SYSTEM AND METHOD FOR REMOTE SENSING A PLASMA

Abstract

The invention provides a method and system to remotely monitor a plasma (3) comprising a magnetic field antenna (2) positioned in the near electromagnetic field of a coupled plasma source wherein the magnetic field antenna is a magnetic loop antenna placed in the near electromagnetic field and measure near field signals emitted from the plasma source. A radio system (1) is utilised to analyse the low power signal levels across a wide frequency band. Plasma paramaters such as series, or geometric, resonance plasma and electron-neutral collision frequencies are evaluated via a fitting of resonant features present on higher harmonics of the driving frequency to identify arcing, pump or matching failure events, common in fabrication plasma systems.

Claims

1. A system to remotely monitor a plasma comprising: an electromagnetic antenna positioned in the near electromagnetic field of a coupled plasma source wherein the electromagnetic antenna is placed in the near electromagnetic field and adapted to measure near field signals emitted from the plasma source, wherein the near field signals comprises near H field signals or near E field signals.

2. The system of claim 1 wherein a magnetic loop antenna is coupled to the plasma source and the system is adapted to analyse near-field radio emissions of the plasma source using a radio emission spectroscopy (RES).

3. (canceled)

4. The system of claim 1 wherein the near H field signal intensity drops with distance as a function of distance from the antenna and the plasma source.

5. The system of claim 4 wherein the signal intensity drops with distance as a function of 1/r.sup.3 where r is the distance from the antenna and the plasma source.

6. The system of 1 comprising a module to perform a frequency analysis of the fundamental drive frequencies and higher harmonics and RF intermixing products present in the near field signal to provide a resonance behaviour dependent to plasma parameters of the plasma source and outputting a condition of the plasma source based on said analysis.

7. The system of claim 6 wherein the frequency analysis is performed for different operating pressures.

8. The system of claim 1 comprising a module to remove noise of from the signal by an on-line background subtraction selected at a suitable point away from the near field.

9. The system of claim 1 wherein the antenna is calibrated to enable a calculation of a frequency dependent coupling factor between a current associated with the plasma and an induced antenna signal.

10. The system of claim 1 wherein a radio system is configured to analyse low power signal levels across a wide frequency band.

11. The system of claim 10 wherein the signal is localised to a proximity of a viewport to enable signal isolation to the plasma source.

12. The system of claim 10 wherein a measured resonance plasma frequency and an electron-neutral collision frequency are correlated via a fitting of resonant features present on higher harmonics of a driving frequency.

13. (canceled)

14. (canceled)

15. (canceled)

16. The system of claim 1 comprising a module to perform a frequency analysis of higher harmonics present in the near H field signals and E field signals to provide a resonance behaviour dependent to plasma parameters of the plasma source.

17. A method to remotely monitor a plasma comprising the steps of: positioning an electromagnetic magnetic field antenna coupled plasma source wherein the antenna placed in the near electromagnetic field; and measuring near field signals emitted from the plasma source, wherein the near field signals comprises near H field signals or near E field signals.

18. The method of claim 17 comprising the steps of measuring a resonance plasma frequency and an electron-neutral collision frequency; and correlating said frequency measurements via a fitting of resonant features present on higher harmonics of a driving frequency.

19. The system of claim 1 comprising a first antenna to measure near H field signals and a second antenna to measure near E field signals.

20. The system as claimed in claim 1, further comprising a device for measuring an optical emission from the plasma source.

21. The system as claimed in claim 20 wherein the device comprises an optical spectrometer.

22. The device as claimed in claim 20 wherein the optical emission measurement comprises one or more of the following: a measurement of plasma ashing of a photoresist coated wafer or other coating; measurement of endpointing of a plasma etch process; a measurement of plasma-based deposition; a measurement of chamber cleanliness; a measurement of contamination or leaks; a measurement of chamber matching.

23. The system of claim 12 wherein the correlation provides a factor to identify one or more of the following: arcing, pump or matching failure events, associated with the plasma source.

24. The method of claim 17 wherein, a first antenna measures the near H field signals and a second antenna measures the near E field signals.

25. The method of claim 17 wherein, measuring an optical emission from the plasma source.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0038] The invention will be more clearly understood from the following description of an embodiment thereof, given by way of example only, with reference to the accompanying drawings, in which:

[0039] FIG. 1 illustrates a system to remotely monitor a low pressure non-equilibrium plasma according to one embodiment of the invention;

[0040] FIG. 2 illustrates (a) Distance dependence (r in FIG. 1) of induced radio signal I.sub.RES. (b) Comparison of I.sub.RES with the bulk plasma current I.sub.bulk.

[0041] (c) Electron density values in centre of discharge using Langmuir probe.

[0042] (d) Resistive component (IR) of the total current measured by an in-line I-V probe;

[0043] FIG. 3 illustrates a correlation of antenna signal with an in-line current measurement of the plasma using an I-V probe;

[0044] FIG. 4 illustrates the radio emission intercepted (see FIG. 1) for the first three harmonics of driving frequency (13.56 MHz) for an O2 plasma;

[0045] FIG. 5 illustrates near field signal frequency analysis: resonance behaviour found in higher harmonics; and

[0046] FIG. 6 illustrates extracted values of the series resonance (ω.sub.g) and electron-neutral collision frequencies (v) from harmonic resonance peaks shown in FIG. 5.

DETAILED DESCRIPTION OF THE DRAWINGS

[0047] FIG. 1 illustrates a system to remotely monitor a low pressure non-equilibrium plasma according to one embodiment of the invention indicated by the reference numeral 1. At least one magnetic field antenna 2 is positioned in the near field of a capacitively coupled plasma source 3. It will be appreciated that the system is applicable to any plasma source, be it capacitively or inductively coupled, or a plasma induced by laser heating or other means. Magnetic flux from plasma currents, present in the vicinity of a viewport 4, is coupled via a calibrated loop antenna 2. The system 1 can be embodied as a radio system (spectrum analyser) and utilised to analyse the low power signal levels across a wide frequency band. The signal is localised to the proximity of a viewport, enabling signal isolation to the nearby plasma source. Series (or geometric) resonance plasma and electron-neutral collision frequencies are evaluated via a fitting of resonant features present on higher harmonics of the driving frequency, as described in more detail below.

[0048] To date, however, the monitoring of wavelengths emitted in the radio frequency portion of the electromagnetic spectrum from low temperature plasma sources remains unexploited. The present invention provides a system and a method for the measurement and analysis of near-field radio emissions near a low pressure non-equilibrium plasma using a concept hereinafter referred to as radio emission spectroscopy (RES). As illustrated in FIG. 1 a near-field loop antenna 2 (typical diameter ˜5-25 mm) intercepts the magnetic flux resulting from currents in proximity to a viewport 4 in the plasma chamber. The loop plane is orientated perpendicular to the viewport 4 to intercept currents transiting between the electrodes. A shielded loop antenna design, often used for magnetic field sensing in electromagnetic interference testing, can be employed here. The spatial behaviour of the magnetic field (strictly magnetostatic field) surrounding plasma currents flowing in proximity to the viewport is given by application of the Biot-Savart law:

[00001]$B\left(r\right)=\frac{{\mu }_0}{4\pi }\int \int {\int }_V\frac{\left(\mathrm{JdV}\right)\times r}{{.Math.r.Math.}^3}$ [0049] where dV is the volume element for current density J, and r represents the separation between the current volume and antenna position r.

[0050] An important aspect of the invention is the fact that measured currents or voltages in the near field fall off is approximately 1/r.sup.3, indicating near field operation. If the signals fall off as 1/r.sup.2, or similar, then they are not listening to the near field. This is illustrated in FIG. 2 where there is shown in (a) Distance dependence (r in FIG. 1) of induced radio signal I.sub.RES. (b) Comparison of I.sub.RES with the bulk plasma current I.sub.bulk. (c) Electron density values in centre of discharge using Langmuir probe. (d) Resistive component (IR) of the total current measured by an in-line I-V probe.

[0051] In the context of the present invention the plasma chamber 5 acts as a radiation source emitting electromagnetic radiation into its environs. The antenna system 2 is positioned in the ‘near’ portion of this radiation field. This is evidenced by observation of the signal intensity drop with distance as 1/r.sup.3. In this scenario multi-pole characteristics of the emitting element (i.e. plasma) dominant the positional dependence of the field intensity. Extension of the Bio-Savart formulation to include dipole contributions of the emitting current leads to such a 1/r.sup.3 dependence.

[0052] This behaviour is typical of antenna operation within the near field of a radiation zone sufficiently remote from an emitter and in contrast to probing within a source where spatial variations deviate from such 1/r.sup.3 behaviour. Indeed, this fact is widely exploited in near field communication systems to enable a remote (‘contact-less’) but localised coupling to a radiation source.

[0053] The ability to localize an emitted radio signal from a plasma 3 by a near-field (magnetic loop) antenna 2 is essential for operation of the invention. This resolution ensures that emissions from nearby sources are effectively minimized as the antenna is sensitive to the H-field near the plasma viewport (or alternatively any other non-conductive surface bounding the plasma).

[0054] The localized nature of the radio emission spectroscopy (RES) signal corroborates the source of the emission as the plasma 3 over any far-field radiation sources that likely includes emissions from nearby plasma chambers, the power unit, the match box, other sections of the transmission line, and ambient radio signals. Noise can also be easily removed from the signal in this scenario by an on-line background subtraction at a suitable point away from the near field, as illustrated in FIG. 2a. In other words the invention provides a practical method for signal extraction and is particularly advantageous for implementation in “radio-noisy” fabrication environments.

[0055] The system 1 can provide a module to perform a frequency analysis of higher harmonics present in the near field signal to provide a resonance behaviour dependent to plasma parameters of the plasma source, as referenced below with respect to FIGS. 3 to 6. The system can output a condition of the plasma source based on said analysis to inform a user that the plasma is operating correctly.

[0056] In operation, the near field loop antenna 2 intercepts the magnetic flux resulting from (displacement) currents transiting between the electrodes in proximity to the viewport. The loop antenna 2 can consists of a flat metal inner conductor coated in a non-conductive shielding blocking electric fields. The antenna can be calibrated using a 50 Ohm micro-strip transmission line and a vector network analyser using a technique commonly employed for electromagnetic compatibility testing in adherence to International Electrotechnical Commission (IEC) directives. It will be appreciated that numerous calibration techniques can be used for example using calibration files provided by RF Explorer (http://j3.rf-explorer.com/downloads) or using a calibration using Helmholtz coils as provided by Beehive Electronics (see for example—https://beehive-electronics.com/datasheets/100SeriesDatasheetCurrent.pdf).

[0057] Calibration enables the calculation of a frequency dependent coupling factor between the (circuit/plasma) current and the induced antenna signal. Low level signals are analysed using a spectrum analyser with a high dynamic range and resolution bandwidth set <100 Hz. A background scan can be performed at a distance sufficiently remote from the plasma (i.e. where the near field signal is lost), as illustrated in FIG. 1 and subtracted from the near field signal to isolate frequencies intercepted from the plasma. The plasma source used here is a Plasma Lab 100 etching system from Oxford Instruments, as provided by Oxford Instruments Ltd. http://www.oxfordplasma.de/systems/100ll.htm. Oxford Instruments Plasma Lab 100.

[0058] The voltage induced in the loop antenna from magnetic fields resulting from plasma currents (I) is based on Faraday's induction principle and can be given by the following:

[00002]$\begin{array}{cc}{V}_{\mathrm{loop}}=k\frac{\partial I}{\partial t}\mathrm{and}{V}_{\mathrm{Loop}}\left(\omega \right)=I\left(\omega \right)+k\left(\omega \right)& \left(1\right)\end{array}$

[0059] where k(ω) represents a frequency dependent coupling factor according to Faraday's induction principle. A correlation of the induced signal with an in-line current measurement (captured with an I-V probe stationed between the matchbox and the powered electrode) is shown in FIG. 3. It was found from a frequency analysis of the higher harmonics present in the near-field signal at lower operating pressures showed resonance behaviour that is linked to fundamental plasma parameters. Extraction of the series (or geometric) plasma and electron—neutral collision frequencies is demonstrated for an oxygen plasma. FIG. 3 illustrates the correlation of antenna signal with an in-line current measurement of the plasma using an I-V probe.

[0060] The signal is dominated by frequencies near the driving frequency (13.56 MHz). FIG. 3 shows this signal as an effective proxy for monitoring current variations in the plasma. The monitored current variations have utility as a contact-less sensor for monitoring arcing, pump or matching failure events in fabrication equipment and in endpoint detection where optical diagnostic are limited (e.g. due to window coating).

[0061] FIG. 4 illustrates the radio emission intercepted (see FIG. 1) for the first three harmonics of driving frequency (13.56 MHz) for an O2 plasma ashing of a photo-resist coated wafer. Measurements of the oxygen 777 nm line intensity are carried out using an optical spectrometer. Endpoint (total removal of photo-resist) occurs as the line intensity plateaus (500 seconds in FIG. 2). Monitoring near field radio emission ‘Radio Emission Spectroscopy’ or RES, according to the invention, is found to be an effective indicator for endpoint here.

[0062] The plasma current in capacitively coupled plasma (CCP) discharges is dominated by displacement current I=I.sub.D=∂D/∂t=∂(ε.sub.pE)/∂t. For a single frequency CCP the frequency content of I.sub.D is dominated by harmonics of the driving frequency (13.56 MHz), however, at lower pressures power is increasingly coupled to higher harmonics which display a distinct resonance behaviour.

[0063] One can consider a circuit model of a capacitively coupled plasma with asymmetric sheaths dominated by a single large ‘high voltage sheath’ present at the powered electrode. This is a common arrangement in industrial plasma etchers. In this model the plasma consists of a capacitive sheath in series with an inductive bulk plasma. The frequency dependence of the total electrical permittivity (ε.sub.p) at harmonics of the driving frequency ω which are larger than the electron-neutral collision frequency v (i.e. ω>>v) can be given by.

[00003]$\begin{array}{cc}{\epsilon }_p={\epsilon }_0\left(\frac{1}{s}+\frac{\left(1-{\omega }_p^2/{\omega }^2\right)}{1-s}\right)& \left(2\right)\end{array}$

[0064] Here s, the sheath width is normalised to the gap width (0<s<1) and ω.sub.p is the plasma frequency.

[0065] Equation 2 has a minimum for ω=√{square root over (sω.sub.p)} corresponding to the well-known series (or geometric) resonance frequency ω=ω.sub.g. As the sheath width oscillates over the applied voltage cycle, ω.sub.g varies in the interval s.sub.min to s.sub.max (approximating a fixed w bulk plasma density). Resonance behaviour in the signals higher harmonics is shown in FIG. 4 for an oxygen plasma. Emission is found to occur primarily around narrow emission bands (≈Δ100 Hz) located at harmonics of the source driving frequency (13.56 MHz). The occurrence of the two primary resonances is found here. This is attributed to the sheath variation over the applied voltage cycle which ranges from s.sub.min to s.sub.max. The acceleration of the Electric field (which is proportional to the induced antenna voltage) coincides with the occurrence of s.sub.min and s.sub.max enhancing the two primary resonances shown in FIG. 5. Damping of the series resonance is due to the electron-neutral collisions given by the frequency v and is constrained in the upward direction by the driving frequency ω (i.e. v>13.56 MHz).

[0066] A Gaussian distribution is fitted to the upper resonance peaks shown in FIG. 4. The geometric (ω.sub.g) and electron-neutral collision (v) frequencies are given by the fitted mean (ω.sub.g=μ) and Full Width at Half Maximum (FWHM) v≈2.355σ shown in FIG. 5. The maximum sheath width is estimated here as 0.23 or 23% of the discharge gap and is found to be approximately static across the power range of interest. This estimation is achieved by employment of the Child sheath law coupled with a combination of Langmuir probe measurements for electron density and temperature and I-V measurements for estimation of the sheath voltage.

[0067] The plasma density can now be calculated using the relation ω.sub.p=ω.sub.g/√{square root over (s)}. The value of 1/√{square root over (s)} is ≈2 here, giving an electron plasma frequency ranging from 575 MHz at 200 W applied power to 653 MHz at 500 W. This compares to Langmuir probe measurements (preformed at the discharge centre) which range from 913 MHz at 200 W to 1.3 GHz at 500 W. The discrepancy in plasma frequency values is due to the lower electron density expected at the chamber wall versus the discharge center which is typically at least an order of magnitude higher. A calibration ratio of ≈4 between the Langmuir probe plasma frequency data taken at the discharge center and the extracted near field geometric plasma frequency across our power range is found here, corroborating a correlative trend.

[0068] FIG. 6 illustrates extracted values of the series resonance (ω.sub.g) and electron-neutral collision frequencies (v) from harmonic resonance peaks shown in FIG. 5. Investigations of the radiated (far field) radio signal were also carried out. Results showed a more limited diagnostic potential and insensitivity to the plasma parameters. Frequency analysis revealed harmonic peaking at wavelengths of ˜0.5-1 meters across a range of applied powers. This insensitivity likely reflects some physical aspect of the transmission line (e.g. chamber diameter) rather than correlation to any plasma parameter.

[0069] A mentioned previously the ability to localise the emitted radio signal from the plasma via a near field (magnetic loop) antenna is important for the operation of the invention. This resolution ensures emissions from nearby sources are effectively minimised as the antenna is sensitive to the H field in the vicinity of the plasma viewport (or alternatively any other non-conductive surface bounding the plasma). This behaviour corroborates the source of the emission as the plasma over far field radiation which likely includes emissions from nearby plasma chambers, the power unit, match box, other sections of the transmission line and ambient radio signals, as illustrated in FIG. 2. Noise can also be easily removed from the signal by an on-line background subtraction at a suitable point away from the near field, as illustrated in FIG. 1.

[0070] Suitably the system can comprise a first antenna to measure near H field signals and a second antenna to measure near E field signals. The module can perform a frequency analysis of higher harmonics present in the near H field signals and E field signals to provide a resonance behaviour dependent to plasma parameters of the plasma source.

[0071] This provides a practical method for signal extraction and is particularly advantageous for implementation in ‘radio-noisy’ fabrication environments.

[0072] The embodiments in the invention described with reference to the drawings comprise a computer apparatus and/or processes performed in a computer apparatus. However, the invention also extends to computer programs, particularly computer programs stored on or in a carrier adapted to bring the invention into practice. For example, recent advances in microprocessor technology have enabled the emergence of “software defined radio” (SDR) in which traditional radio hardware components have been implemented in software. This has led to recent advances in the flexibility and availability of SDR signal acquisition and spectrum analyzer technologies using program software. The program may be in the form of source code, object code, or a code intermediate source and object code, such as in partially compiled form or in any other form suitable for use in the implementation of the method according to the invention. The carrier may comprise a storage medium such as ROM, e.g. CD ROM, or magnetic recording medium, e.g. a memory stick or hard disk. The carrier may be an electrical or optical signal which may be transmitted via an electrical or an optical cable or by radio or other means.

[0073] In the specification the terms “comprise, comprises, comprised and comprising” or any variation thereof and the terms “include, includes, included and including” or any variation thereof are considered to be totally interchangeable and they should all be afforded the widest possible interpretation and vice versa.

[0074] The invention is not limited to the embodiments hereinbefore described but may be varied in both construction and detail.