Specific Process Knowledge/Etch/IBE⁄IBSD Ionfab 300/IBE magnetic stack etch: Difference between revisions

From LabAdviser
Khr (talk | contribs)
No edit summary
Bghe (talk | contribs)
No edit summary
 
(79 intermediate revisions by 3 users not shown)
Line 1: Line 1:
End point detection is achieved by SIMS, and the etch rate is approximately 25 Nm/min.
'''Feedback to this page''': '''[mailto:plasma@nanolab.dtu.dk?Subject=Feed%20back%20from%20page%20http://labadviser.nanolab.dtu.dk/index.php/Specific_Process_Knowledge/Etch/IBE%E2%81%84IBSD_Ionfab_300/IBE_magnetic_stack_etch click here]'''
Resist stripping can be hard due to burned resist, to remedy this try to lover the current; this will though chance the sidewall angle. For help, discussion and further info please contact Kristian Hagsted Rasmussen.
<br> '''''The work on this page was done Kristian Hagsted Rasmussen, DTU Nanolab, unless otherwise stated'''''
=Etching magnetic stacks=
Magnetic stacks can be etched or more precisly milled in the Ion Beam Etcher (IBE). Below is presented some work done on milling stacks of magnetic layers.
 
 
==Results of Design of Experiments optimization of magnetic stack etching (Kristian Hagsted Rasmussen@nanotech.dtu.dk spring 2011)==


==Results from the acceptance test in February 2011==
'''Acceptance test for Ti etch:'''
{| border="2" cellspacing="0" cellpadding="2"
|-
!style="background:silver; color:black;" align="left"|.
|style="background:WhiteSmoke; color:black"|'''Acceptance Criteria'''
|
'''Acceptance Results'''
|-
!style="background:silver; color:black;" align="left"|Substrate information
|style="background:WhiteSmoke; color:black"|
*50 mm SSP Si wafer
*525 µm thick
*Supplied by Danchip
|.
|-
!style="background:silver; color:black" align="left" valign="top" |Material to be etched
|style="background:WhiteSmoke; color:black"|
*E-beam deposited Ti
|.
|-
!style="background:silver; color:black" align="left" valign="top" rowspan="1"|Mask information
|style="background:WhiteSmoke; color:black"|
*E-beam resist mask:
# 400nm of spin coated ZEP520A e-beam resist
#Patterned by E-beam lithography
|.
|-
!style="background:silver; color:black" align="left" valign="top"|Features to be etched
|style="background:WhiteSmoke; color:black"|
*300nm - 3µm dots and lines + a square of 200µmx200µm
|.
|-
!style="background:silver; color:black" align="left" valign="top"|Etch depth
|style="background:WhiteSmoke; color:black"|
*300nm
|
*~270 nm
|-
!style="background:silver; color:black" align="left" valign="top"|Etch rate
|style="background:WhiteSmoke; color:black"|
*>80nm/min
|
*22nm/min +- 0.3nm/min (one standard deviation)
|-
!style="background:silver; color:black" align="left" valign="top"|Etch rate uniformity
|style="background:WhiteSmoke; color:black"|
*<+-2%
|
*+-(0.2% +-0.2%)
|-
!style="background:silver; color:black" align="left" valign="top"|Reproducibility
|style="background:WhiteSmoke; color:black"|
*<+-2%
|
*+-(0.8% +-0.5%)
|-
!style="background:silver; color:black" align="left" valign="top"|Selectivity (Au etch rate/ZEP etch rate)
|style="background:WhiteSmoke; color:black"|
*At least 1:1
|
*0.7:1
|-
!style="background:silver; color:black" align="left" valign="top"|Etch profile
|style="background:WhiteSmoke; color:black"|
*70-90dg.
|
*~65dg @270nm 
*~77dg @123nm
|}


====Process parameters for the acceptance test====
===Process parameters===
{| border="2" cellspacing="2" cellpadding="3"  
To find the optimal parameters, Design of Experiments was applied with the intervals shown on the figure below. The final optimized recipe is listed in the table.
{| align=left border="2" cellspacing="2" cellpadding="3"  
!Parameter
!Parameter
!Ti etch acceptance
!Optimized etch
!DoE low value
!DoE high value
|rowspan="11"|[[image:KHARA-MLS-DoE.png|450x450px|thumb|center|Design of Experiments setup used to find optimal etch of the multi layers stack. Centerpoints are not shown on the figure. The parameters varied were Beam current, Beam Voltage, Accelerator Voltage, and Incident Angle.]]
|-
|-
|Neutalizer current [mA]
|Neutalizer current [mA]
|450
|450
|550
|550
|-
|-
|RF Power [W]
|RF Power [W]
|1200
|800
| -
| -
|-
|-
|Beam current [mA]
|Beam current [mA]
|400
|400
|500
|500
|-
|-
|Beam voltage [V]
|Beam voltage [V]
|500
|400
|600
|600
|-
|-
|Beam accelerator voltage
|Beam accelerator voltage
|500
|400
|400
|600
|-
|-
|Ar flow to neutralizer [sccm]
|Ar flow to neutralizer [sccm]
|6.0
|5.0
| -
| -
|-
|-
|Ar flow to beam [sccm]
|Ar flow to beam [sccm]
|6.0
|10.0
| -
| -
|-
|-
|Rotation speed [rpm]
|Rotation speed [rpm]
|20
|20
| -
| -
|-
|-
|Stage angle [degrees]
|Stage angle [degrees]
|20
|5
|5
|15
|-
|Helium backside cooling [Torr]
|37.5
| -
| -
|-
|-
|}
|}
<br clear="all"/>
===Some SEM profile images of the etched stacks===
{| border="1" cellspacing="1" cellpadding="2"
|
[[image:IBE magnetic stack A19-13.jpg|300x300px|thumb|center|Magnetic stack of Ta/MnIr/NiFe/Ta/Tao/Ta/MnIr/NiFe/Ta etched with the optimal parameters shown above. Redeposition of etched material at photo resist. Profile ~78°]]
|
[[image:IBE magnetic stack A16-13.jpg|300x300px|thumb|center|Etched magnetic stack with poor structure transfer, the parameters chosen was clearly not optimal. Chosen etch parameters result in severe footing]]
|
[[image:IBE magnetic stack A3-13.jpg|300x300px|thumb|center|Etched magnetic stack with poor structure transfer, the parameters chosen was clearly not optimal. Chosen etch parameters result in severe trenching]]
|}
For a good pattern transfer with IBE a large amount of redeposition on the resist edge has been observed. To reduce this redeposition the best option seems to be to use a photo resist just thick enough for the wanted etch depth. An alternative is sidewall sputtering at low incident angle. However experiments have shown poor cleaning rate and for narrow structures low angles will give rise to shadowing effects.
===Endpoint detection with SIMS===


{| border="1" cellspacing="1" cellpadding="2"
|[[image:SIMS_end_point_detection.png|300x300px|thumb|center|The endpoint for etching is determined by the integrated SIMS]]
|}
End point detection is achieved by SIMS, and the etch rate is approximately 25 Nm/min.




===Problems with resists stripping after etching===
Resist stripping after the etch can be hard due to burned resist, to remedy this try to lower the current. Changing the currect will chance the sidewall angle and new studies of etch profiles will be necessary. For help, discussion and further info please contact [mailto:khara@dtu.dk Kristian Hagsted Rasmussen] or the dry etch group [mailto:dryetch@nanolab.dtu.dk].


===Some SEM profile images of the etched Ti===
===Design of Experiment results===
{| border="1" cellspacing="1" cellpadding="2"  
The etch rate and corner angle are dependent on several parameters each. Below two graphs showing these dependencies are shown. Note that the values are fitted and may not represent the actual value after etch, however feel free to use the graphs to estimate the values for your test run.
!
{| border="1" cellspacing="1" cellpadding="2"
[[image:IBE acceptance Ti S10-4.jpg|300x300px|thumb|center|Ti s10-4: 270nm deep - 500nm line. all zep has gone. Profile: ~65 dg.]]
|[[image:IBE magnetic DoE etch rate.jpg |600x300px|thumb|center|The etch rate did not show any dependency on incident angle. The shown results are fitted to the DoE data and may not give an accurate measure of etch rate.]]
!
|[[image:IBE magnetic DoE Corner Angle.jpg|300x300px|thumb|center|The corner angle for the etch samples showed a dependency on all parameters. The general trends can be found from the plot, however for etch structures the resultant angle may differ.]]
[[image:IBE acceptance Ti S10-5.jpg|300x300px|thumb|center|Ti s10-5: 270nm deep - 300nm line. All zep has gone. Profile: ~65 dg.]]
!
[[image:IBE acceptance Ti S7 5.jpg|300x300px|thumb|center|Ti S7 5: 123nm deep - 300nm line. Still zep left. Profile: ~77 dg ]]
|}
|}
===Conclusions===
* Etch rate around 20 nm/min with optimized recipe.
* Good feature definition after etch.
* Good end point detection by SIMS.
* Burned resist: Lower current, 300 mA can limit resist burning. Note this <b>will</b> affect pattern transfer.
* Hare ears (also called fences) due to redeposition, thinner resist can limit the size.

Latest revision as of 15:36, 6 February 2023

Feedback to this page: click here
The work on this page was done Kristian Hagsted Rasmussen, DTU Nanolab, unless otherwise stated

Etching magnetic stacks

Magnetic stacks can be etched or more precisly milled in the Ion Beam Etcher (IBE). Below is presented some work done on milling stacks of magnetic layers.


Results of Design of Experiments optimization of magnetic stack etching (Kristian Hagsted Rasmussen@nanotech.dtu.dk spring 2011)

Process parameters

To find the optimal parameters, Design of Experiments was applied with the intervals shown on the figure below. The final optimized recipe is listed in the table.

Parameter Optimized etch DoE low value DoE high value
Design of Experiments setup used to find optimal etch of the multi layers stack. Centerpoints are not shown on the figure. The parameters varied were Beam current, Beam Voltage, Accelerator Voltage, and Incident Angle.
Neutalizer current [mA] 450 450 550
RF Power [W] 800 - -
Beam current [mA] 400 400 500
Beam voltage [V] 500 400 600
Beam accelerator voltage 500 400 600
Ar flow to neutralizer [sccm] 5.0 - -
Ar flow to beam [sccm] 10.0 - -
Rotation speed [rpm] 20 - -
Stage angle [degrees] 5 5 15
Helium backside cooling [Torr] 37.5 - -


Some SEM profile images of the etched stacks

Magnetic stack of Ta/MnIr/NiFe/Ta/Tao/Ta/MnIr/NiFe/Ta etched with the optimal parameters shown above. Redeposition of etched material at photo resist. Profile ~78°
Etched magnetic stack with poor structure transfer, the parameters chosen was clearly not optimal. Chosen etch parameters result in severe footing
Etched magnetic stack with poor structure transfer, the parameters chosen was clearly not optimal. Chosen etch parameters result in severe trenching

For a good pattern transfer with IBE a large amount of redeposition on the resist edge has been observed. To reduce this redeposition the best option seems to be to use a photo resist just thick enough for the wanted etch depth. An alternative is sidewall sputtering at low incident angle. However experiments have shown poor cleaning rate and for narrow structures low angles will give rise to shadowing effects.

Endpoint detection with SIMS

The endpoint for etching is determined by the integrated SIMS

End point detection is achieved by SIMS, and the etch rate is approximately 25 Nm/min.


Problems with resists stripping after etching

Resist stripping after the etch can be hard due to burned resist, to remedy this try to lower the current. Changing the currect will chance the sidewall angle and new studies of etch profiles will be necessary. For help, discussion and further info please contact Kristian Hagsted Rasmussen or the dry etch group [1].

Design of Experiment results

The etch rate and corner angle are dependent on several parameters each. Below two graphs showing these dependencies are shown. Note that the values are fitted and may not represent the actual value after etch, however feel free to use the graphs to estimate the values for your test run.

The etch rate did not show any dependency on incident angle. The shown results are fitted to the DoE data and may not give an accurate measure of etch rate.
The corner angle for the etch samples showed a dependency on all parameters. The general trends can be found from the plot, however for etch structures the resultant angle may differ.

Conclusions

  • Etch rate around 20 nm/min with optimized recipe.
  • Good feature definition after etch.
  • Good end point detection by SIMS.
  • Burned resist: Lower current, 300 mA can limit resist burning. Note this will affect pattern transfer.
  • Hare ears (also called fences) due to redeposition, thinner resist can limit the size.