Micro-mirror Supervisor: Prof. Kämper Team member: Chun Wa George Young Issis Contreras Ramanathan Swaminathan Spandan Shroff 10-10- 2011 Micromechatronics System FH AACHEN University of Applied Science
Feb 24, 2016
Micro-mirror
Supervisor: Prof. KämperTeam member:Chun Wa George YoungIssis ContrerasRamanathan SwaminathanSpandan Shroff10-10-2011
Micromechatronics SystemFH AACHENUniversity of Applied Science
small sizelow cost,fast response – filter unwanted wavelengthshigh signal to noise ratioreduced complexity and low power consumption
Advantage of MEMS Spectrometer over conventional
Key features of micromirror array
a 100% fill-factorminimum surface roughness and high reflectivity (ideally 100%) in the wavelength range of interestzero insertion losszero noisesimple controlidentical deflection versus input energy response
A unique application of micromachined mirrors can be performance enhancement of a spectrometer by selectively focusing a particular spectral component on a detector thereby reducing the number of detectors required.
improves the signal to noise ratio of the spectrometer device
IR RANGE SPECTROMETER
Source: FhG-IZMLittrow configuration
PORTABLE UNIVERSIAL SPECTROMETER
Small mirror – reducing bandpass - higher resolutionBut low light intensity
Variable band pass filter
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DIFFRACTION GRATING
Monochromatic lightd sina + d sinb = wavelengthSo leading to constructive interference
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DIFFRACTION GRATING
When a diffraction grating is used, care must be taken in the design of broadband monochromators because the diffraction pattern has overlapping orders.
In-plane diffraction refers to a diffraction technique in which both the incident and diffracted beams are nearly parallel to the sample surface.
The spectrum is scanned by rotating the grating; this moves the grating normal relative to the incident and diffracted beams, which (by Eq. (2-1)) changes the wavelength diffracted toward the second mirror.
The grating diffracts the light, which converges toward the exit slit; the spectrum is scanned by rotating the grating to bring different wavelengths into focus at or near the exit slit.
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GRAT SCANNING
The spectrum is scanned by rotating the grating; this moves the grating normal relative to the incident and diffracted beams, which (by Eq. (2-1)) changes the wavelength diffracted toward the second mirror.
The grating diffracts the light, which converges toward the exit slit; the spectrum is scanned by rotating the grating to bring different wavelengths into focus at or near the exit slit.
the grating is rotated to bring different wavelengths into focus at the (stationary) exit slit.
The efficiency is maximal when the grating is used in the Littrow configuration
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PLAN GRATING AND MOUNTS
The Czerny-Turner monochromator
the light incident on and diffracted by the grating is collimated, the spectrum remains at focus at the exit slit for each wavelength,
The Ebert-Fastie monochromator
This design is a special case of a Czerny-Turner mount
DisadvantageThis can be seen by recognizing that the Ebert-Fastie monochromator is a special case of the Czerny-Turner monochromator in which both concave mirror radii are the same, and for which their centers of curvature coincide.AdvantageHowever, an advantage that the Ebert-Fastie mount provides is the avoidance of relative misalignment of the two mirrors
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PLAN GRATING AND MOUNTS
The Monk-Gillieson monochromator
AdvantageOften the angles of reflection (from the primary mirror), incidence and diffraction are small (measured from the appropriate surface normals), which keeps aberrations (especially off-axis astigmatism) to a minimum.DisadvantageConsequently the spectrum cannot remain in focus at a fixed exit slit when the grating is rotated (unless this rotation is about an axis displaced from the central groove of the grating42).
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PLAN GRATING AND MOUNTS
The Littrow monochromator
The same auxiliary optics can be used as both collimator and camera, since the diffracted rays retrace the incident rays.
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DEFINITIONIn-plane diffraction refers to a diffraction technique in which both the incident and diffracted beams are nearly parallel to the sample surface.
The blaze wavelengthis defined as that wavelength, in a given diffraction order m, for which the efficiency curve reaches its maximum.
ml = d (sina + sinb)
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FABRICATION
polysilicon (poly-Si) and gold micromirror is fabricated by a surface -micromachining process
Drawback: residual stressResult: curvature of the mirror surface which results in high insertion loss and crosstalk
So monocrystalline silicon
best results and closely resemblesan ideal reflector surface.
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1 DIMENSION ARRAY MICRO MIRROR
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TYPE OF MICRO MIRROR
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QUESTIONThe proposal is workable?Mirror size?
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OPTICS DEFINITIONAberrations are departures of the performance of an optical system from the predictions of paraxial optics
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SLIT
The entrance slit is placed at the effective focus of the collimator so that the light from the slit reflected from the mirror is collimated (focused at infinity)
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PORTABLE MONOCHROMATOR
300nm – 5um
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PORTABLE MONOCHROMATOR
Light source
Incident ray
reflected ray
InGaAs Detector
HgCdTe Detector
Linear motion
Rotational motion
Diffraction grating with different Blaze wavelength
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