SIGMAKOKI CO., LTD.

61-6949-95 Super Mirror 532nm φ50mm TFHSM-50C08-532

特徴

  • 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.

仕様

  • [ 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: 532nm
  • Outer diameter φD: φ50mm
  • Thickness t: 8mm
  • Reflective ratio: 99.995% (Even though the reflective rate is measured using CRD, it can vary depending on the measuring method and measurement conditions. )
  • Loss: 20ppm (This value wave is reference data. Data will not be attached to the product. )
  • RoHS conform product
  •  
アズワン品番 61-6949-95
型番 TFHSM-50C08-532
標準価格 JPY: 159,500 USD: 992.41
Excange rate 1USD= 160.72JPY
Valid price in Japan
入り数 1piece
在庫数
サプライヤ在庫

商品のバリエーション (Different Sizes, Specifications, Optional Products, etc.)

Product image Order No. 商品名 型番 Quantity 標準価格 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: 615.98

61-6949-92 Super Mirror 532nm φ25mm TFHSM-25C06-532 TFHSM-25C06-532 1piece JPY: 104,500 USD: 650.20

61-6949-93 Super Mirror 532nm φ25.4mm TFHSM-25.4C06-532 TFHSM-25.4C06-532 1piece JPY: 104,500 USD: 650.20

61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532 TFHSM-30C06-532 1piece JPY: 126,500 USD: 787.08

61-6949-95 Super Mirror 532nm φ50mm TFHSM-50C08-532 TFHSM-50C08-532 1piece JPY: 159,500 USD: 992.41

61-6949-96 Super Mirror 1064nm φ12.7mm TFHSM-12.7C06-1064 TFHSM-12.7C06-1064 1piece JPY: 102,300 USD: 636.51

61-6949-97 Super Mirror 1064nm φ25mm TFHSM-25C06-1064 TFHSM-25C06-1064 1piece JPY: 107,800 USD: 670.73

61-6949-98 Super Mirror 1064nm φ25.4mm TFHSM-25.4C06-1064 TFHSM-25.4C06-1064 1piece JPY: 107,800 USD: 670.73

61-6949-99 Super Mirror 1064nm φ30mm TFHSM-30C06-1064 TFHSM-30C06-1064 1piece JPY: 129,800 USD: 807.62

61-6950-01 Super Mirror 1064nm φ50mm TFHSM-50C08-1064 TFHSM-50C08-1064 1piece JPY: 162,800 USD: 1,012.94