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Bijal Vara et al Int. Journal of Engineering Research and Applications www.ijera.com
ISSN : 2248-9622, Vol. 4, Issue 3( Version 1), March 2014, pp.244-247
www.ijera.com 244 | P a g e
Langmuir probe Diagnostic for local parameter measurement in
Magnetized Plasma using LabVIEW
Bijal Vara1
, C S Dalal2
, S Karkari3
, H Kabariya4
1
(Department of instrumentation and control, Dharmsinh Desai University, Nadiad)
2
(Department of instrumentation and control, Dharmsinh Desai University, Nadiad)
3, 4
(Institute of Plasma research, Gandhinagar)
ABSTRACT
In recent years, plasma technology is used by Semiconductor, thin film industries for deposit layers, etching
process and surface modification. So it is necessary to understanding internal plasma parameter. Langmuir
probe is one of the simplest techniques which is used to measure wide range of plasma parameter like plasma
potential, floating potential, electron temperature, electron energy distribution function (EEDF) etc. Langmuir
current voltage characteristic is obtained by varying bias voltage of the probe. LabVIEW is most powerful
Microsoft window compatible software which is used to immediate data acquisition and analysis. In this paper
describes analysis of Langmuir data using LabVIEW software which automatically measure I-V Plasma probe
Characteristics and obtain EEDF of plasma.
Keywords – EEDF, LabVIEW, Langmuir probe, Plasma Diagnostic, Plasma parameter
I. INTRODUCTION
Plasma can be described as ionized gas
consists of equal numbers positive ions and electrons.
Plasma is used by semiconductor and thin film
deposition industry for etching and material
processing. To develop new etch and deposition it is
necessary to understanding basic internal plasma
parameter. Langmuir probe is used to measure
critical plasma parameter helps minimize
development time and optimize plasma process for
desire application. Langmuir probe is one of the most
powerful diagnostic tool which is used to measure the
low temp plasma parameter. The ability to measure
local plasma parameter using Langmuir probe
making them superior than other diagnostic
techniques. Electrostatic Langmuir probe consists of
small metallic conductor that is inserted into plasma
to collect current. The biased voltage applied to probe
is varied and collect the current to probe to generate
I-V trace. From current voltage characteristics plasma
potential, floating potential, electron temperature,
electron density and electron energy distribution can
be obtained. Langmuir probe is vital diagnostic tool
because it can make local measurement. almost all
other techniques, such as spectroscopy or microwave
propagation, give information averaged over large
volume of plasma.[1] This paper present analysis of
plasma using LabVIEW software to extract
meaningful information from the Langmuir I-V trace.
II. EXPERIMENTAL SETUP
Vacuum chamber used for plasma analysis.
An inert background gas (argon) introduced into
chamber up to pressure 1.2 ×10-2
mbar. Langmuir
probe consists of metal electrode of 1mm area of
probe tip was made of SS covered by ceramic tube.
The electrical connection is provided by copper wire
which comes out through the vacuum compatible
BNC connector mounted on SS 304.The SS shaft was
introduced into vacuum chamber through the vacuum
feedthrough such that the probe could be positioned
at the desire locations inside the chamber. Langmuir
probe measure the current for the bias voltage range
from -80V to 30V. The amount of collected probe
current is depends on probe tip area and various
plasma parameter. The output current is measured by
isolation amplifier and applied voltage measured with
Tektronix oscilloscope. This data could be stored in
data storage device. This measurement data is used to
plot I-V characteristics to determine various plasma
parameter.[2] Schematic diagram of probe circuit
shown in fig.1
RESEARCH ARTICLE OPEN ACCESS
Bijal Vara et al Int. Journal of Engineering Research and Applications www.ijera.com
ISSN : 2248-9622, Vol. 4, Issue 3( Version 1), March 2014, pp.244-247
www.ijera.com 245 | P a g e
Fig1: Schematic diagram of Probe Circuit
III. RESULTS AND DISCUSSION
A typical Langmuir characteristic shown in
fig.2 is used to determine various plasma parameters.
LabVIEW is powerful Microsoft compatible software
that provides immediate data acquisition and
analysis. LabVIEW is programming language of
virtual instrument and that allow instrument control,
data acquisition and pre/post processing of data
analysis. LabVIEW program was written to partially
automate to determine various .Fig 3 shows the
LabVIEW front panel, which what the user will see.
The front panel illustrates all the plasma parameter,
all the plot. Floating potential is easiest parameter to
determine, the voltage at the probe collect no current.
From measured I-V data floating potential is -
10.97V.
-100 -80 -60 -40 -20 0 20 40
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
3.0
current
voltage
Fig 2:Typical Langmuir probe Characteristics
Ion saturation current is negative so to
measure the electron temperature and for the further
analysis it is necessary to subtract ion saturation
current from the total current .Isat is negative , but
Iprobe - Isat is almost positive.
Plasma potential can be measured by
different method and resultant value can be averaged.
First method is graphical method. In this method two
line, fitted to curve and intersection of two lines
indicate the plasma potential. From this tangent
method plasma potential is 1.9V. In ideal case plasma
potential corresponds to the maximum of the first
derivative and zero of the second derivative. By using
numerical calculation and differentiation we obtain
first and second derivative. In fig 3 first and
derivative is examined and plasma potential can be
calculated from the maxima in the 1st
derivative is
1.68V and from the zero of the second derivative is
also 1.68V.
Electron temperature can be obtained from
the slope of the logarithmic of electron current and
voltage curve in region between Vf and Vp. [3] by
equation.
(1)
Where I is electron current.
After obtaining electron temperature from the
logarithmic graph of current verses voltage, electron
density can be obtained from equation (2)
(2)
Electron Energy distribution function
(EEDF) is one of the most important property for
fusion and process plasma. As various properties of
plasma depends on different part of EEDF such as
diffusion coefficient depend on the bulk of the EEDF
and ionization or excitation rates depend on the tail of
the EEDF, the determination of the whole
distribution is compelling for a comprehensive
characterization of a plasma. [4]
Druyvesteyn method was derived specially for
EEDF. Particles in gas will have different velocity
and velocities of each particle will be changing due to
interaction with other particles. Electrons with
sufficient velocity component in direction of the
probe will be collected.[5]
(3)
Bijal Vara et al Int. Journal of Engineering Research and Applications www.ijera.com
ISSN : 2248-9622, Vol. 4, Issue 3( Version 1), March 2014, pp.244-247
www.ijera.com 246 | P a g e
Fig 3. LabVIEW Front Panel
Where,
Probe voltage is measured with respect to
ground, plasma is at plasma potential so it necessary
to express electron energy distribution with respect to
plasma potential. This makes plasma potential
reference energy level and the voltage V represents
electron energy relative to the plasma potential
reference.
EEDF is dependent only on the second derivative of
the probe characteristics. (Fig 3)[5]
(4)
Where, ,
Ap is area of the probe, m is electron mass, e is
electron charge, F( ) is Electron energy
distribution.
There are various smoothing techniques are
applied to simulated data and Te and ne are calculated
using Druyvesteyn method. Polynomial fitting for
smoothing data is less effective and it introduced
artificial oscillation. Here Gaussian curve fit method
is use for smoothing data. By comparing smoothed
data with original is used to determine what
information is lost during smoothing process.
[5]Electron temperature and electron number density
also obtained from Druyvesteyn method. Electron
density can be obtained by integral of f( ).
Electron temperature can be obtained from
integral of distribution function,[6]
Current voltage a characteristic of plasma is
obtained using argon gas.
IV. Conclusion
From Langmuir probe I-V data, various
plasma parameter like floating potential, plasma
potential, electron temperature, electron density and
electron energy distribution. Plasma potential is
essential for all analysis performed. By applying
v=Фp-Vp, the plasma potential becomes zero
reference point and EEDF is shifted on the horizontal
axis. So an error in plasma potential shifts the EEDF
and change on electron temperature and number
density.
REFERENCES
Journal Paper:
[1] Mohammed K. Khalaf, Nathera Abass Ali
Al-Tememee, Bahaa T. Chaid, Fwad T.
Ibrahim, Influence of Discharge Pressure on
the Plasma Parameter in a Planar Dc-
Sputtering Discharge of Argon,
International Journal of Recent Research
and Review, Vol. V, March 2013.
Theses:
[2] Satyananda kar, plasma response to
transient high voltage pulses, Doctor of
Bijal Vara et al Int. Journal of Engineering Research and Applications www.ijera.com
ISSN : 2248-9622, Vol. 4, Issue 3( Version 1), March 2014, pp.244-247
www.ijera.com 247 | P a g e
Philosophy, Institute for plasma research,
Gandhinagar.
Journal Papers:
[3] M. Nisha, K. J. Saji, R. S. Ajimsha, N. V.
Joshy, and M. K. Jayaraj, Characterization
of radio frequency plasma using Langmuir
probe and optical emission spectroscopy,
Journal of applied physics 99,
033304(2006).
[4] R Fichert,V Dose, Electron energy
distribution for reconstruction in low
pressure helium plasma from optical
measurement, plasma physics control.
Fusion 41(1999) 1109-1123.
Theses:
[5] Nicholas James Behlman, Electron energy
distribution measurements in the plume
region of a low current hollow
cathode,Degree of master of Science,
Worcester polytechnic institute.
Journal paper:
[6] B Crowley and S Dietrich, A Langmuir
probe system incorporating the Boyd-
Twiddy method for EEDF measurement
applied to an inductively coupled plasma
source, Plasma Source Science and
technology,2009.

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Langmuir Probe Diagnostic for Measuring Magnetized Plasma Parameters

  • 1. Bijal Vara et al Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 3( Version 1), March 2014, pp.244-247 www.ijera.com 244 | P a g e Langmuir probe Diagnostic for local parameter measurement in Magnetized Plasma using LabVIEW Bijal Vara1 , C S Dalal2 , S Karkari3 , H Kabariya4 1 (Department of instrumentation and control, Dharmsinh Desai University, Nadiad) 2 (Department of instrumentation and control, Dharmsinh Desai University, Nadiad) 3, 4 (Institute of Plasma research, Gandhinagar) ABSTRACT In recent years, plasma technology is used by Semiconductor, thin film industries for deposit layers, etching process and surface modification. So it is necessary to understanding internal plasma parameter. Langmuir probe is one of the simplest techniques which is used to measure wide range of plasma parameter like plasma potential, floating potential, electron temperature, electron energy distribution function (EEDF) etc. Langmuir current voltage characteristic is obtained by varying bias voltage of the probe. LabVIEW is most powerful Microsoft window compatible software which is used to immediate data acquisition and analysis. In this paper describes analysis of Langmuir data using LabVIEW software which automatically measure I-V Plasma probe Characteristics and obtain EEDF of plasma. Keywords – EEDF, LabVIEW, Langmuir probe, Plasma Diagnostic, Plasma parameter I. INTRODUCTION Plasma can be described as ionized gas consists of equal numbers positive ions and electrons. Plasma is used by semiconductor and thin film deposition industry for etching and material processing. To develop new etch and deposition it is necessary to understanding basic internal plasma parameter. Langmuir probe is used to measure critical plasma parameter helps minimize development time and optimize plasma process for desire application. Langmuir probe is one of the most powerful diagnostic tool which is used to measure the low temp plasma parameter. The ability to measure local plasma parameter using Langmuir probe making them superior than other diagnostic techniques. Electrostatic Langmuir probe consists of small metallic conductor that is inserted into plasma to collect current. The biased voltage applied to probe is varied and collect the current to probe to generate I-V trace. From current voltage characteristics plasma potential, floating potential, electron temperature, electron density and electron energy distribution can be obtained. Langmuir probe is vital diagnostic tool because it can make local measurement. almost all other techniques, such as spectroscopy or microwave propagation, give information averaged over large volume of plasma.[1] This paper present analysis of plasma using LabVIEW software to extract meaningful information from the Langmuir I-V trace. II. EXPERIMENTAL SETUP Vacuum chamber used for plasma analysis. An inert background gas (argon) introduced into chamber up to pressure 1.2 ×10-2 mbar. Langmuir probe consists of metal electrode of 1mm area of probe tip was made of SS covered by ceramic tube. The electrical connection is provided by copper wire which comes out through the vacuum compatible BNC connector mounted on SS 304.The SS shaft was introduced into vacuum chamber through the vacuum feedthrough such that the probe could be positioned at the desire locations inside the chamber. Langmuir probe measure the current for the bias voltage range from -80V to 30V. The amount of collected probe current is depends on probe tip area and various plasma parameter. The output current is measured by isolation amplifier and applied voltage measured with Tektronix oscilloscope. This data could be stored in data storage device. This measurement data is used to plot I-V characteristics to determine various plasma parameter.[2] Schematic diagram of probe circuit shown in fig.1 RESEARCH ARTICLE OPEN ACCESS
  • 2. Bijal Vara et al Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 3( Version 1), March 2014, pp.244-247 www.ijera.com 245 | P a g e Fig1: Schematic diagram of Probe Circuit III. RESULTS AND DISCUSSION A typical Langmuir characteristic shown in fig.2 is used to determine various plasma parameters. LabVIEW is powerful Microsoft compatible software that provides immediate data acquisition and analysis. LabVIEW is programming language of virtual instrument and that allow instrument control, data acquisition and pre/post processing of data analysis. LabVIEW program was written to partially automate to determine various .Fig 3 shows the LabVIEW front panel, which what the user will see. The front panel illustrates all the plasma parameter, all the plot. Floating potential is easiest parameter to determine, the voltage at the probe collect no current. From measured I-V data floating potential is - 10.97V. -100 -80 -60 -40 -20 0 20 40 -0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0 current voltage Fig 2:Typical Langmuir probe Characteristics Ion saturation current is negative so to measure the electron temperature and for the further analysis it is necessary to subtract ion saturation current from the total current .Isat is negative , but Iprobe - Isat is almost positive. Plasma potential can be measured by different method and resultant value can be averaged. First method is graphical method. In this method two line, fitted to curve and intersection of two lines indicate the plasma potential. From this tangent method plasma potential is 1.9V. In ideal case plasma potential corresponds to the maximum of the first derivative and zero of the second derivative. By using numerical calculation and differentiation we obtain first and second derivative. In fig 3 first and derivative is examined and plasma potential can be calculated from the maxima in the 1st derivative is 1.68V and from the zero of the second derivative is also 1.68V. Electron temperature can be obtained from the slope of the logarithmic of electron current and voltage curve in region between Vf and Vp. [3] by equation. (1) Where I is electron current. After obtaining electron temperature from the logarithmic graph of current verses voltage, electron density can be obtained from equation (2) (2) Electron Energy distribution function (EEDF) is one of the most important property for fusion and process plasma. As various properties of plasma depends on different part of EEDF such as diffusion coefficient depend on the bulk of the EEDF and ionization or excitation rates depend on the tail of the EEDF, the determination of the whole distribution is compelling for a comprehensive characterization of a plasma. [4] Druyvesteyn method was derived specially for EEDF. Particles in gas will have different velocity and velocities of each particle will be changing due to interaction with other particles. Electrons with sufficient velocity component in direction of the probe will be collected.[5] (3)
  • 3. Bijal Vara et al Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 3( Version 1), March 2014, pp.244-247 www.ijera.com 246 | P a g e Fig 3. LabVIEW Front Panel Where, Probe voltage is measured with respect to ground, plasma is at plasma potential so it necessary to express electron energy distribution with respect to plasma potential. This makes plasma potential reference energy level and the voltage V represents electron energy relative to the plasma potential reference. EEDF is dependent only on the second derivative of the probe characteristics. (Fig 3)[5] (4) Where, , Ap is area of the probe, m is electron mass, e is electron charge, F( ) is Electron energy distribution. There are various smoothing techniques are applied to simulated data and Te and ne are calculated using Druyvesteyn method. Polynomial fitting for smoothing data is less effective and it introduced artificial oscillation. Here Gaussian curve fit method is use for smoothing data. By comparing smoothed data with original is used to determine what information is lost during smoothing process. [5]Electron temperature and electron number density also obtained from Druyvesteyn method. Electron density can be obtained by integral of f( ). Electron temperature can be obtained from integral of distribution function,[6] Current voltage a characteristic of plasma is obtained using argon gas. IV. Conclusion From Langmuir probe I-V data, various plasma parameter like floating potential, plasma potential, electron temperature, electron density and electron energy distribution. Plasma potential is essential for all analysis performed. By applying v=Фp-Vp, the plasma potential becomes zero reference point and EEDF is shifted on the horizontal axis. So an error in plasma potential shifts the EEDF and change on electron temperature and number density. REFERENCES Journal Paper: [1] Mohammed K. Khalaf, Nathera Abass Ali Al-Tememee, Bahaa T. Chaid, Fwad T. Ibrahim, Influence of Discharge Pressure on the Plasma Parameter in a Planar Dc- Sputtering Discharge of Argon, International Journal of Recent Research and Review, Vol. V, March 2013. Theses: [2] Satyananda kar, plasma response to transient high voltage pulses, Doctor of
  • 4. Bijal Vara et al Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 3( Version 1), March 2014, pp.244-247 www.ijera.com 247 | P a g e Philosophy, Institute for plasma research, Gandhinagar. Journal Papers: [3] M. Nisha, K. J. Saji, R. S. Ajimsha, N. V. Joshy, and M. K. Jayaraj, Characterization of radio frequency plasma using Langmuir probe and optical emission spectroscopy, Journal of applied physics 99, 033304(2006). [4] R Fichert,V Dose, Electron energy distribution for reconstruction in low pressure helium plasma from optical measurement, plasma physics control. Fusion 41(1999) 1109-1123. Theses: [5] Nicholas James Behlman, Electron energy distribution measurements in the plume region of a low current hollow cathode,Degree of master of Science, Worcester polytechnic institute. Journal paper: [6] B Crowley and S Dietrich, A Langmuir probe system incorporating the Boyd- Twiddy method for EEDF measurement applied to an inductively coupled plasma source, Plasma Source Science and technology,2009.