The variable spiral plate (VSP) is a passive liquid crystal optical
element that is capable to modify a simple laser beam into a vortex
beam, radial polarized beam having orital momentum (L=1 or L=2). The VSP
is a perfectly transparent optical element without scattering or
diffracted ligh losses (apart from the absorption losses of the
material). The conversion from homogenous linear polarized beam to, for
example, radial, azimuthal (or also lemon, spiral or star
distribution) can simply be obtained by placing the VSP in the optical
path of your laser beam. The different output Polarization patterns can
be obtained by simply changing the bias applied on the Q-plate the VSP.
Orbital momentum or helical wavefront generation - spiral phase plate (SPP)
One interesting application of the VSP is the transformation of a
planar wavefront with circular (left or right) Polarization into a beam
with an optical vortex (with an #ff0000 phase in the center of the
beam). Such a beam carries an orbital momentum (OAM) and has a helical
wavefront as shown in the picture below. The retardation of the Q-plate
is controlled by an AC bias and can be adjusted to any wanted value
between 50-1500nm. As an additional feature, the orbital momentum can
switched on and off (within 100ms) simply by changing the bias on the q
plate.
Notice
Radial and azimuthal Polarization
As the ARCoptix radial Polarization converter product (link), the VSP
(with topology q = 0.5) is capable to transform a linear input
Polarization into a radial or an azimuthal Polarization (depending of
the input Polarization). The same Q-plate can be adapted to any
wavelength by simply adjusting an AC voltage (0-5V) that is applied on
the VSP.
Spiral Phase
The variable spiral plate can produce from a simple gaussian beam
with a spiral phase. To proove this, we create a well-known Mac-Zehnder
interferometer setup coupled to a CDD camera to record the interference
pattern at the output of the interferometer. By tilting the two beams of
the interferometer, we obtain regular interference fringes (as shown in
picture) and by introducing a spiral plate (with half wave
retardation), we obtain a phase dislocation (pitchfork hologram). Again,
if the VSP retardation is tuned (via an electric bias) to full wave
retardation, the dislocation disappear as in pictures below.
An interesting recent article published in applied sciences decribed in details the possibilities of the arcoptix S-plate. Here is the link to the article: LINK
VSP switched off-
no disclocation
VSP switched on-
disclocation shows spiral phase
Q=0,5 (OM=1) between crossed polarizers
Radial Polarization
Q=1 (OM=2) between crossed polarizers
Notice that the spiral plate is similar to our radial
Polarization converter product. The principal difference between this
product is that with the spiral plate, one can obtain either a spiral or
a radial Polarization and with the Polarization converter one obtains
always the radial Polarization and the spiral phase at the same time.
The differences between the spiral plate and the ARCoptix Polarization
converter are summarised in the table below.
By looking at the comparaison in the table, it seems clear that the VSP
has many advantages compared to the Polarization converter. Also, the
VSP does not have the PI phase step in the middle of the aperture, which
makes the device simpler to adjust and beam quality will be better. It
is also important to note that Polarization is a proven device that
has already been used by many scientists with full satisfaction. The
VSP is a new product that does not have reference for the moment.
Notice that for optimal quality it is recommended to use a beam size of
at least 5mm in diameter. Results obtained with a beam size below 2-3 mm
may suffer from inperfection dues fundamental LC manufactring
limitatios in the center of the cell.
Features |
Polarization Converter |
Variable spiral plate |
Technology |
Alignment of LC nematic with rubbing |
Alignment LC nematic with polymers aligned with pol. UV light |
Topological charge |
not relevant |
Q=+/- 0.5 standard
Q=1 on demand |
Minimal Beam Size |
2 mm |
5 mm |
Orbital Momentum |
OM= +/- 1 |
OM= +/- 1 on demand +/- 2 |
Wavelength range |
400-1700nm |
400-1700nm |
Broadband wavelength illumination |
Yes possible |
Max wavelength width 100nm |
Generation of various singularities |
Fix singularity |
Singularity can varied with input Polarization and phase retardance |
Radial or azimuthal Polarization |
Yes |
Yes |
Spiral phase |
No |
Yes (with circular pol.) |
Pi phase step |
Yes need to be compensate with phase compensator |
No phase step |
Electrical driving | Yes USB LC driver recommended | Yes USB LC driver recommended |