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Pda36a

Manufactured by Thorlabs
Sourced in United States

The PDA36A is a high-speed, low-noise, Si amplified photodetector. It features a 3.6 mm2 active area and has a gain adjustment from 0 to 60 dB. The PDA36A operates over a wavelength range of 320 to 1100 nm.

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8 protocols using pda36a

1

Voltage Transients in Organic LEDs

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Voltage transients were measured in atmosphere. The same LEDs used in the charge extraction experiment were used to obtain the voltage transients. The LEDs were powered by a Hewlett-Packard 8114A pulse generator, and the voltage transients were recorded by a Tektronix TDS5104B oscilloscope. The spectrum of each LED was measured using an Ocean Optics HR4000 spectrometer and the power output of the LEDs was recorded using a Thorlabs PDA36A amplified silicon photodetector. The values of LD obtained were (11.5±1.2) nm for C60, (8.5±1.0) nm for SubPc, (4.7±0.7) nm for H2Pc, (2.8±0.4) nm for MgPc, (4.7±0.7) nm for CuPc, and (4.6±0.9) nm for PbPc. Values of LD for a single device were determined by averaging three to five voltage transient measurements using LED intensities ranging from about 10 to 150 mW cm−2. Reported LD values are obtained by averaging measurements of twelve C60, twelve SubPc, six H2Pc, three MgPc, fourteen CuPc and three PbPc devices. The error is the standard deviation across all devices and LED intensities.
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2

Two-Photon Imaging of Zebrafish Cerebellum

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Fluorescence was monitored with a custom-designed two-photon microscope (Fig. 1b). The embedded zebrafish were placed under a water immersion 40x/0.8 numerical aperture objective (OBJ1; LUMPlanFl40XW/IR2, Olympus) that focused the excitation light from a MaiTai HP laser (Newport). Multiple horizontal planes through the cerebellum were imaged at a 2 Hz scan rate (512 × 512 pixels, ~3 planes per fish). Emitted light was collected through the 40x objective, and reflected by two dichroic mirrors (DM1, 720dcxruv; DM2, 565dcxr; Chroma Technology) into separate red (F2; ET605\70m-2p, Chroma) and green (F3; ET525\50m-2p; Chroma) channels. Fluorescence signals were detected and amplified by photomultiplier tubes (PMTs, R3896; Hamamatsu), while scattered light from the focal plane was detected by a substage photodetector (PD, PDA36A, Thorlabs). Signals from the PMTs and the PD were acquired by ScanImage93 to generate fluorescence and contrast images of specimen in the focal plane.
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3

Measuring Implant Signal Fidelity

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Signal fidelity of the implant was measured by placing the implant above the cavity while the RF signal was modulated to provide varying pulse widths. The implant was oriented with the LED facing an amplified photodiode (Thorlabs, PDA36A) that was connected to an oscilloscope, measuring the resulting light waveforms. The waveforms were normalized to the maximum recorded voltages.
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4

Confocal Photothermal Microscopy for Protein Aggregates

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The laser platform developed for laser ablation of proteins was converted into a confocal photothermal (PT) microscope as described elsewhere34 (link) by combining the excitation laser beam with a collinear low-power probe laser (633-nm, He–Ne laser, model 117A, Spectra-Physics, Santa Clara, CA). Light absorption by aggregates resulted in formation of a local refractive-index change due to increase in local temperature. Probe beam modulation by this PT phenomenon was monitored with a photodetector (PDA36A, 40 dB amplification, ThorLabs, Newton, NJ) shielded with a narrow-bandpass filter (central wavelength 633 nm, spectral bandwidth 12.5 nm, LL01-633-12.5, Semrock, Inc., Rochester, NY). Data acquisition and system synchronization were performed using a high-speed (200 MHz) analog-to-digital converter board PCI-5124, 12-bit card, 128 MB of memory (National Instruments, Inc., Austin, TX).
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5

Microfluidic Droplet Sorting by Dielectrophoresis

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Droplets were made with
a flow-focusing microfluidic junction using HFE-7500 (3 M Novec;
refractive index nD = 1.29)23 (link) fluorinated oil and 2% 008-FluoroSurfactant
(RAN Biotechnologies). Gas-tight syringes (Hamilton Company) were
operated with syringe pumps (Nemesys, Cetoni). Droplets were sorted
into the positive outlet channel by dielectrophoresis. Electric pulses
were applied using on-chip NaCl electrodes. Optical fibers were used
to pass light from a LED (455 nm, M455F3, Thorlabs) via the detection
point to a photodetector (PDA36A, Thorlabs). Data visualization and
triggering of sorting events were performed as previously described
by Gielen et al.14 (link) A detailed protocol
is provided in the SI. 1,3-Bis(trifluoromethyl)-5-bromobenzene
(Sigma; refractive index nD = 1.427) was
mixed with HFE-7500 at different volume percentages, as described
in the Results and Discussion section. Flow
rates and sorting parameters are provided in the SI.
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6

Zebrafish Calcium Imaging with Two-Photon Microscopy

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A custom-built two photon microscope was used for imaging calcium activity and fluorescence in the embedded zebrafish. A MaiTai HP laser (Newport) was used to focus a 915 nm light beam through a water immersion 40x/0.8 NA objective (OBJ1; LUMPlanFl40XW/IR2, Olympus) onto the fish. Multiple separate horizontal planes of the fish were acquired sequentially in the dark at 2 Hz (256×256 pixels, 550x550 µm). The emitted light from the zebrafish larva was collected by the objective and directed towards two dichroic mirrors (DM1, 720dcxruv; DM2, 565dcxr; Chroma Technology) which reflected this light into two separate channels of green (F3; ET525\50m-2p; Chroma) and red (F2; ET605\70m-2p, Chroma) to be then amplified by the photomultiplier tubes (PMTs, R3896; Hamamatsu). A substage photodetector (PD, PDA36A, Thorlabs) detected light scattered from the focal plane and together with signal from the PMTs was processed by MATLAB based software ScanImage (53) to generate fluorescence images.
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7

Optomagnetic Measurement of Magnetic Nanoparticles

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Optomagnetic measurements were performed on the sample in the cuvette using the system previously described in (Donolato et al., 2015a; Bejhed et al., 2015) (link). In this setup, the magnetic field was applied along the path of the laser light (Sony optical unit, Sony, JP,  = 405 nm, light beam with a diameter of 2 mm). Two electromagnetic coils (1433428C, Murata Power Solutions Inc., U.S.A.) placed on either side of the cuvette provided a magnetic field excitation with an amplitude of 2.6 mT. The transmission of laser light through the cuvette (2 mm) was measured using a photodiode (PDA36A, Thorlabs Inc., U.S.A.). The magnetic field excitation was controlled and the photodetector signal was recorded via LabView using a data acquisition card (NI USB-6341, National Instruments, U.S.A.). The 2 nd harmonic complex lock-in signal was calculated from the time traces in LabView. The spectra were measured from 1 Hz to 1 kHz in 20 logarithmically equidistant steps. A spectrum was recorded in about 2 min.
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8

Optical Thickness of Mouse Ear

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We illuminated the living-mouse ear perpendicularly with a collimated laser beam (beam width ~1.5 mm) and measured the power of the transmitted ballistic light at 2 m away25 ,53 from the ear using a photodiode (PDA36A, Thorlabs, USA) to be (2.8±0.3) × 10−8 of the power of the incident light. Thus, the optical thickness of the mouse ear, defined as the negative natural logarithm of the fraction of unscattered light, was measured to be 17.4±0.1 (for six mice). All mice were under anaesthesia during the measurement.
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