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Pmt2101

Manufactured by Thorlabs
Sourced in United States

The PMT2101 is a high-performance photomultiplier tube (PMT) detector module from Thorlabs. It features a high-gain, low-noise PMT with a quantum efficiency of up to 40% for detection of low-light signals. The PMT2101 provides a compact, pre-assembled solution for photon counting and light detection applications.

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7 protocols using pmt2101

1

High-speed Two-Photon Imaging with SiPM

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The high dynamic range SiPM amplifier was installed in a custom-built two-photon microscope using a 24,000 line per second resonance scanner with a peak pixel rate of 78.0 MP/s and an average rate (accounting for oversampling due to resonant scanning trajectory) of 50.3 MP/s. Individual frames were 2048 × 2048 pixels. Illumination was provided by an 800 nm, 100 fs KMLabs Titanium:Sapphire (Ti:S) oscillator with a maximum power output of 275 mW and a repetition rate of 78 MHz. Thus, at the center of each frame, exactly one laser pulse was incident per pixel. In addition, the system had a Hamamatsu H10770-40PA GaAsP PMT with a transimpedance amplifier (PMT2101, Thorlabs, Inc.). 10× 0.45 NA (MRD70100, Nikon Instruments Inc.) and 16× 0.8 NA (MRP07220, Nikon Instruments Inc.) objectives were used for imaging. Except where noted, 25 MHz low pass filters were installed on both PMT and SiPM detectors to ensure equal bandwidth, and all imaging parameters were identical in all measurements. As in previous work12 (link), the collection optics were designed such that the limiting aperture was inside the microscope objectives. Therefore the difference in active area of the SiPM (3 mm) and the PMT (5 mm) has no effect on light collection. Optical design files are provided along with the PCB designs.
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2

Multimodal Multiphoton Imaging System

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Regarding the detection part, this system is designed to detect NAD(P)H from the 3PAF channel and FAD from the 2PAF channel, combined with noncentrosymmetric structures from the SHG channel and interfacial features from the THG channel, all simultaneously. The reflected multimodal multiphoton signals were spectrally-separated into four detection channels by long-pass dichroic mirrors and appropriate band-pass filters, as shown in Fig. 1. To minimize the crosstalk between individual channels and maximize the detection efficiency of each channel, the four channel filters were chosen with specific bandwidth characteristics and listed in Fig. 1. For this system, the high pulse peak power can enable more than one photon excitation per pulse when operating at low repetition rates. Therefore, the spectrally-separated signals were detected by analog PMTs instead of photon-counting PMTs (PMT2101, Thorlabs for 3PAF/ 2PAF/ THG channels; PMT1001, Thorlabs for SHG channel).
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3

Microfluidic Flow Visualization Technique

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To visualize microfluidic flows,
the fully packaged ND probe (Figure 4a) was connected to external pressure-controlled pumps
(Flow-EZ Module, LU-FEZ-7000, and LU-FEZ-N800, Fluigent) for push
(P2 in Figure 4d) and
pull (P1 in Figure 4b,d) aqueous flows, and a push oil flow (P0 in Figure 4d). Since the top SiNx layer of the probe
is transparent for visible light, standard fluorescence microscopy
was used. Imaging and characterization of flows and droplets were
done with an inverted fluorescence microscope (IX73, Olympus) equipped
with a photomultiplier tube (PMT 2101, Thorlabs), video cameras (EOS
Rebel T7i, Canon, and Hero8, GoPro) and an LED lamp at 400 nm wavelength
(pE-300 White, CoolLED) for fluorescence excitation. To visualize
the flows (e.g., Figure 4d,e), a fluorescein solution in DI water was used at various concentrations
up to 1 mM as specified for each experiment (e.g., Figure 4d).
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4

Multiphoton Imaging with Customized Setup

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It is taken with a commercial multiphoton microscope with both 2P and 3P light path (Bergamo II, Thorlabs). A high numerical aperture (NA) water immersion microscope objective (Olympus XLPLN25XWMP2, 25 X, NA 1.05) is used. For GFP and THG imaging, fluorescence and THG signals are separated and directed to the detector by a 488 nm dichronic mirror (Di02-R488, Semrock) and 562 nm dichronic mirror (FF562-Di03). Then the GFP and THG signals are further filtered by a 525/50 nm band-pass filter (FF03-525/50, Semrock) and 447/60 nm (FF02-447/60, Semrock) band-pass filter, respectively. The signals are finally detected by GaAsP photomultiplier tubes (PMTs) (PMT2101, Thorlabs).
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5

Two-Photon Calcium Imaging in Mouse Cortex

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Ca2+ imaging in the mouse cortex was performed with a custom-built two-photon microscope based on an open-source design (MIMMS 2.0, janelia.org/open-science) and controlled with Scanimage 5.7_R1 software (Vidrio Technologies) and National Instrument electronics. The Ti:Sapphire excitation laser (Tiberius, Thorlabs) was tuned to 930 nm and focused with a 16×0.8 NA objective (Nikon) below the cortical surface. The laser power (typically 25 mW measured at the objective) was modulated with Pockels Cells (350-80-LA-02, Conoptics) and calibrated with a Ge photodetector (DET50B2, Thorlabs). A 550 µm by 550 µm area of cortex was scanned at ≈30 frames/s using a resonant-galvo scanning system (CRS8K/6215H, CRS/671-HP Cambridge Technologies). Emitted fluorescence was detected with GaAsP photomultiplier tubes (PMT2101, Thorlabs) and the acquired 512 × 512 pixel images written in 16 bit format to disk. Behavioral event (trial start and stimulus onset) TTL pulses issued by the Bpod State Machine were received as auxiliary inputs to the Scanimage electronics and their timestamps saved in the headers of the acquired images. The timestamps were used to temporally align neuronal data to behavioral events.
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6

Dendritic Calcium Imaging with 2-Photon Microscopy

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We used a 2-photon imaging system described previously63 . All imaging was conducted using a custom-built 2-photon 8 kHz resonant scanner using large aperture fluorescence collection optics (primary dichroic: 45.0 ×65.0 ×3.0 mm T865lpxrxt Chroma, US; secondary dichroic: 52.0 ×72.0 ×3.0 mm FF560-FDi02-t3 Semrock, US; green emission filter: 50.8 mm FF01-520/70 Semrock, US; red emission filter: 50.8 mm FF01-650/150 Semrock, US; GaAsP PMTs for green and red channels, PMT2101 Thorlabs, US) paired with a Nikon 16x water immersion, 0.8 NA, 3.0 mm working distance objective. Laser power was controlled with a Pockel cell (350-80LA modulator, 320RM 401 driver, Conoptics, US). Image acquisition was controlled through commercial software (ScanImage, Vidriotech, US). jRGECO1a expressing cells were imaged at 1020 nm (Chameleon Ultra II, Coherent, US). All frame scans lasted 1–2 minutes and were acquired at 120-240 Hz (40–60x optical zoom; 64–128 lines/frame, 64–128 pixels/line) from dendrites (oblique and tuft). Dendritic jRGECO1a signals were deconvolved to detect putative events by applying the OASIS software package64 (link),65 (link) using an AR1 model with a pre-computed signal decay constant of 300 ms (Arg = 0.97; event threshold = 0.3). All dendritic calcium analyses were performed on the deconvolved events.
Reagent table can be found as Supplementary Table 1.
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7

Multimodal Neuronal Activity Imaging

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Rats were anesthetized with isoflurane (4% for induction, 0.5% during recording) and sedated with Chlorprothixene Hydrochloride (intramuscular injection of 300µl of 1 mg/ml solution, Sigma) as was used previously in mice to achieve stable recordings with minimal side effects of isoflurane on neuronal activity [17, 21, 23, 27, 28, 38] . Rats were placed on a heating pad, and were restrained and head-fixed to a custom mount under a two-photon microscope (Bergamo II, Thorlabs). Fluorescence signal was recorded using a 950nm wavelength (50-150 mW, Insight X3, Spectra-Physics) using an 8KHz resonant scanner (Cambridge Technology) and GaAsP photomultiplier tube (Thorlabs PMT2101). We collected light from fields of view (FOVs) with 512x512 pixels at 30 frames per second and with a 16x 0.8NA objective (CFI75 LWD, Nikon) for comparing spontaneous activity between GCaMP6f-and jGCaMP7s-labeled neurons, or a 10x 0.5NA objective lens (TL-10X 2P, Thorlabs) for longitudinal activity recording experiments. The respective FOV size was 200x200 or 500x500 µm 2 .
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