Specific Process Knowledge/Lithography/EBeamLithography: Difference between revisions

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'''Feedback to this page''': '''[mailto:labadviser@danchip.dtu.dk?Subject=Feed%20back%20from%20page%20http://labadviser.danchip.dtu.dk/index.php/Specific_Process_Knowledge/Lithography/EBeamLithography click here]'''
'''Feedback to this page''': '''[mailto:labadviser@nanolab.dtu.dk?Subject=Feed%20back%20from%20page%20http://labadviser.nanolab.dtu.dk/index.php/Specific_Process_Knowledge/Lithography/EBeamLithography click here]'''


<div class="keywords" style="display:none;">ebl e-beam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam ebeam writer e-beamwriter ebeamwriter e-beamlithography</div>
Content and illustration by Thomas Pedersen, DTU Nanolab unless otherwise noted.


[[Image:jbx9500.jpg|500x500px|thumb|JEOL JBX-9500 E-beam writer positioned in room E-2]]
[[Category: Equipment |Lithography exposure]]
[[Category: Lithography|Exposure]]
<div class="keywords" style="display:none;">ebl e-beam writer e-beamwriter ebeamwriter e-beamlithography</div>


[[File:TPE02803.jpg|right|600px]]


=Quick links=
[[Specific Process Knowledge/Lithography/EBeamLithography/JEOLRequest|Exposure slot request]]


=Performance of the e-beam writers at DTU Danchip=
[[Specific_Process_Knowledge/Lithography/EBeamLithography/JEOL 9500 User Guide|JEOL 9500 User Guide]]
 
[[Specific_Process_Knowledge/Lithography/EBeamLithography/FirstEBL|My first JEOL 9500 exposure tutorial]]
 
[[Specific_Process_Knowledge/Lithography/EBeamLithography/JEOLAlignment|Alignment exposure]]
 
[[Specific_Process_Knowledge/Lithography/EBeamLithography/Cassettes|JEOL cassette specifications]]
 
[[Specific_Process_Knowledge/Lithography/EBeamLithography/BEAMER|Beamer guide]]
 
[[Specific_Process_Knowledge/Lithography/EBeamLithography/TRACER|Tracer guide]]
 
[[Specific Process Knowledge/Lithography/EBeamLithography/EBLProcessExamples|EBL process examples]]
 
[[Specific_Process_Knowledge/Lithography/EBeamLithography/Dose_Testing|Dose testing setups for JEOL 9500]]
 
= Introduction to E-beam lithography at DTU Nanolab =
 
DTU Nanolab has two E-beam writing systems, a JEOL JBX-9500 FSZ and a Raith eLINE Plus. The two systems are very different and new users should consult the EBL team to dertermine which system is appropriate for a particular project or type of sample. The general specifications of the two tools are given in the table below and may serve as a guideline for choice of system to use, especially the pros and cons list at the end of the table. Newcommers to EBL should start by watching our '''[https://youtu.be/2bFUO201DS4 JEOL 9500 process video]''' to see how a typical process is done.
 
 
Compared to UV lithography EBL is somewhat more complicated and in general a significantly longer process. Writing time (per area) is much higher and thus EBL is only adviseable for structures with Critical Dimensions (CD) below 1 µm. For CD equal to or higher than 1 µm please consider our '''[[Specific_Process_Knowledge/Lithography/UVExposure#Aligner:_Maskless_02 | Maskless Aligner tools.]]'''
 
 
== Getting started and training in E-Beam Lithography ==
The JEOL 9500 system has a fairly steep learning curve and the information below and corresponding links are fairly comprehensive and describes uses and options that first time users of the JEOL 9500 system should not venture into. Instead, first time users of the JEOL 9500 system should consult our dedicated [[Specific Process Knowledge/Lithography/EBeamLithography/FirstEBL|My First JEOL 9500 Exposure guide]] which showcases a JEOL 9500 job from start to finish in a tutorial form.
 
Please request training in E-Beam lithography by sending an email with your process flow to [mailto:training@nanolab.dtu.dk training@nanolab.dtu.dk].
 
==EBL staff at DTU Nanolab==
Questions related to E-beam lithography should be directed to the EBL staff.
 
{| class="wikitable"
|-
|[[File:thope.png|150px]] || [[File:pxshi.png|150px]] || [[File:elelop.png|150px]] || [[File:meenadh.png|150px]]
|-
|[mailto:thope@dtu.dk Thomas Pedersen]
JEOL 9500 & Raith E-Line
|| [mailto:pxshi@dtu.dk Peixiong Shi]
JEOL 9500
|| [mailto:elelop@dtu.dk Elena Lopez Aymerich]
JEOL 9500
|| [mailto:meenadh@dtu.dk Meena Dhankhar]
Raith E-Line
|}
 
== JEOL 9500 and Raith eLine Plus specifications ==


{| border="2" cellspacing="0" cellpadding="10" width="60%"
{| border="2" cellspacing="0" cellpadding="10" width="60%"
!colspan="4" border="none" style="background:silver; color:black;" align="center"|EBL system comparison table
|-


!colspan="2" border="none" style="background:silver; color:black;" align="center"|Equipment  
!colspan="2" border="none" style="background:silver; color:black;" align="center"|Equipment  
|style="background:silver; color:black;" align="left"|'''[[Specific_Process_Knowledge/Lithography/EBeamLithography/JEOL_JBX-9500FSZ|JEOL JBX-9500FSZ]]'''
|style="background:silver; color:black;" align="left"|'''JEOL JBX-9500FSZ'''
|style="background:silver; color:black;" align="left"|'''[[Specific_Process_Knowledge/Lithography/EBeamLithography/RaithElphy|Raith Elphy]]'''
|style="background:silver; color:black;" align="left"|'''[[Specific_Process_Knowledge/Lithography/EBeamLithography/eLINE|Raith eLINE Plus]]'''
|-
|-


!style="background:silver; color:black" align="left" valign="top" rowspan="2"|Performance
!style="background:silver; color:black" align="left" valign="top" rowspan="2"|Performance
|style="background:LightGrey; color:black"|Resolution
|style="background:LightGrey; color:black"|Resolution
|style="background:WhiteSmoke; color:black"|~5 nm beam diameter, ~10 nm lines obtained in 50 nm thick resist (CSAR)
|style="background:WhiteSmoke; color:black"|8 nm  
|style="background:WhiteSmoke; color:black"|~70 nm lines obtained in 50 nm thick resist (CSAR)
|style="background:WhiteSmoke; color:black"|35 nm
|-
|-


|style="background:LightGrey; color:black"|Maximum writing area without stitching
|style="background:LightGrey; color:black"|Maximum writing field
|style="background:WhiteSmoke; color:black"|1mm x 1mm
|style="background:WhiteSmoke; color:black"|1mm x 1mm
|style="background:WhiteSmoke; color:black"|1mm x 1mm
|style="background:WhiteSmoke; color:black"|2mm x 2mm<sup>a</sup>
|-
|-


!style="background:silver; color:black" align="left" valign="top" rowspan="6"|Process parameter range
!style="background:silver; color:black" align="left" valign="top" rowspan="6"|Process parameter range
|style="background:LightGrey; color:black"|E-beam voltage
|style="background:LightGrey; color:black"|Acceleration voltage
|style="background:WhiteSmoke; color:black"|100 kV
|style="background:WhiteSmoke; color:black"|100 kV
|style="background:WhiteSmoke; color:black"|5-25 kV
|style="background:WhiteSmoke; color:black"|1-30 kV
|-
|-


|style="background:LightGrey; color:black"|Scanning speed
|style="background:LightGrey; color:black"|Scan speed
|style="background:WhiteSmoke; color:black"|100 MHz
|style="background:WhiteSmoke; color:black"|200 MHz
|style="background:WhiteSmoke; color:black"|6 MHz
|style="background:WhiteSmoke; color:black"|20 MHz
|-
|-


|style="background:LightGrey; color:black"|Min. electron beam size
|style="background:LightGrey; color:black"|Min. electron beam size
|style="background:WhiteSmoke; color:black"|4 nm
|style="background:WhiteSmoke; color:black"|4 nm
|style="background:WhiteSmoke; color:black"|Not measured
|style="background:WhiteSmoke; color:black"|10 nm
|-
|-


|style="background:LightGrey; color:black"|Min. step size
|style="background:LightGrey; color:black"|Min. step size
|style="background:WhiteSmoke; color:black"|0.25 nm
|style="background:WhiteSmoke; color:black"|1 nm
|style="background:WhiteSmoke; color:black"|1 nm
|style="background:WhiteSmoke; color:black"|1 nm<sup>a</sup>
|-
|-


|style="background:LightGrey; color:black"|Beam current range
|style="background:LightGrey; color:black"|Beam current range
|style="background:WhiteSmoke; color:black"|0.1nA to 60nA in normal conditions
|style="background:WhiteSmoke; color:black"|0.1 nA to 100 nA
|style="background:WhiteSmoke; color:black"|0.01 to 5 nA<sup>a</sup>
|style="background:WhiteSmoke; color:black"|0.01 to 12 nA
|-
|-


|style="background:LightGrey; color:black"|Dose range
|style="background:LightGrey; color:black"|Minimum dwell time
|style="background:WhiteSmoke; color:black"| 0.001 - 100000µC/cm<sup>2</sup>
|style="background:WhiteSmoke; color:black"| 5 ns
|style="background:WhiteSmoke; color:black"| 0.000001 µC/cm<sup>2</sup> to infinity<sup>a,b</sup>
|style="background:WhiteSmoke; color:black"| 50 ns
|-
|-


Line 65: Line 119:
*2 x 4" wafers
*2 x 4" wafers
*1 x 6" wafer
*1 x 6" wafer
*Special wafer cassette with slit openings of 20 mm (position A), 12 mm (position B), 8 mm (position C) and 4 mm (position D).
*1 x 8" wafer
|style="background:WhiteSmoke; color:black"| Only chips, max dimension about 20 x 20 mm.
*Special chip cassette with slit openings of 20 mm (position A), 12 mm (position B), 8 mm (position C) and 4 mm (position D).
(If at least one dimension is less than 23 mm, bigger chips (e.g. 40 x 20) may be allowed - contact Danchip)
|style="background:WhiteSmoke; color:black"|  
*Chips up to 75 x 75 mm  
*4" wafer holder
*6" wafer holder (stage movement limited to central 100 x 100 mm region)
|-
|-


Line 79: Line 136:
*Wafers with layers of silicon oxide or silicon (oxy)nitride
*Wafers with layers of silicon oxide or silicon (oxy)nitride
*Wafers with layers of metal
*Wafers with layers of metal
|}
|-


<sup>a</sup> The Raith tool with the attached LEO SEM allows ample freedom in the choice of most parameters. The limits indicated here refer to best cases and may be further constrained by your current selection of microscope and patterning parameters.
!style="background:silver; color:black" align="left" valign="top" rowspan="2"|General considerations
|style="background:LightGrey; color:black"|Pros
|style="background:WhiteSmoke; color:black"|
*100 kV
*Sub 10 nm resolution
*Automatic beam optimization
*High current and process speed
*Automatic sample exchange
*High level of programmability for automatic job execution
*EBL workhorse for large designs
|style="background:WhiteSmoke; color:black"|
*Readily available
*More intuitive software
*Easier SEM mode alignment
*Build in SEM automation for post exposure process control
*2D stacks (HBN/graphene) allowed without Al coating
*Excellent for small chips or small area design exposure
|-


<sup>b</sup> For all applicable purposes.
|style="background:LightGrey; color:black"|Cons
<br clear="all" />
|style="background:WhiteSmoke; color:black"|
*Steep learning curve
*Availability - booking calendar is usually full 5 weeks ahead
|style="background:WhiteSmoke; color:black"|
*Maximum 30 kV
*User dependent performance/beam optimization
*Minimum feature size >35 nm
*Difficult to handle design files >1 GB
*Slower writing speed


= E-beam resists =
|}


<span style="font-size: 90%; text-align: right;">[[Specific_Process_Knowledge/Lithography/EBeamLithography#top|Go to top of this page]]</span>
=Fundementals of EBL pattern writing=
==Electron exposure==
An E-beam writing system utilizes a focused electron beam to expose an electron sensitive resist in order to define a pattern on a substrate. For a positive tone resist the electron beam will scission polymer bonds within the resist to increase the dissolution rate when the substrate is placed in a developer solution. In this way the exposed part of the resist can be dissolved while maintaining the unexposed resist on the substrate. For a negative resist the electron beam will make the resist less soluble and hence the unexposed resist can be removed with a developer.


== E-beam resists in the cleanroom ==
{| style="border: none; border-spacing: 0; margin: 1em auto; text-align: center;"
 
|-
[[File:bottle.jpg|150px|right]]
| [[image:PositiveNegative.png|700px]]
 
|-
We recommend all groups or users to have their own bottle of e-beam resist inside the cleanroom.
| colspan="1" style="text-align:center;|
Exposure and development result of a positive resist (left) and a negative resist (right).
|}


* Find a blue-capped glass bottle in the cupboard next to office 055 in 346 (outside the cleanroom).
* Bring the bottle inside gowning; clean it thoroughly '''on the outside''' with water or alcohol
* Bring the bottle to a fumehood inside the cleanroom; clean the bottle and the lid thoroughly '''on the inside''' with the main solvent of your resist. For CSAR, ZEP, mr EBL, and most PMMAs, it is anisole. If in doubt which solvent your e-beam resist contains, read the MSDS of the resist to be found [http://kemibrug.dk/searchpage/ here].
* If you need to dilute the resist, find a measurement beaker and clean it thorughly in same solvent as your own bottle. For CSAR, ZEP, mr EBL, and anisole-based PMMA, you can use the measurement beaker in the box inside the fumehood in E-4.
* Let the bottle dry in the fumehood.
* Bring the (main) bottle of resist to the fumehood. Carefully unscrew the lid of the resist bottle. '''If necessary, wipe the thread of the resist bottle before you pour resist into your own bottle'''; dried resists may sit on the thread and be transferred into your bottle (or worse into the large resist bottle) when pouring.
* Clean all bottles on the outside with anisole or IPA, let them fume off in the fumehood. Clean the measurement beaker as well.
* Find a label to your resist bottle; bottles without labels will be removed from the cleanroom.
* Write name, Lotnumber, group and date on your bottle.


In order to define a pattern in the resist enough electrons have to be supplied to the exposed area, i.e. the exposure dose has to be sufficiently high. The area exposure dose is expressed in units of µC/cm<sup>2</sup>. The dose to clear the resist (for a positive resist) can be obtained from a contrast curve such as the one below. Dose to clear varies a lot between different resist types and is also dependent on processing parameters such as


When spin coating e-beam resist, you should use a pipette to transfer resist from your bottle to the substrate. If you pour the resist directly from your bottle, you will leave resist in the thread that will soon dry out and leave particles in the resist.
*Acceleration voltage
The disposable pipettes need to be thoroughly cleaned with a N2 gun before use (app. 20 s). After some trainning, you can obtain particle-free 4" wafers if bottle and pipette (and spin coater) are properly cleaned.
*Resist thickness
<br>
*Developer agent and concentration
Keep your resist bottles in up-right position, do not tilt or shake them too much, this can spread particles from the sidewall into the resist.
*Post exposure baking


<br>


== E-beam resists and Process flow ==
In general it is always advisable to do a dose test of the pattern one intends to define to experimentally establish the optimum dose. For more information on resist dose please refer to the [[Specific Process Knowledge/Lithography/EBeamLithography/EBLsubstratePrep| EBL substrate preparation guide.]]


The table describes the e-beam resist used in the cleanroom for standard e-beam exposure. Some of resists are not provided by DTU Danchip and some are not yet approved for common use in the cleanroom and are currently being tested. If you wish to test some of these resists or other resists, please contact [mailto:lithography@danchip.dtu.dk Lithography].


Standard DTU Danchip resists purchased and tested by DTU Danchip:


{|border="1" cellspacing="1" cellpadding="3" style="text-align:left;" width="95%"
{| style="border: none; border-spacing: 0; margin: 1em auto; text-align: center;"
|-
|-
| [[image:ContrastCurvesCSAR March2016 log.png|600px]]
|-
| colspan="1" style="text-align:center;|
Contrast curve for AR-P 6200 exposed at 100 kV with the JEOL 9500 exposure system. Illustration: Tine Greibe.
|}


|-
==Writing principle==
|-style="background:silver; color:black"
Both of our EBL systems lets the user define a desired area dose to expose the resist with. Based on the beam current the systems will then calculate the necessary beam dwell to achieve the requested dose in the drawn areas. It is always the drawn (filled) parts of a pattern that will get exposed. In addition to area dose the Raith eLine tool allows the user to define a line dose for exposure of single lines. The JEOL 9500 system does not allow that.
|'''Resist'''
|'''Polarity'''
|'''Manufacturer'''
|'''Comments'''
|'''Technical reports'''
|'''Spin Coater'''
|'''Thinner'''
|'''Developer'''
|'''Rinse'''
|'''Remover'''
|'''Process flows (in docx-format)'''
 
|-


|-
Before the pattern is exposed onto the substrate the pattern is broken down (fractured) into simple trapezoids and each trapezoidal shape is filled with beam shots, i.e. individual beam positions that together will make up the pattern. This is illustrated below with a simple pattern consisting of a square. The actual beam spot size is dependent on beam current and the pitch between beam positions is (within certain limitations) defined by the user.  
|-style="background:WhiteSmoke; color:black"
|'''[[Specific_Process_Knowledge/Lithography/CSAR|CSAR]]'''
|Positive
|[http://www.allresist.com AllResist]
|Standard positive resist, very similar to ZEP520.
|[[media:Allresist_CSAR62_English.pdf‎|Allresist_CSAR62_English.pdf‎]],, [[media:CSAR_62_Abstract_Allresist.pdf‎|CSAR_62_Abstract_Allresist.pdf‎]]
|See table <u>[[Specific_Process_Knowledge/Lithography/Coaters#Coaters:_Comparison_Table|here]] </u>
|Anisole
|AR-600-546, AR-600-548, N50, MIBK:IPA
|IPA
|AR-600-71, 1165 Remover
|[[media:Process_Flow_CSAR.docx‎|Process Flow CSAR.docx‎]] <br> [[media:Process Flow CSAR ESPACER.docx|Process Flow CSAR with ESPACER]] <br> [[media:Process Flow CSAR with Al.docx|Process Flow CSAR with Al]] <br> [[media:Process_Flow_LOR5A_CSAR_Developer_TMAH_Manual.docx|Process Flow LOR5A with CSAR]] <br>




{| style="border: none; border-spacing: 0; margin: 1em auto; text-align: center;"
|-
|-
|-style="background:LightGrey; color:black"
| [[image:EBLBeamShots.png|200px]]
|'''[[Specific_Process_Knowledge/Lithography/ZEP520A|ZEP520A]]''' (not supplied by Danchip anymore)
|-
|Positive resist, contact [mailto:Lithography@danchip.dtu.dk Lithography] if you plan to use this resist
| colspan="1" style="text-align:center;|
|ZEON
Simple shape filled in with beam shots.
|Positive resist
|}
|[[media:ZEP520A.pdf|ZEP520A.pdf]], [[media:ZEP520A.xls|ZEP520A spin curves on SSE Spinner]]
|See table <u>[[Specific_Process_Knowledge/Lithography/Coaters#Coaters:_Comparison_Table|here]] </u>
|Anisole
|ZED-N50/Hexyl Acetate,n-amyl acetate, oxylene. [[media:JJAP-51-06FC05.pdf‎|JJAP-51-06FC05.pdf‎]], [[media:JVB001037.pdf‎|JVB001037.pdf‎]]
|IPA
|acetone/1165
|[[media:Process_Flow_ZEP.docx|Process_Flow_ZEP.docx]]
 




The electron source is continuously emitting electrons and exposure of the beam towards the sample is controlled by a beam blanker. The position of the beam is controlled by the beam deflector and scanning coils. The pattern is written one beam shot at a time in a serial process as this


|-
#Beam positioning for 1st beam position of current trapezoidal shape
|-style="background:WhiteSmoke; color:black"
#Unblank the beam
|'''[[Specific_Process_Knowledge/Lithography/ARP617|Copolymer AR-P 617]]'''
##Exposure
|Positive
##Reposition for next beam shot
|[http://www.allresist.com AllResist]
#Blank the beam at end of trapezoidal shape
|Approved, not tested yet. Used for trilayer (PE-free) resist-stack or double-layer lift-off resist stack. Please contact [mailto:Lithography@danchip.dtu.dk Lithography] for information.
|[[media:AR_P617.pdf‎|AR_P617.pdf‎]]
|See table <u>[[Specific_Process_Knowledge/Lithography/Coaters#Coaters:_Comparison_Table|here]] </u>
|PGME
|AR 600-55, MIBK:IPA
|
|acetone/1165
|Trilayer stack: [[media:Process_Flow_Trilayer_Ebeam_Resist.docx‎|Process_Flow_Trilayer_Ebeam_Resist.docx‎]]
 
|-
|-style="background:LightGrey; color:black"
|'''[[Specific_Process_Knowledge/Lithography/mrEBL6000|mr EBL 6000.1]]'''
|Negative
|[http://http://www.microresist.de/home_en.htm MicroResist]
|Standard negative resist
|[[media:mrEBL6000 Processing Guidelines.pdf‎|mrEBL6000 processing Guidelines.pdf‎]]
|See table <u>[[Specific_Process_Knowledge/Lithography/Coaters#Coaters:_Comparison_Table|here]] </u>
|Anisole
|mr DEV
|IPA
|mr REM
|[[media:Process_Flow_mrEBL6000.docx‎|Process_Flow_mrEBL6000.docx‎]]


Steps 2.1 and 2.2 continues in a loop until all beam shots of the current trapezoidal shape has been executed after which the beam is blanked and the system moves on to the next trapezoidal shape. It is obvious that exposure in such a way is relatively slow and has an overhead on top of the actual exposure time since time is also spent on beam positioning and blanking/unblanking the beam.


==Exposure grid and exposure field==
Both systems have a maximum writing field size of 1000 x 1000 µm<sup>2</sup> since the deflection of the beam is limited to ±500 µm in both x- and y-direction. Patterns inside a writing filed is written by beam deflection only and hence the substrate stage remains stationary. Geometry larger than a single writing field will be fractured across multiple writing fields and hence between fields the substrate stage will move to reposition the substrate directly under the column as illustrated below. 


{| style="border: none; border-spacing: 0; margin: 1em auto; text-align: center;"
|-
|-
|-style="background:WhiteSmoke; color:black"
| [[image:EBLFields.png|600px]]
|'''HSQ (XR-1541)'''
|-  
|Negative
| colspan="1" style="text-align:center;|
|DOW Corning
Illustration of a waveguide spanning four exposure fields. Between fields the stage will reposition the substrate below the column.
|Approved. Standard negative resist
|}
|[[media:DowCorningHSQA.pdf|HSQ Dow Corning]], [[media:MSDS HSQ.pdf|MSDS HSQ]]
|See table <u>[[Specific_Process_Knowledge/Lithography/Coaters#Coaters:_Comparison_Table|here]] </u>
|
|TMAH, AZ400K:H2O
|H2O
|
|[[media:Process Flow HSQ.docx|process flow HSQ]]
[[/High resolution patterning with HSQ|High resolution patterning with HSQ]]
|-
|-style="background:LightGrey; color:black"
|'''AR-N 7520'''
|Negative
|[http://www.allresist.com AllResist]
|Both e-beam, DUV and UV-sensitive resist. Currently being tested, contact [mailto:pxshi@danchip.dtu.dk Peixiong Shi] for information.
|[[media:AR-N7500-7520.pdf‎|AR-N7500-7520.pdf‎]]
|See table <u>[[Specific_Process_Knowledge/Lithography/Coaters#Coaters:_Comparison_Table|here]] </u>
|PGMEA
|AR 300-47, TMAH
|H2O
|
|


If neighbouring writing fields are not properly aligned features fractured across multiple writing fields may suffer from stitching errors, i.e. pattern discontinuities where the patterns do not align properly to each other. On the JEOL system write field alignment is ensured by a fully automated calibration sequence using internal alignment features. This ensures field stitching usually on the order of 10-15 nm or less. On the Raith system write field alignment is performed on the users own substrate and accuracy can vary.


|}
The beam shots described above are placed onto the systems exposure grid, hence the resolution of beam shot placement is governed by the exposure grid. The resolution of this grid is determined by the positioning DAC of the system, on the JEOL 9500 this is 20 bit and on the Raith eLine it is 16 bit. Hence the JEOL 9500 system has in principle 2<sup>20</sup> = 1.048.576 grid positions along each axis while the Raith system has 2<sup>16</sup> = 65.384 grid positions along each axis. This means the JEOL system can maintain a 1 nm exposure grid over the entire 1000 x 1000 µm<sup>2</sup> writing field whereas the Raith tool will have a 16 nm exposure grid at the maximum writing field.




Non-standard DTU Danchip resists not purchased by DTU Danchip:
==Beam pitch, beam current and exposure dose relationship==
A sample is exposed at a certain beam current. On the JEOL system this is selectable (in certain discrete steps) while on the Raith tool the beam current is bound by the choice of acceleration voltage and aperture. The user will input an area dose for the resist to be exposed with and the system will calculate the shot time (dwell time) of the beam to provide the requested dose. It is clear that high doses will require long dwell times whereas low doses will require short dwell times for the same beam current. There is however another important parameter to the dwell time calculation and that is the beam/shot pitch, i.e. how far beam shots are placed from each other. The beam scanner on the JEOL 9500 system is 100 MHz, thus the temporal resolution is 10 ns and it is not possible to have a beam shot (or dwell time) less than 10 ns. The Raith system has a 20 MHz beam scanner and hence the minimum shot time is 50 ns. This, in combination with beam current and exposure dose will set a lower limit on the beam pitch.


{|border="1" cellspacing="1" cellpadding="3" style="text-align:left;" width="95%"
The relation might not be obvious at first and is illustrated below. The two identical features are filled with beam shots at two different pitches. the right version has a lower beam pitch (half of the other) and thus there are simply many more beam shots. Consequently, to provide the same area exposure dose the shot time for the right side feature will be much shorter. At half the pitch there will be four times the number of beam shots and thus the shot time will be 1/4 the shot time of the left feature.
|-


{| style="border: none; border-spacing: 0; margin: 1em auto; text-align: center;"
|-
|-
|-style="background:silver; color:black"
| [[image:BeamPitch.png|500px]]
|'''Resist'''
|-  
|'''Polarity'''
| colspan="1" style="text-align:center;|
|'''Manufacturer'''
Example feature filled with beam shots at one times beam diameter (left) and half beam diameter (right).
|'''Comments'''
|}
|'''Technical reports'''
|'''Spinner'''
|'''Thinner'''
|'''Developer'''
|'''Rinse'''
|'''Remover'''
|'''Process flows (in docx-format)'''
 
|-
 


The shot time can be calculated as ''t = D·p<sup>2</sup>/I'', where ''D'' is the dose in µC/cm<sup>2</sup>, ''p'' is beam pitch and ''I'' is current. As a practical example let us consider an exposure at 2 nA beam current and a desired dose of 250 µC/cm<sup>2</sup>. At 4 nm beam pitch the shot time will come out to 20 ns, while at 2 nm beam pitch it will come out at 5 ns and thus violate the hardware limitation of 10 ns for the JEOL system. In order to expose the pattern with 2 nm shot pitch one would have to choose a lower beam current at the expense of increased writing time.


The shot time is in fact such an important number that both systems will tell the user what it is. On the JEOL system the shot time is displayed in a table after job compilation, see below. On the Raith tool it is indicated in the '''Patterning Parameter Calculation''' box, see below.




{| style="border: none; border-spacing: 0; margin: 1em auto; text-align: center;"
|-
|-
|-style="background:WhiteSmoke; color:black"
| <pre>
|'''[[Specific_Process_Knowledge/Lithography/PMMA|PMMA]]'''
Start estimation writing time  -----
|Positive
Shot counting start -----
| [http://www.allresist.com AllResist]
  thopeQU23008a.v30                                              at 11-MAR-2023 14:53:40
|We have various types of PMMA in the cleanroom. Please contact [mailto:Lithography@danchip.dtu.dk Lithography] for information.
Shot counting end -----
|
|See table <u>[[Specific_Process_Knowledge/Lithography/Coaters#Coaters:_Comparison_Table|here]] </u>
|Anisole
|MIBK:IPA (1:3), IPA:H2O
|IPA
|acetone/1165/Pirahna
|
 


|-
  Seq.  writing time    shottime[nsec]  resist[uC/cm2]  stdcur[nA]  scanstep
|-style="background:LightGrey; color:black"
  1        0:52:27            16.000          200.000        2.000        16
|'''ZEP7000'''
  2        0:13:46            13.500          200.000      12.000        36
|Positive
  3        0:11:15            12.000          100.000      12.000        48
|ZEON
  4        0:12:10            13.500         200.000      12.000        36
|Not approved. Low dose to clear, can be used for trilayer (PEC-free) resist-stack. Please contact [mailto:Lithography@danchip.dtu.dk Lithography] for information.  
  5        0:11:14            12.000          100.000      12.000        48
|[[media:ZEP7000.pdf|ZEP7000.pdf]]
Total :    1:40:51
|See table <u>[[Specific_Process_Knowledge/Lithography/Coaters#Coaters:_Comparison_Table|here]] </u>
|Anisole
|ZED-500/Hexyl Acetate,n-amyl acetate, oxylene.
|IPA
|acetone/1165
|Trilayer stack: [[media:Process_Flow_Trilayer_Ebeam_Resist.docx‎|Process_Flow_Trilayer_Ebeam_Resist.docx‎]]


Estimation result file : thopeQU23008a.csv
End estimation writing making time    -----
</pre> || [[image:eLine_dose.PNG|600px]]
|-
| colspan="2" style="text-align:center;|
Shot time as calculated by the JEOL system (left) and Raith eLine system (right).
|}
|}


<br/>
==Exposure time==
 
E-beam exposure is a serial writing process and the writing time (t) will scale with dose (D), area (A) and beam current (I) as:
If the resist is not adhering properly to the substrate, the coating looks like full of pinholes and the edge is not covered, try to remove the resist, dip 30s. in BHF, rinse 5 mins and spin dry, the spin coat again.
t = D*A/I
 
<br/>
<br/>
<br/>
 
= Proximity Error Correction =
 
 
<span style="font-size: 90%; text-align: right;">[[Specific_Process_Knowledge/Lithography/EBeamLithography#top|Go to top of this page]]</span>
 
 
Even though the electron beam diameter is below 5 nm, the feature and pitch resolution in resist is limited by the forward and backward scattering of the electrons. The forward scattering depends on the electron acceleration voltage, the resist material and thickness. The backward scattering depends on the electron acceleration voltage and the substrate material [http://en.wikipedia.org/wiki/Electron-beam_lithography], [http://en.wikipedia.org/wiki/Proximity_effect_%28electron_beam_lithography%29].


As the travel distance of backscattered electrons is fairly large, e-beam patterned structures will be influenced by adjacent e-beam patterned structures, i.e. a proximity effect. These proximity effects can be avoided either by simulating a proximity error correction (PEC) in BEAMER or by using the right stack of e-beam resist.
It is thus essential to find the right balance between the area that needs to be defined and a beam current that will provide sufficient pattern fidelity and quality. During pattern writing the tool will also use time on cyclic calibration and stage movement as defined by the job path and pattern layout. The exposure time can be estimated based on the [[:File:Writing Time Estimator.xlsx|Writing Time Estimator Excel sheet]].


= Exposure information =
== Generalized workflow ==
While the EBL workflow resembles that of UV lithography there are a few additional complications and the parameter space is somewhat larger. The complications all arise from using electrons rather than light for exposure. Since a beam of electrons is used for exposure the substrate must be sufficiently conductive and grounded in order not to build up a charge. If the substrate in itself is not conductive a thin metal film or other conductive surface layer must be applied to it, read more on this in the resist section. Another complication is secondary exposure from backscattered electrons. This is a much bigger topic and covered in the pattern preparation section. A generalised workflow is shown below.


== Proximity Error Correction (PEC) in BEAMER ==
[[File:EBLWorkflow.png|1200px|frameless|center|alt=Generalized EBL workflow.|Generalized EBL workflow.]]


[[Image:beamer5.jpg|frame|250x250px|right]]
Since substrate preparation and development processes are (nearly) identical for the JEOL and Raith eLine systems they are described in common below. Pattern preparation, job preparation and job execution are fairly different between the two tools and hence these steps are described on the specific tool pages.


BEAMER is endowed with a software that corrects for proximity errors in the e-beam exposure. You can read more about this function in the BEAMER manual [[Specific_Process_Knowledge/Lithography/EBeamLithography/BEAMER|here]] and in the BEAMER presentation here [[media:BEAMERPresentation.pdf‎|BEAMERPresentation.pdf‎]].
== Substrate preparation and resist information==
Substrates must be prepared for EBL by applying an e-beam sensitive resist and possibly a discharge layer. Please consult the EBL substrate preparation guide on how to prepare your substrate and to find resist information.


The proximity error correction require a forward and a backward range parameter, alfa and beta, and a ratio of backscattered energy to the forward scattered energy, eta. As alfa depends on the electron acceleration voltage, which is constant at 100kV, alfa is in BEAMER fixed to 0.007. Help to find beta and eta can be found [http://nanolithography.gatech.edu/proximity.htm here].
*[[Specific Process Knowledge/Lithography/EBeamLithography/EBLsubstratePrep| EBL substrate preparation guide]]


Alternatively, a [http://en.wikipedia.org/wiki/Proximity_effect_%28electron_beam_lithography%29 point-spread function] can be used in BEAMER to calculate the optimised dose-variation.
== Pattern preparation ==
Pattern preparation is somewhat different depending on if a pattern is exposed on JEOL 9500 or Raith eLine Plus. Please refer to the correct pattern preparation section below.


[[Specific Process Knowledge/Lithography/EBeamLithography/JEOLPatternPreparation|Pattern preparation for exposure on JEOL 9500.]]


<br clear="all" />
[[Specific Process Knowledge/Lithography/EBeamLithography/RaithPatternPreparation|Pattern preparation for exposure on Raith eLine Plus.]]


== Trilayer resist stack ==
== Job preparation ==
As an alternative to PEC, a trilayer reists stack with a thin layer of thermally evaporated Ge can be used [http://avspublications.org/jvst/resource/1/jvstal/v19/i4/p1304_s1]. This reists stack has not yet been tested at DTU Danchip. A process flow for this procedure can be found here [[media:Process_Flow_Trilayer_Ebeam_Resist.docx‎|Process_Flow_Trilayer_Ebeam_Resist.docx‎]], but please contact [mailto:Lithography@danchip.dtu.dk Lithography] before use.
Job preparation is also different depending on if a pattern is exposed on JEOL 9500 or Raith eLine Plus. Please refer to the correct job preparation section below.


[[Specific Process Knowledge/Lithography/EBeamLithography/JEOLJobPreparation|Job preparation for exposure on JEOL 9500.]]


<br clear="all" />
[[Specific Process Knowledge/Lithography/EBeamLithography/RaithJobPreparation|Job preparation for exposure on Raith eLine Plus.]]


= Charging of non-conductive substrates=
== Job execution ==
Job execution is very different between the JEOL and Raith systems. The procedures are described on their respective user guide pages:


<span style="font-size: 90%; text-align: right;">[[Specific_Process_Knowledge/Lithography/EBeamLithography#top|Go to top of this page]]</span>
*[[Specific Process Knowledge/Lithography/EBeamLithography/JEOL 9500 User Guide|Job execution on JEOL 9500]]
*[https://labmanager.dtu.dk/d4Show.php?id=18413&mach=445 Raith eLine Plus user manual]


All substrates are grounded to the cassette when properly loaded. In a non-conducting substrate, the accumulation of charges in the substrates will however destroy the e-beam patterning. To avoid this, a charge dissipating layer is added on top of the e-beam resist; this will provide a conducting layer for the electrons to escape, while high-energy electrons will pass through the layer to expose the resist.
== Development ==


If you wish to investigate the charge dissipation using other methods than below, please contact [mailto:lithography@danchip.dtu.dk Lithography].
AR 600-546 and ZED N-50 developers are available in a semi automatic puddle developer [[Specific_Process_Knowledge/Lithography/Development#Developer:_E-beam|Developer: E-beam]] in E-4, mainly intended for development of AR-P 6200 and ZEP 520A. It has automatic recipes for puddle development cycles for 10, 30 and 60 seconds of either of the two developers, each finishing off with an IPA rinse and drying cycle. The system can handle chips, 2", 4" and 6" wafers.


== ESPACER ==


Espacer is a chemical that works as a discharging layer; it is spun onto the wafer on top of the resist and easily rinsed off the wafer after e-beam exposure. Visit this page for more information: [[Specific_Process_Knowledge/Lithography/Espacer|Espacer]]
Other resist have to be developed in the E-beam developer fumehood in E-4 in beakers. Please notice there are specific beaker sets for alkaline developers and for solvent based developers.


== Post development inspection ==
After development it is often necesarry to evaluate the result by SEM to verify feature dimensions. This can conviently be done in the Raith eLine Plus tool which apart from being an EBL tool is also a semiautomatic SEM. The strong suit of the tool is the ability to link/align a design file to the substrate and simply define image positions in the design file. The user can then set up a long list of image locations and the tool will acquire the SEM images without further user input. When set up correctly the system can acquire about one image per 5 seconds which is very advantageous for large arrays of structures. For an introduction to this, please refer to our [https://youtu.be/YoZF_6FeVb4 automatic SEM introduction video.]


== Aluminum coating ==


At DTU Danchip, we recommend to use a thin (20 nm) layer of thermally evaporated [[Specific Process Knowledge/Thin film deposition/Deposition of Aluminium|aluminum]] on top of the e-beam resist. Preferably, the thickness of Al and the e-beam dose should be optimised to the features you wish to e-beam pattern [http://nedds.co.uk/wp-content/uploads/2013/06/Greer-et-al-DRM-29-July-2012.pdf]. A good starting point is 20 nm Al; from here dose and development can be optimised to reach the resolution and feature size required.
After image acquisition the images can be semi automatically processed with ProSEM to determine feature sizes. For large image sets the software can generate an Excel sheet with various dimension outputs.


The process flow for a standard e-beam exposure on CSAR with Al on top can be found here [[media:Process Flow CSAR with Al.docx|Process Flow CSAR with Al]].
=EBL process examples=
Process examples and results can be found [[Specific Process Knowledge/Lithography/EBeamLithography/EBLProcessExamples|on this page.]]


= Literature on E-beam Lithography =
= Literature on E-beam Lithography =

Latest revision as of 12:47, 26 June 2024

Feedback to this page: click here

Content and illustration by Thomas Pedersen, DTU Nanolab unless otherwise noted.

Quick links

Exposure slot request

JEOL 9500 User Guide

My first JEOL 9500 exposure tutorial

Alignment exposure

JEOL cassette specifications

Beamer guide

Tracer guide

EBL process examples

Dose testing setups for JEOL 9500

Introduction to E-beam lithography at DTU Nanolab

DTU Nanolab has two E-beam writing systems, a JEOL JBX-9500 FSZ and a Raith eLINE Plus. The two systems are very different and new users should consult the EBL team to dertermine which system is appropriate for a particular project or type of sample. The general specifications of the two tools are given in the table below and may serve as a guideline for choice of system to use, especially the pros and cons list at the end of the table. Newcommers to EBL should start by watching our JEOL 9500 process video to see how a typical process is done.


Compared to UV lithography EBL is somewhat more complicated and in general a significantly longer process. Writing time (per area) is much higher and thus EBL is only adviseable for structures with Critical Dimensions (CD) below 1 µm. For CD equal to or higher than 1 µm please consider our Maskless Aligner tools.


Getting started and training in E-Beam Lithography

The JEOL 9500 system has a fairly steep learning curve and the information below and corresponding links are fairly comprehensive and describes uses and options that first time users of the JEOL 9500 system should not venture into. Instead, first time users of the JEOL 9500 system should consult our dedicated My First JEOL 9500 Exposure guide which showcases a JEOL 9500 job from start to finish in a tutorial form.

Please request training in E-Beam lithography by sending an email with your process flow to training@nanolab.dtu.dk.

EBL staff at DTU Nanolab

Questions related to E-beam lithography should be directed to the EBL staff.

Thomas Pedersen

JEOL 9500 & Raith E-Line

Peixiong Shi

JEOL 9500

Elena Lopez Aymerich

JEOL 9500

Meena Dhankhar

Raith E-Line

JEOL 9500 and Raith eLine Plus specifications

EBL system comparison table
Equipment JEOL JBX-9500FSZ Raith eLINE Plus
Performance Resolution 8 nm 35 nm
Maximum writing field 1mm x 1mm 1mm x 1mm
Process parameter range Acceleration voltage 100 kV 1-30 kV
Scan speed 200 MHz 20 MHz
Min. electron beam size 4 nm 10 nm
Min. step size 0.25 nm 1 nm
Beam current range 0.1 nA to 100 nA 0.01 to 12 nA
Minimum dwell time 5 ns 50 ns
Samples Batch size

Wafer cassettes:

  • 6 x 2" wafers
  • 2 x 4" wafers
  • 1 x 6" wafer
  • 1 x 8" wafer
  • Special chip cassette with slit openings of 20 mm (position A), 12 mm (position B), 8 mm (position C) and 4 mm (position D).
  • Chips up to 75 x 75 mm
  • 4" wafer holder
  • 6" wafer holder (stage movement limited to central 100 x 100 mm region)
Substrate material allowed
  • Silicon, quartz, pyrex, III-V materials
  • Wafers with layers of silicon oxide or silicon (oxy)nitride
  • Wafers with layers of metal
  • Silicon, quartz, pyrex, III-V materials
  • Wafers with layers of silicon oxide or silicon (oxy)nitride
  • Wafers with layers of metal
General considerations Pros
  • 100 kV
  • Sub 10 nm resolution
  • Automatic beam optimization
  • High current and process speed
  • Automatic sample exchange
  • High level of programmability for automatic job execution
  • EBL workhorse for large designs
  • Readily available
  • More intuitive software
  • Easier SEM mode alignment
  • Build in SEM automation for post exposure process control
  • 2D stacks (HBN/graphene) allowed without Al coating
  • Excellent for small chips or small area design exposure
Cons
  • Steep learning curve
  • Availability - booking calendar is usually full 5 weeks ahead
  • Maximum 30 kV
  • User dependent performance/beam optimization
  • Minimum feature size >35 nm
  • Difficult to handle design files >1 GB
  • Slower writing speed

Fundementals of EBL pattern writing

Electron exposure

An E-beam writing system utilizes a focused electron beam to expose an electron sensitive resist in order to define a pattern on a substrate. For a positive tone resist the electron beam will scission polymer bonds within the resist to increase the dissolution rate when the substrate is placed in a developer solution. In this way the exposed part of the resist can be dissolved while maintaining the unexposed resist on the substrate. For a negative resist the electron beam will make the resist less soluble and hence the unexposed resist can be removed with a developer.

Exposure and development result of a positive resist (left) and a negative resist (right).


In order to define a pattern in the resist enough electrons have to be supplied to the exposed area, i.e. the exposure dose has to be sufficiently high. The area exposure dose is expressed in units of µC/cm2. The dose to clear the resist (for a positive resist) can be obtained from a contrast curve such as the one below. Dose to clear varies a lot between different resist types and is also dependent on processing parameters such as

  • Acceleration voltage
  • Resist thickness
  • Developer agent and concentration
  • Post exposure baking


In general it is always advisable to do a dose test of the pattern one intends to define to experimentally establish the optimum dose. For more information on resist dose please refer to the EBL substrate preparation guide.


Contrast curve for AR-P 6200 exposed at 100 kV with the JEOL 9500 exposure system. Illustration: Tine Greibe.

Writing principle

Both of our EBL systems lets the user define a desired area dose to expose the resist with. Based on the beam current the systems will then calculate the necessary beam dwell to achieve the requested dose in the drawn areas. It is always the drawn (filled) parts of a pattern that will get exposed. In addition to area dose the Raith eLine tool allows the user to define a line dose for exposure of single lines. The JEOL 9500 system does not allow that.

Before the pattern is exposed onto the substrate the pattern is broken down (fractured) into simple trapezoids and each trapezoidal shape is filled with beam shots, i.e. individual beam positions that together will make up the pattern. This is illustrated below with a simple pattern consisting of a square. The actual beam spot size is dependent on beam current and the pitch between beam positions is (within certain limitations) defined by the user.


Simple shape filled in with beam shots.


The electron source is continuously emitting electrons and exposure of the beam towards the sample is controlled by a beam blanker. The position of the beam is controlled by the beam deflector and scanning coils. The pattern is written one beam shot at a time in a serial process as this

  1. Beam positioning for 1st beam position of current trapezoidal shape
  2. Unblank the beam
    1. Exposure
    2. Reposition for next beam shot
  3. Blank the beam at end of trapezoidal shape

Steps 2.1 and 2.2 continues in a loop until all beam shots of the current trapezoidal shape has been executed after which the beam is blanked and the system moves on to the next trapezoidal shape. It is obvious that exposure in such a way is relatively slow and has an overhead on top of the actual exposure time since time is also spent on beam positioning and blanking/unblanking the beam.

Exposure grid and exposure field

Both systems have a maximum writing field size of 1000 x 1000 µm2 since the deflection of the beam is limited to ±500 µm in both x- and y-direction. Patterns inside a writing filed is written by beam deflection only and hence the substrate stage remains stationary. Geometry larger than a single writing field will be fractured across multiple writing fields and hence between fields the substrate stage will move to reposition the substrate directly under the column as illustrated below.

Illustration of a waveguide spanning four exposure fields. Between fields the stage will reposition the substrate below the column.

If neighbouring writing fields are not properly aligned features fractured across multiple writing fields may suffer from stitching errors, i.e. pattern discontinuities where the patterns do not align properly to each other. On the JEOL system write field alignment is ensured by a fully automated calibration sequence using internal alignment features. This ensures field stitching usually on the order of 10-15 nm or less. On the Raith system write field alignment is performed on the users own substrate and accuracy can vary.

The beam shots described above are placed onto the systems exposure grid, hence the resolution of beam shot placement is governed by the exposure grid. The resolution of this grid is determined by the positioning DAC of the system, on the JEOL 9500 this is 20 bit and on the Raith eLine it is 16 bit. Hence the JEOL 9500 system has in principle 220 = 1.048.576 grid positions along each axis while the Raith system has 216 = 65.384 grid positions along each axis. This means the JEOL system can maintain a 1 nm exposure grid over the entire 1000 x 1000 µm2 writing field whereas the Raith tool will have a 16 nm exposure grid at the maximum writing field.


Beam pitch, beam current and exposure dose relationship

A sample is exposed at a certain beam current. On the JEOL system this is selectable (in certain discrete steps) while on the Raith tool the beam current is bound by the choice of acceleration voltage and aperture. The user will input an area dose for the resist to be exposed with and the system will calculate the shot time (dwell time) of the beam to provide the requested dose. It is clear that high doses will require long dwell times whereas low doses will require short dwell times for the same beam current. There is however another important parameter to the dwell time calculation and that is the beam/shot pitch, i.e. how far beam shots are placed from each other. The beam scanner on the JEOL 9500 system is 100 MHz, thus the temporal resolution is 10 ns and it is not possible to have a beam shot (or dwell time) less than 10 ns. The Raith system has a 20 MHz beam scanner and hence the minimum shot time is 50 ns. This, in combination with beam current and exposure dose will set a lower limit on the beam pitch.

The relation might not be obvious at first and is illustrated below. The two identical features are filled with beam shots at two different pitches. the right version has a lower beam pitch (half of the other) and thus there are simply many more beam shots. Consequently, to provide the same area exposure dose the shot time for the right side feature will be much shorter. At half the pitch there will be four times the number of beam shots and thus the shot time will be 1/4 the shot time of the left feature.

Example feature filled with beam shots at one times beam diameter (left) and half beam diameter (right).

The shot time can be calculated as t = D·p2/I, where D is the dose in µC/cm2, p is beam pitch and I is current. As a practical example let us consider an exposure at 2 nA beam current and a desired dose of 250 µC/cm2. At 4 nm beam pitch the shot time will come out to 20 ns, while at 2 nm beam pitch it will come out at 5 ns and thus violate the hardware limitation of 10 ns for the JEOL system. In order to expose the pattern with 2 nm shot pitch one would have to choose a lower beam current at the expense of increased writing time.

The shot time is in fact such an important number that both systems will tell the user what it is. On the JEOL system the shot time is displayed in a table after job compilation, see below. On the Raith tool it is indicated in the Patterning Parameter Calculation box, see below.


Start estimation writing time   -----
Shot counting start -----
  thopeQU23008a.v30                                               at 11-MAR-2023 14:53:40
Shot counting end -----

  Seq.   writing time    shottime[nsec]   resist[uC/cm2]   stdcur[nA]   scanstep 
   1         0:52:27            16.000          200.000        2.000         16
   2         0:13:46            13.500          200.000       12.000         36
   3         0:11:15            12.000          100.000       12.000         48
   4         0:12:10            13.500          200.000       12.000         36
   5         0:11:14            12.000          100.000       12.000         48
 Total :     1:40:51

Estimation result file : thopeQU23008a.csv
End estimation writing making time     -----

Shot time as calculated by the JEOL system (left) and Raith eLine system (right).

Exposure time

E-beam exposure is a serial writing process and the writing time (t) will scale with dose (D), area (A) and beam current (I) as: t = D*A/I

It is thus essential to find the right balance between the area that needs to be defined and a beam current that will provide sufficient pattern fidelity and quality. During pattern writing the tool will also use time on cyclic calibration and stage movement as defined by the job path and pattern layout. The exposure time can be estimated based on the Writing Time Estimator Excel sheet.

Exposure information

Generalized workflow

While the EBL workflow resembles that of UV lithography there are a few additional complications and the parameter space is somewhat larger. The complications all arise from using electrons rather than light for exposure. Since a beam of electrons is used for exposure the substrate must be sufficiently conductive and grounded in order not to build up a charge. If the substrate in itself is not conductive a thin metal film or other conductive surface layer must be applied to it, read more on this in the resist section. Another complication is secondary exposure from backscattered electrons. This is a much bigger topic and covered in the pattern preparation section. A generalised workflow is shown below.

Generalized EBL workflow.
Generalized EBL workflow.

Since substrate preparation and development processes are (nearly) identical for the JEOL and Raith eLine systems they are described in common below. Pattern preparation, job preparation and job execution are fairly different between the two tools and hence these steps are described on the specific tool pages.

Substrate preparation and resist information

Substrates must be prepared for EBL by applying an e-beam sensitive resist and possibly a discharge layer. Please consult the EBL substrate preparation guide on how to prepare your substrate and to find resist information.

Pattern preparation

Pattern preparation is somewhat different depending on if a pattern is exposed on JEOL 9500 or Raith eLine Plus. Please refer to the correct pattern preparation section below.

Pattern preparation for exposure on JEOL 9500.

Pattern preparation for exposure on Raith eLine Plus.

Job preparation

Job preparation is also different depending on if a pattern is exposed on JEOL 9500 or Raith eLine Plus. Please refer to the correct job preparation section below.

Job preparation for exposure on JEOL 9500.

Job preparation for exposure on Raith eLine Plus.

Job execution

Job execution is very different between the JEOL and Raith systems. The procedures are described on their respective user guide pages:

Development

AR 600-546 and ZED N-50 developers are available in a semi automatic puddle developer Developer: E-beam in E-4, mainly intended for development of AR-P 6200 and ZEP 520A. It has automatic recipes for puddle development cycles for 10, 30 and 60 seconds of either of the two developers, each finishing off with an IPA rinse and drying cycle. The system can handle chips, 2", 4" and 6" wafers.


Other resist have to be developed in the E-beam developer fumehood in E-4 in beakers. Please notice there are specific beaker sets for alkaline developers and for solvent based developers.

Post development inspection

After development it is often necesarry to evaluate the result by SEM to verify feature dimensions. This can conviently be done in the Raith eLine Plus tool which apart from being an EBL tool is also a semiautomatic SEM. The strong suit of the tool is the ability to link/align a design file to the substrate and simply define image positions in the design file. The user can then set up a long list of image locations and the tool will acquire the SEM images without further user input. When set up correctly the system can acquire about one image per 5 seconds which is very advantageous for large arrays of structures. For an introduction to this, please refer to our automatic SEM introduction video.


After image acquisition the images can be semi automatically processed with ProSEM to determine feature sizes. For large image sets the software can generate an Excel sheet with various dimension outputs.

EBL process examples

Process examples and results can be found on this page.

Literature on E-beam Lithography