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HYPERFINE

Related Applay:

Sub picometer resolution

The HyperFine series of spectrometers for low intensity sources are designed for measuring hyperfine spectra and subtle spectral shifts from scattered light or distributed sources.  The HyperFine spectrometer from LightMachinery is a compact  spectrometer capable of 1 picometer resolution.   Enabled by VIPA etalons produced by LightMachinery's patented fluid jet polishing technology. 

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Introduction

  • Specifications

Part Number

Spectral Region

Form
  Factor

Total range

Simultaneous range

Resolution*

Resolution




with grating rotation

at a fixed grating position

pm

1/cm

HF-8888-UV

UV

C

200 - 400nm

Fixed 60nm range

<30pm

0.9/cm

HF-8888-UVLIBS

UV (Gated)

C

200 - 400nm

Fixed 60nm range

<30pm

0.9/cm

HF-9332

VIS

C

450 - 700nm

Fixed 250nm range

<25pm

0.9/cm

HF-9353

NIR

C

750 -1050nm

Fixed 300nm range

<40pm

0.5/cm

HF-8989-1

VIS

A

425 - 500 nm

17 nm

1.7 pm

0.08/cm

HF-8989-2

VIS

A

500 - 600 nm

16 nm

1.6 pm

0.05/cm

HF-8989-2e

VIS

A

525 - 640 nm

16 nm

1.6 pm

0.05/cm

HF-8989-3

VIS

A

600 - 700 nm

16 nm

1.6 pm

0.04/cm

HF-8995-1

NIR

A

700 - 800 nm

20 nm

2.0 pm

0.03/cm

HF-8991-3

NIR

A

800-950 nm

25 nm

2.0 pm

0.02/cm

HF-8995-2

NIR

A

950 - 1100 nm

25 nm

2.5 pm

0.02/cm

HF-8995-3-PLASMA

NIR

D

775-900nm

9 nm

0.9 pm

0.01/cm

HF-8999-PK-LLL-**

VIS

D


See Brillouin HyperFine

1.0 pm

0.04/cm

*-UHR

2X resolution upgrade to any model.



  • Notes

u  Form Factors (enclosure dimensions, does not include camera or input port)

Ø A  dimensions; 250 x 600 x 150mm,  weight; 20kg

Ø B  dimensions; 200 x 200 x 90mm,  weight; 2kg

Ø C  dimensions; 160 x 200 x 100mm,  weight; 1.5kg

Ø D  dimensions; 700 x 150 x 400mm,  weight; 28kg

Ø E dimensions; 700 x 150 x 250mm, weight 28kg

Ø F dimensions; 400 x 500 x 150mm, weight 24kg

u  *Range and resolution are measured at the middle of the wavelength range

u  Accuracy: < 200pm for fixed grating units, <20pm for all others following calibration, an external calibration source is required

u  Dynamic Range: 100:1 to 500:1 in a single shot measurement, up to 50dB with exposure bracketing

u  Simultaneous range / resolution: >10,000 at 532nm

u  Acquisition speed: >10Hz typical

u  **HF-8999-532-AUTO is specifically designed for Brillouin scattering and includes a multi-pass etalon for 532nm elastic scattering suppression.


  • Options

u  MMF input with a 10um slit, SMF input with no slit is standard

u Low resolution mode, covers the total range with 0.2nm resolution

u  Camera Options; 

Ø CMOS for laser characterization, passive element characterization, Brillouin, Raman and solar spectroscopy

Ø CCD for low light applications (non -scanning of Brillouin biological samples)

Ø Scientific CMOS for low light applications requiring fast acquisition

Ø ICCD for applications requiring gating (LIBS)

Ø UV C-MOS with good quantum efficiency down to 260nm

 

  • Features

u  FAST, No moving parts (single shot laser spectrum analysis)

u  Sub picometer resolution

u  Fiber optic input

u  Quick data acquisition and export

u  Simple USB interface

u  LabView Drivers

  • Benefits

u  Fast

u  Compact

u  Can resolve hyper fine spectra below 1 picometer

u  Ultra-reliable

u  LightMachinery's legendary customer support

 

  • APPLICATION

Light sources characterization

u  Lasers of all types

u  Single shot pulsed laser spectrum 

u  Super luminescent diodes

u  Gas discharge lamps, etc

Spectroscopy

u  Plasma spectroscopy

u High-precision gas spectroscopy

u  Brillouin or Raman spectroscopy

u  Femtosecond comb fingerprinting spectroscopy

u Spectral-domain optical coherence tomography, etc

u  Solar spectroscopy

u  Astronomical spectroscopy

u  Ultra low frequency Raman

u  Undergraduate physics and chemistry laboratories

Ø Zeeman splitting

Ø Hyperfine magnetic structure of elements

Ø Hydrogen structure

Ø Doppler shift of Fraunhofer lines due to sun rotation

Passive components characterization

u Notch filters

u  Etalons

u  Fiber Bragg gratings, etc

  • How Does it Work?

Light enters the HyperFine Spectrometer though a fiber.   A VIPA etalon, manufactured using LightMachinery's proprietary fluid jet polishing technology,  is used to produce very high dispersion in the vertical axis with sub picometer resolution.  This is followed by a conventional grating to disperse overlapping orders in the horizontal direction and produce a 2D spectrum of the input light.  LightMachinery software unwraps the spectrum to produce an ultra high resolution wavelength spectrum of the input light.  A secondary camera provides a wide wavelength range, lower resolution view of the spectrum.