Abstract

Laser-produced Sn plasma sources are used to generate extreme ultraviolet (EUV) light in state-of-the-art nanolithography. An ultraviolet and optical spectrum is measured from a droplet-based laser-produced Sn plasma, with a spectrograph covering the range 200 - 800 nm. This spectrum contains hundreds of spectral lines from lowly charged tin ions Sn$^{1+}$ - Sn$^{4+}$ of which a major fraction was hitherto unidentified. We present and identify a selected class of lines belonging to the quasi-one-electron, Ag-like ([Kr]$4d^{10} nl$ electronic configuration), Sn$^{3+}$ ion, linking the optical lines to a specific charge state by means of a masking technique. These line identifications are made with iterative guidance from COWAN code calculations. Of the 53 lines attributed to Sn$^{3+}$, some 20 were identified from previously known energy levels, and 33 lines are used to determine previously unknown level energies of 13 electronic configurations, i.e., $ 7p $, $ (7,8)d $, $ (5,6)f $, $ (6-8)g $, $ (6-8)h $, $ (7,8)i $. The consistency of the level energy determination is verified by the quantum-defect scaling procedure. The ionization limit of Sn$^{3+}$ is confirmed and refined to 328908.4 cm$^{-1}$ with an uncertainty of 2.1 cm$^{-1}$. The relativistic Fock space coupled cluster (FSCC) calculation of the measured level energies are generally in good agreement with experiment, but fail to reproduce the anomalous behavior of the $5d$ $^2$D and $nf$ $^2$F terms. By combining the strengths of FSCC, COWAN code calculations, and configuration interaction many-body perturbation theory (CI+MBPT), this behavior is shown to arise from interactions with doubly-excited configurations.

Highlights

  • Since the early compilation [24] of almost 60 years ago, the only extension of the electronic energy-level structure of SnIV stems from EUV spectroscopy by Ryabtsev and coworkers [30] in which they extend the ns series from n = 8 up to n = 10 and add the 7d 2D term

  • Besides the singly excited levels, some doubly excited energy levels belonging to the 4d9 5s 5p configuration are identified in laser- and vacuum-spark-produced tin plasmas [30,35,36,37,38,39]

  • The laser energy is varied without changing the beam shape by using the combination of a half-wave plate (λ/2) and a thin-film polarizer (TFP), reflecting part of the light into a beamdump (BD)

Read more

Summary

Introduction

Emission of light by neutral tin atoms and lowly charged tin ions, SnI–SnV, is abundant in a wide variety of plasmas, ranging from laser-produced extreme-ultraviolet (EUV) light generating Sn plasma for nanolithography [1,2], divertor plasma when using tin-containing materials in future thermonuclear fusion reactors [3,4,5], and discharge plasma between tin whiskers causing short circuits [6] to astrophysical environments [7,8,9,10,11,12,13,14,15] Spectroscopic investigations of these kinds of plasmas can help characterize plasma parameters [16,17,18,19,20,21,22] such as ion and electron densities and temperatures by study of the observed line strengths and their shapes. The narrow, inverted fine structure of the 4f 2F term in Ag-like Sn3+ has been

Methods
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call