Light sharing in multi-flat-panel-PMT PEM detectors

Large are a detectors, such as those used in positron emission mammography (PEM) and scintimammography, utilize arrays of discrete semtillator elements mounted on arrays of position sensitive photomultiplier tubes (PSPMT). Scintillator elements can be packed very densely (minimizing area between elements), allowing good detection sensitivity and spatial resolution. And, while new flat panel PSPMTS have minimal inactive edges, when they are placed in arrays significant dead spaces where scintillation light is undetectable are created. To address this problem, a light guide is often placed between the detector and PSPMT array to spread scintillation light so that these gaps can be bridged. In this investigation we studied the effect of light guides of various thickness on system performance. A 10×10 element array of LYSO detector elements was coupled to the center of a 2×2 array of PSPMTs through varying thicknesses (1 to 4 mm) of UV glass. The spot size of the imaged elements and distortions in the regular square pattern of the imaged scintillator arrays were evaluated. Energy resolution was measured by placing single elements of LYSO at several locations of the PSPMT array. Spatial distortions in the images of the array were reduced by using thicker light guides (3–4 mm). Use of thicker light guides, however, resulted in reduced pixel resolution and slight degradation of energy resolution. Therefore, some loss of pixel and energy resolution will accompany the use of thick light guides (minimum of 3 mm) required for optimum identification of detector elements.     

CdTe compact gamma camera for coded aperture imaging in radioguided surgery

The aim of this work was to assess the performance of a prototype compact gamma camera (MediPROBE) based on a CdTe semiconductor hybrid pixel detector, for coded aperture imaging. This probe can be adopted for various tasks in nuclear medicine such as preoperative sentinel lymph node localization, breast imaging with ^99mTc radiotracers and thyroid imaging, and in general in radioguided surgery tasks. The hybrid detector is an assembly of a 1-mm thick CdTe semiconductor detector bump-bonded to a photon-counting CMOS readout circuit of the Medipix2 series or energy-sensitive Timepix detector. MediPROBE was equipped with a set of two coded aperture masks with 0.07-mm or 0.08-mm diameter holes. We performed laboratory measurements of field of view, system spatial resolution, and signal-difference-to-noise ratio, by using gamma-emitting radioactive sources (¹⁰⁹Cd, ¹²⁵I, ²⁴¹Am, ^99mTc). The system spatial resolution in the lateral direction was 0.56 mm FWHM (coded aperture mask with holes of 0.08 mm and a 60 keV source) at a source-collimator distance of 50 mm and a field of view of 40 mm by side. Correspondingly, the longitudinal resolution in 3D source localization tasks was about 3 mm. MediPROBE showed a significant improvement in terms of spatial resolution when equipped with the high-resolution coded apertures, with respect to the performance previously reported with 1–2 mm pinhole apertures as well as with respect to adopting a 0.35 mm pinhole aperture.     

Exploring TOF capabilities of PET detector blocks based on large monolithic crystals and analog SiPMs

Monolithic scintillators are more frequently used in PET instrumentation due to their advantages in terms of accurate position estimation of the impinging gamma rays both planar and depth of interaction, their increased efficiency, and expected timing capabilities. Such timing performance has been studied when those blocks are coupled to digital photosensors showing an excellent timing resolution.In this work we study the timing behaviour of detectors composed by monolithic crystals and analog SiPMs read out by an ASIC. The scintillation light spreads across the crystal towards the photosensors, resulting in a high number of SiPMs and ASIC channels fired. This has been studied in relation with the Coincidence Timing Resolution (CTR). We have used LYSO monolithic blocks with dimensions of 50 × 50 × 15 mm³ coupled to SiPM arrays (8 × 8 elements with 6 × 6 mm² area) which compose detectors suitable for clinical applications.While a CTR as good as 186 ps FWHM was achieved for a pair of 3 × 3 × 5 mm³ LYSO crystals, when using the monolithic block and the SiPM arrays, a raw CTR over 1 ns was observed. An optimal timestamp assignment was studied as well as compensation methods for the time-skew and time-walk errors. This work describes all steps followed to improve the CTR. Eventually, an average detector time resolution of 497 ps FWHM was measured for the whole thick monolithic block. This improves to 380 ps FWHM for a central volume of interest near the photosensors. The timing dependency with the photon depth of interaction and planar position are also included.     

Evaluation of a dual-panel PET camera design to breast cancer imaging

We are developing a novel, portable dual-panel positron emission tomography (PET) camera dedicated to breast cancer imaging. With a sensitive area of ∼ 150 cm², this camera is based on arrays of lutetium oxyorthosilicate (LSO) crystals (1×1×3 mm³) coupled to 11×11-mm² position-sensitive avalanche photodiodes (PSAPD). GATE open source software was used to perform Monte Carlo simulations to optimize the parameters for the camera design. The noise equivalent counting (NEC) rate, together with the true, scatter, and random counting rates were simulated at different time and energy windows. Focal plane tomography (FPT) was used for visualizing the tumors at different depths between the two detector panels. Attenuation and uniformity corrections were applied to images.     

Phantom evaluations of a dedicated dual-head scintimammography system

Results of aboratory evaluations are presented of the dual-head scintimammography system using two opposed and co-registered compact gamma heads. The system is intended for clinical studies imaging suspicious lesions in a compressed breast. The studies were performed using 5 cm and 6 cm compressed breast phantoms with lesion sizes from 6 to 10 mm and lesion to breast tissue activity ratios from 6 to 10. Two imagers with a field-of-view (FOV) of 15 cm×20 cm were placed on the opposite sides of the breast phartoms. In some studies anthropomorphic torso phantom was used to simulate realistic scatter gamma radiation field. Two types of parallel-hole lead collimators were employed. Combining the co-registered images from both detector heads resulted in an over two-fold increase in lesioin contrast in the central plane of the phantom and substantially increased detection sensitivity over the whole breast volume, especially of asymmetrically placed small lesions. The results confirm the important advantage of a co-registoed two-head scintimammography system over a single head system in lesion detection and localization.     

Commissioning and performance testing of the first prototype of AlignRT InBore™ a Halcyon™ and Ethos™-dedicated surface guided radiation therapy platform

PurposeTo commission and assess the performance of AlignRT InBore™, a Halcyon™ and Ethos™-dedicated Surface Guided Radiation Therapy (SGRT) platform which combines ceiling-mounted cameras for patient setup and bore-mounted cameras for in-bore tracking.MethodsTo check the potential impact of InBore™ cameras on dose delivery, 16 SRS, H&N, breast and pelvis patients’ quality assurance (QA) treatment plans were measured with/without AlignRT InBore™ and using ArcCHECK® and SRS MapCHECK®. Impact on image quality was determined using Catphan® 540 phantom and considering all available MV and CBCT protocols (head, breast, chest and pelvis). The stability, accuracy and overall performance of AlignRT InBore™ was assessed using an MV Cube and anthropomorphic phantoms.ResultsComparison of 2D dose distributions with/without AlignRT InBore™ showed no impact on treatment delivery for all 16 QA checks (p-value > 0.25). 2D and CBCT images showed no artefacts or change in the contrast-to-noise ratio, resolution and noise values measured with Catphan® 540. Anti-collision sensors were unaffected by the bore-mounted cameras. Additionally, AlignRT InBore™ cameras allowed for motion detection with sub-0.5 mm accuracy and sub-0.4 mm stability with surface coverage of >50 × 60 × 35 cc. Accurate transition (sub-0.3 mm) from virtual to treatment isocentres was achieved. Finally, Halcyon™ rotations during CBCT and beam delivery resulted in limited camera vibrations with translation uncertainty <0.5 mm in left-right and anterior-posterior directions and <0.1 mm in head-feet direction.ConclusionAlignRT InBore™ provides SGRT setup and intrafraction monitoring capabilities with a performance comparable to standard SGRT solutions while having no adverse effect on Halcyon™.     

Beam Steering Plasma Reflectarray/Transmitarray Antennas

The aim of this paper is to design and analyze plasma reflectarray/transmitarray antennas which include investigation of performance parameters for these antennas in free space. The unit cell element for both arrays consists of a cubic glass box with fixed dimensions filled by argon gas. The plasma frequency of the argon gas is varied by changing the applied voltage at both ends of the glass box. This allows steering the reflected/transmitted wave to a certain direction. Full-wave simulations using the finite element method (FEM) and finite integral technique (FIT) are used to optimize and analyze different plasma reflectarray and plasma transmitarray antennas. The plasma reflectarray antenna is composed of 13?×?13 elements and covered an area of 208?×?208 mm². A circular horn is used to feed the antenna at a distance of 20.8 cm (focal-to-diameter ratio (F/D)?=?1). The reflectarray is designed at f?=?12 GHz. The radiation patterns of the plasma reflectarray for scanning angles of 10° to 70° angles are illustrated. For larger scanning angles, significant sidelobe levels are produced. The maximum value of beam scanning gain patterns is reduced. The half-power beamwidth (HPBW) is increased. The plasma transmitarray is composed of 9?×?9 cell elements and covered an area of 72?×?72 mm². The feed is a linearly polarized circular horn. The F/D ratio is set to 1. The transmitarray is operating at f?=?15 GHz. The radiation patterns of the plasma transmitarray for scanning angles of ?40° to +40° are demonstrated. Significant sidelobe levels are produced at large scanning angles.     

High resolution scintimammography helps in differentiating benign from malignant findings in scintigraphic hot spots

Several efforts have been focusing on the development of detectors devoted to high solution ^99mTc sestamibi scintimammography to improve sensitivity for non palpable lesions. To this aim new high resolution scintillation gamma camera was developed under the “Integiated Mammographic Imaging” project. The gamma camera, made by CAEN and Pol.Hi.Tech, has an overall dimension of 112×120×75mm3. It consists of an array of 1 in. PSPMTs Hamamatsu H8520-C12 closely packed, a NaI(T1) scintillation array (1.8×1.8×6mm³ pixel) and a general purpose collimator. By this gamma camera a clinical experience on a few patients with breast cancer suspicion was performed. In this paper we show how high resolution approach allows to better categorize the lesions on the basis of the morphology of the spatial distribution of the radiotracer in the breast tissue. By comparing conventional and high resolution images of a young patient (29 y.o.) with breast cancer suspicion, it appears clear how the Anger, camera images showed a defined hot spot, highly suggestive of malignant lesion; on the contrary, the high resolution scan shown a large and inhomogeneous uptake area with the absence of clear and focal character of the uptake, to be considered as a probably non malignant lesions. This resuh was confirmed by byoptical findings that diagnosed the echographic findings as a benign inflammatory lesion.     

Real-time protein biosensor arrays based on surface plasmon resonance differential phase imaging

This paper reports the application of differential phase surface plasmon resonance (SPR) imaging in two-dimensional (2D) protein biosensor arrays. Our phase imaging approach offers a distinct advantage over the conventional angular SPR technique in terms of utilization efficiency of optical sensor elements in the imaging device. In the angular approach, each biosensor site in the biosensor array requires a linear array of optical detector elements to locate the SPR angular dip. The maximum biosensor density that a two-dimensional imaging device can offer is a one-dimensional SPR biosensor array. On the other hand, the phase-sensitive SPR approach captures data in the time domain instead of the spatial domain. It is possible that each pixel in the captured interferogram represents one sensor site, thus offering high-density two-dimensional biosensor arrays. In addition, our differential phase approach improves detection resolution through removing common-mode disturbances. Experimental results demonstrate a system resolution of 8.8 x 10(-7)RIU (refractive index unit). Real-time monitoring of bovine serum albumin (BSA)/anti-BSA binding interactions at various concentration levels was achieved using a biosensor array. The detection limit was 0.77 microg/ml. The reported two-dimensional SPR biosensor array offers a real-time and non-labeling detection tool for high-throughput protein array analysis. It may find promising applications in protein therapeutics, drug screening and clinical diagnostics.     

Macrophotography of Thick Sections and Gels with A Regular Photographic Enlarger

At present, we have a program at Yerkes Regional Primate Research Center for the gross mapping of histochemical localization of various enzymes in the squirrel monkey brain and spinal cord, to characterize various regions. For these studies, sections about 50 μ thick must be used. The preparations measure from 4 × 5 mm in transverse sections of spinal cord to 20 × 40 mm in sagittal sections of cerebral hemispheres. Because of their dimensions, an ordinary camera attached to a microscope or even a plate camera could not be used satisfactorily for photographing them. However, projection with a darkroom enlarger has given very satisfactory pictures.     

Variation of heartwood and sapwood in 18-year-old Eucalyptus globulus trees grown with different spacings

Heartwood and sapwood development was studied in 18-year-old Eucalyptus globulus trees from pulpwood plantations with different spacings (3 × 2, 3 × 3, 4 × 3, 4 × 4 and 4 × 5 m), on cross-sectional discs taken at breast height. The trees possessed a large proportion of heartwood, on average 60% of the wood cross-sectional surface. Spacing was a statistically significant source of variation of heartwood area, which ranged between 99 and 206 cm² for the closer (3 × 2) and wider (4 × 5) spacings, respectively. There was a positive and high statistical significant correlation between heartwood diameter and tree diameter (heartwood diameter = −0.272 + 0.616 dbh; r ² = 0.77; P < 0.001), and larger trees contained more heartwood regardless of spacing. Heartwood proportion in cross-section remained practically constant between spacings but increased with tree diameter class: 55.1, 62.2, 65.0 and 69.5% for diameter at breast height classes <15, 15–20, 20–25 and >25 cm, respectively. The sapwood width did not depend on tree diameter growth and remained practically constant at an average of 18 mm (range 15–21 mm), but sapwood area showed a good linear regression with tree diameter. Therefore, tree growth enhancement factors, such as wide spacings, will induce formation of larger heartwoods that can negatively impact raw-material quality for pulping. The increase in heartwood in relation with tree dimensions should therefore be taken into account when designing forest management guidelines.     

Preliminary Crystallographic Analysis of a Proteolytically Modified Form of E. coli Single Stranded DNA Binding Protein

Abstract

A proteolytically modified form of the Escherichia coli single-stranded DNA-Binding protein (SSB) has been crystallized from 15% saturated sodium citrate. Crystals as large as 1.0mm × 0.3mm × 0.2mm were obtained and these diffract beyond 3Å resolution. X-ray photographic analysis demonstrated a rhombohedral unit cell of space group R3 with an equivalent triple centered hexagonal unit cell having dimensions of a = b = 62.9 A and c = 264.3A. These crystals were judged to be adequate for a three dimensional structure determination.     

Thaumatin-like proteins are differentially expressed and localized in phloem tissues of hybrid poplar

Background  

Two thaumatin-like proteins (TLPs) were previously identified in phloem exudate of hybrid poplar (Populus trichocarpa × P. deltoides) using proteomics methods, and their sieve element localization confirmed by immunofluorescence. In the current study, we analyzed different tissues to further understand TLP expression and localization in poplar, and used immunogold labelling to determine intracellular localization.     

Photobioreactor with photosynthetic bacteria immobilized on porous glass for hydrogen photoproduction

A photobioreactor was constructed with porous glass as an immobilization matrix. The reactor was a rectangular glass chamber (inner dimensions: 125 × 50 × 2.5 mm) containing a porous glass sheet (125 × 50 × 0.5 mm) on which Rhodobacter sphaeroides RV was immobilized (11.2 mg dry wt./ml porous glass). The maximum rate of hydrogen evolution was 1.3 ml/h/ml porous glass. The conversion efficiency of succinate into hydrogen reached 75%. Stable and efficient hydrogen evolution continued for up to 40 d.     

Evaluation of scanning resolution,detector choice and detector orientation to be used for accurate and time-efficient commissioning of a 6MV clinical linear accelerator

The present study is aimed at exploring different scanning parameters, detectors and their orientations for time-efficient and accurate commissioning of a 6 MV clinical linear accelerator (LINAC). Beam profiles and percentage depth dose (PDD) curves were measured with a PTW dosimetry diode, a PTW Semiflex and a PinPoint ion chamber in different orientations. To acquire beam data, equidistant (step size of 0.5 mm, 1 mm, 2 mm and 3 mm) and fanline (step size of 2–0.5 mm, 2–1 mm, 3–0.5 mm and 3-1 mm) scanning modes were employed and data measurement time was recorded. Scan time per measurement point was also varied (0.2 s, 0.5 s and 1.0 s) to investigate its effect on the accuracy and acquisition time of beam data. Accuracy of the measured data was analyzed on the basis of the variation between measured data and data modeled by a treatment planning system. Beam profiles (particularly in penumbra region) were found to be sensitive to variation in scanning resolution and showed an improved accuracy with decrease in step size, while PDD curves were affected negligibly. The accuracy of beam data obtained with the PTW dosimetry diode and the PinPoint ion chamber was higher than those obtained with the PTW Semiflex ion chamber for small fields (2?×?2 cm² and 3?×?3 cm²). However, the response of the PTW diode and the PinPoint ion chamber was significantly indifferent in these fields. Furthermore, axial orientation of the PTW Semiflex ion chamber improved accuracy of profiles and PDDs as compared to radial orientation, while such a difference was not significant for the PinPoint ion chamber. It is concluded that a scan time of 0.2 s/point with a fanline scanning resolution of 2–1 mm for beam profiles and 3 mm for PDDs are most favorable in terms of accuracy and time efficiency. For small fields (2?×?2 cm² and 3?×?3 cm²), a PinPoint ion chamber in radial orientation or a dosimetry diode in axial orientation are recommended for both beam profiles and PDDs. If a PinPoint ion chamber and a PTW dosimetry diode are not available, a Semiflex ion chamber in axial orientation may be used for small fields.

     

Packed-column supercritical fluid chromatography of artemisinin (qinghaosu) with electron-capture detection

In this preliminary report, a supercritical fluid chromatographic method is described for the determination of artemisinin in whole blood. The chromatography is carried out on a 20 cm × 1 mm I.D. Deltabond cyano supercritical fluid chromatographic column with detection of the artemisinin via an electron-capture detector. The sample work-up uses a liquid-liquid extraction with hexane, giving a recovery of 82%. The current limit of detection using 1 ml of blood is 20 ng/ml. We speculate that the endoperoxide moiety accounts for the response to the electron-capture detector and thus provides a new approach by which this class of compounds may be analyzed.     

CZT detectors: How important is energy resolution for nuclear breast imaging?

Semiconductor detectors, such as Cadmium Zinc Telluride (CZT), offer improved energy resolution (ER) and potentially improved tumor contrast in breast imaging. We evaluated the effect of changes in ER on tumor contrast. Studies were performed on a prototype CZT detector, a commercial CZT-based system, a multicrystal CsI system and a conventional NaI system. The same low energy high resolution collimator was used on each system and the same total counts (250 kcts) were acquired in each image. CZ-Tmodules in a detector can exhibit different ERs. We imaged a breast phantom containing 4 tumors (diameters 4.9, 7.2, 7.2, and 9.8 mm) over individual CZT modules with intrinsic ers of 5.8–17.5%. Tumor to background ratio was 6.2:1 and tumors were placed 1 and 4 cm deep in the 6-cm thick breast phantom. A standard ±10% energy window and narrower energy windows (−5%/+10% and −7%/ +10%) were used. Tumor contrast was determined by maximum tumor intensity divided by mean background intensity. Tumor contrast was not significantly affected by differences in ER between CZT modules. Tumor contrast improved by 2–10% with a narrow energy window. At the same ER, the CZT systems yielded slightly better contrast than the CsI system. All pixilated systems performed better than the NaI system. Scatter in the breast was found to be low and accounts for only ∼11% of counts in a ±10% energy window for a 6 cm- thick breast. No strong relationship was observed between ER and tumor detectability, which may be due to low scatter in the breast. Detector element size in pixilated systems appears to be more important than ER in determining tumor contrast.     

Quantitative Analysis of Flavonoids in Chamomile Flowers (<Emphasis Type="Italic">Matricaria chamomilla</Emphasis> L.) by Microcolumn HPLC-UV

A reverse-phase microcolumn HPLC method with UV detection (330 nm) was developed for quantitative analysis of flavonoids of Matricaria chamomilla flowers using a ProntoSIL-120-5-C18 AQ column (60 mm × 1 mm × 5 μm), gradient elution system 0.2 M LiClO₄/0.006 M HClO₄–acetonitrile and cosmosiin as a reference compound. Optimal conditions for the hydrolytic process of flavonoids (KOH concentration 0.25%, extraction time 30 min) and the parameters of flavonoids extraction (particle size 0.25 mm, extraction temperature 60°C, a single extraction step lasting 30 min at a ratio 1: 100) were selected. Validation analysis showed that the proposed method is characterized by satisfactory metrological parameters. The limit of detection (LOD) and limit of quantification (LOQ) of cosmosiin were 84 and 255 ng/mL, respectively. The accuracy for cosmosiin content levels 80–120% was less than 101.93–103.00%. The method was used for the analysis of introduced and commercial samples of M. chamomilla flowers.     

Estimation of extremely small field radiation dose for brain stereotactic radiotherapy using the Vero4DRT system

The purpose of this study was a dosimetric validation of the Vero4DRT for brain stereotactic radiotherapy (SRT) with extremely small fields calculated by the treatment planning system (TPS) iPlan (Ver.4.5.1; algorithm XVMC). Measured and calculated data (e.g. percentage depth dose [PDD], dose profile, and point dose) were compared for small square fields of 30 × 30, 20 × 20, 10 × 10 and 5 × 5 mm² using ionization chambers of 0.01 or 0.04 cm³ and a diamond detector. Dose verifications were performed using an ionization chamber and radiochromic film (EBT3; the equivalent field sizes used were 8.2, 8.7, 8.9, 9.5, and 12.9 mm²) for five brain SRT cases irradiated with dynamic conformal arcs.The PDDs and dose profiles for the measured and calculated data were in good agreement for fields larger than or equal to 10 × 10 mm² when an appropriate detector was chosen. The dose differences for point doses in fields of 30 × 30, 20 × 20, 10 × 10 and 5 × 5 mm² were +0.48%, +0.56%, −0.52%, and +11.2% respectively. In the dose verifications for the brain SRT plans, the mean dose difference between the calculated and measured doses were −0.35% (range, −0.94% to +0.47%), with the average pass rates for the gamma index under the 3%/2 mm criterion being 96.71%, 93.37%, and 97.58% for coronal, sagittal, and axial planes respectively.The Vero4DRT system provides accurate delivery of radiation dose for small fields larger than or equal to 10 × 10 mm².     

A very simple high‐performance liquid chromatographic method with fluorescence detection for the determination of gemifloxacin in human breast milk

A high‐performance liquid chromatographic method with fluorescence detection was developed and validated for the determination of gemifloxacin in human breast milk. The proposed method allows the determination of gemifloxacin in breast milk samples without complex sample preparation. The samples were mixed with a mobile phase and filtered with a 0.45 µm polytetrafluoroethylene filter before analysis. Chromatographic separation was carried out on a C18 column (150 × 4.6 mm, 5 µm I.D.) using methanol:50 mM ortho‐phosphoric acid solution (40:60) as the mobile phase with a 1.0 mL/min flow rate. Quantitation was performed using fluorescence detection with an excitation wavelength at 272 nm and an emission wavelength at 395 nm. The linear range was found to be 0.1–2.5 µg/mL. The method was applied successfully for the determination of gemifloxacin in breast milk obtained from a breastfeeding mother after oral administration of a single tablet that included 320 mg gemifloxacin per gemifloxacin tablet. Copyright © 2015 John Wiley & Sons, Ltd.