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Estimate of the departure from excitation equilibrium of a laser-induced plasma obtained in Ar-H mixtures

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HAL Id: hal-02314863

https://hal.archives-ouvertes.fr/hal-02314863

Submitted on 14 Oct 2019

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Estimate of the departure from excitation equilibrium of a laser-induced plasma obtained in Ar-H mixtures

Aurélien Favre, Arnaud Bultel, Vincent Morel, Stevica Djurovic, Zoran Mijatovic

To cite this version:

Aurélien Favre, Arnaud Bultel, Vincent Morel, Stevica Djurovic, Zoran Mijatovic. Estimate of the departure from excitation equilibrium of a laser-induced plasma obtained in Ar-H mixtures. EMSLIBS 2019, Sep 2019, Brno, Czech Republic. 2019. �hal-02314863�

(2)

10th Euro-Mediterranean Symposium on Laser-Induced Breakdown Spectroscopy, Brno, Czech Republic, 8 – 13th September 2019

CONTEXT & OBJECTIVES

Diagnostic technique LIBS

There are different ways to characterize (i.e. determination of the electron temperature T

e

and density n

e

) a plasma (supposed to be at local thermodynamic equilibrium). One efficient procedure is to integrate the Radiative Transfer Equation to build up a theoretical spectrum. The plasma parameters can be estimated once theoretical and experimental spectra match to each other.

The determination can be more or less accurate depending on the studied spectral region. In the case of an Argon – Hydrogen plasma, it can be done by focusing on Ar lines broadening or shifting. A previous study on Acetone-saturated plasma showed that the determination from 𝐇

𝛂

𝐥eads to an over-estimation of electron density compared to 𝐇

𝛃

values which are quite close from Ar determination.

Estimate of the departure from excitation equilibrium of a laser-induced plasma obtained in Ar-H mixtures

1

CORIA, UMR CNRS 6614, Normandie Université, 76801 Saint-Étienne du Rouvray, F

RANCE

2

Department of Physics, Faculty of Sciences, University of Novi Sad, Novi Sad, 21000, Serbia

aurelien.favre@coria.fr

A URÉLIEN FAVRE 1 , A RNAUD BULTEL 1 , V INCENT MOREL 1 , S TEVICA DJUROVIC 2 , Z ORAN MIJATOVIC 2

Objectives

Describe the influence of major parameters on the determination :

- auto-absorption size - hydrogen dilution

Quantify accurately electron density and temperature from Argon lines

EXPERIMENTAL SETUP

PLASMA SIZE INFLUENCE

W

Air At t = 4 ns

50 µm r

01

CONCLUSIONS & PERSPECTIVES

A nanosecond laser pulse is focused to reach target energy threshold.

The is generated in the chamber. Its radiation is collected on a second optical axis to be analysed with the spectrometer.

Experiments in gases:

Argon – Hydrogen mixtures maintained at atmospheric pressure.

Comments

Non linear response of (n

e

; T

e

) with plasma diameter

Intensified signals are needed to clearly observe 𝐇

𝛃

Temporally resolved determination of (n

e

; T

e

) from [455;480] nm Ar lines

Parameters sensitive to plasma diameter with non-linear response

Hydrogen dilution involves electron density decreasing: dissociation of H

2

Adding hydrogen impacts the level of excitation temperature at long time

Working on 𝐇 𝛂 and 𝐇 𝛃 shifts could be a way to validate the present parameters obtained

Accuracy can be improved by working only on lines (non continuum considered: radiative recombination is strongly density dependent)

Additional experiments are planned to work more closely on 𝐇 𝛂 and 𝐇 𝛃 profiles (to validate acetone behavior with Ar-H mixtures)

PLEIADES characteristics :

LASER : Q-SMART 450 (532 nm, 6 ns, 40 mJ) FOCUSING LENS : f

L

= 125 mm

SPECTROMETER : SCT-320 (f = 0.32m, f/4.6) GRATING : 600 l/mm

CAMERAS : PI-MAX 4 V-UV and PI-MAX 4 V-IR

HYDROGEN DILUTION INFLUENCE

W

Air At t = 4 ns

50 µm r

01

Comments

Correlation with experiment:

Dilution involves a global decrease in n

e

while T

e

remains high with time

DETERMINATION MONITORING

W

Air At t = 4 ns

50 µm r

01

Comments

The more we dilute the less we are accurate (lower densities)

Correlation looks promising in global…

…but we notice that some ionic lines are under-estimated

Hydrogen broadening involves

determination

uncertainties (around

500 nm)

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