The COBE data have provided detections of the CIB at some wavelengths and limits elsewhere within the spectral range of the two instruments. Since foreground sources and the CMB dominate the observed sky brightness in all directions throughout the 1-1000 µm spectral range, all of these results require discrimination and removal of non-CIB contributions. Assessment of the reality of a potential CIB measurement therefore requires careful analysis of the random and systematic uncertainties in the residuals from the measured sky brightness. The residual must also be demonstrated to be isotropic, and not likely to arise from any unmodeled foreground.
Quantitative results from all of the investigations described here are
listed in Table 1. Error bars for reported
detections are 1. Upper and
lower limits are shown at the 95% CL, with actual values and
1
uncertainties shown in
parentheses. The third column indicates whether some degree of isotropy
was demonstrated. The fourth column indicates whether the investigators
claimed a detection (yes), a possible detection (tentative), or a limit
(no). The designation ``no'' is also used for any case where the result
is less than 3 times the quoted uncertainty. For illustrative purposes,
the values shown in bold type in Table 1 are
plotted in Figure 1.
![]() | ![]() ![]() | Isotropy | Detection | Reference |
(µm) | (nW m-2 sr-1) | test passed | ||
1.25 | < 75 (33±21) | no | no | Hauser et al. 1998 |
1.25 | < 68 (27±21) | no | no | Dwek & Arendt 1998 |
1.25 | < 57 (27.8±14.5) | no | no | Wright 2000 |
2.2 | < 39 (15±12) | no | no | Hauser et al. 1998 |
2.2 | 23.1±5.9 | yes | yes | Wright & Reese 2000 |
2.2 | 22.4±6.0 | no | tentative | Gorjian et al. 2000 |
2.2 | 19.9±5.3 | yes | yes | Wright 2000 |
3.5 | < 23 (11±6) | no | no | Hauser et al. (1998) |
3.5 | 14.4±4.6 | no | tentative | Dwek & Arendt 1998 |
3.5 | 11.0±3.3 | no | tentative | Gorjian et al. 2000 |
3.5 | 12.4±3.2 | yes | yes | Wright & Reese 2000 |
4.9 | < 41 (25±8) | no | no | Hauser et al. 1998 |
4.9 | < 36 (23±6) | no | no | Dwek & Arendt 1998 |
12 | < 468 (192±138) | no | no | Hauser et al. 1998 |
12-100 | < 15 | no | no | Kashlinsky et al. 1996b |
25 | < 504 (192±156 ) | no | no | Hauser et al. 1998 |
60 | < 75 (21±27) | no | no | Hauser et al. 1998 |
60 | 28.1±7.2 | yes | tentative | Finkbeiner et al. 2000 |
100 | < 34 (22±6) | no | no | Hauser et al. 1998 |
100 | > 5 (11±3) | no | no | Dwek et al. 1998 |
100 | 23.4±6.3 | no | yes | Lagache et al. 2000 |
100 | 24.6±8.4 | yes | tentative | Finkbeiner et al. 2000 |
140 | 32±6.5 | yes | tentative | Schlegel et al. 1998 |
140 | 25±7 | yes | yes | Hauser et al. 1998 |
140 | < 28 (15.3±6.4) | no | no | Lagache et al. 1999 |
140 | < 47 (24.2±11.6) | no | no | Lagache et al. 2000 |
240 | 17±2 | yes | tentative | Schlegel et al. 1998 |
240 | 13.6±2.5 | yes | yes | Hauser et al. 1998 |
240 | 11.4±1.9 | no | yes | Lagache et al. 1999 |
240 | < 25 (11.0±6.9) | no | no | Lagache et al. 2000 |
200-1000 | (see Figure 1) | yes | tentative | Puget et al. 1996 |
200-1000 | a (![]() ![]() ![]() ![]() | yes | yes | Fixsen et al. 1998 (a) |
200-1000 | a (![]() ![]() ![]() ![]() | yes | yes | Lagache et al. 1999 (b) |
(a) a = (1.3 ± 0.4) × 10-5,
k = 0.64 ± 0.12, T = (18.5 ± 1.2) K,
![]() | ||||
(b) a = 8.8 × 10-5, k = 1.4,
T = 13.6 K,
![]() |
Since the DIRBE team provided extensive foreground models, some of which
have been used by other investigators, it is convenient to describe the
results and methods of the DIRBE team first.
The DIRBE team searched for the CIB in the data from all 10 DIRBE
wavelength bands, and results based upon the final photometric reduction
of the DIRBE data were reported by
Hauser et
al. (1998).
Since there is no direction in the sky devoid of foreground radiation
from the solar system and Galaxy, the faintest measured sky brightness
at each wavelength is a conservative upper limit on the CIB. These dark
sky limits (95% CL) are
I
< 398, 151,
64, 193, 2778, 2820, 315, 94, 73, and 28 nW m-2
sr-1 at 1.25, 2.2., 3.5, 4.9, 12, 25, 60, 100, 140 and 240
µm respectively. While these limits are free of model
assumptions, they are too dominated by foreground sources to be of
cosmological interest.
After modeling and removing the contributions from all foreground
sources, the DIRBE team found isotropic residuals exceeding
3 only at 140 and 240
µm, as indicated in Table 1. The
DIRBE team further argued that these residuals could not plausibly arise
from unmodeled components of the solar system or Galaxy
(Dwek et al. 1998),
and concluded that the CIB had been measured at those wavelengths. At
all other DIRBE wavelengths they reported CIB upper limits (95% CL)
based upon the residuals and estimated uncertainties. They also
determined a lower limit at 100 µm based on the argument
that a thermal source producing the spectrum detected at 140 and 240
µm could not be fainter than this level at 100
µm
(Dwek et al. 1998).
![]() |
Figure 1. Summary of COBE-based CIB
measurements. Detections are shown with
2 |
The uncertainties reported by the DIRBE team were dominated by systematic uncertainties in the foreground determination. This met the mission objective of searching for the CIB to the limits imposed by our astrophysical environment. Major sources of uncertainty were the stellar foreground model (1.2-3.5 µm), the interplanetary dust model (1.25-100 µm), and the interstellar medium model (100-240 µm). Because DIRBE data can yield improved measurements of the CIB as the foregrounds are better determined, it is worth summarizing how the DIRBE team analysis was done.
The interplanetary dust contribution presents the most difficult problem except at the longest wavelengths, since it dominates the measured sky brightness from 1-140 µm even at high galactic and ecliptic latitude (see Figure 2, Hauser et al. 1998). The contribution from the IPD was determined by fitting a parameterized model of the spatial distribution and scattering and radiative properties of the dust cloud to the apparent annual variation of the sky brightness over the whole sky (Kelsall et al. 1998). Though this model was quite successful, reproducing the seasonal variation well and leaving evident map artifacts only at the few percent level, the uncertainties in the small residual differences between the measured brightness and the model are still quite substantial. Furthermore, it is not possible to determine a unique IPD model from sky brightness measurements from within the cloud. Kelsall et al. considered a number of different shapes for the cloud density distribution which gave comparably good fits to the time dependence, and estimated the model uncertainty by the spread in residual values at high Galactic latitude between these models.
Arendt et al. (1998) described the DIRBE team methods for determining the contribution of Galactic sources. Discrete bright sources within the Galaxy and the Magellanic Clouds were blanked out of the DIRBE maps. The contribution from discrete Galactic sources fainter than the DIRBE direct detection limit (about 5th magnitude at 2.2 µm) was calculated from 1.25 to 25 µm using a faint source model based on the SKY model of Wainscoat et al. (1992). The SKY model fits star count data over many wavelengths very well.
The contribution from the interstellar medium (ISM) was identified by
its angular variation over the sky. The 100 µm map, after
removal of the IPD contribution and an estimated value of the 100
µm CIB, was used as a template for ISM emission. The
estimate of the 100 µm CIB was obtained by correlating 100
µm emission with H I column density at well-studied dark
fields near the North Ecliptic Pole and the Lockman Hole and
extrapolating the correlation to zero H I column density. This
correlation is linear at low column densities. If all of the Galactic
infrared emission were correlated with H I gas, extrapolation of this
correlation to zero column density would yield the extragalactic
light. If there is additional infrared emission associated with other
gas components not correlated with H I, this procedure would not yield
accurate results.
Arendt et al. (1998)
chose these two fields because the molecular gas has also been mapped,
and low limits on the contribution from ionized gas could be set using
pulsar dispersion measures and
H measurements. The residual
maps at all wavelengths other
than 100 µm, after removal of the IPD contribution and
blanking of bright sources, were correlated with the ISM template to
determine a global color for each. The template was then scaled by that
color and subtracted from each map. These final residual maps were
tested for positive residuals and isotropy at high galactic latitude
where foregrounds are least bright. Note that an error in the estimated
100 µm CIB would not have affected the isotropy tests of the
residual maps, only the brightness of the residual. The uncertainty in
the estimated
100 µm CIB was included in estimating the CIB uncertainties
at all other wavelengths. The residual maps at 140 and
240 µm showed significant, isotropic residuals in dark
regions of the sky, but the most precise determination of the brightness
of the residual at these wavelengths was obtained by correlating the
emission at these wavelengths with H I column density in the dark fields
in the Lockman Hole and North Ecliptic Pole regions, as described
above. To remove the ISM from the 100 µm map for purposes of
looking for an isotropic residual at 100 µm, the H I map of
Stark et al. (1992)
was used as the ISM template. The final 100 µm residual map
did not pass the isotropy tests.
Prior to publication of the DIRBE team results, a tentative identification of the CIB using DIRBE data was reported by Schlegel, Finkbeiner, & Davis (1998). In the course of preparing Galactic reddening maps based on the far infrared data from IRAS and DIRBE, they removed the zodiacal emission contribution using the DIRBE 25 µm map as a template. Correlating the residual maps with H I maps they found a significant constant additional term at 140 and 240 µm which they identified as a possible measurement of the CIB. However, they were not certain that the residual constant could not be an instrumental effect. They were therefore not confident that the CIB had been detected, and noted that the results of the DIRBE team would be more definitive. As Table 1 shows, their tentative values for the CIB are consistent with those of Hauser et al. (1998) within the stated uncertainties.
Puget et al. (1996)
reported the first tentative identification of the CIB. Analyzing the
initial release of FIRAS data, they concluded that there was a residual
uniform background from 200 µm to 2 mm in excess of
contributions from the CMB, interplanetary dust, and interstellar
dust. They constructed a simple model for the IPD brightness based upon
DIRBE 25 and 100 µm data and the assumption that the
zodiacal emission is only a function of ecliptic latitude. They
extrapolated this model to longer wavelengths assuming
I
3. Since the IPD
contribution to the sky brightness at these wavelengths is small, an
accurate IPD model is not required. They assumed that the interstellar
emission at high galactic latitude and low H I column density is traced
by H I, and that the submillimeter emission correlated with H I can be
represented by a single temperature medium with a
2 emissivity law. They
also made a correction for infrared emission associated with ionized gas
not correlated with the H I, which significantly reduced their residual
at the shortest wavelengths (200-400 µm). Their residual
maps showed no significant gradients with galactic latitude or
longitude, so the residual background was at least approximately
isotropic. Figure 1 shows the residual spectra
of Puget et al. with and without the ionized gas correction, with a
break around 500 µm due to the shift between the FIRAS high
and low frequency channels. The lower intensity curve includes the
correction for Galactic emission from ionized gas.
A more extensive analysis of the FIRAS data, based upon the final photometric reduction of those data, was presented by Fixsen et al. (1998). They subtracted the CMB contribution and a contribution from interplanetary dust using an extrapolation of the DIRBE team model (Kelsall et al. 1998) out to 500 µm. They used three different methods to look for an isotropic residual distinct from emission from the ISM. One method assumed that the ISM spectrum is the same in all directions, but the intensity is spatially varying. The second method assumed that the neutral and ionized phases of the ISM are traced by a combination of maps of H I 21-cm line emission and of C II (158 µm) line emission. The latter was mapped over the sky by FIRAS (Bennett et al. 1994). Each component, including a term proportional to the square of the H I intensity, was allowed to have a distinct spectrum. In the third method, they assumed that the ISM emission is traced by a linear combination of the DIRBE ISM maps at 140 and 240 µm (Arendt et al. 1998), each term again having its own spectrum. Though each of these methods is subject to quite different systematic errors, the three methods yielded a consistent residual isotropic background, providing confidence that this is a robust determination of the submillimeter spectrum of the CIB. Figure 1 shows the mean spectrum found by Fixsen et al., which is consistent with the DIRBE results of Hauser et al. (1998). Table 1 gives an analytic representation of the mean CIB found by Fixsen et al.
Lagache et
al. (1999)
extended the study of the far infrared emission of the Galaxy at high
galactic latitude using FIRAS data, finding a component of the emission
not correlated with H I emission but which follows a csc(b)
law. They attributed this emission to the warm ionized medium in the
Galaxy. Subtracting the emission associated with these two gas-phase
components from the mean FIRAS spectrum in low H I column density
regions, they obtained the spectrum of the CIB longward of 200
µm. The result is consistent, within the uncertainties, with
that of
Fixsen et
al. (1998).
An analytic representation of this result is given in
Table 1. They also obtained reduced values of the
DIRBE residual in the Lockman Hole region at 140 and 240
µm. As shown in Table 1, the 240
µm value is within 1 of the
Hauser et al. (1998)
value, and the 140 µm value, which differs by less than
2
, is positive by <
3
and therefore most
confidently provides an upper limit.
Recently,
Lagache et
al. (2000)
extended the study of infrared emission from the warm ionized medium
using data from the
Wisconsin H Mapper (WHAM)
sky survey of
Reynolds et al. (1998).
They analyzed diffuse emission regions covering about 2% of
the sky at high galactic latitude. Assuming a constant electron density
so they could relate emission measure to H+ column density,
they found a marginally better correlation of infrared emission at
FIRAS resolution with a linear combination of H I and H+
column density than with H I alone. Their results suggest that 20-30%
of the far-infrared emission at high galactic latitudes is uncorrelated
with H I gas. Their resulting values for the CIB at submillimeter
wavelengths are consistent with those of
Fixsen et
al. (1998) and
Lagache et
al. (1999).
At 140 and 240 µm their results are consistent with those of
Hauser et
al. (1998),
but with residuals less than
3
positive due to the small
sky area analyzed and the uncertainties in the WHAM data. They obtained
a significantly positive residual at 100 µm similar to that
of
Hauser et
al. (1998),
but did not demonstrate that this residual was isotropic.