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- Bruker Announces New High-Performance Scientific Instruments and Analytical Solutions for Life-Science Research, Industrial and Applied Markets at Analytica 2012
- Bruker Announces Acquisition of SkyScan, a Leading Provider of Micro-CT Systems for 3D X-Ray Imaging in Materials Research and Preclinical Studies
- Bruker Acquires Hecus MICROcaliX(R) Product Line to Expand Product Portfolio for Small Angle X-ray Scattering (SAXS)
- Bruker Introduces the Alloy Guide App for Mobile Devices
- Bruker Announces $1.3 Million Contract with ThyssenKrupp Stainless USA
Upcoming Events
- OrthoTec 2012
Jun 06-07, Winona Lake, IN, USA - Introducing XFlash® 6
Jun 13, Webinar - ACHEMA 2012
Jun 18-22, Frankfurt/M., Germany - Seeing at the Nanoscale 2012
Jul 09-11, Bristol, UK - ACA Annual Meeting
Jul 28-Aug 01, Boston, Massachusettes, USA - ACS Fall
Aug 19-21, Philadelphia, Pennsylvania, USA
Technology
The combination of innovative ideas with most modern X-ray technology results in a new generation of a very compact, portable TXRF spectrometer:
- a specially designed, very compact and air-cooled micro focus X-ray tube in metal-ceramics technology
- a modern multi-layer X-ray optics for beam focussing and monochromatization
- a Peltier-cooled, high resolution XFlash® X-ray detector (SDD) of the latest generation.
As a result, this TXRF-spectrometer is totally independent of liquid nitrogen and cooling water! The maximum power consumption is only 180 W, which makes it especially interesting for mobile applications.
Working principle
The S2 PICOFOX working principle is based on the method of total reflection X-ray fluorescence (TXRF) analysis. An air-cooled X-ray tube typically with molybdenum target generates an X-ray beam, which is reduced to a narrow energy range by a multi-layer monochromator. The fine beam impinges on a polished sample carrier at a very small angle (< 0.1°) and is totally reflected. The characteristic fluorescence of the sample is emitted and measured in an energy-dispersive X-ray detector. Due to the short distance to the carrier, the fluorescence yield is very high and the absorption by air is very low.
The main difference between TXRF and conventional XRF spectrometers is the use of monochromatic radiation and total reflection optics. Illuminating the sample with a totally reflected beam reduces absorption and scattering of the beam in the sample matrix. Resulting benefits include a significantly enhanced fluorescence yield, largely reduced background noise, and consequently much higher sensitivities to elements present even in trace amounts.
In addition, the preparation of the sample substance as a thin layer avoids matrix effects. Therefore quantitative analysis can easily be performed using an internal standard.
Specifications
| Specifications | |
| Element range | Mo excitation: Al to U (with exception of Nb to Ru) W excitation: K to U |
| Concentration | ppb to % |
| Detection limit | < 3 pg Nickel (Mo excitation with High Efficiency Module) |
| Sample types | Liquids, suspensions, powders, particles, metals, thin layers, tissues, wipes, filters etc. |
| Sample volume | Liquids and suspensions from 1 to 50 μl Particles up to 100 μm in diameter, powders up to 10 μg |
| Sample carrier | 25 quartz and 100 acrylic glass carriers (30 mm diameter) included in shipment |
| Sample changer | Manual version for single samples Automatic version with cassette for up to 25 samples |
| X-ray tube | 30 W or 50 W metal-ceramic, max. 50 kV, 1 mA air-cooled, Mo or W target |
| X-ray optics | Multilayer monochromator |
| Detector | Peltier-cooled XFlash® Silicon Drift Detector No need for liquid nitrogen 30 mm² active area Energy resolution < 150 eV at 100 kcps (Mn Ka) |
| Interface | Control and data exchange via RS232 serial interface |
| Mains | 100/240 V, 50/60 Hz, max. power consumption 180 W |
| Size | 300 x 590 x 450 mm (height x width x depth) |
| Weight | 37 kg |
| Accessories | Washing cassette for sample carriers Sample cassette for 25 carriers Starter Set for TXRF (pipettes, tips, racks, tubes, mortar, spatula) |



