61-6884-60 ［Discontinued］High Power Polarizing Beamsplitter 1064nm 10mm PBSHP-10-10640
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［Discontinued］High Power Polarizing Beamsplitter 1064nm 10mm PBSHP-10-10640 61-6884-60 【AXEL GLOBAL】<!--@[ss-27]@--> アズワン<!--@/[ss-27]@-->
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SIGMAKOKI CO., LTD.
61-6884-60 ［Discontinued］High Power Polarizing Beamsplitter 1064nm 10mm PBSHP-10-10640
特徴
- Polarization beam splitter designed for pulsed laser such as YAG laser.
- Since the adhesive is not used on the surface of the prism, it is joined by optical contact, it can withstand high-power laser.
- By transmitting P-polarized light and reflecting S-polarized light, the polarization state of the incident light can be divided into orthogonal components.
- Since a dielectric multilayer film is used for coating, light loss is small and polarization separation can be achieved efficiently.
- Since it is a cube type, the optical axis of the emitted light will not be translated if the beam is incident perpendicularly.
- Also, even if a beam of the same size as the effective diameter is injected, the transmitted or reflected light will not be lost or reduced.
- A Grantomson Prism (GTPC) with a high extinction ratio is also available.
- * The characteristics of transmittance and extinction ratio may change if light enters from the prism side which is not marked with ○.
- * Before use, make sure that the energy density of the incident laser beam does not exceed the laser capacity.
- * If the laser beam is narrowly narrowed by a lens or concave reflection, the energy density may exceed the laser capacity of the device and the device may be damaged.
- * The extinction ratio of reflected light is slightly lower than that of transmitted light. (Approx. 3/100)
- * Transmittance and extinction ratio will be poor when using at wavelengths other than the applicable wavelength.
- * Wavelength dispersion occurs in transmitted and reflected light due to the refractive index of the material and the thickness of the glass. In addition, chromatic aberration and spherical aberration may occur when a converging or diverging beam is injected.
Spec
- [
common specification]
- Material: BK7 synthetic quartz
- Base material surface accuracy: λ/4
- Transmitted beam polarization angle: ＜10′
- Coating: Slope dielectric multi-layered film, Side 4 surfaces reflective prevention film
- Incident angle: 0°
- P-polarized light transmittance: ＞97%
- Transmission extinction ratio: Ts: Tp＝1: 200
- Scratch - dig: 20-10
- Effective range: Circle inscribed to 85% of outer dimensions of square
- [Individual specification]
- Adaptive wavelength: 1064nm
- A＝B＝C: 10mm
- Material: BK7
- S polarized light reflective ratio: ＞97％
- Laser durability *: 7J/cm2
- *Laser pulse width 10ns, Repeat frequency 20Hz
- RoHS conform product
-
Order No.
61-6884-60
Model No.
PBSHP-10-10640
Standard price
JPY: 53,200
USD: 333.48
Excange rate 1USD= 159.53JPY
Valid price in Japan
Quantity
1piece
Stock in Japan
-
Product Variations (Different Sizes, Specifications, Optional Products, etc.)
商品イメージ
アズワン品番
商品名
型番
入り数
標準価格
標準価格(ドル)
アズワン在庫
[サプライヤ在庫]
61-6884-52
High Power Polarizing Beamsplitter 355nm 10mm PBSHP-10-3550
PBSHP-10-3550
1piece
JPY: 63,700
USD: 399.30
61-6884-53
High Power Polarizing Beamsplitter 355nm 12.7mm PBSHP-12.7-3550
PBSHP-12.7-3550
1piece
JPY: 63,700
USD: 399.30
61-6884-54
High Power Polarizing Beamsplitter 355nm 15mm PBSHP-15-3550
PBSHP-15-3550
1piece
JPY: 71,000
USD: 445.06
61-6884-55
High Power Polarizing Beamsplitter 355nm 20mm PBSHP-20-3550
PBSHP-20-3550
1piece
JPY: 91,900
USD: 576.07
61-6884-56
［Discontinued］High Power Polarizing Beamsplitter 532nm 10mm PBSHP-10-5320
PBSHP-10-5320
1piece
JPY: 53,200
USD: 333.48
-
61-6884-57
［Discontinued］High Power Polarizing Beamsplitter 532nm 12.7mm PBSHP-12.7-5320
PBSHP-12.7-5320
1piece
JPY: 53,200
USD: 333.48
-
61-6884-58
［Discontinued］High Power Polarizing Beamsplitter 532nm 15mm PBSHP-15-5320
PBSHP-15-5320
1piece
JPY: 59,850
USD: 375.17
-
61-6884-59
［Discontinued］High Power Polarizing Beamsplitter 532nm 20mm PBSHP-20-5320
PBSHP-20-5320
1piece
JPY: 78,850
USD: 494.26
-
61-6884-60
［Discontinued］High Power Polarizing Beamsplitter 1064nm 10mm PBSHP-10-10640
PBSHP-10-10640
1piece
JPY: 53,200
USD: 333.48
-
61-6884-61
［Discontinued］High Power Polarizing Beamsplitter 1064nm 12.7mm PBSHP-12.7-10640
PBSHP-12.7-10640
1piece
JPY: 53,200
USD: 333.48
-
61-6884-62
［Discontinued］High Power Polarizing Beamsplitter 1064nm 15mm PBSHP-15-10640
PBSHP-15-10640
1piece
JPY: 59,850
USD: 375.17
-
61-6884-63
［Discontinued］High Power Polarizing Beamsplitter 1064nm 20mm PBSHP-20-10640
PBSHP-20-10640
1piece
JPY: 78,850
USD: 494.26
-
関連商品
61-6884-60 ［Discontinued］High Power Polarizing Beamsplitter 1064nm 10mm PBSHP-10-10640
特徴
- Polarization beam splitter designed for pulsed laser such as YAG laser.
- Since the adhesive is not used on the surface of the prism, it is joined by optical contact, it can withstand high-power laser.
- By transmitting P-polarized light and reflecting S-polarized light, the polarization state of the incident light can be divided into orthogonal components.
- Since a dielectric multilayer film is used for coating, light loss is small and polarization separation can be achieved efficiently.
- Since it is a cube type, the optical axis of the emitted light will not be translated if the beam is incident perpendicularly.
- Also, even if a beam of the same size as the effective diameter is injected, the transmitted or reflected light will not be lost or reduced.
- A Grantomson Prism (GTPC) with a high extinction ratio is also available.
- * The characteristics of transmittance and extinction ratio may change if light enters from the prism side which is not marked with ○.
- * Before use, make sure that the energy density of the incident laser beam does not exceed the laser capacity.
- * If the laser beam is narrowly narrowed by a lens or concave reflection, the energy density may exceed the laser capacity of the device and the device may be damaged.
- * The extinction ratio of reflected light is slightly lower than that of transmitted light. (Approx. 3/100)
- * Transmittance and extinction ratio will be poor when using at wavelengths other than the applicable wavelength.
- * Wavelength dispersion occurs in transmitted and reflected light due to the refractive index of the material and the thickness of the glass. In addition, chromatic aberration and spherical aberration may occur when a converging or diverging beam is injected.
Spec
- [
common specification] - Material: BK7 synthetic quartz
- Base material surface accuracy: λ/4
- Transmitted beam polarization angle: ＜10′
- Coating: Slope dielectric multi-layered film, Side 4 surfaces reflective prevention film
- Incident angle: 0°
- P-polarized light transmittance: ＞97%
- Transmission extinction ratio: Ts: Tp＝1: 200
- Scratch - dig: 20-10
- Effective range: Circle inscribed to 85% of outer dimensions of square
- [Individual specification]
- Adaptive wavelength: 1064nm
- A＝B＝C: 10mm
- Material: BK7
- S polarized light reflective ratio: ＞97％
- Laser durability *: 7J/cm2
- *Laser pulse width 10ns, Repeat frequency 20Hz
- RoHS conform product
| Order No. | 61-6884-60 | |
|---|---|---|
| Model No. | PBSHP-10-10640 | |
| Standard price |
JPY: 53,200
USD: 333.48
Excange rate 1USD= 159.53JPY
Valid price in Japan |
|
| Quantity | 1piece | |
|
|
||
| Stock in Japan | - | |
Product Variations (Different Sizes, Specifications, Optional Products, etc.)
| 商品イメージ | アズワン品番 | 商品名 | 型番 | 入り数 | 標準価格 | 標準価格(ドル) | アズワン在庫 [サプライヤ在庫] |
|
|---|---|---|---|---|---|---|---|---|
|
61-6884-52 | High Power Polarizing Beamsplitter 355nm 10mm PBSHP-10-3550 | PBSHP-10-3550 | 1piece | JPY: 63,700 | USD: 399.30 |
|
|
|
61-6884-53 | High Power Polarizing Beamsplitter 355nm 12.7mm PBSHP-12.7-3550 | PBSHP-12.7-3550 | 1piece | JPY: 63,700 | USD: 399.30 |
|
|
|
61-6884-54 | High Power Polarizing Beamsplitter 355nm 15mm PBSHP-15-3550 | PBSHP-15-3550 | 1piece | JPY: 71,000 | USD: 445.06 |
|
|
|
61-6884-55 | High Power Polarizing Beamsplitter 355nm 20mm PBSHP-20-3550 | PBSHP-20-3550 | 1piece | JPY: 91,900 | USD: 576.07 |
|
|
|
61-6884-56 | ［Discontinued］High Power Polarizing Beamsplitter 532nm 10mm PBSHP-10-5320 | PBSHP-10-5320 | 1piece | JPY: 53,200 | USD: 333.48 |
-
|
|
|
61-6884-57 | ［Discontinued］High Power Polarizing Beamsplitter 532nm 12.7mm PBSHP-12.7-5320 | PBSHP-12.7-5320 | 1piece | JPY: 53,200 | USD: 333.48 |
-
|
|
|
61-6884-58 | ［Discontinued］High Power Polarizing Beamsplitter 532nm 15mm PBSHP-15-5320 | PBSHP-15-5320 | 1piece | JPY: 59,850 | USD: 375.17 |
-
|
|
|
61-6884-59 | ［Discontinued］High Power Polarizing Beamsplitter 532nm 20mm PBSHP-20-5320 | PBSHP-20-5320 | 1piece | JPY: 78,850 | USD: 494.26 |
-
|
|
|
61-6884-60 | ［Discontinued］High Power Polarizing Beamsplitter 1064nm 10mm PBSHP-10-10640 | PBSHP-10-10640 | 1piece | JPY: 53,200 | USD: 333.48 |
-
|
|
|
61-6884-61 | ［Discontinued］High Power Polarizing Beamsplitter 1064nm 12.7mm PBSHP-12.7-10640 | PBSHP-12.7-10640 | 1piece | JPY: 53,200 | USD: 333.48 |
-
|
|
|
61-6884-62 | ［Discontinued］High Power Polarizing Beamsplitter 1064nm 15mm PBSHP-15-10640 | PBSHP-15-10640 | 1piece | JPY: 59,850 | USD: 375.17 |
-
|
|
|
61-6884-63 | ［Discontinued］High Power Polarizing Beamsplitter 1064nm 20mm PBSHP-20-10640 | PBSHP-20-10640 | 1piece | JPY: 78,850 | USD: 494.26 |
-
|
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