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Nirvana 640st

Manufactured by Teledyne
Sourced in United States

The NIRvana 640ST is a high-performance shortwave infrared (SWIR) camera from Teledyne. It features a 640 x 512 pixel InGaAs detector array with a spectral response range of 0.9 to 1.7 microns. The camera is designed for applications that require high-sensitivity SWIR imaging.

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7 protocols using nirvana 640st

1

Electrical Characterization of QDLEFET

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Electrical characterization
of the QDLEFET was done using a Keithley 4200-SCS semiconductor parameter
analyzer. Electroluminescence and photoluminescence spectra were collected
using a spectrometer and recorded by an Andor iDus 1.7 μm InGaAs
camera. The electroluminescence EQE was calculated using a calibrated
photodiode, put in contact with the back side of the substrate. Using
these data, the camera was calibrated to estimate the EQE of the electroluminescence
and photoluminescence at low temperature. For low-temperature measurements,
the substrate was placed in a He-cooled cryostat with spring-loaded
contact pins for reliable electrical connection. Channel imaging was
done by a cooled 2D InGaAs camera (640 × 512 pixels NIRvana 640ST,
Princeton Instruments), using a 50× objective.
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2

Angle-Resolved Optical Characterization

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Transmission
spectra were
recorded with a V-770 (JASCO) spectrophotometer. For angle-resolved
reflectivity measurements, a white light source (Ocean Optics, HL-2000-FHSA)
was focused onto the sample by an infinity corrected ×100 nIR
objective with 0.85 NA (Olympus, LCPLN100XIR). The resulting spot
diameter of ∼2 μm defined the investigated area on the
sample. For angle-resolved PL, the white light source was replaced
with a 640 nm laser diode (Coherent OBIS, 5 mW, continuous wave) and
the reflected laser light was blocked by an 850 nm cutoff long-pass
filter. The reflected/emitted light from the sample was imaged onto
the entrance slit of an imaging spectrometer (Princeton Instruments
IsoPlane SCT 320) using a 4f Fourier imaging system (f1 = 200 mm and f2 = 300 mm).
The resulting angle-resolved spectra were recorded with a 640 ×
512 InGaAs array (Princeton Instruments, NIRvana:640ST). A linear
polarizer was placed in front of the spectrometer to select between
s and p polarization.
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3

Non-invasive Near-Infrared Imaging System

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NIR fluorescence images were collected using a home-built imaging system (Fig. 4a). The excitation light was provided by a 48 W, 735 nm LED (IP-307TC5, Lanics) and filtered by an 800-nm short-pass filter (#84-729, Edmund Optics Inc.). The emitted light from the mouse was filtered by a 1,000-nm long-pass filter (ITF-50S-100RM, Sigma Koki) to reject excitation light and autofluorescence, and then collected by a 640 × 512 pixel two-dimensional InGaAs array (NIRvana 640ST, Princeton Instruments) equipped with an objective lens (COSMICAR, PENTAX). The camera was set vertically at 16 cm from the imaging stage. The excitation LED was located at 14 cm from the imaging stage with the elevation angle 60°. LED light intensity at the surface of the mouse was about 40 mW cm−2. Temperature raise of the mouse body by LED irradiation was confirmed to satisfy the regulations approved by the Animal Care and Use Committee of AIST. The exposure time for all images was 100 ms. The numerical aperture of the lens was adjusted depending on the experiments: 2.8 and 4 for comparative vascular imaging in 100 and 200 μl injection, respectively, 5.6 for dynamic imaging, and 1.4 for low-dose imaging.
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4

Photoluminescence Characterization of FET Devices

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Photoluminescence (PL) images
and spectra were acquired from FETs (dielectric variation devices: L = 20 μm, ttmgb devices: L = 10
μm) through the glass substrate with a near-infrared ×20
objective (Olympus, NA 0.4), a Princeton Instruments IsoPlane SCT
320 spectrometer, and a thermo-electrically cooled InGaAs camera (NIRvana
640ST, Princeton Instruments, 512 × 640 pixels). The excitation
laser beam (640 nm, continuous-wave, OBIS, Coherent) was expanded
with a plano convex lens (focal length f = 125 mm)
in front of the objective, and PL spectra were recorded and averaged
over an area of 700 μm2. Scattered laser light was
blocked using a 700 and an 850 nm long-pass filter. The PL spectra
were corrected for the detector sensitivity and the absorption of
the optics in the detection path. Spectra were fitted with three Lorentzians
after Jacobian conversion54 (link) of wavelength
to energy scale. PL quenching was induced by applying a constant gate
voltage using a Keysight B1500A semiconductor parameter analyzer.
A small drain voltage of Vd = 0.01 V was
applied during PL quenching experiments to record current flow without
significantly altering the charge carrier distribution along the channel.
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5

Near-Infrared Fluorescence Imaging System

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A home-built imaging system was used for the mouse whole body imaging and paraffin-embedded tissues as described previously18 (link). A lamp (IP-307TCS, Lanics; 800-nm short pass filter, FIT Leadintex, Inc., Tokyo, Japan) was placed obliquely above the mouse, and the NIR camera (InGaAs-array video camera, NIRvana 640ST, Princeton Instruments, Trenton, NJ, USA), above the mouse. An objective lens (Cosmicar, Pentax, RICOH Imaging Company, Ltd., Tokyo, Japan) and 1000 nm long-pass filter were used to exclude lights other than CNT fluorescence. The NIR camera exposure time was 100 ms.
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6

Angle-Resolved Reflectivity and Photoluminescence Measurements

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For angle-resolved reflectivity measurements, the emission of a calibrated lamp was focused onto the sample by an NIR corrected × 100 objective with 0.8 NA (Olympus LMPL100xIR). The resulting spot diameter of ∼2 μm defines the investigated area on the sample. For PL measurements, the white light source was replaced by a laser diode (OBIS, Coherent Inc., 640 nm, cw, ∼10 mW). The light reflected/emitted by the cavity was imaged onto the entrance slit of a spectrometer (Princeton Instruments IsoPlane) using a 4f Fourier imaging system and was recorded by a 640 × 512 InGaAs camera (Princeton Instruments, NIRvana:640ST). Additionally, a long-pass filter (cut-off wavelength, 850 nm) and a linear polarizer were placed in front of the spectrometer. Angle calibration of the system was done by fitting the measured cavity mode of a reference sample of known refractive index.
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7

Imaging of Single-Walled Carbon Nanotubes

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Cells were harvested during the mid-exponential growth phase (OD750nm between 1 and 1.5), pelleted by centrifugation, washed twice with 1 mM HEPES buffer (pH 7.4), and re-suspended in the same buffer to obtain an OD750nm = 0.9. Cells were fixed onto poly-L-lysine coated glass-bottom petri dishes by spotting 30 µL of the cell–SWCNT suspensions for 10 min, followed by washing with 1 mM HEPES buffer (pH 7.4). Fixed cells were treated with 50 µL LSZ–SWCNTs (concentration of 2 mg/L) and incubated at room temperature for 10 min in the dark prior to washing with 1 mM HEPES buffer (pH 7.4).
Cells were imaged using a custom-built optical setup consisting of an inverted microscope (Eclipse Ti-E, Nikon AG Instruments) with an oil-immersion TIRF Apo 100 × objective (N.A. 1.49, Nikon) coupled to a CREST X-Light spinning-disk confocal imaging system (CREST Optics) (60 µm pinholes) and an InGaAs camera (NIRvana 640 ST, Princeton Instruments). The setup has an axial resolution of 0.6 ± 0.1 μm and a lateral resolution 0.5 ± 0.1 μm. Samples were illuminated using a TriLine LaserBank system (Cairn Research) at 640 nm and 780 nm, and fluorescence was collected using either an 800 nm (Chroma) or a 980 nm long-pass filter (Semrock). Images were acquired using the Nikon NIS-Elements software (Nikon Instruments).
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