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6,9,10,15,40,41 The experiments reported in the companion paper are at the lower end of the scale. Even then, the role of the ions can be enhanced by the presence of a static dc field. This second-order synergetic effect deserves a separate examination in its own right
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6,9,10,15,40,41 The experiments reported in the companion paper are at the lower end of the scale. Even then, the role of the ions can be enhanced by the presence of a static dc field. This second-order synergetic effect deserves a separate examination in its own right.
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44
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The same conclusion will follow if we consider first the effect of the field and then the additional coupling due to the core. Due to the high degeneracy, the field alone will lead to clumping of lifetimes, which will be evened out by the coupling due to the core
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The same conclusion will follow if we consider first the effect of the field and then the additional coupling due to the core. Due to the high degeneracy, the field alone will lead to clumping of lifetimes, which will be evened out by the coupling due to the core.
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46
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85033048820
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2) will, on the average, be larger for the shorter lifetimes
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2) will, on the average, be larger for the shorter lifetimes.
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85033060708
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49 have provided a clear and detailed discussion of this point and include references to earlier papers
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49 have provided a clear and detailed discussion of this point and include references to earlier papers.
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52
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85033048798
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1) as the origin of this elongation
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1) as the origin of this elongation.
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85033057062
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j in the jth eigenvalues of the effective Hamiltonian
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j in the jth eigenvalues of the effective Hamiltonian.
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58
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85033037217
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58-61 Quantum fluctuations about the mean are to be expected
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58-61 Quantum fluctuations about the mean are to be expected.
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64
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85033038707
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The general question of the spectral representation of the evolution operator is discussed in some detail in ref 63
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The general question of the spectral representation of the evolution operator is discussed in some detail in ref 63.
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65
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85033059998
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5/2Ry where Ry is the Rydberg constant
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5/2Ry where Ry is the Rydberg constant.
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67
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85033061825
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66
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66
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69
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85033060587
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68
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68
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70
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85033059593
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-1) is too broad to resolve the Stark components and that beyond the Inglis-Teller limit the Stark broadening is in any case sufficient to make adjacent Stark manifolds overlap
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-1) is too broad to resolve the Stark components and that beyond the Inglis-Teller limit the Stark broadening is in any case sufficient to make adjacent Stark manifolds overlap.
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71
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85033071493
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5, as a convenient marker
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5, as a convenient marker.
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72
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85033059010
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21,27,31 This also means that n can decrease only by so much under the combined influence of the core and the field. On the other hand, the strength of the coupling to the core increases for lower n's
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21,27,31 This also means that n can decrease only by so much under the combined influence of the core and the field. On the other hand, the strength of the coupling to the core increases for lower n's.
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