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"Fast reset" ASIC Preamplifier

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1 "Fast reset" ASIC Preamplifier
INFN - Milano University of Milano Department of Physics "Fast reset" ASIC Preamplifier Cutting-edge circuit technology able to boost the dynamic range of CMOS charge-sensitive preamplifiers far beyond their saturation limit Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 " Oct. 30, 2012

2 "GASPARD-HYDE-TRACE Workshop 2012 "
Outline Context and goal of the research Large volume HPGe detectors & required specs for charge preamps The issue of saturation & dynamic range for integrated preamplifiers Technique to handle saturated signals with low-noise CMOS preamps Charge information recovery: extending the dynamic range beyond the saturation limit of the preamplifier Reset-mode high-resolution spectroscopy Conclusions Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 " Speaker: Stefano Capra "GASPARD-HYDE-TRACE Workshop 2012"

3 "GASPARD-HYDE-TRACE Workshop 2012 "
Context and goal Context New generation of nuclear-physics experiments with high- intensity ion beams. A technical advance for the new gamma-ray spectrometers is required. Goal of the research New paradigm: high-resolution spectroscopy is possible even working with a deeply saturated CSP ! Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 " Speaker: Stefano Capra "GASPARD-HYDE-TRACE Workshop 2012"

4 emitting radionuclide
Large volume HPGe detectors High-resolution gamma-ray spectroscopy  investigation of nuclear structure under very extreme conditions of stability ~ 9 cm Main features: operated at cryogenic temperature (liquid nitrogen used as cooling 77 K) electrodes capacitance values: pF energy of detected gamma-rays: from a few keV to a few tens of MeV excellent intrinsic energy resolution: 0.1% - 0.2% in the typical 1 MeV region segmentation of the outer electrode  position-sensitivity: ~ 1 mm 3D resolution Gamma-ray tracking Gamma-ray Compton imaging can take advantage of the excellent energy/position resolution of HPGe emitting radionuclide Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

5 Charge-preamplifier specifications
low noise (gamma spectroscopy grade: MeV) excellent stability of the gain and of the shape of the preamplifier response (loop gain ~ 103) wide bandwidth: rise time of ~ 20 ns (pulse shape analysis) low power consumption (especially for the devices operated in the cryostat) LARGE DYNAMIC RANGE: - at least ~104 : from a few keV to MeV - up to ~30 MeV depending on the physics experiment (i.e. giant resonances) - minimization of the dead time in a much larger energy range up to MeV γ ( 1-10MeV) extremely hostile background of highly energetic charge particles in next-generation nuclear physics experiments with high-intensity exotic beams p K ( MeV) HPGe segmented detectors of AGATA (Advanced GAmma-ray Tracking Array) Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

6 The issue of a wide dynamic range
Old-style solution: hybrid DISCRETE preamplifiers high flexibility in the design use of high voltage power supply (ex: +/- 12 V) Modern CMOS integrated solutions: a mandatory task the high segmentation of the read-out electrodes yields a higher and higher count of read-out channels small dimensions & low power dissipation radio-purity and full functionality at cryogenic temperature Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

7 The issue of a wide dynamic range
Old-style solution: hybrid DISCRETE preamplifiers high flexibility in the design use of high voltage power supply (ex: +/- 12 V) Modern CMOS integrated solutions: a mandatory task the high segmentation of the read-out electrodes yields a higher and higher count of read-out channels small dimensions & low power dissipation radio-purity and full functionality at cryogenic temperature Intrinsically low available voltage swing of scaled CMOS technologies A decrease of the preamplifier sensitivity (energy-to-voltage gain) would compromise the signal-to-noise ratio and the spectroscopic performances Saturation of a CMOS preamplifier for HPGe detectors is expected for input energies > 5-10 MeV Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

8 Charge-Sensitive Preamplifier (CSP) Mode Threshold of Comparator
Time-variant circuit structure*: typical-amplitude signals Charge-Sensitive Preamplifier (CSP) Mode For “normal” amplitude signals (up to a few MeV) the comparator keeps switch “S” in the right position The circuit is a Low-Noise Charge-sensitive preamplifier Allows for high-resolution energy measurements Normal CSP External discrete components: BF862 Si JFET, RF=1GW, CF=0.2pF X Comparator S CSP Mode Threshold of Comparator CSP Mode *see also Radeka, Overload Recovery Circuit for Charge Amplifiers, IEEE Trans. Nucl. Sci., vol. 17, no. 1, p. 269, 1970 Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

9 Threshold of Comparator
Time-variant circuit structure*: large signals Fast-Reset Mode Minimizes the preamplifier dead time and prevents from the paralysis of the acquisition system in the case of extremely high background counting rates Allows for charge information even in the saturation condition Allows for high-resolution energy measurements  extending the dynamic range of photons/particles spectroscopy External discrete components: BF862 Si JFET, RF=1GW, CF=0.2pF + Q I const Fast Reset Mode Comparator S Threshold of Comparator Reset Time *see also Radeka, Overload Recovery Circuit for Charge Amplifiers, IEEE Trans. Nucl. Sci., vol. 17, no. 1, p. 269, 1970 Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

10 The charge preamplifier
Layout 0.35mm 5V mid-oxide CMOS Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

11 The Schmitt trigger comparator
Schmitt trigger configuration with a positive feedback loop lower reset threshold set at 0V by the ground voltage reference external feedback resistances to adjust the upper reset threshold (~ preamplifier saturation voltage) Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

12 "GASPARD-HYDE-TRACE Workshop 2012 "
The current sink the comparator output signal drives a transmission gate so as to deviate the reset current to the input node of the preamplifier Reset current NMOSFET inserted into the negative feedback loop of an operational amplifier Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

13 "GASPARD-HYDE-TRACE Workshop 2012 "
Realized chip Pre OUT Pre IN IRESET Comp_IN- Curr IN + - Comp_IN+ + - VEE RSINK INHIB Comp OUT VEE Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

14 Charge information recovery
Computer simulation During saturation, the physical information, i.e. the charge released by the germanium crystal, is not lost but temporarily stored on the total capacitance at the input node of the circuit Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

15 Charge information recovery
The bounce of the input node voltage (virtual ground) is actually negligible because the capacitance of HPGe detectors (20-50 pF) is typically two order of magnitude larger than the feedback capacitance ( pF) Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

16 Charge information recovery
Preamp response to a detector like test signal (200ns width) Computer simulation The bounce of the input node voltage (virtual ground) is actually negligible because the capacitance of HPGe detectors (20-50 pF) is typically two order of magnitude larger than the feedback capacitance ( pF) VG voltage bounce Computer simulation Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

17 Charge information recovery
Computer simulation Computer simulation The bounce of the input node voltage (virtual ground) is actually negligible because the capacitance of HPGe detectors (20-50 pF) is typically two order of magnitude larger than the feedback capacitance ( pF) Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

18 Remove Q and measure T The larger Q the longer the time T needed for complete removal Constant current  rate of removed Charge over Time is constant from the definition of electric current  Q and T are proportional Nonlinearity of preamplifier working condition must not influence Q vs T linearity Precise charge measurements are possible in saturated conditions Parasitic DC paths Virtual ground bounces So, the issue of the intrinsically low available voltage swing of scaled CMOS technologies may be skipped through Time-over-Threshold measurements !! Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

19 Proportional relation between input charge and reset time
Active Fast Reset Computer simulations Digital pulses delivered by the comparator: a time-over-threshold measurement provides the reset time Preamplifier output signals of different amplitudes (negative holes signals) Proportional relation between input charge and reset time Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

20 Reset time - Input charge Relation
Energy in Ge The percent error in the fitting mainly comes from the numerical approximation of the simulation program and has to be considered as a maximum upper limit 1 pC 2 pC 3 pC 4 pC 5 pC 18.2 MeV 36.4 MeV 54.5 MeV 72.7 MeV 90.9 MeV Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

21 Reset time - Input charge Relation
IRESET = constant reset current VSAT = output saturation voltage RF = feedback resistance T = reset time Q0 = offset term Q = (IRESET + VSAT/RF) T + Q0 (VSAT/RF)T = charge removed (~0.8%) by the current flowing on RF while the output signal is saturated Q0= offset term due (i) to the mismatch between the baseline voltage and the 2nd reset threshold (~0V), (ii) to the constant charge removed by the current flowing in RF out of the saturation condition second-order effects on the bias conditions of the detector and JFET p-n junctions, due to the virtual ground bounce, are found to be negligible in our computer simulations Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

22 “Reset-mode” spectroscopy
“Reset-mode” high-resolution spectroscopy has been demonstrated Hybrid charge preamplifier with second-stage active fast reset Reset-mode 241Am+Be spectrum resolution on Ni line: 9MeV See: F.Zocca, A.Pullia, D.Bazzacco, G.Pascovici, “A Time-over-Threshold technique for wide dynamic range gamma-ray spectroscopy with the AGATA detector”, IEEE Trans. Nucl. Sci., vol. 56, no. 4, pp , Aug. 2009 Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

23 “Reset-mode” spectroscopy
Experimental results with “Fast reset” ASIC preamplifier Excellent linearity also in Fast Reset mode Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

24 “Reset-mode” spectroscopy
Experimental results with “Fast reset” ASIC preamplifier ENC: equivalent noise charge with 15 pF (higher value) and 0 pF (lower value) detector capacitance Series 1/f noise Series white noise Parallel white noise Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

25 "GASPARD-HYDE-TRACE Workshop 2012 "
Conclusions Design & computer simulation of a JFET-CMOS preamplifier (0.35mm) for HPGe detectors equipped with a fast reset device for charge sensing stage de-saturation Dead time minimization in the cases of high background counting rates Charge measurements even in a condition of deep saturation → boost of useful dynamic range for high- resolution energy measurements Experimental tests performed on the realized test chip Speaker: Stefano Capra  "GASPARD-HYDE-TRACE Workshop 2012 "

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