Skip to main content Accessibility help
×
Hostname: page-component-586b7cd67f-dlnhk Total loading time: 0 Render date: 2024-11-20T17:24:56.790Z Has data issue: false hasContentIssue false

5 - Scintillators, phosphors and NEADs

Published online by Cambridge University Press:  21 May 2010

Get access

Summary

Introduction

This chapter describes the uses-past, present and proposed-of three types of solid X-ray converter in soft X-ray astronomy: scintillators and phosphors, which work by the conversion of X-ray energy into visible light and negative electron affinity detectors (NEADs), which rely on external photoemission from a surface activated to a state of negative electron affinity. Although the terms scintillator and phosphor are formally synonyms (Thewlis, 1962), we shall adopt the usage prevalent in the detector literature and distinguish between bulk, crystalline materials such as Nal(Tl) and CsI(Na) (scintillators) and thin, granular layers of, for example, the rare earth oxysulphides (phosphors). Phosphors are often identified by a commercial T-number’. A partial list of such numbers is given by Gruner et al (1982).

The use of luminescent solids in nuclear physics has a long tradition. Rutherford's nuclear model of the atom (1909), for example, had as its experimental basis the observation, by eye, of α-particle induced light flashes (scintillations) on a zinc sulphide screen. The substitution of a photomultiplier tube for the human observer, which first occurred towards the end of the second world war, produced a sensitive electronic counter for γ-rays and particles, whose operation is described in texts such as those of Curran (1953), Birks (1964) and Knoll (1979).

The first use of a scintillation counter in X-ray astronomy was in a balloon-borne observation of the Crab Nebula in 1964 (Clark, 1965). As described in section 1.2, such balloon payloads were limited, because of atmospheric opacity, to the spectral band E > 20 ke V, where source fluxes decrease rapidly with increasing X-ray energy.

Type
Chapter
Information
Publisher: Cambridge University Press
Print publication year: 1989

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

Save book to Kindle

To save this book to your Kindle, first ensure [email protected] is added to your Approved Personal Document E-mail List under your Personal Document Settings on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part of your Kindle email address below. Find out more about saving to your Kindle.

Note you can select to save to either the @free.kindle.com or @kindle.com variations. ‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi. ‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.

Find out more about the Kindle Personal Document Service.

Available formats
×

Save book to Dropbox

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Dropbox.

Available formats
×

Save book to Google Drive

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Google Drive.

Available formats
×