Skip to main content Accessibility help
×
Hostname: page-component-76fb5796d-vfjqv Total loading time: 0 Render date: 2024-04-28T18:26:46.689Z Has data issue: false hasContentIssue false

4 - Identifying Functions and Directions

Published online by Cambridge University Press:  05 August 2015

Allan Pinkus
Affiliation:
Technion - Israel Institute of Technology, Haifa
Get access

Summary

In this chapter we consider the following inverse problem. Assume that we are given a function F that we know is of the form

for some choice of positive integer r, unknown functions fi, and either known or unknown directions ai. The question we ask is how to determine these unknowns parameters based on our knowledge of F. In the first section we assume that we know the directions ai, while in the second section we assume they are unknown. In Section 4.3 we pose these same questions for generalized ridge functions. In the case of unknown Ai we are able only to analyze the case r = 1. Thematerial of Sections 4.1 and 4.2 may be found in Buhmann and Pinkus [1999].

Known Directions

Assume that we know an F of the form (4.1) with given directions ai. How can we theoretically identify the functions fi? (We will, of course, assume that the directions ai are pairwise linearly independent.) As we have seen, from the previous chapters, we have a degree of non-unicity. However, assuming that F is smooth and fiB for all i, then from Theorem 3.1 the fi are determined, at the very least, up to polynomials of degree at most r − 2.

Let us now detail how we might determine the fi. When r = 1 we need make no assumptions as

F(x) = f1(a1 · x).

Choosing c ∊ Rn such that a1 · c = 1, we have

F(tc) = f1(t),

which gives us f1. Similarly, for r = 2 we can find a c ∊ Rn satisfying a1 · c = 1 and a2 · c = 0, and thus

F(tc) = f1(t) + f2(0),

which determines f1 up to a constant. In this same manner we determine f2 up to a constant.

Type
Chapter
Information
Ridge Functions , pp. 28 - 35
Publisher: Cambridge University Press
Print publication year: 2015

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
×