Alkali D Line Data - Steck

Alkali D Line Data - Steck

3 Hyperfine Structure 5 trapping experiments are also given here. The recoil temperature is the temperature corresponding to an ensemble with a one-dimensional rms momentum of one photon recoil ~k

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Cesium D Line Data - Steck

Cesium D Line Data Daniel A. Steck Theoretical Division (T-8), MS B285 Los Alamos National Laboratory Los Alamos, NM 87545 23 January 1998 …

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Alkali D Line Data - Steck

1 Introduction 3 1 Introduction In this reference we present many of the physical and optical properties of cesium that are relevant to various quantum optics experiments.

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Rubidium 87 D Line Data - Steck

Rubidium 87 D Line Data Daniel A. Steck Theoretical Division (T-8), MS B285 Los Alamos National Laboratory Los Alamos, NM 87545 …

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Sodium D Line Data - Steck

Sodium D Line Data Daniel A. Steck Theoretical Division (T-8), MS B285 Los Alamos National Laboratory Los Alamos, NM 87545 27 May 2000 (revision 1.6, 14 October 2003)

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Rubidium 87 D Line Data - Steck

balance of Doppler cooling and recoil heating [13]. Of course, in Zeeman-degenerate atoms, sub-Doppler cooling mechanisms permit temperatures substantially below this limit [14]. 3 Hyperfine Structure 3.1 Energy Level Splittings The 5 2S 1/2 −→ 5 2P 3/2 and 5 2S 1/2 −→ 5 P 1/2 transitions are the components of a fine-structure doublet ...

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Alkali D Line Data - Steck

4 2 Rubidium 85 Physical and Optical Properties totypicallaboratoryconditions(1atmpressure,23 Ctemperature,and40%relativehumidity).Theindexof ...

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Cesium D Line Data - Steck

23 January 1998 (revision 1.6, 14 October 2003) 1 Introduction In this reference we present many of the physical and optical properties of cesium that are relevant to various quantum optics experiments. In particular, we giveparameters that are useful in treating the mechanical effects of lighton cesium atoms.

  1998, Cesium

KEK

Lecture Note on Photon In teractions and Cross Sections Hideo Hira y ama KEK, High Energy Accelerator Researc h Organization, 1-1, Oho, Tsukuba, Ibaraki, 305-0801 Japan

  Photon

Alkali D Line Data - Steck

3 Hyperfine Structure 5 because ∆ωsw/2πis the beat frequency of the two waves, and λ/2 is the spatial periodicity of the standing wave. For a standing wave velocity of vr, Eq.(8) gives ∆ωsw = 4ωr.Two temperatures that are useful in cooling and trapping experiments are also given here.

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WIZARD® Automatic Gamma Counters: Superior …

Effective lead shielding means constant background and minimal crosstalk. In a universal gamma counter, the lead shielding around the detector is another important factor in determining the

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304 Chapter21.Blackholes Hawking radiation: black holes ...

304 Chapter21.Blackholes such phenomena, scientists hope to learn what some of the basic fea-tures of quantum gravity may be. Hawking radiation: black holes are truly black bodies

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REQUIREMENTS FOR MEDICAL IMAGING MONITORS (part I)

REQUIREMENTS FOR MEDICAL IMAGING MONITORS (part I) ... White

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Noteson&Atomic&Structure& - TAPIR at Caltech

& & A.BASICSTRUCTURE&!! Hydrogen!is!the!simplest!atom,!consisting!of!a!single!electron!and!a!nucleus.!!We!will! treat!the!hydrogenlike!atoms!generally,!allowing!for!a ...

Thursday 9 June 2016 – Afternoon - ocr.org.uk

Thursday 9 June 2016 – Afternoon AS GCE PHYSICS A G482/01 Electrons, Waves and Photons INSTRUCTIONS TO CANDIDATES † Write your name, centre number and candidate number in …