SIGMAKOKI CO., LTD.

61-6949-97 Super Mirror 1064nm φ25mm TFHSM-25C06-1064

Features

  • Fabry-Perot resonators (cavities) are used to obtain the ultimate accuracy of distance and time using light.
  • In order to improve the performance of this resonator, the super mirror is an ultra-high performance mirror with the reflectivity as close as possible to 1.
  • Dense, defect-free, high-quality films have been deposited using ion beam sputtering (IBS).
  • Using a special polishing technique, we use a low scattering substrate with a surface roughness of Ra0.1nm or less.
  • We have achieved a reflective film with a reflectivity of 99.999% through our long-established film design technology.
  • The scattering loss due to the substrate and film is very small, and very narrow spectral width and high finesse can be expected when the cavity is constructed.
  • Available in 2 types with wavelengths of 532 nm and 1064 nm.
  • * When the mirror is used alone, it does not transmit due to its high reflectivity.
  • * In order to use the transmitted light, please assemble the cavity before use.
  • * Handle and measure the mirror in a clean environment.
  • * Trash, dust, and even trace amounts of gas in the air can greatly affect the measured value.
  • * If the cavity is composed of two flat mirrors, the output from the cavity may become unstable.
  • * If you are configuring a stable cavity, make sure that one or both of them are concave mirrors.

Spec

  • [ common specification]
  • Material: Synthetic quartz
  • Shape: Flat surface substrate
  • Parallelism: <5″
  • Substrate surface accuracy: λ/10
  • Coating: Surface, dielectric multi-layered high reflective coat, Back, dielectric multi-layered reflective prevention coat
  • Incident angle: 0°
  • Reflective prevention film: R<0.15%
  • Effective diameter: 80% of the outer diameter
  • Scratch - dig: 10-5
  • [Individual specification]
  • Adaptive wavelength: 1064nm
  • Outer diameter φD: φ25mm
  • Thickness t: 6mm
  • Reflective ratio: 99.999% (Even though the reflective rate is measured using CRD, it can vary depending on the measuring method and measurement conditions. )
  • Loss: 8 ppm (This value wave is reference data. Data will not be attached to the product. )
  • RoHS conform product
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Order No. 61-6949-97
Model No. TFHSM-25C06-1064
Standard price JPY: 107,800 USD: 675.74
Excange rate 1USD= 159.53JPY
Valid price in Japan
Quantity 1piece
Stock in Japan
Supplier Stock

Product Variations (Different Sizes, Specifications, Optional Products, etc.)

Product image Order No. Name Model No. Quantity Standard price Valid price in Japan Stock
[Supplier Stock]
61-6949-91 Super Mirror 532nm φ12.7mm TFHSM-12.7C06-532 TFHSM-12.7C06-532 1piece JPY: 99,000 USD: 620.57

61-6949-92 Super Mirror 532nm φ25mm TFHSM-25C06-532 TFHSM-25C06-532 1piece JPY: 104,500 USD: 655.05

61-6949-93 Super Mirror 532nm φ25.4mm TFHSM-25.4C06-532 TFHSM-25.4C06-532 1piece JPY: 104,500 USD: 655.05

61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532 TFHSM-30C06-532 1piece JPY: 126,500 USD: 792.95

61-6949-95 Super Mirror 532nm φ50mm TFHSM-50C08-532 TFHSM-50C08-532 1piece JPY: 159,500 USD: 999.81

61-6949-96 Super Mirror 1064nm φ12.7mm TFHSM-12.7C06-1064 TFHSM-12.7C06-1064 1piece JPY: 102,300 USD: 641.26

61-6949-97 Super Mirror 1064nm φ25mm TFHSM-25C06-1064 TFHSM-25C06-1064 1piece JPY: 107,800 USD: 675.74

61-6949-98 Super Mirror 1064nm φ25.4mm TFHSM-25.4C06-1064 TFHSM-25.4C06-1064 1piece JPY: 107,800 USD: 675.74

61-6949-99 Super Mirror 1064nm φ30mm TFHSM-30C06-1064 TFHSM-30C06-1064 1piece JPY: 129,800 USD: 813.64

61-6950-01 Super Mirror 1064nm φ50mm TFHSM-50C08-1064 TFHSM-50C08-1064 1piece JPY: 162,800 USD: 1,020.50