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Igor pro 9

Manufactured by Wavemetrics
Sourced in United States

Igor Pro 9 is a powerful data analysis and visualization software designed for scientific and engineering applications. It provides a comprehensive set of tools for data acquisition, analysis, and presentation. Igor Pro 9 offers a user-friendly interface and a wide range of features to facilitate the processing and interpretation of complex data sets.

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21 protocols using igor pro 9

1

Statistical Analysis Techniques in Research

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All statistical analyses were performed using Igor Pro 9 software (WaveMetrics, USA), OriginPro 2023 (OriginLab, USA), or GraphPad Prism (GraphPad Software Inc., USA). A significance level of α = 0.05 was used for all analyses, and P values were adjusted for multiple comparisons where relevant. Unless otherwise noted, the normality of distributions was tested by the Shapiro-Wilk test. When it failed, the Kruskal-Wallis test and Mann-Whitney’s U test were used to compare the two groups. When several conditions were compared, one-way analysis of variance (ANOVA) and the Kruskal-Wallis test were used for the analysis of multiple groups with a single independent variable. The Dunnett’s and Dunn’s tests were used as follow-up tests to the Kruskal-Wallis test, where Dunn’s test was used to compare every mean with every other mean, and the Dunnett’s test was used to compare every mean to a control mean. The F test was used to compare the variance of two groups: P > 0.05, not significant; *P < 0.05, **P < 0.01, and ***P < 0.001 were considered statistically significant. Data are represented as the means ± SDs.
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2

FTIR Analysis of PHBV Samples

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Fourier-Transform Infrared Spectroscopy (FTIR) was performed on PHBV samples, in duplicate, using a Nicolet-iS5 spectrometer (Thermo-Scientific, Madison, WI, USA) equipped with an attenuated total reflectance (ATR) accessory (ZnSe, ID5). Spectra were baseline corrected, averaged, and analyzed using Omnic v9.5 software (Thermo-Scientific, Madison, WI, USA). The carbonyl index (IC=O A1720/A1740) was determined on normalized spectra that were curve-fitted using Igor Pro 9 software (WaveMetrics, Portland, OR, USA) [25 (link),26 (link)]. The area (A) of each carbonyl band at 1720 cm−1 and 1740 cm−1 were Gaussian curve fitted using a peak width at half height of 10 cm−1 and integrated.
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3

Statistical Analysis of Experimental Data

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Unless otherwise noted, results are reported as the mean ± standard error of the mean (SEM). Significance levels are denoted using asterisks (*p < 0.05, **p < 0.01, ***p < 0.001). Pairwise comparisons were carried out using a two-tailed Student’s t-test for equal means. If an equality of variances F test gave p < 0.05, we employed the unequal variances t-test. Wilcoxon-Mann-Whitney’s non-parametric test was always used in parallel to the t-test, yielding similar outcomes. Statistical tests were performed in Igor Pro 9 (Wavemetrics).
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4

Whole-cell patch-clamp analysis of TMEM-16 Cl- currents

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Current-voltage (I/V) relationships of Cl current through TMEM-16 stably expressed in HEK-293 cells were recorded using the whole cell mode of the patch-clamp technique [100 (link)]. During experiments, cells were perfused at a rate of 1 ml/min with an external Ringer’s solution of the following ionic composition (in mM): 145 CsCl, 2 MgCl2, 2 CaCl2, 5.5 Glucose, 10 HEPES, pH 7.4 (1 N CsOH). The pipette resistance used for whole cell recording ranged from 2-3 MΩ when filled with the following solution (in mM): 135 CsCl, 10 KCl, 2 MgCl2, 0.1 EGTA, 5.5 glucose, 10 HEPES, pH 7.2 (1 N CsOH). All measurements were performed at room temperature. Data were recorded and stored onto the hard drive of a computer equipped with pClamp software (Molecular Devices, San Jose, CA) and interfaced to an Axon amplifier Axopatch 200B (molecular devices) with Digitata 1440A (Molecular devices). Data were analyzed using Clampfit (molecular devices) and plotted using Igor Pro 9 (Wavemetrics, Lake Oswego, OR) or GraphPad Prism 9.3 (GraphPad software, San Diego, CA).
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5

Statistical Analysis and Graphing Protocol

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Data analysis and presentation were perform using Igor Pro 9 (Wavemetrics, Lake Oswego, OR) or GraphPad Prism 9.3 (GraphPad Software, San Diego, CA). Data were summarized as means ± SE. Statistical significance between groups was performed using ANOVA, followed by Tukey’s test for multigroup comparisons. P < 0.05 was considered significant.
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6

Statistical Analysis of Luminescent Intensities

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Statistical analysis was performed for log-transformed values of relative luminescent intensities with Igor Pro 9 software (https://www.wavemetrics.com/products/igorpro) ver 9.0.2.4 (WaveMetrics).
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7

Measuring GFET Drain Current Dynamics

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GFETs were measured by using a homemade
electrical measurement device produced by TOSHIBA Corporation. While
drain current was measured, we set the drain voltage (Vd) at 16 or
20 mV, and back gate voltage (Vg) at 0 V. Drain voltage was chosen
with the maximum value in the Id measurable range. The real-time response
of the drain current was measured every 0.5 s. For data analysis,
we used Igor Pro 9 (WaveMetrics) and Python.
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8

Neurophysiology of NPY Neurons

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Statistical analyses were performed using R 4.1.0 (The R Project for Statistical Computing), Igor Pro 9 (Wavemetrics), and MATLAB R2021a (MathWorks). For the comparison of the intrinsic physiology between NPYgfp and NPYflp neurons, we used Welch’s t-test, and the significance level (α) was adjusted to account for multiple comparisons using Bonferroni correction. For the remaining experiments, effects were considered significant when p < 0.05. Data are shown as mean ± SD. Principal component analysis (PCA) was performed using the “coeff” function in MATLAB. The first component of the PCA explained 97.18% of the data. After PCA, a k-means clustering analysis was performed using the “kmeans” function in MATLAB. The “elbow method” was used to determine how many clusters to divide the data into.
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9

SAXS Analysis of Molecular Structures

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SAXS measurements were performed at the DuPont-Northwestern-Dow Collaborative Access Team (DND-CAT) beamline at Argonne National Laboratory’s Advanced Photon Source (Argonne, IL, USA) with 10 keV (wavelength λ = 1.24 Å) collimated X-rays. All the samples (5 mg/mL) were analyzed in the q-range (0.001–0.5 Å−1), with a sample-to-detector distance of approximately 8.5 m and an exposure time of 5 s. The beamline was calibrated using silver behenate and gold coated silicon grating with 7,200 lines/mm The momentum transfer vector q is defined as q = 4πsinθλ−1, where 2θ is the scattering angle. Data reduction and buffer subtraction were performed using IRENA 2.71 package within IGOR PRO 9 software (Wavemetrics). Model fitting was completed using SasView 5.0.5 software package wherecore-shell sphere model was utilized to fit and analyze the data.
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10

Visualizing Colonic Peristalsis in Mice

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Ex vivo video imaging and analysis of colonic peristalsis were carried out as described previously (Obata et al., 2020 (link)) on age-matched male mice. Colons were dissected, flushed with sterile PBS, and pinned into an organ bath chamber (Tokai Hit, Japan) filled with Dulbecco’s Modified Eagle Medium (DMEM). DMEM was oxygenated (95% O2 and 5% CO2), run through the chamber using a peristaltic pump (MINIPULS 3, Gilson), and kept at 37 °C. Colons were allowed to equilibrate to the organ chamber for 20 min before video recording. Time-lapse images of colonic peristalsis were captured with a camera (MOMENT, Teledyne photometrics) using PVCAM software (500 ms time-lapse delay) and recorded for 45 min.
For analysis of colonic migrating motor complexes (CMMC), videos consisting of 5400 sequential image frames were stitched together in Fiji and read into Igor Pro 9 (WaveMetrics) to generate spatiotemporal maps using a customized algorithm developed by the Pieter Vanden Berghe lab at the University of Leuven, Belgium (Roosen et al., 2012 (link)). The generated spatiotemporal maps were used to determine the frequency and period of CMMCs. Each CMMC on the spatiotemporal map was further projected onto the axes to obtain the distance traveled (millimeters) and the time for the CMMC to travel such distance (seconds), allowing us to calculate the velocity (millimeter/second) of CMMCs.
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