Skip to main content Accessibility help
×
Hostname: page-component-76fb5796d-vvkck Total loading time: 0 Render date: 2024-04-29T19:04:50.980Z Has data issue: false hasContentIssue false

Appendix H - Energy and stress densities

Published online by Cambridge University Press:  05 June 2012

Richard M. Martin
Affiliation:
University of Illinois, Urbana-Champaign
Get access

Summary

Summary

A density is a field defined at each position r, for example the particle number density n(r), which is a well-defined, experimentally measurable function. It would be desirable to have expressions for other densities, in particular, energy and stress densities. However, energy and stress densities are not unique on a microscopic quantum scale, even though they are the basis of the theory of elasticity on a macroscopic scale. This appendix brings out three points: (1) certain integrals of energy and stress densities are unique and very useful; (2) there are important contributions to the energy or stress density that are completely unique – these include all terms that arise from the fact that electrons are a many-body system of fermions; (3) all other terms that are non-unique can be shown to involve only the single scalar number density – there are different possible choices for these terms, each involving only derivatives of the density n(r) or the classical Coulomb potential VCC(r) which is directly related to n(r). It follows that all the issues of non-uniqueness are exactly the same as in a one-particle problem.

Only one density is widely used in electronic structure – the particle density n(r). It is the fundamental measurable quantity in quantum mechanics and the fundamental density in density functional theory. Theoretical expressions for n(r) are well defined and lead to unique results. Here we emphasize that other densities have the potential to play a useful role in electronic structure theory.

Type
Chapter
Information
Electronic Structure
Basic Theory and Practical Methods
, pp. 519 - 528
Publisher: Cambridge University Press
Print publication year: 2004

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 coreplatform@cambridge.org 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
×