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Photomultiplier tube detector

Manufactured by Hamamatsu Photonics
Sourced in Japan, United States

A photomultiplier tube (PMT) is a vacuum tube device that converts light signals into electrical signals. It consists of a photocathode that emits electrons when exposed to light, a series of dynodes that multiply the initial electrons through secondary emission, and an anode that collects the amplified signal. PMTs are highly sensitive detectors capable of detecting single photons and are commonly used in various applications, such as spectroscopy, medical imaging, and high-energy physics.

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4 protocols using photomultiplier tube detector

1

Fluorescence Spectroscopy of Oocyte Currents

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Excitation was provided by an LED source (X-Cite) operated at minimum (5%) output at 505–545 nm through a 20×/0.46 NA objective (Olympus). The illumination intensity was further reduced using a 0.4 ND (Semrock) filter to minimize photobleaching and filtered through a 525/50-nm bandpass filter (Semrock). A 562-nm dichroic (Semrock) and a 593/46-nm bandpass filter (Semrock) were used to separate fluorescence emission from reflected light. Fluorescence signals were detected with a Hamamatsu photomultiplier tube detector and transmitted directly to the Digidata 1440 A A/D converter at a frequency of 10 kHz. Oocytes were recorded from a 0-mV holding potential, or −60-mV holding potential with a −110-mV prepulse for 500 ms in paired recordings as was done for gating current recordings. Interpulse duration was 2 min and test pulse duration was 25 s for all recordings.
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2

Single-Laser Fluorescence Detection System

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A custom‐built single‐laser, single‐color fluorescence detection system was designed for electrophoretic separation and laser‐induced fluorescence (LIF) detection (Figure S2). The microdevice is placed on a metal stage that can be heated for electrophoresis and adjusted in three dimensions to focus the incident laser through a hole in the stage into the middle of the separation channel of the microfluidic device. Voltage‐driven electrophoresis was achieved by placing platinum electrodes connected to a high‐voltage power supply in the 3D printed reservoirs on the microfluidic chip seated on the metal stage. The custom‐built voltage supply system is controlled by LabVIEW. The fluorescence detection system consisted of a 488‐nm solid‐state laser for excitation, which was directed to a mirror, through a 525‐nm short pass dichroic mirror, and into the end of a 40× LD Acroplan, 0.6 NA objective (Zeiss, Thornwood, NY, USA) where it focused into the microdevice separation channel. The emission beam was passed back through the objective, reflected off the dichroic mirror, and passed through a 505‐nm long pass filter toward a photomultiplier tube detector (Hamamatsu, Tokyo, Japan). Data collection and electrophoresis conditions were controlled by a custom‐made LabVIEW program.
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3

Quantifying Nuclear Rim Localization

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Fluorescence images were obtained at RT with Zen 2010 software using an LSM700 upright confocal microscope (Zeiss) with an oil-immersed 63×/1.4 NA PLAN APO objective and two photomultiplier tube detectors (Hamamatsu). Nuclear rim staining quantification was performed using ImageJ software (National Institutes of Health). Raw data for both DAPI and Kapβ1 channels were first duplicated. The nuclear rim of each permeabilized cell was then defined as a region of interest by converting the DAPI channel into a binary image, followed by the processes of (a) filling holes (to fill up the whole nucleus), (b) outlining (to obtain the nuclear rim outline), and (3) dilating (to generate an ∼700-nm width for the nuclear rim). This region of interest was then applied to measure the mean fluorescence intensity of endoKapβ1 or exoKapβ1 in the Kapβ1 channel as well as in the Kapα channel. The intensity of Ran mix–treated samples was normalized to transport buffer–treated control samples. The mean fluorescence intensity of MG-NLS or MG was measured from the nuclear region defined by the DAPI channel. Similarly, the intensity was normalized to the control samples. Analyzed cell numbers are specified in respective figure legends.
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4

Imaging Vascular Smooth Muscle Cells in Collagen

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Vascular smooth muscle cells suspended in type I collagen as described above were imaged with a custom-built non-linear optical microscope as previously described (Larson and Yeh, 2006 (link)). Briefly, 10 femtosecond (fs) ultrashort pulses at 800 nm from a Ti:Sapphire oscillator (Femtolasers, Vienna, Austria) were pre-compensated with double-chirped mirrors (Femtolasers, Vienna, Austria), coupled into an upright microscope (Carl Zeiss, Thornwood, New York, United States) by x-y scanners (Cambridge Technologies, Cambridge, MA, United States), and focused with a 1.0 NA, 20× objective (Carl Zeiss, Thornwood, NY, United States). Second harmonic generation (SHG) and two-photon excited fluorescence from samples were collected by the same objective and separated with a dichroic mirror (430 nm long pass) and bandpass filters (405/20 nm for collagen I SHG and 450/60 nm for cellular auto-fluorescence) before being focused onto photomultiplier tube detectors (Hamamatsu, Bridgewater, NJ, United States). Voxel dimensions were 0.5 μm × 0.5 μm × 0.5 μm.
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