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Germanium

Germanium is a metalloid element with the atomic number 32.
It is used in a variety of electronic and optical applications, such as transistors, fiber-optic cables, and infrared detectors.
Germanium has unique semiconductir properties that make it an important material in the field of nanotechnology and microelectronics.
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Most cited protocols related to «Germanium»

In total, nine blood samples ≤ 28 ml were obtained from three healthy test persons (age: 31, 57, 60 years) at different days using Li-Heparin blood collecting tubes (Sarstedt, S-Monovette). Each blood sample was split into 3.5 ml aliquots. One non-exposed sample was used to determine the individual background focus rate. Blood aliquots (3.5 ml) were added to the 1 ml radioactive solution, followed by incubation for 1 h at 37°C on a roller-mixer (35 rpm, Marienfeld GmbH, Germany) to uniformly blend the samples during the exposure time. A 100 μl aliquot of the blood solution was removed to determine the exact activity concentration in the respective blood sample using a germanium detector. After incubation, 3.5 ml of the radionuclide-containing blood solution were filled into a CPT Vacutainer tube (BD, Germany). The white blood cells were separated by 20 minute density centrifugation at 1500 g according to manufacturer’s instructions (BD). Then, the leucocytes were recovered above the interphase and washed twice in phosphate buffered saline (PBS). Ice-cold 99.9% ethanol was added to the cell suspension to result in a solution of 70% ethanol [23 (link)].
The fixed white blood cells were stored at least for 24 hours at -20°C and shipped to the Bundeswehr Institute of Radiobiology in Munich, Germany where they were subjected to two-color immunofluorescent staining for γ-H2AX and 53BP1 [12 (link)]. Radiation-induced co-localizing γ-H2AX and 53BP1 foci were counted manually in the nuclei of 100 cells using a red/green double band pass filter (Chroma) of a Zeiss Axioobserver 2 epifluorescence microscope by an experienced observer (H.S.). Foci values were expressed as average foci/cell values and the standard deviations were calculated from the experiments assuming a Poisson distribution. The number of radiation-induced damage foci per cell was then obtained by subtracting the background focus rate for each sample.
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Publication 2015
BLOOD Cell Nucleus Cells Centrifugation Cold Temperature Electromagnetic Radiation Ethanol Fluorescent Antibody Technique Germanium Heparin Interphase Leukocytes Microscopy Phosphates Radioactivity Radioisotopes Saline Solution TP53BP1 protein, human

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Publication 2009
Cyclotrons EBCO Electrochemical Techniques Gamma Rays Genie Germanium Protons Radioactivity Radioisotopes Radiotherapy Spectrum Analysis Yttrium-86 yttrium chloride
The main components in this measurement were the detector, radioactive point source, lead collimator and the glass samples or an absorber needed for measuring. The schematic diagram of these components is illustrated in Figure 1. The High Pure Germanium (HPGe) Detector of model: GC1520 (Manufacturer of radiation detection and analysis instrumentation, Meriden, USA) was used. The relative efficiency of the detector was 15% and the resolution (FWHM) at 1.33 MeV was 2 keV. Three point sources were used in the measurement to cover a wide range of energies. The Am-241 point source is a very important source that emits a line in low energy (59.54 keV), and the initial activity of this source was 259 kBq. Cs-137 point source emits two lines (32, 661.6 keV) but the line due to X-ray emission (32 keV) was totally absorbed and therefore the most probable line and higher emission probability is (661.6 keV), the initial activity of this source is 385 kBq. Eu-152 is a multi-line source and covered more energies from low to high energy. The lines were chosen according to the higher emission probability (121.78, 244.69, 344.28, 964.13 and 1408.1 keV), the initial activity of this source is 290 kBq. The reference date of all three point sources was 1 June 2009 [27 (link),28 (link)].
The narrow beam method was used in measurements by the lead collimator. The detector first was calibrated and the background was measured using Genei 2000 software (V3.3, Mirion Technologies (Canberra), Inc., Canberra, Australia) [29 (link)]. The measurement occurred within and outside the glass sample with different sources to obtain the net peak area or the count rate of the line which represent the intensity of this line. So, the intensity of the line outside the absorber (I0) and within the absorber (I) can be calculated. By knowing the thickness of the glass absorber (x), the linear attenuation coefficient (LAC) easily estimated via the relation [30 (link)].
LAC=ln(II0)x
The MAC can be calculated experimentally by dividing the LAC on the density of an absorber (ρ). The MAC examined theoretically by the XCOM program for all present glass samples using the chemical composition of each sample. Other related parameters were investigated such as HVL, TVL, and MFP, as well as RPE. The HVL and TVL are the thickness layers of an absorber needed to reduce the count rate of a line a half and a tenth of its original value, respectively, and are given by the following equations [31 (link)].
HVL=Ln2LAC
TVL=Ln10 LAC
The mean-free path can be estimated by Equation (4) [32 (link)].
MFP=1LAC
The shielding efficiency of an absorber sample can be investigated using a parameter called the radiation protection efficiency (RPE) and given by the next equation [33 (link)].
RPE=(1II0)×100
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Publication 2021
Cesium-137 chemical composition Enzyme Multiplied Immunoassay Technique Germanium Radiation Radiation Protection Radioactivity Radiography
The KXRF bone Pb measurement system was used to measure tibia bone Pb as a metric of each individual’s cumulative lead exposure. The setup was the same as used in previous studies (Nie, 2005 ; Nie et al., 2004 ; Specht et al., 2014 ). The system uses four 16 mm diameter high-purified germanium detectors with 10 mm thickness, four feedback resistance pre-amplifiers, four digital signal processing systems and a computer. A 135 mCi Cd-109 source with 0.8 mm copper filter is used to irradiate tibia bone to produce the Pb K X-rays. Before measurement, the subjects’ legs were cleaned using alcohol and EDTA cotton swabs to remove any Pb contamination. For the KXRF measurement, the subject would sit on a wooden chair. The subject’s leg was immobilized by using two Velcro straps to attach their leg to the leg of the chair at the ankle and just below the knee. The measurement site was mid-tibia with the source at a distance to maintain ~30% dead time during the measurement. The measurement was taken for 30 min while the subject watched a movie. Finally, the spectra were analyzed using an in-house peak-fitting program, which gave results and error for each of the four detectors (Bevington & Robinson, 2003 ; Nie, 2005 ; Somervaille et al., 1989 (link)). This error and result was combined using inverse variance weighting (Todd, 2000 (link)). XRF provides a point estimate of Pb concentration, which can be negative if an individual’s bone Pb is close to zero. It is important to include these negative values, as with their associated uncertainties they are still a point estimate of that individual’s bone Pb.
The whole body effective dose delivered to the subject from this system was estimated to be less than 5 µSv for this population (Nie et al., 2007 ).
Publication 2016
Ankle Bones Copper Edetic Acid Ethanol Germanium Gossypium Human Body Knee Radiotherapy Tibia Tibial Fractures X-Rays, Diagnostic
Participants and procedures. Participants in the current study, the Folate and Oxidative Stress (FOX) Study, were recruited between February and July of 2008 in Araihazar, Bangladesh. Potential participants were identified on the basis of well water As (wAs) concentrations obtained from a well survey in the year 2000 (van Geen et al. 2002 (link)) in order to ensure a wide range of As exposures for the examination of dose-dependent relationships. A new water sample was collected at the time of enrollment for analysis of wAs concentration. Individuals were eligible to participate in FOX if they a) were between 30 and 65 years of age; b) were not pregnant; c) were not taking nutritional supplements; d) did not have known diabetes, cardiovascular or renal disease, chronic obstructive pulmonary disease, or cancer; and e) had been drinking water from their current well for at least 3 months. Trained recruiters identified eligible participants, explained the nature of the study, obtained informed consent, and scheduled a field clinic visit. Because GSH is unstable and therefore requires that blood samples be processed immediately, all visits were conducted in the laboratory at our field clinic in Araihazar. During the field clinic visit, a trained interviewer administered a detailed questionnaire to each participant, and a physician collected a venous blood sample. Urine samples were collected in 50-mL acid-washed polypropylene tubes and frozen at –20°C.
The primary aim of this study was to examine the dose–response relationship between As exposure and measures of oxidative stress. We aimed to recruit 75 participants each from five wAs concentration categories: < 10, 10–100, 101–200, 201–300, and > 300 µg/L. However, the final sample included more particpants with lower exposures because many households switched to lower-As wells after wells in the region were surveyed for As in 1999–2000 (Chen et al. 2007 (link)). Therefore, the final distribution among well wAs exposure categories was < 10 µg/L (n = 76), 10–100 µg/L (n = 104), 101–200 µg/L (n = 86), 201–300 µg/L (n = 67), and > 300 µg/L (n = 45).
Oral informed consent was obtained by our Bangladeshi field staff physicians, who read an approved assent form to the study participants. This study was approved by the Bangladesh Medical Research Council and the institutional review board of Columbia University Medical Center.
Sample collection and handling. After the initial processing of blood samples in the field clinic, the blood and plasma aliquots were immediately frozen at –80°C. Samples on dry ice were transported in batches to Dhaka, Bangladesh, by car and again stored at –80°C (blood and plasma) or –20°C (urine). Samples were then packed on dry ice in coolers and transported by air to Columbia University.
wAs. Field sample collection and laboratory analysis procedures have been previously described in detail (Cheng et al. 2004 (link); van Geen et al. 2005 (link)). Water samples were collected in 20-mL polyethylene scintillation vials. The samples were acidified to 1% with high-purity Optima HCl (Fisher Scientific, Pittsburg, PA, USA) at least 48 hr before analysis (van Geen et al. 2007 ). Water samples were analyzed by high-resolution inductively coupled plasma mass spectrometry (ICP-MS) after 1:10 dilution and addition of a germanium spike to correct fluctuations in instrument sensitivity. The detection limit of the method is typically < 0.2 μg/L (Cheng et al. 2004 (link)). A standard with an As concentration of 51 µg/L was run multiple times in each batch. The intraassay and interassay coefficients of variation (CVs) for this standard were 6.01% and 3.76%, respectively.
Total urinary As. All urine samples were analyzed for total urinary As (uAs) in the Columbia University Trace Metals Core Laboratory by graphite furnace atomic absorption spectrometry (Nixon et al. 1991 (link)) using the AAnalyst 600 graphite furnace system (PerkinElmer, Shelton, CT, USA). A method based on the Jaffe reaction was used to measure urinary creatinine concentrations (Slot 1965 (link)). Method and instrument precision was checked by running four different urine samples with known concentrations (to cover the whole linearity range of the standard curve) every day immediately after the instrument calibration with aqueous standards. A urine sample with an As concentration in the middle of the linearity range was run after every 10 study samples. The intraassay and interassay CVs based on this quality control sample were 3.9% and 5.6%, respectively. For duplicate study samples, the intraassay and interassay CVs were 3.8% and 5.1%, respectively.
Total blood As. We used a Perkin-Elmer Elan DRC II ICP-MS equipped with an AS 93+ autosampler to analyze whole blood samples for total blood As (bAs) concentration, as described previously (Hall et al. 2006 (link)). The intraassay and interassay CVs were 3.2% and 5.7%, respectively, for quality control samples. For study samples, the intraassay and interassay CVs were 2.1% and 4.9%, respectively.
Blood GSH and GSSG and plasma Cys and CySS. Whole blood GSH and GSSG and plasma Cys and CySS were assayed essentially as described by Jones et al. (1998) (link). Blood was collected with a butterfly needle and syringe and then immediately transferred into Eppendorf tubes. For whole blood measurements, the Eppendorf tubes contained 5% perchloric acid, 0.1 M boric acid, and γ-glutamyl glutamate as an internal standard. For plasma measurements, the tubes contained 0.53 g l-serine, 25 mg heparin, 50 mg bathophenanthrolene, 300 mg iodoacetic acid, and 10 mL borate buffer stock (12.4 g boric acid, 19 g sodium tetraborate decahydrate, and 500 mL distilled water). The samples for plasma measurements were centrifuged for 1 min, and 200 µL of supernatant was transferred into Eppendorf tubes containing an equal volume of 10% perchloric acid and 0.2 M boric acid. For derivatization, plasma samples were centrifuged at 13,000 rpm for 2 min, 300 µL of supernatant was transferred to a fresh tube, and the pH was adjusted to 9.0. After incubating for 20 min at room temperature, dansyl chloride was added, and samples were incubated at room temperature in the dark for 24 hr. The derivatized samples were then stored at –80°C until delivered to Columbia University for analysis. Free dansyl chloride was extracted from thawed samples with 500 µL chloroform, and then 20 µL of the sample was injected onto the HPLC. Separation was achieved using a Supelcosil LC-NH2 column (catalog no. 58338; Sigma Chemical Co., St. Louis, MO, USA). Initial solvent conditions were 60% A (80% methanol, 20% water), 40% B (acetate-buffered methanol, pH 4.6) run at 1 mL/min for 10 min. A linear gradient to 20% A, 80% B was run during the 10- to 50-min period. From 50 to 52 min, the conditions were returned to 60% A, 40% B. Metabolites were detected using a Waters 474 scanning fluorescence detector (Waters Corp., Milford, MA, USA), with 335 nm excitation and 515 nm emission. Within-assay CVs were all between 0.05 and 0.10, and interassay CVs were between 0.11 and 0.18.
Plasma folate. Plasma folate was analyzed by radio protein-binding assay (SimulTRAC-S; MP Biomedicals, Orangeburg, NY, USA). To determine folate concentrations, we used folic acid as pteroylglutamic acid for calibration, and its 125I-labeled analog as the tracer. The intraassay and interassay CVs were 0.06 and 0.14, respectively.
Calculation of the reduction potential. The reduction potential (Eh) of the thiol/disulfide GSH/GSSG and Cys/CySS redox pairs (blood GSH Eh and plasma Cys Eh, respectively) were calculated using the Nernst equation:
Eh = Eo + RT/nF ln(acceptor/(donor)2,
where Eo is the standard potential for the redox couple, R is the gas constant, T is the absolute temperature, n = 2 for the number of electrons transferred, and F is Faraday’s constant (Jones et al. 2002 (link)). For GSH and GSSG, the equation simplifies to
Eh (mV) = −264 + 30 log[(GSSG)/(GSH2)],
where (GSH) and (GSSG) are molar concentrations, and the Eo value assumes a physiologic pH of 7.4. A more positive Eh value indicates a more oxidized redox state.
Statistical methods. We calculated descriptive statistics for characteristics of the study sample, As exposure variables (wAs, uAs, and bAs), and outcome variables (blood GSH and GSSG, plasma Cys and CySS), both for the total sample and by sex. Bivariate associations were examined using scatter plots and Spearman’s correlation coefficients. To examine the bivariate associations between dichotomous covariates and As exposure variables or continuous outcome variables we used t-tests or the nonparametric Wilcoxon rank sum test.
We used linear regression models to further examine the associations between As exposure variables, as continuous variables, and the outcome variables, with and without adjustment for potential confounders. Age and sex were included in all covariate-adjusted regression models. Other covariates considered for inclusion in the regression models were variables reported to be associated with the exposures or outcomes based on previous publications and/or variables associated with the exposure and outcome variables in the present study population. These variables included television ownership (as a surrogate for socioeconomic status), cigarette smoking, body mass index (BMI), urinary creatinine, and plasma folate. We adjusted for GSH laboratory batch (as a categorical variable) in order to reduce extraneous variation in the outcome variables. We also calculated the change in R2 between models for each outcome that included covariates only and corresponding models that included both the covariates and As exposure.
To facilitate comparisons among the different measures of exposure (wAs, uAs, and bAs), we report the estimated change in the mean value of blood GSH, blood GSH Eh, plasma CySS, and plasma Cys Eh associated with an interquartile range (IQR) increase in each exposure. For outcome variables that were natural log-transformed (blood GSSG and plasma Cys) we report the ratio of estimated geometric means for an IQR change in As exposure.
To examine possible nonlinear relationships, we also created quintiles of As exposure variables and computed covariate-adjusted mean values of the outcome variables for categories of As exposure; plots of quintile-specific adjusted mean values were examined to determine if the association was approximately linear.
We ran separate linear regression models to examine the covariate-adjusted associations between As exposure and the outcome variables stratified by sex or by folate status. We then used a Wald test to detect differences in the covariate-adjusted associations between As exposure and outcome variables by sex or by folate status. All analyses were performed using SAS (version 9.2; SAS Institute Inc., Cary, NC, USA); all statistical tests were two-sided with a significance level of 0.05.
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Publication 2013
Acetate Acids Biological Assay BLOOD Borates borax boric acid Butterflies Cardiovascular System Chloroform Chronic Obstructive Airway Disease Clinic Visits Creatinine cysteinylcysteine dansyl chloride Diabetes Mellitus Dietary Supplements Disulfides Dry Ice Electrons Ethics Committees, Research Fluorescence Folate Folic Acid Freezing Germanium Glutamate Glutathione Disulfide Graphite Heparin High-Performance Liquid Chromatographies Households Hypersensitivity Index, Body Mass Interviewers Iodoacetic Acid Kidney Diseases Malignant Neoplasms Mass Spectrometry Metals Methanol Molar Needles Oxidation-Reduction Oxidative Stress Perchloric Acid Physicians physiology Plasma Polyethylene Polypropylenes Serine Solvents Specimen Collection Spectrophotometry, Atomic Absorption Sulfhydryl Compounds Syringes Technique, Dilution Tissue Donors Urine Veins

Most recents protocols related to «Germanium»

Powder X-ray diffraction (PXRD) analyses were performed on an STOE-STADI MP powder diffractometer equipped with an asymmetrically curved germanium monochromator (Cu-Kα1 radiation, λ = 1.54056 Å) and a one-dimensional silicon strip detector (MYTHEN2 1K from DECTRIS). Samples for superstructural analysis were measured at room temperature in transmission mode. The simulated PXRD patterns were calculated using Mercury software 4.3.0.
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Publication 2023
Germanium Mercury Powder Radiotherapy Silicon Transmission, Communicable Disease X-Ray Diffraction
This research bears several limitations. First, the price surge of materials for EV engines and battery systems, including aluminum, copper, ferrum, etc., and materials used for electricity generation, including neodymium, dysprosium, indium, germanium, argentum, tellurium, etc., could also affect the EV adoption4 (link),5 (link). In addition, if the affordability of critical materials use is not guaranteed, carbon emission reductions in both transportation and the related industries would be held back80 (link). Further work could expand this analysis to assess how the economic competitiveness of other crucial low-carbon technologies would be affected by the foreseeing surge in the prices of critical materials, how various technologies would compete with each other more strategically, and ultimately how this would influence the realization of climate targets. Second, we do not consider the impact of phosphorus price changes on EV penetration when considering the adoption of LFP batteries given the negligible share of phosphorus in battery cost. However, the surging interest in LFP combined with the rising demand for phosphate from agriculture, the price of phosphorus (and other critical minerals) may move up along a non-stationary path and thus deserves further investigation in future research. Although the price of critical materials is a significant factor affecting the penetration of EVs, we cannot ignore the influence of other factors on the adoption of EVs (e.g., increasing availability and choice in EV models), which should also be paid attention to in future research. Third, it is worth noting that this study does not fully capture price linkages between materials, for example, cobalt prices may decrease with the adoption of low-cobalt batteries and nickel prices may increase accordingly, or lithium prices may increase further with the adoption cobalt-free LFP batteries.
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Publication 2023
Aluminum ARID1A protein, human Attention Bears Carbon Climate Cobalt Copper Dysprosium Electricity Germanium Indium Iron Lithium Minerals Neodymium Nickel Phosphates Phosphorus Tellurium
Samples for Raman spectroscopy were measured in HPLC glass vials in an FT-Raman RFS100/S spectrometer device with a germanium detector (Bruker Optics, Germany). The wavelength of the Nd:YAG laser was 1064 nm. The measurement range was 4000 to 0 cm−1, with a spectral resolution of 4.0 cm−1. Data were obtained at either 64 or 128 accumulations of the measured spectra. The software OPUS and OMNIC were used to process the Raman spectra.
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Publication 2023
Eye Germanium High-Performance Liquid Chromatographies Medical Devices Neodymium-Doped Yttrium Aluminum Garnet Lasers Spectrum Analysis, Raman
All chemicals were obtained from commercial sources and were used without further purification. 44Ti/44Sc solution (111.0 MBq, 421.8 MBq/mg titanium) was obtained from Brookhaven National Laboratory, Department of Energy. Both ZR resin and 0.43-mL ZR resin cartridges were obtained from TRISKEM International. Radioactivity amounts of 44Sc were measured with a dose calibrator (CAPINTEC, CRC-15R) or a 2480 WIZARD2 automatic γ-counter (PerkinElmer). Radiochemical purity was analyzed with high-purity germanium gamma ray detector (HPGe, ORTEC, GEM-50195-S), and spectral acquisitions were acquired and analyzed by Gamma-Vision Software (version 8.0, Ametek). PEEK columns were obtained from VICI precision sampling, Inc for assembly of the ZR resin column. Deionized water (18.2 MΩcm, Rephile) and 99.999% trace-metal HCl (37 wt% in H2O) were used for preparation of 44Sc elution. Female Swiss Webster mice (6–8 weeks from Charlies River Laboratories) were purchased for in vivo pharmacokinetic studies. All radioactive material handling and animal experimentation were conducted in compliance with institutional regulations and approved by Environmental Health and Safety Radioactive Materials protocol #1169-01 and Institutional Animal Care and Use Committee protocol #22-0023.
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Publication 2023
Females Gamma Rays Germanium Institutional Animal Care and Use Committees Metals Mouse, Swiss polyetheretherketone Radioactivity Radiopharmaceuticals Resins, Plant Rivers Safety Titanium Vision
Fourier-transformed infrared (FTIR) spectra of the Aβ42 oligomers prepared with 0–500 µM Ni(II) acetate, as described in the materials section, were recorded on a Tensor 37 FTIR spectrometer (Bruker Optics, Germany) operating in transmission mode at room temperature and equipped with a liquid nitrogen-cooled MeCdTe detector and a sample shutter. During the measurements, the instrument was continuously purged with dry air. 8–10 µL of the 80 µM Aβ42 oligomer samples were placed between two flat CaF2 discs, which were separated by a 50 µm plastic spacer that had been covered with vacuum grease at the periphery. The mounted IR cuvette was put in a holder inside the sample chamber, and was then allowed to sit for at least 20 min after the chamber lid was closed, to remove H2O vapor. FTIR spectra were recorded between 1900 and 800 cm−1, at a resolution of 2 cm−1 and with 6 mm aperture. The IR intensity above 2200 cm−1 was blocked with a germanium filter, and that below 1500 cm−1 with a cellulose membrane, to increase the light intensity in the relevant spectral range91 (link). The OPUS 5.5 software was used for analysis and plotting of the spectra. Second derivatives were computed with a smoothing factor of 17.
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Publication 2023
Acetate Cellulose derivatives Eye factor A Germanium Light Nitrogen Tissue, Membrane Transmission, Communicable Disease Vacuum

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Germanium, Ge, metalloid, atomic number 32, electronics, optics, transistors, fiber-optic cables, infrared detectors, nanotechnology, microelectronics, PubCompare.ai, OPUS software, Nicolet iS10, Spectrum 100, MYTHEN2 1K, D8 Advance, High-purity germanium detector, Nitric acid, Discovery ST PET-CT system, Vertex 70 FTIR spectrometer, Stadi P, semiconducting properties, analytical instruments, medical imaging, spectroscopic applications