Canonical Name: | HESS J1837-069 |
TeVCat Name: | TeV J1837-069 |
Other Names: | 1HWC J1838-060 1HWC J1836-074c 2HWC J1837-069 FGES J1836.5-0652 1LHAASO J1837-0654u |
Source Type: | PWN |
R.A.: | 18 37 38.4 (hh mm ss) |
Dec.: | -06 57 00 (dd mm ss) |
Gal Long: | 25.18 (deg) |
Gal Lat: | -0.12 (deg) |
Distance: | 6.6 kpc |
Flux: | 0.531 (Crab Units) |
Energy Threshold: | 1000 GeV |
Spectral Index: | 2.27 |
Extended: | Yes |
Size (X): | 0.36 (deg) |
Size (Y): | 0.36 (deg) |
Discovery Date: | 2005-03 |
Discovered By: | H.E.S.S. |
TeVCat SubCat: | Default Catalog |
Source Notes:
| H.E.S.S. Galactic Plane Survey (HGPS, 2018): |
| A selection of information for each of the 78 sources in the HGPS is provided in TeVCat. For full details, visit the HGPS website. |
| Name: | HESS J1837-069 |
| Source Class: | PWN |
| Identified Object: | PSR J1838-0655 |
| R.A. (J2000): | 279.37 deg (18 37 29) |
| Dec. (J2000): | -6.96 deg (-06 57 36) |
| Positional uncertainty: | 0.033 deg |
| Spatial Model: | 3-Gaussian |
| Size: | 0.355 +/- 0.031 deg |
| Spectral Model: | power law |
| Integral Flux > 1 TeV: | 1.15e-11 +/- 4.94e-13 cm-2 s-1 |
| Pivot Energy, E0: | 0.95 TeV |
| Diff. Flux at E0: | 2.00e-11 +/- 6.86e-13 cm-2 s-1 TeV-1 |
| Spectral Index: | 2.54 +/- 0.04 |
| HGPS Source Notes: | |
| | |
The following is the text from the HGPS paper:
The HGPS analysis of HESS J1837-069 finds a size of 0.36 +/- 0.03 deg based on modeling the VHE gamma-ray emission as three Gaussian
components. This is larger than the size previously derived using a single asymmetric Gaussian
(Aharonian et al. 2006), i.e., 0.12 deg by 0.05 deg ; and using a single Gaussian
(Marandon et al. 2008), i.e., 0.22 deg . The more complex modeling of the HGPS, which also takes into account
more of the extended nebular emission from this identified PWN, explains the apparent discrepancy. Consequently, we used a larger region (twice the radius compared to
Aharonian et al. 2006) to derive
the spectrum, leading to an integral flux above 1 TeV that is larger by a factor of approximeately 3 than in the dedicated publication.
This is one of the 31 firmly-identified objects among the HGPS sources. Seven possible associations are listed in Table A.9. "This is a
list of astronomical objects, extracted from catalogs of plausible counterparts, which are are found to be spatially coincident with the HGPS source":
- J1838-0655 (PSR)
- 2FHL J1836.5-0655e (2FHL)
- 3FGL J1836.5-0655e (3FGL)
- 2FHL J1837.4-0717 (2FHL)
- 3FGL J1837.6-0717 (3FGL)
- G25.2+0.3 (PWN)
- 3FGL J1838.9-0646 (3FGL)
Source position and its uncertainty:
From
MAGIC Collaboration (2018):
- R.A. (J2000): 279.26 +/- 0.02 deg = 18h 37m 02.4s
- Dec. (J2000): -6.99 +/- 0.01 deg = -06 59' 24''
From
Aharonian et al. (2006):
This is the position that is quoted in the TeVCat table.
- l: 25.185 +/- 0.012 (deg)
- b: -0.106 +/- 0.016 (deg)
- R.A. (deg): 279.41 (Convert to HMS: 18 37 38.4)
- Dec. (deg): -6.95 (Convert to HMS: -06 57 00)
Source Extent:
From
MAGIC Collaboration (2018):
- an extension of 0.23 +/- 0.01 deg is reported
From
H.E.S.S. Collaboration (2018):
- 0.36 +/- 0.03 deg based on modeling the VHE gamma- ray emission as
three Gaussian components
"This is larger than the size previously derived using a single
asymmetric Gaussian (
Aharonian et al. 2006),
i.e., 0.12deg by 0.05deg ; and using a single Gaussian (
Marandon et al. 2008),
i.e., 0.22deg. The more complex modeling of the HGPS, which also
takes into account more of the extended nebular emission from this
identified PWN, explains the apparent discrepancy. Consequently, we
used a larger region (twice the radius compared to
Aharonian et al. 2006)
to derive the spectrum, leading to an integral flux above 1 TeV that
is larger by a factor of approx. 3 than in the dedicated publication."
From
Aharonian et al. (2006):
- semi-major axis: 7 +/- 1' = 0.12 +/- 0.02 deg
- semi-minor axis: 3 +/- 1' = 0.05 +/- 0.02 deg
- angle: 149 +/- 10
...measured counter-clk wrt the positive Gal. Lat. axis
Spectral Properties:
From
MAGIC Collaboration (2018):
- spectral index: 2.29 +/- 0.04
- flux normalisation at decorrelation energy: 4.4 +/ 0.2 10e-12 TeV-1 cm-2 s-1
- decorrelation energy: 1.25 TeV
From
H.E.S.S. Collaboration (2018):
- spectral index: 2.54 +/- 0.04
- Flux (> 1 TeV): 11.55 +/- 0.49 10e-12 cm-2 s-1
- this corresponds to the "Flux_Spec_Int_1TeV" parameter which is defined as "power law integral flux above 1 TeV"
"... we used a larger region (twice the radius compared to
Aharonian et al. 2006)
to derive the spectrum, leading to an integral flux above 1 TeV that
is larger by a factor of approx. 3 than in the dedicated publication"
Source Classification:
140702: The source classification was updated from UNID to PWN due to
some of the analyses described below.
From
Cristofari (2021):
- 2HWC J1825-134 has been listed as a possible PeVatron
From
Banik & Bhadra (2021):
- "Recently the MAGIC telescope observed three TeV gamma-ray extended sources
in the galactic plane in the neighborhood of radio SNR G24.7+0.6. Among them,
the PWN
HESS J1837-069 was detected earlier by the HESS observatory during its
first galactic plane survey. The other two sources,
MAGIC J1835-069 and
MAGIC J1837-073 are detected for the first time at such high energies. Here
we shall show that the observed gamma-rays from the SNR G24.7+0.6 and the
HESS J1837-069 can be explained in terms of hadronic interactions of the
PWN/SNR accelerated cosmic rays with the ambient matter. We shall further
demonstrate that the observed gamma-rays from the
MAGIC J1837-073 can be
interpreted through hadronic interactions of runaway cosmic-rays from PWN
HESS J1837-069 with the molecular cloud at the location of
MAGIC J1837-073.
No such association has been found between
MAGIC J1835-069 and SNR G24.7+0.6
or PWN
HESS J1837-069. We have examined the maximum energy attainable by
cosmic-ray particles in the SNR G24.7+0.6/ PWN
HESS J1837-069 and the
possibility of their detection with future gamma-ray telescopes. The study
of TeV neutrino emissions from the stated sources suggests that the
HESS J1837-069 should be detected by IceCube Gen-2 neutrino telescope in a
few years of observation."
From
Cao et al. (2021):
- HESS J1837-069 may be associated with
LHAASO J1839-0545
From
MAGIC Collaboration (2018):
The field of view of SNR G24.7+0.6 was observed and three distinct sources were detected:
- the brightest source is identified with HESS J1837-069
- an excess to the south of this source,
MAGIC J1837-073, coincident with 3FGL J1837.6-0717
-
MAGIC J1835-069 that is perhaps associated with SNR G24.7+0.6
From
H.E.S.S. Collaboration (2018):
- this source is listed as being a PWN that is associated with PSR J1838-0655
From
Katsuta et al. (2017):
- The authors describe a study of the extended emission detected by
Fermi LAT from the G25.0+0.0 region. They divide the emission into
various components comprising three main sources, each with a number
of subregions. They associate one of these subregions, G25B1, with the
TeV source HESS J1837-069.
- "G25B1 is spatially coincident with HESS J1837-069. The X-ray
observation found PSR J1838-0655 embedded in a PWN with an extent of
1.3 arcmin at the edge of HESS J1837-069 (
Gotthelf & Halpern 2008).
The H.E.S.S. source is a TeV PWN powered by this PSR with a spindown
luminosity of 5.5 x 10e36 erg s−1. The SED measured by the LAT
smoothly connects to that measured by H.E.S.S., which suggests that
photons of the LAT and H.E.S.S. data have the same origin. G25B1 has a
photon index of about 1.5, which is consistent with the expected
relativistic electron distribution of PWNe ... G25B1 is most likely a
PWN powered by PSR J1838−0655."
From
Abeysekara et al. (2017):
- "
2HWC J1837-065 is the principal maximum of an elongated region
containing multiple known extended sources which are not resolved in
the present analysis. It may be associated with the close
by TeV source HESS J1837-069 (distance of ∼0.4 deg )."
From
Abeysekara et al. (2015):
- "1HWC J1838-060 is detected at 6.1sigma post trials and is located
in the middle of the known TeV sources HESS J1837-069 and HESS
J1841-055"
- "1HWCJ1836-074c has a post-trials significance of 3.2σ, with the
nearest TeV PWN, HESS J1837-069, approx. 0.5deg away with a compatible
differential flux."
From
Fujita et al. (2013):
- "... we conclude that the gamma-rays detected from HESS J1837-069
are not created through proton-proton interactions, and may more
plausibly originate from the pulsar that was recently found near RSGC 1."
From
Acero et al. (2013):
- Analysis of the LAT data from this source leads to its
classification as a PWN candidate
From
Gotthelf & Halpern (2008):
- It is postulated that the TeV emission comes from a PWN.
- "At an assumed distance of 6.6 kpc by association with an adjacent
massive star cluster, the efficiency of PSR J1838-0655 converting
spin-down luminosity to radiation is ... ~3% for the >200 GeV emission
of HESS J1837-069, making it a plausible power source for the latter."
- "A second X-ray source adjacent to the TeV emission, AX
J1837.3-0652, is resolved into an apparent pulsar/PWN; it may also
contribute to HESS J1837-069. The star cluster RSGC 1 may have given
birth to one or both pulsars, while fueling TeV emission from the
extended PWN with target photons for inverse Compton scattering."
A PeVatron:
From
Cao et al. (2024):
- This source is listed as being a UHE source in Table 2. This means
that it has a detection above 100 TeV at a significance level
corresponding to a test statistic of greater than 20.
Seen by: H.E.S.S., HAWC, MAGIC, LHAASO
-
The First LHAASO Catalog of Gamma-Ray Sources
Cao, Zhen et al., ApJS 271 p25 (2024) [LINK]
-
The Hunt for Pevatrons: The Case of Supernova Remnants
Cristofari, P., arXiv e-prints parXiv:2110.07956 (2021) [LINK]
-
An interacting molecular cloud scenario for production of gamma-rays and neutrinos from MAGIC J1835-069, and MAGIC J1837-073
Banik, Prabir and Bhadra, Arunava, European Physical Journal C 81 p478 (2021) [LINK]
-
Ultrahigh-energy photons up to 1.4 petaelectronvolts from 12 gamma-ray Galactic sources
Cao, Z., Aharonian, F.A., An, Q., et al., Nature 594 p33-36 (2021) [LINK]
-
Diffuse gamma-ray emission from the vicinity of young massive star cluster RSGC 1
Sun, Xiao-Na et al., arXiv e-prints parXiv:2006.02052 (2020) [LINK]
-
The H.E.S.S. Galactic plane survey
H.E.S.S. Collaboration et al., A&A 612 pA1 (2018) [LINK]
-
Discovery of TeV gamma-ray emission from the neighbourhood of the supernova remnant G24.7+0.6 by MAGIC
MAGIC Collaboration et al., arXiv e-prints p (2018) [LINK]
-
The 2HWC HAWC Observatory Gamma-Ray Catalog
Abeysekara, A.U. et al., ApJ 843 p40 (2017) [LINK]
-
Extended Gamma-Ray Emission from the G25.0+0.0 Region: A Star-forming Region Powered by the Newly Found OB Association?
Katsuta, J. et al., ApJ 839 p129 (2017) [LINK]
-
Search for TeV Gamma-Ray Emission from Point-like Sources in the Inner Galactic Plane with a Partial Configuration of the HAWC Observatory
Abeysekara, A.U. et al., ArXiv e-prints p (2015) [LINK]
-
The Environment around the Young Massive Star Cluster RSGC 1 and HESS J1837-069
Fujita, Y. et al., ArXiv e-prints p (2013) [LINK]
-
Constraints on the Galactic Population of TEV Pulsar Wind Nebulae Using Fermi Large Area Telescope Observations
Acero, F. et al., ArXiv e-prints p (2013) [LINK]
-
Implications on the X-ray emission of evolved pulsar wind nebulae based on VHE gamma-ray observations
Mayer, M.J. et al., ArXiv e-prints p (2012) [LINK]
-
X-Ray Studies of HESS J1837-069 with Suzaku and ASCA: a VHE Gamma-Ray Source Originated from the Pulsar Wind Nebula
Anada, T. et al., PASJ 61 p183-+ (2009) [LINK]
-
A closer look at HESS J1837-069 following the pulsar discovery
Marandon, V. et al., AIP Conf. Proc. 1085 p320-323 (2008) [LINK]
-
Discovery of a Young, Energetic 70.5 ms Pulsar Associated with the TeV Gamma-Ray Source HESS J1837-069
Gotthelf, E.V. and Halpern, J.P., ApJ 681 p515-521 (2008) [LINK]
-
The H.E.S.S. Survey of the Inner Galaxy in Very High Energy Gamma Rays
Aharonian, F. et al., ApJ 636 p777-797 (2006) [LINK]
-
A New Population of Very High Energy Gamma-Ray Sources in the Milky Way
Aharonian, F. et al., Science 307 p1938-1942 (2005) [LINK]
Want a reference added? Send a bibtex entry to
the TeVCat Team