Blue laser cooling transitions in Tm I
Identifieur interne : 000705 ( Pascal/Curation ); précédent : 000704; suivant : 000706Blue laser cooling transitions in Tm I
Auteurs : N. Kolacheysky [Russie] ; A. Akimov [Russie] ; I. Tolstikhina [Russie] ; K. Chebakov [Russie] ; A. Sokolov [Russie] ; P. Rodionov [Russie] ; S. Kanorski [Russie] ; V. Sorokin [Russie]Source :
- Applied physics. B, Lasers and optics : (Print) [ 0946-2171 ] ; 2007.
Descripteurs français
- Pascal (Inist)
- Refroidissement par laser, Faisceau atomique, Laser bleu, Horloge atomique, Spectrométrie absorption, Etat fondamental, Domaine temps ns, Structure fine, Spectrométrie saturation, Structure hyperfine, Transition dipolaire magnétique, Lanthanide Atome, Thulium 169, Thulium Atome, 3270C, 3280P, Tm, 3280F, 0630F.
English descriptors
- KwdEn :
Abstract
We have studied possible candidates for laser cooling transitions in 109Tm in the spectral region of 41U-42U nm. By means of saturation absorption spectroscopy, we have measured the hyperfine structure and rates of two nearly closed cycling transitions from the ground state 4 f136s2 (2F0) (Jg = 7/2) to upper states 4f12(3H5)5d3/26s2(Je = 9/2) at 410.6 nm and 4f12(3F4)5d5/26s2(Je = 9/2) at 420.4 nm and evaluated the life times of the excited levels as 15.9(8) ns and 48(6)ns, respectively. Decay rates from these levels to neighboring opposite-parity levels are evaluated by means of Hartree-Fock calculations. We conclude that the strong transition at 410.6 nm has an optical leak rate of less then 2 x 10-5 and can be used for efficient laser cooling of 169Tm from a thermal atomic beam. The hyperfine structure of two other even-parity levels, which can be excited from the ground state at 409.5 nm and 418.9 nm, is also measured by the same technique. In addition, we give a calculated value of 7(2) s-1 for the rate of magnetic-dipole transition at 1.14 μm between the fine structure levels (Jg = 7/2) ↔ (J'g = 5/2) of the ground state which can be considered as a candidate for applications in atomic clocks.
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<term>Atomic beams</term>
<term>Atomic clocks</term>
<term>Blue laser</term>
<term>Fine structure</term>
<term>Ground states</term>
<term>Hyperfine structure</term>
<term>Laser cooling</term>
<term>Magnetic dipole transition</term>
<term>Rare earths Atoms</term>
<term>Saturation spectroscopy</term>
<term>Thulium 169</term>
<term>Thulium Atoms</term>
<term>ns range</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Refroidissement par laser</term>
<term>Faisceau atomique</term>
<term>Laser bleu</term>
<term>Horloge atomique</term>
<term>Spectrométrie absorption</term>
<term>Etat fondamental</term>
<term>Domaine temps ns</term>
<term>Structure fine</term>
<term>Spectrométrie saturation</term>
<term>Structure hyperfine</term>
<term>Transition dipolaire magnétique</term>
<term>Lanthanide Atome</term>
<term>Thulium 169</term>
<term>Thulium Atome</term>
<term>3270C</term>
<term>3280P</term>
<term>Tm</term>
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<front><div type="abstract" xml:lang="en">We have studied possible candidates for laser cooling transitions in 109Tm in the spectral region of 41U-42U nm. By means of saturation absorption spectroscopy, we have measured the hyperfine structure and rates of two nearly closed cycling transitions from the ground state 4 f<sup>13</sup>
6s<sup>2</sup>
(<sup>2</sup>
F<sub>0</sub>
) (J<sub>g</sub>
= 7/2) to upper states 4f<sup>12</sup>
(3H5)5d3/26s2(Je = 9/2) at 410.6 nm and 4f<sup>12</sup>
(<sup>3</sup>
F<sub>4</sub>
)5d<sub>5/2</sub>
6s<sup>2</sup>
(J<sub>e</sub>
= 9/2) at 420.4 nm and evaluated the life times of the excited levels as 15.9(8) ns and 48(6)ns, respectively. Decay rates from these levels to neighboring opposite-parity levels are evaluated by means of Hartree-Fock calculations. We conclude that the strong transition at 410.6 nm has an optical leak rate of less then 2 x 10<sup>-5</sup>
and can be used for efficient laser cooling of <sup>169</sup>
Tm from a thermal atomic beam. The hyperfine structure of two other even-parity levels, which can be excited from the ground state at 409.5 nm and 418.9 nm, is also measured by the same technique. In addition, we give a calculated value of 7(2) s<sup>-1</sup>
for the rate of magnetic-dipole transition at 1.14 μm between the fine structure levels (Jg = 7/2) ↔ (J'<sub>g</sub>
= 5/2) of the ground state which can be considered as a candidate for applications in atomic clocks.</div>
</front>
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<fC01 i1="01" l="ENG"><s0>We have studied possible candidates for laser cooling transitions in 109Tm in the spectral region of 41U-42U nm. By means of saturation absorption spectroscopy, we have measured the hyperfine structure and rates of two nearly closed cycling transitions from the ground state 4 f<sup>13</sup>
6s<sup>2</sup>
(<sup>2</sup>
F<sub>0</sub>
) (J<sub>g</sub>
= 7/2) to upper states 4f<sup>12</sup>
(3H5)5d3/26s2(Je = 9/2) at 410.6 nm and 4f<sup>12</sup>
(<sup>3</sup>
F<sub>4</sub>
)5d<sub>5/2</sub>
6s<sup>2</sup>
(J<sub>e</sub>
= 9/2) at 420.4 nm and evaluated the life times of the excited levels as 15.9(8) ns and 48(6)ns, respectively. Decay rates from these levels to neighboring opposite-parity levels are evaluated by means of Hartree-Fock calculations. We conclude that the strong transition at 410.6 nm has an optical leak rate of less then 2 x 10<sup>-5</sup>
and can be used for efficient laser cooling of <sup>169</sup>
Tm from a thermal atomic beam. The hyperfine structure of two other even-parity levels, which can be excited from the ground state at 409.5 nm and 418.9 nm, is also measured by the same technique. In addition, we give a calculated value of 7(2) s<sup>-1</sup>
for the rate of magnetic-dipole transition at 1.14 μm between the fine structure levels (Jg = 7/2) ↔ (J'<sub>g</sub>
= 5/2) of the ground state which can be considered as a candidate for applications in atomic clocks.</s0>
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<fC03 i1="01" i2="3" l="FRE"><s0>Refroidissement par laser</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Laser cooling</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Faisceau atomique</s0>
<s5>04</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Atomic beams</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Laser bleu</s0>
<s5>11</s5>
</fC03>
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<s5>11</s5>
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<s5>12</s5>
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<s5>12</s5>
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<fC03 i1="05" i2="3" l="FRE"><s0>Spectrométrie absorption</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Absorption spectroscopy</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Etat fondamental</s0>
<s5>41</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Ground states</s0>
<s5>41</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Domaine temps ns</s0>
<s5>42</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>ns range</s0>
<s5>42</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Structure fine</s0>
<s5>43</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Fine structure</s0>
<s5>43</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Spectrométrie saturation</s0>
<s5>61</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Saturation spectroscopy</s0>
<s5>61</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Structure hyperfine</s0>
<s5>62</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Hyperfine structure</s0>
<s5>62</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE"><s0>Transition dipolaire magnétique</s0>
<s5>63</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG"><s0>Magnetic dipole transition</s0>
<s5>63</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA"><s0>Transición dipolar magnética</s0>
<s5>63</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Lanthanide Atome</s0>
<s2>NC</s2>
<s5>64</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Rare earths Atoms</s0>
<s2>NC</s2>
<s5>64</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Thulium 169</s0>
<s5>65</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Thulium 169</s0>
<s5>65</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Thulium Atome</s0>
<s2>NC</s2>
<s5>66</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Thulium Atoms</s0>
<s2>NC</s2>
<s5>66</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>3270C</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>3280P</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Tm</s0>
<s4>INC</s4>
<s5>85</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>3280F</s0>
<s4>INC</s4>
<s5>86</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>0630F</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fN21><s1>028</s1>
</fN21>
</pA>
</standard>
</inist>
</record>
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