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61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532 【AXEL GLOBAL】<!--@[ss-27]@--> アズワン<!--@/[ss-27]@-->
取扱点数300万点
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AXEL GLOBALAXEL GLOBALnit">
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532 【AXEL GLOBAL】<!--@[ss-27]@--> アズワン<!--@/[ss-27]@-->
取扱点数300万点
How to use
English
China
Indonesia
Korea
Thailand
Vietnam
Contact us
すべてのカテゴリ
すべてのカテゴリ
Lab Instruments & Supplies
Factory Work Tools & Supplies
Clean Room/Anti Static Supplies
Medical, Nursing & Care Products
Food Sanitation & Inspection
Office Supplies and Stationery
Emergency Supplies
Education, Learning Supplies
Specially Ordered Item
Featured Products
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Quote
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AXEL GLOBAL
カテゴリ一覧
Lab Instruments & Supplies
Analyzer, Testing Equipment
Laser & Optical Equipment, Parts
Optical Element
Super Mirror 532nm φ30mm 等
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532
SIGMAKOKI CO., LTD.
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532
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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: φ30mm
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.
61-6949-94
Model No.Model No. class="init">
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532 【AXEL GLOBAL】<!--@[ss-27]@--> アズワン<!--@/[ss-27]@-->
取扱点数300万点
How to use
English
China
Indonesia
Korea
Thailand
Vietnam
Contact us
すべてのカテゴリ
すべてのカテゴリ
Lab Instruments & Supplies
Factory Work Tools & Supplies
Clean Room/Anti Static Supplies
Medical, Nursing & Care Products
Food Sanitation & Inspection
Office Supplies and Stationery
Emergency Supplies
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Specially Ordered Item
Featured Products
Contact us
Quote
Other Requests
AXEL GLOBAL
カテゴリ一覧
Lab Instruments & Supplies
Analyzer, Testing Equipment
Laser & Optical Equipment, Parts
Optical Element
Super Mirror 532nm φ30mm 等
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532
SIGMAKOKI CO., LTD.
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532
印刷
PDF
他のバリエーション
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: φ30mm
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
61-6949-94
型番
TFHSM-30C06-532
Standard price
JPY:
126,500
USD:
793.50
Excange rate 1USD= 159.42JPY
Valid price in Japan
Quantity
1piece
Stock in Japan
Supplier Stock
Quote
Other Requests
Product VariationsProduct Variations">
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532 【AXEL GLOBAL】<!--@[ss-27]@--> アズワン<!--@/[ss-27]@-->
取扱点数300万点
How to use
English
China
Indonesia
Korea
Thailand
Vietnam
Contact us
すべてのカテゴリ
すべてのカテゴリ
Lab Instruments & Supplies
Factory Work Tools & Supplies
Clean Room/Anti Static Supplies
Medical, Nursing & Care Products
Food Sanitation & Inspection
Office Supplies and Stationery
Emergency Supplies
Education, Learning Supplies
Specially Ordered Item
Featured Products
Contact us
Quote
Other Requests
AXEL GLOBAL
カテゴリ一覧
Lab Instruments & Supplies
Analyzer, Testing Equipment
Laser & Optical Equipment, Parts
Optical Element
Super Mirror 532nm φ30mm 等
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532
SIGMAKOKI CO., LTD.
61-6949-94 Super Mirror 532nm φ30mm TFHSM-30C06-532
印刷
PDF
他のバリエーション
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: φ30mm
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
61-6949-94
型番
TFHSM-30C06-532
標準価格
JPY:
126,500
USD:
793.50
Excange rate 1USD= 159.42JPY
Valid price in Japan
入り数
1piece
在庫数
サプライヤ在庫
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その他のお問い合わせ
商品のバリエーション
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アズワン品番
商品名
Model No.
Quantity
Standard price
標準価格(ドル)
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
