1987
DOI: 10.1103/physrevlett.59.2040
|View full text |Cite
|
Sign up to set email alerts
|

Three-step excitation of highly excited autoionizing states in atomic sodium by use of laser beams and synchrotron radiation

Abstract: We have studied highly excited autoionizing states in atomic sodium, using two laser beams and synchrotron radiation. We have observed the electron spectra resulting from the decay of these 2p 5 3s4p, 2p 5 3s4d, and 2p 5 3s5s states to the 2p 6 l So ground state of Na + . The excitation energies and the relative oscillator strengths of inner-shell transitions in the excited atoms have been measured.PACS numbers: 32.80.Fb, 32.80.Dz, 32.80.Hd, 32.80.Wr In this Letter, we present the first experimental evidenc… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

3
25
0

Year Published

1991
1991
2009
2009

Publication Types

Select...
4
2
1

Relationship

0
7

Authors

Journals

citations
Cited by 23 publications
(28 citation statements)
references
References 11 publications
(8 reference statements)
3
25
0
Order By: Relevance
“…This is also the origin of the quadratic pressure dependence of the high harmonic signals, as well as their unusual strengths, that had been found in the very first experimental observations (e.g. [38,39]). …”
Section: Dipole Expectation Valuesupporting
confidence: 55%
See 1 more Smart Citation
“…This is also the origin of the quadratic pressure dependence of the high harmonic signals, as well as their unusual strengths, that had been found in the very first experimental observations (e.g. [38,39]). …”
Section: Dipole Expectation Valuesupporting
confidence: 55%
“…Both the experimental and the theoretical spectra in Fig. 13 show the Ramanallowed series II: (10 , 18 , 26 , 34 , 42 , ..) Bc, but not the series I: (6,14,22,30,38, ..) Bc, seen for N 2 . The anomalous series III: (20, 28, 36, 44,..)…”
Section: E Signals In the Frequency Domainmentioning
confidence: 91%
“…These modifications are sizable and can modify dramatically the interaction of the atomic system with soft or hard x-rays. For example the binding energy of the 2p electron varies from 38 eV for a ground state Na atom to 44.9 eV when the outer electron is promoted to 5s using two dye lasers [129][130][131]. This represents an energy shift of 6.9 eV for the 2p core level, a shift that is much larger than the corresponding shifts due to the laser-induced Stark effect for the 2p electron at the laser power of interest here (~10 14 W/cm 2 ).…”
Section: Bound State Structure and Modification Of X-ray Absorptionmentioning
confidence: 99%
“…A few examples are photon-ion interactions, in which either the ion beam after the collision 2], or electrons emitted are detected; these ions can be highly charged. Other examples are coincidence experiments [3], where low collection efficiencies require intense photonbeams;experiments withactinide targets, wherematerial iseither scarce orhighlyradioactive; and laser-excited targets [4]. Many otherapplications inatomicphysics have been considered [5].…”
Section: Atomic Physics and Highly Charged Ionsmentioning
confidence: 99%