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Low Background Systems

Finally, it should be recognized that when using Marinelli beakers at count-rates that are close to background, the presence of the sample itself represents an extra layer of absorber to the gamma-rays. The background count rate (the environmental background Bg) will be lower with the filled Marinelli beaker than without [Pg.262]

Background radiation comes from the following sources  [Pg.262]

An interesting, and useful, paper to consult in relation to this section is that by Bossew (2005), in which he discusses the gamma-rays detected in a spectrum representing 3.3 years of counting time. In fact, this spectrum is the sum of 333 separate background spectra, accumulated over 16 years. The paper also contains some discussion of the temporal variability of background, and in the case of the Rn daughters, the monthly variabdity. [Pg.263]

Assuming that there is no local contamination of the environment, within a background spectrum of a detector at, or near, ground level, there could be peaks originating from the following sources  [Pg.263]

All of the peaks due to the nuclides mentioned above will be sat on a continuum due to Compton scattering of the gamma-rays and backscattering and bremmstrahlung due to direct interaction of cosmic particles. This will be discussed further in Section 13.4.6. [Pg.263]


Table IV compares the performance of several y spectrometry systems for many nuclides found in the environment. The f -y coincidence system is seen to offer significantly lower detection limits for many of the nuclides. Longer counting times could be used to establish even lower limits of detection, especially for low background systems. Table IV compares the performance of several y spectrometry systems for many nuclides found in the environment. The f -y coincidence system is seen to offer significantly lower detection limits for many of the nuclides. Longer counting times could be used to establish even lower limits of detection, especially for low background systems.
The detector holder, clamps and cooling rod in a standard detector would normally be of OFHC copper, but selected copper of much higher purity would be used for a low background system. A berylhum window will be of specially selected material stainless-steel screws replaced by brass or low-cobalt stainless-steel and rubber O-rings might be replaced by indium metal. Even such careful selection may have unexpected consequences indium has a high capture cross-section for thermal neutrons. [Pg.264]

The vacuum-getter within the evacuated detector chamber is often, in normal systems, a molecular sieve -an aluminium/silicon material - that will unavoidably contain very significant amounts of uranium, thorium and potassium (see Table 13.6). For low background systems, this is replaced by activated charcoal, which, while not necessarily being completely free of radioactive materials, will have a lower activity than a molecular sieve. [Pg.264]

Liquid scintillation counting has been used frequently for the measurement of environmental technetium. The specimens to be analyzed are treated by chemical procedures to obtain a technetium-bearing sample solution, which is mixed with a cocktail for scintillation counting. A low background scintillation counter with an anticoincidence system can be used for high precision measurements at a detection limit of 1-25 mBq. [Pg.24]

The analytical performance of CL microscopy imaging in terms of detectability, precision, accuracy, and spatial resolution was previously reported by us [25], The system allowed for the detection of 400 amol of enzymes such as F1RP or AP, with a spatial resolution as low as 1 pm and very low background. CL coupled with optical microscopy thus represents a useful tool for enzyme, antigen,... [Pg.486]

When electrochemical detection systems are used, it is essential that the mobile phases used are electrically conductive but only result in a low background current at the voltage selected. Cell volumes are of the order of 1 /d and the control of flow rate, pH and temperature is critical for reliable detection. [Pg.105]

The object of this paper is to discuss some of these problems. We start with the evidence for the new system of ionic radii. X-rays are diffracted by electrons in principle therefore X-ray diffraction should always locate the few outer electrons involved in bonding, but in fact this requires sophisticated treatment of meticulous measurements on crystals of high symmetry [6—9). But it has long been clear that some ionic crystals show round each ion an electron density which is approximately spherical but falls away to a very low background the following Table shows a typical example. [Pg.54]

Carbon paste Lightly polished Very low background, easily renewable, reproducible Slow kinetics for some systems, limited solvent compatability Widely used for aqueous oxidations, easy to modify 1... [Pg.328]


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