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Dichroic mirror

Manufactured by Chroma Technology
Sourced in Germany, Japan

A dichroic mirror is an optical device that selectively reflects or transmits certain wavelengths of light while allowing other wavelengths to pass through. It is a type of interference filter that is designed to reflect one set of wavelengths and transmit another set, based on the specific design and coating of the mirror.

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6 protocols using dichroic mirror

1

Visualizing Polystyrene Bead Rotation

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The rotation of a polystyrene bead attaching to the γ-subunit was visualized under an inverted microscope (Ti-E; Nikon) equipped with 100× objective lens (Apo TIRF N.A. 1.49; Nikon), a condenser unit (LWD0.52; Nikon), LED (pE-100 660 nm; CoolLed), IR laser (YLM-2-1064-LP; IPG), an optical bench (RS2000TM; Newport), and three CCDs (CCD1 in Fig. 1A, CS8430i; Toshiba Teli, CCD2, Luca; Andor, and high-speed CCD3, LRH20000B; DigiMo). CCD2 and CCD3 were synchronized with TTL signal to identify the moment when optical trapping was turned on with a custom modification in CCD3. Dichroic mirrors, DM1 and DM2 in Fig. 1A, were custom made (Chroma Technology) and purchased (Asahi Spectra), respectively. A highly-stable customized sample-stage (Chukousha) was adjusted three actuators (SGSP-13ACTR; Sigma Koki). The optical system for 3-D tracking system was described previously14 (link),36 ; the calibration factor to determine z-position from Δx was set as 1 in all measurements. Most apparatuses except PCs and displays were compartmented in a custom-made thermostatic chamber (Nihon Freezer), and all operations were done from the outside of the chamber. The Measurements were done at 23 ± 0.2 °C. speed of camera was set as 30 and 500 f.p.s. for low and high-load, respectively.
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2

Live Tracking of Calcium Signaling

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Arabidopsis seedlings were grown vertically in 1/2MS solid medium for 7 d. Samples were then gently mounted on a perfusion chamber and stabilized with cotton wool soaked in 200 μl of imaging buffer (10 mM MES Tris base; 1 mM CaCl2; 5 mM KCl pH 5.8); an ISMATEC pump was used to administrate stimuli in continuous, setting the flow rate at 3 ml/min; each stimulus was added into the imaging buffer. The seedlings were kept under continuous perfusion. For Cameleon (Krebs and Schumacher 2013 (link)) analysis, the FRET CyanoFP/YellowFP (CFP/YFP) optical block A11400-03 (Emission 1, 483/32 nm for CFP and Emission 2 542/27 nm for the FRET) with a dichroic 510 nm mirror (Hamamatsu Photonics, Shizuoka, Giappone) was used for the simultaneous CFP and FRET acquisitions (cpVenus for YC3.6 and YC4.6). Images were acquired in 5-s intervals with an exposure time of 500 ms. Filters and dichroic mirrors were purchased from Chroma Technology, Olching, Germany. The NIS-Element (Nikon) was used to control the microscope, illuminator, camera, and post-acquisition analyses, as previously reported (Giovanna Loro et al. 2016 (link)). FRET efficiency values were calculated as previously described (Loro et al. 2013 (link)).
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3

Visualizing GLUT3 Transporter Dynamics

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Cells expressing GLUT3-EGFP were visualised with an objective-based total internal reflection fluorescence (TIRF) microscope. A 473-nm solid-state diode laser was focused onto a single-mode optical fibre and transmitted via the rear illumination port of an Olympus IX71 inverted microscope. Laser light was reflected on a dichroic mirror (Chroma Technology), passed through a high numerical aperture objective (x 60, NA 1.49, oil immersion, Olympus) and was totally internally reflected at the glass-water interface. Under these experimental conditions, fluorescent objects were observed at the evanescent field (180 nm of the glass-water interface under our experimental conditions). Treatments were performed with 10 mM MβCD for 15 minutes and with 30 µg/ml SyntheChol for 20 minutes.
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4

Two-Photon Microscopy for Axial Imaging

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Samples were measured on a home-built two-photon microscope based on an Axiovert 200 microscope (Zeiss, Thornwood, NY) interfaced with a Ti:Sapphire laser (Tsunami, Spectra Physics, Mountain View, CA) with an excitation wavelength of 1000 nm and a power of ~1 mW. The fluorescence was collected with a 63x C-Apochromat water immersion objective lens (NA = 1.2, Zeiss) and registered by a photodetector (HPM-100-40, Becker & Hickl, Berlin, Germany) connected to a photon counting acquisition card (ISS, Champaign, IL), which recorded data with a frequency of 20 kHz. A dichroic mirror (Chroma Technology, Rockingham, VT) served to separate excitation and emission light. The z-scan was performed by moving the stage (PZ2000 piezo stage, ASI, Eugene, OR) along the direction of the beam path [6 (link)]. The stage was driven by a voltage signal from an arbitrary waveform generator (33250A, Agilient Technologies, Santa Clara, CA). The signal waveform was a linear ramp function with a frequency of 0.1 Hz and a peak-to-peak amplitude of 0.8 V, which corresponds to 8.04 μm of axial travel. The z-scan intensity profile was sampled at 20 kHz.
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5

Optical Tweezers for Microscale Manipulation

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Optical tweezers [40 (link)] were built upon an near infrared (NIR)-diode laser (Renishaw, UK), with a square beam profile (size 5 mm) operating at 830 nm ± 1 nm with an average power of 300 mW ± 30 mW. The power at the sample was about 148 mW. The wavelength of the laser (830 nm) was chosen to minimize heating and photodamage of the sample [43 (link)]. All equipment was mounted on a XYZ-translation stage (Thorlabs Inc., USA) to ensure precise alignment. The beam of the trapping laser was steered through a system of mirrors (Thorlabs Inc., USA) into the microscope oil immersion objective (100 ×, 1.4 NA, Olympus, Japan) through a dichroic mirror (Chroma Technology, USA). The intensity profile of the laser beam overfilled the back focal plane of the objective; hence no beam expansion was necessary. The optical trap, situated at the focal distance of the microscope objective, was aligned to the centre of the field-of-view of the Charge Coupled Device (CCD) camera of the microscope.
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6

Two-Photon Imaging of Olfactory Bulb

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The optical setup consists of a two-photon microscope (Ultima IV, Bruker) combined with an ultra-short pulsed laser (Mai Tai Deep See HP, Spectra-Physics-Newport) tuned to 800 nm for Fura-2 excitation. Freely programmable galvanometric mirrors allow for fast and variable scanning. All images were acquired using a 20× water-immersion objective (NA 1.0, Olympus). The fluorescence was collected in epi-configuration, separated by a dichroic mirror (Chroma Technology Corporation), filtered by a 70 nm band-pass centred at 525 nm, and detected by photomultiplier tubes (Hamamatsu Photonics). Optimal signal-to-noise ratio was achieved with laser power of ≈10 mW without any indication of photo-bleaching, even after repeated exposure. Functional data acquisition was performed scanning along a custom 1D trajectory at 50 Hz. To avoid any bias due to anatomical and functional asymmetries (Rigosi et al., 2011 (Rigosi et al., , 2015)) , all imaging experiments were conducted on the right AL.
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