LASER LIGHT SCATTERING AND EEDF MEASUREMENTS IN A NANODUSTY PLASMA

Slides:



Advertisements
Similar presentations
Chapter 21 - Colligative Properties Explain how solutes effect the properties of a solution. Use Raoult’s Law to calculate vapor pressure of solution.
Advertisements

Winfred Stoffels STOOR. Plasma research at the group EPG Winfred Stoffels.
Nonequilibrium Thermodynamics Laboratories The Ohio State University OH Laser-Induced Fluorescence Measurements in Nanosecond Pulse Discharge Plasmas Inchul.
PROPERTIES OF NONTHERMAL CAPACITIVELY COUPLED PLASMAS GENERATED IN NARROW QUARTZ TUBES FOR SYNTHESIS OF SILICON NANOPARTICLES* Sang-Heon Song a), Romain.
Chapter 22 Section 2 Review Page 560
The Spatiotemporal Evolution of an RF Dusty Plasma: Comparison of Numerical Simulations and Experimental Measurements Steven Girshick, Adam Boies and Pulkit.
Laser Plasma and Laser-Matter Interactions Laboratory The effect of ionization on condensation in ablation plumes M. S.
Interfacial transport So far, we have considered size and motion of particles In above, did not consider formation of particles or transport of matter.
Research Opportunities in Radiation-Induced Chemical Dynamics Scientific Opportunities for Studying Laser Excited Dynamics at the LCLS: David Bartels Notre.
WEEK20 PHYSICAL SCIENCE VOCABULARY. 1) THERMAL ENERGY Total amount of energy in all of the particles contained in a sample of matter.
Wittaya Julklang, Boris Golman School of Chemical Engineering Suranaree University of Technology STUDY OF HEAT AND MASS TRANSFER DURING FALLING RATE PERIOD.
VUV PHOTON SOURCE OF A MICROWAVE EXCITED MICROPLASMAS AT LOW PRESSURE*
EUROPEAN COOPERATION IN SCIENCE AND TECHNOLOGY COST is supported by the EU RTD Framework Programme ESF provides the COST Office through an EC contract.
Mechanical vs. Electromagnetic Waves. Mechanical Waves Waves that require a material medium Examples include water, sound, and waves along a spring.
Science study guide. SC.A The kinetic of matter- states that all of the particles that make up matter are constantly in motion. Temperature is a.
Photos placed in horizontal position with even amount of white space between photos and header Sandia National Laboratories is a multi-program laboratory.
Plasma diagnostics using spectroscopic techniques
Unit 3 Lesson 3 Energy Transfer
Temperature and Heat Transfer Food and Cooking Unit Mrs. Caldwell’s Class.
Real-Time Optical Diagnostics of Rapid Graphene Growth CNMS Staff Science Highlight Real-time Raman spectroscopy, optical reflectivity, and microscope.
DRY ETCHING OF Si 3 N 4 USING REMOTE PLASMA SOURCES SUSTAINED IN NF 3 MIXTURES* Shuo Huang and Mark J. Kushner Department of Electrical Engineering and.
Changes of State Solid, Liquid, Gas, Plasma, Bose- Einstein Condensate.
Zhouqian, Wan baonian and spectroscopy team
DOE Plasma Science Center Control of Plasma Kinetics
INSIGHTS INTO THE MECHANISM OF IN-PLASMA PHOTO-ASSISTED ETCHING
WHY DOES FRESH NUCLEATION OCCUR IN A DUSTY PLASMA VOID?
ADVANCES IN HYBRID KINETIC-FLUID SOLVERS FOR GAS DISCHARGE PLASMAS
DOE Plasma Science Center Control of Plasma Kinetics
PLASMA-WATER: SOLVATED ELECTRONS
ENERGY LOADING AND DECAY OF N2 VIBRATION
University of Michigan 8th Annual Graduate Student Symposium (MIPSE)
N2 Vibrational Temperature, Gas Temperature,
TRANSPORT IN MAGNETIZED PLASMAS INTERROGATED BY LCIF
ELECTRIC FIELD MEASUREMENTS IN ns ATMOSPHERIC PRESSURE AIR PLASMA
DOE Plasma Science Center Control of Plasma Kinetics
DOE Plasma Science Center Control of Plasma Kinetics
COMPLEX ELECTRON ENERGY DISTRIBUTIONS IN ASYMMETRIC RF-DC DISCHARGES
Crystal Whisker Growth on Porous Coatings
Ch 2 notes Honors Biology Book.
PLASMA DIAGNOSTICS IN AIR PLASMAS CONTAINING WATER DROPLETS
LASER-COLLISION INDUCED FLUORESCENCE IN ARGON DISCHARGES
ANTIMICROBIAL PLASMA-ACTIVATED WATER SYNERGIZES WITH UV A PHOTONS
Changing States of Matter
DIAGNOSTICS OF ATMOSPHERIC PRESSURE PLASMAS UTILIZING ULTRAFAST LASERS
DOE Plasma Science Center Control of Plasma Kinetics
DOE Plasma Science Center Control of Plasma Kinetics
ELECTRIC FIELD VECTOR MEASUREMENTS
DOE Plasma Science Center Control of Plasma Kinetics
Sub-Ns Electric Field Measurements
DOE Plasma Science Center Control of Plasma Kinetics
DOE Plasma Science Center Control of Plasma Kinetics
STREAMER SIMULATIONS WITH FLUID & PIC
EFFECT OF RF VOLTAGE ON STRUCTURE OF A NANOPARTICLE CLOUD
PULSED DUSTY PLASMA FOR CONTROL OF NANOPARTICLE FLUXES TO A SUBSTRATE
GENERATION OF NOVEL EEDFS IN A TANDEM PLASMA REACTOR
New Diagnostic for Electric Field
OH KINETICS IN A SHIELDED ATMOSPHERIC PRESSURE PLASMA JET
Changing States of Matter
Electron Transfer in cluster Anions:
DOE Plasma Science Center Control of Plasma Kinetics
INTERACTION BETWEEN PLASMA AND WATER
CONTROL OF PLASMA-BIOINTERACTIONS BY TUNING PLASMA CHEMISTRY
DOE Plasma Science Center Control of Plasma Kinetics
NON-MONOTONIC DISTRIBUTIONS OF EXCITED ATOMS IN
Diagnostics for Metastable species and Electric
PLASMA-SURFACE INTERACTION (PSI) AT
Heat Transfer.
Characteristics of Water
Yunbo Zhong, Li Zhihua, Zhongming Ren Shanghai University
SPATIAL & TEMPORAL EVOLUTION OF
Presentation transcript:

LASER LIGHT SCATTERING AND EEDF MEASUREMENTS IN A NANODUSTY PLASMA Using a Langmuir probe, electron energy probability functions (EEPF) are measured in a nanodusty plasma maintained between two parallel plates. Simultaneously, laser light scattering is used to visualize the particles. As particles nucleate and grow, low energy electrons are depleted by attachment to the particles. Scattering Intensity Pristine Ar plasma 27 mm t = 30 s t = 90 s t = 150 s t = 180 s EEPF in a SiH4/Ar = 98.4/1.6 plasma during growth of Si nanoparticles at 80 mTorr, 40 W. Laser Scattering DOE Plasma Science Center Control of Plasma Kinetics PLSC_0614 HIGHLIGHT 1

[OH], liquid surface at y=0 RADICAL SPECIES MEASUREMENTS IN IONIZATION WAVE PLASMAS AT LIQUID-VAPOR INTERFACE 2-D distributions of absolute OH and H densities measured in ns pulse, surface ionization wave plasma at liquid water / saturated water vapor interface, using line images taken by calibrated LIF and TALIF laser diagnostics. Peak H and OH mole fractions ≈1.6% and ≈0.03%, H recombines very slowly, diffuses and convects with buffer Ar flow. Demonstrated capability of absolute, time- and space-resolved, in situ radical measurements (H, OH, O, NO, N) in liquid-vapor interface plasmas (aqueous solutions, alcohols). Insight into kinetics of liquid-vapor interface plasma chemical reactions [OH], liquid surface at y=0 [H], flow left to right DOE Plasma Science Center Control of Plasma Kinetics PLSC_0614 HIGHLIGHT 2