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365 nm pulsed nitrogen laser

Manufactured by Spectra-Physics

The 365-nm pulsed nitrogen laser is a compact and reliable laser source that generates ultraviolet pulses at a wavelength of 365 nanometers. It is designed for a wide range of scientific and industrial applications that require a stable and consistent UV light source.

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6 protocols using 365 nm pulsed nitrogen laser

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

Immunostaining for DNA Damage Foci

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For immunostaining, cells were grown on coverslips and irradiated via the 365-nm pulsed nitrogen laser (Spectra-Physics) or 8 Gy of IR. For the cells irradiated with the laser, the coverslip was placed in a dark box and the cells were allowed to recover at 37°C for 30 min. The cells were subsequently washed with ice cold PBS three times and then fixed via incubation with 4% paraformaldehyde at room temperature for 20 min. The cells were permeablized with PBS containing 0.5% Triton X-100 on ice for 10 min, blocked with PBS containing 5% normal goat serum overnight at 4°C and then incubated with the primary antibodies at room temperature for 1 h. After washing with cold PBS, cells were incubated with the second antibodies conjugated with Alexa 488 (Invitrogen, A11001) or Texas red (Invitrogen, T2767). Following IR with 8 Gy, focus formation of RPA and Rad51 was detected using fluorescent immunostaining at various time points as described in the figure legends and as previously described (30 (link)).
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4

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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5

Live Cell Imaging and Laser Micro-Irradiation

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Live cell imaging combined with laser micro-irradiation was performed as previously described (6 (link),7 (link)). Fluorescence was monitored via an Axiovert 200 M microscope (Carl Zeiss, Inc.), with a Plan-Apochromat 63×/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 five 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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6

Laser-Induced DNA Double-Strand Breaks

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A 365‐nm pulsed nitrogen laser (Spectra‐Physics) was applied to generate DSBs in a defined area of the nucleus in cells. At 30 minutes after laser radiation, cells were fixed and subjected to immunofluorescence.
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