1064nm Fiber-Optic 10G/20G/40G Phase Modulators     


The 1064nm lithium niobate (LiNbO₃) low half-wave output voltage quadrature phase modulator uses titanium diffusion or proton process exchange to make optical waveguides. The input and output devices are precisely obliquely coupled to the waveguide, and the electro-optical effect of the lithium niobate material is used to achieve the phase of the optical signal. Poor modulation.

Titanium diffusion (Ti-indiffusion) or proton exchange (APE) waveguide processes can achieve bipolar or uniaxial phase modulation respectively.



Product model


Name Model Price
1064nm Fiber-Optic 50G Phase Modulators   [PDF]  [RFQ]

LIM-1064-D-PA
(Stock NO. Not entered)
[Please inquire]
1064nm Fiber-Optic 20G Phase Modulators   [PDF]  [RFQ]

LIM-1064-C-PA
(Stock NO. Not entered)
[Please inquire]
1064nm Fiber-Optic 10G Phase Modulators   [PDF]  [RFQ]

LIM-1064-B-PA
Stock NO.: D80020058
[Please inquire]


Parameter



Features

● Low insertion loss

● Low Driving Voltage

● Low backlight reflection

● Small package size and light weight

● Good long-term stability

Specifications

Intensity Modulator Specifications

Parameters

Unit

Value

10GHz

20GHz

40GHz

Optical

Operation wavelength

nm

9601100

Insertion loss

dB

≤3.5

Max input power

mW

100

Return Loss

dB

≤-55

Residual intensity modulation


≤0.3%

Electrical

RF half-wave voltage@50kHz

V

≤2.0

≤2.5

≤3.0

Maximum input RF power

dBm


33


Working frequency

GHz

0.01 10

0.01 20

0.0140

Bandwidth(-3dBe)

GHz

≥10

≥18

≥30

Electrical reflection

dB

≤-10

Mechanical

Optical connector


FC/APC   or FC/PC

Electrical connector


SMA   or K(2.92mm)

V(1.85mm)

Pigtail type

PM or SM Fiber

Environment

Working temperature

0+70

Storage temperature

-55+85

*The maximum input optical power 300mW, 500mW, 1000mW can be customized


These modulators are designed for use at the specified wavelengths. Using the modulator at other wavelengths may cause an increase in the optical loss that is not covered under warranty. In some cases, this loss can be temporary; for instance, the increase in loss caused by shorter wavelengths can usually be reversed by heating the modulator to 80 °C for an hour.

The LIM-1550-B-PA includes a bias circuit that couples the DC bias onto the RF drive electrode. Depending on the application, an external DC block may be needed at the RF input.


What is the Pockel's Effect?

Both our phase and our amplitude modulators are based upon the Pockel's effect: the electro-optic effect where the refractive index along one or more axes is proportional to an externally applied electric field. Therefore, by applying a voltage across the electrodes of an electro-optic crystal, you can change the phase of light as it passes through the crystal. By placing the crystal between crossed polarizers, this phase modulation can be converted into amplitude modulation.

t2.jpg

Maximum Ratings for LiNbO3 Modulators

Optical Input Power

100 mW

Input RF Power

27dBm

Operating Temperature Range

0 °C - 70 °C

Storage Temperature Range

-40 °C - 85 °C


Dimension

PIN Diagrams


2.5.png

10Ghz LiNbO3 Phase Modulator


t3.png

20Ghz LiNbO3 Phase Modulator


t4.png

40Ghz LiNbO3 Phase Modulator


S21 Test Graph

t5.jpg


Application

● RF-Over-Fiber (RFOF) and Microwave Photonics

● High-Speed Telecommunications

● WDM Transmission

Ordering Info

M-□□□□-☆-XX( LIM stands for LiNbO3 Intensity modulator)

□□□□:Wavelength

850: 850nm

1064: 1064nm

☆ :Modulation Bandwidth

A: >2.5GHZ

B: >10GHZ

C: >20GHZ

D: >40GHZ

XX: Fiber and Connector Type 

SA=HI1060+ FC/APC

SP=HI1060+ FC/PC   

PP=PM980 Fiber+FC/PC

PA=PM980 Fiber+FC/APC



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