61-6876-52 Dielectric Cube Half Mirror 400-700nm A = B = C: 50mm CSMH-50-550
Features
- A cube-type half-mirror that splits unpolarized light, such as a white light source or an LED light source, equally between transmitted and reflected light.
- Accurate branching characteristics can be obtained in wide wavelength bands of white light and LED light sources.
- Since a dielectric multilayer film is used for coating, light loss is small and light can be efficiently separated.
- Since it is a cube type, the optical axis of the emitted light will not be translated if the beam is incident vertically.
- 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. *Enter light from the prism side marked with ○.
- * Reflectivity and reflectance wavelength characteristics may differ when light is inserted from the opposite prism.
- * When using linearly polarized light such as laser light, the reflectivity and transmittance vary greatly depending on the polarization direction.
- * When adjusting the branching ratio to 1:1, tilt the polarization azimuth to 45 degrees or use circularly polarized light.
- * The phase difference of the incident light is not stored in transmitted light or reflected light.
- * Use a wave plate to compensate for the phase difference.
- * Wavelength dispersion occurs in transmitted and reflected light due to the refractive index of the material and the thickness of the glass.
SpecSpec class="init">
61-6876-52 Dielectric Cube Half Mirror 400-700nm A = B = C: 50mm CSMH-50-550 【AXEL GLOBAL】<!--@[ss-27]@--> アズワン<!--@/[ss-27]@-->
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SIGMAKOKI CO., LTD.
61-6876-52 Dielectric Cube Half Mirror 400-700nm A = B = C: 50mm CSMH-50-550
特徴
- A cube-type half-mirror that splits unpolarized light, such as a white light source or an LED light source, equally between transmitted and reflected light.
- Accurate branching characteristics can be obtained in wide wavelength bands of white light and LED light sources.
- Since a dielectric multilayer film is used for coating, light loss is small and light can be efficiently separated.
- Since it is a cube type, the optical axis of the emitted light will not be translated if the beam is incident vertically.
- 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. *Enter light from the prism side marked with ○.
- * Reflectivity and reflectance wavelength characteristics may differ when light is inserted from the opposite prism.
- * When using linearly polarized light such as laser light, the reflectivity and transmittance vary greatly depending on the polarization direction.
- * When adjusting the branching ratio to 1:1, tilt the polarization azimuth to 45 degrees or use circularly polarized light.
- * The phase difference of the incident light is not stored in transmitted light or reflected light.
- * Use a wave plate to compensate for the phase difference.
- * Wavelength dispersion occurs in transmitted and reflected light due to the refractive index of the material and the thickness of the glass.
仕様
- [
common specification]
- Material: BK7
- Base material surface accuracy: λ/4
- Transmitted beam polarization angle: ＜5′
- Coating: Slope dielectric multi-layered film, Side 4 surfaces reflective prevention film
- Incident angle: 0°
- Branching ratio (reflection: Transmission): 1: 1
- Polarization condition of the incident light: Unpolarized light, Linear polarization or circularly polarized light of the 45 degrees azimuth
- Laser durability: 0.3J/cm2 (pulse width 10ns, Repeat frequency 20Hz)
- Scratch - dig: 20-10
- Effective range: Circle inscribed to 85% of outer dimensions of square (A=B=C ≦ 7mm: Circle inscribed to 80% of outer dimensions of square)
- [Individual specification]
- Adaptive wavelength: 400 - 700nm
- A＝B＝C: 50mm
- Transmittance (average value of P polarized light and S polarized light): Average 50 ±5%
- RoHS conform product
-
Order No.
61-6876-52
Model No.
CSMH-50-550
Standard price
JPY: 86,700
USD: 539.45
Excange rate 1USD= 160.72JPY
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]
61-6876-37
Dielectric Cube Half Mirror 390-410nm A = B = C: 10mm CSMH-10-405
CSMH-10-405
1piece
JPY: 16,700
USD: 103.91
61-6876-38
Dielectric Cube Half Mirror 390-410nm A = B = C: 12.7mm CSMH-12.7-405
CSMH-12.7-405
1piece
JPY: 17,600
USD: 109.51
61-6876-39
Dielectric Cube Half Mirror 390-410nm A = B = C: 15mm CSMH-15-405
CSMH-15-405
1piece
JPY: 18,800
USD: 116.97
61-6876-40
Dielectric Cube Half Mirror 390-410nm A = B = C: 20mm CSMH-20-405
CSMH-20-405
1piece
JPY: 24,000
USD: 149.33
61-6876-41
Dielectric Cube Half Mirror 390-410nm A = B = C: 25mm CSMH-25-405
CSMH-25-405
1piece
JPY: 29,200
USD: 181.68
61-6876-42
Dielectric Cube Half Mirror 390-410nm A = B = C: 30mm CSMH-30-405
CSMH-30-405
1piece
JPY: 43,800
USD: 272.52
61-6876-43
Dielectric Cube Half Mirror 400-700nm A = B = C: 5mm CSMH-05-550
CSMH-05-550
1piece
JPY: 16,700
USD: 103.91
61-6876-44
Dielectric Cube Half Mirror 400-700nm A = B = C: 7mm CSMH-07-550
CSMH-07-550
1piece
JPY: 16,700
USD: 103.91
61-6876-45
Dielectric Cube Half Mirror 400-700nm A = B = C: 10mm CSMH-10-550
CSMH-10-550
1piece
JPY: 16,700
USD: 103.91
61-6876-46
Dielectric Cube Half Mirror 400-700nm A = B = C: 12.7mm CSMH-12.7-550
CSMH-12.7-550
1piece
JPY: 17,600
USD: 109.51
61-6876-47
Dielectric Cube Half Mirror 400-700nm A = B = C: 15mm CSMH-15-550
CSMH-15-550
1piece
JPY: 18,800
USD: 116.97
61-6876-48
Dielectric Cube Half Mirror 400-700nm A = B = C: 20mm CSMH-20-550
CSMH-20-550
1piece
JPY: 24,000
USD: 149.33
61-6876-49
Dielectric Cube Half Mirror 400-700nm A = B = C: 25mm CSMH-25-550
CSMH-25-550
1piece
JPY: 29,200
USD: 181.68
61-6876-50
Dielectric Cube Half Mirror 400-700nm A = B = C: 30mm CSMH-30-550
CSMH-30-550
1piece
JPY: 43,800
USD: 272.52
61-6876-51
Dielectric Cube Half Mirror 400-700nm A = B = C: 40mm CSMH-40-550
CSMH-40-550
1piece
JPY: 61,600
USD: 383.28
61-6876-52
Dielectric Cube Half Mirror 400-700nm A = B = C: 50mm CSMH-50-550
CSMH-50-550
1piece
JPY: 86,700
USD: 539.45
61-6876-53
Dielectric Cube Half Mirror 750-850nm A = B = C: 10mm CSMH-10-800
CSMH-10-800
1piece
JPY: 16,700
USD: 103.91
61-6876-54
Dielectric Cube Half Mirror 750-850nm A = B = C: 12.7mm CSMH-12.7-800
CSMH-12.7-800
1piece
JPY: 17,600
USD: 109.51
61-6876-55
Dielectric Cube Half Mirror 750-850nm A = B = C: 15mm CSMH-15-800
CSMH-15-800
1piece
JPY: 18,800
USD: 116.97
61-6876-56
Dielectric Cube Half Mirror 750-850nm A = B = C: 20mm CSMH-20-800
CSMH-20-800
1piece
JPY: 24,000
USD: 149.33
61-6876-57
Dielectric Cube Half Mirror 750-850nm A = B = C: 25mm CSMH-25-800
CSMH-25-800
1piece
JPY: 29,200
USD: 181.68
61-6876-58
Dielectric Cube Half Mirror 750-850nm A = B = C: 30mm CSMH-30-800
CSMH-30-800
1piece
JPY: 43,800
USD: 272.52
61-6876-59
Dielectric Cube Half Mirror 1300-1550nm A = B = C: 10mm CSMH-10-1400
CSMH-10-1400
1piece
JPY: 16,700
USD: 103.91
61-6876-60
Dielectric Cube Half Mirror 1300-1550nm A = B = C: 12.7mm CSMH-12.7-1400
CSMH-12.7-1400
1piece
JPY: 17,600
USD: 109.51
61-6876-61
Dielectric Cube Half Mirror 1300-1550nm A = B = C: 20mm CSMH-20-1400
CSMH-20-1400
1piece
JPY: 24,000
USD: 149.33
61-6876-52 Dielectric Cube Half Mirror 400-700nm A = B = C: 50mm CSMH-50-550
特徴
- A cube-type half-mirror that splits unpolarized light, such as a white light source or an LED light source, equally between transmitted and reflected light.
- Accurate branching characteristics can be obtained in wide wavelength bands of white light and LED light sources.
- Since a dielectric multilayer film is used for coating, light loss is small and light can be efficiently separated.
- Since it is a cube type, the optical axis of the emitted light will not be translated if the beam is incident vertically.
- 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. *Enter light from the prism side marked with ○.
- * Reflectivity and reflectance wavelength characteristics may differ when light is inserted from the opposite prism.
- * When using linearly polarized light such as laser light, the reflectivity and transmittance vary greatly depending on the polarization direction.
- * When adjusting the branching ratio to 1:1, tilt the polarization azimuth to 45 degrees or use circularly polarized light.
- * The phase difference of the incident light is not stored in transmitted light or reflected light.
- * Use a wave plate to compensate for the phase difference.
- * Wavelength dispersion occurs in transmitted and reflected light due to the refractive index of the material and the thickness of the glass.
仕様
- [
common specification] - Material: BK7
- Base material surface accuracy: λ/4
- Transmitted beam polarization angle: ＜5′
- Coating: Slope dielectric multi-layered film, Side 4 surfaces reflective prevention film
- Incident angle: 0°
- Branching ratio (reflection: Transmission): 1: 1
- Polarization condition of the incident light: Unpolarized light, Linear polarization or circularly polarized light of the 45 degrees azimuth
- Laser durability: 0.3J/cm2 (pulse width 10ns, Repeat frequency 20Hz)
- Scratch - dig: 20-10
- Effective range: Circle inscribed to 85% of outer dimensions of square (A=B=C ≦ 7mm: Circle inscribed to 80% of outer dimensions of square)
- [Individual specification]
- Adaptive wavelength: 400 - 700nm
- A＝B＝C: 50mm
- Transmittance (average value of P polarized light and S polarized light): Average 50 ±5%
- RoHS conform product
| Order No. | 61-6876-52 | |
|---|---|---|
| Model No. | CSMH-50-550 | |
| Standard price |
JPY: 86,700
USD: 539.45
Excange rate 1USD= 160.72JPY
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] |
|
|---|---|---|---|---|---|---|---|---|
|
61-6876-37 | Dielectric Cube Half Mirror 390-410nm A = B = C: 10mm CSMH-10-405 | CSMH-10-405 | 1piece | JPY: 16,700 | USD: 103.91 |
|
|
|
61-6876-38 | Dielectric Cube Half Mirror 390-410nm A = B = C: 12.7mm CSMH-12.7-405 | CSMH-12.7-405 | 1piece | JPY: 17,600 | USD: 109.51 |
|
|
|
61-6876-39 | Dielectric Cube Half Mirror 390-410nm A = B = C: 15mm CSMH-15-405 | CSMH-15-405 | 1piece | JPY: 18,800 | USD: 116.97 |
|
|
|
61-6876-40 | Dielectric Cube Half Mirror 390-410nm A = B = C: 20mm CSMH-20-405 | CSMH-20-405 | 1piece | JPY: 24,000 | USD: 149.33 |
|
|
|
61-6876-41 | Dielectric Cube Half Mirror 390-410nm A = B = C: 25mm CSMH-25-405 | CSMH-25-405 | 1piece | JPY: 29,200 | USD: 181.68 |
|
|
|
61-6876-42 | Dielectric Cube Half Mirror 390-410nm A = B = C: 30mm CSMH-30-405 | CSMH-30-405 | 1piece | JPY: 43,800 | USD: 272.52 |
|
|
|
61-6876-43 | Dielectric Cube Half Mirror 400-700nm A = B = C: 5mm CSMH-05-550 | CSMH-05-550 | 1piece | JPY: 16,700 | USD: 103.91 |
|
|
|
61-6876-44 | Dielectric Cube Half Mirror 400-700nm A = B = C: 7mm CSMH-07-550 | CSMH-07-550 | 1piece | JPY: 16,700 | USD: 103.91 |
|
|
|
61-6876-45 | Dielectric Cube Half Mirror 400-700nm A = B = C: 10mm CSMH-10-550 | CSMH-10-550 | 1piece | JPY: 16,700 | USD: 103.91 |
|
|
|
61-6876-46 | Dielectric Cube Half Mirror 400-700nm A = B = C: 12.7mm CSMH-12.7-550 | CSMH-12.7-550 | 1piece | JPY: 17,600 | USD: 109.51 |
|
|
|
61-6876-47 | Dielectric Cube Half Mirror 400-700nm A = B = C: 15mm CSMH-15-550 | CSMH-15-550 | 1piece | JPY: 18,800 | USD: 116.97 |
|
|
|
61-6876-48 | Dielectric Cube Half Mirror 400-700nm A = B = C: 20mm CSMH-20-550 | CSMH-20-550 | 1piece | JPY: 24,000 | USD: 149.33 |
|
|
|
61-6876-49 | Dielectric Cube Half Mirror 400-700nm A = B = C: 25mm CSMH-25-550 | CSMH-25-550 | 1piece | JPY: 29,200 | USD: 181.68 |
|
|
|
61-6876-50 | Dielectric Cube Half Mirror 400-700nm A = B = C: 30mm CSMH-30-550 | CSMH-30-550 | 1piece | JPY: 43,800 | USD: 272.52 |
|
|
|
61-6876-51 | Dielectric Cube Half Mirror 400-700nm A = B = C: 40mm CSMH-40-550 | CSMH-40-550 | 1piece | JPY: 61,600 | USD: 383.28 |
|
|
|
61-6876-52 | Dielectric Cube Half Mirror 400-700nm A = B = C: 50mm CSMH-50-550 | CSMH-50-550 | 1piece | JPY: 86,700 | USD: 539.45 |
|
|
|
61-6876-53 | Dielectric Cube Half Mirror 750-850nm A = B = C: 10mm CSMH-10-800 | CSMH-10-800 | 1piece | JPY: 16,700 | USD: 103.91 |
|
|
|
61-6876-54 | Dielectric Cube Half Mirror 750-850nm A = B = C: 12.7mm CSMH-12.7-800 | CSMH-12.7-800 | 1piece | JPY: 17,600 | USD: 109.51 |
|
|
|
61-6876-55 | Dielectric Cube Half Mirror 750-850nm A = B = C: 15mm CSMH-15-800 | CSMH-15-800 | 1piece | JPY: 18,800 | USD: 116.97 |
|
|
|
61-6876-56 | Dielectric Cube Half Mirror 750-850nm A = B = C: 20mm CSMH-20-800 | CSMH-20-800 | 1piece | JPY: 24,000 | USD: 149.33 |
|
|
|
61-6876-57 | Dielectric Cube Half Mirror 750-850nm A = B = C: 25mm CSMH-25-800 | CSMH-25-800 | 1piece | JPY: 29,200 | USD: 181.68 |
|
|
|
61-6876-58 | Dielectric Cube Half Mirror 750-850nm A = B = C: 30mm CSMH-30-800 | CSMH-30-800 | 1piece | JPY: 43,800 | USD: 272.52 |
|
|
|
61-6876-59 | Dielectric Cube Half Mirror 1300-1550nm A = B = C: 10mm CSMH-10-1400 | CSMH-10-1400 | 1piece | JPY: 16,700 | USD: 103.91 |
|
|
|
61-6876-60 | Dielectric Cube Half Mirror 1300-1550nm A = B = C: 12.7mm CSMH-12.7-1400 | CSMH-12.7-1400 | 1piece | JPY: 17,600 | USD: 109.51 |
|
|
|
61-6876-61 | Dielectric Cube Half Mirror 1300-1550nm A = B = C: 20mm CSMH-20-1400 | CSMH-20-1400 | 1piece | JPY: 24,000 | USD: 149.33 |
|