I was recently fortunate enough to be able to spend a few days evaluating a Phase One IQ4 Achromatic camera back, courtesy of Teamwork Digital Ltd here in the UK. This back really interested me as it is a medium format (53.4mm x 40.0mm) back side illuminated sensor with no Bayer filter layer. Given my work imaging outside of the visible spectrum, this had a lot of potential, so I wanted to see what it could do. I wont go through all specs of the camera here, but this is prestige piece of imaging equipment and for more information about it head to the Phase One website.

Working with a sensor this large does present some challenges if you are used to cameras will full frame or APS-C sensors, chiefly that of the image circle produced by the lens you use. I have a few Hasselblad lenses designed for the old 6×6 cameras from my film camera days, but more on that in a future post. For the work I’ll be showing here I actually used an El-Nikkor 80mm f5.6 enlarger lens (old version with the chrome body), and this is shown mounted on the camera below.

Mounting the enlarger lens was relatively straightforward – Teamwork provided me with an adapter to go from the Phase One XF body to Hasselblad, and then I had a Hasselblad to M39 adapter setup from Zörk which has a ball joint (for tilt work) and a helicoid (for focusing). A setup like this makes macro imaging nice and simple, and this older version of the El-Nikkor 80mm has good UV transmission as well.

Subject wise, I used some lovely flowers from my local florist – Tangerine and Green, Englefield Green – as I knew I could get some which would have nice UV signatures. Lighting was done using a single Bowens GM500 studio flash head with a quartz flash tube which I had custom made. Images were taken in the UV using a Baader U filter, and in visible light using a filter stack of Schott S8621 1.5mm and a 420nm longpass filter.

Firstly, a sunflower in UV.

The UV sunflower image shows the expected behaviour of the dark centre to the flower, and the dark inner parts of the petals. The image above is the full frame shot captured by the camera – no cropping. Obviously the image above has been reduced in resolution for sharing here. As an example of how much information there is in one of the images produced by this IQ4 back, take a look at the two images below.

The images above shows the sunflower in UV again, this time with a red square that in the original full size photo would be 1000 x 1000 pixels. A crop showing this area in the original image resolution is shown below.

The amount of information contained within one of the images that the IQ4 back can produce is staggering. And keep in mind, I’m using an enlarger lens here, not one of the new lenses built for these cameras, so I doubt the resolution in my images is as good as what can be obtained.

The imaging setup for the flower close-ups is shown below along with a second flower that was imaged. I’ll be honest I’m not sure what this flower is (could be a Dahlia, however that is a bit of a guess), but it looked nice, and I thought it would make an interesting subject.

This is how the flower looked when imaged in visible light.

And now the same flower under UV light.

This flower looked very different under UV – it goes from being very pale in the visible spectrum to absorbing most of the UV light and looking almost black, apart from right in the centre.

Overall I was really impressed with the Phase One IQ4 Achromatic. There’s no doubting it is a premium product and it does come with a premium price tag, but the images it is capable of producing are certainly up there in terms of quality. Thanks again to the guys at Teamwork Digital Ltd for making this work possible, and to you for reading this. I will be sharing more images taken with this camera in future posts, including some Infrared ones, so check back in and see what else there is. If you’d like to know more about this or any other aspect of my work, I can be reached here.

Those that have read my posts before will know that I have a bit of a thing for UV imaging, and that I have been been building a UV microscope capable of imaging down to and below 300 nm. While doing so I’m always on the look out for second hand equipment which can either help with the work, or is of historical value to the whole area of UV microscopy. Today’s post provides some historical context to the development of UV microscopy and shows a couple of the early objectives designed for that job – the Zeiss Monochromats.

The key reason for the development of UV microscopy was the goal of improving resolution – as the wavelength decreases the maximum theoretical resolution that can be reached improves. It made sense therefore to move from visible to UV to see what could be achieved. This increase in resolving power is quite marked, as was noted in ‘Practical Photo-Micrography’ by JE Barnard, 1911, “The objectives made for direct use with ultra-violet light are called ‘monochromats’, and the wave-length for which these are corrected is 275 µµ [275 nm]. The N.A. of the highest power lens in the series is 1.25; but by the virtue of the shortness of the wave-length of the light, the resolving-power is equal to an objective used with white light of 2.5 N.A. – an objective which of course at the present time it has not been possible to produce.”. And nor is it today over a 100 years later. As a side note, the textbook used 275 µµ for the wavelength, and I added the [275 nm] as nm is more commonly used today. As a good friend reminded me, the way the book showed it is a little odd and a more correct way of showing it would be 275 mµ, or as is given on the objectives below 0.275 µ. Not sure why it was shown like this, but wanted to clarify in case of confusion.

What are these ‘monochromats’? Zeiss produced a range of them with focusing distances from 16 mm down to 1.7 mm, and these were summarized in a table in ‘Die Wissenschaftliche und Angewandte Photographie’ by Kurt Michel, 1957;

The Monochromat objectives were made from quartz lens elements, and were designed to be used dry (trockensystem) or with glycerin immersion. Glycerin rather than oil is used for these UV objectives as it remains transparent even down to 250 nm unlike the oils. They were also designed for use at specific wavelengths in the UV – 0,257 µ [257 nm] and 0,275 µ [275 nm]. These wavelengths were chosen as they are the strong emission lines for mercury (in mercury xenon lamps) and cadmium (from a cadmium arc source) respectively. This does not mean that they can be used at other wavelengths, but it is likely that image quality would suffer as a result. The 16 mm Monochromat might be a later edition to the range, as although it is mentioned in Michel’s book of 1957, it did not appear in Barnard’s text of 1911 (which only mentioned 6 mm, 2.5 mm and 1.7 mm objectives).

Enough waffle from me, what do these look like? I’ve been fortunate enough to find two of these objectives a 16 mm one and a 1.7 mm one. The 1.7 mm one was for sale on a ‘well known internet auction site’ and has come over to the UK from Ukraine, the 16mm one came from Germany where it became available for ‘the cost of the shipping to the UK’ as it was of no use to the original owner. It’s nice when that happens.

Here’s the 1.7 mm one, with its original objective keeper.

And the 16 mm one;

Both of these were designed to be used with the Cadmium line at 275 nm and both are RMS threaded. In theory they should be for a 160 mm tube length microscope, which is what I have, so I will certainly be trying these out. However it wont be at 275 nm – the lowest I can go with my current setup is 313 nm, and I have no plans on building a cadmium arc lamp (‘elf and safety and all that). I’m expecting relatively soft images, especially when compared with the Ultrafluar lenses, but you never know. Slightly worryingly, JA Needham in ‘The Practical Use of the Microscope’, 1958, said that “The quartz monochromats were corrected for one wavelength (275 mµ) [275 nm] and could not be employed with other wavelengths in the ultra-violet.”. However we shall see after some testing. I’ll also run these through my lens transmission measurement setup to get their transmission between 280 nm and 420 nm. While I’m not expecting any surprises with them (as they should be of all quartz construction), I like to check all new lenses that come in.

The history of imaging and microscopy is fascinating, especially when you dig into the details of how these amazing scientists and engineers tried to push the boundaries of what was achievable at the time. UV microscopy while being a technique that developed over a 100 years ago, is seldom used today as other ways of improving resolution have since come along. However it has huge potential in the field of imaging sunscreens, so is an area I will be continuing to explore and develop. Thanks for reading, and if you want to know more about this or other aspects of my work, I can be reached here.

When I’ve had a good experience with a supplier I like to try and mention them on my page, if nothing else as a bit of thank you. This brings me to Tangsinuo, a Chinese optical filter supplier. I recently found myself in need of some UV transmitting filters in larger sizes than I would normally be able to buy from Schott or other conventional suppliers. Big filters tend to command big (really) price tags even when they are available and this ruled out the more conventional suppliers for this work. ZWB glass is often seen advertised on ebay and other sites as being ‘equivalent’ UG1, UG11 and others, although some of the transmission graphs that come with the adverts have left me wondering how good they actually are.

One supplier – Tangsinuo – has been mentioned a few times on the UV photography forum which I’m member of, so I reached out to them to see if they could do large filters (200mm square) using the glasses I was interested in and was pleasantly surprised to find out that they could, and that they were very cost effective. In the end I placed an order for some 200mm square ZWB1 and ZWB3 glass, some 77mm diameter mounted filters in ZWB1 and 3, some 52mm filters in ZWB3 at different thicknesses, and also a load of fused silica 1mm thick microscope slides (75mm x 25mm) which are normally quite expensive items. All in all the price as extremely good even when I paid for expedited delivery – just over a week from China to the UK using tracked delivery.

So, how did they look? Transmission spectra of the filters, and the filter thicknesses, are given below (as measured using my Ocean Insight FX and STS spectrometers).

ZWB1 is said to be equivalent to Schott UG11, and it looks similar, although does leak a bit more IR than the Schott for an equivalent thickness. ZWB3 is said to be equivalent to Schott UG5, and again it looks similar. Overall, very impressive especially given the price.

I’ve not shared the transmission spectra of the fused silica microscope slides here, as well they are pretty much a flat line from 250nm to 1100nm and no where near as interesting as the filters.

My filters had a good surface finish (no surface striations which can sometimes be seen with some of these Chinese filters – I have a couple myself) and were chamfered at the edges.

So, thank you Tangsinuo. It should also be noted that they are open to working with customers on custom sizes and thicknesses too which is great to hear. Great prices and professional customer service are nice to experience, so please keep it up. If you’d like to know more about this or any other aspect of my work, you can reach me here.

As a photographer who spends a lot of time working outside of the visible spectrum I regularly use filters on my lenses or inside my camera to isolate the wavelengths of light I’m interested in seeing.

However filter choice can be far from straightforward, especially when imaging in the UV region. Today, I’ll give a quick example of why this can be a problem. First though a question – when is a filter not a filter? Take a red filter, which is often used in black and white photography to darker skies and lighten foliage. What is it doing to the light? What a dumb question, it’s letting red light through. Well, yes, it is, but then a simple clear glass filter would let red light through. With filters it’s not so much about what they are letting through (although that is obviously important), it’s about what they don’t let through. A red filter is red because it blocks light that isn’t red – it lets red through while blocking other wavelengths. When imaging in the UV region, this blocking becomes very important, because cameras are relatively insensitive in the UV region compared to the visible and IR regions. If the blocking on the lens isn’t up to scratch hen wavelengths you’re not interested in can make it through to the sensor and contaminate the image.

There are two main types of filters that photographers use – ionic filters such as Schott UG11 or Hoya U-340 which filter the light using the bulk properties of the glass itself, and dichroic filters which have a thin coating on one or both surfaces the glass which provides the filtering. Dichroic filters can just be on plain, colourless glass or they can be applied to an ionic filter, so the filtration is provided by the coating in addition to the bulk of the glass. An example of a dichroic filter in widespread use for UV photography is the Baader Venus U (commonly known as the Baader U).

Dichroic filters can be tailored to allow for very sharp cutoffs on the filters, and also high transmission, while ionic filters tend to have much smoother transitions. On the face of it, dichroic filter would seem to be perfect, for the UV photographer, offering high transmission and in theory excellent blocking of out of band wavelengths.

But there is a bit of an issue with dichroic filters which can be a problem if not considered. That is the effect that the angle between the incoming light and the filter has on its transmission properties.

Let me explain. I shall start with an example of an ionic glass UV filter – the LaLa U made by UVIRoptics. The LaLa U is an ionic filter stack which lets UV through while blocking visible and IR. Here’s what the transmission through the filter looks like at two angles – light incoming at 90 degrees to the filter, and at approximately 45 degrees.

Transmission was measured using an Ocean Insight FX spectrometer and light source. Tilting the filter to 45 degrees drops the transmission (as the light is going through a lot more glass), but the shape of the transmission peak doesn’t change. If the graph is replotted to look for leaks, I get the following.

As expected, the LaLa U has good blocking in the visible and IR regions, and tilting it does not make a difference.

Now, what happens when we look at the dichroic Baader U filter in the same way? First graph, full scale, second graph magnification to look for leaks.

The Baader U behaves very differently as it is tilted. Unlike the ionic LaLa U filter, the Baader U transmission spectra shifts to a shorter wavelength when the light is at 45 degrees to the surface of the filter. In addition the UV transmission profile is much more jagged in shape. Also, and even more concerning it is now letting in light above 680nm, and while 0.2% transmission may not seem like a lot, this can be an issue for UV imaging.

Some dichroic filters have even tighter transmission regions than the Baader U. Examples of these include Edmund Optics and Thorlabs 10nm bandpass filters. These both claim to have high blocking of out of band wavelengths, while at the same time giving high throughput in the region of interest. I use these for filtering light sources and also for imaging in front of camera lenses, although they are normally used more for filtering light sources than imaging.

How do these behave? Firstly, the Edmund Optics 330nm, 10nm bandpass filter which claims OD4 blocking (<0.01% in the out of band regions) and has a mirror finish on both surfaces of the filter as a result of coatings.

And next, the Thorlabs 340nm 10nm bandpass filter.

First, I should mention that the Edmund and Thorlabs graphs highlight some of the issues when using a solid state spectrometer like the one I have for looking at filters with really sharp peaks, and that is the artefacts that can occur at either side of the main peak in the profiles. The slight dip in transmission below 420nm and above 700nm for them both is not the spectrometers fault. That was all mine. I didn’t recalibrate the baseline while running these 4 filters, so the last two (Edmund Optics and Thorlabs) are showing a slight drop below 0% transmission below about 420nm and above 700nm. It was a sunday morning, I hadn’t had my coffee yet. Excuses over, and despite those effects, how does tilting impact the spectra? With the Edmund Optics filter, peak transmission drops from 330nm to 310nm, and reduces in intensity. Very worryingly though, it starts to let significant amounts of light through across the visible spectra and into the IR. This would be expected to seriously contaminate a UV image if not dealt with properly.

The Thorlabs filter peak transmission drops from 340nm to about 315nm, along with a huge drop in intensity. However unlike the Edmund Optics filter, it doesn’t develop obvious leaks in the visible or IR region (at least up to 800nm).

I should emphasize at this stage that these Edmund Optics and Thorlabs filters have not been developed for use as camera filters, and are designed to work with the light hitting them at 90 degrees to their surface, so it is not unexpected to see their performance being degraded when the light hits them at 45 degrees. Also, I’m not clear on whether other filters in their ranges behave in exactly the same way. Dichroic filters are tailored for the wavelength they are to be used at, as such they could well vary in the transmission they show at different angles.

If you’ve made it this far and are suffering from graphical overload, you can now take a breather – no more graphs. Why are these changes important and more importantly, what can be done about them if using these filters for photography?

As for the ‘why’ consider how light goes through a lens and reaches a camera sensor. It doesn’t just come from directly in front of the camera, but as a cone of light. The wider the focal length of the lens, the wider this cone. 45 degree either side of normal to the lens is pretty wide, equating to a focal length of about 22mm on a camera with a sensor the size of a 35mm SLR. As a result of this the spectral distribution of the light reaching the edges of the image could be very different to the light in the middle of the image, leading to strange colour shifts across the final UV image.

The 45 degrees used for the test here is a pretty tough harsh based on this, and the effects would be expected to become less severe as the angle gets closer to 90 degrees to the surface of the filter. For example a 105mm focal length lens has angle of about 23 degrees on a full frame (35mm) sensor camera. On longer focal length lenses, like a 105mm one, the effects described here would be expected to be much less pronounced.

What can be done about this? Longer focal length lenses will be less of an issue, so be aware that dichroic filters can have an issue when using wide angle lenses. Use a good and appropriately sized filter hood to block as much light coming in from the side as possible. If the mechanics allows for it, try mounting the filter behind the lens (between the lens and body of the camera). Although be aware that mounting a mirror finish filter just in front of the sensor can present its own problems with reflections. Perhaps the most obvious thing to do is consider using an ionic glass filter stack instead of a dichroic one. If the slightly reduced transmission is something you can live with, and there is no need for ultra sharp cutoffs to the light, then this can be the most flexible approach and can be used on a wide range of focal length lenses without changing the spectral distribution of the wavelengths getting through to the sensor.

This aim of todays discussion is not to have a downer on dichroic filters – they are extremely useful, offering high transmission and well defined cutoffs – the aim is to point out that depending on how they are being used they can have issues which need to be dealt with to get the best out of them.

There’s been a lot of graphs today, so well done if you’ve made it this far. Thanks for reading, and if you want to know any more about this or any other aspect of my work, you can reach me here.

The Collodion imaging process harkens back to to early days of photography. A photosensitive layer comprising a nitrocellulose carrier and silver halide on a glass plate forms the image capture media, and the result is a negative image of the subject – essentially a precursor to the more recent use of film photography.

Unlike modern films and digital cameras, Collodion plates are not sensitive to the full visible spectrum, being essentially unable to capture the longer wavelengths, while at the same time being sensitive to some UV. As such the images captured with them look very different to modern images, with very washed out skies being a common feature, along with darkened foliage. Skin tends to be captured as darker than it appears in normal visible light images (due to the increased absorption of short wavelength light be melanin) along with an emphasis of surface texture (again due to the short wavelengths being imaged).

Something I’ve wondered about since starting with digital photography is how to go about replicating the effects of Collodion in a digital camera. The first step was to try and understand the spectral response for Collodion plates. Some work has been done on this by LundPhotographics, who showed that it was mainly sensitive between 320nm and 520nm. This correlates well with the spectral response of an un-sensitized photographic plate as shown in “The Theory of the Photographic Process” 4th Ed by TH James (Figure 17.42 on page 512) which showed sensitivity between about 360nm and 510nm. With the work discussed by TH James they acknowledge that drop in sensitivity towards the blue end was a factor of the use of tungsten light which has limited blue and UV. Therefore the LundPhotographics range of 320nm to 520nm is a good start point, especially when imaging with sunlight.

The next stage was filter choice. I had a feeling Schott BG25 would be a good filter material to use for this as it has good transmission in the UV and blue regions. However it has a problem in that it transmits IR as well, and as digital cameras are very sensitive to IR this would need to be blocked. There are a range of filters which can be used for this such as Schott s8612 and BG39. During an eBay trip one day I came across a seller who had some 2mm thick BG25 along with 2mm thick BG18 (which is also a good IR blocker). Even better these were large – 75mm diameter – and cheap. So a quick purchase later, and some 77mm filter rings from Kood International, and I had some filters which could be used on lenses with a 77mm filter thread making them very versatile.

This first thing to do was measure the transmission spectra of the filters, and I did this using my Ocean Insight FX (UV and visible) and STS-NIR spectrometers which I use for a lot of my work. This gave me transmission spectra for the filters between 250nm and 1100nm as shown below.

By combining the two filters, the result was transmission between about 330nm and 510nm, with good blocking at shorter and longer wavelengths (especially the IR) – the green line in the graph above. This correlates well with the range for Collodion sensitivity derived by LundPhotographics. One slightly odd thing with the spectra – the BG25 was letting through less IR than I would have expected for a 2mm thick one based on the Schott online filter calculator. Measurement of the thickness showed it to be 2.1-2.15mm thick, but even that could not account for the transmission in the IR. Perhaps it’s just an odd batch (the filters were old ones) or perhaps the specs have changed slightly over the years. I’ll never know for sure on that. However the BG18 would do a good job of blocking even if the IR transmission of the BG25 was little more than it is.

To capture an image, I need a camera which was sensitive to the 300-550nm region, and for this I used my Canon EOS 5DSR multipectral conversion. The lens was a Canon 17-40 f4 (at 19mm). Image captured in my garden in direct sunlight, and as a comparison shot, a visible light image taken with a camera phone at the same time.

Firstly the digital Collodion image.

And the normal visible light image.

As expected the digital Collodion image has washed out sky and darker green foliage when compared to the visible light image. In hindsight I could have used a monochrome converted camera as this would have boosted the UV sensitivity compared to the camera used here, although this would have needed me to use a different lens as well, as this one wouldn’t have let that much UV through. So my Collodion image here isn’t as ‘UV heavy’ as it could be and is mainly comprised of long wavelength UV from about 380nm and blue light. Lens and camera choice is certainly something to consider for future work with the filters.

Revisiting old photographic processes forces us to think about the image capture process as a whole and the factors that are important to it. In doing so we learn more about the methods we are using, their limitations and how they can be improved. This type of thought process is vital to the world of supporting claims for products, as without knowing how the methods we use work, how can we understand their limitations – what they can and can’t be used for?

If you made it this far, thanks for reading and if you’d like to know more about this or any other aspect of my work, you can reach me here.

I try and publish as much as I can about the work I do – it gets the science out there so it can be built on by others which is hugely important for pushing research forward. Sometimes I may not have enough experience or data in a specific field myself to be able to pull together an entire publication, however I do get asked to help with work in a wide range of research fields especially with regards to imaging.

One area which has strong links with skin and imaging is that of forensics, and UV photography has applications in that field. Due to my work on the measurement of lens transmission in the UV, Dr Kevin Farrugia, at De Montfort University, approached me in 2020 with some questions about UV imaging, which led to some interesting and thought provoking discussions about what was actually important when doing UV imaging.

Dr Farrugia recently published an article on UV imaging of fingerprints, and looking at how the choice of equipment can influence the results. The article “A pseudo-operational trial: An investigation into the use of longwave reflected UV imaging of cyanoacrylate developed fingermarks” was recently published in Forensic Science International.

Always nice to get a mention in the acknowledgements on a paper (you’d be shocked to find out how often this doesn’t happen after these types of discussions), so thanks Kevin. Part of having expertise in an area is the responsibility to teach others and pass on that knowledge, especially to Universities, and it is something I will continue to do in the future.

Some purchasing experiences can be a bit of nightmare. Unfriendly or unhelpful staff, packages that go ‘missing’ during shipment, and courier companies that feel as though leaving your parcel on someone else’s doorstep and providing you with some tantalizing clues as to where it is, is as much fun as going on an organized treasure hunt.

Other companies though, just get it right. Enter Thorlabs. Thorlabs produce and sell a huge range of optical components, and I often use their parts and adapters when building lenses such as a UV lens I made based on their 79mm UV Aspheric lens.

This has proved to be used for UV imaging and can potentially even be useful well down into the short wavelength UVC region.

But this where they get a big ‘tick’ from me – customer service. When you ring them up and ask for advice, they genuinely sound as though they want to help. Thank you, thank you, thank you. Add that to the range of kit they sell and the good prices and you have a winning combination. And then we come to the icing on the cake. In with the deliveries you often get Lab Snacks – nibbles and treats to help make the day go more smoothly (by the way Thorlabs, my wife says thank you so much for these).

In a world of mediocre customer service, it is great when you get something like this. Thank you Thorlabs, I’m a very satisfied customer and shall continue to buy many more optical components from you in the future.

As part of life’s journey sometimes it is useful to look back to see where you’ve come from, so today, please excuse my self indulgence as that is just what I’m going to do with regards to my experiences with ultraviolet (UV) photography. I’ll put a few links to pieces I’ve written along the way, to provide more background where needed. I’ll also mention a few of the UV equipment related suppliers and contacts I’ve made along the way, although I’d like to make it clear that I am in no way sponsored or funded by them.

Photography has been a part of my life for a long time – even when a boy I would often have a camera in my hand, and I suppose I have one of my brothers to thank for that. He was a film cameraman so was (and still is) a great inspiration to me. My other brother (also an inspiration) while not a photographer was an artist so pictures and picture taking was always around while I was growing up. In 2000 I bought my first proper film camera under supervision of a good friend from University and of course being a scientist looked for things to do with it beyond taking ‘snaps’.  This led me to infra-red (IR) photography and the even more mysterious UV photography. UV imaging was one of those mythical areas which used mysterious lenses made of exotic materials such as quartz and calcium fluoride, and needed strange filters which blocked all the visible light, and it was all very intriguing. I even tried doing some with a normal camera lens and some UV sensitive film, and got some ‘less than optimal’ results. So as a technique I filed it away as one of those ‘to be done later’ approaches.

Fast forward a few years and I was working for P&G in their Skin Care group, and again UV imaging appeared as an area of interest from my mentor. Like me he found it a fascinating area and even had some of these mythical UV lenses from his research. However it was still well beyond my means at the time to go into this in any serious way, and I settled for IR photography as a way of getting my geeky fix for non-visible photography.

We now jump a few years forward again to the winter of 2017 and someone I was working with asked me if I could come up with a way of visualising sunscreens and how they spread to help with development of new topical sun protection products. Given how sunscreens absorb UV light, it immediately got me wondering whether UV photography could be used for this. But there was a problem – when you hit a film of sunscreen with a bright light, you get a lot of reflection from its surface which hides information on the film morphology. Easy I thought, let’s just cross polarize the light source and camera like I do for visual light photography. Oh, the naivety of youth. As with many things UV related this proved to be a little less straightforward than I originally thought, but it started me down the route of seriously looking at UV photography. This was where I jumped down the rabbit hole…..

After working with a UK supplier (Advanced Camera Services Ltd) to get a UV converted camera, a lens and UV flash, I then designed a cross polarisation setup for it, the result of which was a system which could do cross polarised images of sunscreen films showing the film morphology. This was written up and published in the International Journal of Cosmetic Science, as being able to combine UV absorption of the film with information about the film morphology looked to be giving a more accurate correlation with in-vivo measured SPF values that did not considering the morphology.

It was about this time that I also came across the Ultraviolet Photography forum. This collection of individuals from around the world had a tremendous background knowledge of all things UV photography related, and time spent on the forum was time well spent. I also found Dr Klaus Schmitt who is a UV imaging expert and dealer in unusual lenses. This led me to my first personal UV purchase – an Asahi Ultra Achromatic Takumar 85mm f4.5.

There’s something very special about looking at a camera lens and then realising that those lovely lens elements aren’t actually glass (or plastic as is sometimes the case these days). Of course I was bitten by the bug after getting the Asahi, and I’ve been fortunate enough to get hold of a few other unusual UV lenses since then, including a 105mm f4.3 Zeiss UV Sonnar (designed for medium format 6×6 cameras), a prototype Leitz Elcan 52mm f5.6 which was designed as a UV lens, a Katoptaron LDM-1/s 800mm long distance microscope, a Zeiss 60mm f4 UV Objektiv, a Nye Optical 150mm f1.4 mirror lens and an Astro Berlin Quarz 120mm f2.1 large format lens.

I suppose I’ve become a bit of a collector, but I see it more as the role of a curator. Being made in small numbers most of these are of historical interest, so I look after them and will eventually pass them on to the next generation of photographers. All of these lenses have good (and some bad qualities) when it comes to use in UV but some of them have enough reach to get down well into the UV region below 300nm. The plan is to eventually write up research done on or with all of these lenses at some point. Somehow I get the feeling this will end up being a retirement project…. I also make my own lenses from the range of parts that Thorlabs sells (big boys Lego).

Of course lenses are only part of the story and you need a camera to capture the image. For my initial sunscreen work I bought a UV converted camera from Advanced Camera Services Ltd in the UK, which I still use for day to day UV imaging. Having a built in UV filter over the sensor is great for an SLR camera as you can still use the eyepiece (although focus point will likely be different in the UV depending on the lens). One of the big issues with modern camera sensors with regards to UV imaging is the presence of the Bayer filter – the transparent coloured layer which creates the red, green and blue image on most sensors. While this is great for the visible region, the dyes used absorb loads of UV, especially at the shorter wavelengths, so has a big impact on camera sensitivity. Fairly early on I came across a company in the US – MaxMax (Llewellyn Data Processing LLC) – who were offering monochrome conversions of cameras, where they were removing this Bayer filter layer in a very controlled way, so I got one of my cameras converted. In fact I was so impressed with his work, that I’ve ended up getting various cameras worked on by him, including two Canon EOS 5DS R’s (one to monochrome and one just for multispectral imaging with the Bayer filter still intact). It was these Canon cameras which were the basis for my publication in the Royal Photographic Society Imaging Science Journal in which I used a device I’d built for measuring camera sensor sensitivity to look at how thee conversions impacted UV imaging ability. I actually have another paper looking in more depth at monochrome camera conversions and spectral sensitivity in the UV, visible and IR which will hopefully be published later this year.

Next we come to filters. Blimey, filters for UV imaging. This can be a bit of tricky area as of course a filter for UV imaging needs to be able to effectively block anything which isn’t UV. For a typical camera sensor this mean blocking from 400nm up to around 1200nm and because camera sensors tend to be more sensitive to visible and IR than to UV, the blocking of these wavelengths needs to be good. Very good. A lot of people use the Baader U filter from Baader Planetarium for their work. This is a filter designed for telescopes, so typically needs a bit of modification for using on a camera lens, and is dichroic which can lead to some odd colour fringing on wide angle lenses. I’ve also found the filters made by UVIRoptics to be very good, and he offers non-dichroic ones which don’t have the colour fringing issue with wide angle lenses. Also Invisible Vision here in the UK offer a good 308nm UVB filter with a mount suitable for normal camera lenses. I must admit, I’m a bit of a filter junkie and have far too many of them, but the set of 10nm band pass filters which go from 310nm to 390nm from Edmund Optics and Thorlabs have been very very useful, although they are only 1″ diameter, they are fine with the 105mm UV Rayfact macro lens (and other small element lenses).

Actually, while working in the UV I’ve found that a lot of stuff needs to be built as it cannot be bought (or if it can be bought, you need very, very deep pockets). This has led me to building my own setups for measuring camera sensor sensitivity and lens transmission, both of which have led to publications in peer reviewed journals. The paper containing the lens transmission work was awarded the Paper of the Year for 2020 in the International Journal of Cosmetic Science which was a great honour to receive.

The last year has of course been hugely difficult for many people. When the first lock down came around I found myself in need of a new project to keep busy. As I had relatively little experience with microscopy, and given its very visual nature, I thought it would be a good skill to learn to compliment my other imaging work. I decided to buy an older microscope in need of fixing up, so settled on an Olympus BHB from the 1980’s. This poor thing looked like it has been stored in a field for a while, but could be taken apart and cleaned with relatively simple tools. Like many projects it became somewhat obsessional for me, and I soon got to wondering whether it could be transformed into a UV transmission microscope. This would be no simple task as there is a lot of glass in a microscope. So I set about learning about UV microscopy and kept an eye out for second hand equipment such as objectives and condensers. I had a couple of lucky purchases relatively early on and managed to find a Leitz 16x UV objective with good UV transmission down to and below 300nm, and an vintage Zeiss quartz condenser (although I did also make my own condenser at one point using a UV fused silica half ball lens).

I also came across the Quekett Microscopical Club which was founded in 1865 and even has its own peer reviewed journal. What better place to learn about old microscopy equipment I thought and applied to join. As with the photography I’ve found myself no collecting anything related to UV that I can find and use so have a wide range of UV lenses, both refractive (such as the Zeiss Ultrafluars), and reflecting (mirror lenses). All of these have been bought second hand as new they would have had eye-wateringly high prices.

The UV microscope is now complete, although as a tinkerer it will be improved upon, and I am starting to do research into sunscreens using it.

Scientifically, my UV journey has been challenging, fascinating, frustrating at times, but ultimately very rewarding and is an area I shall be continuing to work with in the future. In addition to the obvious areas of interest such as sunscreens and skin imaging, my plan is to explore different areas such as forensics, geology and even anthropology to see what looking at things in a different way can bring to research in those fields. Microscopy has proved to be a fascinating research area for me and I’ve already written a couple of UV related articles on it with more to come in the future.

Thank you for reading and if you’d like to know more about my work you can reach me here. I’ve included a small publication list at the end of the article which includes some of the key articles I’ve written on this area along with the talks I’ve given to date.

UV related publications and talks

“Yooperlite – Imaging the fire within using UV”, JM Crowther, Quekett Bulletin, 2021, 80, 53-56.

“Chapter 28 – Dermatological imaging – A survey of techniques“, A Davies, JM Crowther, in Photography in Clinical Medicine, Ed. P Pasquali, 2020. ISBN 978-3-030-24543-6. https://doi.org/10.1007/978-3-030-24544-3_28

“Chapter 29 – Beyond the visible: UV, IR and fluorescence imaging of the skin“, JM Crowther, A Davies, in Photography in Clinical Medicine, Ed. P Pasquali, 2020. ISBN 978-3-030-24543-6. https://doi.org/10.1007/978-3-030-24544-3_29

“UV reflectance photography – what are you imaging?“, JM Crowther, International Journal of Cosmetic Science, 2020, 42(2), 136-145. https://doi.org/10.1111/ics.12591

“Visualising Sunscreens Using UV Photography”, presented at the Sun Protection Conference, London, UK, 2019.

“Imaging of the skin – UV, visible, IR”, presented at the Royal Photographic Society Imaging Science Group meeting, London, 2019.

“The big reveal: UV imaging uncovers sun protection, skin dryness and microbiome“, JM Crowther, Cosmetics and Toiletries, Sept 2019, p.32-45.

“Understanding colour reproduction in multispectral imaging: measuring camera sensor response in the ultraviolet, visible and infrared“, JM Crowther, The Imaging Science Journal, 2019, 67(5), 268-276. https://doi.org/10.1080/13682199.2019.1638664

“Calibrating UVA reflectance photographs – standardisation using a low-cost method“, JM Crowther, Journal of Visual Communication in Medicine, 2018, 41(3), 109-117. doi: 10.1080/17453054.2018.1476819.

“UV Photographic Imaging – Sunscreens and Skin“, The Cosmetic Chemist, 2018, 15th October.

“Understanding sunscreen SPF performance using cross polarised UVA reflectance photography”, JM Crowther, International Journal of Cosmetic Science, 2018, 40(2), 127-133.

Have you ever wondered what the inside of a microscope objective lens looks like? Why am I even asking that, of course you have, haven’t we all. All the tiny components, the little lenses. Very cool. Sometimes we get to see schematics of what they look like in cross section in manufacturers brochures or in other publications, but usually that is as close as we get to actually seeing what is going on in there.

I recently saw an objective for sale which had been sectioned from end to end by Spectrographic Ltd in the UK, so put in a bid and was lucky enough to buy it. The objective was an Olympus HI M100 1.30 which was unfortunately broken (no working lenses were sacrificed in the making of this section). Looking from the side it looks ok, a bit beaten up perhaps, but ok;

However turn it around and it looks very different.

Keep in mind that this objective lens is only about 25mm long. By sectioning it the amazing engineering that it takes to make one of these is revealed. The lens elements themselves are remarkable, as can be seen when we zoom in on them.

Going from left to right it looks like there are two singlets, and then two cemented doublets. Keep in mind that these are only a few mm across.

The images were captured using a Hoya Super EL 60mm enlarger lens as a macro lens as discussed here.

I’m very impressed by the quality of the section from Spectrographic Ltd, especially considering it is such a small item. This is something that is handy to have when explaining about microscopy – being able to show someone the inside of an objective is a step up from just looking at a sketch on a screen. Now then, where is that broken Beck reflecting objective I got a while back…..

Thanks for looking and if you’d like to know more about this or my other work you can reach me here. And please remember that the images in my site are copyrighted to JMC Scientific Consulting Ltd. If you’d like to share them, please ask first.

Sometimes in the world of photography we fall into the trap of ‘must buy that expensive lens everyone has been talking about’. However it is possible to use rather humble lenses to take good photos and they can often produce very high quality images for what is a very modest outlay.

Enter the Hoya Super EL 60mm f4 enlarger lens. This one cost me the princely sum of £30 on ebay. Here’s the lens;

As mentioned above this was a lens for an enlarger. It has a rather unusual 8 element 4 group lens construction and was designed to cover 6x6cm. The thread is M39 (common for enlargers) and is easy enough to adapt to M42 which is mountable to most cameras with an adapter. I used a helicoid on mine to, to allow me to vary the focus more easily.

What are the images from it like? Here’s a few from the garden, taken at either f8 or f11 on my Canon Eos 5DS R and hand held. I’ve reduced the resolution for easier sharing here.

Overall I like the images it produces, and the colours are nice. But how about resolution? The image below was pretty much the full frame of the original shot.

And now a crop from the middle of the flower image, kept at the original pixel resolution (i.e. not reduced for sharing).

I think there is plenty of sharpness there.

Enlarger lenses like this tend to make very good macro lenses and can often be had for very little money. Normally they are M39 threaded as well, so once you have the right adapters for your camera it is easy enough to swap between them if you want to try different ones.

We often want the latest and greatest in terms of equipment, but always keep in mind that new equipment isn’t everything. Also, check out the abundant web resources such as the MFlenses forum, and Photomacrography.net for inspiration and get snapping.

Thanks for looking and if you’d like to know more about this or my other work you can reach me here. And please remember that the images in my site are copyrighted to JMC Scientific Consulting Ltd. If you’d like to share them, please ask first.