CONFOCALMICROSCOPY Archives

May 2004

CONFOCALMICROSCOPY@LISTS.UMN.EDU

Options: Use Monospaced Font
Show Text Part by Default
Show All Mail Headers

Message: [<< First] [< Prev] [Next >] [Last >>]
Topic: [<< First] [< Prev] [Next >] [Last >>]
Author: [<< First] [< Prev] [Next >] [Last >>]

Print Reply
Subject:
From:
Reply To:
Confocal Microscopy List <[log in to unmask]>
Date:
Mon, 24 May 2004 10:44:30 +1000
Content-Type:
text/plain
Parts/Attachments:
text/plain (63 lines)
Search the CONFOCAL archive at
http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal

Re Jim Pawley's comments:

First off 1 Airy means that the diameter of the pinhole equals
the diameter of the Airy disk (and of course the radius of the
pinhole equals the radius of the Airy disk).  Under these conditions
the Rayleigh 2-point resolution will be equal to the radius of
the Airy disk.

It is true that in confocal microscopy one is exciting the sample
above and below the plane of focus so some fluorescence is wasted.
In principle one could recover some of this by deconvolution and
a partly open pinhole.  Like any other deconvolution method this
would work best with a sparse dataset.  However there is a very
important practical reason why this is actually a VERY bad idea.
That is that practical confocal microscopes do not expand the
beam sufficiently to fill the back focal plane of the objective
with a uniform field (even microscopes with beam-expanding optics.)
So if you open the pinhole beyond 1 Airy, instead of getting wide-
field resolution, as theory would suggest, your resolution gets
dranatically worse.  The theory and practice are covered in a
recent paper:

Guy Cox & Colin Sheppard, 2004. Practical limits of resolution  in confocal
and
non-linear microscopy.  Microscopy Research & Technique, 63, 18-22

The practical answer is to use multiphoton excitation, so you
don't excite outside the focal volume and no photons are wasted.

Where deconvolution is most useful in confocal microscopy is in
improving the Z-resolution (or at least the perceived Z-resolution).
Not only is the resolution worse in Z, the spread function is
a rather problematic shape which doesn't go to zero (ie some
small amount of out of focus light always gets through the
pinhole). This also seems to be the most useful factor for
Perveen's work.  See:

G.C. Cox and C. Sheppard, 1993.  Effects of image deconvolution on optical
sectioning in conventional and confocal microscopes.  Bio-Imaging 1, 82-95.

G.C. Cox and Colin Sheppard, 1999  Appropriate Image Processing for Confocal
Microscopy.  In: P.C. Cheng, P P Hwang, J L. Wu, G Wang & H Kim (eds)
Focus on Multidimensional  Microscopy.  World Scientific Publishing,
Singapore,
New Jersey, London & Hong Kong.  Volume 2, pp 42-54  ISBN 981-02-3992-0

In this case it is definitely best to work with a 1-Airy pinhole.

                                                Guy Cox

Assoc. Prof. Guy Cox,                 ooOOOOOOoo
E.M. Unit, F09            #       oOOOO  |  |  OOOOo       #
University of Sydney     ###    OOO|  |  |  |  |  |OOO    ###
NSW 2006, Australia      ###  OOO  |  |  |  |  |  |  OOO  ###
Ph:  02 9351 3176        ### OO |  |  |  |  |  |  |  | OO ###
Fax: 02 9351 7682       #####   |  |  |  |  |  |  |  |   #####
                      ==#####============================#####==
http://www.guycox.net   #####                            #####
http://www.guycox.com ~~#####~~~~~~~~~~~~~~~~~~~~~~~~~~~~#####~~

ATOM RSS1 RSS2