61-6949-93 Super Mirror 532nm φ25.4mm TFHSM-25.4C06-532
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: φ25.4mm
- Thickness t: 6mm
- 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 | 61-6949-93 | |
|---|---|---|
| 型番 | TFHSM-25.4C06-532 | |
| 標準価格 |
JPY: 104,500
USD: 655.50
Excange rate 1USD= 159.42JPY
Valid price in Japan |
|
| 入り数 | 1piece | |
| 在庫数 |
|
|
| Supplier Stock |
|
|
Product VariationsASONEs="init">
61-6949-93 Super Mirror 532nm φ25.4mm TFHSM-25.4C06-532 【AXEL GLOBAL】 アズワン
Contact us
SIGMAKOKI CO., LTD.
61-6949-93 Super Mirror 532nm φ25.4mm TFHSM-25.4C06-532
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: 532nm
- Outer diameter φD: φ25.4mm
- Thickness t: 6mm
- 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
-
Order No.
61-6949-93
Model No.
TFHSM-25.4C06-532
Standard price
JPY: 104,500
USD: 655.50
Excange rate 1USD= 159.42JPY
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: 621.00


61-6949-92
Super Mirror 532nm φ25mm TFHSM-25C06-532
TFHSM-25C06-532
1piece
JPY: 104,500
USD: 655.50


61-6949-93
Super Mirror 532nm φ25.4mm TFHSM-25.4C06-532
TFHSM-25.4C06-532
1piece
JPY: 104,500
USD: 655.50


61-6949-94
Super Mirror 532nm φ30mm TFHSM-30C06-532
TFHSM-30C06-532
1piece
JPY: 126,500
USD: 793.50


61-6949-95
Super Mirror 532nm φ50mm TFHSM-50C08-532
TFHSM-50C08-532
1piece
JPY: 159,500
USD: 1,000.50


61-6949-96
Super Mirror 1064nm φ12.7mm TFHSM-12.7C06-1064
TFHSM-12.7C06-1064
1piece
JPY: 102,300
USD: 641.70


61-6949-97
Super Mirror 1064nm φ25mm TFHSM-25C06-1064
TFHSM-25C06-1064
1piece
JPY: 107,800
USD: 676.20


61-6949-98
Super Mirror 1064nm φ25.4mm TFHSM-25.4C06-1064
TFHSM-25.4C06-1064
1piece
JPY: 107,800
USD: 676.20


61-6949-99
Super Mirror 1064nm φ30mm TFHSM-30C06-1064
TFHSM-30C06-1064
1piece
JPY: 129,800
USD: 814.20


61-6950-01
Super Mirror 1064nm φ50mm TFHSM-50C08-1064
TFHSM-50C08-1064
1piece
JPY: 162,800
USD: 1,021.20

61-6949-93 Super Mirror 532nm φ25.4mm TFHSM-25.4C06-532
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: 532nm
- Outer diameter φD: φ25.4mm
- Thickness t: 6mm
- 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
| Order No. | 61-6949-93 | |
|---|---|---|
| Model No. | TFHSM-25.4C06-532 | |
| Standard price |
JPY: 104,500
USD: 655.50
Excange rate 1USD= 159.42JPY
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: 621.00 |
|
|
![]() |
61-6949-92 | Super Mirror 532nm φ25mm TFHSM-25C06-532 | TFHSM-25C06-532 | 1piece | JPY: 104,500 | USD: 655.50 |
|
|
![]() |
61-6949-93 | Super Mirror 532nm φ25.4mm TFHSM-25.4C06-532 | TFHSM-25.4C06-532 | 1piece | JPY: 104,500 | USD: 655.50 |
|
|
![]() |
61-6949-94 | Super Mirror 532nm φ30mm TFHSM-30C06-532 | TFHSM-30C06-532 | 1piece | JPY: 126,500 | USD: 793.50 |
|
|
![]() |
61-6949-95 | Super Mirror 532nm φ50mm TFHSM-50C08-532 | TFHSM-50C08-532 | 1piece | JPY: 159,500 | USD: 1,000.50 |
|
|
![]() |
61-6949-96 | Super Mirror 1064nm φ12.7mm TFHSM-12.7C06-1064 | TFHSM-12.7C06-1064 | 1piece | JPY: 102,300 | USD: 641.70 |
|
|
![]() |
61-6949-97 | Super Mirror 1064nm φ25mm TFHSM-25C06-1064 | TFHSM-25C06-1064 | 1piece | JPY: 107,800 | USD: 676.20 |
|
|
![]() |
61-6949-98 | Super Mirror 1064nm φ25.4mm TFHSM-25.4C06-1064 | TFHSM-25.4C06-1064 | 1piece | JPY: 107,800 | USD: 676.20 |
|
|
![]() |
61-6949-99 | Super Mirror 1064nm φ30mm TFHSM-30C06-1064 | TFHSM-30C06-1064 | 1piece | JPY: 129,800 | USD: 814.20 |
|
|
![]() |
61-6950-01 | Super Mirror 1064nm φ50mm TFHSM-50C08-1064 | TFHSM-50C08-1064 | 1piece | JPY: 162,800 | USD: 1,021.20 |
|



