Optics

The MaxFR series filters are optimized for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi's Epsilon astrographs. These filters are specifically designed to isolate the key emission lines: OIII, H-alpha, and SII. With a full width at half maximum (FWHM) of 12nm or 6nm, they provide exceptional imaging performance for capturing deep-sky objects.

The MaxFR series filters are specifically designed for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi's Epsilon astrographs. These filters are optimized to isolate the three key emission lines: OIII, H-alpha, and SII. With a full width at half maximum (FWHM) of 12nm or 6nm, they deliver exceptional performance for capturing deep-sky objects.

The MaxFR series filters are optimized for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi's Epsilon astrographs. These filters are designed to isolate the three most important emission lines: OIII, H-alpha, and SII. With a full width at half maximum (FWHM) of 12nm or 6nm, they ensure high-quality imaging for deep-sky objects.

The MaxFR series filters are specifically optimized for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi's Epsilon astrographs. These filters are designed to enhance imaging by isolating the three key emission lines: OIII, H-alpha, and SII. With a full width at half maximum (FWHM) of 12nm or 6nm, they provide exceptional performance for capturing deep-sky objects.

The MaxFR series filters are specifically designed for astrophotography with ultra-fast telescopes, such as the Celestron RASA telescopes or Takahashi's Epsilon astrographs. These filters are optimized for capturing the three key emission lines: OIII, H-alpha, and SII, and are available with full widths at half maximum (FWHM) of either 12nm or 6nm.

The MaxFR series filters are tailored for astrophotography with ultra-fast telescopes, such as the Celestron RASA or Takahashi's Epsilon astrographs. These filters are designed to capture the three critical emission lines: OIII, H-alpha, and SII, with available full widths at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series filters are specifically designed for astrophotography with very fast telescopes, such as the Celestron RASA or Takahashi's Epsilon astrographs. These filters are optimized for capturing the three key emission lines: OIII, H-alpha, and SII, with full widths at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series filters are designed for astrophotography with very fast telescopes, such as the Celestron RASA or Takahashi's Epsilon astrographs. These filters are optimized to capture the three major emission lines: OIII, H-alpha, and SII, with full widths at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series filters are specifically optimized for astrophotography with very fast telescopes, such as the Celestron RASA or Takahashi's Epsilon astrographs. These filters are designed to capture the three critical emission lines: OIII, H-alpha, and SII, with full widths at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series filters are optimized for astrophotography with very fast telescopes, such as the Celestron RASA or Takahashi's Epsilon astrographs. These filters are designed to capture the three key emission lines: OIII, H-alpha, and SII, with full widths at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series filters are specifically optimized for astrophotography with very fast telescopes, such as the Celestron RASA or Takahashi's Epsilon astrographs. These filters are designed to capture the three essential emission lines: OIII, H-alpha, and SII, with full widths at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series filters are designed for astrophotography with very fast telescopes, such as the Celestron RASA or Takahashi's Epsilon astrographs. These filters are optimized to capture the three key emission lines: OIII, H-alpha, and SII, with full widths at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is specifically designed for astrophotography with fast telescopes, such as Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters are optimized for capturing the most important emission lines in astrophotography: OIII, H-alpha, and SII. They are available with a full width at half maximum (FWHM) of either 12nm or 6nm.

The MaxFR series of filters is tailored for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters are specifically designed to capture the three key emission lines in astrophotography: OIII, H-alpha, and SII, with options for a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is designed for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters target the three key emission lines in astrophotography: OIII, H-alpha, and SII, with options for a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is optimized for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters are designed to capture the three critical emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is specifically designed for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters are ideal for capturing the three key emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is optimized for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters are designed to capture the three key emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is specifically designed for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters are optimized to capture the three essential emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is designed for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters are optimized to capture the three key emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is specifically optimized for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi Epsilon astrographs. These filters are designed to capture the three key emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is specially designed for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi's Epsilon astrographs. These filters are optimized to capture the three critical emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is optimized for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi's Epsilon astrographs. These filters are designed to capture the three key emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.

The MaxFR series of filters is optimized for astrophotography with very fast telescopes, such as the Celestron RASA telescopes or Takahashi's Epsilon astrographs. These filters are designed to capture the three key emission lines in astrophotography: OIII, H-alpha, and SII, with a full width at half maximum (FWHM) of 12nm or 6nm.