Southeastern Microscopy Society meeting

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Amanda M. Lawrence Amanda M. Lawrence
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Southeastern Microscopy Society meeting

On behalf of the Southeastern Microscopy Society (SEMS) Local
Arrangements and Program Committees I would like to invite you to the
SEMS annual meeting which will be held from May 24-26, 2010 at the
Francis Marion hotel in historical Charleston, South Carolina.
Microscopy Society of America, Microbeam Analysis Society, and SEMS
sponsored speakers include:
Dr. David Piston (MSA President) * Vanderbilt University
Dr. David Joy * University of Tennessee
Dr. Paul Kotula * Sandia National Laboratories
Dr. Michael Postek * NIST
Dr. Elaine Schumacher * McCrone Associates, Inc
Dr. John Lemasters * Medical University of South Carolina
Dr. Sue Lessner * University of South Carolina
Dr. Heather Evans-Anderson * Winthrop University
Dr. Anand Ramamurthi * Clemson University
Assistance for travel and meeting costs for students competing in the
SEMS Ruska Award and technologists is available. There are also
opportunities to participate in pre-meeting workshops on Confocal
Microscopy and Digital Imaging, a tour of the Robert Bosch Company
Facility, and post-meeting tours of the Yorktown and Fort Sumter.
For further information on abstract submission, registration, and
participation in the above workshops and tours please visit:
http://www.southeasternmicroscopy.org/index-2.html      and
http://www.southeasternmicroscopy.org/meetings_doc/SEMSBro_web.pdf
The deadline for abstract submission is Thursday, April 1, 2010. I hope
all of you will be able to attend.  
Sincerely,

Robert L. Price President, SEMS
mmodel mmodel
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tube lens and spherical aberration

(I apologize if this is a second post, I got some strange errors from the first one)

Dear List

It's not a confocal question, it's strictly a wide-field question... When people talk about spherical aberration they typically start with a parallel beam falling on an objective, and then, for whatever reason, the objective fails to bring all the rays into a common focus. In wide-field, one has a luminous spot in the object space, and the effect of spherical aberration would be a failure of the objective to collect all the rays into a single parallel beam. Some rays will form a converging (or diverging) cone instead. Then, this cone will be received (I suspect that in the case of a diverging cone, some light may even get lost on its way) by a tube lens and form a blurry spot on the image plane. My question is, Is this situation really equivalent to the standard one considered in all books? (I suspect, it's not because even the distance to the tube lens should make a difference). But I would be very interested in the opinion of those who understand optics better than I do. Thanks!

Mike Model

Michael Model, Ph.D.
Confocal Microscopy,
Dpt Biological Sciences,
1275 University Esplanade,
Kent State University, Kent, OH 44242
tel. 330-672-2874
Andreas Bruckbauer Andreas Bruckbauer
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Re: tube lens and spherical aberration

Just go the other way, from a perfect spot in the image plane to the diffuse spot in the object plane, then you are back to the standard situation. You can always reverse the light path in linear optics.

best wishes

Andreas



-----Original Message-----
From: MODEL, MICHAEL <[hidden email]>
To: [hidden email]
Sent: Fri, 26 Feb 2010 20:54
Subject: tube lens and spherical aberration

(I apologize if this is a second post, I got some strange errors from the first 
one)

Dear List

It's not a confocal question, it's strictly a wide-field question... When people
talk about spherical aberration they typically start with a parallel beam
falling on an objective, and then, for whatever reason, the objective fails to
bring all the rays into a common focus. In wide-field, one has a luminous spot
in the object space, and the effect of spherical aberration would be a failure
of the objective to collect all the rays into a single parallel beam. Some rays
will form a converging (or diverging) cone instead. Then, this cone will be
received (I suspect that in the case of a diverging cone, some light may even
get lost on its way) by a tube lens and form a blurry spot on the image plane.
My question is, Is this situation really equivalent to the standard one
considered in all books? (I suspect, it's not because even the distance to the
tube lens should make a difference). But I would be very interested in the
opinion of those who understand optics better than I do. Thanks!

Mike Model

Michael Model, Ph.D.
Confocal Microscopy,
Dpt Biological Sciences,
1275 University Esplanade,
Kent State University, Kent, OH 44242
tel. 330-672-2874
mmodel mmodel
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Re: tube lens and spherical aberration

Andreas, thanks for your response. I understand that the path can be reversed for a ray but it seems to me that the size of the blur in the image will depend, for example, on the distance between the objective and the tube lens. Which is not part of the standard formula.
 
Mike
 

From: Confocal Microscopy List [[hidden email]] On Behalf Of Andreas Bruckbauer [[hidden email]]
Sent: Friday, February 26, 2010 5:06 PM
To: [hidden email]
Subject: Re: tube lens and spherical aberration

Just go the other way, from a perfect spot in the image plane to the diffuse spot in the object plane, then you are back to the standard situation. You can always reverse the light path in linear optics.

best wishes

Andreas



-----Original Message-----
From: MODEL, MICHAEL <[hidden email]>
To: [hidden email]
Sent: Fri, 26 Feb 2010 20:54
Subject: tube lens and spherical aberration

(I apologize if this is a second post, I got some strange errors from the first 
one)

Dear List

It's not a confocal question, it's strictly a wide-field question... When people
talk about spherical aberration they typically start with a parallel beam
falling on an objective, and then, for whatever reason, the objective fails to
bring all the rays into a common focus. In wide-field, one has a luminous spot
in the object space, and the effect of spherical aberration would be a failure
of the objective to collect all the rays into a single parallel beam. Some rays
will form a converging (or diverging) cone instead. Then, this cone will be
received (I suspect that in the case of a diverging cone, some light may even
get lost on its way) by a tube lens and form a blurry spot on the image plane.
My question is, Is this situation really equivalent to the standard one
considered in all books? (I suspect, it's not because even the distance to the
tube lens should make a difference). But I would be very interested in the
opinion of those who understand optics better than I do. Thanks!

Mike Model

Michael Model, Ph.D.
Confocal Microscopy,
Dpt Biological Sciences,
1275 University Esplanade,
Kent State University, Kent, OH 44242
tel. 330-672-2874
Lutz Schaefer Lutz Schaefer
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Re: tube lens and spherical aberration

In reply to this post by mmodel
Michael,

spherical aberration (SA) is mostly caused by refractive index mismatches
between immersion and embedding. Also, using cover slips and immersion media
that are different from the manufacturers recommendations will cause more or
less SA. Often we model the system between front element and sample with 3
parallel layers of RI. Optimally, the manufacturer has corrected the
objective with aberrations of the opposite sign, so your induced SA cancels
out. Still, for example whenever the embedding has different RI than the
immersion, the best way to have the least amount of SA is to stay close to
the cover slip with your sample. Now, if you have no ICS optics (older
microscopes) you may have a chance to do some SA compensation by changing
that tube length, which will also slightly change the working distance. The
same is true for changing other parameters in the 3 layer system. In an ICS
you can only do the latter. Although SA depends linear on some of the model
parameters, you cant really say that the wave front generally diverges or
converges in presence of SA, because that could rather somewhat better
explain defocus. Because it is hard to describe in a few simple words how a
wave front behaves, one usually uses diffraction theory (e.g. "Principles of
optics", Born & Wolf). This is a very well understood, rigorous theory,
enabling to quantify complex amplitudes and their polarization, or if you
wish just intensities. I would understand, when not all aspects of
diffraction theory are detailed in a book that focuses on general
microscopy, but then I am not sure what books you were referring to.

Regards
Lutz

____________________________________
Lutz Schaefer
Advanced Imaging Methodology Consultation
16-715 Doon Village Rd.
Kitchener, Ontario, N2P 2A2
Phone/Fax: (519) 894 8870
Email:     [hidden email]
Website: http://home.golden.net/~lschafer/
____________________________________


--------------------------------------------------
From: "MODEL, MICHAEL" <[hidden email]>
Sent: Friday, February 26, 2010 3:54 PM
To: <[hidden email]>
Subject: tube lens and spherical aberration

> (I apologize if this is a second post, I got some strange errors from the
> first one)
>
> Dear List
>
> It's not a confocal question, it's strictly a wide-field question... When
> people talk about spherical aberration they typically start with a
> parallel beam falling on an objective, and then, for whatever reason, the
> objective fails to bring all the rays into a common focus. In wide-field,
> one has a luminous spot in the object space, and the effect of spherical
> aberration would be a failure of the objective to collect all the rays
> into a single parallel beam. Some rays will form a converging (or
> diverging) cone instead. Then, this cone will be received (I suspect that
> in the case of a diverging cone, some light may even get lost on its way)
> by a tube lens and form a blurry spot on the image plane. My question is,
> Is this situation really equivalent to the standard one considered in all
> books? (I suspect, it's not because even the distance to the tube lens
> should make a difference). But I would be very interested in the opinion
> of those who understand optics better than I do. Thanks!
>
> Mike Model
>
> Michael Model, Ph.D.
> Confocal Microscopy,
> Dpt Biological Sciences,
> 1275 University Esplanade,
> Kent State University, Kent, OH 44242
> tel. 330-672-2874
Shalin Mehta Shalin Mehta
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Re: tube lens and spherical aberration

In reply to this post by mmodel
Hi Michael,
I think your misgivings are true. If I understood correctly - you are wondering whether illumination-side spherical aberration is different from imaging-side spherical aberration. I think they are different. Plus they do different things when one uses confocal scanning geometry vs. widefield geometry.  Perhaps different sources of spherical aberration can be explained thus:

- The case considered in most of the microscopy text is of RI mismatch between embedding and immersion media in confocal imaging. The mismatch causes the focused illumination spot to be worse than the diffraction-limited hour-glass, reducing the signal that can be collected by PMT after the pin-hole. So in confocal, spherical aberration = bad SNR. Plus, the signal appears to be coming from the wrong place as spherical aberration shifts the peak intensity in the focal volume.

Since in confocal, both illumination and detection perform imaging and we pick-up the intensity in the center of the imaging volume by using a pin-hole --- I wonder what does the PSF of spherically aberrated confocal look like. I think there are papers by Sheppard and Min Gu that need to be consulted. 

- In widefield imaging, one uses Kohler type of arrangement to bring light from mercury filament onto the specimen. Otherwise, one will see filament imprinted on the specimen. The source of widefield illumination being incohernet (unlike coherent laser illumination of confocal), the aberrations seen by it on the way to specimen are unimportant. The PSF of the widefield system is strictly that of the imaging path - the 'mere' use of illumination is to excite fluorophores uniformly. 

Consequently, as you say, the above RI mismatch will give rise to converging or diverging wavefront from the focal volume between the tube-lens and the objective *in the detection path*. The imaging path's PSF will be therefore have distorted look like the standard spherical aberrated PSF that we see in Born and Wolf or Hecht.

best
Shalin


On Sat, Feb 27, 2010 at 7:52 AM, MODEL, MICHAEL <[hidden email]> wrote:
Andreas, thanks for your response. I understand that the path can be reversed for a ray but it seems to me that the size of the blur in the image will depend, for example, on the distance between the objective and the tube lens. Which is not part of the standard formula.
 
Mike
 

From: Confocal Microscopy List [[hidden email]] On Behalf Of Andreas Bruckbauer [[hidden email]]
Sent: Friday, February 26, 2010 5:06 PMSubject: Re: tube lens and spherical aberration

Just go the other way, from a perfect spot in the image plane to the diffuse spot in the object plane, then you are back to the standard situation. You can always reverse the light path in linear optics.

best wishes

Andreas



-----Original Message-----
From: MODEL, MICHAEL <[hidden email]>
To: [hidden email]
Sent: Fri, 26 Feb 2010 20:54
Subject: tube lens and spherical aberration

(I apologize if this is a second post, I got some strange errors from the first 
one)

Dear List

It's not a confocal question, it's strictly a wide-field question... When people
talk about spherical aberration they typically start with a parallel beam
falling on an objective, and then, for whatever reason, the objective fails to
bring all the rays into a common focus. In wide-field, one has a luminous spot
in the object space, and the effect of spherical aberration would be a failure
of the objective to collect all the rays into a single parallel beam. Some rays
will form a converging (or diverging) cone instead. Then, this cone will be
received (I suspect that in the case of a diverging cone, some light may even
get lost on its way) by a tube lens and form a blurry spot on the image plane.
My question is, Is this situation really equivalent to the standard one
considered in all books? (I suspect, it's not because even the distance to the
tube lens should make a difference). But I would be very interested in the
opinion of those who understand optics better than I do. Thanks!

Mike Model

Michael Model, Ph.D.
Confocal Microscopy,
Dpt Biological Sciences,
1275 University Esplanade,
Kent State University, Kent, OH 44242
tel. 330-672-2874

Shalin Mehta Shalin Mehta
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Re: tube lens and spherical aberration

Since in confocal, both illumination and detection perform imaging and we pick-up the intensity in the center of the imaging volume by using a pin-hole --- I wonder what does the PSF of spherically aberrated confocal look like. I think there are papers by Sheppard and Min Gu that need to be consulted. 

And also Jim Pawley's experimental papers and the confocal book should be looked up.

best
Shalin 
Guy Cox-2 Guy Cox-2
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Re: tube lens and spherical aberration

In reply to this post by mmodel
I don't think that is true.  A lot of published versions start out from
an objective forming an image of a point object.

Many years ago I got a bit incensed at a diagram in a textbook,
purporting to show SA introduced by a coverslip.  The rays leaving the
coverslip were not parallel to those entering it!  I wanted a diagram to
show my students, and this obviously wasn't it.

So I sat down with pencil, paper and ruler.  First of all I drew a
perfect lens forming an image of a point.  Then I drew a coverslip in
the way, looked up the sines of the angles as measured, and constructed
the ray paths.  Lo and behold, there was the classic caustic curve.
(And, need I say, the rays exited the coverslip at the same angle they
entered.)  So I traced it on OHP film and used it in my lectures
thereafter (long before Powerpoint!).  And the students were much more
willing to take it on board since it was constructed without any complex
formulae - nothing more than Snell's Law.  

                                                    Guy

-----Original Message-----
From: Confocal Microscopy List [mailto:[hidden email]]
On Behalf Of MODEL, MICHAEL
Sent: Saturday, 27 February 2010 7:55 AM
To: [hidden email]
Subject: tube lens and spherical aberration

(I apologize if this is a second post, I got some strange errors from
the first one)

Dear List

It's not a confocal question, it's strictly a wide-field question...
When people talk about spherical aberration they typically start with a
parallel beam falling on an objective, and then, for whatever reason,
the objective fails to bring all the rays into a common focus. In
wide-field, one has a luminous spot in the object space, and the effect
of spherical aberration would be a failure of the objective to collect
all the rays into a single parallel beam. Some rays will form a
converging (or diverging) cone instead. Then, this cone will be received
(I suspect that in the case of a diverging cone, some light may even get
lost on its way) by a tube lens and form a blurry spot on the image
plane. My question is, Is this situation really equivalent to the
standard one considered in all books? (I suspect, it's not because even
the distance to the tube lens should make a difference). But I would be
very interested in the opinion of those who understand optics better
than I do. Thanks!

Mike Model

Michael Model, Ph.D.
Confocal Microscopy,
Dpt Biological Sciences,
1275 University Esplanade,
Kent State University, Kent, OH 44242
tel. 330-672-2874

No virus found in this incoming message.
Checked by AVG - www.avg.com
Version: 9.0.733 / Virus Database: 271.1.1/2710 - Release Date: 02/26/10
06:57:00
James Pawley James Pawley
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Re: tube lens and spherical aberration

In reply to this post by mmodel
Hi Mike,

I agree with Guy. In fact going back to the "mental optical diagram"
in your original post, the "blurry spot" that you suggest occurs in
the intermediate image plane (and, larger, on your retina) is just
the caustic that he describes. This is not only because the rays
"fail to come to a common focus," but because they do this in a
specific way: the rays from around the periphery of the optic come to
a focus that is either closer to it or farther away from from it than
the focus of the paraxial rays near the optical axis.

However, regarding: "(I suspect, it's not because even the distance
to the tube lens should make a difference)", in the case the tube
lens is essentially part of the objective. Together, (and only
together)  they will form an aberration-free image a certain distance
behind the tube lens.

Wrong tube lens, NG.

Wrong distance: NG.

In short, one can ONLY design an aberration-free optical system once
one has first defined the positions of the object and final image
planes (In incoherent imaging  such as fluorescence, the optical
system is everything between the object and final image plane). This
is why we have objectives designed for different magnifications. One
could use a 100x objective is a lens with a focal length of about 2
mm. Despite what is written on the barrel, it could be used to form
an image that was, say, only 15x larger than the object. But if you
positioned the objective to make this occur, the plane at which this
this 15x image appears will be near the back of the objective itself
and it would be highly aberrated (and aberrated not just because the
light had yet to pass through the tube lens. It would even be
aberrated if the objective was a fixed-conjugate, rather than an
infinity, objective).

When I learned microscopy, I was taught that, although SA could be
completely corrected in the LM, as all EM (cylindrical) lenses
intrinsically had positive SA it could not be corrected in EM. Now it
is the EM guys who have corrected SA (by employing multipole lenses)
and the LM'ers now have a serious SA problems because they have
started to look at thick specimens that have the "wrong" RI.

Must be time to retire.

Jim Pawley

               **********************************************
Prof. James B. Pawley,                          Ph.
608-263-3147 Room 223, Zoology Research Building,              
FAX  608-265-5315
1117 Johnson Ave., Madison, WI, 53706  [hidden email]
3D Microscopy of Living Cells Course, June 12-24, 2010, UBC, Vancouver Canada
Info: http://www.3dcourse.ubc.ca/             Applications due by March 15, 2010
               "If it ain't diffraction, it must be statistics." Anon.

>I don't think that is true.  A lot of published versions start out from
>an objective forming an image of a point object.
>
>Many years ago I got a bit incensed at a diagram in a textbook,
>purporting to show SA introduced by a coverslip.  The rays leaving the
>coverslip were not parallel to those entering it!  I wanted a diagram to
>show my students, and this obviously wasn't it.
>
>So I sat down with pencil, paper and ruler.  First of all I drew a
>perfect lens forming an image of a point.  Then I drew a coverslip in
>the way, looked up the sines of the angles as measured, and constructed
>the ray paths.  Lo and behold, there was the classic caustic curve.
>(And, need I say, the rays exited the coverslip at the same angle they
>entered.)  So I traced it on OHP film and used it in my lectures
>thereafter (long before Powerpoint!).  And the students were much more
>willing to take it on board since it was constructed without any complex
>formulae - nothing more than Snell's Law.
>                                                     Guy
>
>-----Original Message-----
>From: Confocal Microscopy List [mailto:[hidden email]]
>On Behalf Of MODEL, MICHAEL
>Sent: Saturday, 27 February 2010 7:55 AM
>To: [hidden email]
>Subject: tube lens and spherical aberration
>
>(I apologize if this is a second post, I got some strange errors from
>the first one)
>
>Dear List
>
>It's not a confocal question, it's strictly a wide-field question...
>When people talk about spherical aberration they typically start with a
>parallel beam falling on an objective, and then, for whatever reason,
>the objective fails to bring all the rays into a common focus. In
>wide-field, one has a luminous spot in the object space, and the effect
>of spherical aberration would be a failure of the objective to collect
>all the rays into a single parallel beam. Some rays will form a
>converging (or diverging) cone instead. Then, this cone will be received
>(I suspect that in the case of a diverging cone, some light may even get
>lost on its way) by a tube lens and form a blurry spot on the image
>plane. My question is, Is this situation really equivalent to the
>standard one considered in all books? (I suspect, it's not because even
>the distance to the tube lens should make a difference). But I would be
>very interested in the opinion of those who understand optics better
>than I do. Thanks!
>
>Mike Model
>
>Michael Model, Ph.D.
>Confocal Microscopy,
>Dpt Biological Sciences,
>1275 University Esplanade,
>Kent State University, Kent, OH 44242
>tel. 330-672-2874
>
>No virus found in this incoming message.
>Checked by AVG - www.avg.com
>Version: 9.0.733 / Virus Database: 271.1.1/2710 - Release Date: 02/26/10
>06:57:00


--
               **********************************************
Prof. James B. Pawley,                          Ph.
608-263-3147 Room 223, Zoology Research Building,              
FAX  608-265-5315
1117 Johnson Ave., Madison, WI, 53706  [hidden email]
3D Microscopy of Living Cells Course, June 12-24, 2010, UBC, Vancouver Canada
Info: http://www.3dcourse.ubc.ca/             Applications due by March 15, 2010
               "If it ain't diffraction, it must be statistics." Anon.
--
James and Christine Pawley, 21 N. Prospect Ave. Madison, WI, 53726
Phone: 608-238-3953
mmodel mmodel
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Re: tube lens and spherical aberration

Thank you, Jim and others who replied to my question! - Mike

-----Original Message-----
From: Confocal Microscopy List [mailto:[hidden email]] On Behalf Of James Pawley
Sent: Tuesday, March 02, 2010 11:55 PM
To: [hidden email]
Subject: Re: tube lens and spherical aberration

Hi Mike,

I agree with Guy. In fact going back to the "mental optical diagram"
in your original post, the "blurry spot" that you suggest occurs in
the intermediate image plane (and, larger, on your retina) is just
the caustic that he describes. This is not only because the rays
"fail to come to a common focus," but because they do this in a
specific way: the rays from around the periphery of the optic come to
a focus that is either closer to it or farther away from from it than
the focus of the paraxial rays near the optical axis.

However, regarding: "(I suspect, it's not because even the distance
to the tube lens should make a difference)", in the case the tube
lens is essentially part of the objective. Together, (and only
together)  they will form an aberration-free image a certain distance
behind the tube lens.

Wrong tube lens, NG.

Wrong distance: NG.

In short, one can ONLY design an aberration-free optical system once
one has first defined the positions of the object and final image
planes (In incoherent imaging  such as fluorescence, the optical
system is everything between the object and final image plane). This
is why we have objectives designed for different magnifications. One
could use a 100x objective is a lens with a focal length of about 2
mm. Despite what is written on the barrel, it could be used to form
an image that was, say, only 15x larger than the object. But if you
positioned the objective to make this occur, the plane at which this
this 15x image appears will be near the back of the objective itself
and it would be highly aberrated (and aberrated not just because the
light had yet to pass through the tube lens. It would even be
aberrated if the objective was a fixed-conjugate, rather than an
infinity, objective).

When I learned microscopy, I was taught that, although SA could be
completely corrected in the LM, as all EM (cylindrical) lenses
intrinsically had positive SA it could not be corrected in EM. Now it
is the EM guys who have corrected SA (by employing multipole lenses)
and the LM'ers now have a serious SA problems because they have
started to look at thick specimens that have the "wrong" RI.

Must be time to retire.

Jim Pawley

               **********************************************
Prof. James B. Pawley,                          Ph.
608-263-3147 Room 223, Zoology Research Building,
FAX  608-265-5315
1117 Johnson Ave., Madison, WI, 53706  [hidden email]
3D Microscopy of Living Cells Course, June 12-24, 2010, UBC, Vancouver Canada
Info: http://www.3dcourse.ubc.ca/             Applications due by March 15, 2010
               "If it ain't diffraction, it must be statistics." Anon.

>I don't think that is true.  A lot of published versions start out from
>an objective forming an image of a point object.
>
>Many years ago I got a bit incensed at a diagram in a textbook,
>purporting to show SA introduced by a coverslip.  The rays leaving the
>coverslip were not parallel to those entering it!  I wanted a diagram to
>show my students, and this obviously wasn't it.
>
>So I sat down with pencil, paper and ruler.  First of all I drew a
>perfect lens forming an image of a point.  Then I drew a coverslip in
>the way, looked up the sines of the angles as measured, and constructed
>the ray paths.  Lo and behold, there was the classic caustic curve.
>(And, need I say, the rays exited the coverslip at the same angle they
>entered.)  So I traced it on OHP film and used it in my lectures
>thereafter (long before Powerpoint!).  And the students were much more
>willing to take it on board since it was constructed without any complex
>formulae - nothing more than Snell's Law.
>                                                     Guy
>
>-----Original Message-----
>From: Confocal Microscopy List [mailto:[hidden email]]
>On Behalf Of MODEL, MICHAEL
>Sent: Saturday, 27 February 2010 7:55 AM
>To: [hidden email]
>Subject: tube lens and spherical aberration
>
>(I apologize if this is a second post, I got some strange errors from
>the first one)
>
>Dear List
>
>It's not a confocal question, it's strictly a wide-field question...
>When people talk about spherical aberration they typically start with a
>parallel beam falling on an objective, and then, for whatever reason,
>the objective fails to bring all the rays into a common focus. In
>wide-field, one has a luminous spot in the object space, and the effect
>of spherical aberration would be a failure of the objective to collect
>all the rays into a single parallel beam. Some rays will form a
>converging (or diverging) cone instead. Then, this cone will be received
>(I suspect that in the case of a diverging cone, some light may even get
>lost on its way) by a tube lens and form a blurry spot on the image
>plane. My question is, Is this situation really equivalent to the
>standard one considered in all books? (I suspect, it's not because even
>the distance to the tube lens should make a difference). But I would be
>very interested in the opinion of those who understand optics better
>than I do. Thanks!
>
>Mike Model
>
>Michael Model, Ph.D.
>Confocal Microscopy,
>Dpt Biological Sciences,
>1275 University Esplanade,
>Kent State University, Kent, OH 44242
>tel. 330-672-2874
>
>No virus found in this incoming message.
>Checked by AVG - www.avg.com
>Version: 9.0.733 / Virus Database: 271.1.1/2710 - Release Date: 02/26/10
>06:57:00


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               **********************************************
Prof. James B. Pawley,                          Ph.
608-263-3147 Room 223, Zoology Research Building,
FAX  608-265-5315
1117 Johnson Ave., Madison, WI, 53706  [hidden email]
3D Microscopy of Living Cells Course, June 12-24, 2010, UBC, Vancouver Canada
Info: http://www.3dcourse.ubc.ca/             Applications due by March 15, 2010
               "If it ain't diffraction, it must be statistics." Anon.
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James and Christine Pawley, 21 N. Prospect Ave. Madison, WI, 53726
Phone: 608-238-3953
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Re: tube lens and spherical aberration

Re: tube lens and spherical aberration
Thank you, Jim and others who replied to my question! - Mike


You are welcome.

I forgot one more point that you might find interesting.

As the proper correction of SA depends on the image plane being a specific distance behind the tube lens, it follows that one can change the SA correction by changing this distance. Indeed, in older microscopes, one could adjust the tube length specifically to give the best SA correction under whatever imaging conditions were in use.

Of course, changing the tube length also changes the magnification and this is presumably the main reason why modern instruments lack this convenient adjustment.

Cheers,

Jim Pawley

              **********************************************
Prof. James B. Pawley,                                          Ph.  608-263-3147 
Room 223, Zoology Research Building,                                  FAX  608-265-5315
1117 Johnson Ave., Madison, WI, 53706                                [hidden email]
3D Microscopy of Living Cells Course, June 12-24, 2010, UBC, Vancouver Canada
Info: http://www.3dcourse.ubc.ca/            Applications due by March 15, 2010
               "If it ain't diffraction, it must be statistics." Anon.

-----Original Message-----
From: Confocal Microscopy List [mailto:[hidden email]] On Behalf Of James Pawley
Sent: Tuesday, March 02, 2010 11:55 PM
To: [hidden email]
Subject: Re: tube lens and spherical aberration

Hi Mike,

I agree with Guy. In fact going back to the "mental optical diagram"
in your original post, the "blurry spot" that you suggest occurs in
the intermediate image plane (and, larger, on your retina) is just
the caustic that he describes. This is not only because the rays
"fail to come to a common focus," but because they do this in a
specific way: the rays from around the periphery of the optic come to
a focus that is either closer to it or farther away from from it than
the focus of the paraxial rays near the optical axis.

However, regarding: "(I suspect, it's not because even the distance
to the tube lens should make a difference)", in the case the tube
lens is essentially part of the objective. Together, (and only
together)  they will form an aberration-free image a certain distance
behind the tube lens.

Wrong tube lens, NG.

Wrong distance: NG.

In short, one can ONLY design an aberration-free optical system once
one has first defined the positions of the object and final image
planes (In incoherent imaging  such as fluorescence, the optical
system is everything between the object and final image plane). This
is why we have objectives designed for different magnifications. One
could use a 100x objective is a lens with a focal length of about 2
mm. Despite what is written on the barrel, it could be used to form
an image that was, say, only 15x larger than the object. But if you
positioned the objective to make this occur, the plane at which this
this 15x image appears will be near the back of the objective itself
and it would be highly aberrated (and aberrated not just because the
light had yet to pass through the tube lens. It would even be
aberrated if the objective was a fixed-conjugate, rather than an
infinity, objective).

When I learned microscopy, I was taught that, although SA could be
completely corrected in the LM, as all EM (cylindrical) lenses
intrinsically had positive SA it could not be corrected in EM. Now it
is the EM guys who have corrected SA (by employing multipole lenses)
and the LM'ers now have a serious SA problems because they have
started to look at thick specimens that have the "wrong" RI.

Must be time to retire.

Jim Pawley

               **********************************************
Prof. James B. Pawley,                                         Ph.
608-263-3147 Room 223, Zoology Research Building,
FAX  608-265-5315
1117 Johnson Ave., Madison, WI, 53706  [hidden email]
3D Microscopy of Living Cells Course, June 12-24, 2010, UBC, Vancouver Canada
Info: http://www.3dcourse.ubc.ca/            Applications due by March 15, 2010
       "If it ain't diffraction, it must be statistics." Anon.

>I don't think that is true.  A lot of published versions start out from
>an objective forming an image of a point object.
>
>Many years ago I got a bit incensed at a diagram in a textbook,
>purporting to show SA introduced by a coverslip.  The rays leaving the
>coverslip were not parallel to those entering it!  I wanted a diagram to
>show my students, and this obviously wasn't it.
>
>So I sat down with pencil, paper and ruler.  First of all I drew a
>perfect lens forming an image of a point.  Then I drew a coverslip in
>the way, looked up the sines of the angles as measured, and constructed
>the ray paths.  Lo and behold, there was the classic caustic curve.
>(And, need I say, the rays exited the coverslip at the same angle they
>entered.)  So I traced it on OHP film and used it in my lectures
>thereafter (long before Powerpoint!).  And the students were much more
>willing to take it on board since it was constructed without any complex
>formulae - nothing more than Snell's Law.
>                                                     Guy
>
>-----Original Message-----
>From: Confocal Microscopy List [mailto:[hidden email]]
>On Behalf Of MODEL, MICHAEL
>Sent: Saturday, 27 February 2010 7:55 AM
>To: [hidden email]
>Subject: tube lens and spherical aberration
>
>(I apologize if this is a second post, I got some strange errors from
>the first one)
>
>Dear List
>
>It's not a confocal question, it's strictly a wide-field question...
>When people talk about spherical aberration they typically start with a
>parallel beam falling on an objective, and then, for whatever reason,
>the objective fails to bring all the rays into a common focus. In
>wide-field, one has a luminous spot in the object space, and the effect
>of spherical aberration would be a failure of the objective to collect
>all the rays into a single parallel beam. Some rays will form a
>converging (or diverging) cone instead. Then, this cone will be received
>(I suspect that in the case of a diverging cone, some light may even get
>lost on its way) by a tube lens and form a blurry spot on the image
>plane. My question is, Is this situation really equivalent to the
>standard one considered in all books? (I suspect, it's not because even
>the distance to the tube lens should make a difference). But I would be
>very interested in the opinion of those who understand optics better
>than I do. Thanks!
>
>Mike Model
>
>Michael Model, Ph.D.
>Confocal Microscopy,
>Dpt Biological Sciences,
>1275 University Esplanade,
>Kent State University, Kent, OH 44242
>tel. 330-672-2874
>
>No virus found in this incoming message.
>Checked by AVG - www.avg.com
>Version: 9.0.733 / Virus Database: 271.1.1/2710 - Release Date: 02/26/10
>06:57:00


--
               **********************************************
Prof. James B. Pawley,                                         Ph.
608-263-3147 Room 223, Zoology Research Building,
FAX  608-265-5315
1117 Johnson Ave., Madison, WI, 53706  [hidden email]
3D Microscopy of Living Cells Course, June 12-24, 2010, UBC, Vancouver Canada
Info: http://www.3dcourse.ubc.ca/      Applications due by March 15, 2010
       "If it ain't diffraction, it must be statistics." Anon.
--
James and Christine Pawley, 21 N. Prospect Ave. Madison, WI, 53726
Phone: 608-238-3953


--