The Mauna Kea Observatories Near-Infrared Filter Set
Alan T. Tokunaga
Institute for Astronomy
University of Hawaii
01 May 2005
Contents
- Rationale for the filter set
- The Mauna Kea near-infrared filter
set
- Photometric standards based on the filter
set.
- The Y filter
- 5. The 2004 production run
- 6. Manufacturing Specifications
The "Mauna Kea Observatories Near-Infrared Filter Set"
is described in detail in the following papers. The filter set was optimized to be insensitive to atmospheric effects for observatories
at altitudes higher than 2 km. These filters have been adopted by observatories at Mauna Kea and elsewhere.
- Simons & Tokunaga, Paper I
"Mauna Kea Observatories Near-Infrared Filter Set.
I. Defining Optimal 1-5 Micron Bandpasses", 2002, PASP, 114, 169
(pdf format; 469KB)
- Tokunaga, Simons, & Vacca, Paper II
"The Mauna Kea Observatories Near-Infrared Filter Set.
II. Specifications for a New JHKL'M' Filter Set for Infrared Astronomy",
2002, PASP, 114, 180
(pdf format; 164KB)
- Tokunaga & Vacca, Paper III
"The Mauna Kea Observatories Near-Infrared Filter Set.
III. Isophotal Wavelengths and Absolute Calibration", 2005, PASP, 117, 421
(pdf format; 67KB)
See also erratum, 2005, PASP,
117, 1459. (pdf format; 16KB)
The specified center, cut-on, and cut-off filter wavelengths (micrometers)
are given below.
The cut-on and cut-off are the wavelengths where the transmission is 50% of
the peak.
Broad-band Filter Wavelengths
λ | center | cut-on | cut-off |
J | 1.250 | 1.170 | 1.330 |
H | 1.635 | 1.490 | 1.780 |
K' | 2.120 | 1.950 | 2.290 |
K_s | 2.150 | 1.990 | 2.310 |
K | 2.200 | 2.030 | 2.370 |
L' | 3.770 | 3.420 | 4.120 |
M' | 4.680 | 4.570 | 4.790 |
The filter profiles for the 1998 production run may be obtained at:
Mauna Kea Filters
Standard star magnitudes and color transformations obtained at the UKIRT
with these filters are given at:
IZJHKL'M' Standard Star Magnitudes.
Color transformations obtained at the IRTF are given at:
Characterization of New Mauna Kea IR Filter Set
.
For the 2004 production run of these filters I have added the Y filter
since this filter is important in the identification of brown dwarfs.
This filter has been been designated as "Z" in the past. However, I
recommend using the label "Y" to avoid confusion with the "Z"
filters commonly used with CCDs at <1 micron.
A discussion of the Y filter can be found in L.A. Hillenbrand
et al. 2002, PASP, 114, 708. A detailed justification
for the filter bandpass and central wavelength adopted here
is given by the
WFCAM project.
The Y Filter
λ | center | cut-on | cut-off |
Y | 1.02 | 0.97 | 1.07 |
We are fabricating the Y,J,H,Ks,L', and M' filters in 2004. We are not
producing the K and K' filters for the reason that the Ks filter was
used by the 2MASS survey and this filter has good performance at both
low and high altitudes. By producing only the Ks filter we can maximize
the number of orders and therefore reduce the cost per filter.
The manufacturing specifications are given below. These specifications
can be used for ordering filters. One should also require the
production of a witness sample that is scanned at 77 K. The vendor
should provide a plot showing the measured change in wavelength
with temperature.
- Out of band transmission <0.0001 out to 5.6 µm (in other
words OD 4 required to 5.6 µm).
- All parameters for 65 K; cold filter scans of witness samples to be
provided with prediction of wavelength shift with temperature.[a]
- >80% average transmission (goal >90%).
- Peak transmission of broad band filters to have a ripple of less than
±5% of average transmission between 80% points.
- Cut-on and cut-off: ±0.5%.[b]
- Roll-off spec: %slope ≤2.5%.
%slope = [λ(90% trans.) - λ(10% trans.)] / λ(10%
trans.) *100.
- Substrate flatness.
For Adaptive Optics:
Substrate flatness <0.0138*lambda/(n-1), where n is the index of
refraction of the substrate (compatible with AO systems). For example,
for n=1.5, lambda=2200 nm, the substrate flatness should be <61 nm.
For n=3.4, lambda=2200 nm, the substrate flatness should be <13 nm,
where lambda = wavelength of the filter.[c]
For non-Adaptive Optics:
For ≤65 mm size, 1/2 fringe at 0.656 microns across the
filter diameter or diagonal. For >65 mm size, 1 fringe at 0.656
microns across the filter diameter or diagonal. (If tested in
reflection, 1 fringe = 1/2 wave.)
- Scratch/Dig: 40/20.
- Entire coated area shall be free of pinhole defects (best effort).
- Substrate surfaces parallel to 5 arcsec or better to suppress ghost
images.
- Filter to be designed for a tilt of 5 degrees to suppress ghost
images.
- Size: Up to TBD mm clear aperture. Dimensional tolerance +-0.1mm.
Note: may be round or square.
- Maximum thickness: 0.1*size.
- Must be single piece filters (cemented filters are not acceptable).
- No radioactive materials such as thorium to be used (may cause
spurious noise spikes in the detector).
Notes:
- We expect the filters to be used at 50-77 K. The filters should
be designed for 65K.
- The cut-on and cut-off are the wavelengths where the transmission is
50% of the peak. This is also referred to as the "half-power
points".
- This is a flatness spec, not a roughness spec. The filters will bend
after coating, but the front and back surfaces will remain
parallel.
- Environmental conditions: Operation in vacuum at temperature ≤77K.
Laboratory handling and storage at room temperature, pressure, and
humidity (15-25 deg. C; 5%-90% humidity). Require long-term storage
with no degradation.
- Coating durability: Filters should pass the scotch tape test for
adhesion and strokes with pencil erasure for abrasion resistance.