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Spectrap ElectronicsEvaluation of Cryogenic Components Begin 2009
Stefan Stahl
measurements by
Stefan Stahl & Zoran Angelkovic
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Preface: main objectivesPreface: main objectives
challenge : important to have low final temperature=> new amplifier
design
• Resistive Cooling of captured ions to T = 4.2K and ion detectionResistive Cooling of captured ions to T = 4.2K and ion detection
• Rotating Wall CompressionRotating Wall Compression
• FT-ICR Detection (optional)FT-ICR Detection (optional)
challenge : FT-ICR and rotating wall compression at the same time
m · D²
q² · R
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Novel Amplifier DesignNovel Amplifier Design
• FET with low input capacitance => low heating of LC circuit
• Additional cascode circuitry further lowers CIN
Main former problem (GaAs-FETs) : 1/f-noise and input capacitance lead to increased axial ion temperature of 30 – 70 K
(see: g-factor experiments, Gabrielse-setups)
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Noise Chart of designed amplifierNoise Chart of designed amplifier
LC circuit at trap will show about 22nV/(Hz)1/2 @ 2MHzCin determined to 1.8pF strong decoupling 6:1 possiblePresumably low Tnoise~ 6K
Using NEC 3508 „super low noise“ HJ-FET (GaAs)
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Rotating Wall CompressionRotating Wall Compression
T = 300K
T = 4.2K
non-linear filters reduce noise and allow FT-ICR at the same time
Low pass functionality, overruled at high amplitudes
Established 2008
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Frequency and Amplitude responseFrequency and Amplitude response
Observations:General functionality verifiedClear Voltage Threshold as expectedOutput Excitation amplitudes somewhat too low Failure of diodes at Uin ~ 12Vpk or 240mApk => modifications will be tested coming weeks
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Geometrical ArrangementGeometrical Arrangement
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Another Idea: Charge Detector for AdjustmentAnother Idea: Charge Detector for Adjustment
Sensitive cryogenic charge amplifier on back side
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Summary and OutlookSummary and Outlook• Low input capacitance amplifier design verified
and tested => suitable for axial detection and resistive cooling
• Filter unit successfully tested; some weak point discovered, to be solved soon
• Several components (capacitors, resistors, diodes and FETs) verified for compatibility with 4.2K environment
• Refine overall circuitry design and adapt to latest geometrical changes
• Eventually add functionality of cryogenic destructive charge detector
• Test of completed cryo setup after connecting the trap and room temperature electronics
• Software control of devices
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Thanks a lot foryour attention.
Email: [email protected] www.stahl-electronics.com
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Spare Slides:Spare Slides:
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Examples of Coil-Design
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Pickup-Elektrode
Pickup-Elektrode
x
y
Detection of Image Charges, FT-ICRDetection of Image Charges, FT-ICR
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Pickup-Elektrode
Pickup-Elektrode
ion currentsignal
I
t
Detection of Image Charges, FT-ICRDetection of Image Charges, FT-ICR
x
y
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Pickup-Elektrode
Pickup-Elektrode
ion currentsignal
I
Detection of Image Charges, FT-ICRDetection of Image Charges, FT-ICR
x
y
very smallsignal ~fA
Signal strength
D ~ distance of pickup electrodes
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Pickup-Elektrode
Pickup-Elektrode
ion currentsignal
z
Voltage/Current Amplifier
Pe nning Tra p(c ro ss se c tio n)
ra d ia lly sp lit e le c tro d eslit
FFTFou rie r-Transfo rm - spectra l analyser
excited ion
m agnetic fie ld
low noiseAm p.
timetime-domain frequency-domain
I
frequency
dP /d fion current signal
mass spectrum
FFT
q/mspectrum
II
t f
x
y
very smallsignal ~fA
Detection of Image Charges, FT-ICRDetection of Image Charges, FT-ICR
„FT-ICR“ Fourier-Transform Ion Cyclotron Resonance
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Detection of Image Charges, FT-ICRDetection of Image Charges, FT-ICR
• Method is non-destructive
• Many ion species can be detected at the same time
• Small sensitivity to space charges compared to TOFSmall sensitivity to space charges compared to TOF
• Useful over a very wide range of ion numbersUseful over a very wide range of ion numbers
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
FT-ICR CircuitryFT-ICR Circuitry
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
First HFirst H22OO++ Resonance: Resonance:
Spectrap Collaboration Meeting, April 2, 2009
Spectrap Evaluation of Cryogenic Components
Shot Noise by Ions and ElectronsShot Noise by Ions and Electrons
Creating shot noise while flying through
1010 electrons/sec. ~ 6 fA/ (Hz)1/2 1012 ions/sec. ~ 700 fA/ (Hz)1/2