The Chinese pulsar timing array data release I - Polarimetry for 56 millisecond pulsars

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Table 1.

Pulse width and polarization degree of CPTA pulsars. The total, linear, circular, and absolute circular degree of polarization are $Π_{P} \equiv \frac{⟨ P ⟩}{⟨ I ⟩}$ $\Pi_{\mathrm{P}}\equiv\frac{\langle P\rangle}{\langle I\rangle}$ , $Π_{L} \equiv \frac{⟨ L ⟩}{⟨ I ⟩}$ $\Pi_{\mathrm{L}}\equiv\frac{\langle L\rangle}{\langle I\rangle}$ , $Π_{V} \equiv \frac{⟨ V ⟩}{⟨ I ⟩}$ $\Pi_{\mathrm{V}}\equiv\frac{\langle V\rangle}{\langle I\rangle}$ , and $Π_{| V |} \equiv \frac{⟨ | V | ⟩}{⟨ I ⟩}$ $\Pi_{\mathrm{|V|}}\equiv\frac{\langle |V|\rangle}{\langle I\rangle}$ , where the phase average is denoted with ⟨⟩. The detectable pulse width and the effective width are W_det and W_eff, respectively.

Pulsar	W_det	W_eff	Π_P	Π_L	Π_V	Π_\|V\|
	%	%	%	%	%	%
J0023+0923	40.1	7.8	30.6	30.0	3.3	4.4
J0030+0451	82.1	14.3	33.4	33.1	0.8	3.1
J0034−0534	71.9	25.5	17.9	9.4	−12.1	12.1
J0154+1833	22.6	5.2	32.2	31.8	0.7	4.1
J0340+4130	81.2	9.3	19.4	18.9	−2.5	2.9
J0406+3039	57.5	10.3	33.9	32.0	−5.4	8.8
J0509+0856	96.7	28.2	35.3	34.0	1.6	4.5
J0605+3757	45.0	9.6	46.5	46.6	−0.3	0.4
J0613−0200	66.5	16.6	19.9	19.6	0.6	3.1
J0621+1002	57.4	5.1	28.1	21.3	−16.2	16.3
J0636+5128	28.2	5.6	40.3	38.1	−2.2	6.3
J0645+5158	38.7	2.4	22.0	20.0	0.9	6.7
J0732+2314	82.3	28.6	33.2	23.6	17.5	21.1
J0751+1807	82.3	11.2	30.5	27.3	−9.3	11.6
J0824+0028	66.8	13.5	47.6	45.1	6.5	11.3
J1012+5307	94.2	15.7	59.2	58.6	0.1	6.6
J1024−0719	86.3	13.0	62.4	61.9	1.0	3.6
J1327+3423	18.7	2.6	44.2	30.5	27.2	27.6
J1453+1902	86.2	9.1	62.9	62.7	−1.7	2.9
J1630+3734	79.5	11.8	41.3	39.8	0.1	4.3
J1640+2224	36.0	7.0	16.6	12.9	4.4	8.5
J1643−1224	79.2	10.2	22.5	17.1	−2.6	12.1
J1710+4923	94.7	16.5	19.2	15.4	−1.1	7.5
J1713+0747	91.8	4.3	31.7	31.1	−1.6	3.0
J1738+0333	41.6	6.5	25.2	24.7	−1.8	3.9
J1741+1351	41.4	4.1	21.7	20.9	2.5	4.3
J1744−1134	47.0	4.1	88.8	88.8	−1.9	1.9
J1745+1017	75.5	12.7	53.9	51.8	−9.7	10.1
J1832−0836	71.4	10.2	29.9	27.2	−2.3	7.4
J1843−1113	49.3	6.4	37.5	36.8	−0.7	2.2
J1853+1303	58.8	11.4	33.6	26.2	3.5	16.9
J1857+0943	75.2	12.5	15.3	14.2	−0.1	4.3
J1903+0327	83.0	17.5	15.2	9.7	−10.8	10.8
J1910+1256	32.8	4.4	22.4	16.3	−0.4	14.1
J1911−1114	53.6	13.1	26.7	22.1	−5.9	9.5
J1911+1347	67.2	4.4	46.6	36.5	21.0	24.3
J1918−0642	61.7	5.7	21.4	19.5	−5.0	6.1
J1923+2515	58.8	10.8	22.5	21.7	−2.6	3.0
J1944+0907	90.0	22.9	17.7	13.5	7.7	8.9
J1946+3417	93.6	12.9	20.9	18.9	−4.7	5.3
J1955+2908	81.2	14.2	35.8	26.1	−7.5	21.5
J2010−1323	18.8	5.0	20.0	17.9	1.2	7.0
J2017+0603	69.5	10.7	38.5	38.2	−1.9	3.5
J2019+2425	79.5	18.8	40.7	40.1	1.0	3.0
J2022+2534	79.5	13.1	25.5	24.1	2.5	5.3
J2033+1734	46.1	6.0	37.9	32.0	−1.6	13.1
J2043+1711	76.0	9.8	60.3	59.3	1.9	4.5
J2145−0750	87.7	6.9	19.8	16.9	5.9	7.8
J2150−0326	37.0	5.5	15.1	14.8	−0.8	1.8
J2214+3000	72.4	9.4	38.9	39.0	0.4	0.5
J2229+2643	35.5	14.1	19.4	17.0	4.0	7.5
J2234+0611	71.5	4.2	36.9	36.8	2.6	2.7
J2234+0944	89.6	11.5	23.5	21.4	5.9	6.3
J2302+4442	92.2	21.1	56.5	56.3	−1.4	2.7
J2317+1439	52.0	11.7	32.4	29.9	7.2	7.3
J2322+2057	53.4	9.2	13.5	11.2	−1.1	5.8

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