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Sp 2300i

Manufactured by Teledyne
Sourced in United States

The SP-2300i is a high-performance spectrophotometer designed for accurate and reliable measurements. It features a wide wavelength range, high-resolution optics, and advanced data analysis capabilities.

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6 protocols using sp 2300i

1

Topological Cavity Optical Characterization

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A 980-nm pulsed laser diode (1.6% duty cycle; 1 MHz period) was used to optically pump the fabricated topological cavities at room temperature. The light emitted from the cavities was collected by a 50× long-focal objective lens with a numerical aperture of 0.42 (M Plan Apo NIR B, Mitutoyo) and focused onto a spectrometer (SP 2300i, Princeton Instruments). The grating with 300 grooves mm−1 blazed at 1.2 μm was used to spectrally disperse the PL emission from the cavities. The light was sent to either an IR array detector (PyLoN, Princeton Instruments) or an InGaAs IR camera (C10633, Hamamatsu) using a flip mirror in the spectrometer. For conventional mode imaging (not spectral imaging), a mirror was placed instead of the grating.
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2

Raman Spectroscopy Characterization Protocol

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The measurements
were performed using a bespoke Raman system consisting of a monochromatic
laser (HeNe, ThorLabs) with a beam splitter and a long-pass filter
(RazorEdge, Semrock), an inverted optical microscope (IX71, Olympus),
a spectrograph (SP-2300i, Princeton Instruments), and a CCD camera
(iDus 401, Andor).55 (link),68 (link)−70 (link) A 50×
objective was used to focus the laser (532 nm wavelength, 5 mW incident
power regulated by an attenuator) and collect the Raman and fluorescence
signals with an exposure time of 2 s in an accumulation mode (10 accumulations).
The CCD camera was calibrated over the spectral window using the Raman
spectrum of toluene. To take spatial variability into consideration,
an average signal from 10 different spots on the sample was reported.
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3

Raman-Based Electric Field-Tuned PEF Measurement

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PEF measurements were undertaken
using a bespoke Raman system that consisted of an inverted optical
microscope (IX71, Olympus), a monochromatic laser (green laser, ThorLabs)
with a beam splitter and long-pass filter (RazorEdge, Semrock), a
spectrograph (SP-2300i, Princeton Instruments), and a CCD camera (IXON,
Andor).12 (link),13 (link) To focus the laser (532 nm wavelength, 5
mW incident power), a 50× objective was used. PEF spectra were
collected with an exposure time of 1 s. A 30 μL sample of the
analyte molecule TMPyP, RhB, or QDs with and without PMMA at a concentration
of 10–9 M was deposited (drop-casting) above the
aligned FFNTs in the presence and absence of AgNPs. The average of
typically 10 measurements is reported. PEF measurements were performed
during an in situ applied electric field generated
through the application of 0–60 V, in steps of 5 V; the voltage
was applied using a PEW0028 DC power supply, following a process reported
previously.12 (link),35 (link) Electrical cables or bonding
wire was used to connect the microfabricated chip using silver paint,
and then a DC voltage was applied during in situ Raman
measurements as shown in Figure 1a. Relaxation was also recorded after removing the
applied electric field or by applying low electric field values. The
current flow in the microfabricated chip was measured using a TENMA
digital multimeter (72-7725).
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4

Nanoscale PL Characterization of InGaN/GaN MQWs

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A home-built tuning fork based NSOM was employed for nanoscopic PL measurements, using an aluminum coated optical fiber tip with ~100 nm aperture (MF001, NT-MDT, Russia). A 405 nm diode laser (L405P150, Thorlab, USA) was used as the excitation source to excite the InGaN/GaN MQWs samples. The excitation source was coupled with optical fiber using an optical fiber coupler (9131-M, Newport, USA) and illuminated the NSOM tip through an optical fiber. The luminescence of the sample was collected by an objective lens. Finally, the luminescence of the sample was filtered by a long-pass filter (LP02–407RU-25, Semrock, USA) and spectrally resolved using a monochromator (SP-2300i, Princeton Instruments, USA), and then measured using an electron multiplying charge coupled detector (ProEM, Princeton Instruments, USA). For the power dependent NSOM PL measurement, each level of laser power was measured in front of the optical fiber coupler. The results of the NSOM PL were analyzed using home-built software.
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5

Optical Characterization of AuNIs

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All absorption
spectra of AuNIs were calculated by using the measured transmittance
and reflectance spectra with a collimated white LED (MCWHL5-C1, Thorlabs,
Inc.) coupled spectrometer (SP-2300i, Princeton Instruments, Inc.).
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6

Single-Particle Scattering Spectroscopy and Imaging

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Single-particle dark-field scattering spectroscopy and imaging were performed with an upright optical microscope (Olympus, BX53M) integrated with a quartz–tungsten–halogen lamp (100 W), a digital colour camera with a resolution of 1200 × 1600 pixels (Olympus, DP73), and a monochromator (Princeton Instruments, SP2300i, cooled to −70 °C). A 100× dark-field objective with a numerical aperture of 0.9 was used for both the excitation of the individual nanoparticles with white light and the collection of the scattered light. For the emission polarization characterization, a linear polarizer (U-AN360, Olympus) was placed in front of the camera. A pattern-matching method was applied to correlate the optical images from single-particle dark-field scattering characterization with the geometrical structure of the individual nanoparticles from SEM imaging.
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