application of thomson scattering on a high pressure mercury lamp
DESCRIPTION
Application of Thomson Scattering on a high pressure mercury lamp. Nienke de Vries, Xiaoyan Zhu Erik Kieft, Joost van der Mullen. Outlook. Introduction Thomson Scattering on a real lamp Thomson Scattering results Equilibrium assumptions Conclusions. h i. e -. Area n e - PowerPoint PPT PresentationTRANSCRIPT
Application of Thomson Scattering on Application of Thomson Scattering on a high pressure mercury lampa high pressure mercury lamp
Nienke de Vries, Xiaoyan Zhu
Erik Kieft, Joost van der Mullen
OutlookOutlook
IntroductionIntroduction Thomson Scattering on a real lamp Thomson Scattering on a real lamp
Thomson Scattering resultsThomson Scattering results Equilibrium assumptionsEquilibrium assumptions ConclusionsConclusions
Thomson ScatteringThomson ScatteringIntroductionIntroduction
Free electrons oscillate in external Free electrons oscillate in external em-fieldem-field
Accelerated electrons in turn emit Accelerated electrons in turn emit radiation (TS light)radiation (TS light)
e-
hi
ne
TeArea ne
Width Te
TS-spectrum
Thomson ScatteringThomson ScatteringIntroductionIntroduction
Scattering parameter Scattering parameter • << << dd < 0.1 < 0.1
Incoherent scattering on random fluctuations in nIncoherent scattering on random fluctuations in nee
• >> >> dd >> 1.0 >> 1.0 Coherent scattering on correlated nCoherent scattering on correlated nee variations variations
d
2
1
24 en
Tk
e
eBd
: : Wavelength shift Wavelength shift scattered radiation scattered radiation dd: : Debye lengthDebye length
Thomson Scattering Set-upThomson Scattering Set-upIntroductionIntroduction
Nd:YAG 532nm
dichroicmirrors
plasma
lenses
TGS
beamdump
iCCD
d
Low pressure gas dischargeLow pressure gas discharge model model lamp lamp • Stray light prevention:Stray light prevention:
Brewster windows Brewster windows Extension tubes (120 cm)Extension tubes (120 cm)
• Incoherent scatteringIncoherent scattering
QL-lampQL-lampIntroductionIntroduction
RF-Coil
11 cm 60 cm60 cm
Brewsterwindow
• Model lampModel lamp Brewster windowsBrewster windows Extension tubes Extension tubes
(60 cm)(60 cm)
• Coherent Coherent scatteringscattering
• In cooperation In cooperation with Bochumwith Bochum
Argon model lampArgon model lampIntroductionIntroduction
• Electron density:Electron density: 10102020 < n <10 < n <1022 22 mm-3-3
• Electron temperature:Electron temperature: TTee 6600 K 6600 K
• Gas pressureGas pressure:: p p 1.5 bar 1.5 bar
High pressure mercury lamp
Hg-lampHg-lampThomson scattering on a real lampThomson scattering on a real lamp
0.2 < < 1.2
Coherent Scattering
Set-up for TS on the Hg-lampSet-up for TS on the Hg-lampThomson scattering on a real lampThomson scattering on a real lamp
Nd:YAG 532nm
mirror
Hg-lamp
imagerotator
grating 1
mask grating 2
intermediateslit
grating 3
polariser
iCCD
d
entranceslit
diaphragm
beamsplitter
beam dump
Triple Grating Spectrograph
lenses
Stray light reduction Stray light reduction • Broad maskBroad mask• Blocking sides of the entrance slitBlocking sides of the entrance slit
Lamp damage due to laser beamLamp damage due to laser beam• Low laser powerLow laser power• Smaller focal length (1m Smaller focal length (1m 0.25m) 0.25m)
Laser induced plasmaLaser induced plasma• Low laser intensityLow laser intensity
Instrumental problemsInstrumental problemsThomson scattering on a real lampThomson scattering on a real lamp
ContributionsContributions Thomson radiationThomson radiation
Plasma radiationPlasma radiation
Stray lightStray light
Dark current Dark current
iCCD image of a measured spectrum
Measured spectrum Measured spectrum Thomson scattering resultsThomson scattering results
Coherent scattering Coherent scattering Thomson scattering on a real lampThomson scattering on a real lamp
Hg-lamp: 0.2 < < 1.2
Spectrum is flattened, width depends on Te
Shape of TS-spectrum depends on scattering parameter
Coherent scattering Coherent scattering Thomson scattering resultsThomson scattering results
TS power
S(k, ): Spectral distribution function
Salpeter approximation used for S(k, ).
Valid for
–Te Tg
–Maxwellian velocity distribution
Fit of TS-spectrum
Central points blocked by a mask
Alternating current: sine wave Alternating current: sine wave Radial profiles of nRadial profiles of nee and T and Tee
• different phases of the currentdifferent phases of the current
Results Results Thomson scattering resultsThomson scattering results
Thermal Equilibrium Thermal Equilibrium • One temperature for all species: TOne temperature for all species: Tee T Tgasgas T Tionion
Thermal Equilibrium in the Hg-lamp?Thermal Equilibrium in the Hg-lamp?• TTee from TS: T from TS: Tee = 7000 = 7000 740 K 740 K
• TTgasgas from X-ray: T from X-ray: Tgasgas = 5200 = 5200 520 K 520 K
• TTe e TTgasgas
Thermal EquilibriumThermal EquilibriumEquilibrium assumptionsEquilibrium assumptions
Chemical Equilibrium Chemical Equilibrium Equilibrium assumptionsEquilibrium assumptions
n1s
Ip
neSahaTe
-1
Electricalproperties
Saha-Boltzman Saha balance :
Hg + e- Hg+ + 2 e-
eee
es
kT
I
kTm
hnn 1
32
1 exp24
Saha equation:
Atomic state distribution function
Chemical Equilibrium Chemical Equilibrium Equilibrium assumptionsEquilibrium assumptions
SahaTe
-1
n1s
Ip
n1
Texc-1
ASDF of an ionising plasma
Overpopulation factor: b1 = n1/n1
s
n1 : Ideal gas law
n1s : Saha equation
Ionising plasma : b1 > 10
Overpopulation of n1,
Slope Texc Te
Chemical EquilibriumChemical EquilibriumEquilibrium assumptionsEquilibrium assumptions
Radial profiles for different phases
Deviations from Saha-BoltzmannDeviations from Saha-Boltzmann• Excitation temperature from ASDF: TExcitation temperature from ASDF: Texcexc= 5200 K= 5200 K
• Electron temperature from TS: TElectron temperature from TS: Tee = 7000 K = 7000 K
Overpopulation factors: bOverpopulation factors: b11 > 10 > 10• Minimum in the centre.Minimum in the centre.• Increase with increasing filling gas.Increase with increasing filling gas.• Maximum at zero crossing of the current Maximum at zero crossing of the current
Chemical Equilibrium Chemical Equilibrium Equilibrium assumptionsEquilibrium assumptions
ConclusionsConclusions
TS for the first time applied on real lampTS for the first time applied on real lamp Indications that the LTE assumption is not Indications that the LTE assumption is not
valid valid • Thermal: TThermal: Tee T Tgasgas
• Chemical: TChemical: Texcexc T Tee, b, b11 >10 >10
RecommendationsRecommendations• Model of Hg lamp including molecular processes Model of Hg lamp including molecular processes