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Dpo7254

Manufactured by Tektronix
Sourced in United States

The DPO7254 is a digital phosphor oscilloscope from Tektronix. It has a bandwidth of 2.5 GHz and can sample at up to 40 GS/s. The instrument is capable of capturing and displaying waveforms with a high level of detail and precision.

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8 protocols using dpo7254

1

Characterization of Plasma Discharge

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Applied voltage and current profile during plasma discharge were measured by a high voltage probe (P6015A Tektronix, Beaverton, OR, USA) and fast current monitor (6585 Pearson Electronics, Palo Alto, CA, USA), respectively. The two signals were recorded using an oscilloscope (Tektronix, DPO7254). The plasma behavior was recorded using a digital camera (EOS-7D Mark II, Cannon, Tokyo, Japan). The image was taken under the following conditions: f-number 3.5, iso of 400, and exposure time of 1/200 s. The emissions characteristic of the plasma was measured using spectroscopy (HR4000CG-UV-NIR, Ocean Optics, Orlando, FL, USA) with an optical cable (Ocean Optics/QP400-2-SR). To collect the spectra during discharge, an optical lens was placed perpendicularly to the pin axis. Spectra were recorded at an integration time of 1 s and wavelength range of 200 to 1000 nm.
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2

Spectroscopic Analysis of TMPyP4/TiO2 Photosensitizers

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The TMPyP4 concentration in the TMPyP4/TiO2 suspensions was determined by UV Vis absorption spectroscopy in quartz cells of 1 cm path length, in the spectral range 200–800 nm. The measurements were achieved by using a spectrophotometer Lambda 950 (Perkin-Elmer, Waltham, MA, USA).
FTIR spectrometer (Nicolet iS50, Thermo Scientific, Waltham, MA, USA) in absorption mode with a resolution of 4 cm−1 was used to record the IR spectra. Each sample was placed on a KRS-5 crystal and dried in direct air flux.
The generation of singlet oxygen by the PS samples was investigated by time-resolved phosphorescence emitted at 1270 nm [27 (link),28 (link)]. The excitation was made with the second harmonic generation (SHG) of a pulsed Nd:YAG laser (Minilite II, Continuum, Excel Technology, Milpitas, CA, USA), λ = 532 nm, 6 ns FWHM, 10 Hz, and the pulse energy 3 mJ. The solutions were placed in a quartz cuvette with an optical path of 1 cm. A near-IR photomultiplier tube (PMT) module (Hamamatsu H10330 Module) was placed at a 90-degree angle with respect to the incident laser beam to collect the signal. Interferential optical filters were used to eliminate wavelengths other than 1270. The PMT was coupled with a Digital Phosphor Oscilloscope (Tektronix type DPO-7254) to measure the signal.
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3

Monitoring FMN Triplet State Lifetime

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An additional 633 nm cw laser was added to the optical setup to monitor the FMN triplet state lifetime in a flash-photolysis experiment31 (link). The polarization of the cw laser was oriented at the magic angle with respect to the excitation beam polarization. The laser beam was passing through the sample area excited with the pulsed laser. The time-resolved absorption at 633 nm was measured with an avalanche photodiode (Thorlabs, APD110A2) connected to a digitizing oscilloscope (Tektronix, DPO 7254). The average signal of 2500 laser pulses was acquired consecutively throughout the irradiation experiment. Eighteen decay curves were measured during the 75 minutes interval. The protein concentration was 25 µM.
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4

Photoacoustic Calorimetry Experimental Setup

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The photoacoustic waves were generated with a pulsed 6 ns FWHM Nd:YAG laser (EKSPLA NL301G NdYAG) that when necessary was coupled with an OPO (EKSPLA OPO PG-122) or with a 30 ps FWHM Nd:YAG laser (EKSPLA 2143A), with a diameter of 2 mm. With the ns pulse laser, a fluence of 10 mJ cm−2 was used, while with the ps laser, a fluence of 2 mJ cm−2 was used. The presence of high frequencies was analyzed using a front-face irradiation setup (Fig. 1) developed by our group for photoacoustic calorimetry experiments,29 (link) with a 225 MHz contact transducer (Panametrics/Olympus, model V2113). We used a quartz mirror capable of reflecting >99% of the incident light to ensure the safety of the detector. It must be noted that the results were obtained using this quartz mirror of 1 cm between the material to be analyzed and the transducer, so high frequencies may be significantly attenuated. The piezophotonic material was placed on top of the mirror, which is inside of a support, and we applied silicon or water gel to improve the acoustic coupling. Finally, a heavy material (1.5 kg) with an optical window was placed over the film to ensure confinement. The signal was recorded using an oscilloscope (DPO7254 Tektronix, 2.5 GHz bandwidth) with an average of at least 200 waveforms. Films were replaced whenever they appeared to be damaged.
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5

Colon Tissue Autofluorescence Measurement

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Tissue autofluorescence was excited with 355 nm pulsed laser (<0.6 ns per pulse, >2 μ J per pulse, repetition rate 4 kHz; TEEM photonics STV-02E, Meylan, France). A 400 μ m core diameter multimode fiber placed perpendicular to the sample was used to deliver and collect the light. A second multimode fiber (600 μ m in core diameter) was used to guide the tissue autofluorescence to a monochomator (MicroHR, Horiba, Kyoto, Japan). Light was detected with a gated microchannel plate photomultiplier tube (R5916U-50, Hamamatsu, Hamamatsu, Japan) connected to a high-speed amplifier (C5594, Hamamatsu), and digitized by an oscilloscope (DPO7254, Tektronix, Beaverton, OR, USA). The laser power at the sample plane was kept under 5 mW. Fluorescence decays were acquired from 370 to 600 nm with 2 nm increments and a 0.08 ns resolution. Each data point was an average of 64 decays.
Data were acquired from three points along the length of the colon corresponding to the proximal, the middle, and the distal ends. Three measurements were taken on each position. The results presented in Figure 2 represent the mean (solid thick line) over 4 independent samples (2 female and 2 male) and their corresponding standard deviation (shaded area). Samples were kept in phosphate buffer saline (PBS) for the duration of imaging.
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6

Laser Diode Performance Evaluation

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To test the performance of the laser diode over extended periods of times, we connected two laser diodes TB450B (Osram, Germany) and HL63193MG (Oclaro, USA) to an optical fiber (M45L01; Thorlabs, USA) to simulate the conditions of the setup shown in Fig. 1b. Light at the output of the fiber was attenuated with an absorptive Neutral Density filter (optical density of 2; NE20B-A; Thorlabs, USA) and measured with a photodiode (DE10A/M; Thorlabs, USA). Attenuation was necessary to avoid photodiode saturation. We employed bursts of 500 pulses at a repetition rate of 625 kHz repeated every 2.4 ms to mimic the scan parameters employed in the imaging of the mouse ear in vivo. The applied voltage on the current driver was 300 V. The photodiode signals were recorded by a digital oscilloscope (DPO 7254; Tektronix, USA) with 2.5 GS/s sampling rate and averaged 500 times; the peak voltage and FWHM pulse width of each averaged optical pulse was saved on the PC. Measurements were run over 140 h, in many intermittent sections over a course of 2 weeks.
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7

Coincidence Waveform Acquisition with LFS Detectors

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Coincidence waveforms were acquired using two identical detectors (Figure 1), each consisting of a 5 × 5 × 10 mm lutetium fine silicate (LFS) crystal wrapped with 5 layers of Teflon tape and coupled to a single channel photomultiplier tube (PMT, Hamamatsu R12844) using pressure sensitive optical adhesive (3M 8194). The face-to-face distance between detectors was ~ 40 cm. A 100 kBq 68Ge point source was stepped between the detectors at 5 mm increments over a 15 cm range (−7.5 cm to +7.5 cm from the mid-point between detectors), so that a total of 29 datasets were acquired. The PMT waveforms were digitized at 10 GS/s using a bench-top oscilloscope (Tektronix DPO7254), and approximately 15,000 coincidence waveforms were acquired for each source position.
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8

Characterization of ZnO Nanorod Optoelectronic Properties

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The morphology of the nanorods and the device were characterized using a field emission scanning electron microscope (Model JSM-6700F) and the QD diameter and morphology were measured using transmission electron microscopy (Model JEOL 2010f ). The steady-state PL was measured using a homebuilt PL system. Samples were excited using a 325 nm line from a Hd-Cd continuous-wave laser and the fluorescence was dispersed by double gratings and collected using a Hamamatsu R928 photomultiplier tube. A lock-in amplifier was integrated in the system to increase the signal to noise ratio. Transient PL of the ZnO green emission was excited using a 325 nm laser line of a wavelength tunable pulsed laser (5 ns pulse width, repetition rate 20 Hz). The above mentioned PMT was applied to collect the green emission signal and the output was stored on a digital phosphor oscilloscope (Tektronix DPO 7254) and averaged over 500 periods to improve the signal-to-noise ratio. The QD lifetime was measured using DCS-120 Confocal Scanning FLIM Systems with a temporal resolution of 100 ps. The excitation wavelength was 375 nm.
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