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VACUUM ARC DEPOSITION Principles of Vacuum Arc Deposition (VAD) Cathode Spots Reactive VAD Magnetic Field in VAD Filtered Vacuum Arc Deposition Hybrid VAD Systems Substrate Ion Bombardment – Ion Plating Ion Current Measurements Coating Deposition Rate Appendix 1- Ion Plating Lecture 6 2009
VACUUM ARC DEPOSITION (VAD) ,[object Object],[object Object]
CATHODE-SPOT VACUUM ARC ,[object Object]
CATHODE SPOT VACUUM ARC Example:  Hot Refractory Anode Vacuum Arc (HRAVA), Movie 1 ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
CATHODE SPOT VACUUM ARC DISCHARGE ,[object Object],[object Object],[object Object],[object Object]
CATHODE SPOTS ,[object Object],[object Object],[object Object],[object Object],[object Object]
EROSION OF MATERIAL FROM CATHODE SPOTS ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
CATHODE EROSION TRACE ,[object Object],[object Object],R. Boxman et al., Ref. [1]
CATHODE SPOT EROSION SPECIES AND VACUUM ARC PLASMA ,[object Object],[object Object],[object Object],Boxman, Goldsmith, 1987
CATHODE SPOT  VACUUM ARC PLASMA ,[object Object],[object Object],[object Object],[object Object],[object Object]
VACUUM ARC PLASMA   FROM CATHODE SPOTS TO THE SUBSTRATE  VACUUM ARC DEPOSITION (VAD) Tracks of Cathode Spot Motion Multiple spots Ti, I arc ~100 A Single spot Cu, Iarc~30-50 A Plasma produced by a cathode spot Scheme of Cathodic Vacuum Arc Plasma Deposition
VACUUM ARC PLASMA CHARACTERISTICS ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
MULTIPLE IONIZATION: EXAMPLE Ti Plasma in Vacuum, Arc Current 100 A ,[object Object],[object Object],[object Object],103 34 6 +3 79 39 67 +2 65 65 27 +1 Total energy, E i , eV Average energy, E i /Z i  , eV Ion fraction, % Charge state Z i
VACUUM ARC PLASMA CHARACTERISTICS   ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
COLD CATHODE – HOT CATHODE ,[object Object],[object Object],[object Object]
VACUUM ARC PLASMA JET ,[object Object],[object Object]
MACROPATICLES  IN PLASMA JET ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
MACROPARTICLES  IN VAD COATINGS
CURRENT-VOLTAGE CHARACTERISTICS  OF A DISCHARGE TUBE
COMPARISON OF PLASMAS IN VACUUM ARC DEPOSITION AND SPUTTERING SYSTEMS: High voltage (few hundreds V - ~1 kV), low current (~10 -2 -1 A) discharge High current  (I arc =30-500 A),  low voltage (10-50 V) discharge Electrical characteristics Bombardment by of target by plasma ions to eject particles (atoms/molecules) of material to be deposited Production of charged particle jet to be deposited on substrate Function of plasma Glow discharge induced in low pressure background working gas Metal (mainly) plasma, cathode erosion species Type of plasma SPUTTERING VACUUM ARC FEATURE
COMPARISON OF PLASMAS (CONTINUE) 10 14 -10 18 10 16 -10 20 Plasma density, m -3 (3-6)  10 3  (Ar ions) (1-2)  10 4 Ion velocity, m/s 10-40 50-150 Ion energy, eV No Yes Macroparticles SPUTTERING VACUUM ARC FEATURE
VACUUM ARC DEPOSITON HISTORY - I ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
VACUUM ARC DEPOSITON HISTORY - II ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
VACUUM ARC DEPOSITON HISTORY - III ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
VACUMM ARC DEPOSITION Process Definitions, Terms ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
TYPICAL VACUUM ARC DEPOSITION (VAD) SYSTEM   ,[object Object],[object Object],[object Object],[object Object],VAD SYSTEM WITH CYLINDRICAL CATHODE AND ANNULAR ANODE
ARC INITIATION ,[object Object],[object Object],[object Object],[object Object],[object Object]
ARC OPERATION ,[object Object],[object Object],[object Object],[object Object],[object Object]
CATHODE SPOTS ,[object Object],[object Object],[object Object],[object Object],[object Object],Tracks of cathode spot motion on Ti cathode surface, I arc ~100 A
ARC CURRENT (I arc ) AND ION CURRENT (I ion ) PRODUCED BY VACUUM ARC PLASMA SOURCE ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
ARC POWER AND HEAT FLUX ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
COMMERCIAL VACUUM ARC DEPOSITION APPARATUS “Bulat-3”  - NEW EPOCH IN CUTTING TOOL INDUSTRY (former USSR, 1981) Anode – water cooled vacuum chamber 3 independent plasma guns Chamber diameter ~ 60 cm
SCHEME OF COMMERCIAL VAD SYSTEM (“Bulat”- Type)
SCHEME OF COMMERCIAL TRIPLE CATHODE VAD SYSTEM
TRIPLE CATHODE VAD SYSTEM AT TAU
COATINGS TYPES THAT MAY BE FABRICATED USING VAD TECHNIQUES ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
COATINGS TYPES THAT MAY BE FABRICATED USING VAD TECHNIQUES (Continue) ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
REACTIVE VACUUM ARC DEPOSITION ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
REACTIVE VAD - HARD WEAR RESISTANT COATING DEPOSITION   ,[object Object],[object Object],[object Object],[object Object],[object Object]
REACTIVE VAD OF TiN COATING Model by M.Sakaki & T.Sakakibara,  IEEE. Trans. Plasma Sci.,  vol. 22 (1994), p. 1049-1054 ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
ION PLATING – SUBSTRATE BOMBARDMENT BY POSITIVE PLAMA IONS ION PLATING IN VAD Role of  negative bias voltage  on  surface bombardment  by plasma ions and coating deposition process
NEGATIVE BIAS VOLTAGE APPLIED  TO THE SUBSTRATE IN VAD PROCESS Negative bias voltage to the substrate relative the grounded anode Substrate ion bombardment  by positive metal ions
COATING DEPOSITION RATE vs BIAS VOLTAGE TO THE SUBSTRATE ,[object Object],[object Object]
BIAS VOLTAGE APPLICATION: ACTION OF HIGH |V bias | ,[object Object],[object Object],[object Object],[object Object],[object Object]
BIAS VOLTAGE APPLICATION: ACTION OF LOW |V bias | ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
INFLUENCE OF BIAS VOLTAGE ON COATING STRUCTURE AND PROPERTIES ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
BIAS VOLTAGE: CONVENTIONAL COATING DEPOSITION PROCESS ,[object Object],[object Object],[object Object]
POSSIBLE NEGATIVE EFFECTS OF BIAS APPLICATION TO THE SUBSTRATE ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
CALCULATION OF HEAT FLUX TO THE SUBSTRATE ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
DEBYE LENGTH ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
ION FLUX TO THE SUBSTRATE IN VAD  - EFFECTIVENESS OF DEPOSITION PROCESS ,[object Object],[object Object],[object Object]
MEASUREMENT OF ION FLUX TO THE SUBSTRATE (ION CURRENT) Negatively biased Langmuir probe –  saturation ion current measurement Saturation ion current characterizes deposition system effectiveness
VOLTAGE-CURRENT CHARACTERISTICS  OF LANGMUIR PROBE Evaluation of deposition rate –  saturated ion current is important
SATURATION ION CURRENT AND DEPOSITION RATE ,[object Object],J i  – ion current density m i  – ion mass z – average ion charge number e – electron charge    - density  =0.8-0.9 – sticking coefficient
ION CURRENT AND DEPOSITION RATE ,[object Object],[object Object],[object Object],[object Object],[object Object]
MAGNETIC FIELD IN VACUUM ARC DEPOSITION ,[object Object],[object Object],[object Object],[object Object]
MAGNETIC FIELD IN VACUUM ARC PLASMA DEPOSITION SYSTEMS EDPL, TAU – System 3
MAIN FUNCTIONS OF MAGNETIC FIELD IN VAD SYSTEMS ,[object Object],[object Object],[object Object],[object Object]
CATHODE SPOT MOTION ON THE FACE SURFACE OF CYLINDRICAL CATHODE. NO MAGNETC FIELD ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Random spot motion on cathode surface
MAGNETIC FIELD EFFECT ON THE CATHODE SPOT MOTION ,[object Object],[object Object],[object Object],[object Object]
1. RETROGRADE  (-E x B) CATHODE SPOT MOTION IN MAGNETIC FIELD ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
2. “ACUTE ANGLE” RULE. CYLINDRICAL CATHODE - TWO CASES OF MAGNETIC FIELD CONFIGURATION ,[object Object],[object Object],Spots move outside the cathode  surface – unstable arcing “ Arched field” – spot motion on  circumferential trajectory on cathode
EFFECT OF MAGNETIC FIELD ON CATHODE SPOT MOTION ,[object Object],[object Object],[object Object],[object Object]
“ ARCHED FIELD” - CIRCUMFERENTIAL SPOT MOTION ON DEFINED TRAJECTORY ,[object Object],[object Object],Magnetic field plot in the cathode vicinity Cathode erosion track V. Zhitomirsky  et al.,  1994
SPOT MOTION ON ROUND CATHODE SURFACE (Ti arc, System 2) No magnetic field – random spot motion Acute angle directed outwards –  Spot operation on  the cathode side “ Arched” field – circumferential spot motion V. Zhitomirsky, JVST, 1995
“ ARCHED FIELD” CYLINDRICAL CATHODE ,[object Object],Water-cooled cavity Cathode surface Cathodes
“ ARCHED” FIELD -  RECTANGULAR CATHODE DESIGH Magnetic field  configuration: QuickField TM  plot Cathode spot  Motion track Rectangular cathode, System 4, EDPL
EFFECT OF “ACUTE ANGLE” IN CONE CATHODE DESIGN – SPOT CONFINEMENT IN CATHODE CENTER Cathode Anode Focusing  Coil Guiding Coil Acute angle    - between the magnetic line and cathode cone surface   –  spot motion towards the cathode center Axial magnetic  field – spot  confinement  in the cathode center Cone cathode in  axial field Cathode Coil
MAGNETIC PLASMA GUIDING TO THE SUBSTRATE   IN THE STRAIGHT CYLINDRICAL DUCT   Axial magnetic field produced by coils 2-4 positioned co-axially with  duct axis  - significant increase in plasma flux to the substrate System 3, EDPL
PLOT OF MAGNETIC FIELD LINES PRODUCED BY AXIAL COILS (Axial Cross-Section) ,[object Object],[object Object],[object Object],Substrate Cathode
PRINCIPLES OF PLASMA GUIDING IN THE MAGNETIC FIELD PLASMA TRANSPORT IN THE STRAIGHT AND CURVILINEAR DUCT
MOTION OF A CHARGED PARTICLE IN MAGNETIC FIELD ,[object Object],[object Object],[object Object],[object Object],[object Object]
LARMOR RADIUS OF PARTICLE GYRATION ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
GUIDING OF A PLASMA JET IN AN AXIAL MAGNETIC FIELD ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
GUIDING OF A PLASMA JET IN A RELATIVELY WEAK MAGNETIC FIELD ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
PARTICLE MAGNETIZATION  EXAMPLE ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
ELECTRON CUT-OFF FROM THE ANODE IN MAGNETIC FIELD – UNSTABLE ARCING ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],B
SPATIAL DISTRIBUTION OF THE PLASMA BEAM IN MAGNETIC FIELD ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Spatial distribution of ion current density Multi-probe for distribution measurement V. Zhitomirsky  et al . Surf. Coat. Technol. 1995
FILTERED VACUUM ARC DEPOSITION (FVAD) ,[object Object],[object Object],[object Object],[object Object],[object Object]
VAD SYSTEM WITH A QUARTER -TORUS MAGNETIC FILTER Plasma flux is guided by toroidal magnetic field to the substrate positioned in the chamber, while macroparticles are fully or mainly removed from the flux System 2, EDPL
SCHEME OF FILTERED VAD (FVAD) SYSTEM (System 2 at TAU)
MAGNETIC FIELD CONFIGURATION IN THE TOROIDAL DUCT ,[object Object],[object Object],[object Object],[object Object]
MACROPARTICLE FILTERING: VAD SYSTEM WITH A QUARTER TORUS FILTER ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
COATINGS DEPOSITED WITH UNFILTERED AND FILTERED VAD Macroparticles in Coating Unfiltered VAD Macroparticle-Free Coating Filtered VAD
“ S-FILTER”   (A. Anders, Berkeley, USA) ,[object Object]
“ OPEN” S-FILTER DESIGN  (A. Anders, Berkeley, USA) TOROIDAL FILTER WITH WALL – part of small macroparticles may  reflect from the filter wall and follow to the substrate with plasma jet “ Open” S-filter (Anders’ design) – macroparticles mainly  exit between windings and leave plasma jet CATHODE To substrate ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
ADVANTAGES AND DISANVANTAGES OF MACROPARTICLE FILTERING ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
DUAL FILTERED VACUUM ARC PLASMA SOURCE ,[object Object],[object Object],From: P. Martin, A. Bendavid,  Thin Solid Films , 2001 More about FVAD sources – see R.L. Boxman and V.N. Zhitomirsky, “ Vacuum Arc Deposition Devices”,  Rev. Sci. Instrum.  77 021101 (2006)
LARGE-AREA RECTANGULAR FVAD SYSTEM  (System 4, EDPL) ,[object Object],[object Object],[object Object]
SCHEME OF RECTANGULAR FVAD SYSTEM AND  CATHODE APPLICATION: Transparent conducting SnO 2  coating deposition on flat substrates Rectangular cathode with cathode spot  trace System 4, EDPL
HOT REFRACTORY ANODE VACUUM ARC (HRAVA) ,[object Object],[object Object],[object Object],Courtesy of Prof. I. Beilis, EDPL-TAU Substrate Substrate Anode region Cathode region Plasma flux from:
CATHODE SPOT MOTION ON A LONG CYLINDRICAL CATHODE ,[object Object],[object Object],[object Object],[object Object]
COMPACT VAD SOURCE WITH CONE CATHODE, TAU, 2004-2008
VACUUM ARC PLASMA EVAPORATION (VAPE)  EXAMPLE: NOT CATHODIC VAD! ,[object Object],Vacuum Arc Plasma Evaporation  (VAPE) – not cathode spot VAD! Arc plasma of gas (Ar+O 2 ) Gas pressure – 0.075-1 Pa  (5  10 -4  -7.5  10 -3  Torr) Power – 2.5 10 kW Evaporated material – sintered  from powders ZnO and Ga 2 O 3 Deposition of Ga-Zn-oxide (GZO) coating
LITERATURE ,[object Object],[object Object]
Multi-Source VAD Systems Hybrid Deposition Systems
MULTI-SOURCE VAD SYSTEMS ,[object Object],[object Object],[object Object],[object Object]
INDUSTRIAL SYSTEM WITH DUAL FILTERED VAD SOURCE   V. Gorokhovsky, SCT 2004
COMBINED (HYBRID) DEPOSITION SYSTEMS ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
HYBRID DEPOSITION SYSTEM BY V. GOROHOVSKY V. Gorokhovsky et. Al., SCT 1993 Substrate Filtered VAD  Source E-Beam Source
LARGE HYBRID SYSTEM WITH VAD AND MAGNETRON SPUTTERING SOURCES CemeCon AG (Germany) By the courtesy of Dr. Christoph Shiffers (CemeCon AG), March 2009
HYBRID VAD-CVD SYSTEM FOR SUPERHARD COATINGS  nc -MeN/ a -Si 3 N 4 ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],P. Martin  et al.,  SCT 2004
APPENDIX 1 Pre-Deposition Substrate Ion Cleaning and Ion Plating in Deposition Processes * ,[object Object],[object Object],[object Object]
ION BOMBARDMENT IN PVD PROCESSES ,[object Object],[object Object],[object Object]
SPUTTER ION CLEANING IN GLOW DISCHARGE PLASMA ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
CATHODIC SPUTTERING: DC TRIODE SYSTEM Negative bias voltage  to the substrate –  Sputter ion cleaning prior to deposition Negative bias voltage  to the target – Sputter deposition
SPUTTER ION CLEANING IN GLOW DISCHARGE PLASMA ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
ION BOMBARDMENT OF COATING DURING DEPOSITION ,[object Object],[object Object],[object Object]
ION BOMBARDMENT IN VACUUM ARC DEPOSION ,[object Object],[object Object],[object Object],[object Object],[object Object]
ION BOMBARDMENT IN VACUUM ARC DEPOSION ,[object Object],[object Object],[object Object],[object Object]

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Vacuum arc deposition (Yan Valsky) - Lecture Dr.V.Zhitomirsky (Coating cource/EDPL/TAU)

  • 1. VACUUM ARC DEPOSITION Principles of Vacuum Arc Deposition (VAD) Cathode Spots Reactive VAD Magnetic Field in VAD Filtered Vacuum Arc Deposition Hybrid VAD Systems Substrate Ion Bombardment – Ion Plating Ion Current Measurements Coating Deposition Rate Appendix 1- Ion Plating Lecture 6 2009
  • 2.
  • 3.
  • 4.
  • 5.
  • 6.
  • 7.
  • 8.
  • 9.
  • 10.
  • 11. VACUUM ARC PLASMA FROM CATHODE SPOTS TO THE SUBSTRATE VACUUM ARC DEPOSITION (VAD) Tracks of Cathode Spot Motion Multiple spots Ti, I arc ~100 A Single spot Cu, Iarc~30-50 A Plasma produced by a cathode spot Scheme of Cathodic Vacuum Arc Plasma Deposition
  • 12.
  • 13.
  • 14.
  • 15.
  • 16.
  • 17.
  • 18. MACROPARTICLES IN VAD COATINGS
  • 19. CURRENT-VOLTAGE CHARACTERISTICS OF A DISCHARGE TUBE
  • 20. COMPARISON OF PLASMAS IN VACUUM ARC DEPOSITION AND SPUTTERING SYSTEMS: High voltage (few hundreds V - ~1 kV), low current (~10 -2 -1 A) discharge High current (I arc =30-500 A), low voltage (10-50 V) discharge Electrical characteristics Bombardment by of target by plasma ions to eject particles (atoms/molecules) of material to be deposited Production of charged particle jet to be deposited on substrate Function of plasma Glow discharge induced in low pressure background working gas Metal (mainly) plasma, cathode erosion species Type of plasma SPUTTERING VACUUM ARC FEATURE
  • 21. COMPARISON OF PLASMAS (CONTINUE) 10 14 -10 18 10 16 -10 20 Plasma density, m -3 (3-6)  10 3 (Ar ions) (1-2)  10 4 Ion velocity, m/s 10-40 50-150 Ion energy, eV No Yes Macroparticles SPUTTERING VACUUM ARC FEATURE
  • 22.
  • 23.
  • 24.
  • 25.
  • 26.
  • 27.
  • 28.
  • 29.
  • 30.
  • 31.
  • 32. COMMERCIAL VACUUM ARC DEPOSITION APPARATUS “Bulat-3” - NEW EPOCH IN CUTTING TOOL INDUSTRY (former USSR, 1981) Anode – water cooled vacuum chamber 3 independent plasma guns Chamber diameter ~ 60 cm
  • 33. SCHEME OF COMMERCIAL VAD SYSTEM (“Bulat”- Type)
  • 34. SCHEME OF COMMERCIAL TRIPLE CATHODE VAD SYSTEM
  • 35. TRIPLE CATHODE VAD SYSTEM AT TAU
  • 36.
  • 37.
  • 38.
  • 39.
  • 40.
  • 41. ION PLATING – SUBSTRATE BOMBARDMENT BY POSITIVE PLAMA IONS ION PLATING IN VAD Role of negative bias voltage on surface bombardment by plasma ions and coating deposition process
  • 42. NEGATIVE BIAS VOLTAGE APPLIED TO THE SUBSTRATE IN VAD PROCESS Negative bias voltage to the substrate relative the grounded anode Substrate ion bombardment by positive metal ions
  • 43.
  • 44.
  • 45.
  • 46.
  • 47.
  • 48.
  • 49.
  • 50.
  • 51.
  • 52. MEASUREMENT OF ION FLUX TO THE SUBSTRATE (ION CURRENT) Negatively biased Langmuir probe – saturation ion current measurement Saturation ion current characterizes deposition system effectiveness
  • 53. VOLTAGE-CURRENT CHARACTERISTICS OF LANGMUIR PROBE Evaluation of deposition rate – saturated ion current is important
  • 54.
  • 55.
  • 56.
  • 57. MAGNETIC FIELD IN VACUUM ARC PLASMA DEPOSITION SYSTEMS EDPL, TAU – System 3
  • 58.
  • 59.
  • 60.
  • 61.
  • 62.
  • 63.
  • 64.
  • 65. SPOT MOTION ON ROUND CATHODE SURFACE (Ti arc, System 2) No magnetic field – random spot motion Acute angle directed outwards – Spot operation on the cathode side “ Arched” field – circumferential spot motion V. Zhitomirsky, JVST, 1995
  • 66.
  • 67. “ ARCHED” FIELD - RECTANGULAR CATHODE DESIGH Magnetic field configuration: QuickField TM plot Cathode spot Motion track Rectangular cathode, System 4, EDPL
  • 68. EFFECT OF “ACUTE ANGLE” IN CONE CATHODE DESIGN – SPOT CONFINEMENT IN CATHODE CENTER Cathode Anode Focusing Coil Guiding Coil Acute angle  - between the magnetic line and cathode cone surface – spot motion towards the cathode center Axial magnetic field – spot confinement in the cathode center Cone cathode in axial field Cathode Coil
  • 69. MAGNETIC PLASMA GUIDING TO THE SUBSTRATE IN THE STRAIGHT CYLINDRICAL DUCT Axial magnetic field produced by coils 2-4 positioned co-axially with duct axis - significant increase in plasma flux to the substrate System 3, EDPL
  • 70.
  • 71. PRINCIPLES OF PLASMA GUIDING IN THE MAGNETIC FIELD PLASMA TRANSPORT IN THE STRAIGHT AND CURVILINEAR DUCT
  • 72.
  • 73.
  • 74.
  • 75.
  • 76.
  • 77.
  • 78.
  • 79.
  • 80. VAD SYSTEM WITH A QUARTER -TORUS MAGNETIC FILTER Plasma flux is guided by toroidal magnetic field to the substrate positioned in the chamber, while macroparticles are fully or mainly removed from the flux System 2, EDPL
  • 81. SCHEME OF FILTERED VAD (FVAD) SYSTEM (System 2 at TAU)
  • 82.
  • 83.
  • 84. COATINGS DEPOSITED WITH UNFILTERED AND FILTERED VAD Macroparticles in Coating Unfiltered VAD Macroparticle-Free Coating Filtered VAD
  • 85.
  • 86.
  • 87.
  • 88.
  • 89.
  • 90. SCHEME OF RECTANGULAR FVAD SYSTEM AND CATHODE APPLICATION: Transparent conducting SnO 2 coating deposition on flat substrates Rectangular cathode with cathode spot trace System 4, EDPL
  • 91.
  • 92.
  • 93. COMPACT VAD SOURCE WITH CONE CATHODE, TAU, 2004-2008
  • 94.
  • 95.
  • 96. Multi-Source VAD Systems Hybrid Deposition Systems
  • 97.
  • 98. INDUSTRIAL SYSTEM WITH DUAL FILTERED VAD SOURCE V. Gorokhovsky, SCT 2004
  • 99.
  • 100. HYBRID DEPOSITION SYSTEM BY V. GOROHOVSKY V. Gorokhovsky et. Al., SCT 1993 Substrate Filtered VAD Source E-Beam Source
  • 101. LARGE HYBRID SYSTEM WITH VAD AND MAGNETRON SPUTTERING SOURCES CemeCon AG (Germany) By the courtesy of Dr. Christoph Shiffers (CemeCon AG), March 2009
  • 102.
  • 103.
  • 104.
  • 105.
  • 106. CATHODIC SPUTTERING: DC TRIODE SYSTEM Negative bias voltage to the substrate – Sputter ion cleaning prior to deposition Negative bias voltage to the target – Sputter deposition
  • 107.
  • 108.
  • 109.
  • 110.