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Plan apochromat 63x na 1.40 oil immersion objective

Manufactured by Zeiss

The Plan-Apochromat 63X/NA 1.40 oil immersion objective is a high-performance microscope lens manufactured by Zeiss. It provides a magnification of 63X and a numerical aperture of 1.40, which enables high-resolution imaging. The objective is designed for use with oil immersion technique to achieve optimal optical performance.

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3 protocols using plan apochromat 63x na 1.40 oil immersion objective

1

Real-Time Recruitment of DNA Repair Factors

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GFP-NBS1, GFP-EXO1, GFP-Ku70, GFP-XLF, or GFP-XRCC4 were transfected into HCT116 DNA-PKcs +/+, −/−, or KD/− cells with JetPrime® (Polyplus) following the manufacturer's instructions. Twenty-four hours after the transfection laser micro-irradiation and real-time recruitment was performed with a Carl Zeiss Axiovert 200M microscope with a Plan-Apochromat 63X/NA 1.40 oil immersion objective (Carl Zeiss) as previously described (28 (link)). DSBs were generated with a 365-nm pulsed nitrogen laser (Spectra-Physics), which was directly coupled to the epifluorescence path of the microscope (28 (link)). Time-lapse images were taken via a Carl Zeiss AxioCam HRm camera. The cells were maintained in a CO2-independent medium (Invitrogen) at 37°C during micro-irradiation and time-lapse imaging. Fluorescence intensities of the micro-irradiated area and control area were determined by Carl Zeiss Axiovision software, v4.5, and the intensity of irradiated was normalized to non-irradiated control area as previously described (26 (link)).
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2

Laser Micro-Irradiation for Live-Cell Imaging

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Live cell imaging combined with laser micro-irradiation was performed as described previously. Fluorescence signal of YFP-DNA-PKcs was monitored by using an Axiovert 200M microscope (Carl Zeiss, Inc), with a Plan-Apochromat 63X/NA 1.40 oil immersion objective (Carl Zeiss, Inc) [20 (link)]. A 365-nm pulsed nitrogen laser (Spectra Physics) was directly coupled to the epifluorescence path of the microscope and used to generate DSBs in a defined area of the nucleus. Analysis of acquired images was done as previously described [34 (link)]. Briefly, fluorescence intensity (IN) of each time point was based on pre-laser background intensity using the formula: IN(t) = Idt/Ibt×IbpreIR [Idt: the difference between the accumulation spot intensity and the undamaged site background intensity of each time point; Ibt: the background intensity of each time point; IbpreIR: the background intensity before irradiation. Relative fluorescence intensity (RF) was calculated using the formula: RF(t) = (INt−INpreIR)/(INmax−INpreIR) [INpreIR: IN of the micro-irradiated area before laser damage; INmax: the maximum IN in the micro-irradiated area of all time points]. Each data point is the average of 10 independent measurements.
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3

Live-Cell Imaging and Laser Micro-Irradiation

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Live cell imaging combined with laser micro-irradiation was carried out as previously described (11 (link),29 (link)). Fluorescence was monitored via an Axiovert 200 M microscope (Carl Zeiss, Inc.), with a Plan-Apochromat 63X/NA 1.40 oil immersion objective (Carl Zeiss, Inc.). A 365-nm pulsed nitrogen laser (Spectra-Physics) was directly coupled to the epifluorescence path of the microscope and used to generate DSBs in a defined area of the nucleus. For quantitative analyses, the same amount of DNA damage was generated under standardized micro-irradiation conditions (minimal laser output of 75% for 5 pulses) in each experiment. Time-lapse images were taken with an AxioCamHRm camera. The fluorescence intensities of micro-irradiated and non-irradiated areas within the cell nucleus were determined using the AxioVision Software, version 4.8 (Carl Zeiss, Inc.). Each data point is the average of 10 independent measurements.
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