CN106413237A - Plasma diagnostic method of multi-amplitude AC bias probe based on data acquisition card - Google Patents
Plasma diagnostic method of multi-amplitude AC bias probe based on data acquisition card Download PDFInfo
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- CN106413237A CN106413237A CN201610925891.0A CN201610925891A CN106413237A CN 106413237 A CN106413237 A CN 106413237A CN 201610925891 A CN201610925891 A CN 201610925891A CN 106413237 A CN106413237 A CN 106413237A
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- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/0006—Investigating plasma, e.g. measuring the degree of ionisation or the electron temperature
- H05H1/0081—Investigating plasma, e.g. measuring the degree of ionisation or the electron temperature by electric means
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Abstract
The invention belongs to the technical field of plasma, and discloses a plasma diagnostic method of a multi-amplitude AC bias probe based on a data acquisition card. The plasma diagnostic method comprises the steps of: generating AC bias signals based on the data acquisition card, driving the signals via a power amplifier, and applying the signals to a probe in plasma through a sampling resistor, meanwhile, acquiring a voltage signal on the sampling resistor by means of a differential simulation input port of the data acquisition card commanded by a computer, sending the voltage signal to the computer, and converting the voltage signal into a current signal by the computer; and carrying out spectral analysis and least square method fitting, and further calculating to obtain an accurate electronic temperature value and an accurate ion density value. The plasma diagnostic method solves the problem that electronic temperature and ion density measured by adopting the existing fixed-amplitude AC bias probe diagnostic technique are inaccurate, can diagnose the plasma especially insulating deposition environment plasma, can automatically complete the plasma diagnosis process, and output the accurate electronic temperature and ion density values.
Description
Technical field
The invention belongs to technical field of plasma, it is related to a kind of many amplitude AC biasing spies based on data collecting card
Pin plasma diagnostic method, for diagnosing plasma, particularly insulate depositional environment plasma, obtain electron temperature and
Ion concentration.
Background technology
Existing probe technique is used for diagnosing plasma parameter, has polytype.The most frequently used Single probe is one
Little metal electrode is that probe is placed in plasma, adds scanning bias voltage between probe and plasma ground electrode,
Then measurement probe current, with the change of scanning bias voltage, obtains VA characteristic curve, then by analyzing VA characteristic curve
Obtain the parameter of plasma.In addition also have double types such as probe, three probes, a something in common of these probe techniques
It is to be required on probe plus DC offset voltage, and the problem that this is brought is:When having in the plasma environment being diagnosed
When insulation deposition occurs, detecting probe surface can deposited material cover, thus losing electric conductivity and cannot working.
The prior art that solves the above problems is to produce a fixed amplitude V with signal generator0AC bias electricity
Pressure is added on probe, measures probe current signal, then using spectrum analyzer, probe current signal is analyzed, obtains
First harmonic amplitude i1ωWith second-harmonic amplitude i2ω, then use formula i1ω/i2ω=I1(eV0/T*)/I2(eV0/ T*) calculate
T* is as electron temperature, then uses formulaCalculate n* as ion concentration, on
In the formula of face two, e is electron charge, I0(eV0/T*)、I1(eV0/ T*) and I2(eV0/ T*) it is eV respectively0The zeroth order of/T*, single order
With second order Bessel function of imaginary argument, A and M is that detecting probe surface amasss and mass of ion respectively.Because alternating current can be with displacement
The form of electric current passes through the insulating barrier of detecting probe surface, even if this technology is in the case that detecting probe surface is covered by megohmite insulant
Can be using it is thus possible to the plasma of diagnosing insulation depositional environment.
But T* and n* that above-mentioned prior art obtains not is accurate electron temperature and ion concentration.This is because on
Its theoretical foundation of diagnostic techniquess stating existing fixed amplitude AC bias probe is infinity plane electrode model it is assumed that electric current
Signal amplitude is unrelated with the amplitude of AC bias potential, and actually used probe is all very little it is impossible to regard infinitely great as
Plane electrode, current signal amplitude is relevant with the amplitude of AC bias potential.This makes the electricity obtaining using prior art
Sub- temperature and ion concentration numerical value change with the change of selected AC bias potential amplitude, and existing fixed amplitude exchange is partially
The diagnostic techniquess putting probe can not accurately obtain electron temperature value and the density value of plasma.
On the other hand, the diagnostic techniquess of existing fixed amplitude AC bias probe utilize signal generator and spectrum analyses
Instrument is it is impossible to be automatically performed plasma diagnostics process, output result.
Content of the invention
The present invention provides a kind of many amplitude AC bias probe plasma diagnostic method based on data collecting card, to solve
The certainly diagnostic techniquess measurement electron temperature of existing fixed amplitude AC bias probe and the inaccurate problem of ion concentration, and energy
Enough it is automatically performed plasma diagnostics process, export accurate electron temperature value and density value.
The technical scheme is that:
A the simulation output port of () computer instruction data collecting card gradually produces amplitude and is respectively V=Vj(j=1,
2 ...) AC bias signal, drive through power amplifier, then be added in, through sample resistance, the probe being placed in plasma
On, meanwhile, the voltage signal that the difference analogue input port of computer instruction data collecting card gathers on sample resistance sends into meter
Calculation machine, and current signal is converted into by computer.
B () computer is to each amplitude AC bias voltage V=VjProbe current signal under (j=1,2 ...) is carried out
Spectrum analyses, obtain first harmonic amplitude i1ωj(j=1,2 ...) and second-harmonic amplitude i2ωj(j=1,2 ...) and calculate
Go out their ratio Pj=i1ωj/i2ωj(j=1,2 ...).
C () computer is to data point (Pj,Vj) (j=1,2 ...) in order to T for variable function I1(eVj/T)/I2(eVj/
T (wherein e is electron charge, I) to carry out least square fitting1(eVj/ T) and I2(eVj/ T) it is eV respectivelyjThe single order of/T and two
Rank Bessel function of imaginary argument), output meets the T value T=T of least square fittinge, TeIt is accurate electron temperature value.
D () computer utilizes Vj(j=1,2 ...), i1ωj(j=1,2 ...) and TeData substitutes into formulaIt is calculated nj(j=1,2 ...), in formula, A and M is that detecting probe surface amasss respectively
And mass of ion, I0(eVj/Te) it is eVj/TeZeroth order Bessel function of imaginary argument, then to data point (nj,Vj) (j=1,
2 ...) carry out Linear Quasi merging continuation to V=0, export value n in V=0 for the fitting a straight line0, n0It is accurate ion concentration
Value.
The invention has the beneficial effects as follows:
Plasma can be diagnosed particularly insulate depositional environment plasma, be automatically performed plasma diagnostics process,
Export accurate electron temperature value and density value.
Brief description
Fig. 1 is the schematic diagram diagnosing plasma using the inventive method.
Fig. 2 is the data point (P being obtained using the inventive methodj,Vj) (j=1,2 ...) and use function I1(eVj/T)/I2
(eVj/ T) it is carried out with the result of least square fitting, and the data point (n being obtained using the inventive methodj,Vj) (j=
1,2 ...) and it is carried out with Linear Quasi merging continuation to the result of V=0.
In figure:1 probe;2 argon plasmas;3 computers;4 director data capture cards;5 simulation output ports;6 power are put
Big device;7 sample resistances;8 difference analogue input ports.
Specific embodiment
Describe the specific embodiment of the present invention with reference to technical scheme and accompanying drawing in detail.
In FIG, probe 1 be an area be 0.15cm2Tinsel, be placed in argon plasma 2.Computer 3 refers to
The simulation output port 5 making data collecting card 4 gradually produces amplitude and is respectively V=VjThe AC bias letter of (j=1,2 ...)
Number, drive through power amplifier 6, then be added on the probe 1 being placed in plasma 2 through sample resistance 7, meanwhile, computer 3
The voltage signal that the difference analogue input port 8 of director data capture card 4 gathers on sample resistance 7 sends into computer 3, by calculating
Machine 3 is converted into current signal.
In Fig. 2, Pj=i1ωj/i2ωj(j=1,2 ...) it is computer 3 to each amplitude AC bias voltage V=Vj(j=
1,2 ...) under probe current signal carry out the first harmonic amplitude i that spectrum analyses obtain1ωj(j=1,2 ...) and secondary humorous
Wave-amplitude i2ωjThe ratio of (j=1,2 ...).Each PjWith corresponding VjConstitute data point (Pj,Vj) (j=1,2 ...) use labelling
"○" represents in figure.
Computer 3 is to data point (Pj,Vj) (j=1,2 ...) in order to T for variable function I1(eVj/T)/I2(eVj/T)
(wherein e is electron charge, I to carry out least square fitting1(eVj/ T) and I2(eVj/ T) it is eV respectivelyjThe single order of/T and second order
Bessel function of imaginary argument).Function I as T=2.35eV1(eVj/T)/I2(eVj/ T) (solid-line curve in Fig. 2) meet right
Data point (Pj,Vj) (j=1,2 ...) least square fitting, export Te=2.35eV is accurate electron temperature value.
In fig. 2, nj(j=1,2 ...) it is that computer utilizes Vj(j=1,2 ...), i1ωj(j=1,2 ...) data
And Te=2.35eV substitutes into formulaResult (the A=0.15cm in formula calculating2It is
Detecting probe surface amasss and M=6.68 × 10-26Kg is argon ion quality).Each njWith corresponding VjConstitute data point (nj,Vj) (j=1,
2 ...) represented in figure with labelling " Δ ".
Computer is to data point (nj,Vj) (j=1,2 ...) (in Fig. 2, void is straight to V=0 to carry out Linear Quasi merging continuation
Line), fitting a straight line is in value n of V=00=9.1 × 109cm-3, export n0=9.1 × 109cm-3For accurate density value.
Claims (1)
1. a kind of many amplitude AC bias probe plasma diagnostic method based on data collecting card is it is characterised in that include
Following steps:
A the simulation output port of the data collecting card of () computer instruction gradually produces amplitude and is respectively V=Vj(j=1,2 ...)
AC bias signal, drive through power amplifier, then be added on the probe being placed in plasma through sample resistance, with
When, the voltage signal that the difference analogue input port of the data collecting card of computer instruction gathers on sample resistance sends into calculating
Machine, and current signal is converted into by computer;
B () computer is to each amplitude AC bias voltage V=VjProbe current signal under (j=1,2 ...) carries out frequency spectrum and divides
Analysis, obtains first harmonic amplitude i1ωj(j=1,2 ...) and second-harmonic amplitude i2ωj(j=1,2 ...) and calculate the two
Ratio Pj=i1ωj/i2ωj(j=1,2 ...);
C () computer is to data point (Pj,Vj) (j=1,2 ...) in order to T for variable function I1(eVj/T)/I2(eVj/ T) enter
Row least square fitting, wherein e are electron charges, I1(eVj/ T) and I2(eVj/ T) it is eV respectivelyjThe single order of/T and second order are empty
Argument Bessel function, output meets the T value T=T of least square fittinge, TeIt is accurate electron temperature value;
D () computer utilizes Vj(j=1,2 ...), i1ωj(j=1,2 ...) and TeData substitutes into formulaIt is calculated nj(j=1,2 ...), in formula, A and M is that detecting probe surface amasss respectively
And mass of ion, I0(eVj/Te) it is eVj/TeZeroth order Bessel function of imaginary argument, then to data point (nj,Vj) (j=1,
2 ...) carry out Linear Quasi merging continuation to V=0, export value n in V=0 for the fitting a straight line0, n0It is accurate ion concentration
Value.
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Cited By (6)
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CN105704900A (en) * | 2016-04-19 | 2016-06-22 | 陈兆权 | Positive and negative amplitude-modulation pulse driven electrostatic probe and data acquisition and analysis integrated device |
CN106851953A (en) * | 2017-02-22 | 2017-06-13 | 大连理工大学 | A kind of convex-concave probe and its plasma diagnostic method |
CN106888543A (en) * | 2017-03-24 | 2017-06-23 | 大连理工常州研究院有限公司 | A kind of automatically scanning emitting probe device |
CN108667506A (en) * | 2018-04-26 | 2018-10-16 | 北京空间飞行器总体设计部 | A kind of satellite electric propulsion system, which modulates signal of communication, influences test system and method |
CN110740558A (en) * | 2019-10-18 | 2020-01-31 | 南昌大学 | method for measuring plasma electron non- time delay parameter |
CN112888128A (en) * | 2021-01-18 | 2021-06-01 | 南昌大学 | Method for measuring plasma ion non-extensive parameter |
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Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105704900A (en) * | 2016-04-19 | 2016-06-22 | 陈兆权 | Positive and negative amplitude-modulation pulse driven electrostatic probe and data acquisition and analysis integrated device |
CN106851953A (en) * | 2017-02-22 | 2017-06-13 | 大连理工大学 | A kind of convex-concave probe and its plasma diagnostic method |
CN106851953B (en) * | 2017-02-22 | 2018-12-21 | 大连理工大学 | A kind of convex-concave probe and its plasma diagnostic method |
CN106888543A (en) * | 2017-03-24 | 2017-06-23 | 大连理工常州研究院有限公司 | A kind of automatically scanning emitting probe device |
CN106888543B (en) * | 2017-03-24 | 2019-04-16 | 大连理工常州研究院有限公司 | A kind of automatically scanning emitting probe device |
CN108667506A (en) * | 2018-04-26 | 2018-10-16 | 北京空间飞行器总体设计部 | A kind of satellite electric propulsion system, which modulates signal of communication, influences test system and method |
CN108667506B (en) * | 2018-04-26 | 2020-11-20 | 北京空间飞行器总体设计部 | System and method for testing influence of satellite electric propulsion system on communication signal modulation |
CN110740558A (en) * | 2019-10-18 | 2020-01-31 | 南昌大学 | method for measuring plasma electron non- time delay parameter |
WO2021073056A1 (en) * | 2019-10-18 | 2021-04-22 | 南昌大学 | Method for measuring plasma electron non-extensive parameter |
CN112888128A (en) * | 2021-01-18 | 2021-06-01 | 南昌大学 | Method for measuring plasma ion non-extensive parameter |
WO2022151982A1 (en) * | 2021-01-18 | 2022-07-21 | 南昌大学 | Method for measuring plasma ion non-extensive parameter |
CN112888128B (en) * | 2021-01-18 | 2023-04-07 | 南昌大学 | Method for measuring plasma ion non-extensive parameter |
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Application publication date: 20170215 |