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Putting Confidence in Ultrasound Characterization of Acoustic Cavitation from a Megasonic Nozzle Transducer for Photomask Cleaning Nicolas Candia (1), Claudio Zanelli (2)†, Johann Brunner (3), Joachim Straka (3), Zhenxing Han (4), Sam Howard (2), Petrie Yam (2) (1) University de Santiago de Chile (2) Onda Corporation, (3) Sonosys Ultraschallsysteme GmbH, (4) Micron Corporation † Correspondence: [email protected] SPIE BACUS 2017 – Monterey, CA September 14, 2017

Characterization of Acoustic Cavitation from a Megasonic

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Page 1: Characterization of Acoustic Cavitation from a Megasonic

Putting Confidence in Ultrasound

Characterization of Acoustic Cavitation from a Megasonic Nozzle Transducer for Photomask Cleaning

Nicolas Candia (1), Claudio Zanelli (2)†, Johann Brunner (3), Joachim Straka (3), Zhenxing Han (4), Sam Howard (2), Petrie Yam (2)

(1) University de Santiago de Chile (2) Onda Corporation, (3) Sonosys Ultraschallsysteme GmbH, (4) Micron Corporation † Correspondence: [email protected]

SPIE BACUS 2017 – Monterey, CA

September 14, 2017

Page 2: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Mask Cleaning Trend: Tighter Process Window

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• Continued use of megasonics in 193i and EUV • Shrinking feature dimensions and more complex patterns

• Tighter process window !

Page 3: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Photomask Cleaning Challenges

3

Skirt-Type Transducer

Nozzle-Type Transducer

Dynamic Process:

• Transducer position • Acoustic uniformity • Acoustic cavitation • Reflections • Flow rate • Water level • Gas concentration • Moving mask & transducer • Temperature • Chemistry • Frequency • Generator power • Substrate material • Process time • And more…

Need in-situ measurement solution to correlate with cleaning Plate-Type

Transducer

Page 4: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Examples of Photomask Transducers

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Page 5: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Calculation of P0, PS, PT, f0

Pressure vs Frequency

Voltage vs Frequency

Quantification of Cavitation Pressure

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Voltage vs Time

Fourier Transform

Apply Hydrophone Calibration

Apply MCT-2000 Algorithms

Acquire data with Hydrophone

t (sec)

V

f (Hz)

P (Pa)

f (Hz)

V

f (Hz)

P (Pa)

P0

PS PT

f0

MCT-2000 Measures: • V vs. t • P vs. f • P0, PS, PT, f0

Page 6: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Cavitation Meter with Mask Sensor

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ACOUSTIC PRESSURE SPECTRUM

3 MHz 5 MHz

Direct Field, P0

Stable Cavitation, Ps

Transient Cavitation, Pt

Page 7: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Acoustic Test Plan

1. Gage Repeatability and Reproducibility (11 repeats)

2. Cavitation Pressure vs Frequency (3, 5, 3+5 MHz)

3. Cavitation Pressure vs Generator Power (10-100%, 35 W)

4. Cavitation Pressure vs Nozzle Distance (5-20 mm)

5. Cavitation Pressure vs Flow Rate (1-1.6 L/min)

6. Cavitation Pressure vs Sensor Position (A, B, C)

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Page 8: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Gage R&R

Static Repeatability (11X) - Without Load/Unload of Mask Sensor

Reproducibility (11X) – With Load/Unload of Mask Sensor

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Static Repeatability (% Std Dev)

Reproducibility (% Std Dev)

P0 2.2 3.7

Ps 1.6 9.4

Pt 1.9 1.4

Test Conditions: • 3 MHz (50%), 5 MHz (50%) • Nozzle Distance: 20 mm • Medium: DIW • Flow rate: 1.6 L/min

Page 9: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017 9

Test Conditions: • 3 MHz (50%), 5 MHz (50%) • Nozzle Distance: 20 mm • Medium: DIW • Flow rate: 1.6 L/min

Cavitation vs. Frequency

Page 10: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Cavitation vs. Generator Power

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3 MHz (10-100%)

5 MHz (10-100%)

3 MHz (50%) + 5 MHz (10-100%)

Test Conditions: • Nozzle Distance: 20 mm • Medium: DIW • Flow rate: 1.6 L/min

Page 11: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

5 + 5 ≠ 110!

11

3 MHz (10-100%)

5 MHz (10-100%)

3 MHz (50%) + 5 MHz (10-100%)

Cavitation vs. Generator Power

~110 kPa ~5 kPa

~5 kPa

Page 12: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017 12

At 20 mm: More static bubbles which promote generation of stable cavitation.

At 5 mm: Lower presence of static bubbles which yields less stable cavitation

Cavitation vs. Nozzle Distance

3 MHz 5 MHz

Page 13: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Cavitation vs. Nozzle Distance

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At 20 mm, Ps/Pt is maximized at low power.

Test Conditions: • 3 MHz (10-100%), 5 MHz (50%) • Nozzle Distance: 5, 20 mm • Medium: DIW • Flow rate: 1.6 L/min

At 20 mm At 5 mm

Page 14: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Cavitation vs. Flow Rate

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Medium Flow (1.3 L/min): Generation of higher level of static bubbles with increasing flow rate

Low Flow (1.0 L/min): Generation of static bubbles from liquid flow

High Flow (1.6 L/min): Static bubbles assist the generation of acoustic cavitation from direct field pressure

Page 15: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Cavitation vs. Flow Rate

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1.0 L/min 1.3 L/min 1.6 L/min

Higher flow rates yield higher levels of static cavitation relative to transient cavitation

Test Conditions: • 3 MHz (10-100%), 5 MHz (50%) • Nozzle Distance: 5, 20 mm • Medium: DIW • Flow rate: 1.0, 1.3, 1.6 L/min

Page 16: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Cavitation vs. Sensor Location

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Nozzle Position fixed over Sensor A

38 mm 38 mm

Page 17: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Cavitation vs. Sensor Location

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At sensor B: •Ps reduced more than 10X •Pt is negligible At sensor C: •Modest level of Ps detected •Pt is negligible

Page 18: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Conclusions

• The in-situ mask sensor enables one to define cavitation limits that correlate to PRE and pattern damage

• Differentiating between stable and transient cavitation is integral to control this process window.

• This solution allows measurement of cavitation as a function of: – Drive frequencies – Electrical power – Nozzle distance – Flow rate – Acoustic pressure distribution

• Future work: acoustically characterize variables such as gas concentration, chemistries, temperature and complex patterns, and understand their correlation to cleaning and damage.

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Page 19: Characterization of Acoustic Cavitation from a Megasonic

September 14, 2017

Thank you

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Page 20: Characterization of Acoustic Cavitation from a Megasonic

Putting Confidence in Ultrasound

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