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Alpha a high performance frequency analyzer

Manufactured by Novocontrol
Sourced in Germany

The Alpha-A High Performance Frequency Analyzer is a laboratory instrument designed for advanced frequency analysis. It offers high-performance frequency domain measurements across a wide range of frequencies. The core function of this device is to accurately measure and analyze the frequency characteristics of various electrical signals and systems.

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10 protocols using alpha a high performance frequency analyzer

1

Broadband Dielectric Spectroscopy Measurements

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The dielectric spectroscopy measurements were performed using a broadband dielectric spectrometer, NOVOCONTROL, with an Alpha-A high-performance frequency analyzer in the LF domain (0.01 to 107 Hz), equipped with WinDETA software. The temperature was controlled within 0.2 K, at a constant ac voltage of 0.5 V.
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2

In-situ Electrochemical Characterization of PLD

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In situ electrochemical measurements during PLD deposition (i-PLD) were conducted with an Alpha-A High Performance Frequency Analyzer equipped with an Electrochemical Test Station POT/GAL 30V/2A setup (both Novocontrol Technologies, Germany). For i-PLD measurements, a sample was placed on the PLD heater and covered with a corundum mask (cutout 0.45 × 0.45 cm2) to prevent short circuiting of the working electrode and counter electrode via the edges of the sample during the subsequent film deposition. The working electrode was brought into contact with a PtIr-needle and the counter electrode via platinum paste brushed onto the heater. A sketch of the measurement setup can be found in Fig. 1.
Impedance measurements were typically conducted in a frequency range from 106 to 10−1 Hz (if needed for resolving the electrode feature, the frequency range was extended to 10−2 Hz), with an AC amplitude of 10 mV root-mean-square, and a resolution of 5 or 10 points per frequency decade. In many cases, oxygen partial pressure and temperature were kept at 600 °C and 0.04 mbar O2 for deposition; in some cases pressure and temperature were varied for a more detailed impedance characterisation.
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3

i-PLD Temperature Measurement Technique

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i-PLD was performed
with a custom-made setup inside the PLD chamber.40 (link) The bottom Ti/Pt grid was contacted with a brushed Pt electrode
on the heating stage, and the top grid was contacted with a Pt/Ir
needle. The temperature during i-PLD was controlled by evaluating
the ohmic offset in an across-plane impedance measurement. This offset
resistance includes contributions from wiring and grid resistances,
which were determined beforehand, as well as from thermally activated
ionic conduction through the electrolyte substrates. With the known
conductivity–temperature relationships for YSZ and LSGM,38 (link),41 (link) this technique allows for a very exact temperature measurement during
the PLD process. Impedance measurements were conducted with an Alpha-A
High Performance Frequency Analyzer and Electrochemical Test Station
POT/GAL 30 V/2A setup by Novocontrol Technologies in the frequency
regime from 106 to 10–1 Hz with an alternating-current
(ac) voltage of 20 mV root mean square (RMS). Ex situ measurements in synthetic air (5.0 purity, Messer, Austria) were
performed with the same setup by Novocontrol Technologies and a measurement
setup in a tube furnace. The temperature was measured with a type
S thermocouple, positioned 1 cm next to the sample.
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4

MEA Electrode Characterization by EIS

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Electrochemical impedance spectroscopy (EIS) measurements were performed with a Novocontrol Technologies Alpha-A High Performance Frequency Analyzer (Novocontrol Technologies GmbH & Co. KG, Montabaur, Germany). Impedance spectra between 100 Hz and 10 MHz were recorded at 200 distinct frequencies in total, applying a sinusoidal voltage of 10 mV amplitude. For the MEA electrode characterization, EIS was performed in a three-electrode arrangement using one MEA electrode as a working electrode (WE), a platinum wire as a counter electrode (CE), and a commercial Silver/Silver-Chloride (Ag/AgCl) (Dri-Ref short, World Precision Instruments, Inc., Sarasota, FL, USA) electrode as reference electrode (RE). These measurements were carried out in Dulbecco’s phosphate buffer saline (PBS) (purchased from Sigma-Aldrich Chemie GmbH, Munich, Germany).
To identify the optimum AC frequency for the electroporation pulse, we determined the normalized impedance, which describes the contribution of the cell layer to the total impedance. Hereby, two EIS measurements were conducted: one without the cells and one after 24 h, when the cells completely adhered to the MEA. These measurements were performed in cell culture medium and all 60 electrodes of the MEA were short-circuited to reduce the total impedance of the WE.
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5

Dielectric Spectroscopy of Materials

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The measurements were performed on a Concept 41 BDS system (Novocontrol Technologies GmbH, Montabaur, Germany) consisting of an Alpha-A High Performance Frequency Analyzer and a Novocool System for temperature control. The samples were mounted between two gold electrodes with a diameter of 30 mm. The measurements were carried out in a temperature range between −100 and 20 °C and in a frequency range between 0.1 and 2 × 107 Hz.
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6

Electrochemical Impedance Spectroscopy of PEDOT:PSS Films

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The PEDOT:PSS and PEDOT:PSS/GO films were initially investigated using EIS. The electrode under test was connected to the WE while an Ag/AgCl pellet served as the CE, and an electrochemical Ag/AgCl RE was connected to the RE port. A Novocontrol Technologies Alpha-A High-Performance Frequency Analyzer (Novocontrol Technologies GmbH & Co. KG, Montabaur, Germany) was used to measure the impedance spectra. The spectra were obtained in the frequency range between 0.1 Hz and 1 MHz, with an applied voltage amplitude of 10 mV in 1× PBS (pH 7.4) as the electrolyte.
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7

LLZO Ionic Conductivity Measurement

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The ionic conductivity of the LLZO samples was measured by electrochemical impedance spectroscopy (EIS) before and after the Li+/H+ exchange experiment. As electrodes, 200 nm thick Au layers were deposited on the top and bottom side of the samples using a MED 020 coating system (Bal-Tec AG, Liechtenstein). For the measurements, which were performed at room temperature (25 °C), an Alpha-A high performance frequency analyzer (Novocontrol Technologies, Germany) in the frequency range from 10 Hz or 1 kHz to 10 MHz was used.
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8

Dielectric Measurements of Thin Films

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The dielectric measurements were performed with an Alpha-A High-Performance Frequency Analyzer with a Novocool cryo-system (Novocontrol Technologies, Montabaur, Germany). The isothermal frequency sweeps, between 0.1 Hz and 2 × 106 Hz, were performed in a temperature range from −100 °C to 70 °C with an increment of 5 K. Specimens with a thickness from 150 µm to 250 µm were mounted between two round gold-plated electrodes in a plate-capacitor arrangement with a diameter of 30 mm.
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9

Comprehensive Characterization of CDI-Cu NF

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The morphology of synthesized CDI-Cu NF was investigated using variable pressure field-effect scanning electron microscope (VP-FESEM, Model: Zeiss Supra 55 VP), 3D-Nanoprofiler (Hawk 3D Optical Surface Profiler from Pemtron Co.Ltd., South Korea), and high-power microscope (Olympus, Japan). Elemental analysis of NF and different chemically modified surfaces were carried out using EDX and mapping method. The chemically modified different LSG surfaces were analyzed elementally using field-transform infrared spectroscopy (FTIR, Model: Perkin Elmer Spectrum One). All the capacitance measurements were carried out at room ambient using a standard two-electrode system (Alpha-A High-Performance Frequency analyzer, Novocontrol Technologies, Germany) in 4 µl PBS as a working solution. The frequency range was set with 1 to 100 kHz and Vrms at 10 mV.
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10

Electrical Characterization of Immunosensor

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Electrical measurements were conducted to analyze signals transduced by the Ag-Ab binding reaction from the PSNG electrode, which were probed via the Au contact pad on the LOC (Fig A in S1 File). AC measurements were conducted using an impedance spectrometer (Alpha-A High Performance Frequency Analyzer, Novocontrol Technologies, Hundsangen, Germany). A two-wire probe station was used with the impedance spectrometer to measure capacitance (C), permittivity (ε), loss tangent (tan δ) and conductivity (σ). Measurement was started at 0.1 V with a scaling factor of 1.4 and a frequency range of (1 x 100 to 1 x 106 Hz). The loss tangent (tan δ) value was continuously monitored during capacitance measurement to ensure it stayed below 100, indicating that the immunosensor was behaving as a capacitor. A Kiethley 6487 Picoammeter was used to measure current-voltage DC characteristics of the PSNG electrode, from which amperometric characteristics and sensitivity of the immunosensor could be analyzed. At each step during hCG detection, the PSNG electrodes were washed with DI water to ensure that measurement data were valid.
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