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http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal Dear all, I find that there is someting I have not understood regarding lateral resolution in our confocal (Zeiss 510 meta). As I understand it, lateral resolution should be dependent on excitation wavelength and NA solely. But what is the case if we open the pinhole a bit above 1 AU? For some (admittedly special) samples, we use up to about 4AU. As far as I understand it, on a 510, using a 40x 1.3 objective, 532ex/575em, zoom 1, the pinhole is 300um, and the object-side projected pinhole diameter is then about 2,2um. As the PMT detector itself is not position-sensitive any light within this 2.2um circle in the focal plane would be detected. The practical resolution would then be determined by the laser spot size (?). Using the zeiss "optimal frame size" calculator for nyqvist sampling on the above setting gives me 2048*2048 pixels, which is the max available, maybe it would calculate an even higher nunber of pixels if the option was available. 2048*2048 gives me a pixel size of 0.11*0.11 um , which to me seems small in relation to the spot size of the laser. Is this reasoning correct, or where am I wrong? Thanks in advance, Jan Grawé Cell Analysis Core Facility Rudbecklaboratoriet/C5 Dag hammarskjölds väg 20 SE-75185 Uppsala SWEDEN Phone: +(0)18-4714657 Cell: +(0)70-2577874 [hidden email] www.rudbeck.uu.se/cellanalys |
Search the CONFOCAL archive at
http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal The resolution, assuming the BFP of the objective is filled (not always the case) will be given in fluorescence by the Rayleigh formula r = 0.5lambda/NA. This applies to widefield or scanned microscopy. With a very small pinhole there is an additional 'confocal' resolution improvement of 1.414 (root 2) (r confocal = r wf / 1.414). The full improvement will only be given by an infinitely small pinhole ... For some examples of finite sized pinholes see Guy Cox & Colin Sheppard, 2004. Practical limits of resolution in confocal and non-linear microscopy. Microscopy Research & Technique, 63, 18-22 . In practice you can get some lateral resolution improvement in reflection mode but you won't get much, if any, in fluorescence. So when you open your pinhole you are not really losing lateral resolution. You are losing depth resolution quite substantially. There really shouldn't be any reason to open the pinhole above 1 Airy unit since (unless the system is misaligned) that will let through all the in focus light. After that you're just letting in out of focus light. Guy Optical Imaging Techniques in Cell Biology by Guy Cox CRC Press / Taylor & Francis http://www.guycox.com/optical.htm ______________________________________________ Associate Professor Guy Cox, MA, DPhil(Oxon) Electron Microscope Unit, Madsen Building F09, University of Sydney, NSW 2006 ______________________________________________ Phone +61 2 9351 3176 Fax +61 2 9351 7682 Mobile 0413 281 861 ______________________________________________ http://www.guycox.net -----Original Message----- From: Confocal Microscopy List [mailto:[hidden email]] On Behalf Of Jan Grawé Sent: Tuesday, 1 April 2008 6:01 PM To: [hidden email] Subject: lateral resolution Search the CONFOCAL archive at http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal Dear all, I find that there is someting I have not understood regarding lateral resolution in our confocal (Zeiss 510 meta). As I understand it, lateral resolution should be dependent on excitation wavelength and NA solely. But what is the case if we open the pinhole a bit above 1 AU? For some (admittedly special) samples, we use up to about 4AU. As far as I understand it, on a 510, using a 40x 1.3 objective, 532ex/575em, zoom 1, the pinhole is 300um, and the object-side projected pinhole diameter is then about 2,2um. As the PMT detector itself is not position-sensitive any light within this 2.2um circle in the focal plane would be detected. The practical resolution would then be determined by the laser spot size (?). Using the zeiss "optimal frame size" calculator for nyqvist sampling on the above setting gives me 2048*2048 pixels, which is the max available, maybe it would calculate an even higher nunber of pixels if the option was available. 2048*2048 gives me a pixel size of 0.11*0.11 um , which to me seems small in relation to the spot size of the laser. Is this reasoning correct, or where am I wrong? Thanks in advance, Jan Grawé Cell Analysis Core Facility Rudbecklaboratoriet/C5 Dag hammarskjölds väg 20 SE-75185 Uppsala SWEDEN Phone: +(0)18-4714657 Cell: +(0)70-2577874 [hidden email] www.rudbeck.uu.se/cellanalys No virus found in this incoming message. Checked by AVG. Version: 7.5.519 / Virus Database: 269.22.2/1353 - Release Date: 31/03/2008 6:21 PM No virus found in this outgoing message. Checked by AVG. Version: 7.5.519 / Virus Database: 269.22.2/1353 - Release Date: 31/03/2008 6:21 PM |
In reply to this post by Jan Grawe
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http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal Dear Jan, As you have indicated, when opening up the pinhole the resolution is determined by the laser beam only. Laterally, your focused laser beam will have a resolution of approx. 250nm. Following Nyquist, the pixel size should indeed be about 100 to 110 nm. So, everything seems to be fine. Best regards, Kevin > -----Oorspronkelijk bericht----- > Van: Confocal Microscopy List [mailto:[hidden email]] > Namens Jan Grawé > Verzonden: dinsdag 1 april 2008 10:01 > Aan: [hidden email] > Onderwerp: lateral resolution > > Search the CONFOCAL archive at > http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal > > Dear all, > > I find that there is someting I have not > understood regarding lateral resolution in our confocal (Zeiss 510 > meta). > As I understand it, lateral resolution should be > dependent on excitation wavelength and NA solely. > But what is the case if we open the pinhole a bit > above 1 AU? For some (admittedly special) samples, we use up to about > 4AU. > As far as I understand it, on a 510, using a 40x > 1.3 objective, 532ex/575em, zoom 1, the pinhole > is 300um, and the object-side projected pinhole > diameter is then about 2,2um. As the PMT detector > itself is not position-sensitive any light within > this 2.2um circle in the focal plane would be > detected. The practical resolution would then be > determined by the laser spot size (?). > Using the zeiss "optimal frame size" calculator > for nyqvist sampling on the above setting gives > me 2048*2048 pixels, which is the max available, > maybe it would calculate an even higher nunber of > pixels if the option was available. 2048*2048 > gives me a pixel size of 0.11*0.11 um , which to > me seems small in relation to the spot size of the laser. > Is this reasoning correct, or where am I wrong? > > Thanks in advance, > > Jan Grawé > Cell Analysis Core Facility > Rudbecklaboratoriet/C5 > Dag hammarskjölds väg 20 > SE-75185 Uppsala > SWEDEN > > Phone: +(0)18-4714657 > Cell: +(0)70-2577874 > [hidden email] > www.rudbeck.uu.se/cellanalys |
Search the CONFOCAL archive at
http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal The correct pixel size is just correct by chance, since the Zeiss software doesn't consider the pinhole diameter in the calculation of XY scaling. Michael > Search the CONFOCAL archive at > http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal > > Dear Jan, > > As you have indicated, when opening up the pinhole the resolution is > determined by the laser beam only. Laterally, your focused laser beam will > have a resolution of approx. 250nm. Following Nyquist, the pixel size > should > indeed be about 100 to 110 nm. So, everything seems to be fine. > > Best regards, > > Kevin > > >> -----Oorspronkelijk bericht----- >> Van: Confocal Microscopy List [mailto:[hidden email]] >> Namens Jan Grawé >> Verzonden: dinsdag 1 april 2008 10:01 >> Aan: [hidden email] >> Onderwerp: lateral resolution >> >> Search the CONFOCAL archive at >> http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal >> >> Dear all, >> >> I find that there is someting I have not >> understood regarding lateral resolution in our confocal (Zeiss 510 >> meta). >> As I understand it, lateral resolution should be >> dependent on excitation wavelength and NA solely. >> But what is the case if we open the pinhole a bit >> above 1 AU? For some (admittedly special) samples, we use up to about >> 4AU. >> As far as I understand it, on a 510, using a 40x >> 1.3 objective, 532ex/575em, zoom 1, the pinhole >> is 300um, and the object-side projected pinhole >> diameter is then about 2,2um. As the PMT detector >> itself is not position-sensitive any light within >> this 2.2um circle in the focal plane would be >> detected. The practical resolution would then be >> determined by the laser spot size (?). >> Using the zeiss "optimal frame size" calculator >> for nyqvist sampling on the above setting gives >> me 2048*2048 pixels, which is the max available, >> maybe it would calculate an even higher nunber of >> pixels if the option was available. 2048*2048 >> gives me a pixel size of 0.11*0.11 um , which to >> me seems small in relation to the spot size of the laser. >> Is this reasoning correct, or where am I wrong? >> >> Thanks in advance, >> >> Jan Grawé >> Cell Analysis Core Facility >> Rudbecklaboratoriet/C5 >> Dag hammarskjölds väg 20 >> SE-75185 Uppsala >> SWEDEN >> >> Phone: +(0)18-4714657 >> Cell: +(0)70-2577874 >> [hidden email] >> www.rudbeck.uu.se/cellanalys |
Search the CONFOCAL archive at
http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal Michael Weber <[hidden email]> writes: > Search the CONFOCAL archive at > http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal > > The correct pixel size is just correct by chance, since the Zeiss software > doesn't consider the pinhole diameter in the calculation of XY scaling. There is some justification for this. Using the Rayleigh criterion, the resolution is defined by the distance to the first minimum of the Ariry disk. A confocal pinhole does not change this at all, although it does reduce the FWHM of the peak (ie the shape changes but the peak still has the same total width). Where a confocal really wins is in Z resolution. Ian |
Search the CONFOCAL archive at
http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal Listers, I strongly recommend to look back 10 years, there was a threat on the confocal listserver mentioning this article: Contrast, resolution, pixelation, dynamic range and signal-to-noise : fundamental limits to resolution in fluorescence light microscopy - E.H.K. Stelzer - J. Microscopy (1998) 189 : 15-24. Basically, to meet the Rayleigh criterion under even moderate noise conditions you need at least 8 samples to achieve the required contrast to distinguish the peaks of 2 neighbouring Airy patterns. Translated for the objective and lambda mentioned (1.3NA, 532nm ex.) this results in a pixelsize of about 58nm(!). The Nyquist calculator from SVI even returns 51nm as the required pixel size. Overall, in my opinion, the pinhole does not improve lateral resolution at all under the conditions encountered in imaging of fluorescently labeled biomaterials. Cheers, jens ***Join the elmi meeting! Extended application deadline 14.4.08. More info: http://elmi08.unibas.ch/index.html *** -----Original Message----- From: Confocal Microscopy List [mailto:[hidden email]] On Behalf Of Ian Dobbie Sent: Mittwoch, 2. April 2008 11:49 To: [hidden email] Subject: Re: lateral resolution Search the CONFOCAL archive at http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal Michael Weber <[hidden email]> writes: > Search the CONFOCAL archive at > http://listserv.acsu.buffalo.edu/cgi-bin/wa?S1=confocal > > The correct pixel size is just correct by chance, since the Zeiss > software doesn't consider the pinhole diameter in the calculation of XY scaling. There is some justification for this. Using the Rayleigh criterion, the resolution is defined by the distance to the first minimum of the Ariry disk. A confocal pinhole does not change this at all, although it does reduce the FWHM of the peak (ie the shape changes but the peak still has the same total width). Where a confocal really wins is in Z resolution. Ian |
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