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C7700 01

Manufactured by Hamamatsu Photonics
Sourced in Japan

The C7700-01 is a photosensor module manufactured by Hamamatsu Photonics. The core function of this product is to convert light signals into electrical signals.

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5 protocols using c7700 01

1

Droop Analysis in Quantum Wells

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The influence of droop related to the carrier density and internal electric field in QWs having different dbarrier are analyzed through various experiments. A source meter (Keithley 2400) was used for current injection. We used the integrated sphere with a fiber-coupled radiometrically calibrated spectrometer to measure the electrical and the optical properties of the LED operation under current injection. The detection of output power were performed by an array charge coupled device (Hamamatsu, S7031-1006, back-thinned CCD array). The L-I curve is measured in a current range of below 150 mA at room temperature. For temperature-dependent electrical experiments, the LED samples were mounted in a closed-cycle cryostat, and temperature was varied from 150 to 300 K. To carry out the time-resolved PL experiment, a mode-locked Ti:sapphire laser (Coherent, Chameleon Ultra II) was used with double frequency. The wavelength, width, and repetition rate of the pulse laser were 375 nm, 200 fs, and 200 kHz, respectively. A streak camera (Hamamatsu, C7700-01) was employed to measure the decay lifetime.
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2

Optoelectronic Properties of InGaN Nanowires

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The room temperature PL was measured on ensembles of InGaN NWs using a 266 nm diode-pumped solid-state (DPSS) laser with an average optical power of 30 mW at the sample surface. The carrier dynamics of the UIF and EIF samples were studied via TRPL using a Ti:sapphire pulsed laser with a small optical power of approximately 10 μW. The PL decays were detected by a streak camera (Hamamatsu, C7700-01) with a time resolution lower than 300 fs and a repetition rate of approximately 4 MHz.
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3

Characterization of MoSe2-mQDs Morphology

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The morphology of MoSe2-mQDs was analyzed using an atomic force microscope (AFM, SPA400, SⅡ, Chiba, Japan) in tapping mode under ambient conditions. UV-Vis spectra (Shimadzu UV-3101PC spectrometer, EVISA, Switzerland), fluorescence spectra (Perkin-Elmer LS 55 luminescence spectrometer, Waltham, MA, USA), and transmission electron microscopy (TEM, Tiatan cubed G2 60-300, FEI, Hillsboro, OR, USA) analyses were conducted. TEM samples were prepared by drying a droplet of the MoSe2-mQDs suspensions on a carbon grid. The photoluminescence (PL) measurements were carried out using a 325 nm He-Cd continues-wave (CW) laser, a monochromatic light from a 300 W-xenon lamp, and UV spectrometers (Maya2000, Ocean Optics, Dunedin, FL, USA) as a PL detector at room temperature. The PL excitations were measured by monochromatic light from a 300 W Xenon lamp and a highly sensitive photomultiplier tube as a PL detector. In order to elucidate the recombination dynamics, we carried out time-resolved PL experiments. A mode-locked femto-second pulsed Ti: sapphire laser (Coherent, Chameleon Ultra II, Santa Clara, CA, USA) system was used as an excitation source, and the five wavelengths of the pulsed Ti:sapphire laser (266 nm, 300 nm, 350 nm, 400 nm, and 450 nm) were employed. A streak camera (Hamamatsu, Japan, C7700-01) was utilized to measure the decay profile of the PL spectra at room temperature.
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4

Picosecond Pulse Radiolysis Spectroscopy

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Pulse radiolysis experiments employed the picosecond laser-triggered electron accelerator, ELYSE, coupled with a time-resolved absorption spectrophotometric detection system. Laser (260 nm) driven Cs2Te photocathode allows the production of short electron pulses with a typical half width of 7 ps, a charge of ∼6 nC, and an energy of ∼7.8 MeV at a repetition rate of 10 Hz. During irradiation, the sample solutions were contained in a fused cell with a path length of 5 mm, connected to a closed circulation system from a 100 mL stock solution that was used to renew the sample in the irradiation cell after each pulse using a peristaltic pump (flow rate: 100 mL/min). The diameter of the electron beam was 3 mm, and the irradiated volume was <0.1 mL.
Absorption spectral measurements were performed using the white light from a homemade Xenon flash lamp. The light was focused on the sample parallel to the electron beam with a smaller diameter and then directed onto a flat field spectrograph (Chromex 250IS), which disperses the light on the entrance optics of a high dynamic range streak-camera (model C-7700-01 from Hamamatsu) to obtain an image resolved in wavelength and time. The kinetic data and absorption spectra were extracted from three series of 200 resulting images. In this work, the transient spectra were measured from 290 to 720 nm at 1 µs and 100 µs.
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5

Picosecond Pulse Radiolysis of Metal Nanoparticles

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Pulse radiolysis experiments were carried out employing the picosecond laser-triggered electron accelerator, ELYSE, coupled with a time-resolved absorption spectrophotometric detection system39 (link). Laser (260 nm) driven Cs2Te photocathode allowed the production of short electron pulses with a typical half width of 7 ps, a charge of ≈6 nC, and energy of ≈7.8 MeV at a repetition rate of 10 Hz. During irradiation, metal NP solutions were contained in a homemade cell with a path length of 1 cm. The diameter of the electron beam was 3 mm, and the irradiated volume was less than 0.1 mL.
Absorption spectral measurements were performed using the white light from a homemade Xenon flash lamp. The light was focused on the sample parallel to the electron beam with a smaller diameter and then directed onto a flat field spectrograph (250IS, Chromex), which disperses the light on the entrance optics of a high dynamic range streak-camera (C-7700-01, HAMAMATSU) to obtain an image resolved in wavelength and time. The kinetic data and absorption spectra were extracted from three series of 250 resulting images. In this work, the transient spectra were measured from 290 to 720 nm at 1 µs, 10 µs, 20 µs, 100 µs, and 1 ms40 (link).
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