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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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56 Chapter 2<br />

2.3.2 X-Ray Observations<br />

Because the surface temperature of neutron stars is in the keV regime<br />

they can be observed only by x-ray satellites such <strong>as</strong> the Einstein Observatory<br />

which w<strong>as</strong> launched in 1979, and more recently by EXOSAT and<br />

Table 2.4. Selected x-ray observations of SN remnants and pulsars. a<br />

Age [yr] Dist.<br />

Remnant (in 1995) [kpc] Pulsar b Teff ∞ [10 6 K]<br />

c d<br />

3C58 (814) (2.6) — 2.2 ± 0.2 E 1<br />

Crab 941 1.7–2 0531+21 < 1.6 R 2<br />

(r, o, x, γ)<br />

RCW 103 1500 ± 500 2 — 2.15 ± 0.15 E 1<br />

< 1.2 R 3<br />

MSH15–52 1850 ± 250 4.2 (r, x) detected E 1<br />

Vela X ∼ 12,000 0.5 0833–45 0.95 ± 0.15 E 1<br />

(r, o, x, γ) 1.6 ± 0.2 R 4<br />

Monogem ∼ 110,000 (0.5) 0656+14 0.90 ± 0.04 R 5<br />

Ring () (r, x) (0.30 ± 0.05)<br />

— ∼ 340,000 0.15–0.4 Geminga 0.52 ± 0.10 R 6<br />

(x, γ)<br />

— ∼ 540,000 0.5–1.5 1055–52 0.65 ± 0.15 X 7<br />

(r, x, γ) 0.75 ± 0.06 R 8<br />

a Adapted from Tsuruta (1986) and updated.<br />

b Pulsed radiation: r = radio, o = optical, x = x-rays, γ = γ-rays.<br />

c E = Einstein, R = ROSAT, X = EXOSAT observation.<br />

d References:<br />

1. See the review by Tsuruta (1986) <strong>for</strong> references to the original literature.<br />

2. Becker and Aschenbach (1995).<br />

3. Becker et al. (1992).<br />

4. Ögelman, Finley, and Zimmermann (1993).<br />

5. Thompson et al. (1991). Finley, Ögelman, and Kiziloğlu (1992).<br />

6. Halpern and Ruderman (1993).<br />

7. Brinkmann and Ögelman (1987).<br />

8. Ögelman and Finley (1993). Anderson et al. (1993).

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