• No results found

New Products and Projects

N/A
N/A
Protected

Academic year: 2021

Share "New Products and Projects"

Copied!
5
0
0

Loading.... (view fulltext now)

Full text

(1)

New Products and

Projects

(2)

New silicon detector fabrication line

Next generation – SDD

plus

Series

Planar Thin Windows

Robust SDD Module

SPEEDY BSE Detector

The pnCCD Cameras

We keep you informed…

More than 10 years of research and development in the field of cutting-edge silicon radiation detectors lead to the success and high performance of PNDetector’s and PNSensor’s products and projects.

Highlights of recent years are:

r

Market leadership in EDX detectors for microanalysis due to the excellent quality of our Silicon Drift Detectors (SDDs with integrated FET, large solid angle, best energy resolution, optimum light element performance and high throughput capacity).

r

Award Winner for the most innovative product for a TEM application (custom specific ultrafast EDX solution).

r

Various publications in Nature on measurements with our pnCCDs which are the largest parallel-readout CCD sensors for Free Electron Laser (FEL) applications available.

r

Advanced solutions for a wide variety of synchrotron applications with our portfolio of large area detectors.

r

Successful integration of focal plane X-ray imaging detectors based on DEPFET Active Pixel Sensor for ESA’s Mercury mission BepiColombo.

Content

The extra large detector SDD field (600 mm2) has been designed for synchrotron applications.) has been designed for synchrotron applications.) has been designed for synchrotron applications.

PND presents their new Planar Thin Window technology for the housing of the detector modules.

The next generation SDDs minimizes the gap to the theoretical measurement limit.

PNS offers compact pnCCD systems for e. g. XRF imaging or as directly converting device for single electron detection in a TEM.

PND & PNS introduce their own advanced clean room for silicon detector fabrication, mounting and testing.

PND offers now a Robust SDD Module for harsh environmental requirements.

The BSE Detector features strongly increased collection efficiency and real TV speed imaging capability.

Editorial

(3)

4 5

New silicon detector fabrication line

Status

The clean room construction started in April 2013 and will be finished in September 2013. The first production of qualification devices will start in January 2014. Its successful completion will be celebrated in a Grand Opening in Summer 2014.

from

We are aiming for:

r

Best performance

r

Optimized throughput

r

Reliability & quality control

r

Flexibility & efficiency

r

Custom specific solutions

r

Advanced technologies

r

Modern equipment

r

Sophisticated designs

PNDetector is expanding

PNDetector’s new clean room will be a worldwide unique facility dedicated to the fabrication of state-of-the-art silicon detectors of highest quality. The clean room design is optimized to permit a continuous and efficient production flow from the raw material, 6 - 8 inch FZ silicon wafers of highest purity level, to the finalized product.

The fully equipped clean room will include various areas of dedicated semiconductor fabrication as well as modern packaging facilities and laboratories for test and qualification, divided in different zones of clean room classes 10 - 1000. The fferent zones of clean room classes 10 - 1000. The ff facilities are situated on the Siemens technology campus in Munich, Germany.

The construction and qualification will take place in two phases:

In Phase 1 a clean room of 400 m2 will be built up for the fabrication and qualification of double sided, high resolution spectroscopic detectors and imagers.

In Phase 2 the clean room will be expanded to 600 m2 by new testing and mounting laboratories featuring highest quality standard and advanced equipment.

Phase 1 Phase 2 Silicon wafers to to Detector Modules SDD Chips, PTWs, pin diodes, pnCCDs …

(4)

6 7

Standard plus

SDD

plus

-10-128pnW PTW

SDDplus FET round housing typ. 127 eV FWHM

10.0 mm2 x 450 μm outer diameter 15 mm @ MnK, -20°C, 10 - 100 kcps round shape design Ø 3.2 mm Zr collimator typ. 135 eV FWHM

polysilicon technology 1-stage Peltier cooler @ MnK, -20°C, 300 kcps

pnWindow Planar Thin Window typ. 55 eV FWHM

(PTW-TP) @ C_K, -20°C, 10 kcps

P/B typ. 5,000 @ MnK

SDD

plus

-30-128pnW UTW SL

SDDplus FET round housing typ. 127 eV FWHM

30.0 mm2 x 450 μm outer diameter 15 mm @ MnK, -30°C, 10 - 100 kcps round shape design Ø 5.8 mm Zr collimator typ. 55 eV FWHM

polysilicon technology 2-stage Peltier cooler @ C_K, -30°C, 10 kcps

pnWindow thin polymere window P/B typ. 7,500 @ MnK

non-magnetic housing

SDD

plus

-60-128pnW UTW SL

SDDplus FET round housing typ. 128 eV FWHM

60.0 mm2 x 450 μm outer diameter 17.5 mm @ MnK, -30°C, 10 - 100 kcps round shape design Ø 8.15 mm Zr collimator typ. 58 eV FWHM

polysilicon technology 2-stage Peltier cooler @ C_K, -30°C, 10 kcps

pnWindow thin polymere window P/B typ. 10,000 @ MnK

non-magnetic housing

SDD

plus

-100-128pnW UTW USL

SDDplus FET round housing typ. 129 eV FWHM

100.0 mm2 x 450 μm outer diameter 18.5 mm @ MnK, -30°C, 10 - 100 kcps round shape design Ø 10.5 mm Zr collimator typ. 62 eV FWHM

polysilicon technology 2-stage Peltier cooler @ C_K, -30°C, 10 kcps

pnWindow thin polymere window P/B typ. 10,000 @ MnK

non-magnetic housing

High resolution plus

SD3

plus

-10-125pnW UTW SL

SDDplus FET round housing typ. 122 eV FWHM

10.0 mm2 x 450 μm outer diameter 15 mm @ MnK, -30°C, 10 - 100 kcps droplet design Ø 3.1 mm Zr collimator typ. 127 eV FWHM

polysilicon technology 2-stage Peltier cooler @ MnK, -30°C, 300 kcps

pnWindow thin polymere window typ. 42 eV FWHM

non-magnetic housing @ C_K, -30°C, 10 kcps

P/B typ. 15,000 @ MnK

SD3

plus

-30-125pnW UTW SL

SDDplus FET round housing typ. 124 eV FWHM

30.0 mm2 x 450 μm outer diameter 15 mm @ MnK, -30°C, 10 - 100 kcps droplet design Ø 5.8 mm Zr collimator typ. 128 eV FWHM

polysilicon technology 2-stage Peltier cooler @ MnK, -30°C, 300 kcps

pnWindow thin polymere window typ. 45 eV FWHM

non-magnetic housing @ C_K, -30°C, 10 kcps

P/B typ. 15,000 @ MnK

Next generation – SDD

plus

Series

High-resolution, high-throughput EDX applications re-quire de tec tors with extremely low input capacitance, providing optimum detector performance at very short processing times.

Here, significant progress has been made by remodeling the geometry of the anode and of the integrated FET with the goal of reducing all parasitic capacitances related to the detector anode. This led to a new generation of SDD detectors – the so-called SDDplus Series.

The low capacitance anode/FET can be adopted to all SDD types (round or droplet shape) and sizes (from 10 and 30 mm2 up to 100 mm2 or multichannel devices).

The SDDplus detectors possess the best spectroscopic per-formance at short shaping times and are suited for all types of applications where ultimate energy resolution is required and where high spectral resolution at high speed is mandatory.

As the size of the FET and of the collecting anode is optimized with respect to minimum input capacitance, the SDDplus devices show improved spectroscopic performance for all detector areas. When applied to the SD3 droplet devices, the optimized FET technology leads to spectroscopic performance at the theoretical Fano limit.

This is especially beneficial at shorter shaping times (122 eV @ 1µs and 126 eV @ 0.25 µs for a 10 mm2 droplet SDDplus device) and for the detection of X-rays in the light element energy range (38 eV @ C_K and B_K). Lithium K-line (54 eV) is also detected.

eee e Standard FET SDDplus FET

Sensor Description Module Design Performance Parameter

122 eV @ 1 μs

SD3 10 mm2 SD3plus 10 mm2

Shaping time [µs] Energy [eV]

Energy [eV] FWHM @ M n-K α [eV ] Number of c oun ts Number of c oun ts C-K line

Next generation – SDD

plus

Series

Robust SEM/XRF SEM/TEM SEM/XRF SEM/XRF SEM SEM/TEM

(5)

To download the complete document

please register at http://www.pndetector.de/broxDL

References

Related documents

• Like other solid state X-ray detectors, silicon drift detectors measure the energy of an incoming photon by the amount of ionization it produces in the detector material.. • In

With massive expansion of its network infrastructure and systems to support one of the busiest and most techni- cally sophisticated roads imaginable, this traffic manage-

On the other hand, the measured data were utilized to determine the relationship between incidence angle with a diffuse radiation, and total solar irradiance with hourly time,

Traditional Model Cloud Model $25 / user - month $9 / user - month $100 / user - month $44 / user - month $12 / year - GB $3 / year - GB $1000 / month $230 / month Savings

In this model: the principle stakeholders are other academics in business schools and universities; excellence can be measured by the RAE; inter-organisational relationships

The Team provides a variety of services to school districts and county offices of education upon request. The District has requested that the Team provide for the assignment

These include: the energy spread of the beam after the MCP foil, the energy straggling due to the detector and the intrinsic time and energy resolutions of the detectors.. The

Relative to this literature, the main contribution and the aim of this paper is to examine the relationship between climate change and migration by studying the effect on