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Eq

Ultra-narrow-band-Tunable-Laserline-Notch-Filter-1.pdf

Ultra-narrow-band-Tunable-Laserline-Notch-Filter-1.pdf

Appl Phys B (2009) 95: 597-601 DOI 10.1007/s00340-009-3447-6 Ultra-narrow-band tunable laserline notch filter C. Moser · F. Havermeyer Received: 5 December 2008 / Revised version: 2 February 2009 / Published online: 3 March 2009 © Springer-Verlag 2009 Abstract We report on an angularly tunable…

COHR DiamondCx-10LDE Plus DS 0618 1a.pdf

COHR DiamondCx-10LDE Plus DS 0618 1a.pdf

…Beam
Output
102 mm
(4.02 in.)
176.5 mm
(6.95 in.)
165.2 mm
(6.51 in.)
4X M3x0.5-6H 8.9 mm (0.35 in.)
EQ SP On Ø25.4 mm (1.0 in.) BC
3X Ø6.7 mm
(0.266 in.) Thru
Ø6.0 mm (0.236 in.)
Purge Connection
Ø10 mm (0.394 in.)
Coolant…

COHR DiamondCx-10LDE plus DS 0219 1.pdf

COHR DiamondCx-10LDE plus DS 0219 1.pdf

…Beam
Output
102 mm
(4.02 in.)
176.5 mm
(6.95 in.)
165.2 mm
(6.51 in.)
4X M3x0.5-6H 8.9 mm (0.35 in.)
EQ SP On Ø25.4 mm (1.0 in.) BC
3X Ø6.7 mm
(0.266 in.) Thru
Ø6.0 mm (0.236 in.)
Purge Connection
Ø10 mm (0.394 in.)
Coolant…

COHR DiamondCx-10LDE plus DS 1219 2.pdf

COHR DiamondCx-10LDE plus DS 1219 2.pdf


Beam
Output
102 mm
(4.02 in.)
176.5 mm
(6.95 in.)
165.2 mm
(6.51 in.)
4X M3x0.5-6H 8.9 mm (0.35 in.)
EQ SP On Ø25.4 mm (1.0 in.) BC
3X Ø6.7 mm
(0.266 in.) Thru
Ø6.0 mm
(0.236 in.)
Purge Connection
Ø10 mm (0.394 in.)

Sample manuscript showing specifications and style

Sample manuscript showing specifications and style

…of a dispersive ECL (eq. 1) is dependent on the collimated beam diameter. It results
from the divergence of a diffraction limited collimated beam and the angular dispersion of the grating illuminated.
- In contrast, the spectral resolution of a non-dispersive ECL (eq. 2) is independent of…

Article

Article

…1035 nm, 517 nm
and 345 nm, respectively, which represents the state-of-the art of industrial ultrafast lasers in use. As expected
from Eq. 5 in Chapter 1, the process speeds decrease with decreasing wavelength for most of the materials
shown. However, there are exceptions, like…

untitled

untitled

…only the lowfrequency Raman spectral region. The crystalline content is calculated using the peak height ratio as per Eq. 3,
and the amorphous uses the peak height ratio as per Eq.
4. Both show a sigmoidal time dependence and do not
include scaling factors to account for the different…

Microsoft Word - 5694-20 submitted.doc

Microsoft Word - 5694-20 submitted.doc

…spectral bandpass of the hologram is determined by the wavelength
Bragg selectivity, which is about 1cm-1 (~0.03nm at 550nm) calculated using Eq. 2.6. However the achievable spectral
resolution is limited by the minimum angle step of the rotation stage. The minimum step of our rotation…

Self-Aligned Non-Dispersive External Cavity Tunable Laser.pdf

Self-Aligned Non-Dispersive External Cavity Tunable Laser.pdf

…a dispersive ECL (eq. 1) is dependent on the collimated
beam diameter. It results from the divergence of a diffraction limited collimated beam and the
angular dispersion of the grating illuminated.
- In contrast, the spectral resolution of a non-dispersive ECL (eq. 2) is independent…

SPIE DSS 2013 Final submitted 4-25-2013x

SPIE DSS 2013 Final submitted 4-25-2013x

…extraction, can lead to temperature gradients within the VHG. The resulting changes in the spectral
properties of the VHG can be understood using eq. (3): A temperature gradient along the optical axis would lead to
broadening (chirp) of the local spectral VHG bandwidth while gradients…

Ultra Narrow-Band Tunable Laserline Notch Filter.pdf

Ultra Narrow-Band Tunable Laserline Notch Filter.pdf

Appl Phys B (2009) 95: 597-601 DOI 10.1007/s00340-009-3447-6 Ultra-narrow-band tunable laserline notch filter C. Moser · F. Havermeyer Received: 5 December 2008 / Revised version: 2 February 2009 / Published online: 3 March 2009 © Springer-Verlag 2009 Abstract We report on an angularly tunable…