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Blue laser cooling transitions in Tm I

Identifieur interne : 000705 ( Pascal/Curation ); précédent : 000704; suivant : 000706

Blue 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 :

RBID : Pascal:08-0061178

Descripteurs français

English descriptors

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.
pA  
A01 01  1    @0 0946-2171
A03   1    @0 Appl. phys., B Lasers opt. : (Print)
A05       @2 89
A06       @2 4
A08 01  1  ENG  @1 Blue laser cooling transitions in Tm I
A11 01  1    @1 KOLACHEYSKY (N.)
A11 02  1    @1 AKIMOV (A.)
A11 03  1    @1 TOLSTIKHINA (I.)
A11 04  1    @1 CHEBAKOV (K.)
A11 05  1    @1 SOKOLOV (A.)
A11 06  1    @1 RODIONOV (P.)
A11 07  1    @1 KANORSKI (S.)
A11 08  1    @1 SOROKIN (V.)
A14 01      @1 P.N. Lebedev Physics Institute, Leninsky prospekt 53 @2 119991 Moscow @3 RUS @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. @Z 6 aut. @Z 7 aut. @Z 8 aut.
A20       @1 589-594
A21       @1 2007
A23 01      @0 ENG
A43 01      @1 INIST @2 16194B @5 354000174363540270
A44       @0 0000 @1 © 2008 INIST-CNRS. All rights reserved.
A45       @0 30 ref.
A47 01  1    @0 08-0061178
A60       @1 P
A61       @0 A
A64 01  1    @0 Applied physics. B, Lasers and optics : (Print)
A66 01      @0 DEU
C01 01    ENG  @0 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.
C02 01  3    @0 001B00F30F
C02 02  3    @0 001B30B70C
C02 03  3    @0 001B30B80P
C02 04  3    @0 001B30B80F
C03 01  3  FRE  @0 Refroidissement par laser @5 03
C03 01  3  ENG  @0 Laser cooling @5 03
C03 02  3  FRE  @0 Faisceau atomique @5 04
C03 02  3  ENG  @0 Atomic beams @5 04
C03 03  3  FRE  @0 Laser bleu @5 11
C03 03  3  ENG  @0 Blue laser @5 11
C03 04  3  FRE  @0 Horloge atomique @5 12
C03 04  3  ENG  @0 Atomic clocks @5 12
C03 05  3  FRE  @0 Spectrométrie absorption @5 30
C03 05  3  ENG  @0 Absorption spectroscopy @5 30
C03 06  3  FRE  @0 Etat fondamental @5 41
C03 06  3  ENG  @0 Ground states @5 41
C03 07  3  FRE  @0 Domaine temps ns @5 42
C03 07  3  ENG  @0 ns range @5 42
C03 08  3  FRE  @0 Structure fine @5 43
C03 08  3  ENG  @0 Fine structure @5 43
C03 09  3  FRE  @0 Spectrométrie saturation @5 61
C03 09  3  ENG  @0 Saturation spectroscopy @5 61
C03 10  3  FRE  @0 Structure hyperfine @5 62
C03 10  3  ENG  @0 Hyperfine structure @5 62
C03 11  X  FRE  @0 Transition dipolaire magnétique @5 63
C03 11  X  ENG  @0 Magnetic dipole transition @5 63
C03 11  X  SPA  @0 Transición dipolar magnética @5 63
C03 12  3  FRE  @0 Lanthanide Atome @2 NC @5 64
C03 12  3  ENG  @0 Rare earths Atoms @2 NC @5 64
C03 13  3  FRE  @0 Thulium 169 @5 65
C03 13  3  ENG  @0 Thulium 169 @5 65
C03 14  3  FRE  @0 Thulium Atome @2 NC @5 66
C03 14  3  ENG  @0 Thulium Atoms @2 NC @5 66
C03 15  3  FRE  @0 3270C @4 INC @5 83
C03 16  3  FRE  @0 3280P @4 INC @5 84
C03 17  3  FRE  @0 Tm @4 INC @5 85
C03 18  3  FRE  @0 3280F @4 INC @5 86
C03 19  3  FRE  @0 0630F @4 INC @5 91
N21       @1 028

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Pascal:08-0061178

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<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>
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<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>
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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>
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<s1>Blue laser cooling transitions in Tm I</s1>
</fA08>
<fA11 i1="01" i2="1">
<s1>KOLACHEYSKY (N.)</s1>
</fA11>
<fA11 i1="02" i2="1">
<s1>AKIMOV (A.)</s1>
</fA11>
<fA11 i1="03" i2="1">
<s1>TOLSTIKHINA (I.)</s1>
</fA11>
<fA11 i1="04" i2="1">
<s1>CHEBAKOV (K.)</s1>
</fA11>
<fA11 i1="05" i2="1">
<s1>SOKOLOV (A.)</s1>
</fA11>
<fA11 i1="06" i2="1">
<s1>RODIONOV (P.)</s1>
</fA11>
<fA11 i1="07" i2="1">
<s1>KANORSKI (S.)</s1>
</fA11>
<fA11 i1="08" i2="1">
<s1>SOROKIN (V.)</s1>
</fA11>
<fA14 i1="01">
<s1>P.N. Lebedev Physics Institute, Leninsky prospekt 53</s1>
<s2>119991 Moscow</s2>
<s3>RUS</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
</fA14>
<fA20>
<s1>589-594</s1>
</fA20>
<fA21>
<s1>2007</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>16194B</s2>
<s5>354000174363540270</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2008 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>30 ref.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>08-0061178</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Applied physics. B, Lasers and optics : (Print)</s0>
</fA64>
<fA66 i1="01">
<s0>DEU</s0>
</fA66>
<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>
</fC01>
<fC02 i1="01" i2="3">
<s0>001B00F30F</s0>
</fC02>
<fC02 i1="02" i2="3">
<s0>001B30B70C</s0>
</fC02>
<fC02 i1="03" i2="3">
<s0>001B30B80P</s0>
</fC02>
<fC02 i1="04" i2="3">
<s0>001B30B80F</s0>
</fC02>
<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>
<fC03 i1="03" i2="3" l="ENG">
<s0>Blue laser</s0>
<s5>11</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE">
<s0>Horloge atomique</s0>
<s5>12</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Atomic clocks</s0>
<s5>12</s5>
</fC03>
<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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