AN ANALYTICAL XRAY SERVICES LABORATORY
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You can never have enough sample holders no matter what machine you’re running. We’ve certainly found this to be true at Texray so we always try to keep a large number of them on-hand. KS Analytical Systems has always made one-off and custom sample holders for the Bruker instruments, but we’re now offering the standard PMMA powder holders as well at significant cost savings over the OEM version. The standard holder (25mm x 1mm deep well) is priced at $55 with bulk discounts starting at 20 holders.

Custom well depths, diameters, grooved floors, side-loading and zero-background versions are available.

Our PMMA holders are compatible with Bruker D8 Focus – D8 Advance (single, FlipStick autosampler, 90-position autosampler), D4 Endeavor and D2 Phaser (single only) systems. D500 and D5000 instruments can also use these holders.

We’ve brought the complete manufacturing process in-house to give us the freedom to make the custom designs our customer have always asked for. This includes custom laser etching. Company logos are a common request, but we’ve also started serializing sample holders on request. At Texray, we even etch them with barcodes for tracking samples through the data collection process.

The pictures below show a custom funnel tool for filling side-loading sample holders. The tool is machined from billet aluminum with an acrylic window on the funnel to make it easier to gauge fill level. The funnel itself is polished and the viewing plate which allows the users to see when the sample well is full is made of sapphire crystal for maximum scratch resistance.

It’s relatively common for us to receive very small volumes of material for analysis. Often this is the total amount available so getting the right answers is extremely important. When these come in as powders, the answer is always to run them on a zero background plate, but sometimes that’s not the case. Luckily, there are other options for analysis of very small quantities.

The most common application for filter-membrane sample holders has always been respirable silica quantification. This is mandated by OSHA and is an extremely common industrial hygiene test. Ambient air is sampled with a fixed or mobile suction system and particles are deposited onto a PVC membrane inside a sealed cartridge. Testing procedures are defined by NIOSH7500 and since this is a total quantification method (not a relative method), it’s critical that the entire sample is measured. Unfortunately, the measurement cannot be completed on the PVC membrane as received. Transferring the sample powder to an Ag membrane is accomplished by dissolving or ashing the PVC away, diluting the remainder in a solvent and depositing it onto the Ag membrane by vacuum filtration. The end result is an extremely low loss of analyte even for very small volumes of material.

This preparation method is also very useful for other types of samples which might have crystalline particulate suspended in a solution. Drying samples can be time-consuming, heating them to boil off liquid can cause phase transitions in the crystalline analyte, and handling dry powder in very small quantities is a very good way to lose material. Vacuum filtration solves all these problems.

 

Our most popular custom sample holder is the SC40F25 which is designed to hold the common 25mm Ag membrane filters used for this type of mounting. The anodized Al body is a time-tested design that works very well and causes almost no interference with the data, unlike the original injection-molded plastic parts. However, the most common method for retaining the membrane has always been to drop a metal support disk behind it and use an ID snap ring to retain both the disk and membrane. This can be a frustrating operation even for experienced hands. Snap rings are hard to control and the high spring tension gouges the inner diameter of the Aluminum body to the point that the holders must be replaced periodically.

After watching so many clients struggling with this system, we thought we could find a better option. The first step was a simple, laser cut acrylic backer instead of the metal disk. The acrylic was thicker which limited the depth to which the snap ring needed to be set. This was an improvement but still required the snap ring.

The next step was 3D printed plugs which could be pushed into the well. These supported the membrane and held it in the plane of diffraction at the same time. A standard pair of pliers was all the was needed to grab the plug and gently rotated it to release the membrane. This seemed like the ideal solution, but we heard from one user who claimed that the plug was causing an interfering peak in his measurements. We’ve been around the block with 3D printed sample holders in general and it’s definitely true that the common thermoplastics used will crystallize when cooled rapidly. This causes lots of problems for routine analysis of powders, but this was the first we’d heard of a peak being visible through an Ag membrane. Perhaps this user had a particularly thin membrane, but regardless, we needed a new solution, both for their lab and our own.

 

Our current solution is a laser cut “spring” backer which again combines the function of retainer and support in one part. The spring is easy to install by hand and can even be removed by hand, but forceps or needle-nose pliers make this easier. These have been working very well so we’re hopeful that this is going to be a long-term solution that we can share with our clients.

 

 

 

Posted by: In: Uncategorized 03 Jan 2018 0 comments Tags: , , , ,

Most of the zero-background sample holders we make are designed with permanently affixed plates. We prefer this dramatically as loose plate are constantly getting dropped, chipped, or lost. However, a permanently affixed plate also gives us the freedom to precisely (within about 0.02mm) set the depth of the plate below the plane of diffraction. This can make a big difference in the results depending upon the volume of powder loaded as the standard “flush mount” puts the plate exactly in the plane of diffraction. This works fine for very small volumes, but it does guaranty the there will be a displacement error of some magnitude regardless of the particle size or volume. For this reason, we always offer custom recessing as an option. The only drawback to the permanently affixed style of mounting is that the offset (or flush mounting height) cannot be changed. Our preferred solution is to simply create a set of holders with various depths to accommodate different sample thicknesses, but we had a request recently for an infinitely variable mounting solution.

Complicating the project is that the holder was to be used in a D2 Phaser with a 6 position autosampler which does not use the same style of base holder as the single-sample variant or any other Bruker XRD that we’re aware of. We discussed several options. The large number of heights needed made multiple holders, spacers, and any other solution that relied on discreet steps unacceptable. The thin-walled sample bases and relatively tight dimensions made a screw-in insert unrealistic as well. The final solution was to build a custom tool for setting the ZBH at a specific depth. This requires the user to work with bare Si plates, but it meets all the design criteria and we’re hopeful that this will work well for them.

The tool is made from acetal (Delrin) plastic which is extremely resistant to chemicals, adhesion, and abrasion. It’s actually an ideal material for threaded parts and machines very well.

The dreaded “amorphous” hump created by x-rays scattering off plastic sample holders has plagued XRD users for decades. It’s a serious enough problem that we make a good volume of these holders from Aluminum which works very well for loose powders. The plastic scatters xrays at around 13 degrees 2Theta (Cu anode tube) which make a real mess of most geological patterns and isn’t fun to model out for Rietveld refinement. Zero background holders like our ZBH-32 work wonderfully in standard sample stages designed for a single sample at a time, but the large plate isn’t compatible with the autosampler.

I recently had a request for a hybrid holder which would allow for analysis of very small volumes of materials while retaining compatibility with the autosampler. This is almost identical to our standard powder holders, but with a well designed specifically for our small ZBH plate.

Key features include:

  • 6061-T6 Al material (anodized or as-machined)
  • Si(510) plate
  • Raised sample well minimizes the area of the sample holder in the plane of diffraction. (Original Siemens design)
  • Beveled well walls minimize the area of Al in the plane of diffraction
  • Other small modifications are made to improve reliability of these holders in the autosampler

One of the fundamental facts of lab-based X-ray production is that our x-ray tubes emit much more than the pure KA1 lines we rely on for material characterization and quantification. Most XRD users are familiar with techniques and hardware for the reduction or elimination of KB1, W LA1 and Bremsstrahlung, but take for granted the inseparable pair of KA1 and KA2 (referred to as the “doublet”). Luckily for us, these energies are present in strict proportion such that we can factor their paired presence into most XRD analysis to the point that one might barely notice their effect. However, the fact remains that we will see peak broadening at lower angles and completely independent additional peaks at higher angles due to this superfluous discrete emission.

Separating the doublet cannot be accomplished electronically or through absorption/attenuation such as might be effective for KB1 energies. It must be done in the primary-beam with an additional diffraction event. Primary-beam monochromators are generally classified by the number of diffraction events required for a photon to pass completely through the device. Single-bounce, 2-bounce and 4-bounce geometries are common with the latter providing the best energy resolution allbeit the lowest intensity (photon flux). My limited experience suggests that while the single-bounce models retain enough intensity to have some application in powder XRD, the others are relegated to HR-XRD applications such as XRR.

The alignment for any of this hardware is not for the faint of heart as it begins with coarse adjustments using fluorescent screens in the beam path. This was essential for us given how dramatically misaligned the monochromator had become after so many attempts to bring it back into operation. We actually needed our SDD system to verify that we were tuning for Cu KA1 energy rather than the KB1 emissions because some of the most basic aspects of the alignment had pushed way beyond their intended position.

Along the way we built ourselves a motorized remote adjustment tool which we’ll return to the user as small adjustments are required on a regular basis with this kind of monochromator to retain maximum intensity. It’s quite useful and even versatile enough to allow for the adjustment of multiple control knobs.

One final note regarding intensity. It’s easy to get excited about energy resolution like this, but bear in mind that we’re looking at ~20x reduction in intensity due to the inherent losses involved in the primary diffraction event. This data was collected at 10x the normal speed and at half the normal 2Theta step increment so it looks very good, but one would need a compelling reason to slow their data collection this much.

Another side effect of performing your energy discrimination in the primary beampath is that other issues such as fluorescence effects (incident x-rays exciting elements in the sample causing high background intensities) are harder to avoid than they would be with a diffracted-beam monochromator. The 4x reduction in intensity inherent in the diffracted-beam monochromatization makes it a poor choice to eliminate these effects when the incident intensities are already so low. We recommend energy-dispersive detectors such as our SDD-150 to eliminate extraneous energies without sacrificing net intensity. We’ve also worked with the Bruker LynxEye XE-T detector which has a very high energy resolution compared to other position sensitive detectors (PSD). Contact KS Analytical Systems for more information on these options.

FCT 0027 Xray decal visual croppedWe’ve been working with XRD machines for about 40 years now and to be quite honest, very little has changed. Most of the really exciting advancements have been software based, but there have certainly been changes to the hardware as well. We’ve introduced a few ourselves such as the KSA-SDD-150 detector. Automatic anti-scatter and divergence slits, additional axes and degrees of control have all increase the versatility of these instruments and opened them up to more advanced and unique experiments, but nothing has had an effect matching the new crop of Position Sensitive Detector (PSD). These have been around for decades, but didn’t really become popular until the a solid state version was introduced. There are still some trade-offs as mentioned in our KSA-SDD-150 post, but when you need speed, a PSD is the way to go.

Until recently, the only option for clients looking for this kind of speed was either a new XRD or a refurbished Bruker D8 system with a LynxEye or Vantec-1. While the D8 is a great machine and the LynxEye is a world class detector, the cost is usually too much for academic or small labs to bear. This has all been changing recently with the introduction of a truly aftermarket detector system from FCT ACTech. No other company that we’re aware of has worked so hard to make their hardware as turnkey as possible so the user isn’t left holding a box of parts and an instruction manual.

We can now offer detector upgrades for D5000 Theta/Theta and D5000 T2T systems with kits soon to be available for D500 systems as well. Software integration with DiffracPlus (standard software for Bruker XRD systems) is seamless and full integration with MDI Datascan is very close to completion. The future is very bright for users of these XRD systems.

Contact us for more information on these detectors


NovaculitesiliconKey features:

  • Data collection at 30x the speed of a standard point detector.
  • Dramatic increase in throughput
  • Plug-and-play retrofit
  • Maintenance free (no gas charge required)
  • Stand-alone operation for custom experiments
  • Excellent angular resolution

 

Technical Specifications:

  • Maximum count rate: 500Kcps / pixcel, 50Mcps global
  • Maximum scanning speed: 120 deg/min
  • Angular resolution: 0.06 deg at 200mm radius
  • Strip pitch: 120um
  • Number of channels: 96
  • Angular span: 3.3 degrees
  • Energy resolution: <10%
  • Energy range: 4.5KeV to 17KeV, efficiency at 30KeV is 10%
  • Compatible with all common XRD tube anodes including Cr, Fe, Co, Cu, Mo and W.

XRD sample holders are easily the most common items we’re asked to machine. Sometimes it’s because they’re no longer available, but usually, it’s to accommodate some special application. Sometimes it’s as simple as making them from Aluminum to allow for cleaning with acetone or other harsh solvents. Other times it has more to do with the clients preferred style of loading or sample volume. The end result is that there’s very little consistency so our process needs to be as versatile as possible. This video highlights the most recent process. It’s hard to see exactly what’s going on through the coolant, but this is a test run of a program to cut special holders for 25mm filter membrane holders for respirable silica measurements (or anything else one might want to deposit onto a 25mm filter). It’s cutting the bottom of one holder and the top of another (each on its own side of the fixture).  A full load of these produces 6 complete holders for every run.

Siemens goniometers are about as sturdy as they come. Large diameter gears and bearings spread out forces across a wide area resulting in smooth and stable performance as well as very high load handling due to the added leverage of this arrangement. For this reason, they’ll run for many years even after the grease inside has become hard and contaminated with dust. Most users don’t even know their goniometer is getting stiff until we check it during a PM. Catching this before the goniometer starts to hang up saves thousands of dollars and weeks of down time. Our goniometer rebuild service involves complete disassembly of the goniometer down to individual ball bearings for a thorough cleaning. We’ve tried to duplicate this procedure on-site with very limited success as the large components are best cleaned in a full size solvent bath and it’s special brackets are required to avoid concentricity issues during reassembly. All the critical electronics are replaced during reassembly along with fresh lubrication. The best case scenario is that we catch issue far enough in advance to get a matching replacement goniometer rebuilt and shipped out. There are too many variants to keep rebuilt units in stock all the time. This way we only need to come to the site once to swap the goniometer and perform the necessary zero alignment. The old goniometer goes back in the same crate and we’re done in a day or two. Waiting till a hard failure of the goniometer means a trip out to identify the problem and disassemble the system. The goniometer is shipped in for a rebuild which can easily take a few days to complete before being shipped back along with a second on-site visit. I’d estimate the extra cost to be right around $6k plus the cost of shipping and two weeks of downtime. We certainly don’t mind going this route, but if it were my money, I’d rather spend it on a comprehensive check of the machine rather than emergency services.

These pictures are from one of our first full rebuilds. This instrument was installed in a D5000-MATIC instrument at a cement plant. I’ve never seen so much dust inside a goniometer. Another particularly rough one was from a horizontal goniometer on a single-crystal system at a university. The students had a terrible habit of breaking Si(100) wafers and dropping them onto the goniometer face. Those little shards made their way into the bearings resulting in a rather perilous rebuild with shards of Si throughout it.

A large part of our business at KS Analytical Systems is refurbishing and reselling WDXRF and XRD instrumentation. We specialize in Siemens and Bruker models because, and I can’t stress this enough, they last. Siemens was 20 years ahead of their time with features like full computer automation, interlocked radiation housings (not just an enclosed beam path) and independent axis control coming standard on most systems. The D500 may well be the most reliable powder diffractometer ever built and for most of our history, it’s outsold all other models of XRD and XRF combined. Most users are simply performing basic powder scans with many running the optional 40-position sample changer, but I always get excited when I find someone pushing the limits of the platform.

Several years ago I was approached by a new professor at a major American university about purchasing a refurbished Siemens D500 XRD. He’d been seriously considering a new instrument from one of the big-three OEMs, but chose to focus on the D500 due to its reputation for low cost of ownership, versatility and nearly identical resolution/intensity to the new system he’d been looking at. It’s been a few years since that unit was delivered and I’ve been very impressed with the improvements that have been made.

The first step was to bring the software up to date with a complete package from Materials Data Inc. (MDI). This included Datascan 5.0 for instrument control and data acquisition as well as the flagship Jade 9.5 analysis package. Whole pattern fitting (Rietveld), semi-automatic phase ID (Search/Match) and a host of other advanced quantitative and modeling options are included. Jade 9.5 is modular and can be purchased with any combination of these options. I’d estimate that 70% of the XRD systems we sell go out with some level of MDI package. We’ve been working with them for 20 years now and have never heard anything other than glowing praise for their excellent products and support. One key feature of Jade is that it was designed to be a universal analysis solution from the ground up so there’s never a problem opening any of the OEM file formats. It’s much easier to justify the cost to upgrade your software when you know it will integrate seamlessly with any other data or instruments you may encounter. Contact KSA if you’d like more information on this.

Jade 9.5

This is Jade 9.5. You’ll notice that it’s a much different interface than the Jade 2010 program I usually use. This option is modular with available plug-ins for all the higher level functions of Jade 2010, but 9.5 is perpetually licensed.

Virtual XRD

This is actually the VirtualXRD program that comes along with Datascan. I don’t use it often, but some of my users run extremely long count times and predicting the affect of a parameter change could save them days of experimentation. It’s a great tool even for users running simple 1 hour scans.

 

 

 

 

 

 

 

 

 

 

 

The next step was more hardware based than anything else. The independent axis control of the D500 (in Theta/Theta or Theta/2Theta configurations) allows for both rocking curves and grazing incidence scans. With the goal of analyzing thin-films in mind, we upgraded the D500 with a grazing incidence attachment. These are designed to minimize scatter while the sample is held at a shallow (usually 3 degrees) incident angle and the scan is performed with the detector alone. The attachment consists of a long collimator coupled with a simple monochromator just before the detector. We’ve performed some rather intense studies with one of these at Texray and were very impressed with its performance. In fact, we use it whenever practical even though we have a dedicated parallel beam optics system in the lab as well. It was about time for a new tube so a new, ceramic Cu long, fine focus tube was included in the upgrade.

Ceramic XRD tubeGrazing incidence attachment

 

 

 

 

 

 

 

 

 

 

Some additional software solutions were developed on-site to facilitate XRR (X-ray Reflectivity) measurements around the same time. I confess that this is not something I’m personally very familiar with, but it seems fascinating. It involves scans at extremely low angles which can require caution since one is working with a very nearly direct beam.

The last upgrade he made is actually the one that most impressed me and the one I had absolutely nothing to do with. In an effort to further expand the capabilities of his instrument, he purchased and installed an energy dispersive detector with an integral digital pulse processor (DPP). Clever mounting and some experimentation allowed him to perform EDXRF elemental (qualitative AND quantitative) analysis on samples while using the D500s X-ray tube as the primary emission source. The flexibility of the D500 platform even allowed him to control the effective layer depth by adjusting the incident beam angle. Since his application involved analysis of a thin film coating, he set the goniometer to a low angle to minimize penetration depth and substrate interference. After seeing how well this worked, I immediately started working on a similar upgrade that we could offer to all our current and future XRD users. I’ll detail my early progress in the next post.

All of the powder XRD (PXRD) systems we work with use either manually interchangeable aperture slits or automatic (stepper motor driven) slits to control divergence and scatter. One of the most common questions I hear from new users is “What is the ideal slit arrangement”. While I realize that there are many instruments out there with “one-size fits all” slits, the D500, D5000, D5005 and D8 optics are what I call “Research Grade”. This means that they can be adjusted and tuned for a particular application to maximize effects that are desirable and minimize those which are not. One of the most common reasons to change the anti-scatter and divergence slits is to reduce scatter over the sample at low angles. This scatter is the primary limiting factor for users who want to see diffracted peaks at very low angles. At Texray, we offer instrument time (data collection) as one of our services and have received requests for starting angles as low as 1 degree 2theta so it occurred to me that now would be a good time to collect some reference data and answer this question once and for all.

The image on the left shows the effect that the anti-scatter and divergence slits have on low angle scatter. The image on the right is of the two primary reflections of quartz (Novaculite) with the same slits. Note the intensity loss. The benefit of automatic slits is that they can be set very small at the beginning of the scan and gradually open up throughout the angular range. Very few users need that kind of flexibility, but since we’re talking about slits, it bears mentioning.

Low angle scans with various slits

This data was collected with matched slits set at 0.2mm, 0.6mm, 1mm and 2mm. These correspond to practical starting angles of 0.6, 0.9, 1.4 and 2.5 degrees 2theta respectively.

Low angle scans with various slits PEAK COMPARISON

Looking at the actual peaks, you can see the affect the smaller slits have on the rest of the data. These were collected without the benefit of a diffracted beam monochromator and with the primary soller slit removed. Neither of these factors would have a dramatic impact on the result, but the lack of a primary beam soller slit explains the asymmetrical peak shape in the second scan range pictured.