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Lock in amplifier

Manufactured by Zurich Instruments
Sourced in Switzerland

A lock-in amplifier is an electronic instrument used to measure small AC signals. It is designed to isolate a signal of a specific frequency from background noise. The lock-in amplifier uses a reference signal to synchronize its measurement, allowing it to detect and measure signals with extremely high precision, even in the presence of significant noise.

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Lab products found in correlation

6 protocols using lock in amplifier

1

Temperature-dependent AC spectroscopy protocol

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Temperature‐dependent AC spectroscopy is performed in a Linkam T95 electrical probe station equipped with a LNP 95 liquid nitrogen cooling system and a Zurich Instruments lock‐in amplifier.
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2

Femtosecond Transient Absorption Spectroscopy

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The experimental
system is based on a 20 W femtosecond Yb:KGW amplifier generating
200 fs pulses at 1030 nm (Pharos from Light Conversion) and operating
at 100 kHz. About 12 W of the output is used to pump a tunable optical
parametric amplifier (Orpheus from Light Conversion) to generate pump
pulses at the desired wavelengths. About 2 W of the output is used
to pump a sapphire substrate to generate white light continuum pulses
to be used as probe pulses. The pump pulses are modulated using a
mechanical chopper (Thorlabs), temporally delayed using a mechanical
translation stage (PI), and focused on the sample at a slight angle
with respect to the probe pulses. The probe pulses are collected after
the sample interaction and directed toward the Fourier transform spectroscopy
system based on a translating-wedge-based identical pulse encoding
system (GEMINI from Nireos srl).77 (link) The
transient absorption signal is then demodulated by using a photodetector
(Femto.de) connected to a lock-in amplifier (Zurich Instruments).
The GEMINI system provides a temporal interferogram of the TA spectrum,
which is a Fourier transform to obtain the experimental spectrum.
To obtain the spectrally integrated dynamics with a high signal-to-noise
ratio, we used optical filters to spectrally filter the desired spectral
ranges and detected the signal with the photodiode:lock-in system
without GEMINI.
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3

Impedance Spectroscopy in Phosphate Buffer

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Impedance measurements were performed in phosphate-buffered saline solution (PBS, same electrical properties as the medium used for neural culturing and plating). For impedance spectroscopy, a commercial potentiostat (Ivium CompactStat, Eindhoven, Netherlands), equipped with a frequency response analyzer (FRA module) was used. Measurements were performed between 1 Hz and 100 kHz with an alternating voltage amplitude of 10 mV peak to peak. Four points per frequency decade were recorded. The applied working potential during the measurements was maintained at 0.3 V against an Ag/AgCl reference electrode. Two-point impedance measurements were performed by using a lock-in amplifier (Zurich Instruments, Zurich, Switzerland) to verify the recordings with the Ivium potentiostat.
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4

Microfluidic Device for Particle Characterization

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The PDMS channel and gold electrodes are treated with oxygen plasma using a plasma chamber (100W power for 60 seconds at 60 cm3 per min of oxygen under vacuum). Immediately after, the PDMS is aligned using a stereomicroscope and placed above the microelectrodes with focusing regions positioned between outer electrodes (Fig. 1c). After soft baking for 1 hour at 60°C, syringe tubing was inserted into PDMS inlet and outlet holes and syringe needles are inserted into the opposite end to facilitate media infusion using a syringe and the NE-300 syringe pump (Southpointe Surgical Supply, Coral Springs, FL, USA). Silver conductive epoxy components (Digi-Key Electronics, Thief River Falls, MN, USA) are combined to connect microfluidic devices with custom printed circuit boards (PCB, Sunstone Circuits, Mulino, OR, USA) and baked at 60°C for 1 hour. The PCB then connects with a custom Veroboard which facilitates transimpedance amplification for signal detection using HF2TA current amplifiers (Zurich Instruments, Zurich, SUI) from outer electrodes and inputs an AC voltage signal at a 303 kHz frequency to the middle electrode using a lock-in amplifier (Zurich Instruments, Zurich, SUI). PS particles (1, 3, 5, 7, and 9 μm diameters, 2.5% w/v, Spherotech, Lake Forest, IL, USA) are diluted in 1X phosphate buffered saline (PBS) and flow is driven through a syringe pump.
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5

Ultrasound-Driven Microbubble Mapping

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The acoustic pressure field is mapped by hydrophone scanning. The transducer and the chip are immersed in a tank containing the electrolyte (80 mg mL−1 aqueous K2SO4 solution). The wiring of the PCB board is waterproofed with a cured polydimethylsiloxane (PDMS) covering. The bottom of the chip is placed in contact with the transducer. A 10-MHz AC signal with 5 Vpp amplitude is applied to the transducer (I3-1008-S-SU, ultrasound aperture 11 mm, Olympus Corporation, Japan). The generated acoustic waves transmit through the chip containing the microbubble pattern. The needle hydrophone (0.2 mm diameter, Precision Acoustics Ltd., UK) measurement across the imaging plane scans each point for 0.1 s, during which the signal from the hydrophone is amplified and filtered by a lock-in amplifier (Zurich Instruments, Switzerland). The scan area is 60–100 mm2, with a lateral resolution of 0.08–0.1 mm. A typical scan is completed in 30–60 min.
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6

Frequency-domain THz-OA Imaging Technique

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The frequency-domain THz-OA system is shown in Figure 6A. The continuous-wave terahertz radiation is generated by a sub-terahertz source (TeraSense, USA) and modulated at 5 kHz by an arbitrary function generator (Tektronix, USA). The output frequency of this source is 0.1 THz, and the average power is 80 mW. The THz-OA signal was detected using a microphone (BSWA, China) and processed by a lock in amplifier (Zurich Instruments, Switzerland). The temperature of the sample within the cell was controlled by a temperature control module, which is mentioned above.
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