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This point is clearly illustrated, for example, by the discovery and subsequent precision work on parity violation in atoms [for a recent review, see M. A. Bouchiat and C. Bouchiat, "Parity violation in atoms," Rep. Prog. Phys. 60 (11), 1351-1394 (1997)], and by several Nobel prizes awarded for the work in this field, including the ones in 1997 for the development of laser trapping and cooling. [See the Nobel lectures by S. Chu, "The manipulation of neutral particles," Rev. Mod. Phys. 70 (3), 685-706 (1998); C. N. Cohen-Tannoudji, "Manipulating atoms with photons," ibid. 70 (3), 707-719 (1998); W. Phillips, "Laser cooling and trapping of neutral atoms," ibid. 70 (3), 721-741 (1998).]
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This point is clearly illustrated, for example, by the discovery and subsequent precision work on parity violation in atoms [for a recent review, see M. A. Bouchiat and C. Bouchiat, "Parity violation in atoms," Rep. Prog. Phys. 60 (11), 1351-1394 (1997)], and by several Nobel prizes awarded for the work in this field, including the ones in 1997 for the development of laser trapping and cooling. [See the Nobel lectures by S. Chu, "The manipulation of neutral particles," Rev. Mod. Phys. 70 (3), 685-706 (1998); C. N. Cohen-Tannoudji, "Manipulating atoms with photons," ibid. 70 (3), 707-719 (1998); W. Phillips, "Laser cooling and trapping of neutral atoms," ibid. 70 (3), 721-741 (1998).]
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We use the convention of Springer-Verlag, New York, in which alignment designates the second (quadrupole) polarization moment, and orientation designates the first (dipole) polarization moment
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The separation of the nonlinear Faraday effect into the hole-burning and the coherence contribution appears very useful in understanding the underlying physical mechanisms of the phenomenon, and in determining the widths of the magneto-optical resonances (Ref. 7). The two contributions are closely related, however, since they both originate from optical pumping. Thus, unified theoretical treatments of these effects are possible (Ref. 9), which are in good agreement with experiment (Ref. 7).
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85033957711
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Environmental Optical Sensors, Inc., Boulder, CO 80301-3376, phone: (303) 530-7785. The EOSI 2010 system has a built-in wavemeter. After initial calibration, it can display absolute wave-length with uncertainty of ±0.1 nm, which is more than adequate to place the laser frequency within a smooth electronic tuning range from an atomic resonance.
-
Environmental Optical Sensors, Inc., Boulder, CO 80301-3376, phone: (303) 530-7785, http://www.eosi.com. The EOSI 2010 system has a built-in wavemeter. After initial calibration, it can display absolute wave-length with uncertainty of ±0.1 nm, which is more than adequate to place the laser frequency within a smooth electronic tuning range from an atomic resonance.
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40
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85033948120
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Stanford Research Systems, Sunnyvale, CA 94089, phone: (408) 744-8040
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Stanford Research Systems, Sunnyvale, CA 94089, phone: (408) 744-8040, http://www.srsys.com.
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National Instruments, Austin, TX 78730-5039, phone: (512) 794-0100.
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S.-. Kim, S.-E. Park, H.-S. Lee, C.-H. Oh, J.-D. Park, and H. Cho, "High-resolution spectroscopy of rubidium atoms," Jpn. J. Appl. Phys., Part 1 32, 3291-3295 (1993); O. Schmidt, K.-M. Knaak, R. Wynands, and D. Meschede, "Cesium saturation spectroscopy revisited: How to reverse peaks and observe narrow resonances," Appl. Phys. B: Lasers Opt. 59 (2), 167-178 (1994); I. M. Beterov, I. I. Ryabtsev, V. M. Entin, and V. B. Elman, "Alignment in Doppler free spectroscopy of 87Rb," ICAP 16 Abstracts, Windsor 1998, p. 345; W. K. Hensinger, A. G. Truscott, H. Rubinsztein-Dunlop, and N. R. Heckenberg, "Variations of relative line intensity in saturation spectroscopy due to low magnetic fields," submitted to Opt. Quantum Electron.
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(1994)
Appl. Phys. B: Lasers Opt.
, vol.59
, Issue.2
, pp. 167-178
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Schmidt, O.1
Knaak, K.-M.2
Wynands, R.3
Meschede, D.4
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44
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0027628356
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Alignment in doppler free spectroscopy of 87Rb
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S.-. Kim, S.-E. Park, H.-S. Lee, C.-H. Oh, J.-D. Park, and H. Cho, "High-resolution spectroscopy of rubidium atoms," Jpn. J. Appl. Phys., Part 1 32, 3291-3295 (1993); O. Schmidt, K.-M. Knaak, R. Wynands, and D. Meschede, "Cesium saturation spectroscopy revisited: How to reverse peaks and observe narrow resonances," Appl. Phys. B: Lasers Opt. 59 (2), 167-178 (1994); I. M. Beterov, I. I. Ryabtsev, V. M. Entin, and V. B. Elman, "Alignment in Doppler free spectroscopy of 87Rb," ICAP 16 Abstracts, Windsor 1998, p. 345; W. K. Hensinger, A. G. Truscott, H. Rubinsztein-Dunlop, and N. R. Heckenberg, "Variations of relative line intensity in saturation spectroscopy due to low magnetic fields," submitted to Opt. Quantum Electron.
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(1998)
ICAP 16 Abstracts, Windsor
, pp. 345
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Beterov, I.M.1
Ryabtsev, I.I.2
Entin, V.M.3
Elman, V.B.4
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45
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0027628356
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Variations of relative line intensity in saturation spectroscopy due to low magnetic fields
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S.-. Kim, S.-E. Park, H.-S. Lee, C.-H. Oh, J.-D. Park, and H. Cho, "High-resolution spectroscopy of rubidium atoms," Jpn. J. Appl. Phys., Part 1 32, 3291-3295 (1993); O. Schmidt, K.-M. Knaak, R. Wynands, and D. Meschede, "Cesium saturation spectroscopy revisited: How to reverse peaks and observe narrow resonances," Appl. Phys. B: Lasers Opt. 59 (2), 167-178 (1994); I. M. Beterov, I. I. Ryabtsev, V. M. Entin, and V. B. Elman, "Alignment in Doppler free spectroscopy of 87Rb," ICAP 16 Abstracts, Windsor 1998, p. 345; W. K. Hensinger, A. G. Truscott, H. Rubinsztein-Dunlop, and N. R. Heckenberg, "Variations of relative line intensity in saturation spectroscopy due to low magnetic fields," submitted to Opt. Quantum Electron.
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Opt. Quantum Electron
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Hensinger, W.K.1
Truscott, A.G.2
Rubinsztein-Dunlop, H.3
Heckenberg, N.R.4
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46
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85033959660
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note
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This cell was manufactured in the early sixties and is a leftover from the intense investigations of optical pumping carried out at UC Berkeley at that time; see, e.g., J. Yellin, Ph.D. thesis, UC Berkeley, 1965; H. M. Gibbs, Ph.D. thesis, UC Berkeley, 1965. Coated (and uncoated) cells are also available commercially, e.g., from EOSI, Boulder, CO.
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47
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0027609556
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Time of flight effects in nonlinear magneto-optical spectroscopy
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E. Pfleghaar, J. Wurster, S. I. Kanorsky, and A. Weis, "Time of flight effects in nonlinear magneto-optical spectroscopy," Opt. Commun. 99, 303-308 (1993).
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(1993)
Opt. Commun.
, vol.99
, pp. 303-308
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Pfleghaar, E.1
Wurster, J.2
Kanorsky, S.I.3
Weis, A.4
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48
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36049055273
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Relaxation of optically pumped Rb atoms on paraffin-coated walls
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M. A. Bouchiat and J. Brossel, "Relaxation of Optically Pumped Rb At-oms on Paraffin-Coated Walls," Phys. Rev. 147 (1), 41-54 (1966).
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(1966)
Phys. Rev.
, vol.147
, Issue.1
, pp. 41-54
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Bouchiat, M.A.1
Brossel, J.2
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49
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0000063794
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Double-resonance atomic magnetometers: From gas discharge to laser pumping
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E. B. Alexandrov, M. V. Balabas, A. S. Pasgalev, A. K. Vershovskii, and N. N. Yakobson, "Double-Resonance Atomic Magnetometers: from Gas Discharge to Laser Pumping," Laser Phys. 6 (2), 244-251 (1996).
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(1996)
Laser Phys.
, vol.6
, Issue.2
, pp. 244-251
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Alexandrov, E.B.1
Balabas, M.V.2
Pasgalev, A.S.3
Vershovskii, A.K.4
Yakobson, N.N.5
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50
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0000260919
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Doppler-free laser polarization spectroscopy
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C. Wieman and T. W. Hänsch, "Doppler-free laser polarization spectroscopy," Phys. Rev. Lett. 36, 1170-1173 (1976).
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(1976)
Phys. Rev. Lett.
, vol.36
, pp. 1170-1173
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Wieman, C.1
Hänsch, T.W.2
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51
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85033947428
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Channel Industries, Inc., tel. (805) 967-0171, change in length type tube, wall thickness 20 mills, material type C-5600
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Channel Industries, Inc., tel. (805) 967-0171, change in length type tube, wall thickness 20 mills, material type C-5600.
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52
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85033942138
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Magnetic Shield Corp. Perfection Mica Company, Bensenville, IL 6010 6, tel. (630) 766-7800
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Magnetic Shield Corp. Perfection Mica Company, Bensenville, IL 6010 6, tel. (630) 766-7800.
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