Hiden EQP Applications Mass/Energy Analyser for Plasma Diagnostics and Characterisation
EQP Overview The Hiden EQP System is an advanced plasma diagnostic tool with combined high transmission ion energy analyser and quadrupole mass spectrometer, acquiring both mass spectra at specified ion energies and ion energy distributions of selected plasma ions. The advanced EQP ioniser allows neutral and radical detection, the electron attachment ionisation feature further enhancing the detection capability for radicals in electronegative plasma chemistries.
The NIST GEC Test Cell Sheath regions Vp a b Ions rf Vb Plasma (capacitively coupled)
6 5 41 amu ArH + 3 4 amu Ar + 4 3 rf pk/pk 25 2 2 1 19v 15 1 5-18 18 36 54 72 9-18 18 36 54 72 9 1 2 8 15 NIST GEC Example 6 4 2 48v 1 5 Energy Spectra -18 15 18 36 54 72 9-18 3 25 18 36 54 72 9 1 2 5 76v 15 1 5-18 18 36 54 72 9-18 18 36 54 72 9 15 2 1 1v 15 1 5 5-18 18 36 54 72 9-18 18 36 54 72 9
NIST GEC Example Data - Conclusions As the rf amplitude is increased both Ar + and ArH + show: Increases in Plasma Potential Increases in Ion Energy Splitting of the high energy peaks - transition time across the sheath rf Ar + also exhibits high concentrations of lower energy ions - due to inelastic collisions between Ar / Ar +
Detection of Negative Hydrogen Ions from bombardment of a Carbon Sample in a Capacitively Coupled Plasma Negative Ion Distribution Functions (NIDFs) obtained using the 45º Sector Field Energy Analyser.
Positive Ion Species from a HIPIMS Plasma N + Ti 2 + Ar + Ti + HIPIMS Discharge on a 2x6 mm 2 Ti Target. TiN + Peak Current Density: 3 A.cm -2, Peak Power Density 3 kw.cm -2.
Intensity, c/s Electron Energy Spectra 1 1 A comparison of the electron energy spectra for the principle cluster ions Fullerene C ++ 6 (m/z = 36) C +++ 6 (m/z = 24 ) C + 6 (m/z = 72) 1 The data compares the appearance potentials for the principle cluster ions formed from Buckminsterfullerene 1 2 4 6 8 1 12 14 16 Electron energy, v
Electron Attachment Cross-Sections 35 3 O - ex CO 2, Plasma off 25 2 15 1 5 4 8 12 16 2 24 28 electron- Attachment cross-sections for CO 2 (Rapp and Briglia) 22 2 18 16 14 12 1 8 6 4 2 O - ex CO, Plasma off. (residual CO 2 yields 8.2 ev peak) 4 12 16 2 24 28 electron- a O - ex neutrals ex CO 2, Plasma on a is O - ex CO 2 b is O - ex CO 2 + e - CO 2- CO+ O - 12 11 1 9 8 7 6 5 4 3 2 1 A b B 4 8 12 16 2 24 28 electron-
Electron Energy Spectra for CF 4 Plasma Plasma off ccl2f2 plasma off -on -off. 18mTorr chamber preasure. Two parent species for CF 2+ can be seen when the plasma is active. 1 1 1 The plasma derived species produce a characteristic feature at lower energies. 1 1 1 1 ccl2f2 plasma off -on -off. 18mTorr chamber preasure. 5 9.16667 13.3333 17.5 21.6667 25.8333 3 Plasma on electron- 1 5 9.16667 13.3333 17.5 21.6667 25.8333 3 electron-
Electron Attachment Spectra HAL4 EQP Low Energy #DE33 HAL4 EQP Low Energy #DE33 12 6 1 5 8 4 6 3 4 2 2 1 2 4 6 8 1 12 14 16 2 4 6 8 1 12 14 16 Cycle number 1 electron- Cycle number 1 electron- O - species may be formed from various precursors e.g. CO, CO 2, N 2 O via electron attachment and subsequent dissociation. The low energy resonant electrons required for this process are characteristic of the precursor involved.
Electron Attachment in a CF 4 Plasma 6 5 Plasma Off Plasma On 4 3 2 1 1 2 3 4 5 6 7 8 9 1 11 12 13 electron Formation of F - species can occur in the absence of plasma but the under working conditions there is a dramatic increase in F - concentration and type from plasma derived precursors.
Plasma Analysis using the Driven Electrode 45 4 2mTorr ar -65vbias -75v ext. Ar + 2 mtorr 21 2 19 18 Ar + 1 mtorr 1mTorr ar -65v bias -75v ext. 17 35 16 15 3 14 13 25 2 V B V P 12 11 1 9 8 15 1 7 6 5 4 3 5 2 1-1 -9-8 -7-6 -5-4 -3-2 -1 Cycle number Energy V 1 2 3 4 5 Cycle number -1-9 -8-7 -6-5 -4-3 -2-1 1 2 3 4 5 Energy V 25mTorr ar -65v bias -75v ext. 1mTorr ar -65v bias -75v ext. 22 2 Ar + 25 mtorr 3 28 26 Ar H + 1 mtorr VP 18 24 16 22 2 14 18 12 16 1 14 12 8 1 6 4 2 8 6 4 2 VB -1-9 -8-7 -6-5 -4-3 -2-1 1 2 3 4 5 Cycle number Energy V -1-9 -8-7 -6-5 -4-3 -2-1 1 2 3 4 5 Cycle number Energy V
Plasma Analysis using the Driven Electrode 44mTorr ar -65v bias -75v ext. Ar + 44 mtorr 5mTorr ar -65v bias -75v ext. Ar + 5 mtorr 17 21 16 2 15 19 14 13 18 17 16 12 15 11 14 1 9 13 12 11 8 1 7 9 6 5 8 7 6 4 5 3 4 2 1 3 2 1-1 -9-8 -7-6 -5-4 -3-2 -1 1 2 3 4 5 Energy V -1-9 -8-7 -6-5 -4-3 -2-1 1 2 3 4 5 Energy V Time 14:54:6 Date 13/3/97 Time 14:8:36 Date 13/3/97 Negative energy ions due to influence of the biased electrode (V b ) V peak corresponds to centre of characteristic rf split peak feature As the pressure in the plasma increases inelastic collisional broadening / energy loss of Ar + (not ArH + ) is seen to dominate
Energy Analysis of Plasma Components 2mTorr arsf6-65vbias -75v ext. 8mTorr ar sf6-4vbias --5v ext. 1 9 8 F + ions 1 9 8 SF + 7 7 6 6 5 5 4 4 3 3 2 2 1 1-1 -9-8 -7-6 -5-4 -3-2 -1 1 2 3 4 5 6 7 8 9 1 Cycle number Energy V -5-45 -4-35 -3-25 -2-15 -1-5 5 1 15 2 25 3 35 4 45 5 Cycle number Energy V 8mTorr ar sf6-4vbias --5v ext. 8mTorr ar sf6-4vbias --5v ext. 1 1 9 8 SF 2 + 9 8 SF 3 + 7 7 6 6 5 5 4 4 3 3 2 2 1 1-5 -45-4 -35-3 -25-2 -15-1 -5 5 1 15 2 25 3 35 4 45 5 Cycle number Energy V -5-45 -4-35 -3-25 -2-15 -1-5 5 1 15 2 25 3 35 4 45 5 Cycle number Energy V Even in an apparently homogeneous plasma the individual component species can exhibit a wide variation in energies.
EQP Studies of a D.C. Magnetron Plasma D.C. -5 V to V 5 m orifice 1-3 Torr 5 cm 5x1-7 Torr V c = -3 V to -38 V Magnetron Cathode: Cu, Al, Mo or Graphite Working Gas: Argon or Sulfur Hexafluoride 6 cm D.C. MAGNETRON EQP PROBE
C/S D.C. Magnetron Plasma Data Fast Neutral Species 1 Power : 4 Watts Ar pressure : 5 mtorr Magnetron / EQP Distance : 3. cm 1 1 1 1 1 2 3 4 5 6 7 8 9 1111213141516171819221 energy / ev High Energy tail (>5 ev) - energetic copper atoms ejected from magnetron cathode and ionised in the Ar plasma close to the EQP orifice and reflect the kinetic energies with which the atoms leave the cathode.
C/S D.C. Magnetron Plasma Data Fast Neutral Species Power : 4 Watts Current : 3 ma Ar pressure : 5 mtorr Magnetron / EQP Distance : 3. cm 1 1 1 nb. The EQP was set to reject ions from plasma hence small background of ca. 2 c/s above 15 ev. 1 1 2 3 4 5 6 7 8 9 1111213141516171819 energy / ev 2 components, one due to strong, thermal energy + weaker feature extending up to 15 ev. Plasma off no copper detected above 3 ev, indicating all kinetic ions produced in the ioniser / cage.
Latest publications Selected Publications Negative-ion surface production in hydrogen plasmas: modelling of negative-ion energy distribution functions and comparison with experiments. 213. A Ahmad et al. Plasma Sources Sci. Technol. 22 256 Spacially enhanced Langmuir probe measurements of a magnetically enhanced hollow cathode arc plasma. 211. B Zimmermann et al. Surface and coatings technology 25 5393-5396 Quantification of the deuterium ion fluxes from a plasma source. 211. A Manhard et al. Plasma Sources Sci. Technol. 2 151 Advantages of highly ionized pulse plasma magnetron sputtering of silver for improved E. coli inactivation. 212. O Baghriche et al. Thin Solid Films 52 3567-3573 Influence of high power impulse magnetron sputtering plasma ionization on the microstructure of TiN thin films. 211. AP Ehiasarian. J. Appl. Phys. 19 14314
Selected Hiden EQP Users INP Greifswald Xi an Modern Chemistry Institute Universite d Orleans Southwest Research Institute KRICT Applied Materials Fraunhofer IWS Ruhr-Universität Bochum
SEM c/s Summary High performance probe for mass and energy analysis of ions, radicals and neutrals from a plasma. A large number of options are available in order to sample from a variety of plasma types. The EQP sees use worldwide in a variety of plasma applications. 5 4 3 2 1 5 1 15 2 Ion Energy ev