首页 Fiber Accessories Fiber & patch cords High Non-Linear Fiber C-band High Non Linear Fiber (HNLF) C-band high nonlinear optical fiber dispersion 0.0±1ps/(nm.km
  • C-band high nonlinear optical fiber dispersion 0.0±1ps/(nm.km

    Nonlinear effects in optical fibers, such as stimulated Raman scattering (SRS), stimulated Brillouin scattering (SBS), and the optical Kerr effect, have many applications in the fields of communications and optical signal processing. In the Kerr effect, the refractive index of the light-guiding medium changes with the optical power, which will lead to a series of secondary effects, such as self-phase modulation (SPM), cross-phase modulation (XPM), four-wave mixing (FWM), and non-steady-state modulation. Applications that utilize the Kerr effect include optical parametric amplification, frequency conversion, phase coupling, pulse compression and generation, and optical soliton transmission. The design of highly nonlinear optical fibers needs to consider the following aspects: first, the optical fiber must have high nonlinearity to obtain effective nonlinear interactions; second, the optical fiber must have low loss to increase the effective action length Leff. Third, for various applications, the optical fiber must have matching dispersion characteristics. Finally, the nonlinear optical fiber must have low polarization mode dispersion (PMD). For silica-based highly nonlinear optical fibers, the design of the refractive index profile plays an important role in meeting the above requirements. In the design of high nonlinear optical fiber, a small core effective area Aeff, a low dispersion slope and a cutoff wavelength much smaller than the working wavelength must be achieved at the same time. High nonlinear optical fiber not only has high nonlinearity, but also has a very low dispersion slope. A flexible W-shaped profile design is adopted to introduce a low refractive index inner cladding around the step refractive index core.

    产品特点Higher nonlinear coefficient、 Zero dispersion wavelength is adjustable in three bands: S, C, and L、 Lower loss and low dispersion slope、 Small additional loss when spliced with ordinary single-mode fiber

    产品货号C80010077

    应用领域Parametric amplification、 Wavelength conversion、 Pulse compression、 Supercontinuum source、 Optical regenerator、 Discrete (or lumped) Raman amplifier

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    Sherry

    电话:16628709332

    邮箱:moli@microphotons.com

    主要参数
  • 核心参数
  • 尺寸图
  • Photoelectric parameters:

    Fiber Type

    NL-1550-POS

    NL-1550-ZERO

    NL-1550-NEG

    Optical properties

    Operating band

    C-band

    Dispersion slope @1550nm (ps/nm2/km)

    <0.035

    <0.030

    <0.030

    Dispersion @1550nm (ps/nm/km)

    >1

    0.0±1

    <-1

    Non-linear coefficient @1550nm (W-1km-1)

    ≥10

    Attenuation coefficient @1550nm (dB/km)

    ≤1.5

    Cut-off wavelength (nm)

    <1480

    Numerical aperture (typical value)

    0.35

    Geometric properties

    Glass cladding diameter (μm)

    125±7

    Cladding non-circularity (%)

    ≤1

    Core cladding concentricity (μm)

    ≤0.5

    Coating diameter (μm)

    245±10

    Note:

    * Provides support for fiber splicing.

    * The fluctuation range of the glass cladding diameter of a specific optical fiber is no more than 2um.

     



    Characteristics

    Conditions

    Data

    Unit

    Geometric properties

    Core diameter

    --

    62.5±2.5

    [μm]

    Core non-circularity

    --

    ≤5.0

    [%]

    Cladding diameter

    --

    125.0±1.0

    [μm]

    Cladding non-circularity

    --

    ≤1.0

    [%]

    Coating diameter

    --

    245±7

    [μm]

    Coating/cladding concentricity

    --

    ≤10.0

    [μm]

    Coating non-circularity

    --

    ≤6.0

    [%]

    Core/cladding concentricity

    --

    ≤1.5

    [μm]

    Fiber length

    --

    Longest to17.6

    [km/coil]

    Optical properties

    Attenuation

    850nm

    ≤2.7

    [dB/km]

    1300nm

    ≤0.6

    [dB/km]

    Full injection bandwidth

    850nm

    ≥200

    [MHz·km]

    1300nm

    ≥500

    [MHz·km]

    Numerical aperture

    --

    0.275±0.015

    --

    Group refractive index

    850nm

    1.496

    --

    1300nm

    1.491

    --

    Zero dispersion wavelength

    --

    1320~1365

    [nm]

    Zero dispersion slope

    1320nm≤ λ0 ≤1348nm

    ≤0.11

    [ps/(nm2·km)]

    1348nm≤ λ0 ≤1365nm

    ≤0.001(1458-λ0 

    [ps/(nm2·km)]

    Macrobending loss

    --

    --

    --

    100 turns, radius 37.5mm

    850nm

    ≤0.50

    [dB]

    1300nm

    ≤0.50

    [dB]

    Backscattering characteristics 1300nm

    Steps (average of bidirectional measurements)

    --

    ≤0.10

    [dB]

    Irregularities and point discontinuities in the length direction

    --

    ≤0.10

    [dB]

    Attenuation non-uniformity

    --

    ≤0.10

    [dB/km]

    Environmental Characteristics 850nm and 1300nm

    Temperature cycle additional attenuation

    -60℃ to 85℃

    ≤0.10

    [dB/km]

    Temperature-humidity cycle additional attenuation

    -10℃ to 85℃,4% to 98% relative humidity

    ≤0.10

    [dB/km]

    Water immersion additional attenuation

    23℃, 30 days

    ≤0.10

    [dB/km]

    Dry heat additional attenuation

    85℃, 30days

    ≤0.10

    [dB/km]

    Additional damp heat attenuation

    85℃ and 85%Relative humidity,30days

    ≤0.10

    [dB/km]


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