Table 6: Total list of all ROSAT PSPC X-ray sources in M 31 merged from the source lists of both surveys. The different symbols in front of the RXJ numbers in Col. (1) are explained at the top of the table. The meaning of the different columns is described in Sect. 3.3. The listed count rate errors are purely statistical. The systematic errors are expected to be less than $\sim$15%. Count rates for bulge sources (marked with $\star$) may be uncertain due to confusion. For sources not detected in a considered energy band, $1\sigma$ upper limits have been calculated indicated by a "<''-symbol in front of the upper limit value. A conversion of count rates into fluxes depends on the assumed spectral shape. For M 31-sources a power law with photon index $\Gamma = -2.0$ and $N_{\rm H} = 9\times 10^{20}~\mbox{ cm}^{-2}$ may be used, leading to a conversion factor $1~\mbox{ct~ks}^{-1} = 3.00\times 10^{-14} \mbox{ erg cm}^{-2} \mbox{ s}^{-1}$ in the 0.1-2.0 keV band (B-band). For foreground stars, the application of this conversion factor leads to an overestimation of the flux.

a Foreground star     b Galaxy    c Supersoft source candidate     d Globular cluster     e SNR
$\star$ bulge source     $\sim$ Variable source (ref. Tables 2, 3 and footnote in Sect. 4.1.1)     $\dagger$ Source with uncertain count rate.
RXJ	SI	RA		(J2000)		Dec		$\sigma_{\rm Pos}$	Cl.	Maxlik	Rate (B)	Rate (S)	Rate (H)	Rate ($H_{\rm 1}$)	Rate ($H_{\rm 2}$)
No.	No.	(h)	(m)	(s)	( $\hbox{$^\circ$ }$)	(')	('')	('')		(LH)	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$
(1)	(2)	(3)	(4)	(5)	(6)	(7)	(8)	(9)	(10)	(11)	(12)	(13)	(14)	(15)	(16)
dRX J0036.3+4053		0	36	21.7	40	53	37	13	4	69.7	$< 0.61 \hspace{8ex}$	$< 0.20 \hspace{8ex}$	$5.73 \pm 0.65$	$< 1.70 \hspace{8ex}$	$4.22 \pm 0.53$
RX J0036.7+4109		0	36	43.0	41	9	2	19	4	27.1	$< 0.43 \hspace{8ex}$	$< 0.16 \hspace{8ex}$	$3.18 \pm 0.71$	$< 0.87 \hspace{8ex}$	$3.56 \pm 0.61$
RX J0036.8+4008		0	36	49.8	40	8	52	12	1	45.0	$10.62 \pm 1.82$	$< 3.50 \hspace{8ex}$	$7.46 \pm 1.43$	$< 3.59 \hspace{8ex}$	$3.74 \pm 1.04$
RX J0036.8+4055		0	36	49.6	40	55	12	18	4	11.8	$< 0.13 \hspace{8ex}$	$< 0.14 \hspace{8ex}$	$1.72 \pm 0.42$	$< 0.99 \hspace{8ex}$	$< 1.20 \hspace{8ex}$
RX J0036.9+4026		0	36	57.4	40	26	10	12	1	12.2	$< 2.13 \hspace{8ex}$	$< 0.62 \hspace{8ex}$	$1.34 \pm 0.43$	$< 0.81 \hspace{8ex}$	$< 1.30 \hspace{8ex}$
RX J0037.1+4022		0	37	11.4	40	22	10	11	1	10.5	$< 1.65 \hspace{8ex}$	$< 0.70 \hspace{8ex}$	$< 1.13 \hspace{8ex}$	$< 0.63 \hspace{8ex}$	$< 0.55 \hspace{8ex}$
RX J0037.2+4045	1	0	37	17.4	40	45	23	6	2	26.7	$2.14 \pm 0.80$	$0.95 \pm 0.80$	$< 0.87 \hspace{8ex}$	$< 0.12 \hspace{8ex}$	$< 0.80 \hspace{8ex}$
RX J0037.3+4029	2-	0	37	18.7	40	29	47	8	1	82.4	$3.43 \pm 0.65$	$< 0.30 \hspace{8ex}$	$3.90 \pm 0.60$	$2.02 \pm 0.43$	$1.79 \pm 0.41$
aRX J0037.3+4043		0	37	22.5	40	43	49	9	1	86.3	$10.19 \pm 1.34$	$5.09 \pm 0.98$	$4.93 \pm 0.90$	$2.97 \pm 0.69$	$1.82 \pm 0.56$
RX J0037.4+4013		0	37	26.2	40	13	7	10	1	20.6	$2.16 \pm 0.60$	$< 0.79 \hspace{8ex}$	$1.63 \pm 0.43$	$< 0.54 \hspace{8ex}$	$1.22 \pm 0.36$
cRX J0037.4+4015	3	0	37	25.3	40	15	16	6	2	15.1	$< 0.31 \hspace{8ex}$	$< 0.31 \hspace{8ex}$	$0.01 \pm 0.00$	$< 0.01 \hspace{8ex}$	$< 0.01 \hspace{8ex}$
RX J0037.5+4009	4-	0	37	34.6	40	9	55	7	1	238.8	$11.48 \pm 1.16$	$< 1.25 \hspace{8ex}$	$9.49 \pm 0.97$	$3.63 \pm 0.61$	$5.63 \pm 0.75$
$\dagger$RX J0037.6+3938	5+	0	37	36.5	39	38	56	6	3	177.2	$2.11 \pm 1.04$	$< 0.01 \hspace{8ex}$	$2.26 \pm 1.12$	$< 0.01 \hspace{8ex}$	$2.15 \pm 1.07$
RX J0037.6+4025		0	37	41.5	40	25	45	10	1	15.9	$< 1.62 \hspace{8ex}$	$< 0.59 \hspace{8ex}$	$0.78 \pm 0.25$	$< 0.36 \hspace{8ex}$	$0.51 \pm 0.19$
RX J0037.7+4004	7-	0	37	43.5	40	4	55	11	1	44.0	$19.11 \pm 2.03$	$< 2.32 \hspace{8ex}$	$14.48 \pm 1.49$	$4.25 \pm 0.89$	$8.80 \pm 1.15$
RX J0037.7+4023		0	37	43.3	40	23	44	8	1	52.3	$2.97 \pm 0.54$	$< 1.30 \hspace{8ex}$	$2.12 \pm 0.39$	$1.64 \pm 0.34$	$< 0.62 \hspace{8ex}$
RX J0037.7+4037	6-	0	37	42.6	40	37	50	10	1	15.9	$< 1.86 \hspace{8ex}$	$< 0.73 \hspace{8ex}$	$0.90 \pm 0.28$	$< 0.45 \hspace{8ex}$	$0.58 \pm 0.22$
aRX J0038.0+4026	8+	0	38	1.1	40	26	28	5	1	847.8	$19.87 \pm 0.83$	$11.64 \pm 0.63$	$7.61 \pm 0.50$	$4.05 \pm 0.45$	$3.90 \pm 0.26$
RX J0038.3+4018	9+	0	38	22.1	40	18	26	5	1	35.5	$1.34 \pm 0.29$	$0.37 \pm 0.26$	$1.07 \pm 0.16$	$0.16 \pm 0.11$	$0.79 \pm 0.09$
RX J0038.3+4040		0	38	20.1	40	40	29	10	1	17.2	$< 1.39 \hspace{8ex}$	$< 0.50 \hspace{8ex}$	$0.75 \pm 0.23$	$< 0.22 \hspace{8ex}$	$0.60 \pm 0.20$
RX J0038.3+4056		0	38	21.3	40	56	40	9	1	52.1	$7.23 \pm 1.16$	$3.23 \pm 0.92$	$3.99 \pm 0.80$	$1.42 \pm 0.50$	$2.49 \pm 0.63$
$\dagger$RX J0038.4+3959	11	0	38	28.0	39	59	52	18	2	10.5	$< 0.29 \hspace{8ex}$	$< 0.03 \hspace{8ex}$	$0.27 \pm 0.15$	$< 0.00 \hspace{8ex}$	$< 0.24 \hspace{8ex}$
$\sim^a$RX J0038.4+4012	10+	0	38	24.1	40	12	57	5	1	706.2	$12.61 \pm 0.66$	$1.91 \pm 0.29$	$9.39 \pm 0.52$	$3.50 \pm 0.33$	$6.95 \pm 0.47$
bRX J0038.4+4136		0	38	27.7	41	36	55	23	4	14.6	$< 0.17 \hspace{8ex}$	$< 0.17 \hspace{8ex}$	$< 2.86 \hspace{8ex}$	$< 0.46 \hspace{8ex}$	$< 0.68 \hspace{8ex}$
cRX J0038.5+4014	12	0	38	32.1	40	14	39	11	1	14.1	$0.80 \pm 0.28$	$0.70 \pm 0.26$	$< 0.03 \hspace{8ex}$	$< 0.03 \hspace{8ex}$	$< 0.01 \hspace{8ex}$
RX J0038.5+4024	13	0	38	34.7	40	24	30	5	1	10.4	$0.46 \pm 0.20$	$< 0.04 \hspace{8ex}$	$0.38 \pm 0.03$	$< 0.05 \hspace{8ex}$	$< 0.34 \hspace{8ex}$
RX J0038.5+4128	14-	0	38	34.5	41	28	51	8	4	2093.6	$55.28 \pm 0.96$	$< 0.40 \hspace{8ex}$	$63.69 \pm 1.42$	$21.82 \pm 0.91$	$35.02 \pm 1.17$
RX J0038.6+4010	16+	0	38	38.1	40	10	33	8	1	26.6	$1.98 \pm 0.36$	$1.20 \pm 0.31$	$0.88 \pm 0.22$	$0.31 \pm 0.15$	$0.51 \pm 0.14$
RX J0038.6+4015	15	0	38	37.6	40	15	19	7	1	12.0	$1.04 \pm 0.26$	$0.54 \pm 0.19$	$0.39 \pm 0.14$	$0.26 \pm 0.13$	$0.15 \pm 0.07$
cRX J0038.6+4019	18+	0	38	40.9	40	20	0	5	1	49.3	$1.73 \pm 0.29$	$1.54 \pm 0.26$	$< 0.05 \hspace{8ex}$	$< 0.02 \hspace{8ex}$	$< 0.04 \hspace{8ex}$
aRX J0038.6+4026	17+	0	38	38.6	40	26	15	5	1	154.0	$3.76 \pm 0.37$	$0.93 \pm 0.28$	$2.94 \pm 0.26$	$< 1.73 \hspace{8ex}$	$< 1.21 \hspace{8ex}$
RX J0038.6+4043		0	38	39.0	40	43	25	10	1	11.7	$< 0.80 \hspace{8ex}$	$< 0.25 \hspace{8ex}$	$< 0.77 \hspace{8ex}$	$< 0.18 \hspace{8ex}$	$0.44 \pm 0.17$
RX J0038.6+4044	19-	0	38	40.8	40	44	57	9	1	20.3	$1.46 \pm 0.39$	$< 0.98 \hspace{8ex}$	$0.78 \pm 0.24$	$< 0.18 \hspace{8ex}$	$0.69 \pm 0.21$
RX J0038.6+4056		0	38	38.6	40	56	54	11	1	26.0	$2.59 \pm 0.71$	$< 0.48 \hspace{8ex}$	$2.57 \pm 0.57$	$< 0.82 \hspace{8ex}$	$2.25 \pm 0.53$
RX J0038.8+4008	20-	0	38	48.2	40	8	3	10	1	23.9	$1.50 \pm 0.44$	$< 0.60 \hspace{8ex}$	$1.39 \pm 0.33$	$< 1.20 \hspace{8ex}$	$0.64 \pm 0.21$
RX J0038.8+4038	21-	0	38	48.6	40	38	12	8	1	39.5	$1.28 \pm 0.31$	$< 0.26 \hspace{8ex}$	$1.18 \pm 0.24$	$0.43 \pm 0.15$	$0.73 \pm 0.19$
RX J0038.8+4044	19-	0	38	50.1	40	44	18	8	1	111.0	$3.28 \pm 0.49$	$< 0.45 \hspace{8ex}$	$3.25 \pm 0.43$	$< 0.87 \hspace{8ex}$	$2.70 \pm 0.38$
RX J0038.9+3955		0	38	56.0	39	55	51	10	1	26.2	$2.52 \pm 0.74$	$< 0.66 \hspace{8ex}$	$2.07 \pm 0.59$	$< 0.73 \hspace{8ex}$	$1.57 \pm 0.50$
RX J0038.9+4016	22	0	38	55.4	40	16	53	7	1	11.9	$0.93 \pm 0.24$	$< 0.42 \hspace{8ex}$	$< 0.47 \hspace{8ex}$	$< 0.32 \hspace{8ex}$	$< 0.21 \hspace{8ex}$

 

Table 6: continued.

a Foreground star    b Galaxy    c Supersoft source candidate    d Globular cluster    e SNR
$\star$ bulge source     $\sim$ Variable source (ref. Tables 2, 3 and footnote in Sect. 4.1.1)     $\dagger$ Source with uncertain count rate.
RXJ	SI	RA		(J2000)		Dec		$\sigma_{\rm Pos}$	Cl.	Maxlik	Rate (B)	Rate (S)	Rate (H)	Rate ($H_{\rm 1}$)	Rate ($H_{\rm 2}$)
No.	No.	(h)	(m)	(s)	( $\hbox{$^\circ$ }$)	(')	('')	('')		(LH)	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$
(1)	(2)	(3)	(4)	(5)	(6)	(7)	(8)	(9)	(10)	(11)	(12)	(13)	(14)	(15)	(16)
RX J0038.9+4029	23	0	38	55.6	40	29	8	5	1	14.8	$0.72 \pm 0.21$	$0.18 \pm 0.17$	$0.45 \pm 0.07$	$0.19 \pm 0.14$	$< 0.35 \hspace{8ex}$
RX J0038.9+4034	25-	0	38	56.3	40	34	52	9	1	43.3	$1.69 \pm 0.34$	$< 0.50 \hspace{8ex}$	$1.35 \pm 0.25$	$< 0.42 \hspace{8ex}$	$1.03 \pm 0.21$
RX J0038.9+4058	24	0	38	56.8	40	58	56	5	2	10.5	$1.05 \pm 0.44$	$0.82 \pm 0.33$	$< 0.12 \hspace{8ex}$	$< 0.10 \hspace{8ex}$	$< 0.03 \hspace{8ex}$
RX J0039.0+4047		0	39	3.6	40	47	43	9	1	10.9	$< 1.03 \hspace{8ex}$	$< 0.37 \hspace{8ex}$	$0.59 \pm 0.20$	$< 0.30 \hspace{8ex}$	$0.39 \pm 0.15$
RX J0039.1+4006	27-	0	39	9.1	40	6	23	12	1	12.8	$< 0.85 \hspace{8ex}$	$< 0.36 \hspace{8ex}$	$< 0.87 \hspace{8ex}$	$< 0.19 \hspace{8ex}$	$0.58 \pm 0.21$
RX J0039.1+4012	28	0	39	10.6	40	12	22	5	1	15.6	$1.10 \pm 0.26$	$< 0.19 \hspace{8ex}$	$< 0.85 \hspace{8ex}$	$< 0.47 \hspace{8ex}$	$< 0.40 \hspace{8ex}$
RX J0039.1+4026	26	0	39	6.6	40	26	55	5	1	10.7	$0.25 \pm 0.16$	$0.07 \pm 0.05$	$0.20 \pm 0.17$	$0.02 \pm 0.01$	$< 0.17 \hspace{8ex}$
RX J0039.1+4035		0	39	11.6	40	35	34	10	1	16.8	$< 1.11 \hspace{8ex}$	$< 0.30 \hspace{8ex}$	$0.66 \pm 0.18$	$0.51 \pm 0.16$	$< 0.23 \hspace{8ex}$
RX J0039.2+4001	31-	0	39	16.5	40	1	6	9	1	25.0	$2.21 \pm 0.61$	$< 2.02 \hspace{8ex}$	$1.69 \pm 0.44$	$< 0.96 \hspace{8ex}$	$1.53 \pm 0.42$
RX J0039.2+4008	29+	0	39	16.4	40	8	28	5	1	83.0	$3.16 \pm 0.39$	$0.44 \pm 0.33$	$3.04 \pm 0.28$	$0.97 \pm 0.27$	$< 1.84 \hspace{8ex}$
RX J0039.2+4013		0	39	12.8	40	13	8	10	1	14.9	$< 1.36 \hspace{8ex}$	$< 0.63 \hspace{8ex}$	$0.56 \pm 0.19$	$< 0.20 \hspace{8ex}$	$0.46 \pm 0.16$
RX J0039.2+4051		0	39	16.6	40	51	17	8	1	35.4	$1.64 \pm 0.38$	$< 0.42 \hspace{8ex}$	$1.33 \pm 0.28$	$< 0.78 \hspace{8ex}$	$0.84 \pm 0.21$
RX J0039.2+4102	30-	0	39	17.9	41	3	0	10	1	33.8	$1.62 \pm 0.47$	$< 0.26 \hspace{8ex}$	$2.17 \pm 0.45$	$< 1.00 \hspace{8ex}$	$1.40 \pm 0.36$
RX J0039.3+4023	33	0	39	23.0	40	23	28	5	1	10.9	$0.29 \pm 0.16$	$< 0.03 \hspace{8ex}$	$0.27 \pm 0.16$	$< 0.05 \hspace{8ex}$	$0.20 \pm 0.14$
RX J0039.3+4047	32	0	39	21.4	40	47	41	14	2	30.2	$< 0.26 \hspace{8ex}$	$0.22 \pm 0.07$	$< 0.01 \hspace{8ex}$	$< 0.01 \hspace{8ex}$	$< 0.00 \hspace{8ex}$
RX J0039.4+4029	34	0	39	24.7	40	29	57	5	1	23.9	$0.49 \pm 0.18$	$< 0.02 \hspace{8ex}$	$0.41 \pm 0.15$	$< 0.15 \hspace{8ex}$	$< 0.31 \hspace{8ex}$
RX J0039.4+4035	36+	0	39	29.9	40	35	54	5	1	25.9	$0.63 \pm 0.23$	$< 0.03 \hspace{8ex}$	$0.56 \pm 0.21$	$< 0.19 \hspace{8ex}$	$< 0.37 \hspace{8ex}$
RX J0039.4+4050	35+	0	39	25.1	40	50	39	8	1	34.8	$2.93 \pm 0.36$	$1.52 \pm 0.24$	$1.37 \pm 0.26$	$0.85 \pm 0.21$	$0.40 \pm 0.11$
RX J0039.4+4105		0	39	25.0	41	5	20	11	1	12.3	$< 1.80 \hspace{8ex}$	$< 0.54 \hspace{8ex}$	$0.98 \pm 0.32$	$< 0.47 \hspace{8ex}$	$0.66 \pm 0.26$
bRX J0039.5+4008	37	0	39	33.3	40	8	43	5	1	18.2	$0.71 \pm 0.26$	$< 0.06 \hspace{8ex}$	$0.61 \pm 0.24$	$< 0.03 \hspace{8ex}$	$0.60 \pm 0.22$
RX J0039.5+4109	38-	0	39	34.6	41	9	34	8	1	93.4	$5.04 \pm 0.81$	$< 0.53 \hspace{8ex}$	$4.87 \pm 0.72$	$1.09 \pm 0.36$	$3.75 \pm 0.63$
aRX J0039.6+4011	40-	0	39	38.3	40	11	6	9	1	26.2	$1.86 \pm 0.41$	$< 0.93 \hspace{8ex}$	$1.04 \pm 0.25$	$0.65 \pm 0.20$	$0.45 \pm 0.16$
RX J0039.6+4035	43-	0	39	39.9	40	35	37	9	1	31.6	$1.18 \pm 0.28$	$< 0.33 \hspace{8ex}$	$1.00 \pm 0.21$	$< 0.50 \hspace{8ex}$	$0.66 \pm 0.16$
RX J0039.6+4048	42-	0	39	38.0	40	48	3	9	1	18.7	$1.02 \pm 0.30$	$< 1.18 \hspace{8ex}$	$0.78 \pm 0.20$	$< 0.38 \hspace{8ex}$	$0.54 \pm 0.16$
cRX J0039.6+4054	39	0	39	38.5	40	54	9	7	2	10.6	$< 0.44 \hspace{8ex}$	$0.45 \pm 0.32$	$< 0.02 \hspace{8ex}$	$< 0.01 \hspace{8ex}$	$< 0.01 \hspace{8ex}$
$\dagger$RX J0039.6+4148	41	0	39	39.6	41	48	10	12	3	28.8	$< 0.05 \hspace{8ex}$	$< 0.00 \hspace{8ex}$	$0.04 \pm 0.01$	$< 0.00 \hspace{8ex}$	$< 0.04 \hspace{8ex}$
RX J0039.7+4030	45+	0	39	47.1	40	30	5	5	1	51.2	$2.03 \pm 0.30$	$1.84 \pm 0.28$	$0.15 \pm 0.10$	$0.15 \pm 0.10$	$< 0.01 \hspace{8ex}$
aRX J0039.7+4039	44-	0	39	42.6	40	39	48	9	1	24.5	$1.03 \pm 0.26$	$< 0.34 \hspace{8ex}$	$0.79 \pm 0.18$	$0.62 \pm 0.16$	$< 0.31 \hspace{8ex}$
RX J0039.7+4116		0	39	43.0	41	16	3	20	1	15.0	$< 11.52 \hspace{8ex}$	$< 0.87 \hspace{8ex}$	$4.67 \pm 1.13$	$< 2.19 \hspace{8ex}$	$3.11 \pm 0.87$
RX J0039.8+4009	50+	0	39	53.6	40	9	2	5	1	112.2	$4.05 \pm 0.41$	$0.61 \pm 0.32$	$3.65 \pm 0.29$	$1.18 \pm 0.28$	$< 1.99 \hspace{8ex}$
RX J0039.8+4013	48	0	39	52.6	40	13	14	5	1	11.9	$0.74 \pm 0.22$	$< 0.04 \hspace{8ex}$	$< 0.67 \hspace{8ex}$	$< 0.01 \hspace{8ex}$	$< 0.64 \hspace{8ex}$
RX J0039.8+4048	49	0	39	53.3	40	48	2	5	1	14.7	$0.87 \pm 0.21$	$0.30 \pm 0.20$	$0.56 \pm 0.06$	$0.26 \pm 0.23$	$< 0.32 \hspace{8ex}$
RX J0039.8+4053	46	0	39	50.4	40	53	38	8	1	10.2	$1.07 \pm 0.25$	$0.88 \pm 0.21$	$0.12 \pm 0.10$	$< 0.03 \hspace{8ex}$	$0.09 \pm 0.06$
RX J0039.8+4055	47	0	39	50.7	40	55	28	10	1	12.0	$0.68 \pm 0.23$	$0.25 \pm 0.22$	$0.48 \pm 0.11$	$< 0.03 \hspace{8ex}$	$0.41 \pm 0.06$
RX J0039.8+4110		0	39	48.8	41	10	8	9	1	22.6	$< 2.03 \hspace{8ex}$	$< 0.35 \hspace{8ex}$	$1.51 \pm 0.39$	$< 0.88 \hspace{8ex}$	$0.88 \pm 0.29$
RX J0039.9+3929		0	39	58.1	39	29	33	37	4	10.3	$< 0.70 \hspace{8ex}$	$< 0.55 \hspace{8ex}$	$< 3.01 \hspace{8ex}$	$< 1.01 \hspace{8ex}$	$< 3.21 \hspace{8ex}$
RX J0039.9+4016	54+	0	39	58.3	40	16	33	5	1	36.1	$1.45 \pm 0.26$	$0.36 \pm 0.29$	$< 1.18 \hspace{8ex}$	$< 0.26 \hspace{8ex}$	$< 0.92 \hspace{8ex}$
RX J0039.9+4027	53+	0	39	58.1	40	27	20	5	1	105.3	$2.39 \pm 0.30$	$0.28 \pm 0.21$	$2.29 \pm 0.24$	$< 1.28 \hspace{8ex}$	$< 0.99 \hspace{8ex}$
RX J0039.9+4041	51-	0	39	56.1	40	41	6	7	1	100.5	$2.44 \pm 0.34$	$< 0.36 \hspace{8ex}$	$1.91 \pm 0.26$	$1.15 \pm 0.20$	$0.76 \pm 0.17$
RX J0039.9+4050	52	0	39	57.7	40	50	33	6	1	10.3	$0.87 \pm 0.21$	$0.53 \pm 0.17$	$0.41 \pm 0.16$	$0.17 \pm 0.04$	$0.22 \pm 0.14$
RX J0039.9+4111		0	39	56.4	41	11	39	10	1	14.0	$< 1.55 \hspace{8ex}$	$< 0.33 \hspace{8ex}$	$1.15 \pm 0.36$	$< 1.27 \hspace{8ex}$	$< 0.53 \hspace{8ex}$
RX J0040.0+4025	56	0	40	1.2	40	25	19	5	1	17.8	$0.89 \pm 0.22$	$< 0.05 \hspace{8ex}$	$< 0.78 \hspace{8ex}$	$< 0.35 \hspace{8ex}$	$< 0.52 \hspace{8ex}$
RX J0040.0+4031	55+	0	40	0.0	40	31	58	5	1	222.1	$3.89 \pm 0.37$	$0.25 \pm 0.21$	$3.98 \pm 0.34$	$1.06 \pm 0.20$	$2.26 \pm 0.20$
RX J0040.0+4033	57	0	40	1.5	40	33	7	5	1	17.7	$0.46 \pm 0.20$	$< 0.11 \hspace{8ex}$	$0.30 \pm 0.15$	$0.03 \pm 0.02$	$0.28 \pm 0.15$
RX J0040.0+4043	59	0	40	2.8	40	43	55	6	1	11.9	$0.94 \pm 0.22$	$0.57 \pm 0.16$	$0.24 \pm 0.09$	$< 0.06 \hspace{8ex}$	$0.23 \pm 0.09$
RX J0040.0+4051	60	0	40	4.0	40	51	42	5	1	20.1	$0.90 \pm 0.21$	$0.24 \pm 0.14$	$0.54 \pm 0.12$	$0.13 \pm 0.08$	$0.44 \pm 0.10$
RX J0040.0+4053	61+	0	40	5.8	40	53	2	5	1	18.4	$0.75 \pm 0.20$	$< 0.13 \hspace{8ex}$	$0.51 \pm 0.09$	$0.24 \pm 0.14$	$< 0.42 \hspace{8ex}$
RX J0040.0+4100	58+	0	40	1.6	41	0	51	7	1	30.9	$2.04 \pm 0.32$	$0.65 \pm 0.22$	$1.29 \pm 0.21$	$0.88 \pm 0.16$	$0.50 \pm 0.17$
aRX J0040.1+4006	65-	0	40	7.6	40	6	28	14	1	11.5	$< 2.23 \hspace{8ex}$	$< 1.24 \hspace{8ex}$	$< 1.27 \hspace{8ex}$	$< 0.18 \hspace{8ex}$	$< 1.34 \hspace{8ex}$
RX J0040.1+4021	62	0	40	6.6	40	21	52	5	1	10.2	$0.46 \pm 0.19$	$< 0.09 \hspace{8ex}$	$0.37 \pm 0.16$	$0.31 \pm 0.15$	$< 0.04 \hspace{8ex}$
aRX J0040.1+4044	63	0	40	8.7	40	44	42	9	1	11.7	$0.80 \pm 0.22$	$0.75 \pm 0.21$	$< 0.03 \hspace{8ex}$	$< 0.02 \hspace{8ex}$	$< 0.01 \hspace{8ex}$
aRX J0040.1+4047	64	0	40	9.2	40	47	7	5	1	27.0	$1.19 \pm 0.23$	$0.41 \pm 0.22$	$0.85 \pm 0.09$	$0.17 \pm 0.10$	$< 0.58 \hspace{8ex}$
RX J0040.1+4047	66	0	40	10.6	40	47	44	5	1	36.2	$1.43 \pm 0.24$	$0.55 \pm 0.18$	$0.82 \pm 0.15$	$0.32 \pm 0.12$	$0.47 \pm 0.09$
RX J0040.1+4059		0	40	11.3	40	59	30	9	1	16.7	$< 1.32 \hspace{8ex}$	$< 0.37 \hspace{8ex}$	$0.78 \pm 0.22$	$< 0.40 \hspace{8ex}$	$0.51 \pm 0.18$

 

Table 6: continued.

a Foreground star     b Galaxy     c Supersoft source candidate     d Globular cluster     e SNR
$\star$ bulge source     $\sim$ Variable source (ref. Tables 2, 3 and footnote in Sect. 4.1.1)     $\dagger$ Source with uncertain count rate.
RXJ	SI	RA		(J2000)		Dec		$\sigma_{\rm Pos}$	Cl.	Maxlik	Rate (B)	Rate (S)	Rate (H)	Rate ($H_{\rm 1}$)	Rate ($H_{\rm 2}$)
No.	No.	(h)	(m)	(s)	( $\hbox{$^\circ$ }$)	(')	('')	('')		(LH)	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$
(1)	(2)	(3)	(4)	(5)	(6)	(7)	(8)	(9)	(10)	(11)	(12)	(13)	(14)	(15)	(16)
RX J0040.2+3953	72-	0	40	17.7	39	53	54	8	1	99.8	$9.65 \pm 1.45$	$< 2.27 \hspace{8ex}$	$7.97 \pm 1.26$	$4.25 \pm 0.91$	$3.67 \pm 0.87$
aRX J0040.2+4015	70+	0	40	15.7	40	15	16	5	1	22.2	$1.33 \pm 0.27$	$0.69 \pm 0.44$	$< 0.74 \hspace{8ex}$	$< 0.29 \hspace{8ex}$	$< 0.39 \hspace{8ex}$
RX J0040.2+4033		0	40	13.9	40	33	52	8	1	59.8	$1.84 \pm 0.32$	$< 0.26 \hspace{8ex}$	$1.59 \pm 0.25$	$0.81 \pm 0.19$	$0.90 \pm 0.18$
$\sim$RX J0040.2+4034	69	0	40	13.9	40	34	49	5	1	14294.	$76.09 \pm 1.10$	$4.87 \pm 0.30$	$65.96 \pm 0.98$	$24.87 \pm 0.59$	$43.88 \pm 0.84$
RX J0040.2+4038	68	0	40	12.3	40	38	24	7	1	11.2	$0.87 \pm 0.22$	$0.56 \pm 0.18$	$0.25 \pm 0.10$	$< 0.06 \hspace{8ex}$	$0.21 \pm 0.07$
bRX J0040.2+4050	67-	0	40	13.5	40	50	10	5	1	16287.	$118.14 \pm 1.78$	$1.72 \pm 0.36$	$124.12 \pm 1.94$	$23.39 \pm 0.87$	$103.45 \pm 1.86$
RX J0040.3+4003		0	40	21.5	40	3	20	13	1	10.6	$< 1.87 \hspace{8ex}$	$< 0.38 \hspace{8ex}$	$< 1.90 \hspace{8ex}$	$< 0.28 \hspace{8ex}$	$1.07 \pm 0.35$
RX J0040.3+4011	71	0	40	19.2	40	11	51	11	1	10.1	$0.70 \pm 0.27$	$0.64 \pm 0.28$	$0.12 \pm 0.10$	$< 0.01 \hspace{8ex}$	$< 0.10 \hspace{8ex}$
RX J0040.3+4036	74+	0	40	22.3	40	36	11	5	1	54.8	$1.25 \pm 0.22$	$< 0.12 \hspace{8ex}$	$1.08 \pm 0.18$	$0.49 \pm 0.11$	$0.58 \pm 0.14$
dRX J0040.3+4043	73+	0	40	20.2	40	43	57	5	1	9790.0	$51.61 \pm 1.07$	$2.24 \pm 0.26$	$49.81 \pm 1.05$	$14.05 \pm 0.55$	$33.80 \pm 0.84$
RX J0040.3+4053	75+	0	40	23.7	40	53	4	5	1	49.1	$1.44 \pm 0.23$	$0.39 \pm 0.19$	$1.14 \pm 0.14$	$< 0.52 \hspace{8ex}$	$< 0.48 \hspace{8ex}$
cRX J0040.4+4009	78	0	40	26.3	40	9	1	9	1	20.5	$0.85 \pm 0.32$	$0.85 \pm 0.33$	$< 0.03 \hspace{8ex}$	$< 0.03 \hspace{8ex}$	$< 0.00 \hspace{8ex}$
RX J0040.4+4013	81	0	40	28.6	40	13	44	8	1	26.6	$0.50 \pm 0.27$	$0.39 \pm 0.23$	$< 0.03 \hspace{8ex}$	$< 0.00 \hspace{8ex}$	$< 0.03 \hspace{8ex}$
RX J0040.4+4029	76+	0	40	24.5	40	29	46	5	1	228.1	$4.00 \pm 0.38$	$< 0.13 \hspace{8ex}$	$3.61 \pm 0.31$	$1.00 \pm 0.20$	$3.14 \pm 0.29$
RX J0040.4+4034		0	40	25.3	40	34	30	10	1	11.2	$< 0.82 \hspace{8ex}$	$< 0.35 \hspace{8ex}$	$< 0.60 \hspace{8ex}$	$< 0.19 \hspace{8ex}$	$0.35 \pm 0.12$
RX J0040.4+4047	77	0	40	25.4	40	47	46	5	1	25.4	$0.72 \pm 0.17$	$< 0.09 \hspace{8ex}$	$0.61 \pm 0.14$	$0.16 \pm 0.09$	$0.49 \pm 0.12$
aRX J0040.4+4050	80	0	40	27.6	40	50	13	5	1	16.3	$1.02 \pm 0.21$	$< 0.57 \hspace{8ex}$	$< 0.53 \hspace{8ex}$	$< 0.21 \hspace{8ex}$	$< 0.30 \hspace{8ex}$
dRX J0040.4+4129	79-	0	40	25.8	41	29	12	12	1	35.6	$8.58 \pm 1.51$	$< 1.31 \hspace{8ex}$	$7.79 \pm 1.28$	$< 1.64 \hspace{8ex}$	$6.94 \pm 1.18$
RX J0040.5+3957		0	40	35.6	39	57	18	12	1	10.4	$2.55 \pm 0.80$	$< 3.27 \hspace{8ex}$	$< 0.99 \hspace{8ex}$	$< 0.44 \hspace{8ex}$	$< 0.60 \hspace{8ex}$
RX J0040.5+4001		0	40	32.1	40	1	12	11	1	16.0	$2.12 \pm 0.63$	$< 1.23 \hspace{8ex}$	$1.49 \pm 0.46$	$< 1.14 \hspace{8ex}$	$< 0.99 \hspace{8ex}$
RX J0040.5+4022	84	0	40	34.0	40	22	47	5	1	11.5	$0.88 \pm 0.23$	$< 0.15 \hspace{8ex}$	$< 0.67 \hspace{8ex}$	$< 0.28 \hspace{8ex}$	$< 0.41 \hspace{8ex}$
dRX J0040.5+4033		0	40	32.4	40	33	28	16	1	12.4	$< 1.08 \hspace{8ex}$	$< 0.42 \hspace{8ex}$	$< 0.73 \hspace{8ex}$	$< 0.16 \hspace{8ex}$	$< 0.94 \hspace{8ex}$
aRX J0040.5+4034	82	0	40	30.4	40	34	34	7	1	13.7	$1.30 \pm 0.30$	$0.76 \pm 0.20$	$0.35 \pm 0.16$	$0.31 \pm 0.16$	$< 0.06 \hspace{8ex}$
RX J0040.5+4100	83	0	40	32.9	41	0	42	5	1	36.8	$1.72 \pm 0.28$	$0.51 \pm 0.20$	$1.11 \pm 0.16$	$0.26 \pm 0.12$	$0.98 \pm 0.13$
RX J0040.6+4015	87	0	40	39.1	40	15	53	5	1	19.2	$1.39 \pm 0.31$	$1.01 \pm 0.29$	$0.50 \pm 0.15$	$0.12 \pm 0.10$	$0.38 \pm 0.11$
RX J0040.6+4022		0	40	41.0	40	22	29	11	1	12.8	$< 1.26 \hspace{8ex}$	$< 0.49 \hspace{8ex}$	$0.68 \pm 0.21$	$< 0.45 \hspace{8ex}$	$0.44 \pm 0.16$
RX J0040.6+4047	86	0	40	37.8	40	47	2	8	1	11.0	$0.94 \pm 0.21$	$< 0.53 \hspace{8ex}$	$< 0.49 \hspace{8ex}$	$< 0.19 \hspace{8ex}$	$< 0.30 \hspace{8ex}$
RX J0040.6+4108		0	40	41.8	41	8	8	19	1	10.8	$< 1.64 \hspace{8ex}$	$< 0.45 \hspace{8ex}$	$< 2.27 \hspace{8ex}$	$< 0.30 \hspace{8ex}$	$< 1.40 \hspace{8ex}$
RX J0040.6+4119	85-	0	40	38.1	41	19	39	14	1	11.1	$< 3.20 \hspace{8ex}$	$< 2.72 \hspace{8ex}$	$< 1.70 \hspace{8ex}$	$< 0.77 \hspace{8ex}$	$< 1.05 \hspace{8ex}$
RX J0040.7+3937		0	40	44.3	39	37	1	12	4	135.1	$11.01 \pm 1.57$	$< 0.85 \hspace{8ex}$	$15.23 \pm 1.32$	$6.17 \pm 0.88$	$8.30 \pm 0.97$
$\dagger$RX J0040.7+3937	91	0	40	45.3	39	37	32	6	3	90.1	$4.58 \pm 0.90$	$< 0.01 \hspace{8ex}$	$4.96 \pm 0.98$	$3.22 \pm 1.08$	$< 1.60 \hspace{8ex}$
$\sim$RX J0040.7+3959		0	40	42.3	39	59	7	8	1	50.8	$5.54 \pm 1.01$	$< 1.89 \hspace{8ex}$	$3.97 \pm 0.77$	$2.55 \pm 0.63$	$1.54 \pm 0.47$
cRX J0040.7+4015	88	0	40	43.2	40	15	18	7	1	33.7	$1.26 \pm 0.32$	$1.17 \pm 0.31$	$< 0.03 \hspace{8ex}$	$< 0.03 \hspace{8ex}$	$< 0.01 \hspace{8ex}$
RX J0040.7+4027	93	0	40	46.5	40	27	18	10	1	12.2	$1.22 \pm 0.30$	$1.11 \pm 0.26$	$< 0.19 \hspace{8ex}$	$0.16 \pm 0.15$	$< 0.01 \hspace{8ex}$
RX J0040.7+4032	89+	0	40	43.2	40	32	41	5	1	13.2	$0.74 \pm 0.22$	$0.19 \pm 0.16$	$0.46 \pm 0.10$	$< 0.30 \hspace{8ex}$	$< 0.25 \hspace{8ex}$
RX J0040.7+4048	90	0	40	44.0	40	48	50	5	1	17.8	$0.60 \pm 0.16$	$< 0.10 \hspace{8ex}$	$0.43 \pm 0.07$	$< 0.05 \hspace{8ex}$	$< 0.40 \hspace{8ex}$
RX J0040.7+4051	92+	0	40	45.8	40	51	31	5	1	74.6	$1.81 \pm 0.24$	$0.36 \pm 0.17$	$1.36 \pm 0.15$	$0.51 \pm 0.16$	$1.02 \pm 0.08$
eRX J0040.7+4055	94	0	40	47.6	40	55	24	5	1	18.7	$0.95 \pm 0.20$	$0.32 \pm 0.17$	$0.53 \pm 0.06$	$< 0.30 \hspace{8ex}$	$< 0.29 \hspace{8ex}$
aRX J0040.8+4011	95+	0	40	48.8	40	11	25	5	1	548.0	$14.10 \pm 0.73$	$11.73 \pm 0.63$	$1.66 \pm 0.28$	$0.71 \pm 0.22$	$1.07 \pm 0.20$
RX J0040.8+4021	100-	0	40	51.6	40	21	12	9	1	15.5	$< 1.04 \hspace{8ex}$	$< 0.23 \hspace{8ex}$	$0.75 \pm 0.22$	$< 0.58 \hspace{8ex}$	$< 0.53 \hspace{8ex}$
RX J0040.8+4030	96+	0	40	48.9	40	30	27	6	1	38.9	$1.63 \pm 0.29$	$0.51 \pm 0.27$	$1.26 \pm 0.17$	$0.47 \pm 0.20$	$< 0.69 \hspace{8ex}$
RX J0040.8+4049	97	0	40	49.2	40	49	27	5	1	19.3	$0.57 \pm 0.16$	$< 0.06 \hspace{8ex}$	$0.50 \pm 0.14$	$0.12 \pm 0.07$	$0.36 \pm 0.12$
RX J0040.8+4132	99-	0	40	53.3	41	32	46	11	1	20.0	$2.26 \pm 0.67$	$< 0.90 \hspace{8ex}$	$2.03 \pm 0.54$	$< 1.20 \hspace{8ex}$	$1.32 \pm 0.44$
RX J0040.8+4153	98-	0	40	48.0	41	53	2	15	4	35.2	$< 0.81 \hspace{8ex}$	$< 0.11 \hspace{8ex}$	$3.59 \pm 0.53$	$1.21 \pm 0.31$	$3.60 \pm 0.49$
RX J0040.9+4003		0	40	58.6	40	3	45	11	1	10.6	$< 2.23 \hspace{8ex}$	$< 0.67 \hspace{8ex}$	$1.08 \pm 0.39$	$< 0.75 \hspace{8ex}$	$< 0.82 \hspace{8ex}$
aRX J0040.9+4056	101	0	40	57.1	40	56	43	5	1	27.1	$1.15 \pm 0.22$	$0.38 \pm 0.16$	$0.65 \pm 0.11$	$0.44 \pm 0.04$	$0.26 \pm 0.12$
RX J0041.0+4022	102	0	41	0.3	40	22	3	9	1	16.4	$1.43 \pm 0.34$	$< 1.11 \hspace{8ex}$	$< 0.21 \hspace{8ex}$	$< 0.03 \hspace{8ex}$	$< 0.20 \hspace{8ex}$
RX J0041.0+4027	103+	0	41	5.7	40	27	6	5	1	46.0	$1.88 \pm 0.35$	$< 0.03 \hspace{8ex}$	$1.78 \pm 0.16$	$0.38 \pm 0.21$	$< 1.50 \hspace{8ex}$
RX J0041.0+4123		0	41	4.8	41	23	58	10	1	24.4	$2.86 \pm 0.60$	$< 1.87 \hspace{8ex}$	$2.12 \pm 0.48$	$1.19 \pm 0.33$	$< 1.32 \hspace{8ex}$

 

Table 6: continued.

a Foreground star     b Galaxy     c Supersoft source candidate     d Globular cluster     e SNR
$\star$ bulge source     $\sim$ Variable source (ref. Tables 2, 3 and footnote in Sect. 4.1.1)     $\dagger$ Source with uncertain count rate.
RXJ	SI	RA		(J2000)		Dec		$\sigma_{\rm Pos}$	Cl.	Maxlik	Rate (B)	Rate (S)	Rate (H)	Rate ($H_{\rm 1}$)	Rate ($H_{\rm 2}$)
No.	No.	(h)	(m)	(s)	( $\hbox{$^\circ$ }$)	(')	('')	('')		(LH)	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$
(1)	(2)	(3)	(4)	(5)	(6)	(7)	(8)	(9)	(10)	(11)	(12)	(13)	(14)	(15)	(16)
$\sim$RX J0041.1+4002	104-	0	41	6.9	40	2	51	10	1	45.4	$5.57 \pm 1.01$	$< 1.49 \hspace{8ex}$	$4.08 \pm 0.80$	$1.42 \pm 0.47$	$3.04 \pm 0.70$
RX J0041.1+4050		0	41	7.3	40	50	57	9	1	20.8	$1.11 \pm 0.27$	$< 0.44 \hspace{8ex}$	$0.72 \pm 0.18$	$< 0.33 \hspace{8ex}$	$0.47 \pm 0.13$
RX J0041.1+4054	105+	0	41	11.9	40	54	16	5	1	88.3	$1.93 \pm 0.25$	$0.36 \pm 0.16$	$1.39 \pm 0.16$	$0.40 \pm 0.13$	$1.22 \pm 0.13$
RX J0041.2+4016		0	41	15.9	40	16	48	9	1	23.4	$1.73 \pm 0.46$	$< 0.60 \hspace{8ex}$	$1.26 \pm 0.32$	$< 0.78 \hspace{8ex}$	$0.71 \pm 0.24$
RX J0041.2+4049		0	41	14.7	40	49	1	12	1	10.7	$1.00 \pm 0.27$	$< 1.12 \hspace{8ex}$	$< 0.27 \hspace{8ex}$	$< 0.11 \hspace{8ex}$	$< 0.22 \hspace{8ex}$
RX J0041.2+4101	106-	0	41	15.8	41	1	7	8	1	46.7	$1.81 \pm 0.33$	$< 0.40 \hspace{8ex}$	$1.37 \pm 0.24$	$< 0.65 \hspace{8ex}$	$0.92 \pm 0.19$
bRX J0041.3+4012	110	0	41	23.8	40	12	17	18	2	13.3	$1.48 \pm 0.48$	$< 0.22 \hspace{8ex}$	$1.13 \pm 0.33$	$0.36 \pm 0.22$	$0.83 \pm 0.26$
aRX J0041.3+4051	107+	0	41	18.3	40	51	57	5	1	435.8	$5.51 \pm 0.37$	$1.05 \pm 0.20$	$4.14 \pm 0.29$	$1.79 \pm 0.24$	$2.80 \pm 0.22$
RX J0041.3+4103	108	0	41	20.9	41	3	38	5	1	12.9	$1.02 \pm 0.32$	$0.27 \pm 0.23$	$0.71 \pm 0.20$	$0.20 \pm 0.16$	$0.54 \pm 0.14$
aRX J0041.3+4109	109	0	41	23.3	41	9	37	30	2	14.2	$0.57 \pm 0.37$	$0.49 \pm 0.34$	$0.03 \pm 0.02$	$< 0.02 \hspace{8ex}$	$< 0.01 \hspace{8ex}$
aRX J0041.4+4025		0	41	28.5	40	25	51	9	1	17.6	$< 1.37 \hspace{8ex}$	$< 0.36 \hspace{8ex}$	$0.91 \pm 0.26$	$< 0.44 \hspace{8ex}$	$0.58 \pm 0.20$
RX J0041.4+4053	112+	0	41	26.3	40	53	23	5	1	179.9	$3.01 \pm 0.29$	$0.48 \pm 0.18$	$2.65 \pm 0.25$	$1.06 \pm 0.20$	$1.44 \pm 0.12$
RX J0041.4+4058	111+	0	41	25.9	40	58	42	5	1	560.5	$7.23 \pm 0.46$	$0.31 \pm 0.16$	$6.05 \pm 0.37$	$2.23 \pm 0.26$	$5.27 \pm 0.37$
RX J0041.4+4102	113	0	41	27.6	41	2	32	6	1	11.4	$0.72 \pm 0.28$	$< 0.06 \hspace{8ex}$	$0.70 \pm 0.22$	$< 0.40 \hspace{8ex}$	$< 0.32 \hspace{8ex}$
RX J0041.4+4136		0	41	24.8	41	36	51	11	1	12.4	$< 1.51 \hspace{8ex}$	$< 0.49 \hspace{8ex}$	$1.07 \pm 0.34$	$0.80 \pm 0.28$	$< 0.37 \hspace{8ex}$
RX J0041.5+4028		0	41	34.6	40	28	56	10	1	14.3	$< 1.50 \hspace{8ex}$	$< 0.70 \hspace{8ex}$	$0.71 \pm 0.22$	$< 0.21 \hspace{8ex}$	$0.57 \pm 0.19$
cRX J0041.5+4040	114	0	41	30.2	40	40	4	6	1	13.1	$0.32 \pm 0.18$	$0.28 \pm 0.17$	$< 0.01 \hspace{8ex}$	$< 0.01 \hspace{8ex}$	$< 0.00 \hspace{8ex}$
$\sim$RX J0041.5+4105		0	41	31.3	41	5	55	6	1	901.2	$12.36 \pm 0.69$	$< 0.19 \hspace{8ex}$	$11.92 \pm 0.64$	$2.84 \pm 0.32$	$9.27 \pm 0.56$
eRX J0041.5+4106	116	0	41	35.8	41	6	57	5	1	23.8	$1.18 \pm 0.30$	$< 0.15 \hspace{8ex}$	$0.87 \pm 0.10$	$< 0.45 \hspace{8ex}$	$< 0.51 \hspace{8ex}$
RX J0041.5+4117	115+	0	41	34.1	41	17	38	8	1	22.2	$1.85 \pm 0.38$	$0.50 \pm 0.38$	$1.46 \pm 0.12$	$0.31 \pm 0.20$	$< 1.04 \hspace{8ex}$
RX J0041.5+4140		0	41	35.9	41	40	6	11	1	14.3	$< 1.95 \hspace{8ex}$	$< 0.51 \hspace{8ex}$	$1.03 \pm 0.35$	$0.91 \pm 0.30$	$< 0.28 \hspace{8ex}$
RX J0041.6+4031		0	41	41.1	40	31	22	10	1	28.4	$1.75 \pm 0.42$	$< 0.54 \hspace{8ex}$	$1.46 \pm 0.30$	$0.64 \pm 0.20$	$0.72 \pm 0.21$
RX J0041.6+4100		0	41	41.3	41	0	10	5	1	16.5	$< 2.12 \hspace{8ex}$	$< 0.33 \hspace{8ex}$	$1.76 \pm 0.36$	$< 0.16 \hspace{8ex}$	$0.56 \pm 0.16$
$\sim$RX J0041.6+4101	118-	0	41	37.6	41	1	13	8	1	85.8	$3.10 \pm 0.40$	$< 1.31 \hspace{8ex}$	$2.30 \pm 0.30$	$0.71 \pm 0.18$	$1.56 \pm 0.24$
aRX J0041.6+4103	119-	0	41	41.4	41	3	32	8	1	46.6	$1.84 \pm 0.33$	$< 0.36 \hspace{8ex}$	$1.45 \pm 0.25$	$0.66 \pm 0.17$	$0.80 \pm 0.19$
aRX J0041.6+4112	117	0	41	36.5	41	12	18	5	1	21.6	$1.21 \pm 0.30$	$< 0.13 \hspace{8ex}$	$1.13 \pm 0.16$	$0.44 \pm 0.30$	$< 0.63 \hspace{8ex}$
RX J0041.7+4021		0	41	44.7	40	22	0	5	1	52.1	$19.66 \pm 1.52$	$< 3.94 \hspace{8ex}$	$5.15 \pm 0.70$	$2.37 \pm 0.48$	$2.58 \pm 0.49$
RX J0041.7+4034	123+	0	41	45.6	40	34	39	5	1	24.5	$1.18 \pm 0.27$	$0.48 \pm 0.23$	$0.63 \pm 0.10$	$0.32 \pm 0.25$	$< 0.40 \hspace{8ex}$
RX J0041.7+4036		0	41	45.7	40	36	24	10	1	10.6	$< 0.98 \hspace{8ex}$	$< 0.92 \hspace{8ex}$	$< 0.56 \hspace{8ex}$	$< 0.12 \hspace{8ex}$	$0.33 \pm 0.13$
aRX J0041.7+4105	121+	0	41	43.4	41	5	5	5	1	135.6	$3.85 \pm 0.44$	$0.88 \pm 0.34$	$3.33 \pm 0.35$	$< 1.64 \hspace{8ex}$	$< 1.47 \hspace{8ex}$
RX J0041.7+4107	124	0	41	46.2	41	7	15	8	1	10.0	$0.63 \pm 0.25$	$< 0.06 \hspace{8ex}$	$0.56 \pm 0.11$	$< 0.39 \hspace{8ex}$	$< 0.20 \hspace{8ex}$
RX J0041.7+4121		0	41	44.1	41	21	19	10	1	26.2	$1.11 \pm 0.33$	$< 0.62 \hspace{8ex}$	$1.60 \pm 0.34$	$< 0.14 \hspace{8ex}$	$0.92 \pm 0.23$
RX J0041.7+4126		0	41	45.2	41	26	25	8	1	49.2	$2.37 \pm 0.46$	$< 0.55 \hspace{8ex}$	$1.91 \pm 0.35$	$0.77 \pm 0.23$	$1.01 \pm 0.25$
RX J0041.7+4131		0	41	47.2	41	31	55	9	1	53.5	$3.08 \pm 0.56$	$< 0.54 \hspace{8ex}$	$3.00 \pm 0.46$	$0.95 \pm 0.27$	$1.62 \pm 0.34$
$\sim^d$RX J0041.7+4134	122-	0	41	43.2	41	34	22	6	1	3463.9	$53.70 \pm 1.83$	$< 1.12 \hspace{8ex}$	$51.53 \pm 1.75$	$14.74 \pm 0.94$	$37.07 \pm 1.49$
RX J0041.7+4217	120	0	41	43.0	42	17	45	20	3	11.5	$< 0.06 \hspace{8ex}$	$< 0.03 \hspace{8ex}$	$0.03 \pm 0.02$	$< 0.00 \hspace{8ex}$	$< 0.03 \hspace{8ex}$
$\sim$RX J0041.8+4015	129-	0	41	49.9	40	15	26	8	1	62.0	$7.02 \pm 1.04$	$2.80 \pm 0.76$	$3.60 \pm 0.68$	$< 2.33 \hspace{8ex}$	$2.20 \pm 0.51$
$\sim^b$RX J0041.8+4021	134-	0	41	52.6	40	21	24	6	1	3614.5	$90.56 \pm 2.85$	$10.27 \pm 1.06$	$76.44 \pm 2.59$	$36.93 \pm 1.80$	$41.22 \pm 1.91$
RX J0041.8+4028		0	41	48.7	40	28	14	10	1	13.0	$< 1.08 \hspace{8ex}$	$< 0.42 \hspace{8ex}$	$0.73 \pm 0.25$	$< 0.27 \hspace{8ex}$	$0.61 \pm 0.21$
RX J0041.8+4046	131	0	41	51.5	40	46	52	7	1	14.7	$0.50 \pm 0.21$	$0.44 \pm 0.21$	$< 0.08 \hspace{8ex}$	$< 0.05 \hspace{8ex}$	$< 0.03 \hspace{8ex}$
cRX J0041.8+4059	128	0	41	49.9	40	59	21	9	1	12.3	$0.49 \pm 0.24$	$0.46 \pm 0.24$	$0.02 \pm 0.01$	$< 0.01 \hspace{8ex}$	$< 0.00 \hspace{8ex}$
$\sim$RX J0041.8+4101	127+	0	41	49.8	41	1	9	5	1	710.7	$11.73 \pm 0.71$	$1.28 \pm 0.30$	$9.54 \pm 0.58$	$3.52 \pm 0.41$	$7.37 \pm 0.52$
RX J0041.8+4110	133	0	41	52.4	41	10	40	5	1	39.8	$1.72 \pm 0.33$	$< 0.18 \hspace{8ex}$	$1.69 \pm 0.23$	$< 0.82 \hspace{8ex}$	$< 0.83 \hspace{8ex}$
RX J0041.8+4113	130+	0	41	50.7	41	13	36	5	1	34.9	$1.61 \pm 0.33$	$< 0.06 \hspace{8ex}$	$1.45 \pm 0.08$	$0.21 \pm 0.16$	$< 1.25 \hspace{8ex}$
RX J0041.8+4114	132-	0	41	51.9	41	14	49	8	1	46.2	$1.85 \pm 0.36$	$< 0.40 \hspace{8ex}$	$1.84 \pm 0.31$	$0.63 \pm 0.18$	$1.21 \pm 0.25$
$\sim$RX J0041.8+4122	126+	0	41	49.2	41	22	23	5	1	217.3	$6.11 \pm 0.58$	$< 0.17 \hspace{8ex}$	$6.27 \pm 0.58$	$1.70 \pm 0.32$	$4.49 \pm 0.48$
RX J0041.8+4151	125-	0	41	51.3	41	51	53	11	1	14.3	$3.28 \pm 0.91$	$< 1.80 \hspace{8ex}$	$1.94 \pm 0.66$	$< 1.43 \hspace{8ex}$	$< 1.17 \hspace{8ex}$
eRX J0041.9+4046	0	41	55.6	40	46	49	15	1	15.1	$< 2.96 \hspace{8ex}$	$< 0.17 \hspace{8ex}$	$2.82 \pm 0.42$	$< 0.92 \hspace{8ex}$	$1.22 \pm 0.25$
RX J0041.9+4133	0	41	54.7	41	33	38	8	1	45.1	$2.10 \pm 0.44$	$< 0.48 \hspace{8ex}$	$1.76 \pm 0.34$	$0.78 \pm 0.23$	$0.91 \pm 0.24$
RX J0042.0+4024	137-	0	42	3.0	40	24	16	10	1	45.9	$3.24 \pm 0.68$	$< 0.62 \hspace{8ex}$	$3.79 \pm 0.64$	$1.56 \pm 0.41$	$2.06 \pm 0.47$
RX J0042.0+4028		0	42	3.2	40	28	56	8	1	46.0	$2.19 \pm 0.47$	$< 0.37 \hspace{8ex}$	$1.84 \pm 0.37$	$0.77 \pm 0.24$	$1.03 \pm 0.28$
aRX J0042.0+4031		0	42	2.6	40	31	18	10	1	16.0	$< 1.40 \hspace{8ex}$	$< 0.49 \hspace{8ex}$	$0.77 \pm 0.24$	$< 0.52 \hspace{8ex}$	$< 0.57 \hspace{8ex}$
aRX J0042.0+4033		0	42	3.3	40	33	8	10	1	12.3	$< 1.15 \hspace{8ex}$	$< 0.39 \hspace{8ex}$	$0.67 \pm 0.22$	$< 0.66 \hspace{8ex}$	$< 0.32 \hspace{8ex}$
aRX J0042.0+4041	135+	0	42	1.0	40	41	15	5	1	331.0	$5.96 \pm 0.44$	$4.91 \pm 0.39$	$0.76 \pm 0.16$	$0.51 \pm 0.12$	$0.28 \pm 0.11$
RX J0042.0+4046	136-	0	42	2.7	40	46	15	8	1	42.1	$1.50 \pm 0.32$	$< 0.44 \hspace{8ex}$	$1.06 \pm 0.22$	$< 0.83 \hspace{8ex}$	$0.91 \pm 0.19$

 

Table 6: continued.

a Foreground star     b Galaxy     c Supersoft source candidate    d Globular cluster     e SNR
$\star$ bulge source     $\sim$ Variable source (ref. Tables 2, 3 and footnote in Sect. 4.1.1)     $\dagger$ Source with uncertain count rate.
RXJ	SI	RA		(J2000)		Dec		$\sigma_{\rm Pos}$	Cl.	Maxlik	Rate (B)	Rate (S)	Rate (H)	Rate ($H_{\rm 1}$)	Rate ($H_{\rm 2}$)
No.	No.	(h)	(m)	(s)	( $\hbox{$^\circ$ }$)	(')	('')	('')		(LH)	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$	$\rm (ct \cdot ks^{-1})$
(1)	(2)	(3)	(4)	(5)	(6)	(7)	(8)	(9)	(10)	(11)	(12)	(13)	(14)	(15)	(16)
dRX J0042.0+4102	138+	0	42	5.4	41	2	51	5	1	60.0	$1.94 \pm 0.34$	$< 0.11 \hspace{8ex}$	$1.67 \pm 0.26$	$0.48 \pm 0.17$	$1.16 \pm 0.18$
aRX J0042.1+4016		0	42	9.6	40	16	47	9	1	36.0	$4.96 \pm 1.07$	$< 1.17 \hspace{8ex}$	$3.77 \pm 0.83$	$1.66 \pm 0.55$	$2.06 \pm 0.60$
RX J0042.1+4053	143	0	42	11.2	40	53	32	9	1	15.5	$0.95 \pm 0.26$	$0.44 \pm 0.18$	$0.38 \pm 0.14$	$0.33 \pm 0.13$	$0.13 \pm 0.11$
RX J0042.1+4100	139+	0	42	7.1	41	0	19	5	1	76.2	$2.07 \pm 0.34$	$< 0.15 \hspace{8ex}$	$1.81 \pm 0.29$	$0.46 \pm 0.16$	$1.45 \pm 0.26$
RX J0042.1+4104	140+	0	42	8.2	41	4	38	5	1	72.4	$2.16 \pm 0.35$	$< 0.05 \hspace{8ex}$	$2.07 \pm 0.26$	$0.70 \pm 0.23$	$1.48 \pm 0.14$
$\sim$RX J0042.1+4110	144+	0	42	11.4	41	10	54	5	1	144.5	$4.20 \pm 0.46$	$0.75 \pm 0.34$	$3.60 \pm 0.34$	$0.80 \pm 0.23$	$2.59 \pm 0.22$
$\sim$RX J0042.1+4118	141-	0	42	9.0	41	18	19	5	1	970.6	$35.01 \pm 1.21$	$< 0.32 \hspace{8ex}$	$27.80 \pm 1.01$	$5.76 \pm 0.48$	$21.32 \pm 0.88$
RX J0042.1+4120	142+	0	42	9.3	41	20	40	5	1	64.7	$2.68 \pm 0.42$	$0.34 \pm 0.30$	$2.23 \pm 0.28$	$0.22 \pm 0.16$	$1.89 \pm 0.21$
$\sim$RX J0042.2+4019		0	42	15.2	40	19	45	6	1	3894.8	$150.77 \pm 4.58$	$14.56 \pm 1.57$	$125.26 \pm 4.09$	$43.66 \pm 2.43$	$80.55 \pm 3.27$
$\sim$RX J0042.2+4039	148-	0	42	13.5	40	39	25	6	1	329.3	$8.12 \pm 0.71$	$< 1.30 \hspace{8ex}$	$6.62 \pm 0.59$	$2.20 \pm 0.34$	$4.45 \pm 0.48$
RX J0042.2+4048	156-	0	42	16.3	40	48	18	11	1	13.9	$< 1.22 \hspace{8ex}$	$< 0.43 \hspace{8ex}$	$0.84 \pm 0.22$	$0.57 \pm 0.17$	$< 0.27 \hspace{8ex}$
$\sim$RX J0042.2+4055	153+	0	42	16.4	40	55	55	5	1	545.2	$10.13 \pm 0.69$	$0.59 \pm 0.28$	$9.43 \pm 0.62$	$3.32 \pm 0.40$	$6.60 \pm 0.52$
$\sim^d$RX J0042.2+4101	150+	0	42	15.6	41	1	16	5	1	3624.9	$35.60 \pm 1.18$	$0.66 \pm 0.27$	$38.05 \pm 1.25$	$5.87 \pm 0.49$	$30.64 \pm 1.10$
aRX J0042.2+4105	147	0	42	13.0	41	5	57	5	1	16.3	$1.19 \pm 0.29$	$0.43 \pm 0.24$	$0.67 \pm 0.11$	$< 0.44 \hspace{8ex}$	$< 0.28 \hspace{8ex}$
RX J0042.2+4109	149	0	42	14.7	41	9	24	7	1	11.8	$0.97 \pm 0.28$	$0.59 \pm 0.22$	$0.28 \pm 0.13$	$0.12 \pm 0.11$	$0.22 \pm 0.10$
$\sim$RX J0042.2+4112	155-	0	42	17.7	41	12	29	5	1	2282.0	$33.74 \pm 0.95$	$3.22 \pm 0.51$	$35.36 \pm 1.11$	$13.32 \pm 0.68$	$21.68 \pm 0.87$
RX J0042.2+4115	145+	0	42	12.1	41	15	0	5	1	46.9	$1.37 \pm 0.32$	$< 0.20 \hspace{8ex}$	$1.15 \pm 0.23$	$0.33 \pm 0.17$	$0.79 \pm 0.15$
RX J0042.2+4117	151	0	42	15.9	41	17	17	5	1	472.7	$8.13 \pm 0.60$	$0.39 \pm 0.22$	$6.78 \pm 0.48$	$1.35 \pm 0.25$	$6.04 \pm 0.46$
$\sim^a$RX J0042.2+4118	146-	0	42	12.4	41	18	31	5	1	1492.6	$36.25 \pm 1.21$	$< 0.38 \hspace{8ex}$	$33.07 \pm 1.10$	$8.65 \pm 0.60$	$29.48 \pm 1.04$
RX J0042.2+4120	152-	0	42	15.6	41	20	31	8	1	47.9	$2.06 \pm 0.37$	$< 0.27 \hspace{8ex}$	$1.79 \pm 0.30$	$0.56 \pm 0.17$	$1.18 \pm 0.24$
RX J0042.2+4131	154+	0	42	17.0	41	31	12	8	1	12.5	$0.82 \pm 0.37$	$0.30 \pm 0.19$	$0.50 \pm 0.31$	$0.04 \pm 0.03$	$0.46 \pm 0.31$
RX J0042.3+4019		0	42	22.9	40	19	42	7	1	815.9	$94.42 \pm 4.08$	$6.63 \pm 1.45$	$48.60 \pm 2.78$	$16.05 \pm 1.63$	$30.90 \pm 2.20$
RX J0042.3+4019	159	0	42	19.7	40	19	48	5	2	5459.9	$136.24 \pm 1.23$	$18.99 \pm 0.50$	$114.45 \pm 1.09$	$48.72 \pm 0.68$	$79.06 \pm 1.02$
RX J0042.3+4044		0	42	22.6	40	44	18	9	1	35.1	$1.26 \pm 0.32$	$< 0.48 \hspace{8ex}$	$0.96 \pm 0.23$	$< 0.19 \hspace{8ex}$	$0.90 \pm 0.21$
RX J0042.3+4059	162+	0	42	22.1	40	59	26	5	1	686.1	$10.93 \pm 0.68$	$1.19 \pm 0.32$	$10.27 \pm 0.64$	$3.43 \pm 0.40$	$7.20 \pm 0.53$
RX J0042.3+4104	161	0	42	20.5	41	4	48	5	1	10.5	$0.98 \pm 0.28$	$0.63 \pm 0.25$	$0.37 \pm 0.15$	$0.30 \pm 0.11$	$< 0.10 \hspace{8ex}$
RX J0042.3+4107	164+	0	42	23.0	41	7	31	5	1	63.5	$2.27 \pm 0.35$	$0.47 \pm 0.25$	$2.02 \pm 0.29$	$< 0.90 \hspace{8ex}$	$< 0.81 \hspace{8ex}$
RX J0042.3+4112	160	0	42	20.3	41	12	10	5	1	26.2	$11.22 \pm 0.73$	$0.88 \pm 0.25$	$9.63 \pm 0.64$	$3.45 \pm 0.34$	$6.17 \pm 0.54$
$\sim^d$RX J0042.3+4113	158+	0	42	19.3	41	13	59	5	1	1416.1	$18.74 \pm 0.87$	$1.79 \pm 0.30$	$14.45 \pm 0.69$	$5.07 \pm 0.45$	$12.14 \pm 0.69$
$\star$RX J0042.3+4113	165+	0	42	24.0	41	13	46	5	1	870.2	$12.31 \pm 0.76$	$1.46 \pm 0.30$	$9.58 \pm 0.61$	$2.62 \pm 0.34$	$7.83 \pm 0.57$
$\star$RX J0042.3+4115	163+	0	42	22.8	41	15	36	5	1	6200.4	$59.95 \pm 1.52$	$3.58 \pm 0.43$	$59.84 \pm 1.55$	$17.86 \pm 0.85$	$42.88 \pm 1.32$
aRX J0042.3+4126		0	42	20.3	41	26	41	9	1	27.9	$1.69 \pm 0.37$	$< 0.40 \hspace{8ex}$	$1.37 \pm 0.28$	$< 0.63 \hspace{8ex}$	$0.91 \pm 0.23$
bRX J0042.3+4129	157+	0	42	18.1	41	29	17	8	1	24.3	$1.27 \pm 0.43$	$0.35 \pm 0.27$	$0.88 \pm 0.32$	$< 0.05 \hspace{8ex}$	$0.77 \pm 0.30$
RX J0042.3+4147		0	42	20.2	41	47	46	12	1	10.1	$< 1.12 \hspace{8ex}$	$< 0.39 \hspace{8ex}$	$0.79 \pm 0.30$	$< 0.47 \hspace{8ex}$	$< 0.72 \hspace{8ex}$
RX J0042.4+3947		0	42	24.8	39	47	38	26	4	10.2	$< 0.78 \hspace{8ex}$	$< 0.32 \hspace{8ex}$	$< 3.91 \hspace{8ex}$	$< 0.85 \hspace{8ex}$	$2.58 \pm 0.67$
RX J0042.4+4028	169-	0	42	25.0	40	28	30	14	1	12.3	$< 2.00 \hspace{8ex}$	$< 0.35 \hspace{8ex}$	$< 2.31 \hspace{8ex}$	$< 0.33 \hspace{8ex}$	$< 2.18 \hspace{8ex}$
cRX J0042.4+4044	171	0	42	27.6	40	44	32	5	1	54.3	$1.69 \pm 0.32$	$1.59 \pm 0.31$	$< 0.06 \hspace{8ex}$	$< 0.03 \hspace{8ex}$	$< 0.03 \hspace{8ex}$
aRX J0042.4+4055	170	0	42	27.0	40	55	24	5	1	62.1	$1.36 \pm 0.33$	$< 0.08 \hspace{8ex}$	$1.29 \pm 0.33$	$< 0.01 \hspace{8ex}$	$1.33 \pm 0.33$
dRX J0042.4+4057	168+	0	42	25.1	40	57	23	5	1	24.0	$1.19 \pm 0.31$	$0.31 \pm 0.28$	$0.86 \pm 0.12$	$< 0.09 \hspace{8ex}$	$0.82 \pm 0.03$
$\sim$RX J0042.4+4104	173-	0	42	29.1	41	4	35	6	1	1118.4	$17.85 \pm 0.83$	$< 1.17 \hspace{8ex}$	$15.22 \pm 0.74$	$5.04 \pm 0.43$	$10.24 \pm 0.60$
aRX J0042.4+4108		0	42	29.2	41	8	26	8	1	43.0	$2.41 \pm 0.39$	$< 2.06 \hspace{8ex}$	$1.59 \pm 0.28$	$0.64 \pm 0.18$	$0.98 \pm 0.21$
RX J0042.4+4110	166	0	42	24.6	41	10	19	6	1	17.4	$1.38 \pm 0.33$	$0.75 \pm 0.16$	$0.60 \pm 0.28$	$< 0.32 \hspace{8ex}$	$< 0.33 \hspace{8ex}$
$\sim$RX J0042.4+4112	172+	0	42	28.5	41	12	19	5	1	1782.2	$22.09 \pm 0.94$	$2.12 \pm 0.39$	$21.65 \pm 0.93$	$6.24 \pm 0.51$	$13.09 \pm 0.65$
$\star$RX J0042.4+4114		0	42	29.7	41	14	30	5	1	317.8	$154.67 \pm 1.01$	$7.28 \pm 0.68$	$97.14 \pm 1.08$	$35.21 \pm 1.10$	$42.28 \pm 1.04$
$\star$RX J0042.4+4119		0	42	27.6	41	19	21	5	1	131.9	$9.20 \pm 0.62$	$< 0.40 \hspace{8ex}$	$8.01 \pm 0.59$	$2.25 \pm 0.34$	$5.37 \pm 0.48$
RX J0042.4+4125	167-	0	42	26.4	41	25	54	7	1	128.8	$4.21 \pm 0.50$	$< 0.25 \hspace{8ex}$	$3.95 \pm 0.43$	$0.85 \pm 0.21$	$3.02 \pm 0.37$
aRX J0042.4+4129	174-	0	42	29.6	41	29	3	8	1	51.7	$1.52 \pm 0.35$	$< 0.39 \hspace{8ex}$	$1.63 \pm 0.28$	$0.54 \pm 0.17$	$1.15 \pm 0.23$
RX J0042.4+4145		0	42	26.9	41	45	30	10	1	15.3	$< 1.04 \hspace{8ex}$	$< 0.22 \hspace{8ex}$	$1.06 \pm 0.31$	$< 0.56 \hspace{8ex}$	$0.66 \pm 0.23$
RX J0042.5+4040		0	42	35.0	40	40	35	11	1	12.9	$< 1.26 \hspace{8ex}$	$< 0.44 \hspace{8ex}$	$0.82 \pm 0.25$	$< 0.41 \hspace{8ex}$	$0.60 \pm 0.21$