Specific Process Knowledge/Thin film deposition/Deposition of Silicon/Si sputter in Sputter-System Metal-Oxide(PC3)

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This page is written by Evgeniy Shkondin @DTU Nanolab if nothing else is stated.
All images and photos on this page belongs to DTU Nanolab.
The fabrication and characterization described below were conducted in 2022 by Evgeniy Shkondin, DTU Nanolab.


This page presents the results of Si deposition using RF and Pulsed-DC Sputtering in Sputter-System Metal-Nitride (PC3) commonly known as "Cluster Lesker". The deposition target is 4" Si. Source #1 was used. Materials from this source can either be deposited with RF or p-DC sputtering. Here, the results from both methods will be covered.


The main focus of the study was the deposition rate, optical functions, and the general performance of deposition from a bigger 4” target. The silicon sputtering from the target of this size allows achieving a higher deposition rate and service to many potential applications where several hundreds of nm are needed to be put uniformly on a wafer of 150mm or similar. Besides, it offers the additional possibility to deposit Si using Cluster Lesker in case another chamber (PC1) where the Si process is also established fails for some reason.

The depositions performed with closed dark space shield configuaration (see photography below). The dark space shield is a circular protection cylinder that sits around the cathode, in its close configuration the top part of the shield is bent toward the target and shadows a few mm of it.

It must be mentioned that the dark space shield should be in a “closed-form” only, as it was observed that the “opened” dark space shield configuration can do a side wall Cu sputtering. This will heavily contaminate the film and gradually damage the tool.

4” magnetron in PC3 has more functionalities compared to the ordinary guns in cluster Lesker. It can(to some degree) moves in Z-direction. This will affect the deposition rate, uniformity and most likely play an important role in reactive sputtering. Besides that, it can be easily tilted if necessary. In this study, two z-high positions have been compared (lowes-“home” and highest –“extended”). The effect of power has also been evaluated.


RF Sputtering of Si in Sputter-System Metal-Nitride(PC3)

The RF Si process recipe in a Sputter-System Metal-Nitride(PC3) is following:

* Recipe Name:  MD PC3_Src1 - RF_Upstream
  • PC Gun Z-shift Position: Home (00.00 mm) and Extended (95.20 mm)
  • Tilt: No (Target in horizontal plane)
  • Deposition mode: Upstream
  • Rotation speed: 10 rpm
  • Pressure: 3 mTorr
  • Power: 120-200 W (It is recomended to use 180W for best uniformity if using "Extended" gun Z-shift position).
  • Deposition time: 1800s
  • Deposition temperature: room temperature


Samples: 6" Si with 300nm SiO2 (from furnace C1 recipe: DRY1100 05:00:00 + 20 min annealing)

Characterization (RF mode)

Spectroscopic ellipsometry (RF mode)

Thicknesses have been measured by spectroscopic ellipsometry (VASE ellipsometer) across different locations on 6" Si wafer with 300nm dry SiO2. The optical model is based on Tauc-Lorentz and two Lorentz oscillators. The deposition parameters are present in the recipe written above. The results are present in a table below:

PC Gun Z-shift Position: Extended (95.20 mm)
Deposition conditions

Power (W)

Time (s) Pressure (mTorr) Average (nm) Standard deviation Minimum Thickness (nm) Maximum Thickness (nm) Rate (nm/s)
120 W 1800 3 42.73 2.22 38.26 45.24 0.024
140 W 1800 3 62.66 2.51 56.89 65.52 0.035
160 W 1800 3 81.23 3.17 74.56 84.54 0.045
180 W 1800 3 102.03 3.13 95.17 105.27 0.057
200 W 1800 3 122.32 3.65 114.99 126.16 0.068


PC Gun Z-shift Position: Home (00.00 mm)
Deposition conditions

Power (W)

Time (s) Pressure (mTorr) Average (nm) Standard deviation Minimum Thickness (nm) Maximum Thickness (nm) Rate (nm/s)
120 W 1800 3 16.36 1.69 12.12 18.09 0.009
140 W 1800 3 23.06 1.42 19.72 24.79 0.013
160 W 1800 3 27.50 1.22 24.57 28.96 0.015
180 W 1800 3 41.48 1.75 38.84 43.70 0.023
200 W 1800 3 52.23 2.24 48.93 56.44 0.029


Deposition rate (RF mode)


  • PC Gun Z-shift Position: Extended (95.20 mm)
Deposition rate (nm/s) =   



  • PC Gun Z-shift Position: Home (00.00 mm)
Deposition rate (nm/s) = 

Uniformity (RF mode)

Optical functions (RF mode)

DC Bias recordings (RF mode)

Any deposition recipe the user runs on Cluster Lesker is getting recorded. Many parameters are stored in the datalog files (in the 1-second interval) that can be accessed and viewed later. Here the DC bias was monitored for the whole experiment.

Pulsed DC Sputtering of Si in Sputter-System Metal-Nitride(PC3)

This section covers the results from the pulsed DC deposition method. It must be mentioned that the lower powers give an unstable plasma and varying DC Bias voltage. This is why it is strongly recommended to run this process at the range of 180W-200W (although not higher since the target can only withstand 20 W/cm2 power density which means the maximum power of approximately 200W for a 4-inch target ). Besides, it is also challenging to ignite and maintain plasma using the pulsed-DC power supply at the very beginning of the process, where the power values are still low. It is strongly recommended to ramp the power with the opened source shutter.


The Pulsed-DC Si process recipe in a Sputter-System Metal-Nitride(PC3) is following:

* Recipe Name:  MD PC3_Src1 - Pulse DC_Upstream
  • PC Gun Z-shift Position: Home (00.00 mm) and Extended (95.20 mm)
  • Tilt: No (Target in horizontal plane)
  • Deposition mode: Upstream
  • Rotation speed: 10 rpm
  • Pressure: 3 mTorr
  • Power: 120-200 W (It is recomended to use 200W for for the most stable DC bias voltage).
  • Frequency: 100 kHz
  • Reverse time: 1 µs
  • Deposition time: 1800s
  • Deposition temperature: room temperature


Samples: 6" Si with 300nm SiO2 (from furnace C1 recipe: DRY1100 05:00:00 + 20 min annealing)

Characterization (p-DC)

Spectroscopic ellipsometry (p-DC)

Thicknesses have been measured by spectroscopic ellipsometry (VASE ellipsometer) across different locations on 6" Si wafer with 300nm dry SiO2. The optical model is based on Tauc-Lorentz and two Lorentz oscillators. The deposition parameters are present in the recipe written above. The results are present in a table below:

PC Gun Z-shift Position: Extended (95.20 mm)
Deposition conditions

Power (W)

Time (s) Pressure (mTorr) Average (nm) Standard deviation Minimum Thickness (nm) Maximum Thickness (nm) Rate (nm/s)
120 W 1800 3 98.10 2.99 91.47 101.35 0.0545
160 W 1800 3 239.87 4.26 229.95 244.61 0.1333
200 W 1800 3 311.43 5.38 299.99 316.45 0.1730


PC Gun Z-shift Position: Home (00.00 mm)
Deposition conditions

Power (W)

Time (s) Pressure (mTorr) Average (nm) Standard deviation Minimum Thickness (nm) Maximum Thickness (nm) Rate (nm/s)
120 W 1800 3 37.49 1.51 34.39 39.86 0.0208
160 W 1800 3 95.83 4.27 89.54 102.62 0.0532
200 W 1800 3 134.73 6.97 123.37 145.90 0.0748


Deposition rate (p-DC)

Uniformity (p-DC)

Optical functions (p-DC)

DC Bias recordings (p-DC)

Any deposition recipe the user runs on Cluster Lesker is getting recorded. Many parameters are stored in the datalog files (in the 1-second interval) that can be accessed and viewed later. Here the DC bias was monitored for the whole experiment.