The result of scattering
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are switched off causing non-optica
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Figure 4.25: Number (■) and tempe
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traps. If we model the ensembles in
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Figure 4.26: Radius of the atomic c
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atoms were removed from the magneti
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trappable |F = 1,mF = −1〉 state
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the short lived 2p state. Atoms whi
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Bibliography [1] R. Frisch, “Expe
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[15] C. C. Bradley, C. A. Sackett,
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[31] E.T. Jaynes, “Information th
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[49] J. Ye, S. Swartz, P. Jungner,
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[66] J.P. Gordon and A. Ashkin, “
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[85] C.-S. Chuu, Direct Study of Qu
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adicals,” Phys. Rev. Lett. 94, 02