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RF pulse amplifier for CVD-diamond particle detectors

MetadataDetails
Publication Date2021-04-01
JournalJournal of Instrumentation
AuthorsC. Hoarau, G. Bosson, J.-L. Bouly, S. Curtoni, D. Dauvergne
InstitutionsLaboratoire de Physique Subatomique et de Cosmologie, Université Grenoble Alpes
Citations10
AnalysisFull AI Review Included

Technical Documentation & Analysis: High-Speed CVD Diamond Detectors for Hadron Therapy

Section titled “Technical Documentation & Analysis: High-Speed CVD Diamond Detectors for Hadron Therapy”

This research details the development of an ultra-low power, high-speed Low Noise Amplifier (LNA) specifically designed for Chemical Vapor Deposition (CVD) diamond particle detectors used in hadron therapy beam monitoring.

  • Application Focus: High-frequency pulsed particle beam monitoring and time-stamping in hadron therapy, requiring sub-nanosecond timing resolution.
  • Performance Achieved: The LNA demonstrates exceptional speed (350 ps rise time) and timing stability (minimum jitter of 43 ps), essential for preserving the high mobility characteristics of diamond.
  • Ultra-Low Power: The design achieves a power consumption of only 72-75 mW per channel, enabling the integration of multi-channel readout (up to 40 strips) necessary for large-area, striped diamond hodoscope designs.
  • Material Requirements: The project utilizes both large-area Polycrystalline CVD (pCVD) (20 x 20 mm2) and high-purity Single Crystal CVD (sCVD) (4.5 x 4.5 mm2 mosaic) sensors, ranging in thickness from 300 ”m to 500 ”m.
  • 6CCVD Value Proposition: 6CCVD specializes in providing the high-purity SCD and large-area PCD substrates, custom cut to precise dimensions, and equipped with application-specific metalization (e.g., strip electrodes) required to replicate and scale this advanced detector technology.

The following hard data points were extracted from the analysis of the LNA performance and detector requirements:

ParameterValueUnitContext
LNA Gain (Maximum)46dBMeasured at 10 MHz
LNA Gain (High Frequency)31dBMeasured at 2 GHz
LNA Power Consumption72 - 75mWTotal power per channel
Output Pulse Rise Time (T20/80)350psSimulation and measurement
Minimum Jitter43psMeasured at 25% trigger level
Equivalent Noise Charge (ENC)230eEstimated
SCD Thickness (Tested)500”mUsed for 241Am source testing
PCD Prototype Dimensions20 x 20mm2300 ”m thickness
SCD Mosaic Dimensions4.5 x 4.5mm2500 ”m thickness (4 crystals)
Applied Electric Field (Typical)1V/”mRequired for charge carrier drift
Detector Bias Voltage (Tested)500VApplied across 500 ”m SCD
Electrode Thickness (Tested)100nmAluminum (Al) electrodes

The following steps outline the critical material and electronic methodologies used to achieve the high-performance diamond detector system:

  1. Detector Material Selection: Two primary diamond types were utilized: large-area Polycrystalline CVD (pCVD) for initial prototypes and high-purity Single Crystal CVD (sCVD) crystals arranged in a mosaic for the final hodoscope design.
  2. Custom Dimensions: SCD crystals were prepared at 4.5 x 4.5 mm2 and 500 ”m thickness, while pCVD plates were 20 x 20 mm2 and 300 ”m thick.
  3. Electrode Fabrication: Detectors were metalized with 100 nm thick Aluminum (Al) electrodes. The final hodoscope design requires double-side strip metalization, fabricated using a lift-off process for particle localization.
  4. LNA Design: A two-stage, surface-mount device (SMD) architecture was employed to minimize parasitic effects and control costs, utilizing RF layout techniques for high-frequency performance.
  5. Active Components: The first stage used a wideband NPN RF Si-Ge Heterojunction Bipolar Transistor (HBT) (Infineon BFP740, FT ~39 GHz) for low noise and timing constraints. The second stage used an integrated Low Noise Amplifier (Infineon BGA427).
  6. High Voltage Biasing: The detector was biased at high voltage (e.g., 500 V) via a T-shaped low-pass filter. The PCB layout ensured a 3 mm spacing between the high voltage line and ground to prevent sparking.
  7. Performance Validation: Time domain measurements were conducted using a calibrated pulse generator and a 241Am alpha source coupled to the 500 ”m SCD detector, confirming the 350 ps rise time and low jitter performance.

6CCVD is uniquely positioned to supply the advanced CVD diamond materials and customization services required to replicate, scale, and extend this high-performance particle detection research.

Research Requirement6CCVD Material SolutionTechnical Advantage
High-Purity SCD (500 ”m)Optical Grade Single Crystal Diamond (SCD)Ultra-low defect density ensures maximum charge collection efficiency (CCE) and preserves the intrinsic high mobility (2064 cm2.V-1.s-1) required for sub-nanosecond timing.
Large-Area PCD (20 x 20 mm2)High-Quality Polycrystalline Diamond (PCD)Available in plates up to 125 mm diameter, easily meeting the 20 x 20 mm2 requirement for large-area beam monitoring prototypes.
Detector Thickness (300 ”m - 500 ”m)Custom Thickness Wafers6CCVD offers precise thickness control for both SCD and PCD from 0.1 ”m up to 500 ”m, ensuring optimal charge collection depth for specific particle energies (e.g., 5.5 MeV alpha particles).

The success of the diamond hodoscope relies on precise material preparation and electrode patterning, areas where 6CCVD provides comprehensive in-house services:

  • Custom Dimensions and Mosaics: The paper requires small 4.5 x 4.5 mm2 SCD crystals. 6CCVD provides precision laser cutting to produce custom-sized plates and wafers, facilitating the assembly of complex mosaic detectors for large-area coverage.
  • Strip Metalization: The final design requires double-sided strip electrodes for particle localization. 6CCVD offers internal metalization capabilities including Au, Pt, Pd, Ti, W, and Cu. We can tailor the metal stack and thickness (e.g., replacing the 100 nm Al with a robust Ti/Pt/Au stack) and utilize advanced lithography techniques to define the high-resolution strip patterns required for the hodoscope.
  • Surface Finish: To ensure optimal electrode adhesion and minimize surface leakage current under high bias (500 V), 6CCVD guarantees ultra-smooth polishing with surface roughness (Ra) less than 1 nm for SCD and less than 5 nm for inch-size PCD.

The development of fast electronics for diamond detectors in High Energy Physics (HEP) and medical physics (hadron therapy) requires deep material expertise. 6CCVD’s in-house PhD engineering team specializes in optimizing CVD diamond properties for high-speed, high-radiation environments. We can assist researchers in selecting the ideal material grade, thickness, and metalization scheme to maximize Charge Collection Efficiency (CCE) and minimize timing jitter for similar Hadron Therapy Beam Monitoring projects.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.

View Original Abstract

Abstract This article introduces a design of a Low Noise Amplifier (LNA), for the field of diamond particle detectors. This amplifier is described from simulation to measurements, which include pulses from α particles detection. In hadron therapy, with high-frequency pulsed particle beams, the diamond detector is a promising candidate for beam monitoring and time-stamping, with prerequisite of fast electronics. The LNA is designed with surface mounted components and RF layout techniques to control costs and to allow timing performance suitable for sub-nanosecond edges of pulses. Also this amplifier offers the possibility of high voltage biasing, a characteristic essential for driving diamond detectors. Finally the greatest asset of this study is certainly the minimization of the power consumption, which allows us to consider designs with multiple amplifiers, in limited space, for striped diamond detectors.

  1. 1980 - A SILICON SURFACE BARRIER MICROSTRIP DETECTOR DESIGNED FOR HIGH-ENERGY PHYSICS [Crossref]
  2. 1991 - CMOS low noise amplifier for microstrip readout: Design and results [Crossref]