X-Ray Spectra of Long Wave-Length

Osgood, Thomas H.

doi:10.1103/physrev.30.567

Cited by 17 publications

(2 citation statements)

References 13 publications

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“…Two comments made by the authors are especially worth noting: firstly, that special pains were taken to employ a grating with a well polished surface and a light ruling, so as to obtain a good reflection from the space between the grooves; and secondly, they could see no reason why wavelength measurements of the type they described should not be made fully as precise as the absolute measurements by reflection from a crystal. A concave grating was first used by Osgood (1927), who measured spectral lines between 4 and 20 nm in a vacuum spectrograph. By the early 1930s widespread research was being undertaken in x-ray spectroscopy.…”

Section: Introductionmentioning

confidence: 99%

Diffraction gratings (manufacture)

Palmer¹,

Hutley²,

Franks³

et al. 1975

Rep. Prog. Phys.

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Recent progress in the techniques of manufacture of spectroscopic diffraction gratings is described. Three main topics are discussed in detail: (i) the mechanical ruling of gratings, and the way in which the mechanical aspects of the ruling process affect the spectroscopic performance of the grating; (ii) the development of interference (or 'holographic') techniques for manufacturing gratings, and the relationship between ruled gratings and those made interferometrically; (iii) x-ray gratings for use at grazing incidence, and the different criteria that arise through the use of gratings in this way. 2.7. Electromagnetic theory of gratings 2.8. Wood's anomalies . 2.9. Surface plasmons . 3.1. Introduction . 3.2. The ruling tool . 3.3. Films for ruled gratings 3.4. Recent studies of the ruling process 3.5. Contemporary ruled gratings . 3.6. Ruling engines . 3.7. Replication. 4.1. Introduction . 4.2. The spectroscopic performance of plane interference gratings 4.3. Blazed interference gratings . 4.4. Focusing and aberration-corrected gratings 4.5. Summary . 5 . X-ray gratings .

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Section: Introductionmentioning

confidence: 99%

Diffraction gratings (manufacture)

Palmer¹,

Hutley²,

Franks³

et al. 1975

Rep. Prog. Phys.

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show abstract

“…These workers used the concave grating in normal incidence mode and consequently extremely shorter wavelengths were not detected due to the rapid fall off in reflectivity with decreasing wavelength. By constructing a grazing incidence concave grating spectrograph, Osgood (1927) observed spectra from ~200 nm down to the K α x-ray line of carbon at 4.4 nm, thus closing the gap between the x-ray and extreme ultraviolet regions.…”

Section: 1mentioning

confidence: 99%

VUV/EUV ionising radiation and atoms and ions: dual laser plasma investigations

Kennedy

Costello

Mosnier

et al. 2004

Radiation Physics and Chemistry

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The interaction of ionizing radiation with atoms and ions is a key fundamental process. This report concentrates on studies of photoexcitation/photoionisation using laser-produced plasmas as continuum sources and synchronized laser plasma plumes to provide the absorbing atom or ion species. Examples from studies of the interaction of ionizing radiation with atoms and ions ranging from few-electron atomic and ionic systems to the many-electron high atomic number actinides are reviewed and illustrate the advantages and limitations of the Dual Laser Plasma technique.

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Soft X-Ray Emission Spectroscopy Using Synchrotron Radiation

Nordgren

1994

New Directions in Research With Third-Generation Soft X-Ray Synchrotron Radiation Sources

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X-Ray Spectra of Long Wave-Length

Cited by 17 publications

References 13 publications

Diffraction gratings (manufacture)

Diffraction gratings (manufacture)

VUV/EUV ionising radiation and atoms and ions: dual laser plasma investigations

Soft X-Ray Emission Spectroscopy Using Synchrotron Radiation

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