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![Page 1: Www.helsinki.fi/yliopisto Antti Meriläinen 1, Ivan Kassamakov 1,2, Kenneth Österberg 1,2 and Edward Hæggström 1 1) Department of Physics, University of.](https://reader035.fdocuments.us/reader035/viewer/2022062802/56649eef5503460f94bff44f/html5/thumbnails/1.jpg)
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Antti Meriläinen1, Ivan Kassamakov1,2, Kenneth Österberg1,2 and Edward Hæggström1
1) Department of Physics, University of Helsinki
2) Helsinki Institute of Physics
Rapid Ultralow Pressure Manometry by Light
Absorption Spectroscopy
4.2.2014 1 of 10
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Motivation
• CLIC main beam vacuum requirements from beam dynamics: H20, CO, CO2 partial pressures < 3*109 mbar
• The RF causes outgassing in CLIC accelerator structures mainly to two mechanism: breakdown and dark current
• Expected pressure rise from simulations: several orders of magnitude on 100 ns time scale. To be verified experimentally.
• Aim: develop method to measure partial pressure changes of ~108 mbar on ~100 ns time scale at a RF test stand (”Xbox”). For the moment focusing on absorption spectroscopy and Cu.
4.2.2014 2 of 10
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Test setup
Quartz crystal microbalance (QCM) as reference
l = 5 ± 0.5 cm
R = 25 mm
RQCM = 6.5 mm
4.2.2014 3 of 10
Photo multiplier tube (PMT)
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Simulated Visualization
Light Source
QCM
CU source
PMT
4.2.2014 4 of 10
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Setup inside vacuum
QCM
Cu vapour source:Cu wire around W wire
1 cm
1 cm
1 mm
l = 5 ± 0.5 cm
4.2.2014 5 of 10
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Results
Measurement 1 Measurement 2
Sample rate: 100 ks/s6 kHz low pass filter for PMT1 Hz low pass filter for QCM
Change in intensity ~5%≈ 2 * 1011 absorbances≈ 10-4 mbar
4.2.2014 6 of 10
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Calibration (Relate intensity change to number of atoms)
Cu-source
QCM → ΔM → N1
Light beam ΔI
• atoms was measured by QCM
- Geometrical correction gives
- Calibration gives
N2
∫∆ 𝐼 ⅆ𝑡∫∆𝑀 ⅆ𝑡
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Progresst – dP – P Diagram
Target
Measurement 1 & 2
Faster PMT
1 ng/s = 1013 Cu atoms/s ≈ 5∙10-5 mbar 4.2.2014 8 of 10
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Achieved:
Measured few ng/s Cu at 10-5 mbar base pressure
Challenges:
Faster response time
Absolute calibration
Interpretation of measurement:
Can one atom have multiple absorptions?
Conclusion
4.2.2014 9 of 10
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Thank You!
Questions and Comments
4.2.201410 of 10
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Light Source
Setup & Cross section dimension
QCM
Cu source
RLight = 25 mm
RQCM = 6.5 mm
l = 5 ± 0.5 cm
Photo multiplier tube (PMT)
4.2.2014
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Absorption spectroscopy
- 324.8 nm and 327.4 nm wavelengths are strongly absorbed in copper vapor
- Light source must be stable- Copper hollow cathode lamp
is suitable low cost light source
- Light intensity changes is measured with Photomultiplier tube (PMT), bandwidth 20 kHz
4.2.2014
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Beer-Lamberts law(Light absorbtion in copper vapour)
Cross section for 324.8 nm and 327.4 nm wavelengths
Emitted intensity of 324.8 nm and 327.4 nm wavelengths
length of light beam in Cu vapornumber of absorbing Cu atoms
Current operation area (Signal > |Noise| )I = 90% - 10% lN = 4.9 * 1011 - 1.2 * 1013 Absorbances/meter
Operation point sensitivity: 9 * 1011 Absorbances/meter
4.2.2014