すざく ( と XMM) による広がった TeV ガンマ 線放射 VER J の X 線観測 (3) Suzaku (and XMM) Observation of the extended TeV gamma-ray source VER J (3)

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すざく ( と XMM) による広がった TeV ガンマ 線放射 VER J2019+368 の X 線観測 (3) Suzaku (and XMM) Observation of the extended TeV gamma-ray source VER J2019+368(3) September 23, 2016@JPS meeting, Miyazaki Tsunefumi Mizuno (Hiroshima Univ.) N. Tanaka, H. Takahashi, J. Katsuta (Hiroshima Univ.), K. Hayashi (Nagoya Univ.), R. Yamazaki (AGU) (based on Mizuno+, submitted) 1/13

Past Obs. by Milagro & VERITAS Milagro reported an extended TeV -ray source MGRO J2019+37 in Cygnus-X direction ( =0.7deg) It was resolved into multiple sources by VERITAS. The most luminous one, VER J2019+368, has the following properties major =0.34deg, positional coincidence with MGRO J2019+37, consistent spectrum in high energy => main contributor Possible X-ray counterpart is PSR J2021+3651 & PWN G75.2+0.1 MGRO J2019+37 E>1TeV E=0.6-1TeV VER J2019+368 ( =1.75, F(1-10TeV)=6.7x10-12 erg/s/cm 2 ) Aliu+14, ApJ 788, 78 Aliu+14, ApJ 788, 78 2/13

Past Obs. in X-Rays Possible X-ray counterpart is PSR J2021+3651 & PWN G75.2+0.1 PSR J2021+3651: young and energetic puldar ( =17.2 kyr, de rot /dt=3.4x10 36 erg/s) Chandra revealed a ~20 x10 pulsar wind nebula (PWN G75.2+0.1) XMM reported faint emission of 5-10 length in east and west 30 10 Hessels+04, ApJ 612, 389 Zabalza+10, J. of Mod. Phys. D. 19, 811 3/13

Issues of the PSR/PWN Scenario Possible X-ray counterpart is PSR J2021+3651 & PWN G75.2+0.1 PSR J2021+3651: =17.2 kyr, de rot /dt=3.4x10 36 erg/s PWN G75.2+0.1: revealed by Chandra and found to extend out 5-10 in length in east and west by XMM Several issues of the PSR/PWN scenario have been pointed out (e.g., Abdo+09, ApJ 799, 1059; Parades+09, A&A507, 241) Large dispersion measure (370 pc/cm 3 ) and rotation measure (524 rad/m 2 ) indicate large distance to the source (d>10 kpc). -ray luminosity of PSR too high compared to de rot /dt Source size (~90 pc for 0.5 deg at 10 kpc) too large for highenergy electrons to propagate before cooling X-rays from only small portion of TeV emission Detailed study of the PWN properties (spectrum, morphology) and search for unknown extended emission by Suzaku-XIS 4/13

X-ray Obs. of VER J2019+368 Two Suzaku observations conducted in 2014 November S1 covers region of the PSR/PWN and TeV centroid S2 covers the west part of VER J2019+368, in which no strong X-ray sources has been reported Also analyzed archival XMM data to complement Suzaku observations Position RA (deg) DEC (deg) Net exp. (ks) Suzaku, S1 305.06 36.87 35.0 Suzaku, S2 304.79 36.83 35.7 XMM, X1 305.27 36.85 127.0 X1 S1 PSR J2021+3651 S2 5/13

XIS Image (soft band) Soft band (0.7-2 kev) intensity map (XIS3, in unit of photos/s/cm 2 /sr, NXB subtracted) PWN clearly detected in S1 No extended emission detected in S2 (see slide #8) background AGN? PSR J2021+3651 USNO-B1.0 1268-044892 6/13

XIS Image (hard band) Hard band (2-10 kev) intensity map (nxb subtracted) PWN clearly detected in S1 No obvious extended emission in S2 Size of PWN similar to that in soft band background AGN? PSR J2021+3651 USNO-B1.0 1268-044892 7/13

PWN-West Morphology Source regions: 25 rectangles of 1 x 5 and 10 rectangles of 1 x 3 along the major axis and minor axis, respectively PWN-west emission is detected at least 15 x 10 for the first time No sifnificant emission beyond the TeV emission peak Count rate profiles (2-10 kev), vignetting corrected major axis minor axis 8/13

PWN-West Spectrum (1) Procedure of the spectral analysis (15 x 5 ) 1) subtract the NXB 2) apply vignetting correction in subtracting the BG (GRXE and CXB) 3) calculate the response (arf) assuming linear decrease of the intensity in 0-15 XIS0 XIS1 XIS3 wabs x PL 2 /d.o.f.=211/188 N(H)=0.83(+/-0.12)x10 22 =2.05(+/-0.12) f(0.5-2 kev)=6.04x10-13 erg/s/cm 2 f(2-10 kev)=20.1x10-13 erg/s/cm 2 Significantly softer spectrum than that of TeV rays ( ~1.75) [XMM data indicates PWN-east and west have similar spectra (flux, )] 9/13

PWN-West Spectrum (2) Procedure of the spectral analysis (15 x 5 ) 1) subtract the NXB 2) apply vignetting correction in subtracting the BG (GRXE and CXB) 3) calculate the response (arf) assuming linear decrease of the intensity in 0-15 A B C D E erg/s/cm 2 ) Reg. N(H) f(0.5-2kev) (10-13 A (0-3 ) 0.82 (+/-0.21) 2.07 (+/-0.21) f(2-10kev) (10-13 erg/s/cm 2 ) 1.96 8.27 B (3-6 ) 0.63 (+/-0.16) 1.96 (+/-0.18) 1.68 6.52 No significant spectral change observed Absorption of ~0.8x10 22 cm -2 indicates d<<10 kpc. We adopted d=1.8 kpc estimated by Kirichenko+15 C (6-9 ) D (9-12 ) E (12-15 ) 0.72 (+/-0.17) 1.28 (+/-0.36) 1.44 (+/-0.51) 2.06 (+/-0.18) 2.30 (+/-0.32) 2.29 (+/-0.42) 1.22 4.71 0.57 2.77 0.30 1.69 10/13

Multiwavelength Spectrum x ~2.05 and ~1.75 require a break of electron spectrum at ~ 100 TeV If we assume constant injection of electrons into uniform B over the lifetime of pulsar for simplicity, synchrotron break at ~ 80 TeV is expected, consistent with x and observed A model assuming B=3 G and a break at 80 TeV from =2.1 to 3.1 explains ~70% of TeV emission => X-ray PWN is a main contributor of VER J2019+368 (The model does not fully account for morphologies in X ray and ray. Future observations by CTA is anticipated to reveal the TeV - ray properties in more detail) 11/13

Particle Transport Absence of spectral softening requires that highest energy electrons (producing 10 kev X-rays) should propagate a distance >=15. If advection is the dominant process, this requires Alternatively, in the case of energy-independent diffusion (e.g., Porth+15), diffusion coefficient should satisfy [In those scenario (under the assumption of uniform B) the absence of X-ray emission beyond the TeV peak position is due to the lower surface brightness of synchrotron X-rays] 12/13

Summary VER J2019+368 is an extended ( major =0.34deg) and hard ( =1.75) TeV -ray source in Cyg-X direction PSR J2021+3651/PWN G75.2+0.1 is a possible counterpart, but several issues are pointed out (distance, morphology) We analyzed X-ray data (Suzaku and XMM) PWN-west detected in 15 x10 with N(H)=8.2x10 21 cm -2, =2.05 (Suzaku) No significant spectral change found (Suzaku) PWN-east shows similar properties (XMM) Properties of the system B~3 G is required ( x and ) X-ray PWN is a major contributor of VER J2019+368 (MW spectrum) β adv and D are constrained from X-ray data Thank you for your Attention 13/13

References Abdo+09, ApJ 700, 1059 Abdo+12, ApJ 753, 159 Aharonian+06, A&A 460, 365 Aliu+14, ApJ 788, 78 Bamba+10, ApJ 719, L116 Hessels+04, ApJ 612, 389 Mattana+09, ApJ 694, 12 Parades+09, A&A 507, 241 Porter+08, ApJ 682, 400 Porth+16, MNRAS 460, 4135 Uchiyama+08, PASJ 60, S35 Van Etten+08, ApJ 680, 1417 Zabalza+10, J. of Mod. Phys. D. 19, 811 14/13

Appendix 15/13

Past Obs. by Milagro & VERITAS Milagro reported an extended TeV -ray source MGRO J2019+37 in Cygnus-X direction ( =0.7deg) It was resolved into multiple sources by VERITAS. The most luminous one, VER J2019+368, has the following properties major =0.34deg, positional coincidence with MGRO J2019+37, consistent spectrum in high energy => Main contributor E>1TeV E=0.6-1TeV Abdo+12, ApJ 753, 159 Aliu+14, ApJ 788, 78 Aliu+14, ApJ 788, 78 16/13

XMM View of the VER J2019+368 Region Advantages of XMM for the study of VER J2019+368 Good spatial resolution => reduction/estimation of the point-source contaminations Large FOV => overall property of the PWN Region N(H) f(0.5-2 kev) 10 22 cm --2 (erg/s/cm 2 ), f(2-10 kev) (erg/s/cm 2 ) West 0.68+/-0.12 2.11+/-0.18 ~4.1 ~14.1 East 0.47+/-0.07 1.85+/-0.13 ~4.6 ~16.8 17/13

Comparison with Other PWNe (1) X-ray PWN and VER J2019+368 show similar properties with those of other PWNe associated with TeV rays (F /Fx could be smaller; see next) Mattana+09 Bamba+10 18/13

Comparison with Other PWNe (2) Comparison with the archetype evolved PWN HESS J1825-137 and its extended PWN (Aharonian+06, Uchiyama+09) Object P, dp/dt, B s (G) characteristic age, de rot /dt F(2-10 kev) (unabsorbed; erg/s/cm 2 ), x F(1-10 TeV) (erg/s/cm 2 ), VER J2019+368 104 ms, 9.6e-14, 3.2e12 17.2 kyr, 3.4e36 erg/s ~6e-12, ~2.05 (no significant softening) 12e-12, ~1.75 HESS J1825+137 101 ms, 7.5e-14, 2.8e12 21.4 kyr 2.8e36 erg/s ~4.5e-12, ~2 (no significant softening) ~50e-12, ~2.4 VER J2019+368 shows harder spectral index in TeV and smaller F /F x ratio, indicating weaker magnetic field or younger age 19/13